diff --git a/.copier-answers.yml b/.copier-answers.yml new file mode 100644 index 000000000..7d155460d --- /dev/null +++ b/.copier-answers.yml @@ -0,0 +1,9 @@ +# Changes here will be overwritten by Copier; NEVER EDIT MANUALLY +_commit: 0.1.0 +_src_path: https://github.com/python-accelerator-middle-layer/pyaml-repository-template.git +distribution_name: accelerator-middle-layer +html_title: pyaml +import_name: pyaml +package_name: pyaml +repository_url: https://github.com/python-accelerator-middle-layer/pyaml +use_docs_extra: false diff --git a/.github/workflows/documentation.yml b/.github/workflows/documentation.yml deleted file mode 100644 index 784e1894f..000000000 --- a/.github/workflows/documentation.yml +++ /dev/null @@ -1,82 +0,0 @@ -defaults: - run: - shell: bash - -on: # Runs on any push event in a PR or any push event to master - pull_request: - push: - branches: - - 'main' - -permissions: write-all - -jobs: - documentation: - name: ${{ matrix.os }} / ${{ matrix.python-version }} - - runs-on: ${{ matrix.os }} - - strategy: - matrix: # only lowest supported Python on latest ubuntu - os: [ubuntu-latest] - python-version: [3.14] - - permissions: - issues: write - pull-requests: write - contents: write - pages: write - - steps: - - uses: actions/checkout@v4 - - - name: Set up Python ${{ matrix.python-version }} - uses: actions/setup-python@v5 - with: - python-version: ${{ matrix.python-version }} - cache: 'pip' - cache-dependency-path: '**/pyproject.toml' - - - name: Get full Python version - id: full-python-version - run: echo ::set-output name=version::$(python -c "import sys; print('-'.join(str(v) for v in sys.version_info))") - - - name: Upgrade pip, setuptools and wheel - run: python -m pip install --upgrade pip - - - name: Install package - run: | - python -m pip install '.[doc]' - - - name: Build documentation - run: make html - working-directory: docs - - - name: Upload build artifacts # upload artifacts so reviewers can have a quick look without building documentation from the branch locally - uses: actions/upload-artifact@v4 - # if: success() && github.event_name == 'pull_request' # only for pushes in PR - with: - name: site-build - path: ./docs/_build - retention-days: 5 - - - name: Trigger RTDs build - uses: dfm/rtds-action@v1 - with: - webhook_url: ${{ secrets.RTDS_WEBHOOK_URL }} - webhook_token: ${{ secrets.RTDS_WEBHOOK_TOKEN }} - commit_ref: ${{ github.ref }} - - - name: Upload documentation - if: success() && github.ref == 'refs/heads/main' # only for pushes to master - uses: JamesIves/github-pages-deploy-action@v4 - with: - GITHUB_TOKEN: ${{ secrets.GITHUB_TOKEN }} - BRANCH: gh-pages - folder: docs/_build # The folder the action should deploy. - - # - name: Publish Docs to gh-pages - # uses: peaceiris/actions-gh-pages@373f7f263a76c20808c831209c920827a82a2847 - # with: - # github_token: ${{ secrets.GITHUB_TOKEN }} - # publish_dir: docs/_build/html diff --git a/.github/workflows/dt4acc-integration.yml b/.github/workflows/dt4acc-integration.yml new file mode 100644 index 000000000..e1c0585f3 --- /dev/null +++ b/.github/workflows/dt4acc-integration.yml @@ -0,0 +1,128 @@ +name: dt4acc integration + +on: + workflow_dispatch: + inputs: + dt4acc_image_uri: + description: "Apptainer ORAS image URI for the dt4acc twin" + required: false + default: "oras://registry.synchrotron-soleil.fr/software_control_system_public/dt4acc-soleil-twin:latest" + pull_request: + branches: ["main"] + paths: + - ".github/workflows/dt4acc-integration.yml" + - "pyaml/**" + - "tests/integration/**" + - "pyproject.toml" + +permissions: + contents: read + +jobs: + smoke: + runs-on: ubuntu-latest + timeout-minutes: 30 + + defaults: + run: + shell: bash -el {0} + + env: + TANGO_HOST: 127.0.0.1:10000 + DT4ACC_IMAGE_URI: ${{ inputs.dt4acc_image_uri || 'oras://registry.synchrotron-soleil.fr/software_control_system_public/dt4acc-soleil-twin:latest' }} + DT4ACC_REGISTRY_USER: ${{ secrets.DT4ACC_REGISTRY_USER }} + DT4ACC_REGISTRY_PASSWORD: ${{ secrets.DT4ACC_REGISTRY_PASSWORD }} + + steps: + - uses: actions/checkout@v4 + with: + repository: ${{ github.event.pull_request.head.repo.full_name || github.repository }} + ref: ${{ github.event.pull_request.head.ref || github.ref_name }} + + - name: Set up Apptainer + uses: eWaterCycle/setup-apptainer@v2 + + - name: Set up Python environment + uses: mamba-org/setup-micromamba@v2 + with: + environment-name: pyaml-dt4acc-integration + create-args: >- + -c conda-forge + python=3.12 + pip + pytest + pytango + cache-environment: true + + - name: Install pyAML and control-system backends + run: | + python -m pip install --upgrade pip + python -m pip install -e ".[test]" + python -m pip install "ophyd-async[tango, ca, pva]" + python -m pip install --no-deps \ + "tango-pyaml @ git+https://github.com/python-accelerator-middle-layer/tango-pyaml.git@1f010735bd675ad2f918958abd0396cb6766f14e" \ + "pyaml-cs-oa @ git+https://github.com/python-accelerator-middle-layer/pyaml-cs-oa.git@0.2.0" + python -c "import tango; import tango.pyaml; import pyaml_cs_oa" + + - name: Log in to GitLab registry + if: ${{ env.DT4ACC_REGISTRY_USER != '' && env.DT4ACC_REGISTRY_PASSWORD != '' }} + run: | + printf '%s' "${DT4ACC_REGISTRY_PASSWORD}" | + apptainer registry login \ + --username "${DT4ACC_REGISTRY_USER}" \ + --password-stdin \ + oras://gitlab-registry.synchrotron-soleil.fr + + - name: Pull dt4acc twin image + run: | + mkdir -p "${RUNNER_TEMP}/apptainer" + apptainer pull --force --disable-cache \ + "${RUNNER_TEMP}/apptainer/dt4acc-soleil-twin.sif" \ + "${DT4ACC_IMAGE_URI}" + + - name: Start dt4acc twin + run: | + LOG_FILE="${RUNNER_TEMP}/dt4acc-twin.log" + PID_FILE="${RUNNER_TEMP}/dt4acc-twin.pid" + + ACCEL_SETUP_FILE=$(python -c "from pyaml_test_lattice import configurations; print(configurations['dt4acc/fodo_1gev_6d_dt4acc_tango.json'])") + LATTICE_FILE=$(python -c "from pyaml_test_lattice import lattices; print(lattices['fodo_1gev_6d.json'])") + + bash tests/integration/start_dt4acc_twin.sh \ + --accelerator-setup-file "${ACCEL_SETUP_FILE}" \ + --lattice-file "${LATTICE_FILE}" \ + --tango-host "${TANGO_HOST%:*}" \ + --tango-port "${TANGO_HOST##*:}" \ + --sif "${RUNNER_TEMP}/apptainer/dt4acc-soleil-twin.sif" \ + --log-file "${LOG_FILE}" \ + --pid-file "${PID_FILE}" \ + --timeout 900 \ + --detach + + - name: Run pyAML dt4acc smoke test + env: + PYAML_DT4ACC_INTEGRATION: "1" + TANGO_HOST: "127.0.0.1:10000" + run: | + python -m pytest -v tests/integration/test_dt4acc_twin_smoke.py + + - name: Stop dt4acc twin + if: always() + run: | + PID_FILE="${RUNNER_TEMP}/dt4acc-twin.pid" + if [ -f "${PID_FILE}" ]; then + TWIN_PID="$(cat "${PID_FILE}")" + kill -- "-${TWIN_PID}" 2>/dev/null || kill "${TWIN_PID}" 2>/dev/null || true + sleep 5 + kill -KILL -- "-${TWIN_PID}" 2>/dev/null || kill -KILL "${TWIN_PID}" 2>/dev/null || true + fi + if [ -f "${RUNNER_TEMP}/dt4acc-twin.log" ]; then + tail -n 200 "${RUNNER_TEMP}/dt4acc-twin.log" || true + fi + + - name: Upload dt4acc logs + if: always() + uses: actions/upload-artifact@v4 + with: + name: dt4acc-twin-log + path: ${{ runner.temp }}/dt4acc-twin.log diff --git a/.github/workflows/github-release.yml b/.github/workflows/github-release.yml new file mode 100644 index 000000000..d92832a9b --- /dev/null +++ b/.github/workflows/github-release.yml @@ -0,0 +1,49 @@ +name: GitHub Release + +on: + push: + tags: + - '[0-9]+.[0-9]+.[0-9]+*' + +permissions: + contents: write + +jobs: + release: + name: Build and create release on GitHub + runs-on: ubuntu-latest + + steps: + - name: Check out source + uses: actions/checkout@v5 + + - name: Set up Python + uses: actions/setup-python@v6 + with: + python-version: "3.11" + + - name: Install Hatch + run: python -m pip install --upgrade hatch + + - name: Build distribution + run: hatch build + + - name: Determine whether this is a pre-release + id: release_type + shell: bash + run: | + tag="${GITHUB_REF_NAME#v}" + + if [[ "$tag" =~ (\.dev[0-9]+|a[0-9]+|b[0-9]+|rc[0-9]+)$ ]]; then + echo "prerelease=true" >> "$GITHUB_OUTPUT" + else + echo "prerelease=false" >> "$GITHUB_OUTPUT" + fi + + - name: Create GitHub release + uses: softprops/action-gh-release@v3 + with: + draft: false + prerelease: ${{ steps.release_type.outputs.prerelease }} + generate_release_notes: true + files: dist/* diff --git a/.github/workflows/ruff_formatting.yml b/.github/workflows/ruff_formatting.yml index bbce2ccbe..326184284 100644 --- a/.github/workflows/ruff_formatting.yml +++ b/.github/workflows/ruff_formatting.yml @@ -4,7 +4,6 @@ on: push: branches: [ main ] pull_request: - branches: [ main ] jobs: ruff-check: diff --git a/.github/workflows/tests.yml b/.github/workflows/unit-tests.yml similarity index 60% rename from .github/workflows/tests.yml rename to .github/workflows/unit-tests.yml index 39f13effc..b0bad8d9e 100644 --- a/.github/workflows/tests.yml +++ b/.github/workflows/unit-tests.yml @@ -1,13 +1,13 @@ -# This workflow will install Python dependencies, run tests and lint with a single version of Python +# This workflow will install Python dependencies, run tests and lint with a several version of Python # For more information see: https://docs.github.com/en/actions/automating-builds-and-tests/building-and-testing-python -name: run tests +name: Run unit tests on: push: branches: [ "main" ] pull_request: - branches: [ "main" ] + workflow_dispatch: permissions: contents: read @@ -16,15 +16,22 @@ jobs: build: runs-on: ubuntu-latest + strategy: + fail-fast: false + matrix: + python-version: >- + ${{ (github.event_name == 'push' || github.event_name == 'workflow_dispatch') + && fromJSON(vars.PYTHON_ALL_SUPPORTED_TEST_VERSIONS) + || fromJSON(vars.PYTHON_DEFAULT_TEST_VERSIONS) }} steps: - - uses: actions/checkout@v4 - with: - submodules: recursive - - name: Set up Python 3.12 - uses: actions/setup-python@v3 + - uses: actions/checkout@v6 + + - name: Set up Python ${{ matrix.python-version }} + uses: actions/setup-python@v7 with: - python-version: ">=3.12" + python-version: ${{ matrix.python-version }} + - name: Install dependencies run: | python -m pip install --upgrade pip @@ -32,11 +39,16 @@ jobs: pip install ./tests/dummy_cs/tango-pyaml pip install ./tests/external pip install flake8 + + - name: Display Python version + run: python -c "import sys; print(sys.version)" + - name: Lint with flake8 run: | # stop the build if there are Python syntax errors or undefined names flake8 . --count --select=E9,F63,F7,F82 --show-source --statistics # exit-zero treats all errors as warnings. The GitHub editor is 127 chars wide flake8 . --count --exit-zero --max-complexity=10 --max-line-length=127 --statistics + - name: Test with pytest run: python -m pytest tests diff --git a/.readthedocs.yaml b/.readthedocs.yaml index 053a457cd..4e993c186 100644 --- a/.readthedocs.yaml +++ b/.readthedocs.yaml @@ -1,39 +1,25 @@ -# .readthedocs.yaml # Read the Docs configuration file # See https://docs.readthedocs.io/en/stable/config-file/v2.html for details # Required version: 2 -# Set the OS, Python version and other tools you might need +# Set the OS, Python version, and other tools you might need build: os: ubuntu-24.04 tools: python: "3.13" - # You can also specify other tool versions: - # nodejs: "23" - # rust: "1.82" - # golang: "1.23" # Build documentation in the "docs/" directory with Sphinx sphinx: - configuration: docs/conf.py + configuration: docs/source/conf.py -# Optionally build your docs in additional formats such as PDF and ePub -# formats: -# - pdf -# - epub - -# Optional but recommended, declare the Python requirements required -# to build your documentation +# Optionally, but recommended, +# declare the Python requirements required to build your documentation # See https://docs.readthedocs.io/en/stable/guides/reproducible-builds.html python: install: + - requirements: docs/requirements.txt - method: pip path: . - extra_requirements: - - doc - -submodules: - include: all - recursive: true + extra_requirements: [] diff --git a/README.md b/README.md index 9e7cd237f..e9080dbb4 100644 --- a/README.md +++ b/README.md @@ -1,32 +1,50 @@ -[![Documentation Status](https://readthedocs.org/projects/pyaml/badge/?version=latest)](https://pyaml.readthedocs.io/en/latest/?badge=latest) -![Current release](https://img.shields.io/github/v/tag/python-accelerator-middle-layer/pyaml) +# pyaml -# Python Accelerator Middle Layer +**Package for the Python Accelerator Middle Layer core** -Python Accelerator Middle Layer (pyAML) is a joint technology platform for design, commissioning and operation of particle accelerators. +[![Documentation Status](https://readthedocs.org/projects/pyaml/badge/?version=stable)](https://pyaml.readthedocs.io/en/stable/?badge=stable) +[![Latest stable release](https://img.shields.io/pypi/v/accelerator-middle-layer.svg)](https://pypi.org/project/accelerator-middle-layer/) -The code is still under development. The features include among others: +## Overview -- A control system agnostic interface to interact with the accelerator. -- Same interface to different backends: live accelerator, virtual accelerator and simulator. -- Machine independence allowing configuration of different type of accelerators and facility specific naming conventions. -- Unit conversions. -- Automatic generation of metadata and standardized format for measurement data. -- A set of standard applications and a framework for developing new applications. + -**This repository is for the core of pyAML.** It is control system independent and provides the core functionality of pyAML. It is intended to be used together with a package that implements the control system specific interface. +Python Accelerator Middle Layer (pyAML) is a joint technology platform for design, commissioning and operation of particle accelerators. This repository is for the core of pyAML. It is control system independent and is intended to be used together with a package that implements the control system specific interface. -Available packages for bindings: +## Installation -TANGO: [tango-pyaml](https://github.com/python-accelerator-middle-layer/tango-pyaml) -TANGO or EPICS: [pyaml-cs-oa](https://github.com/python-accelerator-middle-layer/pyaml-cs-oa) +Install the package from PyPI: -#### Installation +```bash +pip install accelerator-middle-layer +``` -Installation instructions for both user and development installation can be found in the [documentation](https://pyaml.readthedocs.io/en/latest/?badge=latest). +## Development -#### Documentation +Install the development dependencies with: -The documentation is available [here](https://pyaml.readthedocs.io/en/latest/?badge=latest). +```bash +pip install accelerator-middle-layer[dev] +``` -In the documentation there are both examples and Jupyter notebooks available for how to use the package. +Run the test suite with: + +```bash +pytest +``` + +Install the pre-commit hooks with: + +```bash +pre-commit install +``` + +## Documentation + +The documentation is available at: + + + +## Contributing + +Please use the issue tracker or submit a pull request. diff --git a/docs/.gitignore b/docs/.gitignore deleted file mode 100644 index 8edc9a634..000000000 --- a/docs/.gitignore +++ /dev/null @@ -1 +0,0 @@ -api.rst diff --git a/docs/Makefile b/docs/Makefile index 13262b8ca..d0c3cbf10 100644 --- a/docs/Makefile +++ b/docs/Makefile @@ -5,9 +5,8 @@ # from the environment for the first two. SPHINXOPTS ?= SPHINXBUILD ?= sphinx-build -SOURCEDIR = . -BUILDDIR = _build -HTMLDIR = ../docs +SOURCEDIR = source +BUILDDIR = build # Put it first so that "make" without argument is like "make help". help: @@ -15,17 +14,6 @@ help: .PHONY: help Makefile -show: - @python -m webbrowser -n "file://$$(pwd)/$(BUILDDIR)/html/index.html" - -test: Makefile - @$(SPHINXBUILD) -M $@ -d "$(BUILDDIR)/doctrees" "$(SOURCEDIR)" "$(HTMLDIR)" $(SPHINXOPTS) $(O) - -clean: Makefile - rm -f api.rst - rm -rf api/*.rst - @$(SPHINXBUILD) -M $@ "$(SOURCEDIR)" "$(BUILDDIR)" $(SPHINXOPTS) $(O) - # Catch-all target: route all unknown targets to Sphinx using the new # "make mode" option. $(O) is meant as a shortcut for $(SPHINXOPTS). %: Makefile diff --git a/docs/README.rst b/docs/README.rst deleted file mode 100644 index 482d41d55..000000000 --- a/docs/README.rst +++ /dev/null @@ -1,32 +0,0 @@ -################## -pyAML Documentation -################## - -This directory is the source of the pyAML documentation. - -********************************** -Contributing to documentation -********************************** - -Documentation tools -=================== - -The documentation is compiled with -`Sphinx `_. - -For a local check when writing documentation, Sphinx and the -necessary extensions are automatically installed if you install pyAML with -the [doc] option:: - - $ pip install -e ".[doc]" - -When committing the changes it's a good idea to also run the pre-commit. -This can be installed by following the instructions for [developer installation](https://pyaml.readthedocs.io/en/latest/getting-started/installation.html#developer-installation). - -Then, the compilation may be triggered from the ``docs`` directory with:: - - $ cd pyaml/docs - $ make html - -Since the `.rse` files generated by autosummary are kept in version control they are not automatically regenerated from scratch. -If you want to do that to make sure they are up-to-date you need to first delete the folder `api` before doing `make html`. diff --git a/docs/api/.gitignore b/docs/api/.gitignore deleted file mode 100644 index 30d85567b..000000000 --- a/docs/api/.gitignore +++ /dev/null @@ -1 +0,0 @@ -*.rst diff --git a/docs/conf.py b/docs/conf.py deleted file mode 100644 index 37114082b..000000000 --- a/docs/conf.py +++ /dev/null @@ -1,391 +0,0 @@ -# Configuration file for the Sphinx documentation builder. -# -# This file only contains a selection of the most common options. For a full -# list see the documentation: -# https://www.sphinx-doc.org/en/master/usage/configuration.html - -# -- Path setup -------------------------------------------------------------- - -# If extensions (or modules to document with autodoc) are in another directory, -# add these directories to sys.path here. If the directory is relative to the -# documentation root, use os.path.abspath to make it absolute, like shown here. -# -# import sys -# sys.path.insert(0, os.path.abspath('.')) -# sys.path.insert(0, os.path.abspath('../pyat')) -# print(sys.path) - -import pyaml - -# Generate reference API -from pyaml.apidoc.gen_api import gen_doc - -gen_doc() - -# -- Project information ----------------------------------------------------- - -project = "Python Accelerator Middle Layer" -project_copyright = "2024, pyAML Collaboration" -author = "pyAML Collaboration" - -# The full version, including alpha/beta/rc tags -release = ".".join(pyaml.__version__.split(".")[:3]) -version = ".".join(pyaml.__version__.split(".")[:2]) - -# -- General configuration ------------------------------------------------ - -# If your documentation needs a minimal Sphinx version, state it here. -# -# needs_sphinx = '1.0' - -# Add any Sphinx extension module names here, as strings. They can be -# extensions coming with Sphinx (named 'sphinx.ext.*') or your custom -# ones. - -root_doc = "index" -extensions = [ - "sphinx.ext.autosummary", # Automatically generates summary tables and stub pages - # for documented functions, classes, and modules - "sphinx.ext.napoleon", # Adds support for NumPy-style and Google-style docstrings, - # so you don’t have to write reStructuredText by hand. - "sphinx.ext.autodoc", # Adds support for NumPy-style and Google-style docstrings - # code snippets. - "sphinx.ext.intersphinx", # Allows you to link to documentation of other projects - # (e.g. NumPy, Python, SciPy) as if they were local. - "sphinx.ext.githubpages", # Adds support files (like .nojekyll) needed to publish - # docs on GitHub Pages. - "sphinx.ext.viewcode", # Adds links in the docs to view the source code of - # documented Python objects. - "myst_nb", # Enables MyST Markdown and Jupyter Notebook support. - "sphinx_copybutton", # Adds a “copy to clipboard” button to code blocks. - "sphinx_design", # Provides layout and design components - # (cards, grids, tabs, buttons). -] - -intersphinx_mapping = { - "python": ("https://docs.python.org/3", None), - "matplotlib": ("https://matplotlib.org/stable/", None), - "numpy": ("https://numpy.org/doc/stable/", None), - "scipy": ("https://docs.scipy.org/doc/scipy/", None), -} - -# Add any paths that contain templates here, relative to this directory. -templates_path = ["_templates"] - -# List of patterns, relative to source directory, that match files and -# directories to ignore when looking for source files. -# This pattern also affects html_static_path and html_extra_path. -exclude_patterns = ["README.rst", "**/*.so", "_build/*"] - -# Injects content at the top of every reStructuredText file before it’s parsed. -# Defines a custom inline role called :pycode: which renders inline code with Python -# syntax highlighting -rst_prolog = """ -.. role:: pycode(code) - :language: python -""" - -autodoc_default_options = { - # Make sure that any autodoc declarations show the right members - "members": True, - "undoc-members": True, - "show-inheritance": True, - "member-order": "groupwise", -} -autodoc_typehints = "description" -autodoc_typehints_description_target = "documented" -autodoc_typehints_format = "short" -autosummary_generate = True # Make _autosummary files and include them -autosummary_generate_overwrite = False -autosummary_ignore_module_all = False -autoclass_content = "both" # include both class docstring and __init__ - -napoleon_use_rtype = False # More legible -# napoleon_numpy_docstring = False # Force consistency, leave only Google -napoleon_custom_sections = [("Returns", "params_style")] - -add_module_names = False - -# -- Options for the myst markdown parser ------------------------------------ - -myst_enable_extensions = [ - "attrs_inline", - "colon_fence", - "dollarmath", - "replacements", - "deflist", -] -myst_heading_anchors = 3 -nb_execution_mode = "auto" -nb_execution_allow_errors = True - -# -- Options for HTML output ------------------------------------------------- - -# The theme to use for HTML and HTML Help pages. See the documentation for -# a list of builtin themes. -# -# html_theme = 'alabaster' -# html_theme = 'sphinx_rtd_theme' -# html_theme = 'sphinx_book_theme' -html_theme = "pydata_sphinx_theme" -html_logo = "_static/img/logo.png" -html_copy_source = False -html_theme_options = { - "github_url": "https://github.com/python-accelerator-middle-layer/pyaml", - "logo": { - "image_light": "_static/img/logo.png", - "image_dark": "_static/img/dark.png", - }, -} -html_sidebars = { - "index": [], - "common/about": [], -} -# creates an additional page, but impossible to link to it... -# if os.environ.get('READTHEDOCS') == 'True': -# html_additional_pages = { -# "index": "plink.html" -# } - -html_css_files = ["css/custom.css"] - -# Add any paths that contaAddedin custom static files (such as style sheets) here, -# relative to this directory. They are copied after the builtin static files, -# so a file named "default.css" will overwrite the builtin "default.css". -html_static_path = ["_static"] - -# -- Options for latex output ------------------------------------------------- - -# latex_documents = [ -# ( -# "p/index", -# "pyat.tex", -# "PyAT User's Guide", -# "The AT collaboration", -# "manual", -# True, -# ), -# ( -# "common/passmethods", -# "at.tex", -# "AT Integrators", -# "The AT collaboration", -# "manual", -# False, -# ), -# ] -# latex_logo = "images/ATlarge.png" - -latex_documents = [ - (root_doc, "pyaml.tex", "pyAML Documentation", "pyAML collaboration", "manual"), -] - -# -- Options for copybutton ------------------------------------------------- - -copybutton_prompt_text = r">>> |\.\.\. |\$ " -copybutton_prompt_is_regexp = True -copybutton_only_copy_prompt_lines = True - -# extensions = [ -# "sphinx.ext.autodoc", -# "sphinx.ext.doctest", -# "sphinx.ext.todo", -# "sphinx.ext.coverage", -# "sphinx.ext.mathjax", -# "sphinx.ext.viewcode", -# "sphinx.ext.githubpages", -# "sphinx.ext.napoleon", -# "sphinx.ext.autosectionlabel", -# "sphinx.ext.autosummary", -# "myst_nb", -# ] -# autosectionlabel_prefix_document = True -# autosectionlabel_maxdepth = 2 - -# # Add any paths that contain templates here, relative to this directory. -# # templates_path = ['_templates'] - -# # The suffix(es) of source filenames. -# # You can specify multiple suffix as a list of string: -# # -# # source_suffix = ['.rst', '.md'] -# source_suffix = ".rst" - -# # The master toctree document. -# master_doc = "index" - - -# # The language for content autogenerated by Sphinx. Refer to documentation -# # for a list of supported languages. -# # -# # This is also used if you do content translation via gettext catalogs. -# # Usually you set "language" from the command line for these cases. -# language = "en" - -# # List of patterns, relative to source directory, that match files and -# # directories to ignore when looking for source files. -# # This patterns also effect to html_static_path and html_extra_path -# exclude_patterns = [] - -# # The name of the Pygments (syntax highlighting) style to use. -# pygments_style = "sphinx" - -# # If true, `todo` and `todoList` produce output, else they produce nothing. -# todo_include_todos = True - -# # -- Options for HTML output ---------------------------------------------- - -# # The theme to use for HTML and HTML Help pages. See the documentation for -# # a list of builtin themes. -# # - -# # html_theme = 'classic' -# html_theme = "pydata_sphinx_theme" - -# # Theme options are theme-specific and customize the look and feel of a theme -# # further. For a list of options available for each theme, see the -# # documentation. - - -# # Name of an image file (path relative to the configuration directory) -# # that is the logo of the docs, or URL that points an image file for the logo. -# # It is placed at the top of the sidebar; -# # its width should therefore not exceed 200 pixels. -# html_logo = "_static/img/logo.png" -# html_copy_source = False - -# html_theme_options = { -# "collapse_navigation": False, -# "display_version": True, -# "logo_only": True, -# "navigation_depth": 6, -# "rightsidebar": True, -# "relbarbgcolor": "black", -# "github_url": "https://github.com/python-accelerator-middle-layer/pyaml", -# "logo": { -# "image_light": "_static/img/logo.png", -# "image_dark": "_static/img/dark.png", -# }, -# } - -# # Add any paths that contain custom static files (such as style sheets) here, -# # relative to this directory. They are copied after the builtin static files, -# # so a file named "default.css" will overwrite the builtin "default.css". -# # -# html_static_path = ["_static"] - -# # A dictionary of values to pass into the template engine’s context for all -# # pages. Single values can also be put in this dictionary using the -# # -A command-line option of sphinx-build. -# html_context = { -# "display_github": True, -# # the following are only needed if :github_url: is not set -# "github_user": author, -# "github_repo": project, -# "github_version": "main/docs/", -# } - -# # A list of CSS files. The entry must be a filename string or a tuple -# # containing the filename string and the attributes dictionary. -# # The filename must be relative to the html_static_path, or a full URI with -# # scheme like https://example.org/style.css. -# # The attributes is used for attributes of tag. -# # It defaults to an empty list. -# # -# html_css_files = ["css/custom.css"] - -# smartquotes_action = ( -# "qe" # renders only quotes and ellipses (...) but not dashes (option: D) -# ) - -# # Custom sidebar templates, must be a dictionary that maps document names -# # to template names. -# # -# # This is required for the alabaster theme -# # refs: http://alabaster.readthedocs.io/en/latest/installation.html#sidebars -# html_sidebars = { -# "**": [ -# "relations.html", # needs 'show_related': True theme option to display -# "searchbox.html", -# ], -# "index": [], -# "common/about": [], -# } - - -# # -- Options for HTMLHelp output ------------------------------------------ - -# # Output file base name for HTML help builder. -# htmlhelp_basename = "pyamldoc" - -# # -- Options for LaTeX output --------------------------------------------- - -# latex_elements = { -# # The paper size ('letterpaper' or 'a4paper'). -# # -# # 'papersize': 'letterpaper', -# # The font size ('10pt', '11pt' or '12pt'). -# # -# # 'pointsize': '10pt', -# # Additional stuff for the LaTeX preamble. -# # -# # 'preamble': '', -# # Latex figure (float) alignment -# # -# # 'figure_align': 'htbp', -# } - -# # Grouping the document tree into LaTeX files. List of tuples -# # (source start file, target name, title, -# # author, documentclass [howto, manual, or own class]). -# latex_documents = [ -# (master_doc, "pyaml.tex", "pyAML Documentation", "pyAML collaboration", "manual"), -# ] - -# # -- Options for manual page output --------------------------------------- - -# # One entry per manual page. List of tuples -# # (source start file, name, description, authors, manual section). -# man_pages = [(master_doc, "pyaml", "pyAML Documentation", [author], 1)] - -# # -- Options for Texinfo output ------------------------------------------- - -# # Grouping the document tree into Texinfo files. List of tuples -# # (source start file, target name, title, author, -# # dir menu entry, description, category) -# texinfo_documents = [ -# ( -# master_doc, -# "pyaml", -# "pyAML Documentation", -# author, -# "pyaml", -# "One line description of project.", -# "Miscellaneous", -# ), -# ] - -# # -- Autodoc Configuration --------------------------------------------------- - -# # Add here all modules to be mocked up. When the dependencies are not met -# # at building time. Here used to have PyQT mocked. -# autodoc_mock_imports = [ -# "PyQt5", -# "PyQt5.QtGui", -# "PyQt5.QtCore", -# "PyQt5.QtWidgets", -# "matplotlib.backends.backend_qt5agg", -# ] - -# # -- Options for the myst markdown parser ------------------------------------ - -# myst_enable_extensions = [ -# "attrs_inline", -# "colon_fence", -# "dollarmath", -# "replacements", -# "deflist", -# ] -# myst_heading_anchors = 3 -# nb_execution_mode = "off" # "auto" -# nb_execution_allow_errors = True diff --git a/docs/getting-started/configuration.md b/docs/getting-started/configuration.md deleted file mode 100644 index 9df0aa9c6..000000000 --- a/docs/getting-started/configuration.md +++ /dev/null @@ -1,4 +0,0 @@ -Setting up the Configuration -====== - -To write... diff --git a/docs/getting-started/contribute.md b/docs/getting-started/contribute.md deleted file mode 100644 index 5e0621cda..000000000 --- a/docs/getting-started/contribute.md +++ /dev/null @@ -1,5 +0,0 @@ -How to Contribute -================= - -```{include} ../../CONTRIBUTING.md -:start-after: "# Contributing to [Python Accelerator Middle Layer (PyAML)]" diff --git a/docs/getting-started/index.rst b/docs/getting-started/index.rst deleted file mode 100644 index 4be6fe1d3..000000000 --- a/docs/getting-started/index.rst +++ /dev/null @@ -1,13 +0,0 @@ -Getting Started -====== - -If you are a new user or developer you find instructions here for how to get started. - -.. toctree:: - :maxdepth: 1 - - python-basics - installation - test-examples - configuration - contribute diff --git a/docs/getting-started/installation.md b/docs/getting-started/installation.md deleted file mode 100644 index caf720553..000000000 --- a/docs/getting-started/installation.md +++ /dev/null @@ -1,75 +0,0 @@ -Installation -================== - -## User Installation - -The latest release can be installed from PyPI. If you want to communicate with a control system you in addition need to install the bindings you want by specifing extras. - -You need at least Python 3.11. - -**Remember to always install in a virtual environment to avoid breaking your Python environment.** - -### Installing without Control System Bindings - - -For example if you just want to use the simulator. - -``` -pip install accelerator-middle-layer -``` - - -### Installing with Control System Bindings - -Available options for installing with control system bindings are: - -- `tango-pyaml` for the tango-pyaml bindings. -- `cs-oa-epics` for `ophyd-async` bindings with both EPICS channel and PV access. -- `cs-oa-tango` for `ophyd-async` bindings for TANGO. - -Example usage: - -``` -pip install accelerator-middle-layer[cs-oa-epics] -``` - -## Developer Installation - -To do development work you need to clone the source code from GitHub and install in editable mode. - -**Note: if you are not a maintainer of the code and have write permissions to the repository you need to first fork the repository.** - -1. Clone the repository (or your fork) - - The repository uses submodules so they also need to be initialized. This can be done in the same step by including ``--recurse-submodules``. - - Example usage: - - ``` - git clone --recurse-submodules https://github.com/python-accelerator-middle-layer/pyaml.git - ``` - -2. Make a virtual environment and activate it. It needs to use >= Python 3.11. - -3. Install the code in editable mode including development dependencies. - - ``` - cd pyaml - pip install -e .[dev] - ``` - -4. Install the pre-commit hooks. - - ``` - pre-commit install - ``` - -5. Install control system bindings *(optional)* - - If you want to use control system bindings you need to also install the package for the binding you want to use. Follow the installation instructions in the corresponding repository. - - If you want to do development work on the bindings they need to be installed in editable mode, but if not you can install the latest release from PyPI. - -6. Install dummy control system for TANGO *(optional)* - - If you want to test the TANGO bindings without requiring a live machine or virtual accelerator you can install the dummy TANGO control system available in `tests/dummy-cs/tango`. It is a simple emulation that allows to check the interface to the control system. The control system doesn't do anything but is only intended for tests during development. diff --git a/docs/getting-started/python-basics.md b/docs/getting-started/python-basics.md deleted file mode 100644 index 23dd71a0f..000000000 --- a/docs/getting-started/python-basics.md +++ /dev/null @@ -1,100 +0,0 @@ -For Users New to Python -======================== - -If you are a new Python user this page provides some help to get started. It also provides some advice for MATLAB users migrating to Python. - -Python is a large ecosystem with many tools to achieve similar things so this is not intended to be a complete list. Which tool to use is often based on personal preference and the intention of this guide is only to provide a starting point for you to find you preferred setup. - -Integrated Development Environments ------------------------------------------ - -Python can be run directly in a terminal or an [IPython](https://ipython.org/) shell but if you want to do more complex things like debug or develop code it is easier to use an Integrated Development Environment (IDE). There are many IDEs with Python support with different features, user experience etc so the choice is highly personal. Three common ones are: - -- **Spyder**: - [https://www.spyder-ide.org/](https://www.spyder-ide.org/) - - Spyder is designed for scientific computing and data analysis. It has the most MATLAB-like interface which often makes it a preferred choice among MATLAB users. It works well when using standard scientific Python packages but has currently less support for custom Python classes. It also only has basic Git integration and works best with conda environments. There is an plugin for Jupyter notebooks but it is not available for all the installation options yet. - -- **VS Code**: - [https://code.visualstudio.com/](https://code.visualstudio.com/) - - VS Code supports Python through extensions. It also has extensions for other programming languages as well as for Jupyter notebooks. It has a very good Git integration making it a good choice if you are new to using version control and prefer to not use the terminal. It also has very good support for all type of virtual environments. In addition, it has extensions to connect to remote services (such as clusters) and JupyterHub. Many HPC centers therefore provide a web-based version for their users. It however makes heavy use of keyboard shortcuts which can be a bit of a learning curve for new users. - -- **PyCharm**: - [https://www.jetbrains.com/pycharm/](https://www.jetbrains.com/pycharm/) - - PyCharm is a dedicated Python IDE. It has many features and customization possibilities and is often used by software professionals. There is both a community (free) and professional (paid) edition. - -If you are a new user getting started who doesn't know yet what you prefer, a good choice is likely to start with VS Code. - -Jupyter Notebooks ------------------ - -A very common way to run Python in the scientific community is to use [Jupyter notebooks](https://jupyter.org/). Is a browser-based tool which is very useful for data visualisation and interactive work. It can be installed both in a basic version **Jupyter Notebook** or as **JupyterLab** which provides some useful IDE features. It is common that tutorials will be in the form of a notebook. - -Installing Python ------------------ - -There are many different ways to get an installation of Python. An important aspect is that you at some point might need to be able to switch between different versions and have more than one version installed simultaneously. There are different options available for this. Here are some common ones: - -- **pyenv**: - [https://github.com/pyenv/pyenv](https://github.com/pyenv/pyenv) - - This is the most basic choice but probably too basic for most users. There is a plugin [pyenv-virtualenv](https://github.com/pyenv/pyenv-virtualenv) if you also want the tool to manage virtual environments. - -- **conda**: - [https://docs.conda.io/projects/conda/en/stable/](https://docs.conda.io/projects/conda/en/stable/) - - Conda is often used in the scientific community. There are several versions available and some might require a license. A good choice to avoid license issues is to choose [Miniforge](https://github.com/conda-forge/miniforge). This gives you a minimal installation of the free community edition. In addition to different Python versions, it also provides an easy way to manage and create virtual environments. - -- **uv**: - [https://docs.astral.sh/uv/](https://docs.astral.sh/uv/) - - Uv is a new tool which is intended as a single tool to replace the functionality of many other tools. In addition to managing Python versions and virtual environments it can also help to build packages. It however has a bit of a learning curve so is likely mostly a good choice for the experienced user who also wants to do development work. - -Python Packages ------------------ - -After you have installed Python you need to install packages for the code that you want to use. There are two common ways to do this: - -- **pip**: - [https://pip.pypa.io/en/stable/](https://pip.pypa.io/en/stable/) - - Pip is the standard package installer for Python. It is often automatically installed when you install Python and is easy to use. You can install from different sources as explained in the documentation [https://pip.pypa.io/en/stable/getting-started/](https://pip.pypa.io/en/stable/getting-started/). - -- **conda** - - If you are using conda, it also provides its own way of installing packages. You can however still use pip in conda environments in case the package is not available as a conda package. The installation is similar to when using pip [https://www.anaconda.com/docs/getting-started/working-with-conda/packages/install-packages](https://www.anaconda.com/docs/getting-started/working-with-conda/packages/install-packages). - - -Virtual Environments --------------------- - -A key aspect of a good Python setup is to use virtual environments. A virtual environment is a self-contained directory which contains a Python installation for a specific version plus additional packages. The purpose is to install packages without fear of compatibility issues that might cause your entire Python setup to break. If something goes wrong, you can just delete the virtual environment and start over. - -**You should never install Python packages in your default Python environment. It can cause big problems and especially if your computer is using an OS which relies on Python.** - -The recommended workflow is to always create a virtual environment, activate it and then install the Python packages you need into it. There are two different versions of virtual environments: - -- **venv**: - [https://docs.python.org/3/library/venv.html](https://docs.python.org/3/library/venv.html) - - This is the standard way that comes with the Python installation. It is very lightweight but can sometimes be annoying to use because you need to remember the command to activate the environment after it was created. The virtual environment is created in the current working folder so there is also no global way to manage your environments if you want an easy way to switch between environments. However, tools exist to extend the functionality such as [virtualenv](https://virtualenv.pypa.io/en/latest/) and [virtualenvwrapper](https://virtualenvwrapper.readthedocs.io/en/latest/). - -- **conda** - - Conda can also create virtual environments. It provides and easy way to activate and switch between environments so is a good choice for new users. - -Some IDEs has the functionality to help you create and switch between virtual environments. This works for both type of environments and can substantially simplify the workflow compared to using the terminal. - -Example Resources ------------------- - -There are many resources available for learning Python and also dedicated resources tailored for the scientific community. Several organisations provide free courses and material for scientists. Here are some recommendations: - -- **The Python documentation**: [https://www.python.org/](https://www.python.org/) -- **Python Packaging User Guide**: [https://packaging.python.org/en/latest/](https://packaging.python.org/en/latest/) -- **Scientific Python**: [https://scientific-python.org/](https://scientific-python.org/) -- **Carpentries**: [https://carpentries.org/](https://carpentries.org/) -- **CodeRefinery**: [https://coderefinery.org/](https://coderefinery.org/) -- **Software Sustainability Institute.**: [https://www.software.ac.uk/](https://www.software.ac.uk/) diff --git a/docs/getting-started/test-examples.md b/docs/getting-started/test-examples.md deleted file mode 100644 index da8c46175..000000000 --- a/docs/getting-started/test-examples.md +++ /dev/null @@ -1,8 +0,0 @@ -Test Examples -============== - -Test examples are available in the [examples folder](https://github.com/python-accelerator-middle-layer/pyaml/tree/main/examples). - -There you can also find instructions for how to run the examples. - -Some examples exist both as notebooks and scripts depending on how you prefer to run them. diff --git a/docs/how-to/apptainer.md b/docs/how-to/apptainer.md deleted file mode 100644 index 12ce814fc..000000000 --- a/docs/how-to/apptainer.md +++ /dev/null @@ -1,58 +0,0 @@ -Running Virtual Accelerator -============================= - -Virtual accelerators are available as [Apptainer](https://apptainer.org/) containers. -Instructions for how to install and run Apptainer on different OS are available here. -The instructions for how to run a specific virtual accelerator are available in the [examples folder](https://github.com/python-accelerator-middle-layer/pyaml/tree/main/examples). - -## Linux - -Installation instructions are available at [https://apptainer.org/docs/admin/main/installation.html#installation-on-linux](https://apptainer.org/docs/admin/main/installation.html#installation-on-linux). - -Try to first install using the [pre-build packages](https://apptainer.org/docs/admin/main/installation.html#install-from-pre-built-packages) for your Linux distribution. - -If that doesn't work (for example if it requires root permissions which you don't have), do an [unprivileged installation](https://apptainer.org/docs/admin/main/installation.html#install-from-pre-built-packages) instead. - -You should then be able to run Apptainer in a terminal. - -## Windows - -For Windows you need to install and run in [Windows Subsystem for Linux (WSL)](https://learn.microsoft.com/en-us/windows/wsl/). Follow the instructions at [https://apptainer.org/docs/admin/main/installation.html#windows](https://apptainer.org/docs/admin/main/installation.html#windows). - -You can then start the Ubuntu app which opens a Linux terminal where you can run Apptainer. - -## Mac - -For Mac you need to use Lima. Instructions are available at [https://apptainer.org/docs/admin/main/installation.html#mac](https://apptainer.org/docs/admin/main/installation.html#mac) but more detailed instructions are below since some additonal steps are required. - -For ARM-based MacOS server: - -``` -brew install qemu lima - -limactl start –rosetta –vm-type=vz –network=vzNAT template://apptainer -``` - -For Intel-based MacOS server: - -``` -brew install lima - -limactl start –vm-type=vz –network=vzNAT template://apptainer -``` - -To run the container you need to first do: - -``` -limactl shell apptainer -``` - -before you can run Apptainer. - -To stop the container you need to do: - -``` -limactl stop apptainer - -limactl delete apptainer -``` diff --git a/docs/how-to/index.rst b/docs/how-to/index.rst deleted file mode 100644 index a9252c9b0..000000000 --- a/docs/how-to/index.rst +++ /dev/null @@ -1,23 +0,0 @@ -How to Guides -============= - -Here you can find step-by-step guides for both new and experienced users. - -Basics -------- - -.. toctree:: - :maxdepth: 1 - - Load Configuration <../notebooks/load_configuration> - Control Modes <../notebooks/live_design> - Control System <../notebooks/control_system> - Use Arrays <../notebooks/arrays> - -Advanced -------- - -.. toctree:: - :maxdepth: 1 - - apptainer diff --git a/docs/index.rst b/docs/index.rst deleted file mode 100644 index 083423b55..000000000 --- a/docs/index.rst +++ /dev/null @@ -1,34 +0,0 @@ -Python Accelerator Middle Layer -=================== - -Python Accelerator Middle Layer (pyAML) is a joint technology platform for design, commissioning and operation of particle accelerators. - -The code is still under development. The features include among others: - -- A control system agnostic interface to interact with the accelerator. -- Same interface to different backends: live accelerator, virtual accelerator and simulator. -- Machine independence allowing configuration of different type of accelerators and facility specific naming conventions. -- Unit conversions. -- Automatic generation of metadata and standardized format for measurement data. -- A set of standard applications and a framework for developing new applications. - -Installation ------------- - -For installation instructions see :doc:`getting-started/installation`. - -.. toctree:: - :maxdepth: 1 - :hidden: - - getting-started/index - how-to/index - tutorial/index - api - -Indices ------------- - -* :ref:`genindex` -* :ref:`modindex` -* :ref:`search` diff --git a/docs/make.bat b/docs/make.bat index 32bb24529..747ffb7b3 100644 --- a/docs/make.bat +++ b/docs/make.bat @@ -7,8 +7,8 @@ REM Command file for Sphinx documentation if "%SPHINXBUILD%" == "" ( set SPHINXBUILD=sphinx-build ) -set SOURCEDIR=. -set BUILDDIR=_build +set SOURCEDIR=source +set BUILDDIR=build %SPHINXBUILD% >NUL 2>NUL if errorlevel 9009 ( diff --git a/docs/notebooks/arrays.ipynb b/docs/notebooks/arrays.ipynb deleted file mode 100644 index 898cf955f..000000000 --- a/docs/notebooks/arrays.ipynb +++ /dev/null @@ -1,59 +0,0 @@ -{ - "cells": [ - { - "cell_type": "markdown", - "id": "40dec8f5", - "metadata": {}, - "source": [ - "# use of magnet arrays\n", - "\n", - "In pyAML it is possible to configure magnet arrays (families of magnets)\n", - "\n", - "Some families are available by default:\n", - "- dipoles\n", - "- quadrupoles\n", - "- skewquadrupoles\n", - "- sextupoles\n", - "- horcorrectors\n", - "- vercorrectors\n", - "- octupoles\n", - "\n", - "Any other family (in the example my-family-of-quads) may be defined when configuring pyAML, using defined devices.\n", - "\n", - "```\n", - "type: pyaml.accelerator\n", - "name: sr\n", - "arrays:\n", - " - type: pyaml.arrays.magnet\n", - " name: my-family-of-quads\n", - " elements:\n", - " - QD2A-C03\n", - " - QD2E-C04\n", - " - QD2A-C05\n", - "devices: \n", - " - type: pyaml.magnet.quadrupole\n", - " name: QD2A-C03\n", - " - type: pyaml.magnet.quadrupole\n", - " name: QD2E-C04\n", - " - type: pyaml.magnet.quadrupole\n", - " name: QD2A-C05\n", - "```" - ] - }, - { - "cell_type": "markdown", - "id": "a78867b0", - "metadata": {}, - "source": [ - "Below some feature of magnets arrays is presented" - ] - } - ], - "metadata": { - "language_info": { - "name": "python" - } - }, - "nbformat": 4, - "nbformat_minor": 5 -} diff --git a/docs/notebooks/control_system.ipynb b/docs/notebooks/control_system.ipynb deleted file mode 100644 index 2639c6804..000000000 --- a/docs/notebooks/control_system.ipynb +++ /dev/null @@ -1,162 +0,0 @@ -{ - "cells": [ - { - "cell_type": "markdown", - "id": "7a473047", - "metadata": {}, - "source": [ - "# Control System set up" - ] - }, - { - "cell_type": "markdown", - "id": "62672006", - "metadata": {}, - "source": [ - "The control system interface is in a separated package from pyaml\n", - "\n", - "pyaml itself: \\\n", - "pip install accelerator-middle-layer\n", - "\n", - "tango interface to pyaml: \\\n", - "pip install tango-pyaml \n", - "\n", - "ophyd-asynch interface to pyaml: \\\n", - "pip install pyaml-oa-cs \n", - "\n", - "If the above packages are installed the examples below will work \n", - "\n" - ] - }, - { - "cell_type": "code", - "execution_count": null, - "id": "ae7657cc", - "metadata": {}, - "outputs": [], - "source": [ - "from pyaml.accelerator import Accelerator" - ] - }, - { - "cell_type": "markdown", - "id": "ff7bfc05", - "metadata": {}, - "source": [ - "Assuming these lines are present in ../../tests/config/EBSTune_TANGO.yaml\n", - "```\n", - "type: pyaml.accelerator\n", - "name: sr\n", - "energy: 6e9\n", - "controls:\n", - " - type: tango.pyaml.controlsystem\n", - " tango_host: ebs-simu-3:10000\n", - " name: live\n", - "...\n", - "powerconverter:\n", - " type: tango.pyaml.attribute\n", - "...\n", - "tune_h:\n", - " type: tango.pyaml.attribute_read_only\n", - "...\n", - "```" - ] - }, - { - "cell_type": "code", - "execution_count": null, - "id": "86dec08e", - "metadata": {}, - "outputs": [], - "source": [ - "# work with TANGO\n", - "SR_Tango: Accelerator = Accelerator.load(\"../../tests/config/EBSTune.yaml\")" - ] - }, - { - "cell_type": "markdown", - "id": "a61409b3", - "metadata": {}, - "source": [ - "Assuming these lines are present in ../../tests/config/EBSTuneOATango.yaml\n", - "```\n", - "type: pyaml.accelerator\n", - "name: sr\n", - "energy: 6e9\n", - "controls:\n", - " - type: pyaml-cs-oa.pyaml.controlsystem\n", - " name: live\n", - "...\n", - " powerconverter:\n", - " type: pyaml_cs_oa.tangoRW\n", - "...\n", - " tune_h:\n", - " type: pyaml_cs_oa.tangoR\n", - "```" - ] - }, - { - "cell_type": "markdown", - "id": "588bafd1", - "metadata": {}, - "source": [ - "this works with Ophyd-Asynch - tango:\n", - "\n", - "SR_OphydAsynch_Tango: Accelerator = Accelerator.load(\"../../tests/config/EBSTuneOATango.yaml\")" - ] - }, - { - "cell_type": "markdown", - "id": "62dfee77", - "metadata": {}, - "source": [ - "Assuming these lines are present in ../../tests/config/EBSTuneOAEpics.yaml\n", - "```\n", - "type: pyaml.accelerator\n", - "name: sr\n", - "energy: 6e9\n", - "controls:\n", - " - type: pyaml-cs-oa.pyaml.controlsystem\n", - " name: live\n", - "...\n", - " powerconverter:\n", - " type: pyaml_cs_oa.epicsRW\n", - "...\n", - " tune_h:\n", - " type: pyaml_cs_oa.epicsR\n", - "```" - ] - }, - { - "cell_type": "markdown", - "id": "b2da995b", - "metadata": {}, - "source": [ - "This work with Ophyd-Asynch - epics :\n", - "\n", - "SR_OphydAsynch_Epics: Accelerator = Accelerator.load(\"../../examples/BESSY2_example/BESSY2Tune.yaml\")" - ] - } - ], - "metadata": { - "kernelspec": { - "display_name": "pyaml_venv", - "language": "python", - "name": "python3" - }, - "language_info": { - "codemirror_mode": { - "name": "ipython", - "version": 3 - }, - "file_extension": ".py", - "mimetype": "text/x-python", - "name": "python", - "nbconvert_exporter": "python", - "pygments_lexer": "ipython3", - "version": "3.14.0" - } - }, - "nbformat": 4, - "nbformat_minor": 5 -} diff --git a/docs/notebooks/developper_install_instructions.ipynb b/docs/notebooks/developper_install_instructions.ipynb deleted file mode 100644 index 67cdf6993..000000000 --- a/docs/notebooks/developper_install_instructions.ipynb +++ /dev/null @@ -1,168 +0,0 @@ -{ - "cells": [ - { - "cell_type": "markdown", - "id": "29636569", - "metadata": {}, - "source": [ - "# developper installation instructions\n", - "\n", - "## prepare \n", - "cd work_dir\n", - "\n", - "deactivate existing python venv\n", - "\n", - "preconditions: \n", - "verify python version > 3.11 \n", - "verify github keys, or follow link to set them up \n", - "\n", - "## clone repositories for local development\n", - "```bash\n", - "git clone https://github.com/python-accelerator-middle-layer/tango-pyaml.git \n", - "git clone https://github.com/python-accelerator-middle-layer/pyaml.git \n", - "git clone https://github.com/python-accelerator-middle-layer/pyaml-cs-oa.git # optional\n", - "```\n", - "\n", - "## create virtual environment\n", - "python -m venv pyaml_venv \n", - "source ./pyaml_venv/bin/activate \n", - "pip install --upgrade pip \n", - "\n", - "## use latest pyAML version rather than latest release\n", - "```bash\n", - "cd pyaml \n", - "git submodule update --init --recursive \n", - "pip install -e . \n", - "cd .. \n", - "```\n", - "\n", - "## install tango-pyaml \n", - "\n", - "notice: do not do \"pip install -e .\" it does not work\n", - "\n", - "```bash\n", - "cd tango-pyaml \n", - "pip install . \n", - "cd .. \n", - "```\n", - "\n", - "[//]: # (OR latest ophid asych) \n", - "[//]: # (cd ../pyaml-cs-oa/ )\n", - "[//]: # (pip install -e . )\n", - "[//]: # (pip install -e .[dev] (very very long ~10 min on Simone's laptop) )\n", - "[//]: # (pre-commit install )\n", - "\n", - "## install dummy tango control system\n", - "\n", - "this will emulate device as in tango, but will not modify any beam dynamics value. only read/write of device attribute will be updated. read-only values will all return zero.\n", - "\n", - "```bash\n", - "cd pyaml\n", - "pip install ./tests/dummy_cs/tango-pyaml\n", - "cd ..\n", - "```\n", - "\n", - "## install virtual accelerator \n", - "SOLEIL will provide virtual accelerator installation scenario\n", - "\n", - "\n", - "## expected output\n", - "The output of pip list should be similar to: \n", - "```bash\n", - "accelerator-middle-layer 0.1.1 /Users/liuzzo/Desktop/test installation/pyaml \n", - "accelerator-toolbox 0.7.1 \n", - "annotated-types 0.7.0 \n", - "contourpy 1.3.3 \n", - "cycler 0.12.1 \n", - "docstring_parser 0.17.0 \n", - "fonttools 4.61.1 \n", - "h5py 3.15.1 \n", - "kiwisolver 1.4.9 \n", - "matplotlib 3.10.8 \n", - "numpy 2.3.5 \n", - "packaging 25.0 \n", - "pillow 12.0.0 \n", - "pip 25.3 \n", - "psutil 7.1.3 \n", - "pydantic 2.12.5 \n", - "pydantic_core 2.41.5 \n", - "pyparsing 3.2.5 \n", - "pytango 10.1.1 \n", - "python-dateutil 2.9.0.post0 \n", - "PyYAML 6.0.3 \n", - "scipy 1.16.3 \n", - "six 1.17.0 \n", - "tango-pyaml 0.3.1 \n", - "typing_extensions 4.15.0 \n", - "typing-inspection 0.4.2 \n", - "```\n", - "\n", - "## test that the installation is working correctly by running a pyAML example script\n", - "```bash\n", - "python ./pyaml/examples/ESRF_tune_example/esrf_tune_example.py \n", - "```\n", - "\n", - "## look at documentation to further test existing features\n", - "https://pyaml.readthedocs.io/en/latest/?badge=latest \n", - "\n", - "## example of development of pyaml documentation \n", - "```bash\n", - "cd pyaml\n", - "```\n", - "## create a new branch\n", - "```bash\n", - "git checkout -b doc-devnotebook\n", - "```\n", - "\n", - "## push the branch to remote\n", - "```bash\n", - "git push -u origin doc-devnotebook\n", - "```\n", - "\n", - "## modify something or add a file\n", - "```bash\n", - "edit ./pyaml/docs/notebooks/developper_install_instructions.ipynb \n", - "save\n", - "```\n", - "\n", - "## add file to git revision \n", - "```bash\n", - "git add docs/notebooks/developper_install_instructions.ipynb \n", - "```\n", - "\n", - "## test your code developments locally (in this example, build teh documentation locally)\n", - "```bash\n", - "pip install sphinx \n", - "pip install myst_nb \n", - "pip install pydata_sphinx_theme \n", - "python -m sphinx -b html docs ./docs/_build -d ./docs/_build \n", - "```\n", - "\n", - "## commit change\n", - "```bash\n", - "git commit ./docs/notebooks/developper_install_instructions.ipynb -m'some draft notes'\n", - "```\n", - "## push to remote\n", - "```bash\n", - "git push\n", - "```\n", - "### open a pull request to accept your change:\n", - "in a browser navigate to: https://github.com/python-accelerator-middle-layer/pyaml \n", - "click on \"compare and pull request\" \n", - "Add some description and click on Create pull request. \n", - "\n", - "The pull request page will open \n", - "Add reviewers to your pull request: in order to be approved, 2 positive reviews are needed. \n", - "\n", - "\n" - ] - } - ], - "metadata": { - "language_info": { - "name": "python" - } - }, - "nbformat": 4, - "nbformat_minor": 5 -} diff --git a/docs/notebooks/live_design.ipynb b/docs/notebooks/live_design.ipynb deleted file mode 100644 index 0afe46471..000000000 --- a/docs/notebooks/live_design.ipynb +++ /dev/null @@ -1,171 +0,0 @@ -{ - "cells": [ - { - "cell_type": "markdown", - "id": "d3621c17", - "metadata": {}, - "source": [ - "# Live/Design: control modes\n", - "\n", - "With *pyAML* it is possible to use the same commands either:\n", - "1. live: on the real accelerator\n", - "2. design: in simulations\n", - "3. errors: in simulations with errors (and for several seeds)\n", - "4. live (with a different prefix/host): in a virtual control system (same as in point 1. for those laboratories that have a simulated control system)\n", - "\n", - "Those are called \"control modes\" and may be used \n", - "- at a global script level (for testing in simulations and then using in real accelerator measurements with a simple switch/comment) \n", - "- anywhere in the script " - ] - }, - { - "cell_type": "markdown", - "id": "805b0f6c", - "metadata": {}, - "source": [ - "Using pyAML on a real accelerator" - ] - }, - { - "cell_type": "code", - "execution_count": null, - "id": "c4884e24", - "metadata": {}, - "outputs": [], - "source": [ - "import os\n", - "\n", - "import numpy as np\n", - "\n", - "from pyaml.accelerator import Accelerator" - ] - }, - { - "cell_type": "markdown", - "id": "b8ff1736", - "metadata": {}, - "source": [ - "instantiate a pyAML accelerator" - ] - }, - { - "cell_type": "code", - "execution_count": null, - "id": "fc1881d9", - "metadata": {}, - "outputs": [], - "source": [ - "SR: Accelerator = Accelerator.load(\"../../tests/config/EBSTune.yaml\")" - ] - }, - { - "cell_type": "markdown", - "id": "9a3c6e0a", - "metadata": {}, - "source": [ - "**Switch between live and design**" - ] - }, - { - "cell_type": "markdown", - "id": "4e55d6b6", - "metadata": {}, - "source": [ - "Access some magnet families defined in the configuration is simple. One can use sr.live for live control system or sr.design for the simulator part. They provide identical interface." - ] - }, - { - "cell_type": "code", - "execution_count": null, - "id": "31882398", - "metadata": {}, - "outputs": [], - "source": [ - "sr = SR.design # simulations\n", - "# sr = SR.live # act on real accelerator" - ] - }, - { - "cell_type": "code", - "execution_count": null, - "id": "b1fb943f", - "metadata": {}, - "outputs": [], - "source": [ - "quadForTune = sr.get_magnets(\"QForTune\")\n", - "\n", - "tune_device = sr.get_betatron_tune_monitor(\"BETATRON_TUNE\")" - ] - }, - { - "cell_type": "markdown", - "id": "fdc66eea", - "metadata": {}, - "source": [ - "For example a tune response matrix is evaluated below. This script is used identically for computation of theoretical values or to measure the response directly on the accelerator." - ] - }, - { - "cell_type": "code", - "execution_count": null, - "id": "d6dc44d3", - "metadata": {}, - "outputs": [], - "source": [ - "# Build tune response matrix\n", - "initial_tune = tune_device.tune.get()\n", - "print(f\"Tune via pyAML interface for design mode {initial_tune}\")\n", - "tunemat = np.zeros((len(quadForTune), 2))\n", - "\n", - "for idx, m in enumerate(quadForTune):\n", - " str = m.strength.get()\n", - " m.strength.set(str + 1e-4)\n", - " dq = tune_device.tune.get() - initial_tune\n", - " tunemat[idx] = dq * 1e4\n", - " m.strength.set(str)" - ] - }, - { - "cell_type": "markdown", - "id": "bf75c939", - "metadata": {}, - "source": [ - "At any point in the code it is always possible to still access any of the control modes" - ] - }, - { - "cell_type": "code", - "execution_count": null, - "id": "b5cec1f2", - "metadata": {}, - "outputs": [], - "source": [ - "SR.design.get_lattice().disable_6d()\n", - "tune_design = SR.design.get_lattice().get_tune()\n", - "\n", - "print(f\"Tune directly from the lattice {tune_design}\")" - ] - } - ], - "metadata": { - "kernelspec": { - "display_name": "Python 3 (ipykernel)", - "language": "python", - "name": "python3" - }, - "language_info": { - "codemirror_mode": { - "name": "ipython", - "version": 3 - }, - "file_extension": ".py", - "mimetype": "text/x-python", - "name": "python", - "nbconvert_exporter": "python", - "pygments_lexer": "ipython3", - "version": "3.12.3" - } - }, - "nbformat": 4, - "nbformat_minor": 5 -} diff --git a/docs/notebooks/load_configuration.ipynb b/docs/notebooks/load_configuration.ipynb deleted file mode 100644 index f1fe1a3fc..000000000 --- a/docs/notebooks/load_configuration.ipynb +++ /dev/null @@ -1,120 +0,0 @@ -{ - "cells": [ - { - "cell_type": "markdown", - "id": "420c1a3c", - "metadata": {}, - "source": [ - "# Configuration" - ] - }, - { - "cell_type": "code", - "execution_count": null, - "id": "7204f09a", - "metadata": {}, - "outputs": [], - "source": [ - "from pyaml.accelerator import Accelerator\n", - "\n", - "SR: Accelerator = Accelerator.load(\"../../tests/config/EBSTune.yaml\")" - ] - }, - { - "cell_type": "markdown", - "id": "f6ccb72a", - "metadata": {}, - "source": [ - "pyaml/tests/config/EBSTune.yaml is an example pyAML yaml configuration file that defines:\n", - "- a 6GeV Storage ring with\n", - " - 1 array (family) of quadrupoles used for tune correction\n", - " - 1 tune device\n", - " - controlled by Tango\n", - " - simulated with AT\n", - "\n", - "It looks like this: \n", - "\n", - "```\n", - "type: pyaml.accelerator\n", - "name: sr\n", - "energy: 6e9\n", - "simulators:\n", - " - type: pyaml.lattice.simulator\n", - " lattice: sr/lattices/ebs.mat\n", - " name: design\n", - "controls:\n", - " - type: tango.pyaml.controlsystem\n", - " tango_host: ebs-simu-3:10000\n", - " name: live\n", - "\n", - "data_folder: /data/store\n", - " arrays:\n", - " - type: pyaml.arrays.magnet\n", - " name: QForTune\n", - " elements:\n", - " - QD2A-C03\n", - " - QD2E-C04\n", - " - QD2A-C05\n", - " - ...\n", - " devices: \n", - " - type: pyaml.magnet.quadrupole\n", - " name: QD2A-C03\n", - " model:\n", - " type: pyaml.magnet.linear_model\n", - " calibration_factor: 1.002096389\n", - " crosstalk: 0.99912\n", - " curve:\n", - " type: pyaml.configuration.csvcurve\n", - " file: sr/magnet_models/QD2_strength.csv\n", - " unit: 1/m\n", - " powerconverter:\n", - " type: tango.pyaml.attribute\n", - " attribute: srmag/vps-qd2/c03-a/current\n", - " unit: A\n", - " - ... \n", - " - ...\n", - " - ...\n", - " - type: pyaml.diagnostics.tune_monitor\n", - " name: BETATRON_TUNE\n", - " tune_h:\n", - " type: tango.pyaml.attribute_read_only\n", - " attribute: srdiag/tune/tune_h\n", - " unit: mm\n", - " tune_v:\n", - " type: tango.pyaml.attribute_read_only\n", - " attribute: srdiag/tune/tune_v\n", - " unit: mm\n", - "```\n" - ] - }, - { - "cell_type": "code", - "execution_count": null, - "id": "0a3805fd-f96d-4ca0-9246-97b30baa1c32", - "metadata": {}, - "outputs": [], - "source": [] - } - ], - "metadata": { - "kernelspec": { - "display_name": "Python 3 (ipykernel)", - "language": "python", - "name": "python3" - }, - "language_info": { - "codemirror_mode": { - "name": "ipython", - "version": 3 - }, - "file_extension": ".py", - "mimetype": "text/x-python", - "name": "python", - "nbconvert_exporter": "python", - "pygments_lexer": "ipython3", - "version": "3.12.3" - } - }, - "nbformat": 4, - "nbformat_minor": 5 -} diff --git a/docs/requirements.txt b/docs/requirements.txt new file mode 100644 index 000000000..0c8945196 --- /dev/null +++ b/docs/requirements.txt @@ -0,0 +1,4 @@ +sphinx~= 8.1 +pydata-sphinx-theme +myst_parser +sphinx-copybutton diff --git a/docs/_static/img/dark.png b/docs/source/_static/_images/dark.png similarity index 100% rename from docs/_static/img/dark.png rename to docs/source/_static/_images/dark.png diff --git a/docs/_static/img/logo.png b/docs/source/_static/_images/logo.png similarity index 100% rename from docs/_static/img/logo.png rename to docs/source/_static/_images/logo.png diff --git a/docs/_static/img/logosmall.png b/docs/source/_static/_images/logosmall.png similarity index 100% rename from docs/_static/img/logosmall.png rename to docs/source/_static/_images/logosmall.png diff --git a/docs/source/_static/custom.css b/docs/source/_static/custom.css new file mode 100644 index 000000000..299703078 --- /dev/null +++ b/docs/source/_static/custom.css @@ -0,0 +1,7 @@ +.api-root h1 { + display: none; +} + +.api-generation { + display: none; +} diff --git a/pyaml/lattice/element.py b/docs/source/_templates/.gitkeep similarity index 100% rename from pyaml/lattice/element.py rename to docs/source/_templates/.gitkeep diff --git a/docs/source/api.rst b/docs/source/api.rst new file mode 100644 index 000000000..7ab089cef --- /dev/null +++ b/docs/source/api.rst @@ -0,0 +1,14 @@ +API Reference +============= + +.. container:: api-generation + + .. autosummary:: + :toctree: api + :recursive: + + pyaml + +.. container:: api-root + + .. include:: api/pyaml.rst diff --git a/docs/source/conf.py b/docs/source/conf.py new file mode 100644 index 000000000..560eafeda --- /dev/null +++ b/docs/source/conf.py @@ -0,0 +1,73 @@ +# Configuration file for the Sphinx documentation builder. +# +# For the full list of built-in configuration values, see the documentation: +# https://www.sphinx-doc.org/en/master/usage/configuration.html + + +# -- Project information ----------------------------------------------------- +# https://www.sphinx-doc.org/en/master/usage/configuration.html#project-information + +project = "pyaml" +copyright = "2026, pyAML Collaboration" +author = "pyAML Collaboration" + +# -- General configuration --------------------------------------------------- +# https://www.sphinx-doc.org/en/master/usage/configuration.html#general-configuration + +extensions = [ + "sphinx.ext.autodoc", + "sphinx.ext.autosummary", + "sphinx.ext.napoleon", + "myst_parser", + "sphinx_copybutton", +] + +autosummary_generate = True + +# Maybe add "undoc-members": True here later +autodoc_default_options = {"members": True, "show-inheritance": True, "member-order": "groupwise"} + +autodoc_typehints = "description" +autodoc_typehints_description_target = "documented" +autodoc_typehints_format = "short" +# autosummary_generate_overwrite = False +# autosummary_ignore_module_all = False +autoclass_content = "both" # include both class docstring and __init__ + +napoleon_use_rtype = False # More legible +# napoleon_numpy_docstring = False # Force consistency, leave only Google +# napoleon_custom_sections = [("Returns", "params_style")] + +templates_path = ["_templates"] +exclude_patterns = [] + + +# -- Options for HTML output ------------------------------------------------- +# https://www.sphinx-doc.org/en/master/usage/configuration.html#options-for-html-output + +html_theme = "pydata_sphinx_theme" +html_static_path = ["_static"] +html_title = "pyaml" +html_show_sourcelink = False +html_css_files = ["custom.css"] +html_logo = "_static/_images/logo.png" + +html_theme_options = { + "navigation_depth": 4, + "show_nav_level": 2, + "icon_links": [ + { + "name": "GitHub", + "url": "https://github.com/python-accelerator-middle-layer/pyaml", + "icon": "fa-brands fa-github", + "type": "fontawesome", + }, + ], +} + +html_sidebars = { + "**": [ + "sidebar-collapse", + "sidebar-nav-bs", + ], +} diff --git a/docs/source/index.rst b/docs/source/index.rst new file mode 100644 index 000000000..90a87b0f2 --- /dev/null +++ b/docs/source/index.rst @@ -0,0 +1,16 @@ + +.. include:: ../../README.md + :parser: myst_parser.sphinx_ + +.. seealso:: + + This package is part of the + `pyAML ecosystem `__. + See the `main pyAML documentation + `__ + for tutorials, how-to guides, and an overview of the ecosystem. + +.. toctree:: + :hidden: + + api diff --git a/docs/tutorial/index.rst b/docs/tutorial/index.rst deleted file mode 100644 index a8ce84425..000000000 --- a/docs/tutorial/index.rst +++ /dev/null @@ -1,15 +0,0 @@ -Tutorials -============= - -Here you can find tutorials to LEARN how to use the accelerator middle layer software. - -Basics -------- - -.. toctree:: - :maxdepth: 1 - - How to correct tunes - -Advanced ---------- diff --git a/examples/BESSY2_example/BESSY2Chroma.yaml b/examples/BESSY2_example/BESSY2Chroma.yaml deleted file mode 100644 index 3060ff55a..000000000 --- a/examples/BESSY2_example/BESSY2Chroma.yaml +++ /dev/null @@ -1,41 +0,0 @@ -type: pyaml.accelerator -facility: BESSY2 -machine: sr -energy: 1.7e9 -simulators: -- type: pyaml.lattice.simulator - lattice: bessy2_standard_user.mat - name: design -controls: -- type: pyaml_cs_oa.controlsystem - prefix: 'pons:' - name: live -data_folder: /data/store -devices: -- type: pyaml.diagnostics.tune_monitor - name: BETATRON_TUNE - tune_h: - type: pyaml_cs_oa.epicsR - read_pvname: beam:twiss:x:tune - unit: '' - tune_v: - type: pyaml_cs_oa.epicsR - read_pvname: beam:twiss:y:tune - unit: '' -- type: pyaml.diagnostics.chromaticity_monitor - name: KSI - betatron_tune_name: BETATRON_TUNE - rf_plant_name: RF - fit_order: 2 - n_avg_meas: 1 - n_step: 5 - sleep_between_meas: 2 - sleep_between_step: 2 - e_delta: 1e-3 - max_e_delta: 1e-3 -- type: pyaml.rf.rf_plant - name: RF - masterclock: - type: pyaml_cs_oa.epicsW - write_pvname: MCLKHX251C:freq - unit: KHz diff --git a/examples/BESSY2_example/BESSY2Orbit.yaml b/examples/BESSY2_example/BESSY2Orbit.yaml deleted file mode 100644 index 2d1abe962..000000000 --- a/examples/BESSY2_example/BESSY2Orbit.yaml +++ /dev/null @@ -1,3349 +0,0 @@ -type: pyaml.accelerator -machine: sr -facility: BESSY2 -energy: 1.7185e9 -simulators: - - type: pyaml.lattice.simulator - lattice: bessy2_standard_user.mat - name: design -controls: - - type: pyaml_cs_oa.controlsystem - prefix: "pons:" - name: live -data_folder: /data/store -arrays: - - type: pyaml.arrays.magnet - name: HCorr - elements: - - HS4M2D1R - - HS1MT1R - - HS4M1T1R - - HS4M2T1R - - HS1MD2R - - HS4M1D2R - - HS4M2D2R - - HS1MT2R - - HS4M1T2R - - HS4M2T2R - - HS1MD3R - - HS4M1D3R - - HS4M2D3R - - HS1MT3R - - HS4M1T3R - - HS4M2T3R - - HS1MD4R - - HS4M1D4R - - HS4M2D4R - - HS1MT4R - - HS4M1T4R - - HS4M2T4R - - HS1MD5R - - HS4M1D5R - - HS4M2D5R - - HS1MT5R - - HS4M1T5R - - HS4M2T5R - - HS1MD6R - - HS4M1D6R - - HS4M2D6R - - HS1MT6R - - HS4M1T6R - - HS4M2T6R - - HS1MD7R - - HS4M1D7R - - HS4M2D7R - - HS1MT7R - - HS4M1T7R - - HS4M2T7R - - HS1MD8R - - HS4M1D8R - - HS4M2D8R - - HS1MT8R - - HS4M1T8R - - HS4M2T8R - - HS1MD1R - - HS4M1D1R - - type: pyaml.arrays.magnet - name: VCorr - elements: - - VS3M2D1R - - VS2M2D1R - - VS2M1T1R - - VS3M1T1R - - VS3M2T1R - - VS2M2T1R - - VS2M1D2R - - VS3M1D2R - - VS3M2D2R - - VS2M2D2R - - VS2M1T2R - - VS3M1T2R - - VS3M2T2R - - VS2M2T2R - - VS2M1D3R - - VS3M1D3R - - VS3M2D3R - - VS2M2D3R - - VS2M1T3R - - VS3M1T3R - - VS3M2T3R - - VS2M2T3R - - VS2M1D4R - - VS3M1D4R - - VS3M2D4R - - VS2M2D4R - - VS2M1T4R - - VS3M1T4R - - VS3M2T4R - - VS2M2T4R - - VS2M1D5R - - VS3M1D5R - - VS3M2D5R - - VS2M2D5R - - VS2M1T5R - - VS3M1T5R - - VS3M2T5R - - VS2M2T5R - - VS2M1D6R - - VS3M1D6R - - VS3M2D6R - - VS2M2D6R - - VS2M1T6R - - VS3M1T6R - - VS3M2T6R - - VS2M2T6R - - VS2M1D7R - - VS3M1D7R - - VS3M2D7R - - VS2M2D7R - - VS2M1T7R - - VS3M1T7R - - VS3M2T7R - - VS2M2T7R - - VS2M1D8R - - VS3M1D8R - - VS3M2D8R - - VS2M2D8R - - VS2M1T8R - - VS3M1T8R - - VS3M2T8R - - VS2M2T8R - - VS2M1D1R - - VS3M1D1R - - type: pyaml.arrays.bpm - name: BPM - elements: - - BPMZ5D1R - - BPMZ6D1R - - BPMZ7D1R - - BPMZ1T1R - - BPMZ2T1R - - BPMZ3T1R - - BPMZ4T1R - - BPMZ41T1R - - BPMZ5T1R - - BPMZ6T1R - - BPMZ7T1R - - BPMZ1D2R - - BPMZ2D2R - - BPMZ3D2R - - BPMZ4D2R - - BPMZ5D2R - - BPMZ6D2R - - BPMZ7D2R - - BPMZ1T2R - - BPMZ2T2R - - BPMZ3T2R - - BPMZ4T2R - - BPMZ41T2R - - BPMZ42T2R - - BPMZ43T2R - - BPMZ5T2R - - BPMZ6T2R - - BPMZ7T2R - - BPMZ1D3R - - BPMZ2D3R - - BPMZ3D3R - - BPMZ4D3R - - BPMZ5D3R - - BPMZ6D3R - - BPMZ7D3R - - BPMZ1T3R - - BPMZ2T3R - - BPMZ3T3R - - BPMZ4T3R - - BPMZ5T3R - - BPMZ6T3R - - BPMZ7T3R - - BPMZ1D4R - - BPMZ2D4R - - BPMZ3D4R - - BPMZ4D4R - - BPMZ5D4R - - BPMZ6D4R - - BPMZ7D4R - - BPMZ1T4R - - BPMZ2T4R - - BPMZ3T4R - - BPMZ4T4R - - BPMZ5T4R - - BPMZ6T4R - - BPMZ7T4R - - BPMZ1D5R - - BPMZ2D5R - - BPMZ3D5R - - BPMZ4D5R - - BPMZ5D5R - - BPMZ6D5R - - BPMZ7D5R - - BPMZ1T5R - - BPMZ2T5R - - BPMZ3T5R - - BPMZ4T5R - - BPMZ5T5R - - BPMZ6T5R - - BPMZ7T5R - - BPMZ1D6R - - BPMZ2D6R - - BPMZ3D6R - - BPMZ4D6R - - BPMZ41D6R - - BPMZ42D6R - - BPMZ43D6R - - BPMZ44D6R - - BPMZ6D6R - - BPMZ7D6R - - BPMZ1T6R - - BPMZ2T6R - - BPMZ3T6R - - BPMZ4T6R - - BPMZ41T6R - - BPMZ5T6R - - BPMZ6T6R - - BPMZ7T6R - - BPMZ1D7R - - BPMZ2D7R - - BPMZ3D7R - - BPMZ4D7R - - BPMZ5D7R - - BPMZ6D7R - - BPMZ7D7R - - BPMZ1T7R - - BPMZ2T7R - - BPMZ3T7R - - BPMZ4T7R - - BPMZ41T7R - - BPMZ5T7R - - BPMZ6T7R - - BPMZ7T7R - - BPMZ1D8R - - BPMZ2D8R - - BPMZ3D8R - - BPMZ4D8R - - BPMZ5D8R - - BPMZ6D8R - - BPMZ7D8R - - BPMZ1T8R - - BPMZ2T8R - - BPMZ3T8R - - BPMZ4T8R - - BPMZ5T8R - - BPMZ6T8R - - BPMZ7T8R - - BPMZ1D1R - - BPMZ2D1R - - BPMZ3D1R - - BPMZ4D1R - - BPMZ41D1R - - BPMZ42D1R -devices: -- type: pyaml.tuning_tools.orbit_response_matrix - bpm_array_name: BPM - hcorr_array_name: HCorr - vcorr_array_name: VCorr - corrector_delta: 1e-6 - name: DEFAULT_ORBIT_RESPONSE_MATRIX -- type: pyaml.tuning_tools.dispersion - bpm_array_name: BPM - rf_plant_name: RF - frequency_delta: 10 - name: DEFAULT_DISPERSION -- type: pyaml.tuning_tools.orbit - bpm_array_name: BPM - hcorr_array_name: HCorr - vcorr_array_name: VCorr - name: DEFAULT_ORBIT_CORRECTION - singular_values: 16 - response_matrix: file:orm.json -- type: pyaml.rf.rf_plant - name: RF - masterclock: - type: pyaml_cs_oa.epicsW - write_pvname: MCLKHX251C:freq - unit: KHz -- type: pyaml.magnet.hcorrector - name: HS4M2D1R - lattice_names: S4M2D1R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: -0.0044502 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: HS4P2D1R:rdbk - write_pvname: HS4P2D1R:set - unit: A -- type: pyaml.magnet.hcorrector - name: HS1MT1R - lattice_names: S1MT1R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: -0.00553438 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: HS1PT1R:rdbk - write_pvname: HS1PT1R:set - unit: A -- type: pyaml.magnet.hcorrector - name: HS4M1T1R - lattice_names: S4M1T1R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: -0.0044502 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: HS4P1T1R:rdbk - write_pvname: HS4P1T1R:set - unit: A -- type: pyaml.magnet.hcorrector - name: HS4M2T1R - lattice_names: S4M2T1R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: -0.0044502 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: HS4P2T1R:rdbk - write_pvname: HS4P2T1R:set - unit: A -- type: pyaml.magnet.hcorrector - name: HS1MD2R - lattice_names: S1MD2R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: -0.00553438 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: HS1PD2R:rdbk - write_pvname: HS1PD2R:set - unit: A -- type: pyaml.magnet.hcorrector - name: HS4M1D2R - lattice_names: S4M1D2R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: -0.0044502 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: HS4P1D2R:rdbk - write_pvname: HS4P1D2R:set - unit: A -- type: pyaml.magnet.hcorrector - name: HS4M2D2R - lattice_names: S4M2D2R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: -0.0044502 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: HS4P2D2R:rdbk - write_pvname: HS4P2D2R:set - unit: A -- type: pyaml.magnet.hcorrector - name: HS1MT2R - lattice_names: S1MT2R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: -0.00553438 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: HS1PT2R:rdbk - write_pvname: HS1PT2R:set - unit: A -- type: pyaml.magnet.hcorrector - name: HS4M1T2R - lattice_names: S4M1T2R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: -0.0044502 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: HS4P1T2R:rdbk - write_pvname: HS4P1T2R:set - unit: A -- type: pyaml.magnet.hcorrector - name: HS4M2T2R - lattice_names: S4M2T2R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: -0.0044502 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: HS4P2T2R:rdbk - write_pvname: HS4P2T2R:set - unit: A -- type: pyaml.magnet.hcorrector - name: HS1MD3R - lattice_names: S1MD3R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: -0.00553438 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: HS1PD3R:rdbk - write_pvname: HS1PD3R:set - unit: A -- type: pyaml.magnet.hcorrector - name: HS4M1D3R - lattice_names: S4M1D3R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: -0.0044502 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: HS4P1D3R:rdbk - write_pvname: HS4P1D3R:set - unit: A -- type: pyaml.magnet.hcorrector - name: HS4M2D3R - lattice_names: S4M2D3R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: -0.0044502 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: HS4P2D3R:rdbk - write_pvname: HS4P2D3R:set - unit: A -- type: pyaml.magnet.hcorrector - name: HS1MT3R - lattice_names: S1MT3R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: -0.00553438 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: HS1PT3R:rdbk - write_pvname: HS1PT3R:set - unit: A -- type: pyaml.magnet.hcorrector - name: HS4M1T3R - lattice_names: S4M1T3R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: -0.0044502 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: HS4P1T3R:rdbk - write_pvname: HS4P1T3R:set - unit: A -- type: pyaml.magnet.hcorrector - name: HS4M2T3R - lattice_names: S4M2T3R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: -0.0044502 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: HS4P2T3R:rdbk - write_pvname: HS4P2T3R:set - unit: A -- type: pyaml.magnet.hcorrector - name: HS1MD4R - lattice_names: S1MD4R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: -0.00553438 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: HS1PD4R:rdbk - write_pvname: HS1PD4R:set - unit: A -- type: pyaml.magnet.hcorrector - name: HS4M1D4R - lattice_names: S4M1D4R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: -0.0044502 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: HS4P1D4R:rdbk - write_pvname: HS4P1D4R:set - unit: A -- type: pyaml.magnet.hcorrector - name: HS4M2D4R - lattice_names: S4M2D4R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: -0.0044502 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: HS4P2D4R:rdbk - write_pvname: HS4P2D4R:set - unit: A -- type: pyaml.magnet.hcorrector - name: HS1MT4R - lattice_names: S1MT4R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: -0.00553438 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: HS1PT4R:rdbk - write_pvname: HS1PT4R:set - unit: A -- type: pyaml.magnet.hcorrector - name: HS4M1T4R - lattice_names: S4M1T4R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: -0.0044502 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: HS4P1T4R:rdbk - write_pvname: HS4P1T4R:set - unit: A -- type: pyaml.magnet.hcorrector - name: HS4M2T4R - lattice_names: S4M2T4R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: -0.0044502 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: HS4P2T4R:rdbk - write_pvname: HS4P2T4R:set - unit: A -- type: pyaml.magnet.hcorrector - name: HS1MD5R - lattice_names: S1MD5R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: -0.00553438 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: HS1PD5R:rdbk - write_pvname: HS1PD5R:set - unit: A -- type: pyaml.magnet.hcorrector - name: HS4M1D5R - lattice_names: S4M1D5R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: -0.0044502 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: HS4P1D5R:rdbk - write_pvname: HS4P1D5R:set - unit: A -- type: pyaml.magnet.hcorrector - name: HS4M2D5R - lattice_names: S4M2D5R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: -0.0044502 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: HS4P2D5R:rdbk - write_pvname: HS4P2D5R:set - unit: A -- type: pyaml.magnet.hcorrector - name: HS1MT5R - lattice_names: S1MT5R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: -0.00553438 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: HS1PT5R:rdbk - write_pvname: HS1PT5R:set - unit: A -- type: pyaml.magnet.hcorrector - name: HS4M1T5R - lattice_names: S4M1T5R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: -0.0044502 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: HS4P1T5R:rdbk - write_pvname: HS4P1T5R:set - unit: A -- type: pyaml.magnet.hcorrector - name: HS4M2T5R - lattice_names: S4M2T5R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: -0.0044502 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: HS4P2T5R:rdbk - write_pvname: HS4P2T5R:set - unit: A -- type: pyaml.magnet.hcorrector - name: HS1MD6R - lattice_names: S1MD6R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: -0.00553438 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: HS1PD6R:rdbk - write_pvname: HS1PD6R:set - unit: A -- type: pyaml.magnet.hcorrector - name: HS4M1D6R - lattice_names: S4M1D6R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: -0.0044502 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: HS4P1D6R:rdbk - write_pvname: HS4P1D6R:set - unit: A -- type: pyaml.magnet.hcorrector - name: HS4M2D6R - lattice_names: S4M2D6R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: -0.0044502 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: HS4P2D6R:rdbk - write_pvname: HS4P2D6R:set - unit: A -- type: pyaml.magnet.hcorrector - name: HS1MT6R - lattice_names: S1MT6R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: -0.00553438 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: HS1PT6R:rdbk - write_pvname: HS1PT6R:set - unit: A -- type: pyaml.magnet.hcorrector - name: HS4M1T6R - lattice_names: S4M1T6R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: -0.0044502 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: HS4P1T6R:rdbk - write_pvname: HS4P1T6R:set - unit: A -- type: pyaml.magnet.hcorrector - name: HS4M2T6R - lattice_names: S4M2T6R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: -0.0044502 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: HS4P2T6R:rdbk - write_pvname: HS4P2T6R:set - unit: A -- type: pyaml.magnet.hcorrector - name: HS1MD7R - lattice_names: S1MD7R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: -0.00553438 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: HS1PD7R:rdbk - write_pvname: HS1PD7R:set - unit: A -- type: pyaml.magnet.hcorrector - name: HS4M1D7R - lattice_names: S4M1D7R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: -0.0044502 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: HS4P1D7R:rdbk - write_pvname: HS4P1D7R:set - unit: A -- type: pyaml.magnet.hcorrector - name: HS4M2D7R - lattice_names: S4M2D7R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: -0.0044502 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: HS4P2D7R:rdbk - write_pvname: HS4P2D7R:set - unit: A -- type: pyaml.magnet.hcorrector - name: HS1MT7R - lattice_names: S1MT7R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: -0.00553438 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: HS1PT7R:rdbk - write_pvname: HS1PT7R:set - unit: A -- type: pyaml.magnet.hcorrector - name: HS4M1T7R - lattice_names: S4M1T7R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: -0.0044502 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: HS4P1T7R:rdbk - write_pvname: HS4P1T7R:set - unit: A -- type: pyaml.magnet.hcorrector - name: HS4M2T7R - lattice_names: S4M2T7R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: -0.0044502 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: HS4P2T7R:rdbk - write_pvname: HS4P2T7R:set - unit: A -- type: pyaml.magnet.hcorrector - name: HS1MD8R - lattice_names: S1MD8R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: -0.00553438 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: HS1PD8R:rdbk - write_pvname: HS1PD8R:set - unit: A -- type: pyaml.magnet.hcorrector - name: HS4M1D8R - lattice_names: S4M1D8R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: -0.0044502 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: HS4P1D8R:rdbk - write_pvname: HS4P1D8R:set - unit: A -- type: pyaml.magnet.hcorrector - name: HS4M2D8R - lattice_names: S4M2D8R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: -0.0044502 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: HS4P2D8R:rdbk - write_pvname: HS4P2D8R:set - unit: A -- type: pyaml.magnet.hcorrector - name: HS1MT8R - lattice_names: S1MT8R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: -0.00553438 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: HS1PT8R:rdbk - write_pvname: HS1PT8R:set - unit: A -- type: pyaml.magnet.hcorrector - name: HS4M1T8R - lattice_names: S4M1T8R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: -0.0044502 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: HS4P1T8R:rdbk - write_pvname: HS4P1T8R:set - unit: A -- type: pyaml.magnet.hcorrector - name: HS4M2T8R - lattice_names: S4M2T8R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: -0.0044502 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: HS4P2T8R:rdbk - write_pvname: HS4P2T8R:set - unit: A -- type: pyaml.magnet.hcorrector - name: HS1MD1R - lattice_names: S1MD1R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: -0.00553438 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: HS1PD1R:rdbk - write_pvname: HS1PD1R:set - unit: A -- type: pyaml.magnet.hcorrector - name: HS4M1D1R - lattice_names: S4M1D1R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: -0.0044502 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: HS4P1D1R:rdbk - write_pvname: HS4P1D1R:set - unit: A -- type: pyaml.magnet.vcorrector - name: VS3M2D1R - lattice_names: S3M2D1R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.00297607 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: VS3P2D1R:rdbk - write_pvname: VS3P2D1R:set - unit: A -- type: pyaml.magnet.vcorrector - name: VS2M2D1R - lattice_names: S2M2D1R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.00297607 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: VS2P2D1R:rdbk - write_pvname: VS2P2D1R:set - unit: A -- type: pyaml.magnet.vcorrector - name: VS2M1T1R - lattice_names: S2M1T1R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.00297607 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: VS2P1T1R:rdbk - write_pvname: VS2P1T1R:set - unit: A -- type: pyaml.magnet.vcorrector - name: VS3M1T1R - lattice_names: S3M1T1R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.00297607 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: VS3P1T1R:rdbk - write_pvname: VS3P1T1R:set - unit: A -- type: pyaml.magnet.vcorrector - name: VS3M2T1R - lattice_names: S3M2T1R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.00297607 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: VS3P2T1R:rdbk - write_pvname: VS3P2T1R:set - unit: A -- type: pyaml.magnet.vcorrector - name: VS2M2T1R - lattice_names: S2M2T1R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.00297607 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: VS2P2T1R:rdbk - write_pvname: VS2P2T1R:set - unit: A -- type: pyaml.magnet.vcorrector - name: VS2M1D2R - lattice_names: S2M1D2R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.00297607 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: VS2P1D2R:rdbk - write_pvname: VS2P1D2R:set - unit: A -- type: pyaml.magnet.vcorrector - name: VS3M1D2R - lattice_names: S3M1D2R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.00297607 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: VS3P1D2R:rdbk - write_pvname: VS3P1D2R:set - unit: A -- type: pyaml.magnet.vcorrector - name: VS3M2D2R - lattice_names: S3M2D2R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.00297607 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: VS3P2D2R:rdbk - write_pvname: VS3P2D2R:set - unit: A -- type: pyaml.magnet.vcorrector - name: VS2M2D2R - lattice_names: S2M2D2R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.00297607 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: VS2P2D2R:rdbk - write_pvname: VS2P2D2R:set - unit: A -- type: pyaml.magnet.vcorrector - name: VS2M1T2R - lattice_names: S2M1T2R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.00297607 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: VS2P1T2R:rdbk - write_pvname: VS2P1T2R:set - unit: A -- type: pyaml.magnet.vcorrector - name: VS3M1T2R - lattice_names: S3M1T2R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.00297607 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: VS3P1T2R:rdbk - write_pvname: VS3P1T2R:set - unit: A -- type: pyaml.magnet.vcorrector - name: VS3M2T2R - lattice_names: S3M2T2R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.00297607 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: VS3P2T2R:rdbk - write_pvname: VS3P2T2R:set - unit: A -- type: pyaml.magnet.vcorrector - name: VS2M2T2R - lattice_names: S2M2T2R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.00297607 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: VS2P2T2R:rdbk - write_pvname: VS2P2T2R:set - unit: A -- type: pyaml.magnet.vcorrector - name: VS2M1D3R - lattice_names: S2M1D3R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.00297607 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: VS2P1D3R:rdbk - write_pvname: VS2P1D3R:set - unit: A -- type: pyaml.magnet.vcorrector - name: VS3M1D3R - lattice_names: S3M1D3R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.00297607 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: VS3P1D3R:rdbk - write_pvname: VS3P1D3R:set - unit: A -- type: pyaml.magnet.vcorrector - name: VS3M2D3R - lattice_names: S3M2D3R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.00297607 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: VS3P2D3R:rdbk - write_pvname: VS3P2D3R:set - unit: A -- type: pyaml.magnet.vcorrector - name: VS2M2D3R - lattice_names: S2M2D3R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.00297607 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: VS2P2D3R:rdbk - write_pvname: VS2P2D3R:set - unit: A -- type: pyaml.magnet.vcorrector - name: VS2M1T3R - lattice_names: S2M1T3R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.00297607 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: VS2P1T3R:rdbk - write_pvname: VS2P1T3R:set - unit: A -- type: pyaml.magnet.vcorrector - name: VS3M1T3R - lattice_names: S3M1T3R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.00297607 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: VS3P1T3R:rdbk - write_pvname: VS3P1T3R:set - unit: A -- type: pyaml.magnet.vcorrector - name: VS3M2T3R - lattice_names: S3M2T3R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.00297607 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: VS3P2T3R:rdbk - write_pvname: VS3P2T3R:set - unit: A -- type: pyaml.magnet.vcorrector - name: VS2M2T3R - lattice_names: S2M2T3R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.00297607 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: VS2P2T3R:rdbk - write_pvname: VS2P2T3R:set - unit: A -- type: pyaml.magnet.vcorrector - name: VS2M1D4R - lattice_names: S2M1D4R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.00297607 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: VS2P1D4R:rdbk - write_pvname: VS2P1D4R:set - unit: A -- type: pyaml.magnet.vcorrector - name: VS3M1D4R - lattice_names: S3M1D4R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.00297607 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: VS3P1D4R:rdbk - write_pvname: VS3P1D4R:set - unit: A -- type: pyaml.magnet.vcorrector - name: VS3M2D4R - lattice_names: S3M2D4R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.00297607 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: VS3P2D4R:rdbk - write_pvname: VS3P2D4R:set - unit: A -- type: pyaml.magnet.vcorrector - name: VS2M2D4R - lattice_names: S2M2D4R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.00297607 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: VS2P2D4R:rdbk - write_pvname: VS2P2D4R:set - unit: A -- type: pyaml.magnet.vcorrector - name: VS2M1T4R - lattice_names: S2M1T4R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.00297607 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: VS2P1T4R:rdbk - write_pvname: VS2P1T4R:set - unit: A -- type: pyaml.magnet.vcorrector - name: VS3M1T4R - lattice_names: S3M1T4R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.00297607 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: VS3P1T4R:rdbk - write_pvname: VS3P1T4R:set - unit: A -- type: pyaml.magnet.vcorrector - name: VS3M2T4R - lattice_names: S3M2T4R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.00297607 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: VS3P2T4R:rdbk - write_pvname: VS3P2T4R:set - unit: A -- type: pyaml.magnet.vcorrector - name: VS2M2T4R - lattice_names: S2M2T4R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.00297607 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: VS2P2T4R:rdbk - write_pvname: VS2P2T4R:set - unit: A -- type: pyaml.magnet.vcorrector - name: VS2M1D5R - lattice_names: S2M1D5R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.00297607 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: VS2P1D5R:rdbk - write_pvname: VS2P1D5R:set - unit: A -- type: pyaml.magnet.vcorrector - name: VS3M1D5R - lattice_names: S3M1D5R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.00297607 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: VS3P1D5R:rdbk - write_pvname: VS3P1D5R:set - unit: A -- type: pyaml.magnet.vcorrector - name: VS3M2D5R - lattice_names: S3M2D5R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.00297607 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: VS3P2D5R:rdbk - write_pvname: VS3P2D5R:set - unit: A -- type: pyaml.magnet.vcorrector - name: VS2M2D5R - lattice_names: S2M2D5R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.00297607 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: VS2P2D5R:rdbk - write_pvname: VS2P2D5R:set - unit: A -- type: pyaml.magnet.vcorrector - name: VS2M1T5R - lattice_names: S2M1T5R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.00297607 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: VS2P1T5R:rdbk - write_pvname: VS2P1T5R:set - unit: A -- type: pyaml.magnet.vcorrector - name: VS3M1T5R - lattice_names: S3M1T5R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.00297607 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: VS3P1T5R:rdbk - write_pvname: VS3P1T5R:set - unit: A -- type: pyaml.magnet.vcorrector - name: VS3M2T5R - lattice_names: S3M2T5R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.00297607 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: VS3P2T5R:rdbk - write_pvname: VS3P2T5R:set - unit: A -- type: pyaml.magnet.vcorrector - name: VS2M2T5R - lattice_names: S2M2T5R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.00297607 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: VS2P2T5R:rdbk - write_pvname: VS2P2T5R:set - unit: A -- type: pyaml.magnet.vcorrector - name: VS2M1D6R - lattice_names: S2M1D6R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.00297607 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: VS2P1D6R:rdbk - write_pvname: VS2P1D6R:set - unit: A -- type: pyaml.magnet.vcorrector - name: VS3M1D6R - lattice_names: S3M1D6R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.00297607 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: VS3P1D6R:rdbk - write_pvname: VS3P1D6R:set - unit: A -- type: pyaml.magnet.vcorrector - name: VS3M2D6R - lattice_names: S3M2D6R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.00297607 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: VS3P2D6R:rdbk - write_pvname: VS3P2D6R:set - unit: A -- type: pyaml.magnet.vcorrector - name: VS2M2D6R - lattice_names: S2M2D6R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.00297607 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: VS2P2D6R:rdbk - write_pvname: VS2P2D6R:set - unit: A -- type: pyaml.magnet.vcorrector - name: VS2M1T6R - lattice_names: S2M1T6R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.00297607 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: VS2P1T6R:rdbk - write_pvname: VS2P1T6R:set - unit: A -- type: pyaml.magnet.vcorrector - name: VS3M1T6R - lattice_names: S3M1T6R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.00297607 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: VS3P1T6R:rdbk - write_pvname: VS3P1T6R:set - unit: A -- type: pyaml.magnet.vcorrector - name: VS3M2T6R - lattice_names: S3M2T6R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.00297607 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: VS3P2T6R:rdbk - write_pvname: VS3P2T6R:set - unit: A -- type: pyaml.magnet.vcorrector - name: VS2M2T6R - lattice_names: S2M2T6R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.00297607 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: VS2P2T6R:rdbk - write_pvname: VS2P2T6R:set - unit: A -- type: pyaml.magnet.vcorrector - name: VS2M1D7R - lattice_names: S2M1D7R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.00297607 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: VS2P1D7R:rdbk - write_pvname: VS2P1D7R:set - unit: A -- type: pyaml.magnet.vcorrector - name: VS3M1D7R - lattice_names: S3M1D7R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.00297607 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: VS3P1D7R:rdbk - write_pvname: VS3P1D7R:set - unit: A -- type: pyaml.magnet.vcorrector - name: VS3M2D7R - lattice_names: S3M2D7R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.00297607 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: VS3P2D7R:rdbk - write_pvname: VS3P2D7R:set - unit: A -- type: pyaml.magnet.vcorrector - name: VS2M2D7R - lattice_names: S2M2D7R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.00297607 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: VS2P2D7R:rdbk - write_pvname: VS2P2D7R:set - unit: A -- type: pyaml.magnet.vcorrector - name: VS2M1T7R - lattice_names: S2M1T7R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.00297607 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: VS2P1T7R:rdbk - write_pvname: VS2P1T7R:set - unit: A -- type: pyaml.magnet.vcorrector - name: VS3M1T7R - lattice_names: S3M1T7R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.00297607 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: VS3P1T7R:rdbk - write_pvname: VS3P1T7R:set - unit: A -- type: pyaml.magnet.vcorrector - name: VS3M2T7R - lattice_names: S3M2T7R@0 - model: - type: pyaml.magnet.linear_model - 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powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: VS3P1T8R:rdbk - write_pvname: VS3P1T8R:set - unit: A -- type: pyaml.magnet.vcorrector - name: VS3M2T8R - lattice_names: S3M2T8R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.00297607 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: VS3P2T8R:rdbk - write_pvname: VS3P2T8R:set - unit: A -- type: pyaml.magnet.vcorrector - name: VS2M2T8R - lattice_names: S2M2T8R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.00297607 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: VS2P2T8R:rdbk - write_pvname: VS2P2T8R:set - unit: A -- type: pyaml.magnet.vcorrector - name: VS2M1D1R - lattice_names: S2M1D1R@0 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.00297607 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - read_pvname: VS2P1D1R:rdbk - write_pvname: VS2P1D1R:set - unit: A -- type: pyaml.magnet.vcorrector - name: VS3M1D1R - 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model: - type: pyaml.bpm.bpm_simple_model - x_pos_index: 188 - y_pos_index: 189 - x_pos: - type: pyaml_cs_oa.epicsR - read_pvname: ORBITCC:rdPos - unit: nm - y_pos: - type: pyaml_cs_oa.epicsR - read_pvname: ORBITCC:rdPos - unit: nm -- type: pyaml.bpm.bpm - name: BPMZ1T7R - model: - type: pyaml.bpm.bpm_simple_model - x_pos_index: 190 - y_pos_index: 191 - x_pos: - type: pyaml_cs_oa.epicsR - read_pvname: ORBITCC:rdPos - unit: nm - y_pos: - type: pyaml_cs_oa.epicsR - read_pvname: ORBITCC:rdPos - unit: nm -- type: pyaml.bpm.bpm - name: BPMZ2T7R - model: - type: pyaml.bpm.bpm_simple_model - x_pos_index: 192 - y_pos_index: 193 - x_pos: - type: pyaml_cs_oa.epicsR - read_pvname: ORBITCC:rdPos - unit: nm - y_pos: - type: pyaml_cs_oa.epicsR - read_pvname: ORBITCC:rdPos - unit: nm -- type: pyaml.bpm.bpm - name: BPMZ3T7R - model: - type: pyaml.bpm.bpm_simple_model - x_pos_index: 194 - y_pos_index: 195 - x_pos: - type: pyaml_cs_oa.epicsR - read_pvname: ORBITCC:rdPos - unit: nm - y_pos: - type: pyaml_cs_oa.epicsR - read_pvname: ORBITCC:rdPos - unit: nm -- type: pyaml.bpm.bpm - name: BPMZ4T7R - model: - type: pyaml.bpm.bpm_simple_model - x_pos_index: 196 - y_pos_index: 197 - x_pos: - type: pyaml_cs_oa.epicsR - read_pvname: ORBITCC:rdPos - unit: nm - y_pos: - type: pyaml_cs_oa.epicsR - read_pvname: ORBITCC:rdPos - unit: nm -- type: pyaml.bpm.bpm - name: BPMZ41T7R - model: - type: pyaml.bpm.bpm_simple_model - x_pos_index: 198 - y_pos_index: 199 - x_pos: - type: pyaml_cs_oa.epicsR - read_pvname: ORBITCC:rdPos - unit: nm - y_pos: - type: pyaml_cs_oa.epicsR - read_pvname: ORBITCC:rdPos - unit: nm -- type: pyaml.bpm.bpm - name: BPMZ5T7R - model: - type: pyaml.bpm.bpm_simple_model - x_pos_index: 200 - y_pos_index: 201 - x_pos: - type: pyaml_cs_oa.epicsR - read_pvname: ORBITCC:rdPos - unit: nm - y_pos: - type: pyaml_cs_oa.epicsR - read_pvname: ORBITCC:rdPos - unit: nm -- type: pyaml.bpm.bpm - name: BPMZ6T7R - model: - type: pyaml.bpm.bpm_simple_model - x_pos_index: 202 - y_pos_index: 203 - x_pos: - type: pyaml_cs_oa.epicsR - read_pvname: ORBITCC:rdPos - unit: nm - y_pos: - type: pyaml_cs_oa.epicsR - read_pvname: ORBITCC:rdPos - unit: nm -- type: pyaml.bpm.bpm - name: BPMZ7T7R - model: - type: pyaml.bpm.bpm_simple_model - x_pos_index: 204 - y_pos_index: 205 - x_pos: - type: pyaml_cs_oa.epicsR - read_pvname: ORBITCC:rdPos - unit: nm - y_pos: - type: pyaml_cs_oa.epicsR - read_pvname: ORBITCC:rdPos - unit: nm -- type: pyaml.bpm.bpm - name: BPMZ1D8R - model: - type: pyaml.bpm.bpm_simple_model - x_pos_index: 206 - y_pos_index: 207 - x_pos: - type: pyaml_cs_oa.epicsR - read_pvname: ORBITCC:rdPos - unit: nm - y_pos: - type: pyaml_cs_oa.epicsR - read_pvname: ORBITCC:rdPos - unit: nm -- type: pyaml.bpm.bpm - name: BPMZ2D8R - model: - type: pyaml.bpm.bpm_simple_model - x_pos_index: 208 - y_pos_index: 209 - x_pos: - type: pyaml_cs_oa.epicsR - read_pvname: ORBITCC:rdPos - unit: nm - y_pos: - type: pyaml_cs_oa.epicsR - read_pvname: ORBITCC:rdPos - unit: nm -- type: pyaml.bpm.bpm - name: BPMZ3D8R - model: - type: pyaml.bpm.bpm_simple_model - x_pos_index: 210 - y_pos_index: 211 - x_pos: - type: pyaml_cs_oa.epicsR - read_pvname: ORBITCC:rdPos - unit: nm - y_pos: - type: pyaml_cs_oa.epicsR - read_pvname: ORBITCC:rdPos - unit: nm -- type: pyaml.bpm.bpm - name: BPMZ4D8R - model: - type: pyaml.bpm.bpm_simple_model - x_pos_index: 212 - y_pos_index: 213 - x_pos: - type: pyaml_cs_oa.epicsR - read_pvname: ORBITCC:rdPos - unit: nm - y_pos: - type: pyaml_cs_oa.epicsR - read_pvname: ORBITCC:rdPos - unit: nm -- type: pyaml.bpm.bpm - name: BPMZ5D8R - model: - type: pyaml.bpm.bpm_simple_model - x_pos_index: 214 - y_pos_index: 215 - x_pos: - type: pyaml_cs_oa.epicsR - read_pvname: ORBITCC:rdPos - unit: nm - y_pos: - type: pyaml_cs_oa.epicsR - read_pvname: ORBITCC:rdPos - unit: nm -- type: pyaml.bpm.bpm - name: BPMZ6D8R - model: - type: pyaml.bpm.bpm_simple_model - x_pos_index: 216 - y_pos_index: 217 - x_pos: - type: pyaml_cs_oa.epicsR - read_pvname: ORBITCC:rdPos - unit: nm - y_pos: - type: pyaml_cs_oa.epicsR - read_pvname: ORBITCC:rdPos - unit: nm -- type: pyaml.bpm.bpm - name: BPMZ7D8R - model: - type: pyaml.bpm.bpm_simple_model - x_pos_index: 218 - y_pos_index: 219 - x_pos: - type: pyaml_cs_oa.epicsR - read_pvname: ORBITCC:rdPos - unit: nm - y_pos: - type: pyaml_cs_oa.epicsR - read_pvname: ORBITCC:rdPos - unit: nm -- type: pyaml.bpm.bpm - name: BPMZ1T8R - model: - type: pyaml.bpm.bpm_simple_model - x_pos_index: 220 - y_pos_index: 221 - x_pos: - type: pyaml_cs_oa.epicsR - read_pvname: ORBITCC:rdPos - unit: nm - y_pos: - type: pyaml_cs_oa.epicsR - read_pvname: ORBITCC:rdPos - unit: nm -- type: pyaml.bpm.bpm - name: BPMZ2T8R - model: - type: pyaml.bpm.bpm_simple_model - x_pos_index: 222 - y_pos_index: 223 - x_pos: - type: pyaml_cs_oa.epicsR - read_pvname: ORBITCC:rdPos - unit: nm - y_pos: - type: pyaml_cs_oa.epicsR - read_pvname: ORBITCC:rdPos - unit: nm -- type: pyaml.bpm.bpm - name: BPMZ3T8R - model: - type: pyaml.bpm.bpm_simple_model - x_pos_index: 224 - y_pos_index: 225 - x_pos: - type: pyaml_cs_oa.epicsR - read_pvname: ORBITCC:rdPos - unit: nm - y_pos: - type: pyaml_cs_oa.epicsR - read_pvname: ORBITCC:rdPos - unit: nm -- type: pyaml.bpm.bpm - name: BPMZ4T8R - model: - type: pyaml.bpm.bpm_simple_model - x_pos_index: 226 - y_pos_index: 227 - x_pos: - type: pyaml_cs_oa.epicsR - read_pvname: ORBITCC:rdPos - unit: nm - y_pos: - type: pyaml_cs_oa.epicsR - read_pvname: ORBITCC:rdPos - unit: nm -- type: pyaml.bpm.bpm - name: BPMZ5T8R - model: - type: pyaml.bpm.bpm_simple_model - x_pos_index: 228 - y_pos_index: 229 - x_pos: - type: pyaml_cs_oa.epicsR - read_pvname: ORBITCC:rdPos - unit: nm - y_pos: - type: pyaml_cs_oa.epicsR - read_pvname: ORBITCC:rdPos - unit: nm -- type: pyaml.bpm.bpm - name: BPMZ6T8R - model: - type: pyaml.bpm.bpm_simple_model - x_pos_index: 230 - y_pos_index: 231 - x_pos: - type: pyaml_cs_oa.epicsR - read_pvname: ORBITCC:rdPos - unit: nm - y_pos: - type: pyaml_cs_oa.epicsR - read_pvname: ORBITCC:rdPos - unit: nm -- type: pyaml.bpm.bpm - name: BPMZ7T8R - model: - type: pyaml.bpm.bpm_simple_model - x_pos_index: 232 - y_pos_index: 233 - x_pos: - type: pyaml_cs_oa.epicsR - read_pvname: ORBITCC:rdPos - unit: nm - y_pos: - type: pyaml_cs_oa.epicsR - read_pvname: ORBITCC:rdPos - unit: nm -- type: pyaml.bpm.bpm - name: BPMZ1D1R - model: - type: pyaml.bpm.bpm_simple_model - x_pos_index: 234 - y_pos_index: 235 - x_pos: - type: pyaml_cs_oa.epicsR - read_pvname: ORBITCC:rdPos - unit: nm - y_pos: - type: pyaml_cs_oa.epicsR - read_pvname: ORBITCC:rdPos - unit: nm -- type: pyaml.bpm.bpm - name: BPMZ2D1R - model: - type: pyaml.bpm.bpm_simple_model - x_pos_index: 236 - y_pos_index: 237 - x_pos: - type: pyaml_cs_oa.epicsR - read_pvname: ORBITCC:rdPos - unit: nm - y_pos: - type: pyaml_cs_oa.epicsR - read_pvname: ORBITCC:rdPos - unit: nm -- type: pyaml.bpm.bpm - name: BPMZ3D1R - model: - type: pyaml.bpm.bpm_simple_model - x_pos_index: 238 - y_pos_index: 239 - x_pos: - type: pyaml_cs_oa.epicsR - read_pvname: ORBITCC:rdPos - unit: nm - y_pos: - type: pyaml_cs_oa.epicsR - read_pvname: ORBITCC:rdPos - unit: nm -- type: pyaml.bpm.bpm - name: BPMZ4D1R - model: - type: pyaml.bpm.bpm_simple_model - x_pos_index: 240 - y_pos_index: 241 - x_pos: - type: pyaml_cs_oa.epicsR - read_pvname: ORBITCC:rdPos - unit: nm - y_pos: - type: pyaml_cs_oa.epicsR - read_pvname: ORBITCC:rdPos - unit: nm -- type: pyaml.bpm.bpm - name: BPMZ41D1R - model: - type: pyaml.bpm.bpm_simple_model - x_pos_index: 242 - y_pos_index: 243 - x_pos: - type: pyaml_cs_oa.epicsR - read_pvname: ORBITCC:rdPos - unit: nm - y_pos: - type: pyaml_cs_oa.epicsR - read_pvname: ORBITCC:rdPos - unit: nm -- type: pyaml.bpm.bpm - name: BPMZ42D1R - model: - type: pyaml.bpm.bpm_simple_model - x_pos_index: 244 - y_pos_index: 245 - x_pos: - type: pyaml_cs_oa.epicsR - read_pvname: ORBITCC:rdPos - unit: nm - y_pos: - type: pyaml_cs_oa.epicsR - read_pvname: ORBITCC:rdPos - unit: nm diff --git a/examples/BESSY2_example/BESSY2Tune.yaml b/examples/BESSY2_example/BESSY2Tune.yaml deleted file mode 100644 index 3dc795d8c..000000000 --- a/examples/BESSY2_example/BESSY2Tune.yaml +++ /dev/null @@ -1,902 +0,0 @@ -type: pyaml.accelerator -facility: BESSY2 -machine: sr -energy: 1.7e9 -simulators: -- type: pyaml.lattice.simulator - lattice: bessy2_standard_user.mat - name: design -controls: -- type: pyaml_cs_oa.controlsystem - prefix: 'pons:' - name: live -data_folder: /data/store -arrays: -- type: pyaml.arrays.magnet - name: QForTune - elements: - - Q3M2D1R - - Q3M1T1R - - Q3M2T1R - - Q3M1D2R - - Q3M2D2R - - Q3M1T2R - - Q3M2T2R - - Q3M1D3R - - Q3M2D3R - - Q3M1T3R - - Q3M2T3R - - Q3M1D4R - - Q3M2D4R - - Q3M1T4R - - Q3M2T4R - - Q3M1D5R - - Q3M2D5R - - Q3M1T5R - - Q3M2T5R - - Q3M1D6R - - Q3M2D6R - - Q3M1T6R - - Q3M2T6R - - Q3M1D7R - - Q3M2D7R - - Q3M1T7R - - Q3M2T7R - - Q3M1D8R - - Q3M2D8R - - Q3M1T8R - - Q3M2T8R - - Q3M1D1R - - Q4M2D1R - - Q4M1T1R - - Q4M2T1R - - Q4M1D2R - - Q4M2D2R - - Q4M1T2R - - Q4M2T2R - - Q4M1D3R - - Q4M2D3R - - Q4M1T3R - - Q4M2T3R - - Q4M1D4R - - Q4M2D4R - - Q4M1T4R - - Q4M2T4R - - Q4M1D5R - - Q4M2D5R - - Q4M1T5R - - Q4M2T5R - - Q4M1D6R - - Q4M2D6R - - Q4M1T6R - - Q4M2T6R - - Q4M1D7R - - Q4M2D7R - - Q4M1T7R - - Q4M2T7R - - Q4M1D8R - - Q4M2D8R - - Q4M1T8R - - Q4M2T8R - - Q4M1D1R -devices: -# Q3 D1 -- type: pyaml.magnet.quadrupole - name: Q3M1D1R - lattice_names: Q3M1D1R - model: - type: pyaml.magnet.linear_model - calibration_factor: -0.0158575 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - write_pvname: Q3PD1R:set - read_pvname: Q3PD1R:rdbk - unit: A -- type: pyaml.magnet.quadrupole - name: Q3M2D1R - lattice_names: Q3M2D1R - model: - type: pyaml.magnet.linear_model - calibration_factor: -0.0158575 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - write_pvname: Q3PD1R:set - read_pvname: Q3PD1R:rdbk - unit: A -# Q3 T1 -- type: pyaml.magnet.quadrupole - name: Q3M1T1R - lattice_names: Q3M1T1R - model: - type: pyaml.magnet.linear_model - calibration_factor: -0.015735 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - write_pvname: Q3P1T1R:set - read_pvname: Q3P1T1R:rdbk - unit: A -- type: pyaml.magnet.quadrupole - name: Q3M2T1R - lattice_names: Q3M2T1R - model: - type: pyaml.magnet.linear_model - calibration_factor: -0.015735 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - write_pvname: Q3P2T1R:set - read_pvname: Q3P2T1R:rdbk - unit: A -# Q3 D2 -- type: pyaml.magnet.quadrupole - name: Q3M1D2R - lattice_names: Q3M1D2R - model: - type: pyaml.magnet.linear_model - calibration_factor: -0.0158575 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - write_pvname: Q3PD2R:set - read_pvname: Q3PD2R:rdbk - unit: A -- type: pyaml.magnet.quadrupole - name: Q3M2D2R - lattice_names: Q3M2D2R - model: - type: pyaml.magnet.linear_model - calibration_factor: -0.0158575 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - write_pvname: Q3PD2R:set - read_pvname: Q3PD2R:rdbk - unit: A -# Q3 T2 -- type: pyaml.magnet.quadrupole - name: Q3M1T2R - lattice_names: Q3M1T2R - model: - type: pyaml.magnet.linear_model - calibration_factor: -0.015735 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - write_pvname: Q3PT2R:set - read_pvname: Q3PT2R:rdbk - unit: A -- type: pyaml.magnet.quadrupole - name: Q3M2T2R - lattice_names: Q3M2T2R - model: - type: pyaml.magnet.linear_model - calibration_factor: -0.015735 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - write_pvname: Q3PT2R:set - read_pvname: Q3PT2R:rdbk - unit: A -# Q3 D3 -- type: pyaml.magnet.quadrupole - name: Q3M1D3R - lattice_names: Q3M1D3R - model: - type: pyaml.magnet.linear_model - calibration_factor: -0.0158575 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - write_pvname: Q3PD3R:set - read_pvname: Q3PD3R:rdbk - unit: A -- type: pyaml.magnet.quadrupole - name: Q3M2D3R - lattice_names: Q3M2D3R - model: - type: pyaml.magnet.linear_model - calibration_factor: -0.0158575 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - write_pvname: Q3PD3R:set - read_pvname: Q3PD3R:rdbk - unit: A -# Q3 T3 -- type: pyaml.magnet.quadrupole - name: Q3M1T3R - lattice_names: Q3M1T3R - model: - type: pyaml.magnet.linear_model - calibration_factor: -0.015735 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - write_pvname: Q3PT3R:set - read_pvname: Q3PT3R:rdbk - unit: A -- type: pyaml.magnet.quadrupole - name: Q3M2T3R - lattice_names: Q3M2T3R - model: - type: pyaml.magnet.linear_model - calibration_factor: -0.015735 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - write_pvname: Q3PT3R:set - read_pvname: Q3PT3R:rdbk - unit: A -# Q3 D4 -- type: pyaml.magnet.quadrupole - name: Q3M1D4R - lattice_names: Q3M1D4R - model: - type: pyaml.magnet.linear_model - calibration_factor: -0.0158575 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - write_pvname: Q3PD4R:set - read_pvname: Q3PD4R:rdbk - unit: A -- type: pyaml.magnet.quadrupole - name: Q3M2D4R - lattice_names: Q3M2D4R - model: - type: pyaml.magnet.linear_model - calibration_factor: -0.0158575 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - write_pvname: Q3PD4R:set - read_pvname: Q3PD4R:rdbk - unit: A -# Q3 T4 -- type: pyaml.magnet.quadrupole - name: Q3M1T4R - lattice_names: Q3M1T4R - model: - type: pyaml.magnet.linear_model - calibration_factor: -0.015735 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - write_pvname: Q3PT4R:set - read_pvname: Q3PT4R:rdbk - unit: A -- type: pyaml.magnet.quadrupole - name: Q3M2T4R - lattice_names: Q3M2T4R - model: - type: pyaml.magnet.linear_model - calibration_factor: -0.015735 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - write_pvname: Q3PT4R:set - read_pvname: Q3PT4R:rdbk - unit: A -# Q3 D5 -- type: pyaml.magnet.quadrupole - name: Q3M1D5R - lattice_names: Q3M1D5R - model: - type: pyaml.magnet.linear_model - calibration_factor: -0.0158575 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - write_pvname: Q3PD5R:set - read_pvname: Q3PD5R:rdbk - unit: A -- type: pyaml.magnet.quadrupole - name: Q3M2D5R - lattice_names: Q3M2D5R - model: - type: pyaml.magnet.linear_model - calibration_factor: -0.0158575 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - write_pvname: Q3PD5R:set - read_pvname: Q3PD5R:rdbk - unit: A -# Q3 T5 -- type: pyaml.magnet.quadrupole - name: Q3M1T5R - lattice_names: Q3M1T5R - model: - type: pyaml.magnet.linear_model - calibration_factor: -0.015735 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - write_pvname: Q3PT5R:set - read_pvname: Q3PT5R:rdbk - unit: A -- type: pyaml.magnet.quadrupole - name: Q3M2T5R - lattice_names: Q3M2T5R - model: - type: pyaml.magnet.linear_model - calibration_factor: -0.015735 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - write_pvname: Q3PT5R:set - read_pvname: Q3PT5R:rdbk - unit: A -# Q3 D6 -- type: pyaml.magnet.quadrupole - name: Q3M1D6R - lattice_names: Q3M1D6R - model: - type: pyaml.magnet.linear_model - calibration_factor: -0.0158575 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - write_pvname: Q3PD6R:set - read_pvname: Q3PD6R:rdbk - unit: A -- type: pyaml.magnet.quadrupole - name: Q3M2D6R - lattice_names: Q3M2D6R - model: - type: pyaml.magnet.linear_model - calibration_factor: -0.0158575 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - write_pvname: Q3PD6R:set - read_pvname: Q3PD6R:rdbk - unit: A -# Q3 T6 -- type: pyaml.magnet.quadrupole - name: Q3M1T6R - lattice_names: Q3M1T6R - model: - type: pyaml.magnet.linear_model - calibration_factor: -0.015735 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - write_pvname: Q3P1T6R:set - read_pvname: Q3P1T6R:rdbk - unit: A -- type: pyaml.magnet.quadrupole - name: Q3M2T6R - lattice_names: Q3M2T6R - model: - type: pyaml.magnet.linear_model - calibration_factor: -0.015735 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - write_pvname: Q3P2T6R:set - read_pvname: Q3P2T6R:rdbk - unit: A -# Q3 D7 -- type: pyaml.magnet.quadrupole - name: Q3M1D7R - lattice_names: Q3M1D7R - model: - type: pyaml.magnet.linear_model - calibration_factor: -0.0158575 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - write_pvname: Q3PD7R:set - read_pvname: Q3PD7R:rdbk - unit: A -- type: pyaml.magnet.quadrupole - name: Q3M2D7R - lattice_names: Q3M2D7R - model: - type: pyaml.magnet.linear_model - calibration_factor: -0.0158575 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - write_pvname: Q3PD7R:set - read_pvname: Q3PD7R:rdbk - unit: A -# Q3 T7 -- type: pyaml.magnet.quadrupole - name: Q3M1T7R - lattice_names: Q3M1T7R - model: - type: pyaml.magnet.linear_model - calibration_factor: -0.015735 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - write_pvname: Q3PT7R:set - read_pvname: Q3PT7R:rdbk - unit: A -- type: pyaml.magnet.quadrupole - name: Q3M2T7R - lattice_names: Q3M2T7R - model: - type: pyaml.magnet.linear_model - calibration_factor: -0.015735 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - write_pvname: Q3PT7R:set - read_pvname: Q3PT7R:rdbk - unit: A -# Q3 D8 -- type: pyaml.magnet.quadrupole - name: Q3M1D8R - lattice_names: Q3M1D8R - model: - type: pyaml.magnet.linear_model - calibration_factor: -0.0158575 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - write_pvname: Q3PD8R:set - read_pvname: Q3PD8R:rdbk - unit: A -- type: pyaml.magnet.quadrupole - name: Q3M2D8R - lattice_names: Q3M2D8R - model: - type: pyaml.magnet.linear_model - calibration_factor: -0.0158575 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - write_pvname: Q3PD8R:set - read_pvname: Q3PD8R:rdbk - unit: A -# Q3 T8 -- type: pyaml.magnet.quadrupole - name: Q3M1T8R - lattice_names: Q3M1T8R - model: - type: pyaml.magnet.linear_model - calibration_factor: -0.015735 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - write_pvname: Q3P1T8R:set - read_pvname: Q3P1T8R:rdbk - unit: A -- type: pyaml.magnet.quadrupole - name: Q3M2T8R - lattice_names: Q3M2T8R - model: - type: pyaml.magnet.linear_model - calibration_factor: -0.015735 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - write_pvname: Q3P2T8R:set - read_pvname: Q3P2T8R:rdbk - unit: A -# Q4 D1 -- type: pyaml.magnet.quadrupole - name: Q4M1D1R - lattice_names: Q4M1D1R - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.0303165 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - write_pvname: Q4PD1R:set - read_pvname: Q4PD1R:rdbk - unit: A -- type: pyaml.magnet.quadrupole - name: Q4M2D1R - lattice_names: Q4M2D1R - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.0303165 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - write_pvname: Q4PD1R:set - read_pvname: Q4PD1R:rdbk - unit: A -# Q34T1 -- type: pyaml.magnet.quadrupole - name: Q4M1T1R - lattice_names: Q4M1T1R - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.0296695 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - write_pvname: Q4P1T1R:set - read_pvname: Q4P1T1R:rdbk - unit: A -- type: pyaml.magnet.quadrupole - name: Q4M2T1R - lattice_names: Q4M2T1R - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.0296695 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - write_pvname: Q4P2T1R:set - read_pvname: Q4P2T1R:rdbk - unit: A -# Q4 D2 -- type: pyaml.magnet.quadrupole - name: Q4M1D2R - lattice_names: Q4M1D2R - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.0303165 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - write_pvname: Q4PD2R:set - read_pvname: Q4PD2R:rdbk - unit: A -- type: pyaml.magnet.quadrupole - name: Q4M2D2R - lattice_names: Q4M2D2R - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.0303165 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - write_pvname: Q4PD2R:set - read_pvname: Q4PD2R:rdbk - unit: A -# Q4 T2 -- type: pyaml.magnet.quadrupole - name: Q4M1T2R - lattice_names: Q4M1T2R - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.0296695 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - write_pvname: Q4PT2R:set - read_pvname: Q4PT2R:rdbk - unit: A -- type: pyaml.magnet.quadrupole - name: Q4M2T2R - lattice_names: Q4M2T2R - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.0296695 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - write_pvname: Q4PT2R:set - read_pvname: Q4PT2R:rdbk - unit: A -# Q4 D3 -- type: pyaml.magnet.quadrupole - name: Q4M1D3R - lattice_names: Q4M1D3R - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.0303165 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - write_pvname: Q4PD3R:set - read_pvname: Q4PD3R:rdbk - unit: A -- type: pyaml.magnet.quadrupole - name: Q4M2D3R - lattice_names: Q4M2D3R - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.0303165 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - write_pvname: Q4PD3R:set - read_pvname: Q4PD3R:rdbk - unit: A -# Q4 T3 -- type: pyaml.magnet.quadrupole - name: Q4M1T3R - lattice_names: Q4M1T3R - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.0296695 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - write_pvname: Q4PT3R:set - read_pvname: Q4PT3R:rdbk - unit: A -- type: pyaml.magnet.quadrupole - name: Q4M2T3R - lattice_names: Q4M2T3R - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.0296695 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - write_pvname: Q4PT3R:set - read_pvname: Q4PT3R:rdbk - unit: A -# Q4 D4 -- type: pyaml.magnet.quadrupole - name: Q4M1D4R - lattice_names: Q4M1D4R - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.0303165 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - write_pvname: Q4PD4R:set - read_pvname: Q4PD4R:rdbk - unit: A -- type: pyaml.magnet.quadrupole - name: Q4M2D4R - lattice_names: Q4M2D4R - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.0303165 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - write_pvname: Q4PD4R:set - read_pvname: Q4PD4R:rdbk - unit: A -# Q4 T4 -- type: pyaml.magnet.quadrupole - name: Q4M1T4R - lattice_names: Q4M1T4R - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.0296695 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - write_pvname: Q4PT4R:set - read_pvname: Q4PT4R:rdbk - unit: A -- type: pyaml.magnet.quadrupole - name: Q4M2T4R - lattice_names: Q4M2T4R - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.0296695 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - write_pvname: Q4PT4R:set - read_pvname: Q4PT4R:rdbk - unit: A -# Q4 D5 -- type: pyaml.magnet.quadrupole - name: Q4M1D5R - lattice_names: Q4M1D5R - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.0303165 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - write_pvname: Q4PD5R:set - read_pvname: Q4PD5R:rdbk - unit: A -- type: pyaml.magnet.quadrupole - name: Q4M2D5R - lattice_names: Q4M2D5R - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.0303165 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - write_pvname: Q4PD5R:set - read_pvname: Q4PD5R:rdbk - unit: A -# Q4 T5 -- type: pyaml.magnet.quadrupole - name: Q4M1T5R - lattice_names: Q4M1T5R - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.0296695 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - write_pvname: Q4PT5R:set - read_pvname: Q4PT5R:rdbk - unit: A -- type: pyaml.magnet.quadrupole - name: Q4M2T5R - lattice_names: Q4M2T5R - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.0296695 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - write_pvname: Q4PT5R:set - read_pvname: Q4PT5R:rdbk - unit: A -# Q4 D6 -- type: pyaml.magnet.quadrupole - name: Q4M1D6R - lattice_names: Q4M1D6R - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.0303165 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - write_pvname: Q4PD6R:set - read_pvname: Q4PD6R:rdbk - unit: A -- type: pyaml.magnet.quadrupole - name: Q4M2D6R - lattice_names: Q4M2D6R - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.0303165 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - write_pvname: Q4PD6R:set - read_pvname: Q4PD6R:rdbk - unit: A -# Q4 T6 -- type: pyaml.magnet.quadrupole - name: Q4M1T6R - lattice_names: Q4M1T6R - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.0296695 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - write_pvname: Q4P1T6R:set - read_pvname: Q4P1T6R:rdbk - unit: A -- type: pyaml.magnet.quadrupole - name: Q4M2T6R - lattice_names: Q4M2T6R - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.0296695 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - write_pvname: Q4P2T6R:set - read_pvname: Q4P2T6R:rdbk - unit: A -# Q4 D7 -- type: pyaml.magnet.quadrupole - name: Q4M1D7R - lattice_names: Q4M1D7R - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.0303165 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - write_pvname: Q4PD7R:set - read_pvname: Q4PD7R:rdbk - unit: A -- type: pyaml.magnet.quadrupole - name: Q4M2D7R - lattice_names: Q4M2D7R - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.0303165 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - write_pvname: Q4PD7R:set - read_pvname: Q4PD7R:rdbk - unit: A -# Q4 T7 -- type: pyaml.magnet.quadrupole - name: Q4M1T7R - lattice_names: Q4M1T7R - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.0296695 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - write_pvname: Q4PT7R:set - read_pvname: Q4PT7R:rdbk - unit: A -- type: pyaml.magnet.quadrupole - name: Q4M2T7R - lattice_names: Q4M2T7R - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.0296695 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - write_pvname: Q4PT7R:set - read_pvname: Q4PT7R:rdbk - unit: A -# Q4 D8 -- type: pyaml.magnet.quadrupole - name: Q4M1D8R - lattice_names: Q4M1D8R - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.0303165 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - write_pvname: Q4PD8R:set - read_pvname: Q4PD8R:rdbk - unit: A -- type: pyaml.magnet.quadrupole - name: Q4M2D8R - lattice_names: Q4M2D8R - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.0303165 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - write_pvname: Q4PD8R:set - read_pvname: Q4PD8R:rdbk - unit: A -# Q4 T8 -- type: pyaml.magnet.quadrupole - name: Q4M1T8R - lattice_names: Q4M1T8R - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.0296695 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - write_pvname: Q4P1T8R:set - read_pvname: Q4P1T8R:rdbk - unit: A -- type: pyaml.magnet.quadrupole - name: Q4M2T8R - lattice_names: Q4M2T8R - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.0296695 - unit: 1/m - powerconverter: - type: pyaml_cs_oa.epicsRW - write_pvname: Q4P2T8R:set - read_pvname: Q4P2T8R:rdbk - unit: A -- type: pyaml.diagnostics.tune_monitor - name: BETATRON_TUNE - tune_h: - type: pyaml_cs_oa.epicsR - read_pvname: beam:twiss:x:tune - unit: '' - tune_v: - type: pyaml_cs_oa.epicsR - read_pvname: beam:twiss:y:tune - unit: '' -- type: pyaml.tuning_tools.tune - name: DEFAULT_TUNE_CORRECTION - quad_array_name: QForTune - betatron_tune_name: BETATRON_TUNE - response_matrix: file:trm.json -- type: pyaml.tuning_tools.tune_response_matrix - name: DEFAULT_TUNE_RESPONSE_MATRIX - quad_array_name: QForTune - betatron_tune_name: BETATRON_TUNE - quad_delta: 1e-4 diff --git a/examples/BESSY2_example/README.md b/examples/BESSY2_example/README.md deleted file mode 100644 index 6f42e2004..000000000 --- a/examples/BESSY2_example/README.md +++ /dev/null @@ -1,60 +0,0 @@ -# Instructions for how to run the BESSY II examples. - -## Install pyAML - -1. Create a virtual environment and activate it. It needs to have >= Python 3.11. - -2. Install pyAML including the ophyd-async EPICS bindings. - - ```bash - pip install accelerator-middle-layer[cs-ao-epics] - ``` - -## Start the BESSY II virtual accelerator - -1. Install [Apptainer](https://apptainer.org/docs/admin/main/installation.html) by following the instructions in the [documentation](https://pyaml.readthedocs.io/en/latest/how-to/apptainer.html). - - -2. Open a terminal and start the container. - - ```bash - apptainer run oras://registry.hzdr.de/digital-twins-for-accelerators/containers/pyat-softioc-digital-twin:default-v0-5-1-bessy.2711893 - ``` - - ***Keep this terminal running and don't do anything else in it.*** The virtual accelerator will run there and you will be able to interact with it from other terminals, jupyter notebooks, IDEs etc over the network. - -3. If you want to see which PVs are available in the twin you need EPICS tools. A separate container is available for this. - - Open a new terminal and start the container. - - ```bash - apptainer run oras://registry.hzdr.de/digital-twins-for-accelerators/epics-tools:latest - ``` - - In the container run `pvlist`. It will output something like: - - ``` - GUID 0x15EB588C5158BCD5284BE8F0 version 2: tcp@[ 134.30.9.13:5075 134.30.190.240:5075 ] - ``` - - To see the list of available PVs do: - - ``` - pvlist 0x15EB588C5158BCD5284BE8F0 - ``` - - You will see that all PVs start with a prefix corresponding to your username. This is to make the PVs for your virtual accelerator instance unique on the network. - - - ## Run the examples - - 1. Download (or clone) the example files. They exist both as a notebook or scripts depending on what you prefer to use. - - 2. Edit the yaml config files so the control system prefix matches the prefix for your virtual accelerator or you won't be able to connect to it. This is the part to change: - - ```yaml - controls: - - type: pyaml_cs_oa.controlsystem - prefix: "your_prefix:" - name: live - ``` diff --git a/examples/BESSY2_example/bessy2-chroma.ipynb b/examples/BESSY2_example/bessy2-chroma.ipynb deleted file mode 100644 index 4a3e02c71..000000000 --- a/examples/BESSY2_example/bessy2-chroma.ipynb +++ /dev/null @@ -1,25 +0,0 @@ -{ - "cells": [ - { - "cell_type": "code", - "execution_count": null, - "id": "9be4d265", - "metadata": {}, - "outputs": [], - "source": [] - } - ], - "metadata": { - "kernelspec": { - "display_name": "jlp-py312", - "language": "python", - "name": "python3" - }, - "language_info": { - "name": "python", - "version": "3.12.2" - } - }, - "nbformat": 4, - "nbformat_minor": 5 -} diff --git a/examples/BESSY2_example/bessy2-chroma.py b/examples/BESSY2_example/bessy2-chroma.py deleted file mode 100644 index 21872e4c0..000000000 --- a/examples/BESSY2_example/bessy2-chroma.py +++ /dev/null @@ -1,45 +0,0 @@ -"""Chromaticity measurement - -This example shows how to run chromaticity measurement using the simulator -or the virtual accelerator. -If you want to test the virtual accelerator you need to start the -container before running the script. - -""" - -import numpy as np - -from pyaml.accelerator import Accelerator -from pyaml.common.constants import Action - -# ----- Load the configuration ----- -# Remember to change the prefix for the live mode to the one matching -# your virtual accelerator before loading. - -sr = Accelerator.load("BESSY2Chroma.yaml") - -# ----- Define a callback ----- -# This callback is used to print output during the chromaticity measurement. - - -def chroma_callback(action: int, cb_data: dict): - if action == Action.MEASURE: - print(f"Chromaticy measurement: #{cb_data['step']} RF={cb_data['rf']} Tune={cb_data['tune']}") - return True - - -# ----- Get the momentum compaction factor----- -# To get the momentum compaction from the model you need to first turn 6D off. - -sr.design.get_lattice().disable_6d() -alphac = sr.design.get_lattice().get_mcf() -sr.design.get_lattice().enable_6d() -print(f"Moment compaction factor: {alphac}") - -# ----- Measure the chromaticity----- -# The measurement routing will also show a plot. - -chromaticity_monitor = sr.live.get_chromaticity_monitor("KSI") -chromaticity_monitor.measure(do_plot=True, alphac=alphac, callback=chroma_callback) -ksi = chromaticity_monitor.chromaticity.get() -print(ksi) diff --git a/examples/BESSY2_example/bessy2-orbit.ipynb b/examples/BESSY2_example/bessy2-orbit.ipynb deleted file mode 100644 index 4356697d9..000000000 --- a/examples/BESSY2_example/bessy2-orbit.ipynb +++ /dev/null @@ -1,587 +0,0 @@ -{ - "cells": [ - { - "cell_type": "markdown", - "id": "9df36778", - "metadata": {}, - "source": [ - "### Orbit correction\n", - "\n", - "This example shows how to run orbit correction using the simulator or the virtual accelerator. \n", - "If you want to test the virtual accelerator you need to start the container before running the notebook." - ] - }, - { - "cell_type": "code", - "execution_count": 40, - "id": "747364f7", - "metadata": {}, - "outputs": [], - "source": [ - "import json\n", - "import time\n", - "\n", - "import matplotlib.pyplot as plt\n", - "import numpy as np\n", - "\n", - "from pyaml.accelerator import Accelerator" - ] - }, - { - "cell_type": "code", - "execution_count": 41, - "id": "aff4d20f", - "metadata": {}, - "outputs": [ - { - "name": "stdout", - "output_type": "stream", - "text": [ - "23 Apr 2026, 08:36:50 | WARNING | PyAML OA control system binding (0.1.1) initialized with name 'live' and prefix='pons:'\n", - "23 Apr 2026, 08:36:50 | INFO | Setting the rf_weight by default to inf.\n", - "23 Apr 2026, 08:36:50 | INFO | Setting the rf_weight by default to inf.\n", - "23 Apr 2026, 08:36:50 | INFO | Setting the rf_weight by default to inf.\n", - "Controls:\n", - " live\n", - " .\n", - "\n", - "Simulators:\n", - " design\n", - " .\n", - "\n", - "Arrays:\n", - " BPM (pyaml.arrays.bpm_array) size=123\n", - " HCorr (pyaml.arrays.magnet_array) size=48\n", - " VCorr (pyaml.arrays.magnet_array) size=64\n", - " .\n", - "\n", - "Tools:\n", - " DEFAULT_ORBIT_RESPONSE_MATRIX (pyaml.tuning_tools.orbit_response_matrix)\n", - " DEFAULT_DISPERSION (pyaml.tuning_tools.dispersion)\n", - " DEFAULT_ORBIT_CORRECTION (pyaml.tuning_tools.orbit)\n", - " .\n" - ] - } - ], - "source": [ - "# Load the configuration\n", - "# Remember to change the prefix for the live mode to the one matching your virtual\n", - "# accelerator before loading.\n", - "sr = Accelerator.load(\"BESSY2Orbit.yaml\")\n", - "print(sr.yellow_pages)" - ] - }, - { - "cell_type": "markdown", - "id": "edf1d5f4", - "metadata": {}, - "source": [ - "#### Measure the orbit response matrix\n", - "\n", - "If there is no existing orbit response matrix you need to measure it. This can be done on either the design or live mode. \n", - "It is also possible to measure the ORM using the design mode and use it to correct the live mode." - ] - }, - { - "cell_type": "code", - "execution_count": 42, - "id": "9caca764", - "metadata": {}, - "outputs": [], - "source": [ - "# Choose which backend to use.\n", - "SR = sr.design\n", - "# SR = sr.live\n", - "\n", - "# if the ORM is not present measure it\n", - "if sr.design.orbit.response_matrix is None:\n", - " sr.design.orm.measure(set_wait_time=0.0 if SR == sr.design else 2.0)\n", - " sr.design.orm.save(\"orm.json\")" - ] - }, - { - "cell_type": "markdown", - "id": "ddcf4f28", - "metadata": {}, - "source": [ - "#### Load the response matrix\n", - "\n", - "The example does the correction for the live mode but it can also be done on the design mode." - ] - }, - { - "cell_type": "code", - "execution_count": 43, - "id": "50c2e8a4", - "metadata": {}, - "outputs": [ - { - "name": "stdout", - "output_type": "stream", - "text": [ - "23 Apr 2026, 08:37:08 | INFO | Setting the rf_weight by default to inf.\n" - ] - } - ], - "source": [ - "# Load the ORM for the live mode\n", - "sr.live.orbit.load(\"orm.json\")" - ] - }, - { - "cell_type": "code", - "execution_count": 44, - "id": "38dc01be", - "metadata": {}, - "outputs": [], - "source": [ - "# Reset corrector to 0 on the twin\n", - "sr.live.get_magnets(\"HCorr\").strengths.set(np.zeros(48))\n", - "sr.live.get_magnets(\"VCorr\").strengths.set(np.zeros(64))" - ] - }, - { - "cell_type": "code", - "execution_count": null, - "id": "d6e7ba16", - "metadata": {}, - "outputs": [], - "source": [ - "# Set orbit for design\n", - "\n", - "std_kick = 100e-6\n", - "corr_d = sr.design.get_magnet(\"VS3M2D1R\")\n", - "corr_d.strength.set(std_kick)\n", - "\n", - "orbit_d = sr.design.get_bpms(\"BPM\").positions" - ] - }, - { - "cell_type": "markdown", - "id": "47ec4270", - "metadata": {}, - "source": [ - "#### Correct the orbit" - ] - }, - { - "cell_type": "code", - "execution_count": null, - "id": "419ccee1", - "metadata": {}, - "outputs": [], - "source": [ - "# Set orbit for live\n", - "\n", - "std_kick = 100e-6\n", - "corr_l = sr.live.get_magnet(\"VS3M2D1R\")\n", - "corr_l.strength.set(std_kick)\n", - "\n", - "orbit_l = sr.live.get_bpms(\"BPM\").positions" - ] - }, - { - "cell_type": "code", - "execution_count": null, - "id": "f7f03793", - "metadata": {}, - "outputs": [], - "source": [ - "# Plot comparison\n", - "plt.plot(orbit_d.get()[:, 1] * 1e3)\n", - "plt.plot(orbit_l.get()[:, 1] * 1e-6)" - ] - }, - { - "cell_type": "code", - "execution_count": null, - "id": "c2bd7949", - "metadata": {}, - "outputs": [], - "source": [ - "# get the AT ring\n", - "ring = sr.design.get_lattice()\n", - "\n", - "# Get AT element for a given BPM\n", - "# bpm = sr.design.get_bpm(\"BPMZ4D1R\")\n", - "# elt = bpm.positions._RBpmArray__element\n", - "# print(elt)\n", - "\n", - "# Get AT element for a given steerer\n", - "# steer = sr.design.get_magnet(\"VS3M2T6R\")\n", - "# elt = steer.strength._RWStrengthScalar__elements[0]\n", - "# print(elt)" - ] - }, - { - "cell_type": "code", - "execution_count": null, - "id": "484fc6fc", - "metadata": {}, - "outputs": [], - "source": [ - "ring[\"S3M2D1R\"]" - ] - }, - { - "cell_type": "code", - "execution_count": null, - "id": "74ff1047", - "metadata": {}, - "outputs": [], - "source": [ - "ring[\"S4M2D1R\"]" - ] - }, - { - "cell_type": "code", - "execution_count": null, - "id": "b3502dd4", - "metadata": {}, - "outputs": [], - "source": [ - "import at\n", - "\n", - "elements = ring[at.checkattr(\"Corrector\", attrvalue=\"H\")]\n", - "\n", - "for elem in elements:\n", - " print(elem.PolynomA)\n", - " # print(elem.KickAngle)" - ] - }, - { - "cell_type": "code", - "execution_count": null, - "id": "6b263174", - "metadata": {}, - "outputs": [], - "source": [ - "# Get the devices\n", - "hcorr = sr.live.get_magnets(\"HCorr\")\n", - "vcorr = sr.live.get_magnets(\"VCorr\")\n", - "orbit = sr.live.get_bpms(\"BPM\").positions\n", - "\n", - "# Create an initial orbit with errors\n", - "std_kick = 100e-6\n", - "corr = sr.live.get_magnet(\"VS3M2D1R\")\n", - "corr.strength.set(std_kick)\n", - "# hcorr.strengths.set(std_kick)\n", - "# hcorr.strengths.set(std_kick * np.random.normal(size=len(hcorr)))\n", - "# vcorr.strengths.set(std_kick * np.random.normal(size=len(vcorr)))\n", - "time.sleep(3)\n", - "\n", - "print(vcorr.strengths.get())\n", - "\n", - "\n", - "# orbit_initial = orbit.get()\n", - "# print(orbit_initial)" - ] - }, - { - "cell_type": "code", - "execution_count": null, - "id": "0b5e533b", - "metadata": {}, - "outputs": [], - "source": [ - "# Get the devices\n", - "hcorr_d = sr.design.get_magnets(\"HCorr\")\n", - "vcorr_d = sr.design.get_magnets(\"VCorr\")\n", - "orbit_d = sr.design.get_bpms(\"BPM\").positions\n", - "\n", - "# Create an initial orbit with errors\n", - "std_kick = 100e-6\n", - "corr_d = sr.design.get_magnet(\"VS3M2D1R\")\n", - "corr_d.strength.set(std_kick)\n", - "# hcorr.strengths.set(std_kick)\n", - "# hcorr.strengths.set(std_kick * np.random.normal(size=len(hcorr)))\n", - "# vcorr.strengths.set(std_kick * np.random.normal(size=len(vcorr)))\n", - "time.sleep(3)\n", - "\n", - "print(vcorr_d.strengths.get())\n", - "\n", - "\n", - "# orbit_initial = orbit.get()\n", - "# print(orbit_initial)" - ] - }, - { - "cell_type": "code", - "execution_count": null, - "id": "ba50460d", - "metadata": {}, - "outputs": [], - "source": [] - }, - { - "cell_type": "code", - "execution_count": null, - "id": "fcef2603", - "metadata": {}, - "outputs": [], - "source": [ - "print(vcorr.strengths.get())" - ] - }, - { - "cell_type": "code", - "execution_count": null, - "id": "9092481a", - "metadata": {}, - "outputs": [], - "source": [ - "orbit_initial = orbit.get()\n", - "print(orbit_initial)\n", - "\n", - "plt.plot(orbit_initial * 1e-6)" - ] - }, - { - "cell_type": "code", - "execution_count": null, - "id": "1f51011c", - "metadata": {}, - "outputs": [], - "source": [ - "plt.plot(orbit.get()[:, 1])" - ] - }, - { - "cell_type": "code", - "execution_count": null, - "id": "179fa459", - "metadata": {}, - "outputs": [], - "source": [ - "# Compare to MML\n", - "\n", - "mml_values = np.array(\n", - " [\n", - " -0.548395086903857,\n", - " -1.012630432646402,\n", - " -0.862897505672887,\n", - " -0.522995524471487,\n", - " -0.658189856521371,\n", - " -0.516173101625783,\n", - " -0.133057027821788,\n", - " 0.392126054914456,\n", - " 0.563934272606167,\n", - " 0.740274085202912,\n", - " 0.620698379527692,\n", - " 0.355609275038271,\n", - " 0.423333396468476,\n", - " 0.301220987985241,\n", - " 0.066145853113093,\n", - " -0.651251097949268,\n", - " -1.170560020657783,\n", - " -1.120870632419439,\n", - " -0.779628042974558,\n", - " -1.098108137417404,\n", - " -1.039280007232975,\n", - " -0.564055382358618,\n", - " 0.538526284971412,\n", - " 0.577087080051735,\n", - " 0.615647875132058,\n", - " 0.649838446769944,\n", - " 1.107595363627166,\n", - " 1.098222848289203,\n", - " 0.780522962096338,\n", - " 1.116307896849065,\n", - " 1.095279850154315,\n", - " 0.584401801876353,\n", - " -0.212660175271086,\n", - " -0.542094629513108,\n", - " -0.632844890961403,\n", - " -0.527361773381497,\n", - " -0.831735165388016,\n", - " -0.906921111725548,\n", - " -0.656288869430261,\n", - " 0.152637608565171,\n", - " 0.510107802114268,\n", - " 0.634095433537279,\n", - " 0.547794913320217,\n", - " 0.880254059263082,\n", - " 0.992704581728260,\n", - " 0.634065043149221,\n", - " 0.466416157613840,\n", - " 0.647773785871704,\n", - " 0.489669647202759,\n", - " 0.240171949704727,\n", - " 0.236207591023490,\n", - " 0.087170336604686,\n", - " -0.125032463676224,\n", - " -0.512234534072165,\n", - " -0.595737451399580,\n", - " -0.459325090830385,\n", - " -0.227936257211556,\n", - " -0.227839435382618,\n", - " -0.092195396495755,\n", - " 0.058374234146639,\n", - " 0.690818147727373,\n", - " 1.205830275263787,\n", - " 1.134748178819593,\n", - " 0.774249133536717,\n", - " 1.075344527114256,\n", - " 0.997510204603194,\n", - " 0.517264575129486,\n", - " -0.689094833374326,\n", - " -1.135883617362593,\n", - " -1.107761758717994,\n", - " -0.773840868709177,\n", - " -1.092921802241169,\n", - " -1.055434449386964,\n", - " -0.556094229916365,\n", - " -0.488750222978695,\n", - " -0.205031956664856,\n", - " -0.094293028012348,\n", - " 0.223157437268723,\n", - " 0.670960218378011,\n", - " 0.754507772466096,\n", - " 0.611363709323305,\n", - " 0.949153074191396,\n", - " 1.002567634614958,\n", - " 0.459717119030237,\n", - " 0.093438467057282,\n", - " -0.385082846682778,\n", - " -0.756736774143839,\n", - " -0.841579773055778,\n", - " -0.670533979887471,\n", - " -1.030994728204280,\n", - " -1.108871586555440,\n", - " -0.674176224876900,\n", - " -0.292569481789967,\n", - " -0.326424012263231,\n", - " -0.176245513853861,\n", - " -0.018289777369182,\n", - " 0.080420482968790,\n", - " 0.218206834561504,\n", - " 0.302341005180173,\n", - " 0.267295068412974,\n", - " 0.177434401470334,\n", - " -0.001920387408844,\n", - " -0.151210006643998,\n", - " -0.219977657081387,\n", - " -0.426651371994250,\n", - " -0.568250084439999,\n", - " -0.424347192298211,\n", - " -0.651182683604045,\n", - " -1.035004865223722,\n", - " -0.897905345744703,\n", - " -0.552553098168575,\n", - " -0.705228145938345,\n", - " -0.569045105220304,\n", - " -0.175959630086212,\n", - " 0.699461083747587,\n", - " 1.024675280579722,\n", - " 0.918681075556277,\n", - " 0.576846841787854,\n", - " 0.749151978895954,\n", - " 0.637694866837515,\n", - " 0.278751432881705,\n", - " 0.135521946298300,\n", - " 0.104948249372505,\n", - " ]\n", - ")\n", - "\n", - "print(np.size(orbit_initial[:, 1]))\n", - "\n", - "plt.plot(orbit_initial[:, 1] * 1e-6, label=\"Twin\")\n", - "plt.plot(mml_values, label=\"MML\")\n", - "plt.legend()\n", - "plt.xlabel(\"BPM number\")\n", - "plt.ylabel(\"Vertical orbit\")" - ] - }, - { - "cell_type": "code", - "execution_count": null, - "id": "83b7e52c", - "metadata": {}, - "outputs": [], - "source": [ - "# Correct the orbit\n", - "# If you are using the ORM measured on design to correct on live you need to set the\n", - "# gain since the unit for the BPMs are not the same for both modes yet.\n", - "\n", - "sr.live.orbit.correct(gain=1e-9, singular_values_H=48, singular_values_V=64)\n", - "# sr.design.orbit.correct()\n", - "# sr.live.orbit.correct()\n", - "\n", - "time.sleep(3)\n", - "orbit_after = orbit.get()" - ] - }, - { - "cell_type": "markdown", - "id": "02d0b6b0", - "metadata": {}, - "source": [ - "##### Plot the results" - ] - }, - { - "cell_type": "code", - "execution_count": null, - "id": "7c862a7c", - "metadata": {}, - "outputs": [], - "source": [ - "# Remember: if you change the example from live to design you need to change the unit\n", - "# for the orbit when plotting since not the same yet.\n", - "\n", - "fig = plt.figure()\n", - "ax1 = fig.add_subplot(311)\n", - "ax2 = fig.add_subplot(312)\n", - "ax3 = fig.add_subplot(313)\n", - "ax1.plot(orbit_initial[:, 0] * 1e-6, label=\"Orbit before correction\")\n", - "ax2.plot(orbit_initial[:, 1] * 1e-6, label=\"Orbit before correction\")\n", - "ax1.plot(orbit_after[:, 0] * 1e-6, label=\"Orbit after correction\")\n", - "ax2.plot(orbit_after[:, 1] * 1e-6, label=\"Orbit after correction\")\n", - "\n", - "ax3.plot(hcorr.strengths.get(), label=\"H Steerers\")\n", - "ax3.plot(vcorr.strengths.get(), label=\"V Steerers\")\n", - "\n", - "ax1.set_ylabel(\"Horizontal pos. [mm]\")\n", - "ax2.set_ylabel(\"Vertical pos. [mm]\")\n", - "ax2.set_xlabel(\"BPM number\")\n", - "ax3.set_ylabel(\"Strength (rad)\")\n", - "ax3.set_xlabel(\"Steerer number\")\n", - "ax1.legend()\n", - "ax2.legend()\n", - "ax3.legend()\n", - "fig.tight_layout()\n", - "\n", - "plt.show()" - ] - }, - { - "cell_type": "code", - "execution_count": null, - "id": "7bae16d2", - "metadata": {}, - "outputs": [], - "source": [] - } - ], - "metadata": { - "kernelspec": { - "display_name": "jlp-py312", - "language": "python", - "name": "python3" - }, - "language_info": { - "codemirror_mode": { - "name": "ipython", - "version": 3 - }, - "file_extension": ".py", - "mimetype": "text/x-python", - "name": "python", - "nbconvert_exporter": "python", - "pygments_lexer": "ipython3", - "version": "3.12.2" - } - }, - "nbformat": 4, - "nbformat_minor": 5 -} diff --git a/examples/BESSY2_example/bessy2-orbit.py b/examples/BESSY2_example/bessy2-orbit.py deleted file mode 100644 index 3d755b545..000000000 --- a/examples/BESSY2_example/bessy2-orbit.py +++ /dev/null @@ -1,97 +0,0 @@ -"""Orbit correction - -This example shows how to run orbit correction using the simulator or the virtual -accelerator. If you want to test the virtual accelerator you need to start the -container before running the script. - -""" - -import json -import time - -import matplotlib.pyplot as plt -import numpy as np - -from pyaml.accelerator import Accelerator -from pyaml.tuning_tools.orbit_response_matrix_data import OrbitResponseMatrixData - -# ----- Load the configuration ----- -# Remember to change the prefix for the live mode to the one matching your virtual -# accelerator before loading. - -sr = Accelerator.load("BESSY2Orbit.yaml") - -# ----- Measure the orbit response matrix ----- -# If there is no existing orbit response matrix you need to measure it. -# This can be done on either the design or live mode. -# It is also possible to measure the ORM using the design mode and use it to correct -# the live mode. - -# Choose which backend to use. -SR = sr.design -# SR = sr.live - -# if the ORM is not present measure it -if SR.orbit.response_matrix is None: - SR.orm.measure(sleep_between_step=0.0 if SR == sr.design else 2.0) - SR.orm.save("orm.json") - # Load it on orbit correction tool - SR.orbit.load("orm.json") - -# ----- Correct the orbit on live ----- - -# Get the devices -hcorr = SR.get_magnets("HCorr") -vcorr = SR.get_magnets("VCorr") -orbit = SR.get_bpms("BPM").positions - -# Create an initial orbit with errors -std_kick = 10e-6 -hcorr.strengths.set(std_kick * np.random.normal(size=len(hcorr))) -vcorr.strengths.set(std_kick * np.random.normal(size=len(vcorr))) -time.sleep(3) - -orbit_initial = orbit.get() - -# Correct the orbit -# If you are using the ORM measured on design to correct on live you need to set the -# gain since the unit for the BPMs are not the same for both modes yet. - -if SR == sr.design: - SR.orbit.correct() -else: - # BPM are in nm, work around with a 1e-9 weight - SR.orbit.correct(gain=1e-9) - -time.sleep(3) -orbit_after = orbit.get() - -# ----- Plot the results ----- -# Remember: if you change the example from live to design you need to change the unit -# for the orbit when plotting since not the same yet. -# If you are running in VS code you might need to switch the matplotlib backend for -# the plot to show. - -fig = plt.figure() -ax1 = fig.add_subplot(311) -ax2 = fig.add_subplot(312) -ax3 = fig.add_subplot(313) -ax1.plot(orbit_initial[:, 0] * 1e-6, label="Orbit before correction") -ax2.plot(orbit_initial[:, 1] * 1e-6, label="Orbit before correction") -ax1.plot(orbit_after[:, 0] * 1e-6, label="Orbit after correction") -ax2.plot(orbit_after[:, 1] * 1e-6, label="Orbit after correction") - -ax3.plot(hcorr.strengths.get() * 1e6, label="H Steerers") -ax3.plot(vcorr.strengths.get() * 1e6, label="V Steerers") - -ax1.set_ylabel("Horizontal pos. [mm]") -ax2.set_ylabel("Vertical pos. [mm]") -ax2.set_xlabel("BPM number") -ax3.set_ylabel("Strength (urad)") -ax3.set_xlabel("Steerer number") -ax1.legend() -ax2.legend() -ax3.legend() -fig.tight_layout() - -plt.show() diff --git a/examples/BESSY2_example/bessy2-tune.ipynb b/examples/BESSY2_example/bessy2-tune.ipynb deleted file mode 100644 index 5ca7f42b8..000000000 --- a/examples/BESSY2_example/bessy2-tune.ipynb +++ /dev/null @@ -1,128 +0,0 @@ -{ - "cells": [ - { - "cell_type": "markdown", - "id": "61e6520b", - "metadata": {}, - "source": [ - "### Tune correction\n", - "\n", - "This example shows how to run tune correction using the simulator or the virtual accelerator.\n", - "If you want to test the virtual accelerator you need to start the container before running the script." - ] - }, - { - "cell_type": "code", - "execution_count": null, - "id": "1a092dbb", - "metadata": {}, - "outputs": [], - "source": [ - "import time\n", - "\n", - "import numpy as np\n", - "\n", - "from pyaml.accelerator import Accelerator\n", - "from pyaml.common.constants import Action" - ] - }, - { - "cell_type": "code", - "execution_count": null, - "id": "9b63d253", - "metadata": {}, - "outputs": [], - "source": [ - "# ----- Load the configuration -----\n", - "# Remember to change the prefix for the live mode to the one matching\n", - "# your virtual accelerator before loading.\n", - "\n", - "sr = Accelerator.load(\"BESSY2Tune.yaml\")" - ] - }, - { - "cell_type": "code", - "execution_count": null, - "id": "bf603b5f", - "metadata": {}, - "outputs": [], - "source": [ - "# ----- Define a callback -----\n", - "# This callback is used to print output during the tune response measurement.\n", - "\n", - "\n", - "def tune_callback(action: int, cb_data: dict):\n", - " if action == Action.MEASURE:\n", - " # On action measure, the measured dq / dk is passed as argument\n", - " print(f\"Tune response: #{cb_data['step']} {cb_data['magnet']} {cb_data['tune']}\")\n", - " return True" - ] - }, - { - "cell_type": "code", - "execution_count": null, - "id": "d1593276", - "metadata": {}, - "outputs": [], - "source": [ - "# ----- Measure the tune response matrix-----\n", - "# You can measure the tune response matrix on either the design or live mode.\n", - "# At the moment they don't give the same result. This will be fixed later by\n", - "# switching to using SerializedMagnet.\n", - "\n", - "# Choose which backend to use.\n", - "SR = sr.design\n", - "# SR = sr.live\n", - "\n", - "# if the TRM is not present measure it\n", - "if SR.tune.response_matrix is None:\n", - " SR.trm.measure(sleep_between_step=0.0 if SR == sr.design else 2.0, callback=tune_callback)\n", - " SR.trm.save(\"trm.json\")\n", - " # Load it on tune tuning tool\n", - " SR.tune.load(\"trm.json\")" - ] - }, - { - "cell_type": "code", - "execution_count": null, - "id": "153cefd1", - "metadata": {}, - "outputs": [], - "source": [ - "# ----- Correct the tune -----\n", - "\n", - "print(\"\\nRun tune correction:\")\n", - "\n", - "initial_tunes = np.array2string(SR.tune.readback(), precision=6, floatmode=\"fixed\")\n", - "print(f\"Initial tunes: {initial_tunes}\")\n", - "\n", - "SR.tune.set([0.83, 0.84], iter=2, wait_time=3)\n", - "time.sleep(3)\n", - "\n", - "final_tunes = np.array2string(SR.tune.readback(), precision=6, floatmode=\"fixed\")\n", - "print(f\"Final tunes: {final_tunes}\")" - ] - } - ], - "metadata": { - "kernelspec": { - "display_name": "bessy2-tune", - "language": "python", - "name": "python3" - }, - "language_info": { - "codemirror_mode": { - "name": "ipython", - "version": 3 - }, - "file_extension": ".py", - "mimetype": "text/x-python", - "name": "python", - "nbconvert_exporter": "python", - "pygments_lexer": "ipython3", - "version": "3.11.14" - } - }, - "nbformat": 4, - "nbformat_minor": 5 -} diff --git a/examples/BESSY2_example/bessy2-tune.py b/examples/BESSY2_example/bessy2-tune.py deleted file mode 100644 index 2a997cb83..000000000 --- a/examples/BESSY2_example/bessy2-tune.py +++ /dev/null @@ -1,62 +0,0 @@ -"""Tune correction - -This example shows how to run tune correction using the simulator -or the virtual accelerator. -If you want to test the virtual accelerator you need to start the -container before running the script. - -""" - -import time - -import numpy as np - -from pyaml.accelerator import Accelerator -from pyaml.common.constants import Action -from pyaml.magnet.magnet import Magnet - -# ----- Load the configuration ----- -# Remember to change the prefix for the live mode to the one matching -# your virtual accelerator before loading. - -sr = Accelerator.load("BESSY2Tune.yaml") - -# ----- Define a callback ----- -# This callback is used to print output during the tune response measurement. - - -def tune_callback(action: int, cb_data: dict): - if action == Action.MEASURE: - # On action measure, the measured dq / dk is passed as argument - print(f"Tune response: #{cb_data['step']} {cb_data['magnet']} {cb_data['tune']}") - return True - - -# ----- Measure the tune response matrix----- -# You can measure the tune response matrix on either the design or live mode. -# At the moment they don't give the same result. -# This will be fixed later by switching to using SerializedMagnet. - -# Choose which backend to use. -SR = sr.design -# SR = sr.live - -# if the TRM is not present measure it -if sr.design.tune.response_matrix is None: - SR.trm.measure(sleep_between_step=0.0 if SR == sr.design else 2.0, callback=tune_callback) - SR.trm.save("trm.json") - # Load it on tune tuning tool - SR.tune.load("trm.json") - -# ----- Correct the tune ----- - -print("\nRun tune correction:") - -initial_tunes = np.array2string(SR.tune.readback(), precision=6, floatmode="fixed") -print(f"Initial tunes: {initial_tunes}") - -SR.tune.set([0.83, 0.84], iter=2, wait_time=3) -time.sleep(3) - -final_tunes = np.array2string(SR.tune.readback(), precision=6, floatmode="fixed") -print(f"Final tunes: {final_tunes}") diff --git a/examples/ESRF_ORM_example/README.md b/examples/ESRF_ORM_example/README.md deleted file mode 100644 index 0135d41b4..000000000 --- a/examples/ESRF_ORM_example/README.md +++ /dev/null @@ -1,68 +0,0 @@ -# Instructions for how to run the ESRF ORM example. - -## Install pyAML - -1. Create a virtual environment and activate it. It needs to have >= Python 3.11. - -2. Install pyAML including the tango bindings and SimulatedCommissioning (pySC). - - ```bash - pip install accelerator-middle-layer[tango] - pip install accelerator-commissioning - ``` - -3. install EBS dummy Control system. This is valid untill an ESRF virtual machine will be available as for BESSYII and SOLEIL - ```bash - pip install tests/dummy_cs/tango-pyaml - ``` - - ## Run the examples - Several examples are available for ORM correction. - - To run the examples: - 1. navigate to the pyaml root directory - 2. Download (or clone) the example files. - 3. run the files - - ### The correct_orbit.py shows the standard orbit correction - Expected output is: - Creating dummy TangoControlSystem: live - R.m.s. orbit before correction H: 85.1 µm, V: 24.1 µm. - 30 Jan 2026, 14:25:55 | INFO | (Re-)Building pseudoinverse RM with method='svd_values' and parameter=162 with zerosum=True. - 30 Jan 2026, 14:25:55 | INFO | (Re-)Building pseudoinverse RM with method='svd_values' and parameter=162 with zerosum=False. - R.m.s. orbit after correction H: 0.7 µm, V: 0.4 µm, - - ### The measure_dispersion.py shows the standard orbit correction - Expected output is: - 30 Jan 2026, 15:05:47 | WARNING | PyAML Tango control system binding (0.3.2) initialized with name 'live' and TANGO_HOST=ebs-simu-3:10000 - Reading orbit. - Changing RF frequency. - Reading orbit. - Changing RF frequency. - Reading orbit. - Restoring RF frequency. - Reading orbit. - - - ### measure_ideal_ORM.py - Expected output is: - - 30 Jan 2026, 15:02:25 | WARNING | PyAML Tango control system binding (0.3.2) initialized with name 'live' and TANGO_HOST=ebs-simu-3:10000 - 30 Jan 2026, 15:02:27 | INFO | Measuring correctors from the default arrays: HCorr and VCorr. - 30 Jan 2026, 15:02:28 | INFO | Measured response of SH1A-C04-H. - ... - - ### measure_ideal_ORM_and_disp.py - Expected output is: - as the two ouputs above - - ### measure_reduced_ORM.py - Expected output is: - 30 Jan 2026, 15:04:26 | WARNING | PyAML Tango control system binding (0.3.2) initialized with name 'live' and TANGO_HOST=ebs-simu-3:10000 - [0/64], Measured response of SJ2A-C04-H: r.m.s H.: 5.75 mm/mrad, r.m.s. V: 0.00 mm/mrad - [1/64], Measured response of SF2A-C05-H: r.m.s H.: 5.75 mm/mrad, r.m.s. V: 0.00 mm/mrad - [2/64], Measured response of SF2A-C06-H: r.m.s H.: 5.75 mm/mrad, r.m.s. V: 0.00 mm/mrad - ... - [61/64], Measured response of SF2A-C01-V: r.m.s H.: 0.00 mm/mrad, r.m.s. V: 2.08 mm/mrad - [62/64], Measured response of SF2A-C02-V: r.m.s H.: 0.00 mm/mrad, r.m.s. V: 2.08 mm/mrad - [63/64], Measured response of SI2A-C03-V: r.m.s H.: 0.00 mm/mrad, r.m.s. V: 2.08 mm/mrad diff --git a/examples/ESRF_ORM_example/correct_orbit.py b/examples/ESRF_ORM_example/correct_orbit.py deleted file mode 100644 index b3479d6c9..000000000 --- a/examples/ESRF_ORM_example/correct_orbit.py +++ /dev/null @@ -1,77 +0,0 @@ -import time -from pathlib import Path - -import matplotlib.pyplot as plt -import numpy as np - -from pyaml.accelerator import Accelerator - -parent_folder = Path(__file__).parent -pyaml_folder = parent_folder.parent.parent -config_path = pyaml_folder.joinpath("tests/config/EBSOrbit.yaml").resolve() -sr = Accelerator.load(config_path) -# ebs = sr.live -ebs = sr.design - -## get reference -ref_h, ref_v = ebs.get_bpms("BPM").positions.get().T -reference = np.concatenate((ref_h, ref_v)) -######################################################## - -hcorr = ebs.get_magnets("HCorr") -vcorr = ebs.get_magnets("VCorr") -bpms = ebs.get_bpms("BPM") - -if ebs == sr.design: - ## generate some orbit - std_kick = 1e-6 - - np.random.seed(1) - # mangle orbit - hcorr.strengths.set(hcorr.strengths.get() + std_kick * np.random.normal(size=len(hcorr))) - vcorr.strengths.set(vcorr.strengths.get() + std_kick * np.random.normal(size=len(vcorr))) - -h0 = hcorr.strengths.get() -v0 = vcorr.strengths.get() - -positions_bc = bpms.positions.get() -std_bc = np.std(positions_bc, axis=0) -print(f"R.m.s. orbit before correction H: {1e6 * std_bc[0]: .1f} µm, V: {1e6 * std_bc[1]: .1f} µm.") -######################################################## - -ebs.orbit.set_virtual_weight(1000) -## Correct the orbit -ebs.orbit.correct(reference=None, rf=True) -# ebs.orbit.correct(plane="H") -# ebs.orbit.correct(plane="V") -######################################################## - -time.sleep(5) - -## inspect orbit correction -positions_ac = bpms.positions.get() -std_ac = np.std(positions_ac, axis=0) -print(f"R.m.s. orbit after correction H: {1e6 * std_ac[0]: .1f} µm, V: {1e6 * std_ac[1]: .1f} µm,") - -fig = plt.figure() -ax1 = fig.add_subplot(311) -ax2 = fig.add_subplot(312) -ax3 = fig.add_subplot(313) -ax1.plot(positions_bc[:, 0] * 1e6, label="Orbit before correction") -ax2.plot(positions_bc[:, 1] * 1e6, label="Orbit before correction") -ax1.plot(positions_ac[:, 0] * 1e6, label="Orbit after correction") -ax2.plot(positions_ac[:, 1] * 1e6, label="Orbit after correction") - -ax3.plot(hcorr.strengths.get()) -ax3.plot(vcorr.strengths.get()) - -ax1.set_ylabel("Horizontal pos. [μm]") -ax2.set_ylabel("Vertical pos. [μm]") -ax2.set_xlabel("BPM number") -ax3.set_ylabel("Strength (rad)") -ax3.set_xlabel("Steerer number") -fig.tight_layout() - -print(f"Sum of h. corr. trims: {np.sum(hcorr.strengths.get() - h0)}") -print(f"Sum of v. corr. trims: {np.sum(vcorr.strengths.get() - v0)}") -plt.show() diff --git a/examples/ESRF_ORM_example/correct_orbit_disp.py b/examples/ESRF_ORM_example/correct_orbit_disp.py deleted file mode 100644 index ec366d38a..000000000 --- a/examples/ESRF_ORM_example/correct_orbit_disp.py +++ /dev/null @@ -1,75 +0,0 @@ -import json -import logging -from pathlib import Path - -import matplotlib.pyplot as plt -import numpy as np - -from pyaml.accelerator import Accelerator -from pyaml.tuning_tools.orbit import ConfigModel as Orbit_ConfigModel -from pyaml.tuning_tools.orbit import Orbit - -parent_folder = Path(__file__).parent -pyaml_folder = parent_folder.parent.parent -config_path = pyaml_folder.joinpath("tests/config/EBSOrbit.yaml").resolve() -sr = Accelerator.load(config_path) -ebs = sr.design - -## get reference -ref_h, ref_v = ebs.get_bpms("BPM").positions.get().T -reference = np.concatenate((ref_h, ref_v)) -######################################################## - -plant = sr.design.get_rf_plant("RF") -frf = plant.frequency.get() -plant.frequency.set(frf + 100) - - -## generate some orbit -std_kick = 0e-6 -hcorr = ebs.get_magnets("HCorr") -vcorr = ebs.get_magnets("VCorr") -bpms = ebs.get_bpms("BPM") - -# mangle orbit -hcorr.strengths.set(hcorr.strengths.get() + std_kick * np.random.normal(size=len(hcorr))) -vcorr.strengths.set(vcorr.strengths.get() + std_kick * np.random.normal(size=len(vcorr))) - -positions_bc = bpms.positions.get() -std_bc = np.std(positions_bc, axis=0) -print(f"R.m.s. orbit before correction H: {1e6 * std_bc[0]: .1f} µm, V: {1e6 * std_bc[1]: .1f} µm.") -######################################################## - -## Correct the orbit -# ebs.orbit.set_rf_weight(1e7) -ebs.orbit.correct(reference=reference, rf=True, gain_H=1, gain_V=1, gain_RF=1) -ebs.orbit.correct(reference=reference, rf=True, gain_H=1, gain_V=1, gain_RF=1) -# ebs.orbit.correct(plane="H") -# ebs.orbit.correct(plane="V") -######################################################## - -## inspect orbit correction -positions_ac = bpms.positions.get() -std_ac = np.std(positions_ac, axis=0) -print(f"R.m.s. orbit after correction H: {1e6 * std_ac[0]: .1f} µm, V: {1e6 * std_ac[1]: .1f} µm,") - -fig = plt.figure() -ax1 = fig.add_subplot(311) -ax2 = fig.add_subplot(312) -ax3 = fig.add_subplot(313) -ax1.plot(positions_bc[:, 0] * 1e6, label="Orbit before correction") -ax2.plot(positions_bc[:, 1] * 1e6, label="Orbit before correction") -ax1.plot(positions_ac[:, 0] * 1e6, label="Orbit after correction") -ax2.plot(positions_ac[:, 1] * 1e6, label="Orbit after correction") - -ax3.plot(hcorr.strengths.get()) -ax3.plot(vcorr.strengths.get()) - -ax1.set_ylabel("Horizontal pos. [μm]") -ax2.set_ylabel("Vertical pos. [μm]") -ax2.set_xlabel("BPM number") -ax3.set_ylabel("Strength (rad)") -ax3.set_xlabel("Steerer number") -fig.tight_layout() - -plt.show() diff --git a/examples/ESRF_ORM_example/measure_dispersion.py b/examples/ESRF_ORM_example/measure_dispersion.py deleted file mode 100644 index 249e16147..000000000 --- a/examples/ESRF_ORM_example/measure_dispersion.py +++ /dev/null @@ -1,30 +0,0 @@ -from pathlib import Path - -import matplotlib.pyplot as plt - -from pyaml.accelerator import Accelerator -from pyaml.common.constants import Action - -parent_folder = Path(__file__).parent -config_path = parent_folder.parent.parent.joinpath("tests", "config", "EBSOrbit.yaml").resolve() -sr = Accelerator.load(config_path) -ebs = sr.design - - -def callback(action: int, callback_data) -> bool: - if action == Action.APPLY: - print("Changing RF frequency") - elif action == Action.MEASURE: - print("Reading orbit.") - elif action == Action.RESTORE: - print("Restoring RF frequency.") - return True - - -ebs.dispersion.measure(callback=callback) -dispersion_data = ebs.dispersion.get() - -fig = plt.figure() -ax = fig.add_subplot(111) -ax.plot(dispersion_data["frequency_response_x"]) -plt.show() diff --git a/examples/ESRF_ORM_example/measure_ideal_ORM.py b/examples/ESRF_ORM_example/measure_ideal_ORM.py deleted file mode 100644 index 60efa03d3..000000000 --- a/examples/ESRF_ORM_example/measure_ideal_ORM.py +++ /dev/null @@ -1,17 +0,0 @@ -from pathlib import Path - -from pyaml.accelerator import Accelerator -from pyaml.tuning_tools.orbit_response_matrix import ConfigModel as ORM_ConfigModel -from pyaml.tuning_tools.orbit_response_matrix import OrbitResponseMatrix - -parent_folder = Path(__file__).parent -config_path = parent_folder.parent.parent.joinpath("tests", "config", "EBSOrbit.yaml").resolve() -sr = Accelerator.load(config_path) -ebs = sr.design - -if ebs.orm.measure(): - ebs.orm.save(parent_folder / Path("ideal_orm.json")) - ebs.orm.save(parent_folder / Path("ideal_orm.yaml"), with_type="yaml") - ebs.orm.save(parent_folder / Path("ideal_orm.npz"), with_type="npz") - -ormdata = ebs.orm.get() diff --git a/examples/ESRF_ORM_example/measure_ideal_ORM_and_disp.py b/examples/ESRF_ORM_example/measure_ideal_ORM_and_disp.py deleted file mode 100644 index c356a3c49..000000000 --- a/examples/ESRF_ORM_example/measure_ideal_ORM_and_disp.py +++ /dev/null @@ -1,24 +0,0 @@ -import json -from pathlib import Path - -import numpy as np - -from pyaml.accelerator import Accelerator - -parent_folder = Path(__file__).parent -config_path = parent_folder.parent.parent.joinpath("tests", "config", "EBSOrbit.yaml").resolve() -sr = Accelerator.load(config_path) - -ebs = sr.design - -ebs.orm.measure() -orm_data = ebs.orm.get() - -ebs.dispersion.measure() -dispersion_data = ebs.dispersion.get() - -rf_response = dispersion_data["frequency_response_x"] + dispersion_data["frequency_response_y"] - -orm_data["rf_response"] = rf_response - -ebs.orm.save("ideal_orm_disp.json") diff --git a/examples/ESRF_ORM_example/measure_reduced_ORM.py b/examples/ESRF_ORM_example/measure_reduced_ORM.py deleted file mode 100644 index 6bed127c6..000000000 --- a/examples/ESRF_ORM_example/measure_reduced_ORM.py +++ /dev/null @@ -1,51 +0,0 @@ -import logging -from pathlib import Path - -import numpy as np - -from pyaml.accelerator import Accelerator -from pyaml.common.constants import Action - -# disable printing during ORM measurement to illustrate callback. -logger = logging.getLogger("pyaml.tuning_tools.orbit_response_matrix").setLevel(logging.WARNING) - -parent_folder = Path(__file__).parent -config_path = parent_folder.parent.parent.joinpath("tests", "config", "EBSOrbit.yaml").resolve() -sr = Accelerator.load(config_path) -ebs = sr.design -orm = ebs.orm - -hcorr = ebs.get_magnets("HCorr") -vcorr = ebs.get_magnets("VCorr") -corrector_names = ( - hcorr["SJ2A*"].names() - + hcorr["SF2A*"].names() - + hcorr["SI2A*"].names() - + vcorr["SJ2A*"].names() - + vcorr["SF2A*"].names() - + vcorr["SI2A*"].names() -) - - -def callback(action: int, cdata): - if action == Action.RESTORE: - if "response_data" in cdata: - rdata = cdata["response_data"] - i = rdata.last_number - n_bpms = rdata.raw_up.shape[0] // 2 - n_correctors = rdata.raw_up.shape[1] - corrector = rdata.last_input - response = (rdata.raw_up[:, i] - rdata.raw_down[:, i]) / rdata.inputs_delta[i] - std_x_resp = np.std(response[:n_bpms]) - std_y_resp = np.std(response[n_bpms:]) - print( - f"[{i}/{n_correctors}], Measured response of {corrector}: " - f"r.m.s H.: {std_x_resp:.2f} mm/mrad, r.m.s. V: {std_y_resp:.2f} mm/mrad" - ) - return True - - -orm.measure(corrector_names=corrector_names, callback=callback) -orm.save(parent_folder / Path("reduced_orm.json")) - -ormdata = orm.get() diff --git a/examples/ESRF_ORM_example/scan_bpm_weight.py b/examples/ESRF_ORM_example/scan_bpm_weight.py deleted file mode 100644 index b8af7b530..000000000 --- a/examples/ESRF_ORM_example/scan_bpm_weight.py +++ /dev/null @@ -1,61 +0,0 @@ -import json -import logging -from pathlib import Path - -import matplotlib.pyplot as plt -import numpy as np - -from pyaml.accelerator import Accelerator -from pyaml.tuning_tools.orbit import ConfigModel as Orbit_ConfigModel -from pyaml.tuning_tools.orbit import Orbit - -parent_folder = Path(__file__).parent -pyaml_folder = parent_folder.parent.parent -config_path = pyaml_folder.joinpath("tests/config/EBSOrbit.yaml").resolve() -sr = Accelerator.load(config_path) -ebs = sr.design - -## get reference -ref_h, ref_v = ebs.get_bpms("BPM").positions.get().T -reference = np.concatenate((ref_h, ref_v)) -######################################################## - - -## generate some orbit -std_kick = 1e-6 -hcorr = ebs.get_magnets("HCorr") -vcorr = ebs.get_magnets("VCorr") -bpms = ebs.get_bpms("BPM") - -np.random.seed(1) -# mangle orbit -h0 = hcorr.strengths.get() + std_kick * np.random.normal(size=len(hcorr)) -v0 = vcorr.strengths.get() + std_kick * np.random.normal(size=len(vcorr)) - -my_bpm_name = "BPM_C04-05" -my_bpm = ebs.get_bpm(my_bpm_name) - -weights = np.linspace(0.01, 10, 40) -bpm_reading = np.zeros_like(weights) -ref_bpm_reading = my_bpm.positions.get()[0] -######################################################## -for i, w in enumerate(weights): - hcorr.strengths.set(h0) - vcorr.strengths.set(v0) - ebs.orbit.set_weight(my_bpm_name, w, plane="H") - - ebs.orbit.correct(singular_values_H=40, singular_values_V=40) - ebs.orbit.correct(singular_values_H=40, singular_values_V=40) - ebs.orbit.correct(singular_values_H=40, singular_values_V=40) - bpm_reading[i] = my_bpm.positions.get()[0] - -fig = plt.figure() -ax1 = fig.add_subplot(111) -ax1.plot(weights, bpm_reading * 1e6, ".") - - -ax1.set_ylabel("BPM reading [μm]") -ax1.set_xlabel("BPM weight") -fig.tight_layout() - -plt.show() diff --git a/examples/ESRF_ORM_example/scan_corrector_weight.py b/examples/ESRF_ORM_example/scan_corrector_weight.py deleted file mode 100644 index 5187e8d21..000000000 --- a/examples/ESRF_ORM_example/scan_corrector_weight.py +++ /dev/null @@ -1,60 +0,0 @@ -import json -import logging -from pathlib import Path - -import matplotlib.pyplot as plt -import numpy as np - -from pyaml.accelerator import Accelerator -from pyaml.tuning_tools.orbit import ConfigModel as Orbit_ConfigModel -from pyaml.tuning_tools.orbit import Orbit - -parent_folder = Path(__file__).parent -pyaml_folder = parent_folder.parent.parent -config_path = pyaml_folder.joinpath("tests/config/EBSOrbit.yaml").resolve() -sr = Accelerator.load(config_path) -ebs = sr.design - -## get reference -ref_h, ref_v = ebs.get_bpms("BPM").positions.get().T -reference = np.concatenate((ref_h, ref_v)) -######################################################## - - -## generate some orbit -std_kick = 1e-6 -hcorr = ebs.get_magnets("HCorr") -vcorr = ebs.get_magnets("VCorr") -bpms = ebs.get_bpms("BPM") - -np.random.seed(1) -# mangle orbit -h0 = hcorr.strengths.get() + std_kick * np.random.normal(size=len(hcorr)) -v0 = vcorr.strengths.get() + std_kick * np.random.normal(size=len(vcorr)) - -my_corr_name = "SJ2A-C04-H" -my_corr = ebs.get_magnet(my_corr_name) - - -weights = np.linspace(0.01, 2, 100) -corr_settings = np.zeros_like(weights) -######################################################## -for i, w in enumerate(weights): - hcorr.strengths.set(h0) - my_corr.strength.set(0) - vcorr.strengths.set(v0) - ebs.orbit.set_weight(my_corr_name, w) - - ebs.orbit.correct(reference=reference) - corr_settings[i] = my_corr.strength.get() - -fig = plt.figure() -ax1 = fig.add_subplot(111) -ax1.plot(weights, corr_settings * 1e6, ".") - - -ax1.set_ylabel("Corrector setting [μrad]") -ax1.set_xlabel("Corrector weight") -fig.tight_layout() - -plt.show() diff --git a/examples/ESRF_tune_example/README.md b/examples/ESRF_tune_example/README.md deleted file mode 100644 index f0bfdc2e5..000000000 --- a/examples/ESRF_tune_example/README.md +++ /dev/null @@ -1,61 +0,0 @@ -# Instructions for how to run the ESRF Tune example. - -## Install pyAML - -1. Create a virtual environment and activate it. It needs to have >= Python 3.11. - -2. Install pyAML including the tango bindings. - - ```bash - pip install accelerator-middle-layer[tango] - ``` - -3. install EBS dummy Control system. This is valid untill an ESRF virtual machine will be available as for BESSYII and SOLEIL - ```bash - pip install tests/dummy_cs/tango-pyaml - ``` - - ## Run the examples - Two examples are available for tune correction. - The esrf_tune_example.py shows the standard usage - The esrf_tune_example_no_yaml.py shows the same but without using configuration file. - - To run the examples: - 1. navigate to the pyaml root directory - 2. Download (or clone) the example files. - 3. run the files - - ## expected output of esrf_tune_example.py for SR.design is - - 30 Jan 2026, 09:23:13 | WARNING | PyAML Tango control system binding (0.3.2) initialized with name 'live' and TANGO_HOST=ebs-simu-3:10000 - Tune response: #0 QD2E-C04 [ 0.17851726 -1.25993589] - Tune response: #1 QD2A-C05 [ 0.17889514 -1.25969115] - ... - Tune response: #123 QF1A-C03 [ 0.59069308 -0.49430245] - Initial tune: [0.16000001 0.33999986] - Final tune: [0.17 0.32] - - - ## expected output of esrf_tune_example.py for SR.live is - Initial tune: [0. 0.] - MultiAttribute.get(124 values) - MultiAttribute.get(124 values) - MultiAttribute.set(124 values) - //ebs-simu-3:10000/srmag/vps-qd2/c04-e/current:0.8688600876142427 - ... - //ebs-simu-3:10000/srmag/vps-qf1/c02-e/current:1.3024074153237937 - //ebs-simu-3:10000/srmag/vps-qf1/c03-a/current:1.2966875742108155 - Final tune: [0. 0.] - - ## expected output of: esrf_tune_example_no_yaml.py - - Creating dummy TangoControlSystem: live - Tune=Value(0.0, quality='VALID',timestamp='2026-01-30 10:14:20.685681'), Value(0.0, quality='VALID',timestamp='2026-01-30 10:14:20.685764') - MultiAttribute.get(4 values) - MultiAttribute.get(4 values) - MultiAttribute.set(4 values) - //ebs-simu-3:10000/srmag/vps-qf1/c01-a/current:9.77449643229055 - //ebs-simu-3:10000/srmag/vps-qf1/c01-e/current:9.724114177375114 - //ebs-simu-3:10000/srmag/vps-qd2/c01-a/current:7.785894751522811 - //ebs-simu-3:10000/srmag/vps-qd2/c01-e/current:7.778613675036138 - Tune=Value(0.0, quality='VALID',timestamp='2026-01-30 10:14:23.686925'), Value(0.0, quality='VALID',timestamp='2026-01-30 10:14:23.686994') diff --git a/examples/ESRF_tune_example/esrf_tune_example.py b/examples/ESRF_tune_example/esrf_tune_example.py deleted file mode 100644 index 4b3bd5c9d..000000000 --- a/examples/ESRF_tune_example/esrf_tune_example.py +++ /dev/null @@ -1,36 +0,0 @@ -import os - -import numpy as np - -from pyaml.accelerator import Accelerator -from pyaml.common.constants import ACTION_RESTORE -from pyaml.magnet.magnet import Magnet - -sr: Accelerator = Accelerator.load("./tests/config/EBSTune.yaml") -sr.design.get_lattice().disable_6d() - -# switch script from live to design -# sr.design acts on simulations sr.live to act on real machine -SR = sr.live - - -# Callback exectued after each magnet strenght setting -# during the tune response matrix measurement -def tune_callback(step: int, action: int, m: Magnet, dtune: np.array): - if action == ACTION_RESTORE: - # On action restore, the delta tune is passed as argument - print(f"Tune response: #{step} {m.get_name()} {dtune}") - return True - - -# Compute tune response matrix -tune_adjust_design = sr.design.tune -tune_adjust_design.response.measure(callback=tune_callback) -tune_adjust_design.response.save_json("tunemat.json") - -# Correct tune on live or design -tune_adjust = SR.tune -tune_adjust.response.load_json("tunemat.json") -print(f"Initial tune: {tune_adjust.readback()}") -tune_adjust.set([0.17, 0.32], iter=2, wait_time=10) -print(f"Final tune: {tune_adjust.readback()}") diff --git a/examples/ESRF_tune_example/esrf_tune_example_no_yaml.py b/examples/ESRF_tune_example/esrf_tune_example_no_yaml.py deleted file mode 100644 index 0296b04f1..000000000 --- a/examples/ESRF_tune_example/esrf_tune_example_no_yaml.py +++ /dev/null @@ -1,154 +0,0 @@ -import os -import time - -import numpy as np -from tango.pyaml.attribute import Attribute -from tango.pyaml.attribute import ConfigModel as AttributeConfig -from tango.pyaml.attribute_read_only import ( - AttributeReadOnly, -) -from tango.pyaml.attribute_read_only import ( - ConfigModel as AttributeReadOnlyConfig, -) -from tango.pyaml.controlsystem import ( - ConfigModel as ControlSystemConfig, -) -from tango.pyaml.controlsystem import ( - TangoControlSystem, -) - -from pyaml.accelerator import Accelerator -from pyaml.accelerator import ConfigModel as AcceleratorConfigModel -from pyaml.arrays.magnet import ConfigModel as MagnetArrayConfigModel -from pyaml.arrays.magnet import Magnet -from pyaml.configuration import set_root_folder -from pyaml.configuration.csvcurve import ConfigModel as CSVCureveConfig -from pyaml.configuration.csvcurve import CSVCurve -from pyaml.lattice.simulator import ConfigModel as SimulatorConfigModel -from pyaml.lattice.simulator import Simulator -from pyaml.magnet.linear_model import ( - ConfigModel as LinearMagnetModelConfig, -) -from pyaml.magnet.linear_model import ( - LinearMagnetModel, -) -from pyaml.magnet.quadrupole import ConfigModel as QuadrupoleConfig -from pyaml.magnet.quadrupole import Quadrupole - -# Get the directory of the current script -script_dir = os.path.dirname(__file__) - -# Go up one level and then into 'data' -relative_path = os.path.join(script_dir, "..", "..", "tests") - -# Normalize the path (resolves '..') -absolute_path = os.path.abspath(relative_path) - -set_root_folder(absolute_path) - -# Configuration - -tangocs = ControlSystemConfig(name="live", tango_host="ebs-simu-3:10000") -control = TangoControlSystem(tangocs) - -qfCurve = CSVCurve(CSVCureveConfig(file="config/sr/magnet_models/QF1_strength.csv")) -qdCurve = CSVCurve(CSVCureveConfig(file="config/sr/magnet_models/QD2_strength.csv")) - -elemConfig = [ - { - "name": "QF1A-C01", - "attname": "srmag/vps-qf1/c01-a/current", - "calibration_factor": 1.00504, - "curve": qfCurve, - }, - { - "name": "QF1E-C01", - "attname": "srmag/vps-qf1/c01-e/current", - "calibration_factor": 0.998212, - "curve": qfCurve, - }, - { - "name": "QD2A-C01", - "attname": "srmag/vps-qd2/c01-a/current", - "calibration_factor": 1.00504, - "curve": qdCurve, - }, - { - "name": "QD2E-C01", - "attname": "srmag/vps-qd2/c01-e/current", - "calibration_factor": 1.003485189, - "curve": qdCurve, - }, -] - -devices = [] -names = [] -for cfg in elemConfig: - qAtt = Attribute(AttributeConfig(attribute=cfg["attname"], unit="A")) - qModel = LinearMagnetModel( - LinearMagnetModelConfig( - curve=cfg["curve"], - calibration_factor=cfg["calibration_factor"], - powerconverter=qAtt, - unit="1/m", - ) - ) - devices.append(Quadrupole(QuadrupoleConfig(name=cfg["name"], model=qModel))) - names.append(cfg["name"]) - - -simulator = Simulator(SimulatorConfigModel(name="design", lattice="config/sr/lattices/ebs.mat")) - -quads = Magnet(MagnetArrayConfigModel(name="quadsForTune", elements=names)) - -sr = Accelerator( - AcceleratorConfigModel( - machine="sr", - facility="ESRF", - energy=6e9, - controls=[control], - simulators=[simulator], - devices=devices, - arrays=[quads], - data_folder="/tmp", - ) -) - - -# Usage exmaple - -quadForTuneDesign = sr.design.get_magnets("quadsForTune") -quadForTuneLive = sr.live.get_magnets("quadsForTune") - -# Compute tune response matrix for the 4 quads from simulator -sr.design.get_lattice().disable_6d() -tune = sr.design.get_lattice().get_tune() -tunemat = np.zeros((len(quadForTuneDesign), 2)) -for idx, m in enumerate(quadForTuneDesign): - str = m.strength.get() - m.strength.set(str + 1e-4) - dq = sr.design.get_lattice().get_tune() - tune - tunemat[idx] = dq * 1e4 - m.strength.set(str) - -# Compute correction matrix -correctionmat = np.linalg.pinv(tunemat.T) - -# Correct tune on live - -# Here ,as an example, instead of using the betatron tune monitor object, -# we directly connect to th CS -qxAtt, qyAtt = control.attach( - [ - AttributeReadOnly(AttributeReadOnlyConfig(attribute="sys/ringsimulator/ebs/Tune_h", unit="")), - AttributeReadOnly(AttributeReadOnlyConfig(attribute="sys/ringsimulator/ebs/Tune_v", unit="")), - ] -) - -print(f"Tune={qxAtt.readback()}, {qyAtt.readback()}") - -strs = quadForTuneLive.strengths.get() -strs += np.matmul(correctionmat, [0.1, 0.05]) # Ask for correction [dqx,dqy] -quadForTuneLive.strengths.set(strs) -time.sleep(3) -print(f"Tune={qxAtt.readback()}, {qyAtt.readback()}") diff --git a/examples/SOLEIL_examples/01-SOLEIL_II_tune_example.ipynb b/examples/SOLEIL_examples/01-SOLEIL_II_tune_example.ipynb deleted file mode 100644 index f49b94b2d..000000000 --- a/examples/SOLEIL_examples/01-SOLEIL_II_tune_example.ipynb +++ /dev/null @@ -1,671 +0,0 @@ -{ - "cells": [ - { - "cell_type": "code", - "execution_count": 1, - "id": "11bf6fa5-1b3c-4283-a4bc-cb27bac2e988", - "metadata": {}, - "outputs": [], - "source": [ - "import os\n", - "\n", - "import matplotlib.pyplot as plt\n", - "import numpy as np\n", - "\n", - "from pyaml.accelerator import Accelerator\n", - "from pyaml.common.constants import Action\n", - "from pyaml.magnet.magnet import Magnet" - ] - }, - { - "cell_type": "markdown", - "id": "74299a03-49fe-4efe-a66b-3e21bc9feb05", - "metadata": {}, - "source": [ - "### Virtual accelerator setup for emulation of a control system\n", - "For the **live** control mode, you should have some control system emulation running. \n", - "\n", - "!!! *If you want to skip this, you can always run the notebook in **design** mode.* !!!\n", - "\n", - "For the installation you should be able to do \n", - "```\n", - "apptainer pull virtual-accelerator.sif oras://gitlab-registry.synchrotron-soleil.fr/software-control-system/containers/apptainer/virtual-accelerator:latest\n", - "apptainer run virtual-accelerator.sif\n", - "```\n", - "This will run SOLEIL II proof-of-concept digital twin on localhost:11000. You can play with the digital twin itself (without pyAML) via Jive to check that everything is working. You can run Jive in a different terminal with \n", - "```\n", - "apptainer pull jive.sif https://gitlab.synchrotron-soleil.fr/api/v4/projects/2739/packages/generic/jive/latest/jive.sif\n", - "apptainer run jive.sif\n", - "```\n", - "On linux you may additionally configure X11\n", - "```\n", - "export DISPLAY=:0\n", - "xhost +local:root\n", - "```\n", - "Jive is not necessary to run anything but some of you may find it useful to open its `simulator/ringsimulator/ringsimulator` device on the side and see how the global parameters (tune, orbit, chromaticity, etc.) change with your actions in pyAML.\n", - "NOTE: This notebook is just a demonstration of pyAML functionality. Certain things may be done stupidly. The person who wrote this jupyter notebook only cared about showing that the code is working, not about intelligently controlling the accelerator." - ] - }, - { - "cell_type": "code", - "execution_count": 2, - "id": "5a5aa924-ffcd-4aba-a0c2-fb9e4955eb58", - "metadata": {}, - "outputs": [ - { - "name": "stderr", - "output_type": "stream", - "text": [ - "PyAML Tango control system binding (0.3.3) initialized with name 'live' and TANGO_HOST=localhost:11000\n" - ] - }, - { - "data": { - "text/plain": [ - "Accelerator(facility='Synchrotron SOLEIL', machine='sr', energy=2750000000.0, alphac=None, harmonic_number=None, controls=[TangoControlSystem(name='live', tango_host='localhost:11000', debug_level=None, lazy_devices=True, scalar_aggregator='tango.pyaml.multi_attribute', vector_aggregator=None, timeout_ms=3000)], simulators=[Simulator(name='design', lattice='/home/gubaidulin/codes/operation/pyAML/pyaml/examples/SOLEIL_examples/SOLEIL_II_V3631_sym1_V001_database_rf.m', mat_key=None, linker=, description=None)], data_folder='/data/store', description=None)" - ] - }, - "execution_count": 2, - "metadata": {}, - "output_type": "execute_result" - } - ], - "source": [ - "sr = Accelerator.load(\"p.yaml\")\n", - "sr # string representation" - ] - }, - { - "cell_type": "markdown", - "id": "a55eb5f7-7c5f-4a37-96e8-f9b6be67ede6", - "metadata": {}, - "source": [ - "### Control mode choice\n", - "You can choose either sr.live control mode or sr.design control mode\n", - "- **sr.live** is intended for use with control system either digital twin or a real accelerator\n", - "- **sr.design** will just run pyAT without any control system \n", - " \n", - "In this notebook with **sr.design** you can put all wait times to zero or some negligible value. In **sr.live** mode, a wait time of 1.5 seconds is necessary becausethe digital twin is updating every 0.5-1 second." - ] - }, - { - "cell_type": "code", - "execution_count": 3, - "id": "4316ad34-f146-442f-9250-8a750cf6f562", - "metadata": {}, - "outputs": [ - { - "data": { - "text/plain": [ - "Simulator(name='design', lattice='/home/gubaidulin/codes/operation/pyAML/pyaml/examples/SOLEIL_examples/SOLEIL_II_V3631_sym1_V001_database_rf.m', mat_key=None, linker=, description=None)" - ] - }, - "execution_count": 3, - "metadata": {}, - "output_type": "execute_result" - } - ], - "source": [ - "control_mode = sr.design\n", - "wait_time = 0 if control_mode == sr.design else 2.0\n", - "control_mode # string representation" - ] - }, - { - "cell_type": "markdown", - "id": "be59ab58-7662-4e46-a22f-00b134d22d45", - "metadata": {}, - "source": [ - "#### Accessing betatron tune monitor / diagnostics\n", - "Betatron tune monitor object is already defined near the end of the configuration file with a name \"BETATRON_TUNE\"." - ] - }, - { - "cell_type": "code", - "execution_count": 4, - "id": "9881f93b-68c1-41c9-b67d-0db5f9f4571c", - "metadata": {}, - "outputs": [ - { - "name": "stdout", - "output_type": "stream", - "text": [ - "[0.20136665 0.30000589]\n" - ] - }, - { - "data": { - "text/plain": [ - "BetatronTuneMonitor(peer='Simulator:design', name='BETATRON_TUNE', description=None, lattice_names=None, tune_h=AttributeReadOnly(attribute='simulator/ringsimulator/ringsimulator/Tune_h', unit='', range=None), tune_v=AttributeReadOnly(attribute='simulator/ringsimulator/ringsimulator/Tune_v', unit='', range=None), rf_plant_name=None)" - ] - }, - "execution_count": 4, - "metadata": {}, - "output_type": "execute_result" - } - ], - "source": [ - "tune_monitor = control_mode.get_betatron_tune_monitor(\"BETATRON_TUNE\")\n", - "print(tune_monitor.tune.get())\n", - "tune_monitor # string representation" - ] - }, - { - "cell_type": "markdown", - "id": "9ab82b92-d891-45e7-aaab-f6efc313bd1f", - "metadata": {}, - "source": [ - "#### Accessing quadrupolar correctors available in the ring\n", - "The configuration file already has a \"QCORR\" array of magnets defined. get_magnets() method will return a list of magnets. In this notebook we will control each of the correctors individually. " - ] - }, - { - "cell_type": "code", - "execution_count": 5, - "id": "49e98106-dcd3-41f3-861a-a5bdac997ec9", - "metadata": {}, - "outputs": [ - { - "name": "stdout", - "output_type": "stream", - "text": [ - "The ring has 208 quadrupolar correctors. The first one is named QCORR_001 (lattice name).\n" - ] - }, - { - "data": { - "text/plain": [ - "Quadrupole(peer='Simulator:design', name='QCORR_001', model_name='QCORR_001', magnet_model=IdentityMagnetModel(powerconverter=None, physics=Attribute(attribute='AN01-AR/EM-COR/CQLN.03/strength', unit='1/m', range=None), unit='1/m'))" - ] - }, - "execution_count": 5, - "metadata": {}, - "output_type": "execute_result" - } - ], - "source": [ - "qcorrectors = control_mode.get_magnets(\"QCORR\")\n", - "first_qcorrector = qcorrectors[0]\n", - "print(\n", - " f\"The ring has {len(qcorrectors)} quadrupolar correctors. \"\n", - " f\"The first one is named {first_qcorrector.get_name()} (lattice name).\"\n", - ")\n", - "qcorrectors[0] # String representation of the first corrector" - ] - }, - { - "cell_type": "code", - "execution_count": 6, - "id": "0b945d5d-09c9-48eb-a1e9-a8dbec2e76b8", - "metadata": {}, - "outputs": [ - { - "name": "stdout", - "output_type": "stream", - "text": [ - "We can access the strength of the corrector qcorrectors[0].strength.get()=0.00,we can set it to some value with qcorrectors[0].strength.set(0.2)\n", - "Let's check that the readback is what we asked for qcorrectors[0].strength.get()=0.20, \n" - ] - } - ], - "source": [ - "print(\n", - " f\"We can access the strength of the corrector {qcorrectors[0].strength.get()=:.2f},\"\n", - " f\"we can set it to some value with qcorrectors[0].strength.set(0.2)\"\n", - ")\n", - "qcorrectors[0].strength.set(0.2)\n", - "print(f\"Let's check that the readback is what we asked for {qcorrectors[0].strength.get()=:.2f}, \")\n", - "qcorrectors[0].strength.set(0) # setting back to original value" - ] - }, - { - "cell_type": "markdown", - "id": "fda45408-f7c2-4bc0-a985-55fab65b6307", - "metadata": {}, - "source": [ - "### Standard tuning tool for tune correction\n", - "The standard tuning tool for tune correction can be accessed by name \"DEFAULT_TUNE_CORRECTION\". At the same time, this default tune correction can be accessed as a property of a control mode." - ] - }, - { - "cell_type": "code", - "execution_count": 7, - "id": "78ea33ac-fc9d-4943-bdde-694e5f8ce3cf", - "metadata": {}, - "outputs": [ - { - "data": { - "text/plain": [ - "(Tune(peer='Simulator:design', name='DEFAULT_TUNE_CORRECTION', description=None, lattice_names=None, quad_array_name='QCORR', betatron_tune_name='BETATRON_TUNE', response_matrix=ResponseMatrixData(matrix=[[0.1411063797665535, 0.12507210547463288, 0.1250701156868539, 0.12512631205885416, 0.12491874479825249, 0.12181775238373493, 0.1216597552561316, 0.1248778676887774, 0.12495669600987025, 0.12487669303812288, 0.12509619715300735, 0.2525199827177471, 0.2521390414436664, 0.1248823477056904, 0.12498317129350234, 0.12489821923894473, 0.1251142031252761, 0.23389597347489577, 0.5128470461415735, 0.511903112678791, 0.23349704327907395, 0.1248680305476757, 0.12499101129714862, 0.12490278089832829, 0.12510881390703776, 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'QCORR_053', 'QCORR_054', 'QCORR_055', 'QCORR_056', 'QCORR_057', 'QCORR_058', 'QCORR_059', 'QCORR_060', 'QCORR_061', 'QCORR_062', 'QCORR_063', 'QCORR_064', 'QCORR_065', 'QCORR_066', 'QCORR_067', 'QCORR_068', 'QCORR_069', 'QCORR_070', 'QCORR_071', 'QCORR_072', 'QCORR_073', 'QCORR_074', 'QCORR_075', 'QCORR_076', 'QCORR_077', 'QCORR_078', 'QCORR_079', 'QCORR_080', 'QCORR_081', 'QCORR_082', 'QCORR_083', 'QCORR_084', 'QCORR_085', 'QCORR_086', 'QCORR_087', 'QCORR_088', 'QCORR_089', 'QCORR_090', 'QCORR_091', 'QCORR_092', 'QCORR_093', 'QCORR_094', 'QCORR_095', 'QCORR_096', 'QCORR_097', 'QCORR_098', 'QCORR_099', 'QCORR_100', 'QCORR_101', 'QCORR_102', 'QCORR_103', 'QCORR_104', 'QCORR_105', 'QCORR_106', 'QCORR_107', 'QCORR_108', 'QCORR_109', 'QCORR_110', 'QCORR_111', 'QCORR_112', 'QCORR_113', 'QCORR_114', 'QCORR_115', 'QCORR_116', 'QCORR_117', 'QCORR_118', 'QCORR_119', 'QCORR_120', 'QCORR_121', 'QCORR_122', 'QCORR_123', 'QCORR_124', 'QCORR_125', 'QCORR_126', 'QCORR_127', 'QCORR_128', 'QCORR_129', 'QCORR_130', 'QCORR_131', 'QCORR_132', 'QCORR_133', 'QCORR_134', 'QCORR_135', 'QCORR_136', 'QCORR_137', 'QCORR_138', 'QCORR_139', 'QCORR_140', 'QCORR_141', 'QCORR_142', 'QCORR_143', 'QCORR_144', 'QCORR_145', 'QCORR_146', 'QCORR_147', 'QCORR_148', 'QCORR_149', 'QCORR_150', 'QCORR_151', 'QCORR_152', 'QCORR_153', 'QCORR_154', 'QCORR_155', 'QCORR_156', 'QCORR_157', 'QCORR_158', 'QCORR_159', 'QCORR_160', 'QCORR_161', 'QCORR_162', 'QCORR_163', 'QCORR_164', 'QCORR_165', 'QCORR_166', 'QCORR_167', 'QCORR_168', 'QCORR_169', 'QCORR_170', 'QCORR_171', 'QCORR_172', 'QCORR_173', 'QCORR_174', 'QCORR_175', 'QCORR_176', 'QCORR_177', 'QCORR_178', 'QCORR_179', 'QCORR_180', 'QCORR_181', 'QCORR_182', 'QCORR_183', 'QCORR_184', 'QCORR_185', 'QCORR_186', 'QCORR_187', 'QCORR_188', 'QCORR_189', 'QCORR_190', 'QCORR_191', 'QCORR_192', 'QCORR_193', 'QCORR_194', 'QCORR_195', 'QCORR_196', 'QCORR_197', 'QCORR_198', 'QCORR_199', 'QCORR_200', 'QCORR_201', 'QCORR_202', 'QCORR_203', 'QCORR_204', 'QCORR_205', 'QCORR_206', 'QCORR_207', 'QCORR_208'], observable_names=['BETATRON_TUNE.x', 'BETATRON_TUNE.y'])),\n", - " Tune(peer='Simulator:design', name='DEFAULT_TUNE_CORRECTION', description=None, lattice_names=None, quad_array_name='QCORR', betatron_tune_name='BETATRON_TUNE', response_matrix=ResponseMatrixData(matrix=[[0.1411063797665535, 0.12507210547463288, 0.1250701156868539, 0.12512631205885416, 0.12491874479825249, 0.12181775238373493, 0.1216597552561316, 0.1248778676887774, 0.12495669600987025, 0.12487669303812288, 0.12509619715300735, 0.2525199827177471, 0.2521390414436664, 0.1248823477056904, 0.12498317129350234, 0.12489821923894473, 0.1251142031252761, 0.23389597347489577, 0.5128470461415735, 0.511903112678791, 0.23349704327907395, 0.1248680305476757, 0.12499101129714862, 0.12490278089832829, 0.12510881390703776, 0.12183894919831628, 0.1218854100140665, 0.12512083453292133, 0.12495265783368792, 0.12504788875794537, 0.12486094618291421, 0.23342131651754583, 0.5117652399105888, 0.5128123399564255, 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'QCORR_066', 'QCORR_067', 'QCORR_068', 'QCORR_069', 'QCORR_070', 'QCORR_071', 'QCORR_072', 'QCORR_073', 'QCORR_074', 'QCORR_075', 'QCORR_076', 'QCORR_077', 'QCORR_078', 'QCORR_079', 'QCORR_080', 'QCORR_081', 'QCORR_082', 'QCORR_083', 'QCORR_084', 'QCORR_085', 'QCORR_086', 'QCORR_087', 'QCORR_088', 'QCORR_089', 'QCORR_090', 'QCORR_091', 'QCORR_092', 'QCORR_093', 'QCORR_094', 'QCORR_095', 'QCORR_096', 'QCORR_097', 'QCORR_098', 'QCORR_099', 'QCORR_100', 'QCORR_101', 'QCORR_102', 'QCORR_103', 'QCORR_104', 'QCORR_105', 'QCORR_106', 'QCORR_107', 'QCORR_108', 'QCORR_109', 'QCORR_110', 'QCORR_111', 'QCORR_112', 'QCORR_113', 'QCORR_114', 'QCORR_115', 'QCORR_116', 'QCORR_117', 'QCORR_118', 'QCORR_119', 'QCORR_120', 'QCORR_121', 'QCORR_122', 'QCORR_123', 'QCORR_124', 'QCORR_125', 'QCORR_126', 'QCORR_127', 'QCORR_128', 'QCORR_129', 'QCORR_130', 'QCORR_131', 'QCORR_132', 'QCORR_133', 'QCORR_134', 'QCORR_135', 'QCORR_136', 'QCORR_137', 'QCORR_138', 'QCORR_139', 'QCORR_140', 'QCORR_141', 'QCORR_142', 'QCORR_143', 'QCORR_144', 'QCORR_145', 'QCORR_146', 'QCORR_147', 'QCORR_148', 'QCORR_149', 'QCORR_150', 'QCORR_151', 'QCORR_152', 'QCORR_153', 'QCORR_154', 'QCORR_155', 'QCORR_156', 'QCORR_157', 'QCORR_158', 'QCORR_159', 'QCORR_160', 'QCORR_161', 'QCORR_162', 'QCORR_163', 'QCORR_164', 'QCORR_165', 'QCORR_166', 'QCORR_167', 'QCORR_168', 'QCORR_169', 'QCORR_170', 'QCORR_171', 'QCORR_172', 'QCORR_173', 'QCORR_174', 'QCORR_175', 'QCORR_176', 'QCORR_177', 'QCORR_178', 'QCORR_179', 'QCORR_180', 'QCORR_181', 'QCORR_182', 'QCORR_183', 'QCORR_184', 'QCORR_185', 'QCORR_186', 'QCORR_187', 'QCORR_188', 'QCORR_189', 'QCORR_190', 'QCORR_191', 'QCORR_192', 'QCORR_193', 'QCORR_194', 'QCORR_195', 'QCORR_196', 'QCORR_197', 'QCORR_198', 'QCORR_199', 'QCORR_200', 'QCORR_201', 'QCORR_202', 'QCORR_203', 'QCORR_204', 'QCORR_205', 'QCORR_206', 'QCORR_207', 'QCORR_208'], observable_names=['BETATRON_TUNE.x', 'BETATRON_TUNE.y'])))" - ] - }, - "execution_count": 7, - "metadata": {}, - "output_type": "execute_result" - } - ], - "source": [ - "tune_correction = control_mode.get_tune_tuning(\"DEFAULT_TUNE_CORRECTION\")\n", - "tune_response_matrix = control_mode.get_trm_tuning(\"DEFAULT_TUNE_RESPONSE_MATRIX\")\n", - "control_mode.tune, tune_correction # string representation" - ] - }, - { - "cell_type": "markdown", - "id": "d5abc174-b21c-4407-89a5-a2ef3f3f5121", - "metadata": {}, - "source": [ - "Let's try to set the tune using the tune correction tool. This will not be possible because no response matrix is defined at the moment. The response matrix can either be loaded from a file or measured. You can also measure the response matrix in **design** mode and try to use in in **live** mode." - ] - }, - { - "cell_type": "code", - "execution_count": 8, - "id": "e848371d-90d5-4bbe-a034-66eb21d39d0c", - "metadata": {}, - "outputs": [], - "source": [ - "from pyaml import PyAMLException\n", - "\n", - "try:\n", - " tune_correction.set([0.21, 0.31])\n", - "except PyAMLException as e:\n", - " print(f\"We've got an exception (this is intended) throwing the following error: {e}\")" - ] - }, - { - "cell_type": "markdown", - "id": "8c2eef19-8fdb-4297-99aa-3be44f78085b", - "metadata": {}, - "source": [ - "It is not possible to do so without measuring the response matrix (or loading it from a file). In the properties of the tune_correction, we can find a TuneResponse object with a measure() method. However, before doing that, we can define a callback that will print progress during the measurement. The measurement will take a while because of the 1.5-second wait time necessary to get a response from the virtual accelerator. You can try to change this and see what the minimal response time is for your hardware." - ] - }, - { - "cell_type": "code", - "execution_count": 9, - "id": "72bcf013-c4a6-4695-9029-b899a53753bd", - "metadata": {}, - "outputs": [], - "source": [ - "def tune_callback(action: int, cb_data: dict):\n", - " if action == Action.MEASURE:\n", - " # On action measure, the measured dq / dk is passed as argument\n", - " print(f\"Tune response: #{cb_data['step']} {cb_data['magnet']} {cb_data['tune']}\")\n", - " return True" - ] - }, - { - "cell_type": "code", - "execution_count": 10, - "id": "d4712e98-a75a-41ae-8d11-18c3bee23a2a", - "metadata": {}, - "outputs": [ - { - "name": "stdout", - "output_type": "stream", - "text": [ - "Tune response: #0 QCORR_001 [0.20999869 0.31007803]\n", - "Tune response: #0 QCORR_002 [0.21000032 0.3099983 ]\n", - "Tune response: #0 QCORR_003 [0.21000032 0.30999821]\n", - "Tune response: #0 QCORR_004 [0.21000033 0.30999836]\n", - "Tune response: #0 QCORR_005 [0.21000028 0.30999852]\n", - "Tune response: #0 QCORR_006 [0.21000063 0.30999949]\n", - "Tune response: #0 QCORR_007 [0.21000059 0.30999965]\n", - "Tune response: #0 QCORR_008 [0.21000027 0.30999937]\n", - "Tune response: #0 QCORR_009 [0.21000029 0.30999928]\n", - "Tune response: #0 QCORR_010 [0.21000027 0.30999875]\n", - "Tune response: #0 QCORR_011 [0.21000032 0.30999855]\n", - "Tune response: #0 QCORR_012 [0.20998764 0.31000773]\n", - "Tune response: #0 QCORR_013 [0.20998752 0.31000836]\n", - "Tune response: #0 QCORR_014 [0.21000026 0.30999826]\n", - "Tune response: #0 QCORR_015 [0.2100003 0.30999826]\n", - "Tune response: #0 QCORR_016 [0.21000027 0.30999861]\n", - "Tune response: #0 QCORR_017 [0.21000034 0.30999879]\n", - "Tune response: #0 QCORR_018 [0.20998951 0.31000508]\n", - "Tune response: #0 QCORR_019 [0.20996175 0.30998492]\n", - "Tune response: #0 QCORR_020 [0.20996109 0.30998432]\n", - "Tune response: #0 QCORR_021 [0.20998923 0.31000411]\n", - "Tune response: #0 QCORR_022 [0.21000016 0.30999932]\n", - "Tune response: #0 QCORR_023 [0.21000034 0.30999948]\n", - "Tune response: #0 QCORR_024 [0.21000025 0.30999947]\n", - "Tune response: #0 QCORR_025 [0.21000043 0.30999931]\n", - "Tune response: #0 QCORR_026 [0.21000071 0.30999897]\n", - "Tune response: #0 QCORR_027 [0.21000068 0.30999873]\n", - "Tune response: #0 QCORR_028 [0.21000043 0.30999804]\n", - "Tune response: #0 QCORR_029 [0.21000021 0.3099981 ]\n", - "Tune response: #0 QCORR_030 [0.21000031 0.30999867]\n", - "Tune response: #0 QCORR_031 [0.21000017 0.30999893]\n", - "Tune response: #0 QCORR_032 [0.20998928 0.31000532]\n", - "Tune response: #0 QCORR_033 [0.20996117 0.30998503]\n", - "Tune response: #0 QCORR_034 [0.20996177 0.30998437]\n", - "Tune response: #0 QCORR_035 [0.20998953 0.31000427]\n", - "Tune response: #0 QCORR_036 [0.21000032 0.30999958]\n", - "Tune response: #0 QCORR_037 [0.21000024 0.30999972]\n", - "Tune response: #0 QCORR_038 [0.21000026 0.30999956]\n", - "Tune response: #0 QCORR_039 [0.21000027 0.30999931]\n", - "Tune response: #0 QCORR_040 [0.20998938 0.3100065 ]\n", - "Tune response: #0 QCORR_041 [0.20998945 0.31000791]\n", - "Tune response: #0 QCORR_042 [0.21000031 0.30999852]\n", - "Tune response: #0 QCORR_043 [0.21000025 0.30999826]\n", - "Tune response: #0 QCORR_044 [0.21000025 0.30999793]\n", - "Tune response: #0 QCORR_045 [0.21000029 0.30999801]\n", - "Tune response: #0 QCORR_046 [0.21000057 0.30999907]\n", - "Tune response: #0 QCORR_047 [0.21000066 0.30999938]\n", - "Tune response: #0 QCORR_048 [0.21000031 0.30999963]\n", - "Tune response: #0 QCORR_049 [0.21000035 0.30999969]\n", - "Tune response: #0 QCORR_050 [0.21000035 0.30999929]\n", - "Tune response: #0 QCORR_051 [0.2100003 0.30999901]\n", - "Tune response: #0 QCORR_052 [0.21000456 0.31002779]\n", - "Tune response: #0 QCORR_053 [0.21000457 0.31002753]\n", - "Tune response: #0 QCORR_054 [0.21000032 0.30999882]\n", - "Tune response: #0 QCORR_055 [0.21000034 0.30999912]\n", - "Tune response: #0 QCORR_056 [0.21000036 0.30999969]\n", - "Tune response: #0 QCORR_057 [0.21000029 0.30999971]\n", - "Tune response: #0 QCORR_058 [0.21000065 0.30999958]\n", - "Tune response: #0 QCORR_059 [0.21000057 0.30999927]\n", - "Tune response: #0 QCORR_060 [0.21000027 0.30999809]\n", - "Tune response: #0 QCORR_061 [0.21000027 0.30999794]\n", - "Tune response: #0 QCORR_062 [0.21000024 0.3099981 ]\n", - "Tune response: #0 QCORR_063 [0.21000033 0.30999833]\n", - "Tune response: #0 QCORR_064 [0.20998947 0.31000775]\n", - "Tune response: #0 QCORR_065 [0.20998934 0.31000629]\n", - "Tune response: #0 QCORR_066 [0.21000025 0.30999915]\n", - "Tune response: #0 QCORR_067 [0.21000028 0.30999944]\n", - "Tune response: #0 QCORR_068 [0.21000024 0.3099998 ]\n", - "Tune response: #0 QCORR_069 [0.21000034 0.30999971]\n", - "Tune response: #0 QCORR_070 [0.20998955 0.31000449]\n", - "Tune response: #0 QCORR_071 [0.20996182 0.30998447]\n", - "Tune response: #0 QCORR_072 [0.20996109 0.30998505]\n", - "Tune response: #0 QCORR_073 [0.20998924 0.31000543]\n", - "Tune response: #0 QCORR_074 [0.21000015 0.30999913]\n", - "Tune response: #0 QCORR_075 [0.21000033 0.30999886]\n", - "Tune response: #0 QCORR_076 [0.21000022 0.30999813]\n", - "Tune response: #0 QCORR_077 [0.21000044 0.30999801]\n", - "Tune response: #0 QCORR_078 [0.2100007 0.30999855]\n", - "Tune response: #0 QCORR_079 [0.21000071 0.30999877]\n", - "Tune response: #0 QCORR_080 [0.21000045 0.30999919]\n", - "Tune response: #0 QCORR_081 [0.21000022 0.30999941]\n", - "Tune response: #0 QCORR_082 [0.21000033 0.30999961]\n", - "Tune response: #0 QCORR_083 [0.21000015 0.30999949]\n", - "Tune response: #0 QCORR_084 [0.20998923 0.3100043 ]\n", - "Tune response: #0 QCORR_085 [0.20996107 0.3099844 ]\n", - "Tune response: #0 QCORR_086 [0.20996182 0.30998499]\n", - "Tune response: #0 QCORR_087 [0.20998955 0.31000525]\n", - "Tune response: #0 QCORR_088 [0.21000035 0.30999898]\n", - "Tune response: #0 QCORR_089 [0.21000025 0.30999876]\n", - "Tune response: #0 QCORR_090 [0.21000029 0.30999824]\n", - "Tune response: #0 QCORR_091 [0.21000025 0.30999817]\n", - "Tune response: #0 QCORR_092 [0.20998752 0.31000811]\n", - "Tune response: #0 QCORR_093 [0.20998767 0.31000768]\n", - "Tune response: #0 QCORR_094 [0.21000033 0.30999836]\n", - "Tune response: #0 QCORR_095 [0.21000025 0.30999856]\n", - "Tune response: #0 QCORR_096 [0.21000028 0.3099992 ]\n", - "Tune response: #0 QCORR_097 [0.21000026 0.30999936]\n", - "Tune response: #0 QCORR_098 [0.21000057 0.30999981]\n", - "Tune response: #0 QCORR_099 [0.21000064 0.30999968]\n", - "Tune response: #0 QCORR_100 [0.21000028 0.30999867]\n", - "Tune response: #0 QCORR_101 [0.21000035 0.30999846]\n", - "Tune response: #0 QCORR_102 [0.21000034 0.30999812]\n", - "Tune response: #0 QCORR_103 [0.21000032 0.30999815]\n", - "Tune response: #0 QCORR_104 [0.20999868 0.31007742]\n", - "Tune response: #0 QCORR_105 [0.20999871 0.31007788]\n", - "Tune response: #0 QCORR_106 [0.21000033 0.30999812]\n", - "Tune response: #0 QCORR_107 [0.21000032 0.30999803]\n", - "Tune response: #0 QCORR_108 [0.21000034 0.30999829]\n", - "Tune response: #0 QCORR_109 [0.21000027 0.30999851]\n", - "Tune response: #0 QCORR_110 [0.21000062 0.30999964]\n", - "Tune response: #0 QCORR_111 [0.21000058 0.30999983]\n", - "Tune response: #0 QCORR_112 [0.21000026 0.30999952]\n", - "Tune response: #0 QCORR_113 [0.2100003 0.30999938]\n", - "Tune response: #0 QCORR_114 [0.21000027 0.30999867]\n", - "Tune response: #0 QCORR_115 [0.21000034 0.30999842]\n", - "Tune response: #0 QCORR_116 [0.20998766 0.31000752]\n", - "Tune response: #0 QCORR_117 [0.20998749 0.31000823]\n", - "Tune response: #0 QCORR_118 [0.21000025 0.30999808]\n", - "Tune response: #0 QCORR_119 [0.21000031 0.3099981 ]\n", - "Tune response: #0 QCORR_120 [0.21000027 0.3099986 ]\n", - "Tune response: #0 QCORR_121 [0.21000035 0.30999885]\n", - "Tune response: #0 QCORR_122 [0.20998953 0.3100053 ]\n", - "Tune response: #0 QCORR_123 [0.20996179 0.30998503]\n", - "Tune response: #0 QCORR_124 [0.20996102 0.3099843 ]\n", - "Tune response: #0 QCORR_125 [0.2099892 0.31000412]\n", - "Tune response: #0 QCORR_126 [0.21000015 0.30999949]\n", - "Tune response: #0 QCORR_127 [0.21000036 0.30999967]\n", - "Tune response: #0 QCORR_128 [0.21000025 0.30999959]\n", - "Tune response: #0 QCORR_129 [0.21000045 0.30999937]\n", - "Tune response: #0 QCORR_130 [0.21000072 0.30999885]\n", - "Tune response: #0 QCORR_131 [0.21000068 0.30999857]\n", - "Tune response: #0 QCORR_132 [0.21000044 0.30999788]\n", - "Tune response: #0 QCORR_133 [0.2100002 0.30999797]\n", - "Tune response: #0 QCORR_134 [0.2100003 0.30999872]\n", - "Tune response: #0 QCORR_135 [0.21000016 0.30999904]\n", - "Tune response: #0 QCORR_136 [0.20998927 0.31000555]\n", - "Tune response: #0 QCORR_137 [0.20996115 0.30998513]\n", - "Tune response: #0 QCORR_138 [0.20996183 0.30998439]\n", - "Tune response: #0 QCORR_139 [0.20998956 0.31000435]\n", - "Tune response: #0 QCORR_140 [0.21000033 0.30999977]\n", - "Tune response: #0 QCORR_141 [0.21000023 0.30999991]\n", - "Tune response: #0 QCORR_142 [0.21000026 0.30999962]\n", - "Tune response: #0 QCORR_143 [0.21000026 0.30999931]\n", - "Tune response: #0 QCORR_144 [0.20998938 0.31000629]\n", - "Tune response: #0 QCORR_145 [0.20998947 0.31000796]\n", - "Tune response: #0 QCORR_146 [0.21000032 0.30999838]\n", - "Tune response: #0 QCORR_147 [0.21000023 0.30999808]\n", - "Tune response: #0 QCORR_148 [0.21000025 0.30999779]\n", - "Tune response: #0 QCORR_149 [0.21000028 0.30999792]\n", - "Tune response: #0 QCORR_150 [0.21000056 0.30999916]\n", - "Tune response: #0 QCORR_151 [0.21000067 0.30999952]\n", - "Tune response: #0 QCORR_152 [0.2100003 0.30999982]\n", - "Tune response: #0 QCORR_153 [0.21000036 0.30999985]\n", - "Tune response: #0 QCORR_154 [0.21000036 0.30999929]\n", - "Tune response: #0 QCORR_155 [0.2100003 0.30999895]\n", - "Tune response: #0 QCORR_156 [0.21000455 0.31002745]\n", - "Tune response: #0 QCORR_157 [0.21000456 0.3100278 ]\n", - "Tune response: #0 QCORR_158 [0.2100003 0.30999899]\n", - "Tune response: #0 QCORR_159 [0.21000034 0.30999926]\n", - "Tune response: #0 QCORR_160 [0.21000034 0.30999966]\n", - "Tune response: #0 QCORR_161 [0.2100003 0.30999961]\n", - "Tune response: #0 QCORR_162 [0.21000065 0.30999939]\n", - "Tune response: #0 QCORR_163 [0.21000058 0.30999909]\n", - "Tune response: #0 QCORR_164 [0.21000028 0.30999804]\n", - "Tune response: #0 QCORR_165 [0.21000026 0.30999795]\n", - "Tune response: #0 QCORR_166 [0.21000025 0.30999826]\n", - "Tune response: #0 QCORR_167 [0.21000031 0.30999852]\n", - "Tune response: #0 QCORR_168 [0.20998945 0.31000787]\n", - "Tune response: #0 QCORR_169 [0.20998936 0.3100065 ]\n", - "Tune response: #0 QCORR_170 [0.21000027 0.30999929]\n", - "Tune response: #0 QCORR_171 [0.21000027 0.30999953]\n", - "Tune response: #0 QCORR_172 [0.21000025 0.30999971]\n", - "Tune response: #0 QCORR_173 [0.21000033 0.30999957]\n", - "Tune response: #0 QCORR_174 [0.20998953 0.31000429]\n", - "Tune response: #0 QCORR_175 [0.20996177 0.30998439]\n", - "Tune response: #0 QCORR_176 [0.20996115 0.30998502]\n", - "Tune response: #0 QCORR_177 [0.20998926 0.3100053 ]\n", - "Tune response: #0 QCORR_178 [0.21000017 0.30999894]\n", - "Tune response: #0 QCORR_179 [0.21000032 0.30999869]\n", - "Tune response: #0 QCORR_180 [0.21000022 0.30999812]\n", - "Tune response: #0 QCORR_181 [0.21000043 0.30999806]\n", - "Tune response: #0 QCORR_182 [0.21000069 0.30999873]\n", - "Tune response: #0 QCORR_183 [0.2100007 0.30999896]\n", - "Tune response: #0 QCORR_184 [0.21000043 0.30999928]\n", - "Tune response: #0 QCORR_185 [0.21000024 0.30999944]\n", - "Tune response: #0 QCORR_186 [0.21000034 0.30999947]\n", - "Tune response: #0 QCORR_187 [0.21000016 0.30999931]\n", - "Tune response: #0 QCORR_188 [0.20998924 0.31000414]\n", - "Tune response: #0 QCORR_189 [0.2099611 0.30998434]\n", - "Tune response: #0 QCORR_190 [0.20996176 0.30998492]\n", - "Tune response: #0 QCORR_191 [0.20998952 0.31000507]\n", - "Tune response: #0 QCORR_192 [0.21000033 0.30999881]\n", - "Tune response: #0 QCORR_193 [0.21000026 0.30999863]\n", - "Tune response: #0 QCORR_194 [0.21000029 0.30999828]\n", - "Tune response: #0 QCORR_195 [0.21000026 0.30999828]\n", - "Tune response: #0 QCORR_196 [0.20998754 0.31000834]\n", - "Tune response: #0 QCORR_197 [0.20998765 0.31000776]\n", - "Tune response: #0 QCORR_198 [0.21000032 0.30999855]\n", - "Tune response: #0 QCORR_199 [0.21000026 0.30999874]\n", - "Tune response: #0 QCORR_200 [0.21000028 0.30999925]\n", - "Tune response: #0 QCORR_201 [0.21000028 0.30999935]\n", - "Tune response: #0 QCORR_202 [0.21000058 0.30999964]\n", - "Tune response: #0 QCORR_203 [0.21000064 0.30999949]\n", - "Tune response: #0 QCORR_204 [0.21000029 0.30999855]\n", - "Tune response: #0 QCORR_205 [0.21000034 0.30999838]\n", - "Tune response: #0 QCORR_206 [0.21000033 0.30999823]\n", - "Tune response: #0 QCORR_207 [0.21000031 0.3099983 ]\n", - "Tune response: #0 QCORR_208 [0.20999868 0.31007796]\n", - "CPU times: user 41.9 s, sys: 179 ms, total: 42.1 s\n", - "Wall time: 42.2 s\n" - ] - }, - { - "data": { - "text/plain": [ - "True" - ] - }, - "execution_count": 10, - "metadata": {}, - "output_type": "execute_result" - } - ], - "source": [ - "%%time\n", - "tune_response_matrix.measure(callback=tune_callback)" - ] - }, - { - "cell_type": "markdown", - "id": "2c746dcf-c05f-4e5b-88cb-f4680e9dde18", - "metadata": {}, - "source": [ - "The correction matrix can be saved to a file (and added to the configuration file).\n", - "```\n", - "tune_response_matrix.save(\"tune_response_matrix_live.json\")\n", - "tune_correction.load('tune_response_matrix_design.json')\n", - "```" - ] - }, - { - "cell_type": "code", - "execution_count": 12, - "id": "09642999-b579-4abb-a27f-14915f66fff6", - "metadata": {}, - "outputs": [], - "source": [ - "tune_response_matrix.save(\"trm.json\")" - ] - }, - { - "cell_type": "code", - "execution_count": 13, - "id": "e08e4a85-c21b-464b-9715-24404be15e42", - "metadata": {}, - "outputs": [], - "source": [ - "tune_correction.load(\"trm.json\")" - ] - }, - { - "cell_type": "code", - "execution_count": 14, - "id": "40357e20-93d4-40b8-899c-b93a70378af6", - "metadata": {}, - "outputs": [], - "source": [ - "tune_correction.set([0.21, 0.31], iter=10, wait_time=1.2)" - ] - }, - { - "cell_type": "code", - "execution_count": 15, - "id": "bdac5596-9b18-42a7-9670-1a2c825a25b0", - "metadata": {}, - "outputs": [ - { - "name": "stdout", - "output_type": "stream", - "text": [ - "Readback after changing tune is [0.21 0.31]. We can also check the setpoint [0.21 0.31]\n" - ] - }, - { - "data": { - "text/plain": [ - "Tune(peer='Simulator:design', name='DEFAULT_TUNE_CORRECTION', description=None, lattice_names=None, quad_array_name='QCORR', betatron_tune_name='BETATRON_TUNE', response_matrix=ResponseMatrixData(matrix=[[0.14102360783224688, 0.1247736956877521, 0.1247784063651558, 0.1246481795635912, 0.12512932427849455, 0.12169720499499714, 0.12207610030512406, 0.1252274901519801, 0.12505436176257767, 0.1252421814237903, 0.12471476857733865, 0.251560657692218, 0.2527213486122615, 0.12536440930077664, 0.12497398019867267, 0.1252557490932782, 0.12459571048201168, 0.23286692596019565, 0.5104957165136259, 0.5171068874740281, 0.23565770243150208, 0.1263295019007793, 0.12451253126988249, 0.1255077164324936, 0.12361394153115324, 0.12087299659901962, 0.12116595465655466, 0.12368974746601591, 0.12582207524092226, 0.12487114328635363, 0.12628455338115074, 0.23517978625403613, 0.5162366992164658, 0.5102502635032091, 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-0.34207315443512964, -0.332626497961952, -0.3310046193927274, -0.32944483748520437, -0.3301994378679396, -1.126783453100355]], variable_names=['QCORR_001', 'QCORR_002', 'QCORR_003', 'QCORR_004', 'QCORR_005', 'QCORR_006', 'QCORR_007', 'QCORR_008', 'QCORR_009', 'QCORR_010', 'QCORR_011', 'QCORR_012', 'QCORR_013', 'QCORR_014', 'QCORR_015', 'QCORR_016', 'QCORR_017', 'QCORR_018', 'QCORR_019', 'QCORR_020', 'QCORR_021', 'QCORR_022', 'QCORR_023', 'QCORR_024', 'QCORR_025', 'QCORR_026', 'QCORR_027', 'QCORR_028', 'QCORR_029', 'QCORR_030', 'QCORR_031', 'QCORR_032', 'QCORR_033', 'QCORR_034', 'QCORR_035', 'QCORR_036', 'QCORR_037', 'QCORR_038', 'QCORR_039', 'QCORR_040', 'QCORR_041', 'QCORR_042', 'QCORR_043', 'QCORR_044', 'QCORR_045', 'QCORR_046', 'QCORR_047', 'QCORR_048', 'QCORR_049', 'QCORR_050', 'QCORR_051', 'QCORR_052', 'QCORR_053', 'QCORR_054', 'QCORR_055', 'QCORR_056', 'QCORR_057', 'QCORR_058', 'QCORR_059', 'QCORR_060', 'QCORR_061', 'QCORR_062', 'QCORR_063', 'QCORR_064', 'QCORR_065', 'QCORR_066', 'QCORR_067', 'QCORR_068', 'QCORR_069', 'QCORR_070', 'QCORR_071', 'QCORR_072', 'QCORR_073', 'QCORR_074', 'QCORR_075', 'QCORR_076', 'QCORR_077', 'QCORR_078', 'QCORR_079', 'QCORR_080', 'QCORR_081', 'QCORR_082', 'QCORR_083', 'QCORR_084', 'QCORR_085', 'QCORR_086', 'QCORR_087', 'QCORR_088', 'QCORR_089', 'QCORR_090', 'QCORR_091', 'QCORR_092', 'QCORR_093', 'QCORR_094', 'QCORR_095', 'QCORR_096', 'QCORR_097', 'QCORR_098', 'QCORR_099', 'QCORR_100', 'QCORR_101', 'QCORR_102', 'QCORR_103', 'QCORR_104', 'QCORR_105', 'QCORR_106', 'QCORR_107', 'QCORR_108', 'QCORR_109', 'QCORR_110', 'QCORR_111', 'QCORR_112', 'QCORR_113', 'QCORR_114', 'QCORR_115', 'QCORR_116', 'QCORR_117', 'QCORR_118', 'QCORR_119', 'QCORR_120', 'QCORR_121', 'QCORR_122', 'QCORR_123', 'QCORR_124', 'QCORR_125', 'QCORR_126', 'QCORR_127', 'QCORR_128', 'QCORR_129', 'QCORR_130', 'QCORR_131', 'QCORR_132', 'QCORR_133', 'QCORR_134', 'QCORR_135', 'QCORR_136', 'QCORR_137', 'QCORR_138', 'QCORR_139', 'QCORR_140', 'QCORR_141', 'QCORR_142', 'QCORR_143', 'QCORR_144', 'QCORR_145', 'QCORR_146', 'QCORR_147', 'QCORR_148', 'QCORR_149', 'QCORR_150', 'QCORR_151', 'QCORR_152', 'QCORR_153', 'QCORR_154', 'QCORR_155', 'QCORR_156', 'QCORR_157', 'QCORR_158', 'QCORR_159', 'QCORR_160', 'QCORR_161', 'QCORR_162', 'QCORR_163', 'QCORR_164', 'QCORR_165', 'QCORR_166', 'QCORR_167', 'QCORR_168', 'QCORR_169', 'QCORR_170', 'QCORR_171', 'QCORR_172', 'QCORR_173', 'QCORR_174', 'QCORR_175', 'QCORR_176', 'QCORR_177', 'QCORR_178', 'QCORR_179', 'QCORR_180', 'QCORR_181', 'QCORR_182', 'QCORR_183', 'QCORR_184', 'QCORR_185', 'QCORR_186', 'QCORR_187', 'QCORR_188', 'QCORR_189', 'QCORR_190', 'QCORR_191', 'QCORR_192', 'QCORR_193', 'QCORR_194', 'QCORR_195', 'QCORR_196', 'QCORR_197', 'QCORR_198', 'QCORR_199', 'QCORR_200', 'QCORR_201', 'QCORR_202', 'QCORR_203', 'QCORR_204', 'QCORR_205', 'QCORR_206', 'QCORR_207', 'QCORR_208'], observable_names=['BETATRON_TUNE.x', 'BETATRON_TUNE.y']))" - ] - }, - "execution_count": 15, - "metadata": {}, - "output_type": "execute_result" - } - ], - "source": [ - "print(\n", - " f\"Readback after changing tune is {tune_correction.readback()}. We can also check the setpoint {tune_monitor.tune.get()}\"\n", - ")\n", - "tune_correction # string representation" - ] - }, - { - "cell_type": "code", - "execution_count": 16, - "id": "50be3687-e087-4e3a-80ec-c71915642bde", - "metadata": {}, - "outputs": [ - { - "name": "stdout", - "output_type": "stream", - "text": [ - "Tune readback is [0.21 0.31]\n", - "0\n", - "Let's change the tune to qx=0.19, qy=0.28\n", - "Tune readback is [0.19 0.28]\n", - "Let's change the tune to qx=0.21, qy=0.3\n", - "Tune readback is [0.21 0.3 ]\n" - ] - } - ], - "source": [ - "print(f\"Tune readback is {tune_correction.readback()}\")\n", - "print(wait_time)\n", - "qx, qy = 0.19, 0.28\n", - "print(f\"Let's change the tune to {qx=:}, {qy=:}\")\n", - "tune_correction.set([qx, qy], iter=10, wait_time=wait_time)\n", - "print(f\"Tune readback is {tune_correction.readback()}\")\n", - "\n", - "qx, qy = 0.21, 0.3\n", - "print(f\"Let's change the tune to {qx=:}, {qy=:}\")\n", - "\n", - "tune_correction.set([qx, qy], iter=10, wait_time=wait_time)\n", - "print(f\"Tune readback is {tune_correction.readback()}\")\n", - "\n", - "# You can try to do something stupid too!\n", - "# qx, qy = 0.5, 0.0\n", - "# print(f\"Let's do something stupid and change the tune to {qx=:}, {qy=:}\")\n", - "# tune_correction.set([qx, qy])" - ] - } - ], - "metadata": { - "kernelspec": { - "display_name": "Python 3 (ipykernel)", - "language": "python", - "name": "python3" - }, - "language_info": { - "codemirror_mode": { - "name": "ipython", - "version": 3 - }, - "file_extension": ".py", - "mimetype": "text/x-python", - "name": "python", - "nbconvert_exporter": "python", - "pygments_lexer": "ipython3", - "version": "3.12.3" - } - }, - "nbformat": 4, - "nbformat_minor": 5 -} diff --git a/examples/SOLEIL_examples/02-chromaticity_measurement.ipynb b/examples/SOLEIL_examples/02-chromaticity_measurement.ipynb deleted file mode 100644 index caedbede3..000000000 --- a/examples/SOLEIL_examples/02-chromaticity_measurement.ipynb +++ /dev/null @@ -1,245 +0,0 @@ -{ - "cells": [ - { - "cell_type": "code", - "execution_count": 1, - "id": "9fccf447-e065-46ab-88c3-a9763d9ed06b", - "metadata": {}, - "outputs": [], - "source": [ - "import os\n", - "\n", - "import numpy as np\n", - "\n", - "from pyaml.accelerator import Accelerator\n", - "from pyaml.common.constants import Action\n", - "from pyaml.magnet.magnet import Magnet" - ] - }, - { - "cell_type": "code", - "execution_count": 2, - "id": "6c657c45-2d0e-404a-8304-b250becea262", - "metadata": {}, - "outputs": [ - { - "name": "stderr", - "output_type": "stream", - "text": [ - "PyAML Tango control system binding (0.3.3) initialized with name 'live' and TANGO_HOST=localhost:11000\n" - ] - }, - { - "data": { - "text/plain": [ - "Accelerator(facility='Synchrotron SOLEIL', machine='sr', energy=2750000000.0, alphac=None, harmonic_number=None, controls=[TangoControlSystem(name='live', tango_host='localhost:11000', debug_level=None, lazy_devices=True, scalar_aggregator='tango.pyaml.multi_attribute', vector_aggregator=None, timeout_ms=3000)], simulators=[Simulator(name='design', lattice='/home/gubaidulin/codes/operation/pyAML/pyaml/examples/SOLEIL_examples/SOLEIL_II_V3631_sym1_V001_database_rf.m', mat_key=None, linker=, description=None)], data_folder='/data/store', description=None)" - ] - }, - "execution_count": 2, - "metadata": {}, - "output_type": "execute_result" - } - ], - "source": [ - "sr = Accelerator.load(\"p.yaml\")\n", - "sr # string representation" - ] - }, - { - "cell_type": "markdown", - "id": "e300a41c-ee12-47db-80c3-090468b2c293", - "metadata": {}, - "source": [ - "### Virtual accelerator setup for emulation of a control system\n", - "For the **live** control mode, you should have some control system emulation running. \n", - "\n", - "!!! *If you want to skip this, you can always run the notebook in **design** mode.* !!!\n", - "\n", - "For the installation you should be able to do \n", - "```\n", - "apptainer pull virtual-accelerator.sif oras://gitlab-registry.synchrotron-soleil.fr/software-control-system/containers/apptainer/virtual-accelerator:latest\n", - "apptainer run virtual-accelerator.sif\n", - "```\n", - "This will run SOLEIL II proof-of-concept digital twin on localhost:11000. You can play with the digital twin itself (without pyAML) via Jive to check that everything is working. You can run Jive in a different terminal with \n", - "```\n", - "apptainer pull jive.sif https://gitlab.synchrotron-soleil.fr/api/v4/projects/2739/packages/generic/jive/latest/jive.sif\n", - "apptainer run jive.sif\n", - "```\n", - "On linux you may additionally configure X11\n", - "```\n", - "export DISPLAY=:0\n", - "xhost +local:root\n", - "```\n", - "Jive is not necessary to run anything but some of you may find it useful to open its `simulator/ringsimulator/ringsimulator` device on the side and see how the global parameters (tune, orbit, chromaticity, etc.) change with your actions in pyAML.\n", - "NOTE: This notebook is just a demonstration of pyAML functionality. Certain things may be done stupidly. The person who wrote this jupyter notebook only cared about showing that the code is working, not about intelligently controlling the accelerator." - ] - }, - { - "cell_type": "code", - "execution_count": 3, - "id": "a5bde3a2-b1aa-4c64-afaf-068ad61f0f1b", - "metadata": {}, - "outputs": [ - { - "data": { - "text/plain": [ - "Simulator(name='design', lattice='/home/gubaidulin/codes/operation/pyAML/pyaml/examples/SOLEIL_examples/SOLEIL_II_V3631_sym1_V001_database_rf.m', mat_key=None, linker=, description=None)" - ] - }, - "execution_count": 3, - "metadata": {}, - "output_type": "execute_result" - } - ], - "source": [ - "control_mode = sr.design\n", - "wait_time = 2.0 if control_mode == sr.live else 0.1\n", - "control_mode" - ] - }, - { - "cell_type": "code", - "execution_count": 4, - "id": "1da59cb7-ba59-479f-97d2-4fa550574737", - "metadata": {}, - "outputs": [ - { - "data": { - "text/plain": [ - "ChomaticityMonitor(peer='Simulator:design', name='DEFAULT_CHROMATICITY_MEASUREMENT', description=None, lattice_names=None, n_step=15, sleep_between_step=2.0, n_avg_meas=3, sleep_between_meas=2.0, betatron_tune_name='BETATRON_TUNE', rf_plant_name='RF', bpm_array_name=None, e_delta=0.01, max_e_delta=0.05, fit_order=2, fit_disp_order=1, fit_dispersion=False)" - ] - }, - "execution_count": 4, - "metadata": {}, - "output_type": "execute_result" - } - ], - "source": [ - "chromaticity_measurement = control_mode.get_chromaticity_monitor(\"DEFAULT_CHROMATICITY_MEASUREMENT\")\n", - "chromaticity_measurement" - ] - }, - { - "cell_type": "code", - "execution_count": 5, - "id": "cbd5672c-79e6-457f-b388-b2fdcac77d11", - "metadata": {}, - "outputs": [], - "source": [ - "def chroma_callback(action: int, cb_data: dict):\n", - " if action == Action.MEASURE:\n", - " print(f\"Chromaticy measurement: #{cb_data['step']} RF={cb_data['rf']} Tune={cb_data['tune']}\")\n", - " return True" - ] - }, - { - "cell_type": "code", - "execution_count": 6, - "id": "bd984afc-d011-40a6-8a26-983fdc923a5b", - "metadata": {}, - "outputs": [], - "source": [ - "sr.design.get_lattice().disable_6d()\n", - "alphac = sr.design.get_lattice().get_mcf()\n", - "sr.design.get_lattice().enable_6d()" - ] - }, - { - "cell_type": "code", - "execution_count": 7, - "id": "a0e66f14-cf54-4811-b728-652dd9f7025b", - "metadata": {}, - "outputs": [ - { - "name": "stdout", - "output_type": "stream", - "text": [ - "Chromaticy measurement: #0 RF=352314629.3149023 Tune=[0.19179162 0.2886065 ]\n", - "Chromaticy measurement: #0 RF=352314629.3149023 Tune=[0.19179162 0.2886065 ]\n", - "Chromaticy measurement: #0 RF=352314629.3149023 Tune=[0.19179162 0.2886065 ]\n", - "Chromaticy measurement: #1 RF=352314440.70959616 Tune=[0.194552 0.29325077]\n", - "Chromaticy measurement: #1 RF=352314440.70959616 Tune=[0.194552 0.29325077]\n", - "Chromaticy measurement: #1 RF=352314440.70959616 Tune=[0.194552 0.29325077]\n", - "Chromaticy measurement: #2 RF=352314252.10429 Tune=[0.20121916 0.30015277]\n", - "Chromaticy measurement: #2 RF=352314252.10429 Tune=[0.20121916 0.30015277]\n", - "Chromaticy measurement: #2 RF=352314252.10429 Tune=[0.20121916 0.30015277]\n", - "Chromaticy measurement: #3 RF=352314063.49898386 Tune=[0.20984821 0.30918899]\n", - "Chromaticy measurement: #3 RF=352314063.49898386 Tune=[0.20984821 0.30918899]\n", - "Chromaticy measurement: #3 RF=352314063.49898386 Tune=[0.20984821 0.30918899]\n", - "Chromaticy measurement: #4 RF=352313874.8936777 Tune=[0.21855404 0.32022564]\n", - "Chromaticy measurement: #4 RF=352313874.8936777 Tune=[0.21855404 0.32022564]\n", - "Chromaticy measurement: #4 RF=352313874.8936777 Tune=[0.21855404 0.32022564]\n" - ] - }, - { - "data": { - "image/png": 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", - "text/plain": [ - "
" - ] - }, - "metadata": {}, - "output_type": "display_data" - }, - { - "data": { - "text/plain": [ - "True" - ] - }, - "execution_count": 7, - "metadata": {}, - "output_type": "execute_result" - } - ], - "source": [ - "chromaticity_measurement.measure(\n", - " callback=chroma_callback,\n", - " do_plot=True,\n", - " alphac=alphac,\n", - " fit_order=2,\n", - " n_step=5,\n", - " sleep_between_meas=wait_time,\n", - " sleep_between_step=wait_time,\n", - ")" - ] - }, - { - "cell_type": "code", - "execution_count": null, - "id": "5ac230e9-d96d-460a-a425-ae6892465371", - "metadata": {}, - "outputs": [], - "source": [] - }, - { - "cell_type": "code", - "execution_count": null, - "id": "b5114363-ac95-41f9-b1b1-e433d4e7184b", - "metadata": {}, - "outputs": [], - "source": [] - } - ], - "metadata": { - "kernelspec": { - "display_name": "Python 3 (ipykernel)", - "language": "python", - "name": "python3" - }, - "language_info": { - "codemirror_mode": { - "name": "ipython", - "version": 3 - }, - "file_extension": ".py", - "mimetype": "text/x-python", - "name": "python", - "nbconvert_exporter": "python", - "pygments_lexer": "ipython3", - "version": "3.12.3" - } - }, - "nbformat": 4, - "nbformat_minor": 5 -} diff --git a/examples/SOLEIL_examples/03-Orbit_correction.ipynb b/examples/SOLEIL_examples/03-Orbit_correction.ipynb deleted file mode 100644 index 7b5c607b1..000000000 --- a/examples/SOLEIL_examples/03-Orbit_correction.ipynb +++ /dev/null @@ -1,809 +0,0 @@ -{ - "cells": [ - { - "cell_type": "code", - "execution_count": 1, - "id": "68b780c8-534e-46af-b336-6860edeefef4", - "metadata": {}, - "outputs": [], - "source": [ - "import os\n", - "from time import sleep\n", - "\n", - "import matplotlib.pyplot as plt\n", - "import numpy as np\n", - "\n", - "from pyaml.accelerator import Accelerator\n", - "from pyaml.common.constants import Action\n", - "from pyaml.magnet.magnet import Magnet" - ] - }, - { - "cell_type": "code", - "execution_count": 2, - "id": "62dc34e1-bb65-4b56-b596-e05d60a0e0a5", - "metadata": {}, - "outputs": [ - { - "name": "stderr", - "output_type": "stream", - "text": [ - "PyAML Tango control system binding (0.3.3) initialized with name 'live' and TANGO_HOST=localhost:11000\n", - "/home/gubaidulin/codes/operation/pyAML/pyaml/examples/SOLEIL_examples/trm.json: file not found\n" - ] - }, - { - "name": "stdout", - "output_type": "stream", - "text": [ - "27 Apr 2026, 15:50:05 | WARNING | Loading /home/gubaidulin/codes/operation/pyAML/pyaml/examples/SOLEIL_examples/orm.json failed /home/gubaidulin/codes/operation/pyAML/pyaml/examples/SOLEIL_examples/orm.json: file not found\n" - ] - }, - { - "data": { - "text/plain": [ - "Accelerator(facility='Synchrotron SOLEIL', machine='sr', energy=2750000000.0, alphac=None, harmonic_number=None, controls=[TangoControlSystem(name='live', tango_host='localhost:11000', debug_level=None, lazy_devices=True, scalar_aggregator='tango.pyaml.multi_attribute', vector_aggregator=None, timeout_ms=3000)], simulators=[Simulator(name='design', lattice='/home/gubaidulin/codes/operation/pyAML/pyaml/examples/SOLEIL_examples/SOLEIL_II_V3631_sym1_V001_database_rf.m', mat_key=None, linker=, description=None)], data_folder='/data/store', description=None)" - ] - }, - "execution_count": 2, - "metadata": {}, - "output_type": "execute_result" - } - ], - "source": [ - "sr = Accelerator.load(\"p.yaml\")\n", - "sr # string representation" - ] - }, - { - "cell_type": "markdown", - "id": "71e973b4-e9d8-48d7-98dc-8f43fcbacb21", - "metadata": {}, - "source": [ - "### Virtual accelerator setup for emulation of a control system\n", - "For the **live** control mode, you should have some control system emulation running. \n", - "\n", - "!!! *If you want to skip this, you can always run the notebook in **design** mode.* !!!\n", - "\n", - "For the installation you should be able to do \n", - "```\n", - "apptainer pull virtual-accelerator.sif oras://gitlab-registry.synchrotron-soleil.fr/software-control-system/containers/apptainer/virtual-accelerator:latest\n", - "apptainer run virtual-accelerator.sif\n", - "```\n", - "This will run SOLEIL II proof-of-concept digital twin on localhost:11000. You can play with the digital twin itself (without pyAML) via Jive to check that everything is working. You can run Jive in a different terminal with \n", - "```\n", - "apptainer pull jive.sif https://gitlab.synchrotron-soleil.fr/api/v4/projects/2739/packages/generic/jive/latest/jive.sif\n", - "apptainer run jive.sif\n", - "```\n", - "On linux you may additionally configure X11\n", - "```\n", - "export DISPLAY=:0\n", - "xhost +local:root\n", - "```\n", - "Jive is not necessary to run anything but some of you may find it useful to open its `simulator/ringsimulator/ringsimulator` device on the side and see how the global parameters (tune, orbit, chromaticity, etc.) change with your actions in pyAML.\n", - "NOTE: This notebook is just a demonstration of pyAML functionality. Certain things may be done stupidly. The person who wrote this jupyter notebook only cared about showing that the code is working, not about intelligently controlling the accelerator." - ] - }, - { - "cell_type": "code", - "execution_count": 3, - "id": "6727e66d-a4f8-4a88-86b9-a58022d5ea55", - "metadata": {}, - "outputs": [ - { - "data": { - "text/plain": [ - "Simulator(name='design', lattice='/home/gubaidulin/codes/operation/pyAML/pyaml/examples/SOLEIL_examples/SOLEIL_II_V3631_sym1_V001_database_rf.m', mat_key=None, linker=, description=None)" - ] - }, - "execution_count": 3, - "metadata": {}, - "output_type": "execute_result" - } - ], - "source": [ - "control_mode = sr.design\n", - "wait_time = 2.0 if control_mode == sr.live else 0.1\n", - "control_mode" - ] - }, - { - "cell_type": "code", - "execution_count": 4, - "id": "f4918a42-a21b-4815-a747-a96c292405fe", - "metadata": {}, - "outputs": [], - "source": [ - "bpms = control_mode.get_bpms(\"BPM\")" - ] - }, - { - "cell_type": "code", - "execution_count": 5, - "id": "ec4de2fa-b538-4d7c-8ca7-c7c4d6f637cb", - "metadata": {}, - "outputs": [ - { - "data": { - "text/plain": [ - "OrbitResponseMatrix(peer='Simulator:design', name='DEFAULT_ORBIT_RESPONSE_MATRIX', description=None, lattice_names=None, n_step=1, sleep_between_step=0, n_avg_meas=1, sleep_between_meas=0, bpm_array_name='BPM', hcorr_array_name='HCORR', vcorr_array_name='VCORR', corrector_delta=1e-05)" - ] - }, - "execution_count": 5, - "metadata": {}, - "output_type": "execute_result" - } - ], - "source": [ - "orbit_response_matrix = control_mode.get_orm_tuning(\"DEFAULT_ORBIT_RESPONSE_MATRIX\")\n", - "orbit_response_matrix" - ] - }, - { - "cell_type": "code", - "execution_count": 6, - "id": "bbdf07f3-593b-45c3-8ba0-01bb36cef7ae", - "metadata": {}, - "outputs": [ - { - "data": { - "text/plain": [ - "Orbit(peer='Simulator:design', name='DEFAULT_ORBIT_CORRECTION', description=None, lattice_names=None, bpm_array_name='BPM', hcorr_array_name='HCORR', vcorr_array_name='VCORR', rf_plant_name=None, singular_values=16, singular_values_H=None, singular_values_V=None, virtual_target=0, response_matrix=None)" - ] - }, - "execution_count": 6, - "metadata": {}, - "output_type": "execute_result" - } - ], - "source": [ - "orbit_correction = control_mode.get_orbit_tuning(\"DEFAULT_ORBIT_CORRECTION\")\n", - "orbit_correction" - ] - }, - { - "cell_type": "code", - "execution_count": 7, - "id": "19b62db1-e93f-48cc-8351-f09c518379de", - "metadata": {}, - "outputs": [ - { - "name": "stdout", - "output_type": "stream", - "text": [ - "27 Apr 2026, 15:50:08 | INFO | Measuring correctors from the default arrays: HCORR and VCORR.\n", - "27 Apr 2026, 15:50:09 | INFO | Measured response of SH1_COR_001.hcorrector.\n", - "27 Apr 2026, 15:50:10 | INFO | Measured response of SH2_HCOR_001.hcorrector.\n", - "27 Apr 2026, 15:50:10 | INFO | Measured response of SXF11_HCOR_001.hcorrector.\n", - "27 Apr 2026, 15:50:11 | INFO | Measured response of SXF1_HCOR_001.hcorrector.\n", - "27 Apr 2026, 15:50:12 | INFO | Measured response of SXF13_HCOR_001.hcorrector.\n", - "27 Apr 2026, 15:50:12 | INFO | Measured response of SXF13_HCOR_002.hcorrector.\n", - "27 Apr 2026, 15:50:13 | INFO | Measured response of SXF1_HCOR_002.hcorrector.\n", - "27 Apr 2026, 15:50:13 | INFO | Measured response of SXF12_HCOR_001.hcorrector.\n", - "27 Apr 2026, 15:50:14 | INFO | Measured response of SH6_COR_001.hcorrector.\n", - "27 Apr 2026, 15:50:14 | INFO | Measured response of SH4_COR_001.hcorrector.\n", - "27 Apr 2026, 15:50:15 | INFO | Measured response of SH4_COR_002.hcorrector.\n", - "27 Apr 2026, 15:50:15 | INFO | Measured response of SH6_COR_002.hcorrector.\n", - "27 Apr 2026, 15:50:15 | INFO | Measured response of SXF21_HCOR_001.hcorrector.\n", - "27 Apr 2026, 15:50:16 | INFO | Measured response of SXF2_HCOR_001.hcorrector.\n", - "27 Apr 2026, 15:50:16 | INFO | Measured response of SXF22_HCOR_001.hcorrector.\n", - "27 Apr 2026, 15:50:16 | INFO | Measured response of SH9_COR_001.hcorrector.\n", - "27 Apr 2026, 15:50:17 | INFO | Measured response of SH7_COR_001.hcorrector.\n", - "27 Apr 2026, 15:50:17 | INFO | Measured response of SH7_COR_002.hcorrector.\n", - "27 Apr 2026, 15:50:18 | INFO | Measured response of SH9_COR_002.hcorrector.\n", - "27 Apr 2026, 15:50:18 | INFO | Measured response of SXF31_HCOR_001.hcorrector.\n", - "27 Apr 2026, 15:50:18 | INFO | Measured response of SXF3_HCOR_001.hcorrector.\n", - "27 Apr 2026, 15:50:19 | INFO | Measured response of SXF33_HCOR_001.hcorrector.\n", - "27 Apr 2026, 15:50:19 | INFO | Measured response of SXF33_HCOR_002.hcorrector.\n", - "27 Apr 2026, 15:50:19 | INFO | Measured response of SXF3_HCOR_002.hcorrector.\n", - "27 Apr 2026, 15:50:20 | INFO | Measured response of SXF32_HCOR_001.hcorrector.\n", - "27 Apr 2026, 15:50:20 | INFO | Measured response of SH9_COR_003.hcorrector.\n", - "27 Apr 2026, 15:50:20 | INFO | Measured response of SH7_COR_003.hcorrector.\n", - "27 Apr 2026, 15:50:21 | INFO | Measured response of SH7_COR_004.hcorrector.\n", - "27 Apr 2026, 15:50:21 | INFO | Measured response of SH9_COR_004.hcorrector.\n", - "27 Apr 2026, 15:50:21 | INFO | Measured response of SXF41_HCOR_001.hcorrector.\n", - "27 Apr 2026, 15:50:22 | INFO | Measured response of SXF4_HCOR_001.hcorrector.\n", - "27 Apr 2026, 15:50:22 | INFO | Measured response of SXF42_HCOR_001.hcorrector.\n", - "27 Apr 2026, 15:50:22 | INFO | Measured response of SH12_COR_001.hcorrector.\n", - "27 Apr 2026, 15:50:23 | INFO | Measured response of SH10_COR_001.hcorrector.\n", - "27 Apr 2026, 15:50:23 | INFO | Measured response of SH10_COR_002.hcorrector.\n", - "27 Apr 2026, 15:50:23 | INFO | Measured response of SH12_COR_002.hcorrector.\n", - "27 Apr 2026, 15:50:24 | INFO | Measured response of SXF51_HCOR_001.hcorrector.\n", - "27 Apr 2026, 15:50:24 | INFO | Measured response of SXF5_HCOR_001.hcorrector.\n", - "27 Apr 2026, 15:50:24 | INFO | Measured response of SXF53_HCOR_001.hcorrector.\n", - "27 Apr 2026, 15:50:25 | INFO | Measured response of SXF53_HCOR_002.hcorrector.\n", - "27 Apr 2026, 15:50:25 | INFO | Measured response of SXF5_HCOR_002.hcorrector.\n", - "27 Apr 2026, 15:50:25 | INFO | Measured response of SXF52_HCOR_001.hcorrector.\n", - "27 Apr 2026, 15:50:26 | INFO | Measured response of SH14_HCOR_001.hcorrector.\n", - "27 Apr 2026, 15:50:26 | INFO | Measured response of SH13_COR_001.hcorrector.\n", - "27 Apr 2026, 15:50:27 | INFO | Measured response of SH16_COR_001.hcorrector.\n", - "27 Apr 2026, 15:50:27 | INFO | Measured response of SH16_COR_002.hcorrector.\n", - "27 Apr 2026, 15:50:27 | INFO | Measured response of SH13_COR_002.hcorrector.\n", - "27 Apr 2026, 15:50:28 | INFO | Measured response of SH14_HCOR_002.hcorrector.\n", - "27 Apr 2026, 15:50:28 | INFO | Measured response of SXF52_HCOR_002.hcorrector.\n", - "27 Apr 2026, 15:50:29 | INFO | Measured response of SXF5_HCOR_003.hcorrector.\n", - "27 Apr 2026, 15:50:29 | INFO | Measured response of SXF53_HCOR_003.hcorrector.\n", - "27 Apr 2026, 15:50:30 | INFO | Measured response of SXF53_HCOR_004.hcorrector.\n", - "27 Apr 2026, 15:50:30 | INFO | Measured response of SXF5_HCOR_004.hcorrector.\n", - "27 Apr 2026, 15:50:30 | INFO | Measured response of SXF51_HCOR_002.hcorrector.\n", - "27 Apr 2026, 15:50:31 | INFO | Measured response of SH12_COR_003.hcorrector.\n", - "27 Apr 2026, 15:50:31 | INFO | Measured response of SH10_COR_003.hcorrector.\n", - "27 Apr 2026, 15:50:32 | INFO | Measured response of SH10_COR_004.hcorrector.\n", - "27 Apr 2026, 15:50:32 | INFO | Measured response of SH12_COR_004.hcorrector.\n", - "27 Apr 2026, 15:50:33 | INFO | Measured response of SXF42_HCOR_002.hcorrector.\n", - "27 Apr 2026, 15:50:33 | INFO | Measured response of SXF4_HCOR_002.hcorrector.\n", - "27 Apr 2026, 15:50:34 | INFO | Measured response of SXF41_HCOR_002.hcorrector.\n", - "27 Apr 2026, 15:50:34 | INFO | Measured response of SH9_COR_005.hcorrector.\n", - "27 Apr 2026, 15:50:35 | INFO | Measured response of SH7_COR_005.hcorrector.\n", - "27 Apr 2026, 15:50:35 | INFO | Measured response of SH7_COR_006.hcorrector.\n", - "27 Apr 2026, 15:50:36 | INFO | Measured response of SH9_COR_006.hcorrector.\n", - "27 Apr 2026, 15:50:36 | INFO | Measured response of SXF32_HCOR_002.hcorrector.\n", - "27 Apr 2026, 15:50:36 | INFO | Measured response of SXF3_HCOR_003.hcorrector.\n", - "27 Apr 2026, 15:50:37 | INFO | Measured response of SXF33_HCOR_003.hcorrector.\n", - "27 Apr 2026, 15:50:37 | INFO | Measured response of SXF33_HCOR_004.hcorrector.\n", - "27 Apr 2026, 15:50:38 | INFO | Measured response of SXF3_HCOR_004.hcorrector.\n", - "27 Apr 2026, 15:50:38 | INFO | Measured response of SXF31_HCOR_002.hcorrector.\n", - "27 Apr 2026, 15:50:39 | INFO | Measured response of SH9_COR_007.hcorrector.\n", - "27 Apr 2026, 15:50:39 | INFO | Measured response of SH7_COR_007.hcorrector.\n", - "27 Apr 2026, 15:50:40 | INFO | Measured response of SH7_COR_008.hcorrector.\n", - "27 Apr 2026, 15:50:40 | INFO | Measured response of SH9_COR_008.hcorrector.\n", - "27 Apr 2026, 15:50:40 | INFO | Measured response of SXF22_HCOR_002.hcorrector.\n", - "27 Apr 2026, 15:50:41 | INFO | Measured response of SXF2_HCOR_002.hcorrector.\n", - "27 Apr 2026, 15:50:41 | INFO | Measured response of SXF21_HCOR_002.hcorrector.\n", - "27 Apr 2026, 15:50:42 | INFO | Measured response of SH6_COR_003.hcorrector.\n", - "27 Apr 2026, 15:50:42 | INFO | Measured response of SH4_COR_003.hcorrector.\n", - "27 Apr 2026, 15:50:43 | INFO | Measured response of SH4_COR_004.hcorrector.\n", - "27 Apr 2026, 15:50:43 | INFO | Measured response of SH6_COR_004.hcorrector.\n", - "27 Apr 2026, 15:50:44 | INFO | Measured response of SXF12_HCOR_002.hcorrector.\n", - "27 Apr 2026, 15:50:44 | INFO | Measured response of SXF1_HCOR_003.hcorrector.\n", - "27 Apr 2026, 15:50:44 | INFO | Measured response of SXF13_HCOR_003.hcorrector.\n", - "27 Apr 2026, 15:50:45 | INFO | Measured response of SXF13_HCOR_004.hcorrector.\n", - "27 Apr 2026, 15:50:45 | INFO | Measured response of SXF1_HCOR_004.hcorrector.\n", - "27 Apr 2026, 15:50:46 | INFO | Measured response of SXF11_HCOR_002.hcorrector.\n", - "27 Apr 2026, 15:50:46 | INFO | Measured response of SH2_HCOR_002.hcorrector.\n", - "27 Apr 2026, 15:50:47 | INFO | Measured response of SH1_COR_002.hcorrector.\n", - "27 Apr 2026, 15:50:47 | INFO | Measured response of SH1_COR_003.hcorrector.\n", - "27 Apr 2026, 15:50:48 | INFO | Measured response of SH2_HCOR_003.hcorrector.\n", - "27 Apr 2026, 15:50:48 | INFO | Measured response of SXF11_HCOR_003.hcorrector.\n", - "27 Apr 2026, 15:50:49 | INFO | Measured response of SXF1_HCOR_005.hcorrector.\n", - "27 Apr 2026, 15:50:49 | INFO | Measured response of SXF13_HCOR_005.hcorrector.\n", - "27 Apr 2026, 15:50:49 | INFO | Measured response of SXF13_HCOR_006.hcorrector.\n", - "27 Apr 2026, 15:50:50 | INFO | Measured response of SXF1_HCOR_006.hcorrector.\n", - "27 Apr 2026, 15:50:50 | INFO | Measured response of SXF12_HCOR_003.hcorrector.\n", - "27 Apr 2026, 15:50:51 | INFO | Measured response of SH6_COR_005.hcorrector.\n", - "27 Apr 2026, 15:50:51 | INFO | Measured response of SH4_COR_005.hcorrector.\n", - "27 Apr 2026, 15:50:52 | INFO | Measured response of SH4_COR_006.hcorrector.\n", - "27 Apr 2026, 15:50:52 | INFO | Measured response of SH6_COR_006.hcorrector.\n", - "27 Apr 2026, 15:50:53 | INFO | Measured response of SXF21_HCOR_003.hcorrector.\n", - "27 Apr 2026, 15:50:53 | INFO | Measured response of SXF2_HCOR_003.hcorrector.\n", - "27 Apr 2026, 15:50:53 | INFO | Measured response of SXF22_HCOR_003.hcorrector.\n", - "27 Apr 2026, 15:50:54 | INFO | Measured response of SH9_COR_009.hcorrector.\n", - "27 Apr 2026, 15:50:54 | INFO | Measured response of SH7_COR_009.hcorrector.\n", - "27 Apr 2026, 15:50:55 | INFO | Measured response of SH7_COR_010.hcorrector.\n", - "27 Apr 2026, 15:50:55 | INFO | Measured response of SH9_COR_010.hcorrector.\n", - "27 Apr 2026, 15:50:56 | INFO | Measured response of SXF31_HCOR_003.hcorrector.\n", - "27 Apr 2026, 15:50:56 | INFO | Measured response of SXF3_HCOR_005.hcorrector.\n", - "27 Apr 2026, 15:50:57 | INFO | Measured response of SXF33_HCOR_005.hcorrector.\n", - "27 Apr 2026, 15:50:57 | INFO | Measured response of SXF33_HCOR_006.hcorrector.\n", - "27 Apr 2026, 15:50:58 | INFO | Measured response of SXF3_HCOR_006.hcorrector.\n", - "27 Apr 2026, 15:50:58 | INFO | Measured response of SXF32_HCOR_003.hcorrector.\n", - "27 Apr 2026, 15:50:58 | INFO | Measured response of SH9_COR_011.hcorrector.\n", - "27 Apr 2026, 15:50:59 | INFO | Measured response of SH7_COR_011.hcorrector.\n", - "27 Apr 2026, 15:50:59 | INFO | Measured response of SH7_COR_012.hcorrector.\n", - "27 Apr 2026, 15:51:00 | INFO | Measured response of SH9_COR_012.hcorrector.\n", - "27 Apr 2026, 15:51:00 | INFO | Measured response of SXF41_HCOR_003.hcorrector.\n", - "27 Apr 2026, 15:51:01 | INFO | Measured response of SXF4_HCOR_003.hcorrector.\n", - "27 Apr 2026, 15:51:01 | INFO | Measured response of SXF42_HCOR_003.hcorrector.\n", - "27 Apr 2026, 15:51:01 | INFO | Measured response of SH12_COR_005.hcorrector.\n", - "27 Apr 2026, 15:51:02 | INFO | Measured response of SH10_COR_005.hcorrector.\n", - "27 Apr 2026, 15:51:02 | INFO | Measured response of SH10_COR_006.hcorrector.\n", - "27 Apr 2026, 15:51:03 | INFO | Measured response of SH12_COR_006.hcorrector.\n", - "27 Apr 2026, 15:51:03 | INFO | Measured response of SXF51_HCOR_003.hcorrector.\n", - "27 Apr 2026, 15:51:04 | INFO | Measured response of SXF5_HCOR_005.hcorrector.\n", - "27 Apr 2026, 15:51:04 | INFO | Measured response of SXF53_HCOR_005.hcorrector.\n", - "27 Apr 2026, 15:51:05 | INFO | Measured response of SXF53_HCOR_006.hcorrector.\n", - "27 Apr 2026, 15:51:05 | INFO | Measured response of SXF5_HCOR_006.hcorrector.\n", - "27 Apr 2026, 15:51:05 | INFO | Measured response of SXF52_HCOR_003.hcorrector.\n", - "27 Apr 2026, 15:51:06 | INFO | Measured response of SH14_HCOR_003.hcorrector.\n", - "27 Apr 2026, 15:51:06 | INFO | Measured response of SH13_COR_003.hcorrector.\n", - "27 Apr 2026, 15:51:07 | INFO | Measured response of SH16_COR_003.hcorrector.\n", - "27 Apr 2026, 15:51:07 | INFO | Measured response of SH16_COR_004.hcorrector.\n", - "27 Apr 2026, 15:51:08 | INFO | Measured response of SH13_COR_004.hcorrector.\n", - "27 Apr 2026, 15:51:08 | INFO | Measured response of SH14_HCOR_004.hcorrector.\n", - "27 Apr 2026, 15:51:08 | INFO | Measured response of SXF52_HCOR_004.hcorrector.\n", - "27 Apr 2026, 15:51:09 | INFO | Measured response of SXF5_HCOR_007.hcorrector.\n", - "27 Apr 2026, 15:51:09 | INFO | Measured response of SXF53_HCOR_007.hcorrector.\n", - "27 Apr 2026, 15:51:10 | INFO | Measured response of SXF53_HCOR_008.hcorrector.\n", - "27 Apr 2026, 15:51:10 | INFO | Measured response of SXF5_HCOR_008.hcorrector.\n", - "27 Apr 2026, 15:51:11 | INFO | Measured response of SXF51_HCOR_004.hcorrector.\n", - "27 Apr 2026, 15:51:11 | INFO | Measured response of SH12_COR_007.hcorrector.\n", - "27 Apr 2026, 15:51:12 | INFO | Measured response of SH10_COR_007.hcorrector.\n", - "27 Apr 2026, 15:51:12 | INFO | Measured response of SH10_COR_008.hcorrector.\n", - "27 Apr 2026, 15:51:13 | INFO | Measured response of SH12_COR_008.hcorrector.\n", - "27 Apr 2026, 15:51:13 | INFO | Measured response of SXF42_HCOR_004.hcorrector.\n", - "27 Apr 2026, 15:51:13 | INFO | Measured response of SXF4_HCOR_004.hcorrector.\n", - "27 Apr 2026, 15:51:14 | INFO | Measured response of SXF41_HCOR_004.hcorrector.\n", - "27 Apr 2026, 15:51:14 | INFO | Measured response of SH9_COR_013.hcorrector.\n", - "27 Apr 2026, 15:51:15 | INFO | Measured response of SH7_COR_013.hcorrector.\n", - "27 Apr 2026, 15:51:15 | INFO | Measured response of SH7_COR_014.hcorrector.\n", - "27 Apr 2026, 15:51:16 | INFO | Measured response of SH9_COR_014.hcorrector.\n", - "27 Apr 2026, 15:51:16 | INFO | Measured response of SXF32_HCOR_004.hcorrector.\n", - "27 Apr 2026, 15:51:16 | INFO | Measured response of SXF3_HCOR_007.hcorrector.\n", - "27 Apr 2026, 15:51:17 | INFO | Measured response of SXF33_HCOR_007.hcorrector.\n", - "27 Apr 2026, 15:51:17 | INFO | Measured response of SXF33_HCOR_008.hcorrector.\n", - "27 Apr 2026, 15:51:18 | INFO | Measured response of SXF3_HCOR_008.hcorrector.\n", - "27 Apr 2026, 15:51:18 | INFO | Measured response of SXF31_HCOR_004.hcorrector.\n", - "27 Apr 2026, 15:51:19 | INFO | Measured response of SH9_COR_015.hcorrector.\n", - "27 Apr 2026, 15:51:19 | INFO | Measured response of SH7_COR_015.hcorrector.\n", - "27 Apr 2026, 15:51:19 | INFO | Measured response of SH7_COR_016.hcorrector.\n", - "27 Apr 2026, 15:51:20 | INFO | Measured response of SH9_COR_016.hcorrector.\n", - "27 Apr 2026, 15:51:20 | INFO | Measured response of SXF22_HCOR_004.hcorrector.\n", - "27 Apr 2026, 15:51:21 | INFO | Measured response of SXF2_HCOR_004.hcorrector.\n", - "27 Apr 2026, 15:51:21 | INFO | Measured response of SXF21_HCOR_004.hcorrector.\n", - "27 Apr 2026, 15:51:22 | INFO | Measured response of SH6_COR_007.hcorrector.\n", - "27 Apr 2026, 15:51:22 | INFO | Measured response of SH4_COR_007.hcorrector.\n", - "27 Apr 2026, 15:51:22 | INFO | Measured response of SH4_COR_008.hcorrector.\n", - "27 Apr 2026, 15:51:23 | INFO | Measured response of SH6_COR_008.hcorrector.\n", - "27 Apr 2026, 15:51:23 | INFO | Measured response of SXF12_HCOR_004.hcorrector.\n", - "27 Apr 2026, 15:51:24 | INFO | Measured response of SXF1_HCOR_007.hcorrector.\n", - "27 Apr 2026, 15:51:24 | INFO | Measured response of SXF13_HCOR_007.hcorrector.\n", - "27 Apr 2026, 15:51:24 | INFO | Measured response of SXF13_HCOR_008.hcorrector.\n", - "27 Apr 2026, 15:51:25 | INFO | Measured response of SXF1_HCOR_008.hcorrector.\n", - "27 Apr 2026, 15:51:25 | INFO | Measured response of SXF11_HCOR_004.hcorrector.\n", - "27 Apr 2026, 15:51:26 | INFO | Measured response of SH2_HCOR_004.hcorrector.\n", - "27 Apr 2026, 15:51:26 | INFO | Measured response of SH1_COR_004.hcorrector.\n", - "27 Apr 2026, 15:51:27 | INFO | Measured response of SH1_COR_001.vcorrector.\n", - "27 Apr 2026, 15:51:27 | INFO | Measured response of SH3_VCOR_001.vcorrector.\n", - "27 Apr 2026, 15:51:28 | INFO | Measured response of SXD11_VCOR_001.vcorrector.\n", - "27 Apr 2026, 15:51:28 | INFO | Measured response of SXD1_VCOR_001.vcorrector.\n", - "27 Apr 2026, 15:51:28 | INFO | Measured response of SXD13_VCOR_001.vcorrector.\n", - "27 Apr 2026, 15:51:29 | INFO | Measured response of SXD1_VCOR_002.vcorrector.\n", - "27 Apr 2026, 15:51:29 | INFO | Measured response of SXD1_VCOR_003.vcorrector.\n", - "27 Apr 2026, 15:51:30 | INFO | Measured response of SXD12_VCOR_001.vcorrector.\n", - "27 Apr 2026, 15:51:30 | INFO | Measured response of SH6_COR_001.vcorrector.\n", - "27 Apr 2026, 15:51:30 | INFO | Measured response of SH4_COR_001.vcorrector.\n", - "27 Apr 2026, 15:51:31 | INFO | Measured response of SH4_COR_002.vcorrector.\n", - "27 Apr 2026, 15:51:31 | INFO | Measured response of SH6_COR_002.vcorrector.\n", - "27 Apr 2026, 15:51:32 | INFO | Measured response of SXD21_VCOR_001.vcorrector.\n", - "27 Apr 2026, 15:51:32 | INFO | Measured response of SXD2_VCOR_001.vcorrector.\n", - "27 Apr 2026, 15:51:33 | INFO | Measured response of SXD22_VCOR_001.vcorrector.\n", - "27 Apr 2026, 15:51:33 | INFO | Measured response of SH9_COR_001.vcorrector.\n", - "27 Apr 2026, 15:51:33 | INFO | Measured response of SH7_COR_001.vcorrector.\n", - "27 Apr 2026, 15:51:34 | INFO | Measured response of SH7_COR_002.vcorrector.\n", - "27 Apr 2026, 15:51:34 | INFO | Measured response of SH9_COR_002.vcorrector.\n", - "27 Apr 2026, 15:51:35 | INFO | Measured response of SXD31_VCOR_001.vcorrector.\n", - "27 Apr 2026, 15:51:35 | INFO | Measured response of SXD3_VCOR_001.vcorrector.\n", - "27 Apr 2026, 15:51:36 | INFO | Measured response of SXD33_VCOR_001.vcorrector.\n", - "27 Apr 2026, 15:51:36 | INFO | Measured response of SXD3_VCOR_002.vcorrector.\n", - "27 Apr 2026, 15:51:37 | INFO | Measured response of SXD3_VCOR_003.vcorrector.\n", - "27 Apr 2026, 15:51:37 | INFO | Measured response of SXD32_VCOR_001.vcorrector.\n", - "27 Apr 2026, 15:51:37 | INFO | Measured response of SH9_COR_003.vcorrector.\n", - "27 Apr 2026, 15:51:38 | INFO | Measured response of SH7_COR_003.vcorrector.\n", - "27 Apr 2026, 15:51:38 | INFO | Measured response of SH7_COR_004.vcorrector.\n", - "27 Apr 2026, 15:51:39 | INFO | Measured response of SH9_COR_004.vcorrector.\n", - "27 Apr 2026, 15:51:39 | INFO | Measured response of SXD41_VCOR_001.vcorrector.\n", - "27 Apr 2026, 15:51:40 | INFO | Measured response of SXD4_VCOR_001.vcorrector.\n", - "27 Apr 2026, 15:51:40 | INFO | Measured response of SXD42_VCOR_001.vcorrector.\n", - "27 Apr 2026, 15:51:40 | INFO | Measured response of SH12_COR_001.vcorrector.\n", - "27 Apr 2026, 15:51:41 | INFO | Measured response of SH10_COR_001.vcorrector.\n", - "27 Apr 2026, 15:51:41 | INFO | Measured response of SH10_COR_002.vcorrector.\n", - "27 Apr 2026, 15:51:42 | INFO | Measured response of SH12_COR_002.vcorrector.\n", - "27 Apr 2026, 15:51:42 | INFO | Measured response of SXD51_VCOR_001.vcorrector.\n", - "27 Apr 2026, 15:51:42 | INFO | Measured response of SXD5_VCOR_001.vcorrector.\n", - "27 Apr 2026, 15:51:43 | INFO | Measured response of SXD53_VCOR_001.vcorrector.\n", - "27 Apr 2026, 15:51:43 | INFO | Measured response of SXD5_VCOR_002.vcorrector.\n", - "27 Apr 2026, 15:51:44 | INFO | Measured response of SXD5_VCOR_003.vcorrector.\n", - "27 Apr 2026, 15:51:44 | INFO | Measured response of SXD52_VCOR_001.vcorrector.\n", - "27 Apr 2026, 15:51:45 | INFO | Measured response of SH15_VCOR_001.vcorrector.\n", - "27 Apr 2026, 15:51:45 | INFO | Measured response of SH13_COR_001.vcorrector.\n", - "27 Apr 2026, 15:51:46 | INFO | Measured response of SH16_COR_001.vcorrector.\n", - "27 Apr 2026, 15:51:46 | INFO | Measured response of SH16_COR_002.vcorrector.\n", - "27 Apr 2026, 15:51:46 | INFO | Measured response of SH13_COR_002.vcorrector.\n", - "27 Apr 2026, 15:51:47 | INFO | Measured response of SH15_VCOR_002.vcorrector.\n", - "27 Apr 2026, 15:51:47 | INFO | Measured response of SXD52_VCOR_002.vcorrector.\n", - "27 Apr 2026, 15:51:48 | INFO | Measured response of SXD5_VCOR_004.vcorrector.\n", - "27 Apr 2026, 15:51:48 | INFO | Measured response of SXD53_VCOR_002.vcorrector.\n", - "27 Apr 2026, 15:51:49 | INFO | Measured response of SXD5_VCOR_005.vcorrector.\n", - "27 Apr 2026, 15:51:49 | INFO | Measured response of SXD5_VCOR_006.vcorrector.\n", - "27 Apr 2026, 15:51:50 | INFO | Measured response of SXD51_VCOR_002.vcorrector.\n", - "27 Apr 2026, 15:51:50 | INFO | Measured response of SH12_COR_003.vcorrector.\n", - "27 Apr 2026, 15:51:51 | INFO | Measured response of SH10_COR_003.vcorrector.\n", - "27 Apr 2026, 15:51:51 | INFO | Measured response of SH10_COR_004.vcorrector.\n", - "27 Apr 2026, 15:51:51 | INFO | Measured response of SH12_COR_004.vcorrector.\n", - "27 Apr 2026, 15:51:52 | INFO | Measured response of SXD42_VCOR_002.vcorrector.\n", - "27 Apr 2026, 15:51:52 | INFO | Measured response of SXD4_VCOR_002.vcorrector.\n", - "27 Apr 2026, 15:51:53 | INFO | Measured response of SXD41_VCOR_002.vcorrector.\n", - "27 Apr 2026, 15:51:53 | INFO | Measured response of SH9_COR_005.vcorrector.\n", - "27 Apr 2026, 15:51:54 | INFO | Measured response of SH7_COR_005.vcorrector.\n", - "27 Apr 2026, 15:51:54 | INFO | Measured response of SH7_COR_006.vcorrector.\n", - "27 Apr 2026, 15:51:54 | INFO | Measured response of SH9_COR_006.vcorrector.\n", - "27 Apr 2026, 15:51:55 | INFO | Measured response of SXD32_VCOR_002.vcorrector.\n", - "27 Apr 2026, 15:51:55 | INFO | Measured response of SXD3_VCOR_004.vcorrector.\n", - "27 Apr 2026, 15:51:56 | INFO | Measured response of SXD33_VCOR_002.vcorrector.\n", - "27 Apr 2026, 15:51:56 | INFO | Measured response of SXD3_VCOR_005.vcorrector.\n", - "27 Apr 2026, 15:51:57 | INFO | Measured response of SXD3_VCOR_006.vcorrector.\n", - "27 Apr 2026, 15:51:57 | INFO | Measured response of SXD31_VCOR_002.vcorrector.\n", - "27 Apr 2026, 15:51:57 | INFO | Measured response of SH9_COR_007.vcorrector.\n", - "27 Apr 2026, 15:51:58 | INFO | Measured response of SH7_COR_007.vcorrector.\n", - "27 Apr 2026, 15:51:58 | INFO | Measured response of SH7_COR_008.vcorrector.\n", - "27 Apr 2026, 15:51:59 | INFO | Measured response of SH9_COR_008.vcorrector.\n", - "27 Apr 2026, 15:51:59 | INFO | Measured response of SXD22_VCOR_002.vcorrector.\n", - "27 Apr 2026, 15:52:00 | INFO | Measured response of SXD2_VCOR_002.vcorrector.\n", - "27 Apr 2026, 15:52:00 | INFO | Measured response of SXD21_VCOR_002.vcorrector.\n", - "27 Apr 2026, 15:52:00 | INFO | Measured response of SH6_COR_003.vcorrector.\n", - "27 Apr 2026, 15:52:01 | INFO | Measured response of SH4_COR_003.vcorrector.\n", - "27 Apr 2026, 15:52:01 | INFO | Measured response of SH4_COR_004.vcorrector.\n", - "27 Apr 2026, 15:52:02 | INFO | Measured response of SH6_COR_004.vcorrector.\n", - "27 Apr 2026, 15:52:02 | INFO | Measured response of SXD12_VCOR_002.vcorrector.\n", - "27 Apr 2026, 15:52:03 | INFO | Measured response of SXD1_VCOR_004.vcorrector.\n", - "27 Apr 2026, 15:52:03 | INFO | Measured response of SXD13_VCOR_002.vcorrector.\n", - "27 Apr 2026, 15:52:04 | INFO | Measured response of SXD1_VCOR_005.vcorrector.\n", - "27 Apr 2026, 15:52:04 | INFO | Measured response of SXD1_VCOR_006.vcorrector.\n", - "27 Apr 2026, 15:52:04 | INFO | Measured response of SXD11_VCOR_002.vcorrector.\n", - "27 Apr 2026, 15:52:05 | INFO | Measured response of SH3_VCOR_002.vcorrector.\n", - "27 Apr 2026, 15:52:05 | INFO | Measured response of SH1_COR_002.vcorrector.\n", - "27 Apr 2026, 15:52:06 | INFO | Measured response of SH1_COR_003.vcorrector.\n", - "27 Apr 2026, 15:52:06 | INFO | Measured response of SH3_VCOR_003.vcorrector.\n", - "27 Apr 2026, 15:52:07 | INFO | Measured response of SXD11_VCOR_003.vcorrector.\n", - "27 Apr 2026, 15:52:07 | INFO | Measured response of SXD1_VCOR_007.vcorrector.\n", - "27 Apr 2026, 15:52:08 | INFO | Measured response of SXD13_VCOR_003.vcorrector.\n", - "27 Apr 2026, 15:52:08 | INFO | Measured response of SXD1_VCOR_008.vcorrector.\n", - "27 Apr 2026, 15:52:08 | INFO | Measured response of SXD1_VCOR_009.vcorrector.\n", - "27 Apr 2026, 15:52:09 | INFO | Measured response of SXD12_VCOR_003.vcorrector.\n", - "27 Apr 2026, 15:52:09 | INFO | Measured response of SH6_COR_005.vcorrector.\n", - "27 Apr 2026, 15:52:10 | INFO | Measured response of SH4_COR_005.vcorrector.\n", - "27 Apr 2026, 15:52:10 | INFO | Measured response of SH4_COR_006.vcorrector.\n", - "27 Apr 2026, 15:52:11 | INFO | Measured response of SH6_COR_006.vcorrector.\n", - "27 Apr 2026, 15:52:11 | INFO | Measured response of SXD21_VCOR_003.vcorrector.\n", - "27 Apr 2026, 15:52:12 | INFO | Measured response of SXD2_VCOR_003.vcorrector.\n", - "27 Apr 2026, 15:52:12 | INFO | Measured response of SXD22_VCOR_003.vcorrector.\n", - "27 Apr 2026, 15:52:12 | INFO | Measured response of SH9_COR_009.vcorrector.\n", - "27 Apr 2026, 15:52:13 | INFO | Measured response of SH7_COR_009.vcorrector.\n", - "27 Apr 2026, 15:52:13 | INFO | Measured response of SH7_COR_010.vcorrector.\n", - "27 Apr 2026, 15:52:14 | INFO | Measured response of SH9_COR_010.vcorrector.\n", - "27 Apr 2026, 15:52:14 | INFO | Measured response of SXD31_VCOR_003.vcorrector.\n", - "27 Apr 2026, 15:52:15 | INFO | Measured response of SXD3_VCOR_007.vcorrector.\n", - "27 Apr 2026, 15:52:15 | INFO | Measured response of SXD33_VCOR_003.vcorrector.\n", - "27 Apr 2026, 15:52:15 | INFO | Measured response of SXD3_VCOR_008.vcorrector.\n", - "27 Apr 2026, 15:52:16 | INFO | Measured response of SXD3_VCOR_009.vcorrector.\n", - "27 Apr 2026, 15:52:16 | INFO | Measured response of SXD32_VCOR_003.vcorrector.\n", - "27 Apr 2026, 15:52:17 | INFO | Measured response of SH9_COR_011.vcorrector.\n", - "27 Apr 2026, 15:52:17 | INFO | Measured response of SH7_COR_011.vcorrector.\n", - "27 Apr 2026, 15:52:18 | INFO | Measured response of SH7_COR_012.vcorrector.\n", - "27 Apr 2026, 15:52:18 | INFO | Measured response of SH9_COR_012.vcorrector.\n", - "27 Apr 2026, 15:52:18 | INFO | Measured response of SXD41_VCOR_003.vcorrector.\n", - "27 Apr 2026, 15:52:19 | INFO | Measured response of SXD4_VCOR_003.vcorrector.\n", - "27 Apr 2026, 15:52:19 | INFO | Measured response of SXD42_VCOR_003.vcorrector.\n", - "27 Apr 2026, 15:52:20 | INFO | Measured response of SH12_COR_005.vcorrector.\n", - "27 Apr 2026, 15:52:20 | INFO | Measured response of SH10_COR_005.vcorrector.\n", - "27 Apr 2026, 15:52:21 | INFO | Measured response of SH10_COR_006.vcorrector.\n", - "27 Apr 2026, 15:52:21 | INFO | Measured response of SH12_COR_006.vcorrector.\n", - "27 Apr 2026, 15:52:21 | INFO | Measured response of SXD51_VCOR_003.vcorrector.\n", - "27 Apr 2026, 15:52:22 | INFO | Measured response of SXD5_VCOR_007.vcorrector.\n", - "27 Apr 2026, 15:52:22 | INFO | Measured response of SXD53_VCOR_003.vcorrector.\n", - "27 Apr 2026, 15:52:23 | INFO | Measured response of SXD5_VCOR_008.vcorrector.\n", - "27 Apr 2026, 15:52:23 | INFO | Measured response of SXD5_VCOR_009.vcorrector.\n", - "27 Apr 2026, 15:52:24 | INFO | Measured response of SXD52_VCOR_003.vcorrector.\n", - "27 Apr 2026, 15:52:24 | INFO | Measured response of SH15_VCOR_003.vcorrector.\n", - "27 Apr 2026, 15:52:24 | INFO | Measured response of SH13_COR_003.vcorrector.\n", - "27 Apr 2026, 15:52:25 | INFO | Measured response of SH16_COR_003.vcorrector.\n", - "27 Apr 2026, 15:52:25 | INFO | Measured response of SH16_COR_004.vcorrector.\n", - "27 Apr 2026, 15:52:26 | INFO | Measured response of SH13_COR_004.vcorrector.\n", - "27 Apr 2026, 15:52:26 | INFO | Measured response of SH15_VCOR_004.vcorrector.\n", - "27 Apr 2026, 15:52:27 | INFO | Measured response of SXD52_VCOR_004.vcorrector.\n", - "27 Apr 2026, 15:52:27 | INFO | Measured response of SXD5_VCOR_010.vcorrector.\n", - "27 Apr 2026, 15:52:27 | INFO | Measured response of SXD53_VCOR_004.vcorrector.\n", - "27 Apr 2026, 15:52:28 | INFO | Measured response of SXD5_VCOR_011.vcorrector.\n", - "27 Apr 2026, 15:52:28 | INFO | Measured response of SXD5_VCOR_012.vcorrector.\n", - "27 Apr 2026, 15:52:29 | INFO | Measured response of SXD51_VCOR_004.vcorrector.\n", - "27 Apr 2026, 15:52:29 | INFO | Measured response of SH12_COR_007.vcorrector.\n", - "27 Apr 2026, 15:52:30 | INFO | Measured response of SH10_COR_007.vcorrector.\n", - "27 Apr 2026, 15:52:30 | INFO | Measured response of SH10_COR_008.vcorrector.\n", - "27 Apr 2026, 15:52:31 | INFO | Measured response of SH12_COR_008.vcorrector.\n", - "27 Apr 2026, 15:52:31 | INFO | Measured response of SXD42_VCOR_004.vcorrector.\n", - "27 Apr 2026, 15:52:31 | INFO | Measured response of SXD4_VCOR_004.vcorrector.\n", - "27 Apr 2026, 15:52:32 | INFO | Measured response of SXD41_VCOR_004.vcorrector.\n", - "27 Apr 2026, 15:52:32 | INFO | Measured response of SH9_COR_013.vcorrector.\n", - "27 Apr 2026, 15:52:33 | INFO | Measured response of SH7_COR_013.vcorrector.\n", - "27 Apr 2026, 15:52:33 | INFO | Measured response of SH7_COR_014.vcorrector.\n", - "27 Apr 2026, 15:52:34 | INFO | Measured response of SH9_COR_014.vcorrector.\n", - "27 Apr 2026, 15:52:34 | INFO | Measured response of SXD32_VCOR_004.vcorrector.\n", - "27 Apr 2026, 15:52:34 | INFO | Measured response of SXD3_VCOR_010.vcorrector.\n", - "27 Apr 2026, 15:52:35 | INFO | Measured response of SXD33_VCOR_004.vcorrector.\n", - "27 Apr 2026, 15:52:35 | INFO | Measured response of SXD3_VCOR_011.vcorrector.\n", - "27 Apr 2026, 15:52:36 | INFO | Measured response of SXD3_VCOR_012.vcorrector.\n", - "27 Apr 2026, 15:52:36 | INFO | Measured response of SXD31_VCOR_004.vcorrector.\n", - "27 Apr 2026, 15:52:37 | INFO | Measured response of SH9_COR_015.vcorrector.\n", - "27 Apr 2026, 15:52:37 | INFO | Measured response of SH7_COR_015.vcorrector.\n", - "27 Apr 2026, 15:52:38 | INFO | Measured response of SH7_COR_016.vcorrector.\n", - "27 Apr 2026, 15:52:38 | INFO | Measured response of SH9_COR_016.vcorrector.\n", - "27 Apr 2026, 15:52:38 | INFO | Measured response of SXD22_VCOR_004.vcorrector.\n", - "27 Apr 2026, 15:52:39 | INFO | Measured response of SXD2_VCOR_004.vcorrector.\n", - "27 Apr 2026, 15:52:39 | INFO | Measured response of SXD21_VCOR_004.vcorrector.\n", - "27 Apr 2026, 15:52:40 | INFO | Measured response of SH6_COR_007.vcorrector.\n", - "27 Apr 2026, 15:52:40 | INFO | Measured response of SH4_COR_007.vcorrector.\n", - "27 Apr 2026, 15:52:41 | INFO | Measured response of SH4_COR_008.vcorrector.\n", - "27 Apr 2026, 15:52:41 | INFO | Measured response of SH6_COR_008.vcorrector.\n", - "27 Apr 2026, 15:52:41 | INFO | Measured response of SXD12_VCOR_004.vcorrector.\n", - "27 Apr 2026, 15:52:42 | INFO | Measured response of SXD1_VCOR_010.vcorrector.\n", - "27 Apr 2026, 15:52:42 | INFO | Measured response of SXD13_VCOR_004.vcorrector.\n", - "27 Apr 2026, 15:52:43 | INFO | Measured response of SXD1_VCOR_011.vcorrector.\n", - "27 Apr 2026, 15:52:43 | INFO | Measured response of SXD1_VCOR_012.vcorrector.\n", - "27 Apr 2026, 15:52:44 | INFO | Measured response of SXD11_VCOR_004.vcorrector.\n", - "27 Apr 2026, 15:52:44 | INFO | Measured response of SH3_VCOR_004.vcorrector.\n", - "27 Apr 2026, 15:52:44 | INFO | Measured response of SH1_COR_004.vcorrector.\n" - ] - }, - { - "data": { - "text/plain": [ - "True" - ] - }, - "execution_count": 7, - "metadata": {}, - "output_type": "execute_result" - } - ], - "source": [ - "orbit_response_matrix.measure()" - ] - }, - { - "cell_type": "code", - "execution_count": 8, - "id": "2fd3fe46-6156-4b1d-a269-7c8c7b22ee92", - "metadata": {}, - "outputs": [], - "source": [ - "ormdata = orbit_response_matrix.get()" - ] - }, - { - "cell_type": "markdown", - "id": "d00f9cd7-739e-4a85-a5c6-a1229d8b3155", - "metadata": {}, - "source": [ - "Let's visualise the orbit response matrix" - ] - }, - { - "cell_type": "code", - "execution_count": 9, - "id": "7e0ddfe2-241b-4ee1-9eb2-bee4fe06ce03", - "metadata": {}, - "outputs": [ - { - "data": { - "text/plain": [ - "" - ] - }, - "execution_count": 9, - "metadata": {}, - "output_type": "execute_result" - }, - { - "data": { - "image/png": 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", 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" - ] - }, - "metadata": {}, - "output_type": "display_data" - } - ], - "source": [ - "plt.imshow(np.array(ormdata[\"matrix\"]))" - ] - }, - { - "cell_type": "markdown", - "id": "1839afbf-10fe-4b8d-9ed2-38b6e77de57a", - "metadata": {}, - "source": [ - "The response matrix can be save to a file." - ] - }, - { - "cell_type": "code", - "execution_count": 10, - "id": "79628252-7eea-44f1-83f9-5c032dbd75d6", - "metadata": {}, - "outputs": [], - "source": [ - "orbit_response_matrix.save(\"orm.json\")" - ] - }, - { - "cell_type": "markdown", - "id": "ddb679e6-0be7-476f-a857-6d3dd746bfb2", - "metadata": {}, - "source": [ - "To do orbit correction we will need to load the file to the orbit correction object." - ] - }, - { - "cell_type": "code", - "execution_count": 11, - "id": "6c306621-7cc2-45ce-bd5c-e714efe928ab", - "metadata": {}, - "outputs": [ - { - "name": "stdout", - "output_type": "stream", - "text": [ - "27 Apr 2026, 15:52:46 | INFO | Setting the rf_weight by default to inf.\n" - ] - } - ], - "source": [ - "orbit_correction.load(\"orm.json\")" - ] - }, - { - "cell_type": "markdown", - "id": "9cdc7159-bbad-465b-aed9-039e3d4ef073", - "metadata": {}, - "source": [ - "### Mangle orbit for design mode\n", - "To have some orbit in the design mode we have to mangle it by introducing some noise on the H and V correctors. " - ] - }, - { - "cell_type": "code", - "execution_count": 12, - "id": "7c0c30e7-a6f8-458e-a4d5-02f0ca63ad19", - "metadata": {}, - "outputs": [], - "source": [ - "std_kick = 1e-6\n", - "hcorr = control_mode.get_magnets(\"HCORR\")\n", - "vcorr = control_mode.get_magnets(\"VCORR\")\n", - "bpms = control_mode.get_bpms(\"BPM\")\n", - "ref_h, ref_v = control_mode.get_bpms(\"BPM\").positions.get().T\n", - "reference = np.concat((ref_h, ref_v))\n", - "# mangle orbit\n", - "hcorr.strengths.set(hcorr.strengths.get() + std_kick * np.random.normal(size=len(hcorr)))\n", - "vcorr.strengths.set(vcorr.strengths.get() + std_kick * np.random.normal(size=len(vcorr)))" - ] - }, - { - "cell_type": "code", - "execution_count": 13, - "id": "a771c0f2-d09a-4ae6-ae95-f0416f6c570b", - "metadata": {}, - "outputs": [ - { - "name": "stdout", - "output_type": "stream", - "text": [ - "R.m.s. orbit before correction H: 53.6 µm, V: 23.5 µm.\n" - ] - } - ], - "source": [ - "positions_bc = bpms.positions.get()\n", - "std_bc = np.std(positions_bc, axis=0)\n", - "sleep(2)\n", - "print(f\"R.m.s. orbit before correction H: {1e6 * std_bc[0]: .1f} µm, V: {1e6 * std_bc[1]: .1f} µm.\")" - ] - }, - { - "cell_type": "markdown", - "id": "6a6a21e4-3885-4f8c-8e30-36fa74563064", - "metadata": {}, - "source": [ - "Let's visualise the mangled orbit before the correction is applied" - ] - }, - { - "cell_type": "code", - "execution_count": 14, - "id": "5785e582-a8ff-4464-a759-fe731f197420", - "metadata": {}, - "outputs": [ - { - "data": { - "text/plain": [ - "Text(0, 0.5, 'Orbit')" - ] - }, - "execution_count": 14, - "metadata": {}, - "output_type": "execute_result" - }, - { - "data": { - "image/png": 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", - "text/plain": [ - "
" - ] - }, - "metadata": {}, - "output_type": "display_data" - } - ], - "source": [ - "import matplotlib.pyplot as plt\n", - "\n", - "plt.plot(positions_bc[:, 0], label=\"H\")\n", - "plt.plot(positions_bc[:, 1], label=\"V\")\n", - "plt.xlabel(\"BPM number\")\n", - "plt.ylabel(\"Orbit\")" - ] - }, - { - "cell_type": "code", - "execution_count": 20, - "id": "55a46fa6-14fe-497a-891e-a0dcdc1fec88", - "metadata": {}, - "outputs": [ - { - "name": "stdout", - "output_type": "stream", - "text": [ - "27 Apr 2026, 15:52:51 | INFO | (Re-)Building pseudoinverse RM with method='svd_values', parameter=16, plane='H', virtual=True, rf=False.\n", - "27 Apr 2026, 15:52:52 | INFO | (Re-)Building pseudoinverse RM with method='svd_values', parameter=16, plane='V', virtual=False, rf=False.\n" - ] - }, - { - "data": { - "text/plain": [ - "" - ] - }, - "execution_count": 20, - "metadata": {}, - "output_type": "execute_result" - }, - { - "data": { - "image/png": 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- "text/plain": [ - "
" - ] - }, - "metadata": {}, - "output_type": "display_data" - } - ], - "source": [ - "plt.plot(positions_bc[:, 0], label=\"H (before corr)\", color=\"b\", ls=\"--\")\n", - "plt.plot(positions_bc[:, 1], label=\"V (before corr)\", color=\"r\", ls=\"--\")\n", - "\n", - "orbit_correction.correct(reference=reference)\n", - "\n", - "positions_after = bpms.positions.get()\n", - "plt.plot(positions_after[:, 0], label=\"H (after corr)\", color=\"b\", ls=\"-\")\n", - "plt.plot(positions_after[:, 1], label=\"V (after corr)\", color=\"r\", ls=\"-\")\n", - "\n", - "plt.xlabel(\"BPM number\")\n", - "plt.ylabel(\"Orbit\")\n", - "plt.legend()" - ] - } - ], - "metadata": { - "kernelspec": { - "display_name": "Python 3 (ipykernel)", - "language": "python", - "name": "python3" - }, - "language_info": { - "codemirror_mode": { - "name": "ipython", - "version": 3 - }, - "file_extension": ".py", - "mimetype": "text/x-python", - "name": "python", - "nbconvert_exporter": "python", - "pygments_lexer": "ipython3", - "version": "3.12.3" - } - }, - "nbformat": 4, - "nbformat_minor": 5 -} diff --git a/examples/SOLEIL_examples/README.md b/examples/SOLEIL_examples/README.md deleted file mode 100644 index 1e05b7023..000000000 --- a/examples/SOLEIL_examples/README.md +++ /dev/null @@ -1,79 +0,0 @@ -# Instructions for how to run SOLEIL examples. - -## Install pyAML - -1. Create a virtual environment and activate it. You need to have Python 3.11+. - -2. Install pyAML, including the tango-pyaml TANGO bindings. - - ```bash - pip install accelerator-middle-layer[tango-pyaml] - ``` -3. Alternatively, you can install ophyd-async Tango bindings - ```bash - pip install accelerator-middle-layer[pyaml-cs-oa] - ``` - -If this does not work, you can proceed to do a developer installation directly from git repository. -```bash -# pyAML core -git clone git@github.com:python-accelerator-middle-layer/pyaml.git -cd pyaml -pip install -e .[dev] -# pyAML TANGO bindings -git clone git@github.com:python-accelerator-middle-layer/tango-pyaml.git -cd tango-pyaml -pip install -e . -#pyAML ophyd-async bindings (supports both TANGO and EPICS) -git clone git@github.com:python-accelerator-middle-layer/pyaml-cs-oa.git -cd pyaml-cs-oa -pip install -e . -``` - -You can verify that everything is installed correctly by running in Python or IPython terminal the start of the examples. - -```python -from pyaml.accelerator import Accelerator - -sr = Accelerator.load("p.yaml") -sr # string representation -``` - -The following or a similar message will be printed -``` -Accelerator(facility='Synchrotron SOLEIL', machine='sr', energy=2750000000.0, controls=[TangoControlSystem(name='live', tango_host='localhost:11000', debug_level=None, lazy_devices=True, scalar_aggregator='tango.pyaml.multi_attribute', vector_aggregator=None, timeout_ms=3000)], simulators=[Simulator(name='design', lattice='SOLEIL_II_V3631_sym1_V001_database_rf.m', mat_key=None, linker=, description=None)], data_folder='/data/store', description=None) -``` - -pyAML has two control modes: "live" and "design" (named in the config file). "live" connects to a control system (or a control system emulator), "design" only requires pyAT lattice file and will run pyAT. If you want to avoid having any control system connection, you can delete "controls: " section from the configuration file. - -### Start the SOLEIL II virtual accelerator - -SOLEIL II virtual accelerator is an emulation of TANGO control system that runs pyAT under the hood. - -1. Install [Apptainer](https://apptainer.org/docs/admin/main/installation.html) in case you don't already have it. - -For the live control mode, you should have some control system emulation running. It is possible to do -``` -apptainer pull -F virtual-accelerator.sif oras://gitlab-registry.synchrotron-soleil.fr/software-control-system/containers/apptainer/virtual-accelerator:latest -apptainer run virtual-accelerator.sif -``` - -***Keep this terminal running and don't do anything else in it.*** The virtual accelerator will run there, and you will be able to interact with it from other terminals, jupyter notebooks, IDEs, etc., over the network. If you want to put it in the background, using something like tmux would be a good option. - -This will run SOLEIL II proof-of-concept digital twin on localhost:11000. You can play with the digital twin itself (without pyAML) via jive to check that everything is working. You can run Jive in a different terminal with -``` -apptainer pull -F jive.sif https://gitlab.synchrotron-soleil.fr/api/v4/projects/2739/packages/generic/jive/latest/jive.sif -apptainer run jive.sif -``` -On Linux you may need to configure X11 to display Jive -``` -export DISPLAY=:0 -xhost +local:root -``` - -NOTE: This is just a demonstration of pyAML functionality. Certain things may be done stupidly. The person who wrote this jupyter notebook only cared about showing that the code is working, not about intelligently controlling the accelerator. - - - ## Run the examples - - There are three jupyter notebook available with some basic examples. Feel free to play around and modify them. The main configuration entry point is `p.yaml`; it now loads `arrays.yaml`, `devices.yaml`, and `tuning_tools.yaml`, all generated procedurally from the .m lattice file and nomenclature description file. diff --git a/examples/SOLEIL_examples/devices.yaml b/examples/SOLEIL_examples/devices.yaml deleted file mode 100644 index 5bb1e0700..000000000 --- a/examples/SOLEIL_examples/devices.yaml +++ /dev/null @@ -1,13208 +0,0 @@ -- type: pyaml.bpm.bpm - name: BPM_001 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN01-SD/DG-EPOS/BPM.02/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN01-SD/DG-EPOS/BPM.02/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SH1_COR_001 - mapping: - - [B2, SH1_COR_001.sextupole] - - [B0, SH1_COR_001.hcorrector] - - [A0, SH1_COR_001.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0, A0] - units: [1/m**2, '1', '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN01-AR/EM-SX/SHF.01/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN01-AR/EM-COR/SHF.01-CDLH.01/strength - unit: '1' - - type: tango.pyaml.attribute - attribute: AN01-AR/EM-COR/SHF.01-CDLV.01/strength - unit: '1' -- type: pyaml.magnet.cfm_magnet - name: OH1_QCORROCT_1_QT_001 - mapping: - - [B3, OH1_QCORROCT_1_QT_001.octupole] - - [B1, OH1_QCORROCT_1_QT_001.quadrupole] - - [A1, OH1_QCORROCT_1_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN01-AR/EM-OCT/OH.01/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN01-AR/EM-COR/OH.01-CQLN.01/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN01-AR/EM-COR/OH.01-CQLT.01/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SH2_HCOR_001 - mapping: - - [B2, SH2_HCOR_001.sextupole] - - [B0, SH2_HCOR_001.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN01-AR/EM-SX/SHD.02/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN01-AR/EM-COR/SHD.02-CDLH.02/strength - unit: '1' -- type: pyaml.magnet.cfm_magnet - name: OH2_QCORROCT_2_001 - mapping: - - [B3, OH2_QCORROCT_2_001.octupole] - - [B1, OH2_QCORROCT_2_001.quadrupole] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1] - units: [1/m**3, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN01-AR/EM-OCT/OH.02/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN01-AR/EM-COR/OH.02-CQLN.02/strength - unit: 1/m**2 -- type: pyaml.bpm.bpm - name: BPM_002 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN01-AR/DG-EPOS/BPM.03/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN01-AR/DG-EPOS/BPM.03/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SH3_VCOR_001 - mapping: - - [B2, SH3_VCOR_001.sextupole] - - [A0, SH3_VCOR_001.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN01-AR/EM-SX/SHD.03/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN01-AR/EM-COR/SHD.03-CDLV.02/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_001 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN01-AR/EM-COR/CQLN.03/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SXD11_001 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN01-AR/EM-SX/SCD.01/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: OCTF1_QCORROCT_3_QT_001 - mapping: - - [B3, OCTF1_QCORROCT_3_QT_001.octupole] - - [B1, OCTF1_QCORROCT_3_QT_001.quadrupole] - - [A1, OCTF1_QCORROCT_3_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN01-AR/EM-OCT/OC.01/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN01-AR/EM-COR/OC.01-CQLN.04/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN01-AR/EM-COR/OC.01-CQLT.02/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF11_HCOR_001 - mapping: - - [B2, SXF11_HCOR_001.sextupole] - - [B0, SXF11_HCOR_001.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN01-AR/EM-SX/SCF.02/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN01-AR/EM-COR/SCF.02-CDLH.03/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_003 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN01-AR/DG-EPOS/BPM.04/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN01-AR/DG-EPOS/BPM.04/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SXD11_VCOR_001 - mapping: - - [B2, SXD11_VCOR_001.sextupole] - - [A0, SXD11_VCOR_001.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN01-AR/EM-SX/SCD.03/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN01-AR/EM-COR/SCD.03-CDLV.03/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_002 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN01-AR/EM-COR/CQLN.05/strength - unit: 1/m -- type: pyaml.magnet.quadrupole - name: QCORR_003 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN01-AR/EM-COR/CQLN.06/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SXD1_001 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN01-AR/EM-SX/SCD.04/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: OCTF1_QCORROCT_4_QT_001 - mapping: - - [B3, OCTF1_QCORROCT_4_QT_001.octupole] - - [B1, OCTF1_QCORROCT_4_QT_001.quadrupole] - - [A1, OCTF1_QCORROCT_4_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN01-AR/EM-OCT/OC.02/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN01-AR/EM-COR/OC.02-CQLN.07/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN01-AR/EM-COR/OC.02-CQLT.03/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF1_HCOR_001 - mapping: - - [B2, SXF1_HCOR_001.sextupole] - - [B0, SXF1_HCOR_001.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN01-AR/EM-SX/SCF.05/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN01-AR/EM-COR/SCF.05-CDLH.04/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_004 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN01-AR/DG-EPOS/BPM.05/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN01-AR/DG-EPOS/BPM.05/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SXD1_VCOR_001 - mapping: - - [B2, SXD1_VCOR_001.sextupole] - - [A0, SXD1_VCOR_001.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN01-AR/EM-SX/SCD.06/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN01-AR/EM-COR/SCD.06-CDLV.04/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_004 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN01-AR/EM-COR/CQLN.08/strength - unit: 1/m -- type: pyaml.magnet.quadrupole - name: QCORR_005 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN01-AR/EM-COR/CQLN.09/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SXD1_002 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN01-AR/EM-SX/SCD.07/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: OCTF1_QCORROCT_5_QT_001 - mapping: - - [B3, OCTF1_QCORROCT_5_QT_001.octupole] - - [B1, OCTF1_QCORROCT_5_QT_001.quadrupole] - - [A1, OCTF1_QCORROCT_5_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN01-AR/EM-OCT/OC.03/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN01-AR/EM-COR/OC.03-CQLN.10/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN01-AR/EM-COR/OC.03-CQLT.04/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF13_HCOR_001 - mapping: - - [B2, SXF13_HCOR_001.sextupole] - - [B0, SXF13_HCOR_001.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN01-AR/EM-SX/SCF.08/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN01-AR/EM-COR/SCF.08-CDLH.05/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_005 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN01-AR/DG-EPOS/BPM.06/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN01-AR/DG-EPOS/BPM.06/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SXD13_VCOR_001 - mapping: - - [B2, SXD13_VCOR_001.sextupole] - - [A0, SXD13_VCOR_001.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN01-AR/EM-SX/SCD.09/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN01-AR/EM-COR/SCD.09-CDLV.05/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_006 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN01-AR/EM-COR/CQLN.11/strength - unit: 1/m -- type: pyaml.magnet.quadrupole - name: QCORR_007 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN01-AR/EM-COR/CQLN.12/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SXD13_001 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN01-AR/EM-SX/SCD.10/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF13_HCOR_002 - mapping: - - [B2, SXF13_HCOR_002.sextupole] - - [B0, SXF13_HCOR_002.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN01-AR/EM-SX/SCF.11/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN01-AR/EM-COR/SCF.11-CDLH.06/strength - unit: '1' -- type: pyaml.magnet.cfm_magnet - name: OCTF1_QCORROCT_6_QT_001 - mapping: - - [B3, OCTF1_QCORROCT_6_QT_001.octupole] - - [B1, OCTF1_QCORROCT_6_QT_001.quadrupole] - - [A1, OCTF1_QCORROCT_6_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN01-AR/EM-OCT/OC.04/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN01-AR/EM-COR/OC.04-CQLN.13/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN01-AR/EM-COR/OC.04-CQLT.05/strength - unit: 1/m**2 -- type: pyaml.bpm.bpm - name: BPM_006 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN01-AR/DG-EPOS/BPM.07/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN01-AR/DG-EPOS/BPM.07/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SXD1_VCOR_002 - mapping: - - [B2, SXD1_VCOR_002.sextupole] - - [A0, SXD1_VCOR_002.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN01-AR/EM-SX/SCD.12/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN01-AR/EM-COR/SCD.12-CDLV.06/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_008 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN01-AR/EM-COR/CQLN.14/strength - unit: 1/m -- type: pyaml.magnet.quadrupole - name: QCORR_009 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN01-AR/EM-COR/CQLN.15/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SXD1_003 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN01-AR/EM-SX/SCD.13/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF1_HCOR_002 - mapping: - - [B2, SXF1_HCOR_002.sextupole] - - [B0, SXF1_HCOR_002.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN01-AR/EM-SX/SCF.14/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN01-AR/EM-COR/SCF.14-CDLH.07/strength - unit: '1' -- type: pyaml.magnet.cfm_magnet - name: OCTF1_QCORROCT_7_QT_001 - mapping: - - [B3, OCTF1_QCORROCT_7_QT_001.octupole] - - [B1, OCTF1_QCORROCT_7_QT_001.quadrupole] - - [A1, OCTF1_QCORROCT_7_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN01-AR/EM-OCT/OC.05/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN01-AR/EM-COR/OC.05-CQLN.16/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN01-AR/EM-COR/OC.05-CQLT.06/strength - unit: 1/m**2 -- type: pyaml.bpm.bpm - name: BPM_007 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN01-AR/DG-EPOS/BPM.08/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN01-AR/DG-EPOS/BPM.08/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SXD1_VCOR_003 - mapping: - - [B2, SXD1_VCOR_003.sextupole] - - [A0, SXD1_VCOR_003.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN01-AR/EM-SX/SCD.15/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN01-AR/EM-COR/SCD.15-CDLV.07/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_010 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN01-AR/EM-COR/CQLN.17/strength - unit: 1/m -- type: pyaml.magnet.quadrupole - name: QCORR_011 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN01-AR/EM-COR/CQLN.18/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SXD12_001 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN01-AR/EM-SX/SCD.16/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF12_HCOR_001 - mapping: - - [B2, SXF12_HCOR_001.sextupole] - - [B0, SXF12_HCOR_001.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN01-AR/EM-SX/SCF.17/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN01-AR/EM-COR/SCF.17-CDLH.08/strength - unit: '1' -- type: pyaml.magnet.cfm_magnet - name: OCTF1_QCORROCT_8_QT_001 - mapping: - - [B3, OCTF1_QCORROCT_8_QT_001.octupole] - - [B1, OCTF1_QCORROCT_8_QT_001.quadrupole] - - [A1, OCTF1_QCORROCT_8_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN01-AR/EM-OCT/OC.06/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN01-AR/EM-COR/OC.06-CQLN.19/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN01-AR/EM-COR/OC.06-CQLT.07/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXD12_VCOR_001 - mapping: - - [B2, SXD12_VCOR_001.sextupole] - - [A0, SXD12_VCOR_001.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN01-AR/EM-SX/SCD.18/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN01-AR/EM-COR/SCD.18-CDLV.08/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_008 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN01-AR/DG-EPOS/BPM.09/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN01-AR/DG-EPOS/BPM.09/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SH6_COR_001 - mapping: - - [B2, SH6_COR_001.sextupole] - - [B0, SH6_COR_001.hcorrector] - - [A0, SH6_COR_001.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0, A0] - units: [1/m**2, '1', '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN01-AR/EM-SX/SHD.04/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN01-AR/EM-COR/SHD.04-CDLH.09/strength - unit: '1' - - type: tango.pyaml.attribute - attribute: AN01-AR/EM-COR/SHD.04-CDLV.09/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_012 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN01-AR/EM-COR/CQLN.20/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SH5_001 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN01-AR/EM-SX/SHD.05/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: OH5_QCORROCT_9_001 - mapping: - - [B3, OH5_QCORROCT_9_001.octupole] - - [B1, OH5_QCORROCT_9_001.quadrupole] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1] - units: [1/m**3, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN01-AR/EM-OCT/OH.03/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN01-AR/EM-COR/OH.03-CQLN.21/strength - unit: 1/m**2 -- type: pyaml.bpm.bpm - name: BPM_009 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN01-AR/DG-EPOS/BPM.10/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN01-AR/DG-EPOS/BPM.10/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SH4_COR_001 - mapping: - - [B2, SH4_COR_001.sextupole] - - [B0, SH4_COR_001.hcorrector] - - [A0, SH4_COR_001.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0, A0] - units: [1/m**2, '1', '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN01-AR/EM-SX/SHF.06/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN01-AR/EM-COR/SHF.06-CDLH.10/strength - unit: '1' - - type: tango.pyaml.attribute - attribute: AN01-AR/EM-COR/SHF.06-CDLV.10/strength - unit: '1' -- type: pyaml.magnet.cfm_magnet - name: OH4_QCORROCT_10_QT_001 - mapping: - - [B3, OH4_QCORROCT_10_QT_001.octupole] - - [B1, OH4_QCORROCT_10_QT_001.quadrupole] - - [A1, OH4_QCORROCT_10_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN01-AR/EM-OCT/OH.04/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN01-AR/EM-COR/OH.04-CQLN.22/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN01-AR/EM-COR/OH.04-CQLT.08/strength - unit: 1/m**2 -- type: pyaml.bpm.bpm - name: BPM_010 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN02-SD/DG-EPOS/BPM.01/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN02-SD/DG-EPOS/BPM.01/y_pos - unit: mm -- type: pyaml.bpm.bpm - name: BPM_011 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN02-SD/DG-EPOS/BPM.02/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN02-SD/DG-EPOS/BPM.02/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: OH4_QCORROCT_11_QT_001 - mapping: - - [B3, OH4_QCORROCT_11_QT_001.octupole] - - [B1, OH4_QCORROCT_11_QT_001.quadrupole] - - [A1, OH4_QCORROCT_11_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN02-AR/EM-OCT/OH.01/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN02-AR/EM-COR/OH.01-CQLN.01/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN02-AR/EM-COR/OH.01-CQLT.01/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SH4_COR_002 - mapping: - - [B2, SH4_COR_002.sextupole] - - [B0, SH4_COR_002.hcorrector] - - [A0, SH4_COR_002.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0, A0] - units: [1/m**2, '1', '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN02-AR/EM-SX/SHF.01/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN02-AR/EM-COR/SHF.01-CDLH.01/strength - unit: '1' - - type: tango.pyaml.attribute - attribute: AN02-AR/EM-COR/SHF.01-CDLV.01/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_012 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN02-AR/DG-EPOS/BPM.03/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN02-AR/DG-EPOS/BPM.03/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: OH5_QCORROCT_12_001 - mapping: - - [B3, OH5_QCORROCT_12_001.octupole] - - [B1, OH5_QCORROCT_12_001.quadrupole] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1] - units: [1/m**3, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN02-AR/EM-OCT/OH.02/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN02-AR/EM-COR/OH.02-CQLN.02/strength - unit: 1/m**2 -- type: pyaml.magnet.sextupole - name: SH5_002 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN02-AR/EM-SX/SHD.02/strength - unit: 1/m**2 -- type: pyaml.magnet.quadrupole - name: QCORR_013 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN02-AR/EM-COR/CQLN.03/strength - unit: 1/m -- type: pyaml.magnet.cfm_magnet - name: SH6_COR_002 - mapping: - - [B2, SH6_COR_002.sextupole] - - [B0, SH6_COR_002.hcorrector] - - [A0, SH6_COR_002.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0, A0] - units: [1/m**2, '1', '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN02-AR/EM-SX/SHD.03/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN02-AR/EM-COR/SHD.03-CDLH.02/strength - unit: '1' - - type: tango.pyaml.attribute - attribute: AN02-AR/EM-COR/SHD.03-CDLV.02/strength - unit: '1' -- type: pyaml.magnet.sextupole - name: SXD21_001 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN02-AR/EM-SX/SCD.01/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: OCTF2_QCORROCT_13_QT_001 - mapping: - - [B3, OCTF2_QCORROCT_13_QT_001.octupole] - - [B1, OCTF2_QCORROCT_13_QT_001.quadrupole] - - [A1, OCTF2_QCORROCT_13_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN02-AR/EM-OCT/OC.01/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN02-AR/EM-COR/OC.01-CQLN.04/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN02-AR/EM-COR/OC.01-CQLT.02/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF21_HCOR_001 - mapping: - - [B2, SXF21_HCOR_001.sextupole] - - [B0, SXF21_HCOR_001.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN02-AR/EM-SX/SCF.02/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN02-AR/EM-COR/SCF.02-CDLH.03/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_013 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN02-AR/DG-EPOS/BPM.04/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN02-AR/DG-EPOS/BPM.04/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SXD21_VCOR_001 - mapping: - - [B2, SXD21_VCOR_001.sextupole] - - [A0, SXD21_VCOR_001.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN02-AR/EM-SX/SCD.03/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN02-AR/EM-COR/SCD.03-CDLV.03/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_014 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN02-AR/EM-COR/CQLN.05/strength - unit: 1/m -- type: pyaml.magnet.quadrupole - name: QCORR_015 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN02-AR/EM-COR/CQLN.06/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SXD2_001 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN02-AR/EM-SX/SCD.04/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: OCTF2_QCORROCT_14_QT_001 - mapping: - - [B3, OCTF2_QCORROCT_14_QT_001.octupole] - - [B1, OCTF2_QCORROCT_14_QT_001.quadrupole] - - [A1, OCTF2_QCORROCT_14_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN02-AR/EM-OCT/OC.02/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN02-AR/EM-COR/OC.02-CQLN.07/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN02-AR/EM-COR/OC.02-CQLT.03/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF2_HCOR_001 - mapping: - - [B2, SXF2_HCOR_001.sextupole] - - [B0, SXF2_HCOR_001.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN02-AR/EM-SX/SCF.05/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN02-AR/EM-COR/SCF.05-CDLH.04/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_014 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN02-AR/DG-EPOS/BPM.05/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN02-AR/DG-EPOS/BPM.05/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SXD2_VCOR_001 - mapping: - - [B2, SXD2_VCOR_001.sextupole] - - [A0, SXD2_VCOR_001.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN02-AR/EM-SX/SCD.06/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN02-AR/EM-COR/SCD.06-CDLV.04/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_016 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN02-AR/EM-COR/CQLN.08/strength - unit: 1/m -- type: pyaml.magnet.quadrupole - name: QCORR_017 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN02-AR/EM-COR/CQLN.09/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SXD22_001 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN02-AR/EM-SX/SCD.07/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF22_HCOR_001 - mapping: - - [B2, SXF22_HCOR_001.sextupole] - - [B0, SXF22_HCOR_001.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN02-AR/EM-SX/SCF.08/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN02-AR/EM-COR/SCF.08-CDLH.05/strength - unit: '1' -- type: pyaml.magnet.cfm_magnet - name: OCTF2_QCORROCT_15_QT_001 - mapping: - - [B3, OCTF2_QCORROCT_15_QT_001.octupole] - - [B1, OCTF2_QCORROCT_15_QT_001.quadrupole] - - [A1, OCTF2_QCORROCT_15_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN02-AR/EM-OCT/OC.03/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN02-AR/EM-COR/OC.03-CQLN.10/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN02-AR/EM-COR/OC.03-CQLT.04/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXD22_VCOR_001 - mapping: - - [B2, SXD22_VCOR_001.sextupole] - - [A0, SXD22_VCOR_001.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN02-AR/EM-SX/SCD.09/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN02-AR/EM-COR/SCD.09-CDLV.05/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_015 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN02-AR/DG-EPOS/BPM.06/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN02-AR/DG-EPOS/BPM.06/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SH9_COR_001 - mapping: - - [B2, SH9_COR_001.sextupole] - - [B0, SH9_COR_001.hcorrector] - - [A0, SH9_COR_001.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0, A0] - units: [1/m**2, '1', '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN02-AR/EM-SX/SHD.04/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN02-AR/EM-COR/SHD.04-CDLH.06/strength - unit: '1' - - type: tango.pyaml.attribute - attribute: AN02-AR/EM-COR/SHD.04-CDLV.06/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_018 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN02-AR/EM-COR/CQLN.11/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SH8_001 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN02-AR/EM-SX/SHD.05/strength - unit: 1/m**2 -- type: pyaml.magnet.quadrupole - name: QCORR_019 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN02-AR/EM-COR/CQLN.12/strength - unit: 1/m -- type: pyaml.bpm.bpm - name: BPM_016 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN02-AR/DG-EPOS/BPM.07/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN02-AR/DG-EPOS/BPM.07/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SH7_COR_001 - mapping: - - [B2, SH7_COR_001.sextupole] - - [B0, SH7_COR_001.hcorrector] - - [A0, SH7_COR_001.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0, A0] - units: [1/m**2, '1', '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN02-AR/EM-SX/SHF.06/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN02-AR/EM-COR/SHF.06-CDLH.07/strength - unit: '1' - - type: tango.pyaml.attribute - attribute: AN02-AR/EM-COR/SHF.06-CDLV.07/strength - unit: '1' -- type: pyaml.magnet.cfm_magnet - name: OH7_QCORROCT_16_QT_001 - mapping: - - [B3, OH7_QCORROCT_16_QT_001.octupole] - - [B1, OH7_QCORROCT_16_QT_001.quadrupole] - - [A1, OH7_QCORROCT_16_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN02-AR/EM-OCT/OH.03/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN02-AR/EM-COR/OH.03-CQLN.13/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN02-AR/EM-COR/OH.03-CQLT.05/strength - unit: 1/m**2 -- type: pyaml.bpm.bpm - name: BPM_017 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN03-SD/DG-EPOS/BPM.01/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN03-SD/DG-EPOS/BPM.01/y_pos - unit: mm -- type: pyaml.bpm.bpm - name: BPM_018 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN03-SD/DG-EPOS/BPM.02/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN03-SD/DG-EPOS/BPM.02/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: OH7_QCORROCT_17_QT_001 - mapping: - - [B3, OH7_QCORROCT_17_QT_001.octupole] - - [B1, OH7_QCORROCT_17_QT_001.quadrupole] - - [A1, OH7_QCORROCT_17_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN03-AR/EM-OCT/OH.01/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN03-AR/EM-COR/OH.01-CQLN.01/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN03-AR/EM-COR/OH.01-CQLT.01/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SH7_COR_002 - mapping: - - [B2, SH7_COR_002.sextupole] - - [B0, SH7_COR_002.hcorrector] - - [A0, SH7_COR_002.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0, A0] - units: [1/m**2, '1', '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN03-AR/EM-SX/SHF.01/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN03-AR/EM-COR/SHF.01-CDLH.01/strength - unit: '1' - - type: tango.pyaml.attribute - attribute: AN03-AR/EM-COR/SHF.01-CDLV.01/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_019 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN03-AR/DG-EPOS/BPM.03/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN03-AR/DG-EPOS/BPM.03/y_pos - unit: mm -- type: pyaml.magnet.quadrupole - name: QCORR_020 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN03-AR/EM-COR/CQLN.02/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SH8_002 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN03-AR/EM-SX/SHD.02/strength - unit: 1/m**2 -- type: pyaml.magnet.quadrupole - name: QCORR_021 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN03-AR/EM-COR/CQLN.03/strength - unit: 1/m -- type: pyaml.magnet.cfm_magnet - name: SH9_COR_002 - mapping: - - [B2, SH9_COR_002.sextupole] - - [B0, SH9_COR_002.hcorrector] - - [A0, SH9_COR_002.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0, A0] - units: [1/m**2, '1', '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN03-AR/EM-SX/SHD.03/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN03-AR/EM-COR/SHD.03-CDLH.02/strength - unit: '1' - - type: tango.pyaml.attribute - attribute: AN03-AR/EM-COR/SHD.03-CDLV.02/strength - unit: '1' -- type: pyaml.magnet.sextupole - name: SXD31_001 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN03-AR/EM-SX/SCD.01/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: OCTF3_QCORROCT_18_QT_001 - mapping: - - [B3, OCTF3_QCORROCT_18_QT_001.octupole] - - [B1, OCTF3_QCORROCT_18_QT_001.quadrupole] - - [A1, OCTF3_QCORROCT_18_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN03-AR/EM-OCT/OC.01/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN03-AR/EM-COR/OC.01-CQLN.04/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN03-AR/EM-COR/OC.01-CQLT.02/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF31_HCOR_001 - mapping: - - [B2, SXF31_HCOR_001.sextupole] - - [B0, SXF31_HCOR_001.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN03-AR/EM-SX/SCF.02/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN03-AR/EM-COR/SCF.02-CDLH.03/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_020 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN03-AR/DG-EPOS/BPM.04/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN03-AR/DG-EPOS/BPM.04/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SXD31_VCOR_001 - mapping: - - [B2, SXD31_VCOR_001.sextupole] - - [A0, SXD31_VCOR_001.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN03-AR/EM-SX/SCD.03/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN03-AR/EM-COR/SCD.03-CDLV.03/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_022 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN03-AR/EM-COR/CQLN.05/strength - unit: 1/m -- type: pyaml.magnet.quadrupole - name: QCORR_023 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN03-AR/EM-COR/CQLN.06/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SXD3_001 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN03-AR/EM-SX/SCD.04/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: OCTF3_QCORROCT_19_QT_001 - mapping: - - [B3, OCTF3_QCORROCT_19_QT_001.octupole] - - [B1, OCTF3_QCORROCT_19_QT_001.quadrupole] - - [A1, OCTF3_QCORROCT_19_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN03-AR/EM-OCT/OC.02/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN03-AR/EM-COR/OC.02-CQLN.07/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN03-AR/EM-COR/OC.02-CQLT.03/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF3_HCOR_001 - mapping: - - [B2, SXF3_HCOR_001.sextupole] - - [B0, SXF3_HCOR_001.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN03-AR/EM-SX/SCF.05/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN03-AR/EM-COR/SCF.05-CDLH.04/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_021 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN03-AR/DG-EPOS/BPM.05/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN03-AR/DG-EPOS/BPM.05/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SXD3_VCOR_001 - mapping: - - [B2, SXD3_VCOR_001.sextupole] - - [A0, SXD3_VCOR_001.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN03-AR/EM-SX/SCD.06/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN03-AR/EM-COR/SCD.06-CDLV.04/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_024 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN03-AR/EM-COR/CQLN.08/strength - unit: 1/m -- type: pyaml.magnet.quadrupole - name: QCORR_025 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN03-AR/EM-COR/CQLN.09/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SXD3_002 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN03-AR/EM-SX/SCD.07/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: OCTF3_QCORROCT_20_QT_001 - mapping: - - [B3, OCTF3_QCORROCT_20_QT_001.octupole] - - [B1, OCTF3_QCORROCT_20_QT_001.quadrupole] - - [A1, OCTF3_QCORROCT_20_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN03-AR/EM-OCT/OC.03/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN03-AR/EM-COR/OC.03-CQLN.10/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN03-AR/EM-COR/OC.03-CQLT.04/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF33_HCOR_001 - mapping: - - [B2, SXF33_HCOR_001.sextupole] - - [B0, SXF33_HCOR_001.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN03-AR/EM-SX/SCF.08/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN03-AR/EM-COR/SCF.08-CDLH.05/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_022 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN03-AR/DG-EPOS/BPM.06/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN03-AR/DG-EPOS/BPM.06/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SXD33_VCOR_001 - mapping: - - [B2, SXD33_VCOR_001.sextupole] - - [A0, SXD33_VCOR_001.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN03-AR/EM-SX/SCD.09/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN03-AR/EM-COR/SCD.09-CDLV.05/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_026 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN03-AR/EM-COR/CQLN.11/strength - unit: 1/m -- type: pyaml.magnet.quadrupole - name: QCORR_027 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN03-AR/EM-COR/CQLN.12/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SXD33_001 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN03-AR/EM-SX/SCD.10/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF33_HCOR_002 - mapping: - - [B2, SXF33_HCOR_002.sextupole] - - [B0, SXF33_HCOR_002.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN03-AR/EM-SX/SCF.11/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN03-AR/EM-COR/SCF.11-CDLH.06/strength - unit: '1' -- type: pyaml.magnet.cfm_magnet - name: OCTF3_QCORROCT_21_QT_001 - mapping: - - [B3, OCTF3_QCORROCT_21_QT_001.octupole] - - [B1, OCTF3_QCORROCT_21_QT_001.quadrupole] - - [A1, OCTF3_QCORROCT_21_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN03-AR/EM-OCT/OC.04/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN03-AR/EM-COR/OC.04-CQLN.13/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN03-AR/EM-COR/OC.04-CQLT.05/strength - unit: 1/m**2 -- type: pyaml.bpm.bpm - name: BPM_023 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN03-AR/DG-EPOS/BPM.07/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN03-AR/DG-EPOS/BPM.07/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SXD3_VCOR_002 - mapping: - - [B2, SXD3_VCOR_002.sextupole] - - [A0, SXD3_VCOR_002.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN03-AR/EM-SX/SCD.12/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN03-AR/EM-COR/SCD.12-CDLV.06/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_028 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN03-AR/EM-COR/CQLN.14/strength - unit: 1/m -- type: pyaml.magnet.quadrupole - name: QCORR_029 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN03-AR/EM-COR/CQLN.15/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SXD3_003 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN03-AR/EM-SX/SCD.13/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF3_HCOR_002 - mapping: - - [B2, SXF3_HCOR_002.sextupole] - - [B0, SXF3_HCOR_002.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN03-AR/EM-SX/SCF.14/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN03-AR/EM-COR/SCF.14-CDLH.07/strength - unit: '1' -- type: pyaml.magnet.cfm_magnet - name: OCTF3_QCORROCT_22_QT_001 - mapping: - - [B3, OCTF3_QCORROCT_22_QT_001.octupole] - - [B1, OCTF3_QCORROCT_22_QT_001.quadrupole] - - [A1, OCTF3_QCORROCT_22_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN03-AR/EM-OCT/OC.05/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN03-AR/EM-COR/OC.05-CQLN.16/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN03-AR/EM-COR/OC.05-CQLT.06/strength - unit: 1/m**2 -- type: pyaml.bpm.bpm - name: BPM_024 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN03-AR/DG-EPOS/BPM.08/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN03-AR/DG-EPOS/BPM.08/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SXD3_VCOR_003 - mapping: - - [B2, SXD3_VCOR_003.sextupole] - - [A0, SXD3_VCOR_003.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN03-AR/EM-SX/SCD.15/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN03-AR/EM-COR/SCD.15-CDLV.07/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_030 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN03-AR/EM-COR/CQLN.17/strength - unit: 1/m -- type: pyaml.magnet.quadrupole - name: QCORR_031 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN03-AR/EM-COR/CQLN.18/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SXD32_001 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN03-AR/EM-SX/SCD.16/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF32_HCOR_001 - mapping: - - [B2, SXF32_HCOR_001.sextupole] - - [B0, SXF32_HCOR_001.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN03-AR/EM-SX/SCF.17/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN03-AR/EM-COR/SCF.17-CDLH.08/strength - unit: '1' -- type: pyaml.magnet.cfm_magnet - name: OCTF3_QCORROCT_23_QT_001 - mapping: - - [B3, OCTF3_QCORROCT_23_QT_001.octupole] - - [B1, OCTF3_QCORROCT_23_QT_001.quadrupole] - - [A1, OCTF3_QCORROCT_23_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN03-AR/EM-OCT/OC.06/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN03-AR/EM-COR/OC.06-CQLN.19/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN03-AR/EM-COR/OC.06-CQLT.07/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXD32_VCOR_001 - mapping: - - [B2, SXD32_VCOR_001.sextupole] - - [A0, SXD32_VCOR_001.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN03-AR/EM-SX/SCD.18/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN03-AR/EM-COR/SCD.18-CDLV.08/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_025 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN03-AR/DG-EPOS/BPM.09/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN03-AR/DG-EPOS/BPM.09/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SH9_COR_003 - mapping: - - [B2, SH9_COR_003.sextupole] - - [B0, SH9_COR_003.hcorrector] - - [A0, SH9_COR_003.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0, A0] - units: [1/m**2, '1', '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN03-AR/EM-SX/SHD.04/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN03-AR/EM-COR/SHD.04-CDLH.09/strength - unit: '1' - - type: tango.pyaml.attribute - attribute: AN03-AR/EM-COR/SHD.04-CDLV.09/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_032 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN03-AR/EM-COR/CQLN.20/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SH8_003 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN03-AR/EM-SX/SHD.05/strength - unit: 1/m**2 -- type: pyaml.magnet.quadrupole - name: QCORR_033 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN03-AR/EM-COR/CQLN.21/strength - unit: 1/m -- type: pyaml.bpm.bpm - name: BPM_026 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN03-AR/DG-EPOS/BPM.10/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN03-AR/DG-EPOS/BPM.10/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SH7_COR_003 - mapping: - - [B2, SH7_COR_003.sextupole] - - [B0, SH7_COR_003.hcorrector] - - [A0, SH7_COR_003.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0, A0] - units: [1/m**2, '1', '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN03-AR/EM-SX/SHF.06/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN03-AR/EM-COR/SHF.06-CDLH.10/strength - unit: '1' - - type: tango.pyaml.attribute - attribute: AN03-AR/EM-COR/SHF.06-CDLV.10/strength - unit: '1' -- type: pyaml.magnet.cfm_magnet - name: OH7_QCORROCT_24_QT_001 - mapping: - - [B3, OH7_QCORROCT_24_QT_001.octupole] - - [B1, OH7_QCORROCT_24_QT_001.quadrupole] - - [A1, OH7_QCORROCT_24_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN03-AR/EM-OCT/OH.02/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN03-AR/EM-COR/OH.02-CQLN.22/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN03-AR/EM-COR/OH.02-CQLT.08/strength - unit: 1/m**2 -- type: pyaml.bpm.bpm - name: BPM_027 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN04-SD/DG-EPOS/BPM.01/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN04-SD/DG-EPOS/BPM.01/y_pos - unit: mm -- type: pyaml.bpm.bpm - name: BPM_028 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN04-SD/DG-EPOS/BPM.02/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN04-SD/DG-EPOS/BPM.02/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: OH7_QCORROCT_25_QT_001 - mapping: - - [B3, OH7_QCORROCT_25_QT_001.octupole] - - [B1, OH7_QCORROCT_25_QT_001.quadrupole] - - [A1, OH7_QCORROCT_25_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN04-AR/EM-OCT/OH.01/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN04-AR/EM-COR/OH.01-CQLN.01/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN04-AR/EM-COR/OH.01-CQLT.01/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SH7_COR_004 - mapping: - - [B2, SH7_COR_004.sextupole] - - [B0, SH7_COR_004.hcorrector] - - [A0, SH7_COR_004.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0, A0] - units: [1/m**2, '1', '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN04-AR/EM-SX/SHF.01/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN04-AR/EM-COR/SHF.01-CDLH.01/strength - unit: '1' - - type: tango.pyaml.attribute - attribute: AN04-AR/EM-COR/SHF.01-CDLV.01/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_029 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN04-AR/DG-EPOS/BPM.03/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN04-AR/DG-EPOS/BPM.03/y_pos - unit: mm -- type: pyaml.magnet.quadrupole - name: QCORR_034 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN04-AR/EM-COR/CQLN.02/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SH8_004 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN04-AR/EM-SX/SHD.02/strength - unit: 1/m**2 -- type: pyaml.magnet.quadrupole - name: QCORR_035 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN04-AR/EM-COR/CQLN.03/strength - unit: 1/m -- type: pyaml.magnet.cfm_magnet - name: SH9_COR_004 - mapping: - - [B2, SH9_COR_004.sextupole] - - [B0, SH9_COR_004.hcorrector] - - [A0, SH9_COR_004.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0, A0] - units: [1/m**2, '1', '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN04-AR/EM-SX/SHD.03/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN04-AR/EM-COR/SHD.03-CDLH.02/strength - unit: '1' - - type: tango.pyaml.attribute - attribute: AN04-AR/EM-COR/SHD.03-CDLV.02/strength - unit: '1' -- type: pyaml.magnet.sextupole - name: SXD41_001 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN04-AR/EM-SX/SCD.01/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: OCTF4_QCORROCT_26_QT_001 - mapping: - - [B3, OCTF4_QCORROCT_26_QT_001.octupole] - - [B1, OCTF4_QCORROCT_26_QT_001.quadrupole] - - [A1, OCTF4_QCORROCT_26_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN04-AR/EM-OCT/OC.01/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN04-AR/EM-COR/OC.01-CQLN.04/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN04-AR/EM-COR/OC.01-CQLT.02/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF41_HCOR_001 - mapping: - - [B2, SXF41_HCOR_001.sextupole] - - [B0, SXF41_HCOR_001.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN04-AR/EM-SX/SCF.02/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN04-AR/EM-COR/SCF.02-CDLH.03/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_030 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN04-AR/DG-EPOS/BPM.04/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN04-AR/DG-EPOS/BPM.04/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SXD41_VCOR_001 - mapping: - - [B2, SXD41_VCOR_001.sextupole] - - [A0, SXD41_VCOR_001.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN04-AR/EM-SX/SCD.03/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN04-AR/EM-COR/SCD.03-CDLV.03/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_036 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN04-AR/EM-COR/CQLN.05/strength - unit: 1/m -- type: pyaml.magnet.quadrupole - name: QCORR_037 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN04-AR/EM-COR/CQLN.06/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SXD4_001 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN04-AR/EM-SX/SCD.04/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF4_HCOR_001 - mapping: - - [B2, SXF4_HCOR_001.sextupole] - - [B0, SXF4_HCOR_001.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN04-AR/EM-SX/SCF.05/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN04-AR/EM-COR/SCF.05-CDLH.04/strength - unit: '1' -- type: pyaml.magnet.cfm_magnet - name: OCTF4_QCORROCT_27_QT_001 - mapping: - - [B3, OCTF4_QCORROCT_27_QT_001.octupole] - - [B1, OCTF4_QCORROCT_27_QT_001.quadrupole] - - [A1, OCTF4_QCORROCT_27_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN04-AR/EM-OCT/OC.02/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN04-AR/EM-COR/OC.02-CQLN.07/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN04-AR/EM-COR/OC.02-CQLT.03/strength - unit: 1/m**2 -- type: pyaml.bpm.bpm - name: BPM_031 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN04-AR/DG-EPOS/BPM.05/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN04-AR/DG-EPOS/BPM.05/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SXD4_VCOR_001 - mapping: - - [B2, SXD4_VCOR_001.sextupole] - - [A0, SXD4_VCOR_001.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN04-AR/EM-SX/SCD.06/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN04-AR/EM-COR/SCD.06-CDLV.04/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_038 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN04-AR/EM-COR/CQLN.08/strength - unit: 1/m -- type: pyaml.magnet.quadrupole - name: QCORR_039 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN04-AR/EM-COR/CQLN.09/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SXD42_001 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN04-AR/EM-SX/SCD.07/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF42_HCOR_001 - mapping: - - [B2, SXF42_HCOR_001.sextupole] - - [B0, SXF42_HCOR_001.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN04-AR/EM-SX/SCF.08/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN04-AR/EM-COR/SCF.08-CDLH.05/strength - unit: '1' -- type: pyaml.magnet.cfm_magnet - name: OCTF4_QCORROCT_28_QT_001 - mapping: - - [B3, OCTF4_QCORROCT_28_QT_001.octupole] - - [B1, OCTF4_QCORROCT_28_QT_001.quadrupole] - - [A1, OCTF4_QCORROCT_28_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN04-AR/EM-OCT/OC.03/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN04-AR/EM-COR/OC.03-CQLN.10/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN04-AR/EM-COR/OC.03-CQLT.04/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXD42_VCOR_001 - mapping: - - [B2, SXD42_VCOR_001.sextupole] - - [A0, SXD42_VCOR_001.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN04-AR/EM-SX/SCD.09/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN04-AR/EM-COR/SCD.09-CDLV.05/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_032 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN04-AR/DG-EPOS/BPM.06/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN04-AR/DG-EPOS/BPM.06/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SH12_COR_001 - mapping: - - [B2, SH12_COR_001.sextupole] - - [B0, SH12_COR_001.hcorrector] - - [A0, SH12_COR_001.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0, A0] - units: [1/m**2, '1', '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN04-AR/EM-SX/SHD.04/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN04-AR/EM-COR/SHD.04-CDLH.06/strength - unit: '1' - - type: tango.pyaml.attribute - attribute: AN04-AR/EM-COR/SHD.04-CDLV.06/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_040 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN04-AR/EM-COR/CQLN.11/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SH11_001 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN04-AR/EM-SX/SHD.05/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: OH11_QCORROCT_29_001 - mapping: - - [B3, OH11_QCORROCT_29_001.octupole] - - [B1, OH11_QCORROCT_29_001.quadrupole] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1] - units: [1/m**3, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN04-AR/EM-OCT/OH.02/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN04-AR/EM-COR/OH.02-CQLN.12/strength - unit: 1/m**2 -- type: pyaml.bpm.bpm - name: BPM_033 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN04-AR/DG-EPOS/BPM.07/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN04-AR/DG-EPOS/BPM.07/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SH10_COR_001 - mapping: - - [B2, SH10_COR_001.sextupole] - - [B0, SH10_COR_001.hcorrector] - - [A0, SH10_COR_001.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0, A0] - units: [1/m**2, '1', '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN04-AR/EM-SX/SHF.06/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN04-AR/EM-COR/SHF.06-CDLH.07/strength - unit: '1' - - type: tango.pyaml.attribute - attribute: AN04-AR/EM-COR/SHF.06-CDLV.07/strength - unit: '1' -- type: pyaml.magnet.cfm_magnet - name: OH10_QCORROCT_30_QT_001 - mapping: - - [B3, OH10_QCORROCT_30_QT_001.octupole] - - [B1, OH10_QCORROCT_30_QT_001.quadrupole] - - [A1, OH10_QCORROCT_30_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN04-AR/EM-OCT/OH.03/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN04-AR/EM-COR/OH.03-CQLN.13/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN04-AR/EM-COR/OH.03-CQLT.05/strength - unit: 1/m**2 -- type: pyaml.bpm.bpm - name: BPM_034 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN05-SD/DG-EPOS/BPM.01/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN05-SD/DG-EPOS/BPM.01/y_pos - unit: mm -- type: pyaml.bpm.bpm - name: BPM_035 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN05-SD/DG-EPOS/BPM.02/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN05-SD/DG-EPOS/BPM.02/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: OH10_QCORROCT_31_QT_001 - mapping: - - [B3, OH10_QCORROCT_31_QT_001.octupole] - - [B1, OH10_QCORROCT_31_QT_001.quadrupole] - - [A1, OH10_QCORROCT_31_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN05-AR/EM-OCT/OH.01/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN05-AR/EM-COR/OH.01-CQLN.01/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN05-AR/EM-COR/OH.01-CQLT.01/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SH10_COR_002 - mapping: - - [B2, SH10_COR_002.sextupole] - - [B0, SH10_COR_002.hcorrector] - - [A0, SH10_COR_002.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0, A0] - units: [1/m**2, '1', '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN05-AR/EM-SX/SHF.01/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN05-AR/EM-COR/SHF.01-CDLH.01/strength - unit: '1' - - type: tango.pyaml.attribute - attribute: AN05-AR/EM-COR/SHF.01-CDLV.01/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_036 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN05-AR/DG-EPOS/BPM.03/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN05-AR/DG-EPOS/BPM.03/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: OH11_QCORROCT_32_001 - mapping: - - [B3, OH11_QCORROCT_32_001.octupole] - - [B1, OH11_QCORROCT_32_001.quadrupole] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1] - units: [1/m**3, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN05-AR/EM-OCT/OH.02/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN05-AR/EM-COR/OH.02-CQLN.02/strength - unit: 1/m**2 -- type: pyaml.magnet.sextupole - name: SH11_002 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN05-AR/EM-SX/SHD.02/strength - unit: 1/m**2 -- type: pyaml.magnet.quadrupole - name: QCORR_041 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN05-AR/EM-COR/CQLN.03/strength - unit: 1/m -- type: pyaml.magnet.cfm_magnet - name: SH12_COR_002 - mapping: - - [B2, SH12_COR_002.sextupole] - - [B0, SH12_COR_002.hcorrector] - - [A0, SH12_COR_002.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0, A0] - units: [1/m**2, '1', '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN05-AR/EM-SX/SHD.03/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN05-AR/EM-COR/SHD.03-CDLH.02/strength - unit: '1' - - type: tango.pyaml.attribute - attribute: AN05-AR/EM-COR/SHD.03-CDLV.02/strength - unit: '1' -- type: pyaml.magnet.sextupole - name: SXD51_001 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN05-AR/EM-SX/SCD.01/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: OCTF5_QCORROCT_33_QT_001 - mapping: - - [B3, OCTF5_QCORROCT_33_QT_001.octupole] - - [B1, OCTF5_QCORROCT_33_QT_001.quadrupole] - - [A1, OCTF5_QCORROCT_33_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN05-AR/EM-OCT/OC.01/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN05-AR/EM-COR/OC.01-CQLN.04/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN05-AR/EM-COR/OC.01-CQLT.02/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF51_HCOR_001 - mapping: - - [B2, SXF51_HCOR_001.sextupole] - - [B0, SXF51_HCOR_001.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN05-AR/EM-SX/SCF.02/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN05-AR/EM-COR/SCF.02-CDLH.03/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_037 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN05-AR/DG-EPOS/BPM.04/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN05-AR/DG-EPOS/BPM.04/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SXD51_VCOR_001 - mapping: - - [B2, SXD51_VCOR_001.sextupole] - - [A0, SXD51_VCOR_001.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN05-AR/EM-SX/SCD.03/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN05-AR/EM-COR/SCD.03-CDLV.03/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_042 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN05-AR/EM-COR/CQLN.05/strength - unit: 1/m -- type: pyaml.magnet.quadrupole - name: QCORR_043 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN05-AR/EM-COR/CQLN.06/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SXD5_001 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN05-AR/EM-SX/SCD.04/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: OCTF5_QCORROCT_34_QT_001 - mapping: - - [B3, OCTF5_QCORROCT_34_QT_001.octupole] - - [B1, OCTF5_QCORROCT_34_QT_001.quadrupole] - - [A1, OCTF5_QCORROCT_34_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN05-AR/EM-OCT/OC.02/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN05-AR/EM-COR/OC.02-CQLN.07/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN05-AR/EM-COR/OC.02-CQLT.03/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF5_HCOR_001 - mapping: - - [B2, SXF5_HCOR_001.sextupole] - - [B0, SXF5_HCOR_001.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN05-AR/EM-SX/SCF.05/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN05-AR/EM-COR/SCF.05-CDLH.04/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_038 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN05-AR/DG-EPOS/BPM.05/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN05-AR/DG-EPOS/BPM.05/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SXD5_VCOR_001 - mapping: - - [B2, SXD5_VCOR_001.sextupole] - - [A0, SXD5_VCOR_001.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN05-AR/EM-SX/SCD.06/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN05-AR/EM-COR/SCD.06-CDLV.04/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_044 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN05-AR/EM-COR/CQLN.08/strength - unit: 1/m -- type: pyaml.magnet.quadrupole - name: QCORR_045 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN05-AR/EM-COR/CQLN.09/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SXD5_002 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN05-AR/EM-SX/SCD.07/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: OCTF5_QCORROCT_35_QT_001 - mapping: - - [B3, OCTF5_QCORROCT_35_QT_001.octupole] - - [B1, OCTF5_QCORROCT_35_QT_001.quadrupole] - - [A1, OCTF5_QCORROCT_35_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN05-AR/EM-OCT/OC.03/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN05-AR/EM-COR/OC.03-CQLN.10/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN05-AR/EM-COR/OC.03-CQLT.04/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF53_HCOR_001 - mapping: - - [B2, SXF53_HCOR_001.sextupole] - - [B0, SXF53_HCOR_001.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN05-AR/EM-SX/SCF.08/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN05-AR/EM-COR/SCF.08-CDLH.05/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_039 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN05-AR/DG-EPOS/BPM.06/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN05-AR/DG-EPOS/BPM.06/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SXD53_VCOR_001 - mapping: - - [B2, SXD53_VCOR_001.sextupole] - - [A0, SXD53_VCOR_001.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN05-AR/EM-SX/SCD.09/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN05-AR/EM-COR/SCD.09-CDLV.05/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_046 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN05-AR/EM-COR/CQLN.11/strength - unit: 1/m -- type: pyaml.magnet.quadrupole - name: QCORR_047 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN05-AR/EM-COR/CQLN.12/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SXD53_001 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN05-AR/EM-SX/SCD.10/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF53_HCOR_002 - mapping: - - [B2, SXF53_HCOR_002.sextupole] - - [B0, SXF53_HCOR_002.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN05-AR/EM-SX/SCF.11/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN05-AR/EM-COR/SCF.11-CDLH.06/strength - unit: '1' -- type: pyaml.magnet.cfm_magnet - name: OCTF5_QCORROCT_36_QT_001 - mapping: - - [B3, OCTF5_QCORROCT_36_QT_001.octupole] - - [B1, OCTF5_QCORROCT_36_QT_001.quadrupole] - - [A1, OCTF5_QCORROCT_36_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN05-AR/EM-OCT/OC.04/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN05-AR/EM-COR/OC.04-CQLN.13/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN05-AR/EM-COR/OC.04-CQLT.05/strength - unit: 1/m**2 -- type: pyaml.bpm.bpm - name: BPM_040 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN05-AR/DG-EPOS/BPM.07/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN05-AR/DG-EPOS/BPM.07/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SXD5_VCOR_002 - mapping: - - [B2, SXD5_VCOR_002.sextupole] - - [A0, SXD5_VCOR_002.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN05-AR/EM-SX/SCD.12/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN05-AR/EM-COR/SCD.12-CDLV.06/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_048 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN05-AR/EM-COR/CQLN.14/strength - unit: 1/m -- type: pyaml.magnet.quadrupole - name: QCORR_049 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN05-AR/EM-COR/CQLN.15/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SXD5_003 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN05-AR/EM-SX/SCD.13/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF5_HCOR_002 - mapping: - - [B2, SXF5_HCOR_002.sextupole] - - [B0, SXF5_HCOR_002.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN05-AR/EM-SX/SCF.14/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN05-AR/EM-COR/SCF.14-CDLH.07/strength - unit: '1' -- type: pyaml.magnet.cfm_magnet - name: OCTF5_QCORROCT_37_QT_001 - mapping: - - [B3, OCTF5_QCORROCT_37_QT_001.octupole] - - [B1, OCTF5_QCORROCT_37_QT_001.quadrupole] - - [A1, OCTF5_QCORROCT_37_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN05-AR/EM-OCT/OC.05/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN05-AR/EM-COR/OC.05-CQLN.16/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN05-AR/EM-COR/OC.05-CQLT.06/strength - unit: 1/m**2 -- type: pyaml.bpm.bpm - name: BPM_041 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN05-AR/DG-EPOS/BPM.08/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN05-AR/DG-EPOS/BPM.08/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SXD5_VCOR_003 - mapping: - - [B2, SXD5_VCOR_003.sextupole] - - [A0, SXD5_VCOR_003.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN05-AR/EM-SX/SCD.15/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN05-AR/EM-COR/SCD.15-CDLV.07/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_050 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN05-AR/EM-COR/CQLN.17/strength - unit: 1/m -- type: pyaml.magnet.quadrupole - name: QCORR_051 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN05-AR/EM-COR/CQLN.18/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SXD52_001 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN05-AR/EM-SX/SCD.16/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF52_HCOR_001 - mapping: - - [B2, SXF52_HCOR_001.sextupole] - - [B0, SXF52_HCOR_001.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN05-AR/EM-SX/SCF.17/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN05-AR/EM-COR/SCF.17-CDLH.08/strength - unit: '1' -- type: pyaml.magnet.cfm_magnet - name: OCTF5_QCORROCT_38_QT_001 - mapping: - - [B3, OCTF5_QCORROCT_38_QT_001.octupole] - - [B1, OCTF5_QCORROCT_38_QT_001.quadrupole] - - [A1, OCTF5_QCORROCT_38_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN05-AR/EM-OCT/OC.06/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN05-AR/EM-COR/OC.06-CQLN.19/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN05-AR/EM-COR/OC.06-CQLT.07/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXD52_VCOR_001 - mapping: - - [B2, SXD52_VCOR_001.sextupole] - - [A0, SXD52_VCOR_001.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN05-AR/EM-SX/SCD.18/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN05-AR/EM-COR/SCD.18-CDLV.08/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_042 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN05-AR/DG-EPOS/BPM.09/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN05-AR/DG-EPOS/BPM.09/y_pos - unit: mm -- type: pyaml.magnet.quadrupole - name: QCORR_052 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN05-AR/EM-COR/CQLN.20/strength - unit: 1/m -- type: pyaml.magnet.cfm_magnet - name: SH15_VCOR_001 - mapping: - - [B2, SH15_VCOR_001.sextupole] - - [A0, SH15_VCOR_001.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN05-AR/EM-SX/SHD.04/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN05-AR/EM-COR/SHD.04-CDLV.09/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_043 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN05-AR/DG-EPOS/BPM.10/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN05-AR/DG-EPOS/BPM.10/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SH14_HCOR_001 - mapping: - - [B2, SH14_HCOR_001.sextupole] - - [B0, SH14_HCOR_001.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN05-AR/EM-SX/SHD.05/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN05-AR/EM-COR/SHD.05-CDLH.09/strength - unit: '1' -- type: pyaml.magnet.cfm_magnet - name: OH14_QCORROCT_39_001 - mapping: - - [B3, OH14_QCORROCT_39_001.octupole] - - [B1, OH14_QCORROCT_39_001.quadrupole] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1] - units: [1/m**3, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN05-AR/EM-OCT/OH.03/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN05-AR/EM-COR/OH.03-CQLN.21/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SH13_COR_001 - mapping: - - [B2, SH13_COR_001.sextupole] - - [B0, SH13_COR_001.hcorrector] - - [A0, SH13_COR_001.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0, A0] - units: [1/m**2, '1', '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN05-AR/EM-SX/SHF.06/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN05-AR/EM-COR/SHF.06-CDLH.10/strength - unit: '1' - - type: tango.pyaml.attribute - attribute: AN05-AR/EM-COR/SHF.06-CDLV.10/strength - unit: '1' -- type: pyaml.magnet.cfm_magnet - name: OH13_QCORROCT_40_QT_001 - mapping: - - [B3, OH13_QCORROCT_40_QT_001.octupole] - - [B1, OH13_QCORROCT_40_QT_001.quadrupole] - - [A1, OH13_QCORROCT_40_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN05-AR/EM-OCT/OH.04/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN05-AR/EM-COR/OH.04-CQLN.22/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN05-AR/EM-COR/OH.04-CQLT.08/strength - unit: 1/m**2 -- type: pyaml.bpm.bpm - name: BPM_044 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN06-SD/DG-EPOS/BPM.01/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN06-SD/DG-EPOS/BPM.01/y_pos - unit: mm -- type: pyaml.bpm.bpm - name: BPM_045 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN06-SD/DG-EPOS/BPM.02/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN06-SD/DG-EPOS/BPM.02/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: OH16_QCORROCT_41_001 - mapping: - - [B3, OH16_QCORROCT_41_001.octupole] - - [B1, OH16_QCORROCT_41_001.quadrupole] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1] - units: [1/m**3, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN06-SD/EM-OCT/OH.01/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN06-SD/EM-COR/OH.01-CQLN.01/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SH16_COR_001 - mapping: - - [B2, SH16_COR_001.sextupole] - - [B0, SH16_COR_001.hcorrector] - - [A0, SH16_COR_001.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0, A0] - units: [1/m**2, '1', '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN06-SD/EM-SX/SHD.01/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN06-SD/EM-COR/SHD.01-CDLH.01/strength - unit: '1' - - type: tango.pyaml.attribute - attribute: AN06-SD/EM-COR/SHD.01-CDLV.01/strength - unit: '1' -- type: pyaml.magnet.cfm_magnet - name: SH16_COR_002 - mapping: - - [B2, SH16_COR_002.sextupole] - - [B0, SH16_COR_002.hcorrector] - - [A0, SH16_COR_002.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0, A0] - units: [1/m**2, '1', '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN06-SD/EM-SX/SHD.02/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN06-SD/EM-COR/SHD.02-CDLH.02/strength - unit: '1' - - type: tango.pyaml.attribute - attribute: AN06-SD/EM-COR/SHD.02-CDLV.02/strength - unit: '1' -- type: pyaml.magnet.cfm_magnet - name: OH16_QCORROCT_42_001 - mapping: - - [B3, OH16_QCORROCT_42_001.octupole] - - [B1, OH16_QCORROCT_42_001.quadrupole] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1] - units: [1/m**3, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN06-SD/EM-OCT/OH.02/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN06-SD/EM-COR/OH.02-CQLN.02/strength - unit: 1/m**2 -- type: pyaml.bpm.bpm - name: BPM_046 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN06-SD/DG-EPOS/BPM.03/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN06-SD/DG-EPOS/BPM.03/y_pos - unit: mm -- type: pyaml.bpm.bpm - name: BPM_047 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN06-SD/DG-EPOS/BPM.04/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN06-SD/DG-EPOS/BPM.04/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: OH13_QCORROCT_43_QT_001 - mapping: - - [B3, OH13_QCORROCT_43_QT_001.octupole] - - [B1, OH13_QCORROCT_43_QT_001.quadrupole] - - [A1, OH13_QCORROCT_43_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN06-AR/EM-OCT/OH.01/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN06-AR/EM-COR/OH.01-CQLN.01/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN06-AR/EM-COR/OH.01-CQLT.01/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SH13_COR_002 - mapping: - - [B2, SH13_COR_002.sextupole] - - [B0, SH13_COR_002.hcorrector] - - [A0, SH13_COR_002.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0, A0] - units: [1/m**2, '1', '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN06-AR/EM-SX/SHF.01/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN06-AR/EM-COR/SHF.01-CDLH.03/strength - unit: '1' - - type: tango.pyaml.attribute - attribute: AN06-AR/EM-COR/SHF.01-CDLV.03/strength - unit: '1' -- type: pyaml.magnet.cfm_magnet - name: OH14_QCORROCT_44_001 - mapping: - - [B3, OH14_QCORROCT_44_001.octupole] - - [B1, OH14_QCORROCT_44_001.quadrupole] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1] - units: [1/m**3, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN06-AR/EM-OCT/OH.02/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN06-AR/EM-COR/OH.02-CQLN.02/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SH14_HCOR_002 - mapping: - - [B2, SH14_HCOR_002.sextupole] - - [B0, SH14_HCOR_002.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN06-AR/EM-SX/SHD.02/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN06-AR/EM-COR/SHD.02-CDLH.04/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_048 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN06-AR/DG-EPOS/BPM.05/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN06-AR/DG-EPOS/BPM.05/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SH15_VCOR_002 - mapping: - - [B2, SH15_VCOR_002.sextupole] - - [A0, SH15_VCOR_002.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN06-AR/EM-SX/SHD.03/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN06-AR/EM-COR/SHD.03-CDLV.04/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_053 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN06-AR/EM-COR/CQLN.03/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SXD52_002 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN06-AR/EM-SX/SCD.01/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: OCTF5_QCORROCT_45_QT_001 - mapping: - - [B3, OCTF5_QCORROCT_45_QT_001.octupole] - - [B1, OCTF5_QCORROCT_45_QT_001.quadrupole] - - [A1, OCTF5_QCORROCT_45_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN06-AR/EM-OCT/OC.01/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN06-AR/EM-COR/OC.01-CQLN.04/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN06-AR/EM-COR/OC.01-CQLT.02/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF52_HCOR_002 - mapping: - - [B2, SXF52_HCOR_002.sextupole] - - [B0, SXF52_HCOR_002.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN06-AR/EM-SX/SCF.02/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN06-AR/EM-COR/SCF.02-CDLH.05/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_049 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN06-AR/DG-EPOS/BPM.06/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN06-AR/DG-EPOS/BPM.06/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SXD52_VCOR_002 - mapping: - - [B2, SXD52_VCOR_002.sextupole] - - [A0, SXD52_VCOR_002.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN06-AR/EM-SX/SCD.03/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN06-AR/EM-COR/SCD.03-CDLV.05/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_054 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN06-AR/EM-COR/CQLN.05/strength - unit: 1/m -- type: pyaml.magnet.quadrupole - name: QCORR_055 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN06-AR/EM-COR/CQLN.06/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SXD5_004 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN06-AR/EM-SX/SCD.04/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: OCTF5_QCORROCT_46_QT_001 - mapping: - - [B3, OCTF5_QCORROCT_46_QT_001.octupole] - - [B1, OCTF5_QCORROCT_46_QT_001.quadrupole] - - [A1, OCTF5_QCORROCT_46_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN06-AR/EM-OCT/OC.02/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN06-AR/EM-COR/OC.02-CQLN.07/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN06-AR/EM-COR/OC.02-CQLT.03/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF5_HCOR_003 - mapping: - - [B2, SXF5_HCOR_003.sextupole] - - [B0, SXF5_HCOR_003.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN06-AR/EM-SX/SCF.05/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN06-AR/EM-COR/SCF.05-CDLH.06/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_050 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN06-AR/DG-EPOS/BPM.07/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN06-AR/DG-EPOS/BPM.07/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SXD5_VCOR_004 - mapping: - - [B2, SXD5_VCOR_004.sextupole] - - [A0, SXD5_VCOR_004.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN06-AR/EM-SX/SCD.06/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN06-AR/EM-COR/SCD.06-CDLV.06/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_056 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN06-AR/EM-COR/CQLN.08/strength - unit: 1/m -- type: pyaml.magnet.quadrupole - name: QCORR_057 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN06-AR/EM-COR/CQLN.09/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SXD5_005 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN06-AR/EM-SX/SCD.07/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: OCTF5_QCORROCT_47_QT_001 - mapping: - - [B3, OCTF5_QCORROCT_47_QT_001.octupole] - - [B1, OCTF5_QCORROCT_47_QT_001.quadrupole] - - [A1, OCTF5_QCORROCT_47_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN06-AR/EM-OCT/OC.03/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN06-AR/EM-COR/OC.03-CQLN.10/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN06-AR/EM-COR/OC.03-CQLT.04/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF53_HCOR_003 - mapping: - - [B2, SXF53_HCOR_003.sextupole] - - [B0, SXF53_HCOR_003.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN06-AR/EM-SX/SCF.08/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN06-AR/EM-COR/SCF.08-CDLH.07/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_051 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN06-AR/DG-EPOS/BPM.08/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN06-AR/DG-EPOS/BPM.08/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SXD53_VCOR_002 - mapping: - - [B2, SXD53_VCOR_002.sextupole] - - [A0, SXD53_VCOR_002.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN06-AR/EM-SX/SCD.09/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN06-AR/EM-COR/SCD.09-CDLV.07/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_058 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN06-AR/EM-COR/CQLN.11/strength - unit: 1/m -- type: pyaml.magnet.quadrupole - name: QCORR_059 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN06-AR/EM-COR/CQLN.12/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SXD53_002 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN06-AR/EM-SX/SCD.10/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF53_HCOR_004 - mapping: - - [B2, SXF53_HCOR_004.sextupole] - - [B0, SXF53_HCOR_004.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN06-AR/EM-SX/SCF.11/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN06-AR/EM-COR/SCF.11-CDLH.08/strength - unit: '1' -- type: pyaml.magnet.cfm_magnet - name: OCTF5_QCORROCT_48_QT_001 - mapping: - - [B3, OCTF5_QCORROCT_48_QT_001.octupole] - - [B1, OCTF5_QCORROCT_48_QT_001.quadrupole] - - [A1, OCTF5_QCORROCT_48_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN06-AR/EM-OCT/OC.04/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN06-AR/EM-COR/OC.04-CQLN.13/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN06-AR/EM-COR/OC.04-CQLT.05/strength - unit: 1/m**2 -- type: pyaml.bpm.bpm - name: BPM_052 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN06-AR/DG-EPOS/BPM.09/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN06-AR/DG-EPOS/BPM.09/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SXD5_VCOR_005 - mapping: - - [B2, SXD5_VCOR_005.sextupole] - - [A0, SXD5_VCOR_005.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN06-AR/EM-SX/SCD.12/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN06-AR/EM-COR/SCD.12-CDLV.08/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_060 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN06-AR/EM-COR/CQLN.14/strength - unit: 1/m -- type: pyaml.magnet.quadrupole - name: QCORR_061 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN06-AR/EM-COR/CQLN.15/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SXD5_006 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN06-AR/EM-SX/SCD.13/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF5_HCOR_004 - mapping: - - [B2, SXF5_HCOR_004.sextupole] - - [B0, SXF5_HCOR_004.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN06-AR/EM-SX/SCF.14/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN06-AR/EM-COR/SCF.14-CDLH.09/strength - unit: '1' -- type: pyaml.magnet.cfm_magnet - name: OCTF5_QCORROCT_49_QT_001 - mapping: - - [B3, OCTF5_QCORROCT_49_QT_001.octupole] - - [B1, OCTF5_QCORROCT_49_QT_001.quadrupole] - - [A1, OCTF5_QCORROCT_49_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN06-AR/EM-OCT/OC.05/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN06-AR/EM-COR/OC.05-CQLN.16/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN06-AR/EM-COR/OC.05-CQLT.06/strength - unit: 1/m**2 -- type: pyaml.bpm.bpm - name: BPM_053 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN06-AR/DG-EPOS/BPM.10/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN06-AR/DG-EPOS/BPM.10/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SXD5_VCOR_006 - mapping: - - [B2, SXD5_VCOR_006.sextupole] - - [A0, SXD5_VCOR_006.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN06-AR/EM-SX/SCD.15/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN06-AR/EM-COR/SCD.15-CDLV.09/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_062 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN06-AR/EM-COR/CQLN.17/strength - unit: 1/m -- type: pyaml.magnet.quadrupole - name: QCORR_063 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN06-AR/EM-COR/CQLN.18/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SXD51_002 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN06-AR/EM-SX/SCD.16/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF51_HCOR_002 - mapping: - - [B2, SXF51_HCOR_002.sextupole] - - [B0, SXF51_HCOR_002.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN06-AR/EM-SX/SCF.17/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN06-AR/EM-COR/SCF.17-CDLH.10/strength - unit: '1' -- type: pyaml.magnet.cfm_magnet - name: OCTF5_QCORROCT_50_QT_001 - mapping: - - [B3, OCTF5_QCORROCT_50_QT_001.octupole] - - [B1, OCTF5_QCORROCT_50_QT_001.quadrupole] - - [A1, OCTF5_QCORROCT_50_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN06-AR/EM-OCT/OC.06/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN06-AR/EM-COR/OC.06-CQLN.19/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN06-AR/EM-COR/OC.06-CQLT.07/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXD51_VCOR_002 - mapping: - - [B2, SXD51_VCOR_002.sextupole] - - [A0, SXD51_VCOR_002.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN06-AR/EM-SX/SCD.18/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN06-AR/EM-COR/SCD.18-CDLV.10/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_054 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN06-AR/DG-EPOS/BPM.11/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN06-AR/DG-EPOS/BPM.11/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SH12_COR_003 - mapping: - - [B2, SH12_COR_003.sextupole] - - [B0, SH12_COR_003.hcorrector] - - [A0, SH12_COR_003.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0, A0] - units: [1/m**2, '1', '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN06-AR/EM-SX/SHD.04/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN06-AR/EM-COR/SHD.04-CDLH.11/strength - unit: '1' - - type: tango.pyaml.attribute - attribute: AN06-AR/EM-COR/SHD.04-CDLV.11/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_064 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN06-AR/EM-COR/CQLN.20/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SH11_003 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN06-AR/EM-SX/SHD.05/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: OH11_QCORROCT_51_001 - mapping: - - [B3, OH11_QCORROCT_51_001.octupole] - - [B1, OH11_QCORROCT_51_001.quadrupole] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1] - units: [1/m**3, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN06-AR/EM-OCT/OH.03/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN06-AR/EM-COR/OH.03-CQLN.21/strength - unit: 1/m**2 -- type: pyaml.bpm.bpm - name: BPM_055 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN06-AR/DG-EPOS/BPM.12/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN06-AR/DG-EPOS/BPM.12/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SH10_COR_003 - mapping: - - [B2, SH10_COR_003.sextupole] - - [B0, SH10_COR_003.hcorrector] - - [A0, SH10_COR_003.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0, A0] - units: [1/m**2, '1', '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN06-AR/EM-SX/SHF.06/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN06-AR/EM-COR/SHF.06-CDLH.12/strength - unit: '1' - - type: tango.pyaml.attribute - attribute: AN06-AR/EM-COR/SHF.06-CDLV.12/strength - unit: '1' -- type: pyaml.magnet.cfm_magnet - name: OH10_QCORROCT_52_QT_001 - mapping: - - [B3, OH10_QCORROCT_52_QT_001.octupole] - - [B1, OH10_QCORROCT_52_QT_001.quadrupole] - - [A1, OH10_QCORROCT_52_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN06-AR/EM-OCT/OH.04/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN06-AR/EM-COR/OH.04-CQLN.22/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN06-AR/EM-COR/OH.04-CQLT.08/strength - unit: 1/m**2 -- type: pyaml.bpm.bpm - name: BPM_056 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN07-SD/DG-EPOS/BPM.01/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN07-SD/DG-EPOS/BPM.01/y_pos - unit: mm -- type: pyaml.bpm.bpm - name: BPM_057 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN07-SD/DG-EPOS/BPM.02/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN07-SD/DG-EPOS/BPM.02/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: OH10_QCORROCT_53_QT_001 - mapping: - - [B3, OH10_QCORROCT_53_QT_001.octupole] - - [B1, OH10_QCORROCT_53_QT_001.quadrupole] - - [A1, OH10_QCORROCT_53_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN07-AR/EM-OCT/OH.01/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN07-AR/EM-COR/OH.01-CQLN.01/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN07-AR/EM-COR/OH.01-CQLT.01/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SH10_COR_004 - mapping: - - [B2, SH10_COR_004.sextupole] - - [B0, SH10_COR_004.hcorrector] - - [A0, SH10_COR_004.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0, A0] - units: [1/m**2, '1', '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN07-AR/EM-SX/SHF.01/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN07-AR/EM-COR/SHF.01-CDLH.01/strength - unit: '1' - - type: tango.pyaml.attribute - attribute: AN07-AR/EM-COR/SHF.01-CDLV.01/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_058 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN07-AR/DG-EPOS/BPM.03/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN07-AR/DG-EPOS/BPM.03/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: OH11_QCORROCT_54_001 - mapping: - - [B3, OH11_QCORROCT_54_001.octupole] - - [B1, OH11_QCORROCT_54_001.quadrupole] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1] - units: [1/m**3, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN07-AR/EM-OCT/OH.02/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN07-AR/EM-COR/OH.02-CQLN.02/strength - unit: 1/m**2 -- type: pyaml.magnet.sextupole - name: SH11_004 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN07-AR/EM-SX/SHD.02/strength - unit: 1/m**2 -- type: pyaml.magnet.quadrupole - name: QCORR_065 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN07-AR/EM-COR/CQLN.03/strength - unit: 1/m -- type: pyaml.magnet.cfm_magnet - name: SH12_COR_004 - mapping: - - [B2, SH12_COR_004.sextupole] - - [B0, SH12_COR_004.hcorrector] - - [A0, SH12_COR_004.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0, A0] - units: [1/m**2, '1', '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN07-AR/EM-SX/SHD.03/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN07-AR/EM-COR/SHD.03-CDLH.02/strength - unit: '1' - - type: tango.pyaml.attribute - attribute: AN07-AR/EM-COR/SHD.03-CDLV.02/strength - unit: '1' -- type: pyaml.magnet.sextupole - name: SXD42_002 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN07-AR/EM-SX/SCD.01/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: OCTF4_QCORROCT_55_QT_001 - mapping: - - [B3, OCTF4_QCORROCT_55_QT_001.octupole] - - [B1, OCTF4_QCORROCT_55_QT_001.quadrupole] - - [A1, OCTF4_QCORROCT_55_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN07-AR/EM-OCT/OC.01/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN07-AR/EM-COR/OC.01-CQLN.04/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN07-AR/EM-COR/OC.01-CQLT.02/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF42_HCOR_002 - mapping: - - [B2, SXF42_HCOR_002.sextupole] - - [B0, SXF42_HCOR_002.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN07-AR/EM-SX/SCF.02/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN07-AR/EM-COR/SCF.02-CDLH.03/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_059 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN07-AR/DG-EPOS/BPM.04/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN07-AR/DG-EPOS/BPM.04/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SXD42_VCOR_002 - mapping: - - [B2, SXD42_VCOR_002.sextupole] - - [A0, SXD42_VCOR_002.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN07-AR/EM-SX/SCD.03/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN07-AR/EM-COR/SCD.03-CDLV.03/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_066 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN07-AR/EM-COR/CQLN.05/strength - unit: 1/m -- type: pyaml.magnet.quadrupole - name: QCORR_067 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN07-AR/EM-COR/CQLN.06/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SXD4_002 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN07-AR/EM-SX/SCD.04/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: OCTF4_QCORROCT_56_QT_001 - mapping: - - [B3, OCTF4_QCORROCT_56_QT_001.octupole] - - [B1, OCTF4_QCORROCT_56_QT_001.quadrupole] - - [A1, OCTF4_QCORROCT_56_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN07-AR/EM-OCT/OC.02/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN07-AR/EM-COR/OC.02-CQLN.07/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN07-AR/EM-COR/OC.02-CQLT.03/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF4_HCOR_002 - mapping: - - [B2, SXF4_HCOR_002.sextupole] - - [B0, SXF4_HCOR_002.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN07-AR/EM-SX/SCF.05/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN07-AR/EM-COR/SCF.05-CDLH.04/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_060 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN07-AR/DG-EPOS/BPM.05/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN07-AR/DG-EPOS/BPM.05/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SXD4_VCOR_002 - mapping: - - [B2, SXD4_VCOR_002.sextupole] - - [A0, SXD4_VCOR_002.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN07-AR/EM-SX/SCD.06/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN07-AR/EM-COR/SCD.06-CDLV.04/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_068 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN07-AR/EM-COR/CQLN.08/strength - unit: 1/m -- type: pyaml.magnet.quadrupole - name: QCORR_069 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN07-AR/EM-COR/CQLN.09/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SXD41_002 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN07-AR/EM-SX/SCD.07/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF41_HCOR_002 - mapping: - - [B2, SXF41_HCOR_002.sextupole] - - [B0, SXF41_HCOR_002.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN07-AR/EM-SX/SCF.08/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN07-AR/EM-COR/SCF.08-CDLH.05/strength - unit: '1' -- type: pyaml.magnet.cfm_magnet - name: OCTF4_QCORROCT_57_QT_001 - mapping: - - [B3, OCTF4_QCORROCT_57_QT_001.octupole] - - [B1, OCTF4_QCORROCT_57_QT_001.quadrupole] - - [A1, OCTF4_QCORROCT_57_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN07-AR/EM-OCT/OC.03/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN07-AR/EM-COR/OC.03-CQLN.10/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN07-AR/EM-COR/OC.03-CQLT.04/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXD41_VCOR_002 - mapping: - - [B2, SXD41_VCOR_002.sextupole] - - [A0, SXD41_VCOR_002.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN07-AR/EM-SX/SCD.09/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN07-AR/EM-COR/SCD.09-CDLV.05/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_061 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN07-AR/DG-EPOS/BPM.06/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN07-AR/DG-EPOS/BPM.06/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SH9_COR_005 - mapping: - - [B2, SH9_COR_005.sextupole] - - [B0, SH9_COR_005.hcorrector] - - [A0, SH9_COR_005.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0, A0] - units: [1/m**2, '1', '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN07-AR/EM-SX/SHD.04/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN07-AR/EM-COR/SHD.04-CDLH.06/strength - unit: '1' - - type: tango.pyaml.attribute - attribute: AN07-AR/EM-COR/SHD.04-CDLV.06/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_070 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN07-AR/EM-COR/CQLN.11/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SH8_005 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN07-AR/EM-SX/SHD.05/strength - unit: 1/m**2 -- type: pyaml.magnet.quadrupole - name: QCORR_071 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN07-AR/EM-COR/CQLN.12/strength - unit: 1/m -- type: pyaml.bpm.bpm - name: BPM_062 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN07-AR/DG-EPOS/BPM.07/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN07-AR/DG-EPOS/BPM.07/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SH7_COR_005 - mapping: - - [B2, SH7_COR_005.sextupole] - - [B0, SH7_COR_005.hcorrector] - - [A0, SH7_COR_005.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0, A0] - units: [1/m**2, '1', '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN07-AR/EM-SX/SHF.06/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN07-AR/EM-COR/SHF.06-CDLH.07/strength - unit: '1' - - type: tango.pyaml.attribute - attribute: AN07-AR/EM-COR/SHF.06-CDLV.07/strength - unit: '1' -- type: pyaml.magnet.cfm_magnet - name: OH7_QCORROCT_58_QT_001 - mapping: - - [B3, OH7_QCORROCT_58_QT_001.octupole] - - [B1, OH7_QCORROCT_58_QT_001.quadrupole] - - [A1, OH7_QCORROCT_58_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN07-AR/EM-OCT/OH.03/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN07-AR/EM-COR/OH.03-CQLN.13/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN07-AR/EM-COR/OH.03-CQLT.05/strength - unit: 1/m**2 -- type: pyaml.bpm.bpm - name: BPM_063 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN08-SD/DG-EPOS/BPM.01/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN08-SD/DG-EPOS/BPM.01/y_pos - unit: mm -- type: pyaml.bpm.bpm - name: BPM_064 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN08-SD/DG-EPOS/BPM.02/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN08-SD/DG-EPOS/BPM.02/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: OH7_QCORROCT_59_QT_001 - mapping: - - [B3, OH7_QCORROCT_59_QT_001.octupole] - - [B1, OH7_QCORROCT_59_QT_001.quadrupole] - - [A1, OH7_QCORROCT_59_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN08-AR/EM-OCT/OH.01/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN08-AR/EM-COR/OH.01-CQLN.01/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN08-AR/EM-COR/OH.01-CQLT.01/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SH7_COR_006 - mapping: - - [B2, SH7_COR_006.sextupole] - - [B0, SH7_COR_006.hcorrector] - - [A0, SH7_COR_006.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0, A0] - units: [1/m**2, '1', '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN08-AR/EM-SX/SHF.01/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN08-AR/EM-COR/SHF.01-CDLH.01/strength - unit: '1' - - type: tango.pyaml.attribute - attribute: AN08-AR/EM-COR/SHF.01-CDLV.01/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_065 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN08-AR/DG-EPOS/BPM.03/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN08-AR/DG-EPOS/BPM.03/y_pos - unit: mm -- type: pyaml.magnet.quadrupole - name: QCORR_072 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN08-AR/EM-COR/CQLN.02/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SH8_006 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN08-AR/EM-SX/SHD.02/strength - unit: 1/m**2 -- type: pyaml.magnet.quadrupole - name: QCORR_073 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN08-AR/EM-COR/CQLN.03/strength - unit: 1/m -- type: pyaml.magnet.cfm_magnet - name: SH9_COR_006 - mapping: - - [B2, SH9_COR_006.sextupole] - - [B0, SH9_COR_006.hcorrector] - - [A0, SH9_COR_006.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0, A0] - units: [1/m**2, '1', '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN08-AR/EM-SX/SHD.03/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN08-AR/EM-COR/SHD.03-CDLH.02/strength - unit: '1' - - type: tango.pyaml.attribute - attribute: AN08-AR/EM-COR/SHD.03-CDLV.02/strength - unit: '1' -- type: pyaml.magnet.sextupole - name: SXD32_002 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN08-AR/EM-SX/SCD.01/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: OCTF3_QCORROCT_60_QT_001 - mapping: - - [B3, OCTF3_QCORROCT_60_QT_001.octupole] - - [B1, OCTF3_QCORROCT_60_QT_001.quadrupole] - - [A1, OCTF3_QCORROCT_60_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN08-AR/EM-OCT/OC.01/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN08-AR/EM-COR/OC.01-CQLN.04/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN08-AR/EM-COR/OC.01-CQLT.02/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF32_HCOR_002 - mapping: - - [B2, SXF32_HCOR_002.sextupole] - - [B0, SXF32_HCOR_002.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN08-AR/EM-SX/SCF.02/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN08-AR/EM-COR/SCF.02-CDLH.03/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_066 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN08-AR/DG-EPOS/BPM.04/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN08-AR/DG-EPOS/BPM.04/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SXD32_VCOR_002 - mapping: - - [B2, SXD32_VCOR_002.sextupole] - - [A0, SXD32_VCOR_002.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN08-AR/EM-SX/SCD.03/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN08-AR/EM-COR/SCD.03-CDLV.03/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_074 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN08-AR/EM-COR/CQLN.05/strength - unit: 1/m -- type: pyaml.magnet.quadrupole - name: QCORR_075 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN08-AR/EM-COR/CQLN.06/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SXD3_004 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN08-AR/EM-SX/SCD.04/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: OCTF3_QCORROCT_61_QT_001 - mapping: - - [B3, OCTF3_QCORROCT_61_QT_001.octupole] - - [B1, OCTF3_QCORROCT_61_QT_001.quadrupole] - - [A1, OCTF3_QCORROCT_61_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN08-AR/EM-OCT/OC.02/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN08-AR/EM-COR/OC.02-CQLN.07/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN08-AR/EM-COR/OC.02-CQLT.03/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF3_HCOR_003 - mapping: - - [B2, SXF3_HCOR_003.sextupole] - - [B0, SXF3_HCOR_003.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN08-AR/EM-SX/SCF.05/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN08-AR/EM-COR/SCF.05-CDLH.04/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_067 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN08-AR/DG-EPOS/BPM.05/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN08-AR/DG-EPOS/BPM.05/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SXD3_VCOR_004 - mapping: - - [B2, SXD3_VCOR_004.sextupole] - - [A0, SXD3_VCOR_004.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN08-AR/EM-SX/SCD.06/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN08-AR/EM-COR/SCD.06-CDLV.04/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_076 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN08-AR/EM-COR/CQLN.08/strength - unit: 1/m -- type: pyaml.magnet.quadrupole - name: QCORR_077 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN08-AR/EM-COR/CQLN.09/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SXD3_005 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN08-AR/EM-SX/SCD.07/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: OCTF3_QCORROCT_62_QT_001 - mapping: - - [B3, OCTF3_QCORROCT_62_QT_001.octupole] - - [B1, OCTF3_QCORROCT_62_QT_001.quadrupole] - - [A1, OCTF3_QCORROCT_62_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN08-AR/EM-OCT/OC.03/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN08-AR/EM-COR/OC.03-CQLN.10/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN08-AR/EM-COR/OC.03-CQLT.04/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF33_HCOR_003 - mapping: - - [B2, SXF33_HCOR_003.sextupole] - - [B0, SXF33_HCOR_003.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN08-AR/EM-SX/SCF.08/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN08-AR/EM-COR/SCF.08-CDLH.05/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_068 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN08-AR/DG-EPOS/BPM.06/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN08-AR/DG-EPOS/BPM.06/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SXD33_VCOR_002 - mapping: - - [B2, SXD33_VCOR_002.sextupole] - - [A0, SXD33_VCOR_002.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN08-AR/EM-SX/SCD.09/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN08-AR/EM-COR/SCD.09-CDLV.05/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_078 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN08-AR/EM-COR/CQLN.11/strength - unit: 1/m -- type: pyaml.magnet.quadrupole - name: QCORR_079 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN08-AR/EM-COR/CQLN.12/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SXD33_002 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN08-AR/EM-SX/SCD.10/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF33_HCOR_004 - mapping: - - [B2, SXF33_HCOR_004.sextupole] - - [B0, SXF33_HCOR_004.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN08-AR/EM-SX/SCF.11/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN08-AR/EM-COR/SCF.11-CDLH.06/strength - unit: '1' -- type: pyaml.magnet.cfm_magnet - name: OCTF3_QCORROCT_63_QT_001 - mapping: - - [B3, OCTF3_QCORROCT_63_QT_001.octupole] - - [B1, OCTF3_QCORROCT_63_QT_001.quadrupole] - - [A1, OCTF3_QCORROCT_63_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN08-AR/EM-OCT/OC.04/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN08-AR/EM-COR/OC.04-CQLN.13/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN08-AR/EM-COR/OC.04-CQLT.05/strength - unit: 1/m**2 -- type: pyaml.bpm.bpm - name: BPM_069 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN08-AR/DG-EPOS/BPM.07/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN08-AR/DG-EPOS/BPM.07/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SXD3_VCOR_005 - mapping: - - [B2, SXD3_VCOR_005.sextupole] - - [A0, SXD3_VCOR_005.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN08-AR/EM-SX/SCD.12/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN08-AR/EM-COR/SCD.12-CDLV.06/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_080 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN08-AR/EM-COR/CQLN.14/strength - unit: 1/m -- type: pyaml.magnet.quadrupole - name: QCORR_081 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN08-AR/EM-COR/CQLN.15/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SXD3_006 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN08-AR/EM-SX/SCD.13/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF3_HCOR_004 - mapping: - - [B2, SXF3_HCOR_004.sextupole] - - [B0, SXF3_HCOR_004.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN08-AR/EM-SX/SCF.14/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN08-AR/EM-COR/SCF.14-CDLH.07/strength - unit: '1' -- type: pyaml.magnet.cfm_magnet - name: OCTF3_QCORROCT_64_QT_001 - mapping: - - [B3, OCTF3_QCORROCT_64_QT_001.octupole] - - [B1, OCTF3_QCORROCT_64_QT_001.quadrupole] - - [A1, OCTF3_QCORROCT_64_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN08-AR/EM-OCT/OC.05/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN08-AR/EM-COR/OC.05-CQLN.16/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN08-AR/EM-COR/OC.05-CQLT.06/strength - unit: 1/m**2 -- type: pyaml.bpm.bpm - name: BPM_070 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN08-AR/DG-EPOS/BPM.08/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN08-AR/DG-EPOS/BPM.08/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SXD3_VCOR_006 - mapping: - - [B2, SXD3_VCOR_006.sextupole] - - [A0, SXD3_VCOR_006.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN08-AR/EM-SX/SCD.15/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN08-AR/EM-COR/SCD.15-CDLV.07/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_082 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN08-AR/EM-COR/CQLN.17/strength - unit: 1/m -- type: pyaml.magnet.quadrupole - name: QCORR_083 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN08-AR/EM-COR/CQLN.18/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SXD31_002 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN08-AR/EM-SX/SCD.16/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF31_HCOR_002 - mapping: - - [B2, SXF31_HCOR_002.sextupole] - - [B0, SXF31_HCOR_002.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN08-AR/EM-SX/SCF.17/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN08-AR/EM-COR/SCF.17-CDLH.08/strength - unit: '1' -- type: pyaml.magnet.cfm_magnet - name: OCTF3_QCORROCT_65_QT_001 - mapping: - - [B3, OCTF3_QCORROCT_65_QT_001.octupole] - - [B1, OCTF3_QCORROCT_65_QT_001.quadrupole] - - [A1, OCTF3_QCORROCT_65_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN08-AR/EM-OCT/OC.06/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN08-AR/EM-COR/OC.06-CQLN.19/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN08-AR/EM-COR/OC.06-CQLT.07/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXD31_VCOR_002 - mapping: - - [B2, SXD31_VCOR_002.sextupole] - - [A0, SXD31_VCOR_002.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN08-AR/EM-SX/SCD.18/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN08-AR/EM-COR/SCD.18-CDLV.08/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_071 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN08-AR/DG-EPOS/BPM.09/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN08-AR/DG-EPOS/BPM.09/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SH9_COR_007 - mapping: - - [B2, SH9_COR_007.sextupole] - - [B0, SH9_COR_007.hcorrector] - - [A0, SH9_COR_007.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0, A0] - units: [1/m**2, '1', '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN08-AR/EM-SX/SHD.04/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN08-AR/EM-COR/SHD.04-CDLH.09/strength - unit: '1' - - type: tango.pyaml.attribute - attribute: AN08-AR/EM-COR/SHD.04-CDLV.09/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_084 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN08-AR/EM-COR/CQLN.20/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SH8_007 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN08-AR/EM-SX/SHD.05/strength - unit: 1/m**2 -- type: pyaml.magnet.quadrupole - name: QCORR_085 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN08-AR/EM-COR/CQLN.21/strength - unit: 1/m -- type: pyaml.bpm.bpm - name: BPM_072 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN08-AR/DG-EPOS/BPM.10/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN08-AR/DG-EPOS/BPM.10/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SH7_COR_007 - mapping: - - [B2, SH7_COR_007.sextupole] - - [B0, SH7_COR_007.hcorrector] - - [A0, SH7_COR_007.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0, A0] - units: [1/m**2, '1', '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN08-AR/EM-SX/SHF.06/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN08-AR/EM-COR/SHF.06-CDLH.10/strength - unit: '1' - - type: tango.pyaml.attribute - attribute: AN08-AR/EM-COR/SHF.06-CDLV.10/strength - unit: '1' -- type: pyaml.magnet.cfm_magnet - name: OH7_QCORROCT_66_QT_001 - mapping: - - [B3, OH7_QCORROCT_66_QT_001.octupole] - - [B1, OH7_QCORROCT_66_QT_001.quadrupole] - - [A1, OH7_QCORROCT_66_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN08-AR/EM-OCT/OH.02/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN08-AR/EM-COR/OH.02-CQLN.22/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN08-AR/EM-COR/OH.02-CQLT.08/strength - unit: 1/m**2 -- type: pyaml.bpm.bpm - name: BPM_073 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN09-SD/DG-EPOS/BPM.01/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN09-SD/DG-EPOS/BPM.01/y_pos - unit: mm -- type: pyaml.bpm.bpm - name: BPM_074 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN09-SD/DG-EPOS/BPM.02/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN09-SD/DG-EPOS/BPM.02/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: OH7_QCORROCT_67_QT_001 - mapping: - - [B3, OH7_QCORROCT_67_QT_001.octupole] - - [B1, OH7_QCORROCT_67_QT_001.quadrupole] - - [A1, OH7_QCORROCT_67_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN09-AR/EM-OCT/OH.01/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN09-AR/EM-COR/OH.01-CQLN.01/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN09-AR/EM-COR/OH.01-CQLT.01/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SH7_COR_008 - mapping: - - [B2, SH7_COR_008.sextupole] - - [B0, SH7_COR_008.hcorrector] - - [A0, SH7_COR_008.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0, A0] - units: [1/m**2, '1', '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN09-AR/EM-SX/SHF.01/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN09-AR/EM-COR/SHF.01-CDLH.01/strength - unit: '1' - - type: tango.pyaml.attribute - attribute: AN09-AR/EM-COR/SHF.01-CDLV.01/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_075 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN09-AR/DG-EPOS/BPM.03/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN09-AR/DG-EPOS/BPM.03/y_pos - unit: mm -- type: pyaml.magnet.quadrupole - name: QCORR_086 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN09-AR/EM-COR/CQLN.02/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SH8_008 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN09-AR/EM-SX/SHD.02/strength - unit: 1/m**2 -- type: pyaml.magnet.quadrupole - name: QCORR_087 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN09-AR/EM-COR/CQLN.03/strength - unit: 1/m -- type: pyaml.magnet.cfm_magnet - name: SH9_COR_008 - mapping: - - [B2, SH9_COR_008.sextupole] - - [B0, SH9_COR_008.hcorrector] - - [A0, SH9_COR_008.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0, A0] - units: [1/m**2, '1', '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN09-AR/EM-SX/SHD.03/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN09-AR/EM-COR/SHD.03-CDLH.02/strength - unit: '1' - - type: tango.pyaml.attribute - attribute: AN09-AR/EM-COR/SHD.03-CDLV.02/strength - unit: '1' -- type: pyaml.magnet.sextupole - name: SXD22_002 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN09-AR/EM-SX/SCD.01/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: OCTF2_QCORROCT_68_QT_001 - mapping: - - [B3, OCTF2_QCORROCT_68_QT_001.octupole] - - [B1, OCTF2_QCORROCT_68_QT_001.quadrupole] - - [A1, OCTF2_QCORROCT_68_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN09-AR/EM-OCT/OC.01/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN09-AR/EM-COR/OC.01-CQLN.04/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN09-AR/EM-COR/OC.01-CQLT.02/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF22_HCOR_002 - mapping: - - [B2, SXF22_HCOR_002.sextupole] - - [B0, SXF22_HCOR_002.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN09-AR/EM-SX/SCF.02/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN09-AR/EM-COR/SCF.02-CDLH.03/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_076 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN09-AR/DG-EPOS/BPM.04/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN09-AR/DG-EPOS/BPM.04/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SXD22_VCOR_002 - mapping: - - [B2, SXD22_VCOR_002.sextupole] - - [A0, SXD22_VCOR_002.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN09-AR/EM-SX/SCD.03/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN09-AR/EM-COR/SCD.03-CDLV.03/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_088 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN09-AR/EM-COR/CQLN.05/strength - unit: 1/m -- type: pyaml.magnet.quadrupole - name: QCORR_089 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN09-AR/EM-COR/CQLN.06/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SXD2_002 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN09-AR/EM-SX/SCD.04/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF2_HCOR_002 - mapping: - - [B2, SXF2_HCOR_002.sextupole] - - [B0, SXF2_HCOR_002.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN09-AR/EM-SX/SCF.05/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN09-AR/EM-COR/SCF.05-CDLH.04/strength - unit: '1' -- type: pyaml.magnet.cfm_magnet - name: OCTF2_QCORROCT_69_QT_001 - mapping: - - [B3, OCTF2_QCORROCT_69_QT_001.octupole] - - [B1, OCTF2_QCORROCT_69_QT_001.quadrupole] - - [A1, OCTF2_QCORROCT_69_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN09-AR/EM-OCT/OC.02/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN09-AR/EM-COR/OC.02-CQLN.07/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN09-AR/EM-COR/OC.02-CQLT.03/strength - unit: 1/m**2 -- type: pyaml.bpm.bpm - name: BPM_077 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN09-AR/DG-EPOS/BPM.05/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN09-AR/DG-EPOS/BPM.05/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SXD2_VCOR_002 - mapping: - - [B2, SXD2_VCOR_002.sextupole] - - [A0, SXD2_VCOR_002.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN09-AR/EM-SX/SCD.06/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN09-AR/EM-COR/SCD.06-CDLV.04/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_090 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN09-AR/EM-COR/CQLN.08/strength - unit: 1/m -- type: pyaml.magnet.quadrupole - name: QCORR_091 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN09-AR/EM-COR/CQLN.09/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SXD21_002 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN09-AR/EM-SX/SCD.07/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF21_HCOR_002 - mapping: - - [B2, SXF21_HCOR_002.sextupole] - - [B0, SXF21_HCOR_002.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN09-AR/EM-SX/SCF.08/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN09-AR/EM-COR/SCF.08-CDLH.05/strength - unit: '1' -- type: pyaml.magnet.cfm_magnet - name: OCTF2_QCORROCT_70_QT_001 - mapping: - - [B3, OCTF2_QCORROCT_70_QT_001.octupole] - - [B1, OCTF2_QCORROCT_70_QT_001.quadrupole] - - [A1, OCTF2_QCORROCT_70_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN09-AR/EM-OCT/OC.03/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN09-AR/EM-COR/OC.03-CQLN.10/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN09-AR/EM-COR/OC.03-CQLT.04/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXD21_VCOR_002 - mapping: - - [B2, SXD21_VCOR_002.sextupole] - - [A0, SXD21_VCOR_002.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN09-AR/EM-SX/SCD.09/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN09-AR/EM-COR/SCD.09-CDLV.05/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_078 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN09-AR/DG-EPOS/BPM.06/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN09-AR/DG-EPOS/BPM.06/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SH6_COR_003 - mapping: - - [B2, SH6_COR_003.sextupole] - - [B0, SH6_COR_003.hcorrector] - - [A0, SH6_COR_003.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0, A0] - units: [1/m**2, '1', '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN09-AR/EM-SX/SHD.04/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN09-AR/EM-COR/SHD.04-CDLH.06/strength - unit: '1' - - type: tango.pyaml.attribute - attribute: AN09-AR/EM-COR/SHD.04-CDLV.06/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_092 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN09-AR/EM-COR/CQLN.11/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SH5_003 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN09-AR/EM-SX/SHD.05/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: OH5_QCORROCT_71_001 - mapping: - - [B3, OH5_QCORROCT_71_001.octupole] - - [B1, OH5_QCORROCT_71_001.quadrupole] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1] - units: [1/m**3, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN09-AR/EM-OCT/OH.02/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN09-AR/EM-COR/OH.02-CQLN.12/strength - unit: 1/m**2 -- type: pyaml.bpm.bpm - name: BPM_079 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN09-AR/DG-EPOS/BPM.07/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN09-AR/DG-EPOS/BPM.07/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SH4_COR_003 - mapping: - - [B2, SH4_COR_003.sextupole] - - [B0, SH4_COR_003.hcorrector] - - [A0, SH4_COR_003.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0, A0] - units: [1/m**2, '1', '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN09-AR/EM-SX/SHF.06/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN09-AR/EM-COR/SHF.06-CDLH.07/strength - unit: '1' - - type: tango.pyaml.attribute - attribute: AN09-AR/EM-COR/SHF.06-CDLV.07/strength - unit: '1' -- type: pyaml.magnet.cfm_magnet - name: OH4_QCORROCT_72_QT_001 - mapping: - - [B3, OH4_QCORROCT_72_QT_001.octupole] - - [B1, OH4_QCORROCT_72_QT_001.quadrupole] - - [A1, OH4_QCORROCT_72_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN09-AR/EM-OCT/OH.03/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN09-AR/EM-COR/OH.03-CQLN.13/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN09-AR/EM-COR/OH.03-CQLT.05/strength - unit: 1/m**2 -- type: pyaml.bpm.bpm - name: BPM_080 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN10-SD/DG-EPOS/BPM.01/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN10-SD/DG-EPOS/BPM.01/y_pos - unit: mm -- type: pyaml.bpm.bpm - name: BPM_081 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN10-SD/DG-EPOS/BPM.02/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN10-SD/DG-EPOS/BPM.02/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: OH4_QCORROCT_73_QT_001 - mapping: - - [B3, OH4_QCORROCT_73_QT_001.octupole] - - [B1, OH4_QCORROCT_73_QT_001.quadrupole] - - [A1, OH4_QCORROCT_73_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN10-AR/EM-OCT/OH.01/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN10-AR/EM-COR/OH.01-CQLN.01/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN10-AR/EM-COR/OH.01-CQLT.01/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SH4_COR_004 - mapping: - - [B2, SH4_COR_004.sextupole] - - [B0, SH4_COR_004.hcorrector] - - [A0, SH4_COR_004.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0, A0] - units: [1/m**2, '1', '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN10-AR/EM-SX/SHF.01/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN10-AR/EM-COR/SHF.01-CDLH.01/strength - unit: '1' - - type: tango.pyaml.attribute - attribute: AN10-AR/EM-COR/SHF.01-CDLV.01/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_082 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN10-AR/DG-EPOS/BPM.03/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN10-AR/DG-EPOS/BPM.03/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: OH5_QCORROCT_74_001 - mapping: - - [B3, OH5_QCORROCT_74_001.octupole] - - [B1, OH5_QCORROCT_74_001.quadrupole] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1] - units: [1/m**3, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN10-AR/EM-OCT/OH.02/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN10-AR/EM-COR/OH.02-CQLN.02/strength - unit: 1/m**2 -- type: pyaml.magnet.sextupole - name: SH5_004 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN10-AR/EM-SX/SHD.02/strength - unit: 1/m**2 -- type: pyaml.magnet.quadrupole - name: QCORR_093 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN10-AR/EM-COR/CQLN.03/strength - unit: 1/m -- type: pyaml.magnet.cfm_magnet - name: SH6_COR_004 - mapping: - - [B2, SH6_COR_004.sextupole] - - [B0, SH6_COR_004.hcorrector] - - [A0, SH6_COR_004.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0, A0] - units: [1/m**2, '1', '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN10-AR/EM-SX/SHD.03/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN10-AR/EM-COR/SHD.03-CDLH.02/strength - unit: '1' - - type: tango.pyaml.attribute - attribute: AN10-AR/EM-COR/SHD.03-CDLV.02/strength - unit: '1' -- type: pyaml.magnet.sextupole - name: SXD12_002 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN10-AR/EM-SX/SCD.01/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: OCTF1_QCORROCT_75_QT_001 - mapping: - - [B3, OCTF1_QCORROCT_75_QT_001.octupole] - - [B1, OCTF1_QCORROCT_75_QT_001.quadrupole] - - [A1, OCTF1_QCORROCT_75_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN10-AR/EM-OCT/OC.01/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN10-AR/EM-COR/OC.01-CQLN.04/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN10-AR/EM-COR/OC.01-CQLT.02/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF12_HCOR_002 - mapping: - - [B2, SXF12_HCOR_002.sextupole] - - [B0, SXF12_HCOR_002.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN10-AR/EM-SX/SCF.02/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN10-AR/EM-COR/SCF.02-CDLH.03/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_083 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN10-AR/DG-EPOS/BPM.04/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN10-AR/DG-EPOS/BPM.04/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SXD12_VCOR_002 - mapping: - - [B2, SXD12_VCOR_002.sextupole] - - [A0, SXD12_VCOR_002.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN10-AR/EM-SX/SCD.03/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN10-AR/EM-COR/SCD.03-CDLV.03/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_094 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN10-AR/EM-COR/CQLN.05/strength - unit: 1/m -- type: pyaml.magnet.quadrupole - name: QCORR_095 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN10-AR/EM-COR/CQLN.06/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SXD1_004 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN10-AR/EM-SX/SCD.04/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: OCTF1_QCORROCT_76_QT_001 - mapping: - - [B3, OCTF1_QCORROCT_76_QT_001.octupole] - - [B1, OCTF1_QCORROCT_76_QT_001.quadrupole] - - [A1, OCTF1_QCORROCT_76_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN10-AR/EM-OCT/OC.02/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN10-AR/EM-COR/OC.02-CQLN.07/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN10-AR/EM-COR/OC.02-CQLT.03/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF1_HCOR_003 - mapping: - - [B2, SXF1_HCOR_003.sextupole] - - [B0, SXF1_HCOR_003.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN10-AR/EM-SX/SCF.05/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN10-AR/EM-COR/SCF.05-CDLH.04/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_084 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN10-AR/DG-EPOS/BPM.05/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN10-AR/DG-EPOS/BPM.05/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SXD1_VCOR_004 - mapping: - - [B2, SXD1_VCOR_004.sextupole] - - [A0, SXD1_VCOR_004.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN10-AR/EM-SX/SCD.06/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN10-AR/EM-COR/SCD.06-CDLV.04/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_096 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN10-AR/EM-COR/CQLN.08/strength - unit: 1/m -- type: pyaml.magnet.quadrupole - name: QCORR_097 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN10-AR/EM-COR/CQLN.09/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SXD1_005 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN10-AR/EM-SX/SCD.07/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: OCTF1_QCORROCT_77_QT_001 - mapping: - - [B3, OCTF1_QCORROCT_77_QT_001.octupole] - - [B1, OCTF1_QCORROCT_77_QT_001.quadrupole] - - [A1, OCTF1_QCORROCT_77_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN10-AR/EM-OCT/OC.03/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN10-AR/EM-COR/OC.03-CQLN.10/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN10-AR/EM-COR/OC.03-CQLT.04/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF13_HCOR_003 - mapping: - - [B2, SXF13_HCOR_003.sextupole] - - [B0, SXF13_HCOR_003.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN10-AR/EM-SX/SCF.08/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN10-AR/EM-COR/SCF.08-CDLH.05/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_085 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN10-AR/DG-EPOS/BPM.06/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN10-AR/DG-EPOS/BPM.06/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SXD13_VCOR_002 - mapping: - - [B2, SXD13_VCOR_002.sextupole] - - [A0, SXD13_VCOR_002.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN10-AR/EM-SX/SCD.09/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN10-AR/EM-COR/SCD.09-CDLV.05/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_098 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN10-AR/EM-COR/CQLN.11/strength - unit: 1/m -- type: pyaml.magnet.quadrupole - name: QCORR_099 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN10-AR/EM-COR/CQLN.12/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SXD13_002 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN10-AR/EM-SX/SCD.10/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF13_HCOR_004 - mapping: - - [B2, SXF13_HCOR_004.sextupole] - - [B0, SXF13_HCOR_004.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN10-AR/EM-SX/SCF.11/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN10-AR/EM-COR/SCF.11-CDLH.06/strength - unit: '1' -- type: pyaml.magnet.cfm_magnet - name: OCTF1_QCORROCT_78_QT_001 - mapping: - - [B3, OCTF1_QCORROCT_78_QT_001.octupole] - - [B1, OCTF1_QCORROCT_78_QT_001.quadrupole] - - [A1, OCTF1_QCORROCT_78_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN10-AR/EM-OCT/OC.04/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN10-AR/EM-COR/OC.04-CQLN.13/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN10-AR/EM-COR/OC.04-CQLT.05/strength - unit: 1/m**2 -- type: pyaml.bpm.bpm - name: BPM_086 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN10-AR/DG-EPOS/BPM.07/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN10-AR/DG-EPOS/BPM.07/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SXD1_VCOR_005 - mapping: - - [B2, SXD1_VCOR_005.sextupole] - - [A0, SXD1_VCOR_005.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN10-AR/EM-SX/SCD.12/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN10-AR/EM-COR/SCD.12-CDLV.06/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_100 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN10-AR/EM-COR/CQLN.14/strength - unit: 1/m -- type: pyaml.magnet.quadrupole - name: QCORR_101 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN10-AR/EM-COR/CQLN.15/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SXD1_006 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN10-AR/EM-SX/SCD.13/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF1_HCOR_004 - mapping: - - [B2, SXF1_HCOR_004.sextupole] - - [B0, SXF1_HCOR_004.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN10-AR/EM-SX/SCF.14/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN10-AR/EM-COR/SCF.14-CDLH.07/strength - unit: '1' -- type: pyaml.magnet.cfm_magnet - name: OCTF1_QCORROCT_79_QT_001 - mapping: - - [B3, OCTF1_QCORROCT_79_QT_001.octupole] - - [B1, OCTF1_QCORROCT_79_QT_001.quadrupole] - - [A1, OCTF1_QCORROCT_79_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN10-AR/EM-OCT/OC.05/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN10-AR/EM-COR/OC.05-CQLN.16/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN10-AR/EM-COR/OC.05-CQLT.06/strength - unit: 1/m**2 -- type: pyaml.bpm.bpm - name: BPM_087 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN10-AR/DG-EPOS/BPM.08/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN10-AR/DG-EPOS/BPM.08/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SXD1_VCOR_006 - mapping: - - [B2, SXD1_VCOR_006.sextupole] - - [A0, SXD1_VCOR_006.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN10-AR/EM-SX/SCD.15/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN10-AR/EM-COR/SCD.15-CDLV.07/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_102 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN10-AR/EM-COR/CQLN.17/strength - unit: 1/m -- type: pyaml.magnet.quadrupole - name: QCORR_103 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN10-AR/EM-COR/CQLN.18/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SXD11_002 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN10-AR/EM-SX/SCD.16/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF11_HCOR_002 - mapping: - - [B2, SXF11_HCOR_002.sextupole] - - [B0, SXF11_HCOR_002.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN10-AR/EM-SX/SCF.17/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN10-AR/EM-COR/SCF.17-CDLH.08/strength - unit: '1' -- type: pyaml.magnet.cfm_magnet - name: OCTF1_QCORROCT_80_QT_001 - mapping: - - [B3, OCTF1_QCORROCT_80_QT_001.octupole] - - [B1, OCTF1_QCORROCT_80_QT_001.quadrupole] - - [A1, OCTF1_QCORROCT_80_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN10-AR/EM-OCT/OC.06/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN10-AR/EM-COR/OC.06-CQLN.19/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN10-AR/EM-COR/OC.06-CQLT.07/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXD11_VCOR_002 - mapping: - - [B2, SXD11_VCOR_002.sextupole] - - [A0, SXD11_VCOR_002.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN10-AR/EM-SX/SCD.18/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN10-AR/EM-COR/SCD.18-CDLV.08/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_088 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN10-AR/DG-EPOS/BPM.09/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN10-AR/DG-EPOS/BPM.09/y_pos - unit: mm -- type: pyaml.magnet.quadrupole - name: QCORR_104 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN10-AR/EM-COR/CQLN.20/strength - unit: 1/m -- type: pyaml.magnet.cfm_magnet - name: SH3_VCOR_002 - mapping: - - [B2, SH3_VCOR_002.sextupole] - - [A0, SH3_VCOR_002.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN10-AR/EM-SX/SHD.04/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN10-AR/EM-COR/SHD.04-CDLV.09/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_089 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN10-AR/DG-EPOS/BPM.10/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN10-AR/DG-EPOS/BPM.10/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: OH2_QCORROCT_81_001 - mapping: - - [B3, OH2_QCORROCT_81_001.octupole] - - [B1, OH2_QCORROCT_81_001.quadrupole] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1] - units: [1/m**3, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN10-AR/EM-OCT/OH.03/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN10-AR/EM-COR/OH.03-CQLN.21/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SH2_HCOR_002 - mapping: - - [B2, SH2_HCOR_002.sextupole] - - [B0, SH2_HCOR_002.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN10-AR/EM-SX/SHD.05/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN10-AR/EM-COR/SHD.05-CDLH.09/strength - unit: '1' -- type: pyaml.magnet.cfm_magnet - name: OH1_QCORROCT_82_QT_001 - mapping: - - [B3, OH1_QCORROCT_82_QT_001.octupole] - - [B1, OH1_QCORROCT_82_QT_001.quadrupole] - - [A1, OH1_QCORROCT_82_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN10-AR/EM-OCT/OH.04/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN10-AR/EM-COR/OH.04-CQLN.22/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN10-AR/EM-COR/OH.04-CQLT.08/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SH1_COR_002 - mapping: - - [B2, SH1_COR_002.sextupole] - - [B0, SH1_COR_002.hcorrector] - - [A0, SH1_COR_002.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0, A0] - units: [1/m**2, '1', '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN10-AR/EM-SX/SHF.06/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN10-AR/EM-COR/SHF.06-CDLH.10/strength - unit: '1' - - type: tango.pyaml.attribute - attribute: AN10-AR/EM-COR/SHF.06-CDLV.10/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_090 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN11-SD/DG-EPOS/BPM.01/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN11-SD/DG-EPOS/BPM.01/y_pos - unit: mm -- type: pyaml.bpm.bpm - name: BPM_091 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN11-SD/DG-EPOS/BPM.02/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN11-SD/DG-EPOS/BPM.02/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SH1_COR_003 - mapping: - - [B2, SH1_COR_003.sextupole] - - [B0, SH1_COR_003.hcorrector] - - [A0, SH1_COR_003.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0, A0] - units: [1/m**2, '1', '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN11-AR/EM-SX/SHF.01/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN11-AR/EM-COR/SHF.01-CDLH.01/strength - unit: '1' - - type: tango.pyaml.attribute - attribute: AN11-AR/EM-COR/SHF.01-CDLV.01/strength - unit: '1' -- type: pyaml.magnet.cfm_magnet - name: OH1_QCORROCT_83_QT_001 - mapping: - - [B3, OH1_QCORROCT_83_QT_001.octupole] - - [B1, OH1_QCORROCT_83_QT_001.quadrupole] - - [A1, OH1_QCORROCT_83_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN11-AR/EM-OCT/OH.01/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN11-AR/EM-COR/OH.01-CQLN.01/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN11-AR/EM-COR/OH.01-CQLT.01/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SH2_HCOR_003 - mapping: - - [B2, SH2_HCOR_003.sextupole] - - [B0, SH2_HCOR_003.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN11-AR/EM-SX/SHD.02/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN11-AR/EM-COR/SHD.02-CDLH.02/strength - unit: '1' -- type: pyaml.magnet.cfm_magnet - name: OH2_QCORROCT_84_001 - mapping: - - [B3, OH2_QCORROCT_84_001.octupole] - - [B1, OH2_QCORROCT_84_001.quadrupole] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1] - units: [1/m**3, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN11-AR/EM-OCT/OH.02/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN11-AR/EM-COR/OH.02-CQLN.02/strength - unit: 1/m**2 -- type: pyaml.bpm.bpm - name: BPM_092 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN11-AR/DG-EPOS/BPM.03/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN11-AR/DG-EPOS/BPM.03/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SH3_VCOR_003 - mapping: - - [B2, SH3_VCOR_003.sextupole] - - [A0, SH3_VCOR_003.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN11-AR/EM-SX/SHD.03/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN11-AR/EM-COR/SHD.03-CDLV.02/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_105 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN11-AR/EM-COR/CQLN.03/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SXD11_003 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN11-AR/EM-SX/SCD.01/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: OCTF1_QCORROCT_85_QT_001 - mapping: - - [B3, OCTF1_QCORROCT_85_QT_001.octupole] - - [B1, OCTF1_QCORROCT_85_QT_001.quadrupole] - - [A1, OCTF1_QCORROCT_85_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN11-AR/EM-OCT/OC.01/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN11-AR/EM-COR/OC.01-CQLN.04/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN11-AR/EM-COR/OC.01-CQLT.02/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF11_HCOR_003 - mapping: - - [B2, SXF11_HCOR_003.sextupole] - - [B0, SXF11_HCOR_003.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN11-AR/EM-SX/SCF.02/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN11-AR/EM-COR/SCF.02-CDLH.03/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_093 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN11-AR/DG-EPOS/BPM.04/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN11-AR/DG-EPOS/BPM.04/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SXD11_VCOR_003 - mapping: - - [B2, SXD11_VCOR_003.sextupole] - - [A0, SXD11_VCOR_003.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN11-AR/EM-SX/SCD.03/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN11-AR/EM-COR/SCD.03-CDLV.03/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_106 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN11-AR/EM-COR/CQLN.05/strength - unit: 1/m -- type: pyaml.magnet.quadrupole - name: QCORR_107 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN11-AR/EM-COR/CQLN.06/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SXD1_007 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN11-AR/EM-SX/SCD.04/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: OCTF1_QCORROCT_86_QT_001 - mapping: - - [B3, OCTF1_QCORROCT_86_QT_001.octupole] - - [B1, OCTF1_QCORROCT_86_QT_001.quadrupole] - - [A1, OCTF1_QCORROCT_86_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN11-AR/EM-OCT/OC.02/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN11-AR/EM-COR/OC.02-CQLN.07/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN11-AR/EM-COR/OC.02-CQLT.03/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF1_HCOR_005 - mapping: - - [B2, SXF1_HCOR_005.sextupole] - - [B0, SXF1_HCOR_005.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN11-AR/EM-SX/SCF.05/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN11-AR/EM-COR/SCF.05-CDLH.04/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_094 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN11-AR/DG-EPOS/BPM.05/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN11-AR/DG-EPOS/BPM.05/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SXD1_VCOR_007 - mapping: - - [B2, SXD1_VCOR_007.sextupole] - - [A0, SXD1_VCOR_007.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN11-AR/EM-SX/SCD.06/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN11-AR/EM-COR/SCD.06-CDLV.04/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_108 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN11-AR/EM-COR/CQLN.08/strength - unit: 1/m -- type: pyaml.magnet.quadrupole - name: QCORR_109 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN11-AR/EM-COR/CQLN.09/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SXD1_008 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN11-AR/EM-SX/SCD.07/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: OCTF1_QCORROCT_87_QT_001 - mapping: - - [B3, OCTF1_QCORROCT_87_QT_001.octupole] - - [B1, OCTF1_QCORROCT_87_QT_001.quadrupole] - - [A1, OCTF1_QCORROCT_87_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN11-AR/EM-OCT/OC.03/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN11-AR/EM-COR/OC.03-CQLN.10/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN11-AR/EM-COR/OC.03-CQLT.04/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF13_HCOR_005 - mapping: - - [B2, SXF13_HCOR_005.sextupole] - - [B0, SXF13_HCOR_005.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN11-AR/EM-SX/SCF.08/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN11-AR/EM-COR/SCF.08-CDLH.05/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_095 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN11-AR/DG-EPOS/BPM.06/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN11-AR/DG-EPOS/BPM.06/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SXD13_VCOR_003 - mapping: - - [B2, SXD13_VCOR_003.sextupole] - - [A0, SXD13_VCOR_003.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN11-AR/EM-SX/SCD.09/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN11-AR/EM-COR/SCD.09-CDLV.05/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_110 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN11-AR/EM-COR/CQLN.11/strength - unit: 1/m -- type: pyaml.magnet.quadrupole - name: QCORR_111 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN11-AR/EM-COR/CQLN.12/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SXD13_003 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN11-AR/EM-SX/SCD.10/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF13_HCOR_006 - mapping: - - [B2, SXF13_HCOR_006.sextupole] - - [B0, SXF13_HCOR_006.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN11-AR/EM-SX/SCF.11/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN11-AR/EM-COR/SCF.11-CDLH.06/strength - unit: '1' -- type: pyaml.magnet.cfm_magnet - name: OCTF1_QCORROCT_88_QT_001 - mapping: - - [B3, OCTF1_QCORROCT_88_QT_001.octupole] - - [B1, OCTF1_QCORROCT_88_QT_001.quadrupole] - - [A1, OCTF1_QCORROCT_88_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN11-AR/EM-OCT/OC.04/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN11-AR/EM-COR/OC.04-CQLN.13/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN11-AR/EM-COR/OC.04-CQLT.05/strength - unit: 1/m**2 -- type: pyaml.bpm.bpm - name: BPM_096 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN11-AR/DG-EPOS/BPM.07/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN11-AR/DG-EPOS/BPM.07/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SXD1_VCOR_008 - mapping: - - [B2, SXD1_VCOR_008.sextupole] - - [A0, SXD1_VCOR_008.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN11-AR/EM-SX/SCD.12/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN11-AR/EM-COR/SCD.12-CDLV.06/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_112 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN11-AR/EM-COR/CQLN.14/strength - unit: 1/m -- type: pyaml.magnet.quadrupole - name: QCORR_113 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN11-AR/EM-COR/CQLN.15/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SXD1_009 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN11-AR/EM-SX/SCD.13/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF1_HCOR_006 - mapping: - - [B2, SXF1_HCOR_006.sextupole] - - [B0, SXF1_HCOR_006.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN11-AR/EM-SX/SCF.14/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN11-AR/EM-COR/SCF.14-CDLH.07/strength - unit: '1' -- type: pyaml.magnet.cfm_magnet - name: OCTF1_QCORROCT_89_QT_001 - mapping: - - [B3, OCTF1_QCORROCT_89_QT_001.octupole] - - [B1, OCTF1_QCORROCT_89_QT_001.quadrupole] - - [A1, OCTF1_QCORROCT_89_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN11-AR/EM-OCT/OC.05/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN11-AR/EM-COR/OC.05-CQLN.16/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN11-AR/EM-COR/OC.05-CQLT.06/strength - unit: 1/m**2 -- type: pyaml.bpm.bpm - name: BPM_097 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN11-AR/DG-EPOS/BPM.08/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN11-AR/DG-EPOS/BPM.08/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SXD1_VCOR_009 - mapping: - - [B2, SXD1_VCOR_009.sextupole] - - [A0, SXD1_VCOR_009.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN11-AR/EM-SX/SCD.15/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN11-AR/EM-COR/SCD.15-CDLV.07/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_114 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN11-AR/EM-COR/CQLN.17/strength - unit: 1/m -- type: pyaml.magnet.quadrupole - name: QCORR_115 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN11-AR/EM-COR/CQLN.18/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SXD12_003 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN11-AR/EM-SX/SCD.16/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF12_HCOR_003 - mapping: - - [B2, SXF12_HCOR_003.sextupole] - - [B0, SXF12_HCOR_003.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN11-AR/EM-SX/SCF.17/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN11-AR/EM-COR/SCF.17-CDLH.08/strength - unit: '1' -- type: pyaml.magnet.cfm_magnet - name: OCTF1_QCORROCT_90_QT_001 - mapping: - - [B3, OCTF1_QCORROCT_90_QT_001.octupole] - - [B1, OCTF1_QCORROCT_90_QT_001.quadrupole] - - [A1, OCTF1_QCORROCT_90_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN11-AR/EM-OCT/OC.06/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN11-AR/EM-COR/OC.06-CQLN.19/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN11-AR/EM-COR/OC.06-CQLT.07/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXD12_VCOR_003 - mapping: - - [B2, SXD12_VCOR_003.sextupole] - - [A0, SXD12_VCOR_003.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN11-AR/EM-SX/SCD.18/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN11-AR/EM-COR/SCD.18-CDLV.08/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_098 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN11-AR/DG-EPOS/BPM.09/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN11-AR/DG-EPOS/BPM.09/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SH6_COR_005 - mapping: - - [B2, SH6_COR_005.sextupole] - - [B0, SH6_COR_005.hcorrector] - - [A0, SH6_COR_005.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0, A0] - units: [1/m**2, '1', '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN11-AR/EM-SX/SHD.04/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN11-AR/EM-COR/SHD.04-CDLH.09/strength - unit: '1' - - type: tango.pyaml.attribute - attribute: AN11-AR/EM-COR/SHD.04-CDLV.09/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_116 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN11-AR/EM-COR/CQLN.20/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SH5_005 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN11-AR/EM-SX/SHD.05/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: OH5_QCORROCT_91_001 - mapping: - - [B3, OH5_QCORROCT_91_001.octupole] - - [B1, OH5_QCORROCT_91_001.quadrupole] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1] - units: [1/m**3, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN11-AR/EM-OCT/OH.03/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN11-AR/EM-COR/OH.03-CQLN.21/strength - unit: 1/m**2 -- type: pyaml.bpm.bpm - name: BPM_099 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN11-AR/DG-EPOS/BPM.10/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN11-AR/DG-EPOS/BPM.10/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SH4_COR_005 - mapping: - - [B2, SH4_COR_005.sextupole] - - [B0, SH4_COR_005.hcorrector] - - [A0, SH4_COR_005.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0, A0] - units: [1/m**2, '1', '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN11-AR/EM-SX/SHF.06/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN11-AR/EM-COR/SHF.06-CDLH.10/strength - unit: '1' - - type: tango.pyaml.attribute - attribute: AN11-AR/EM-COR/SHF.06-CDLV.10/strength - unit: '1' -- type: pyaml.magnet.cfm_magnet - name: OH4_QCORROCT_92_QT_001 - mapping: - - [B3, OH4_QCORROCT_92_QT_001.octupole] - - [B1, OH4_QCORROCT_92_QT_001.quadrupole] - - [A1, OH4_QCORROCT_92_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN11-AR/EM-OCT/OH.04/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN11-AR/EM-COR/OH.04-CQLN.22/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN11-AR/EM-COR/OH.04-CQLT.08/strength - unit: 1/m**2 -- type: pyaml.bpm.bpm - name: BPM_100 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN12-SD/DG-EPOS/BPM.01/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN12-SD/DG-EPOS/BPM.01/y_pos - unit: mm -- type: pyaml.bpm.bpm - name: BPM_101 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN12-SD/DG-EPOS/BPM.02/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN12-SD/DG-EPOS/BPM.02/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: OH4_QCORROCT_93_QT_001 - mapping: - - [B3, OH4_QCORROCT_93_QT_001.octupole] - - [B1, OH4_QCORROCT_93_QT_001.quadrupole] - - [A1, OH4_QCORROCT_93_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN12-AR/EM-OCT/OH.01/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN12-AR/EM-COR/OH.01-CQLN.01/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN12-AR/EM-COR/OH.01-CQLT.01/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SH4_COR_006 - mapping: - - [B2, SH4_COR_006.sextupole] - - [B0, SH4_COR_006.hcorrector] - - [A0, SH4_COR_006.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0, A0] - units: [1/m**2, '1', '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN12-AR/EM-SX/SHF.01/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN12-AR/EM-COR/SHF.01-CDLH.01/strength - unit: '1' - - type: tango.pyaml.attribute - attribute: AN12-AR/EM-COR/SHF.01-CDLV.01/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_102 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN12-AR/DG-EPOS/BPM.03/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN12-AR/DG-EPOS/BPM.03/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: OH5_QCORROCT_94_001 - mapping: - - [B3, OH5_QCORROCT_94_001.octupole] - - [B1, OH5_QCORROCT_94_001.quadrupole] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1] - units: [1/m**3, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN12-AR/EM-OCT/OH.02/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN12-AR/EM-COR/OH.02-CQLN.02/strength - unit: 1/m**2 -- type: pyaml.magnet.sextupole - name: SH5_006 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN12-AR/EM-SX/SHD.02/strength - unit: 1/m**2 -- type: pyaml.magnet.quadrupole - name: QCORR_117 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN12-AR/EM-COR/CQLN.03/strength - unit: 1/m -- type: pyaml.magnet.cfm_magnet - name: SH6_COR_006 - mapping: - - [B2, SH6_COR_006.sextupole] - - [B0, SH6_COR_006.hcorrector] - - [A0, SH6_COR_006.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0, A0] - units: [1/m**2, '1', '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN12-AR/EM-SX/SHD.03/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN12-AR/EM-COR/SHD.03-CDLH.02/strength - unit: '1' - - type: tango.pyaml.attribute - attribute: AN12-AR/EM-COR/SHD.03-CDLV.02/strength - unit: '1' -- type: pyaml.magnet.sextupole - name: SXD21_003 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN12-AR/EM-SX/SCD.01/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: OCTF2_QCORROCT_95_QT_001 - mapping: - - [B3, OCTF2_QCORROCT_95_QT_001.octupole] - - [B1, OCTF2_QCORROCT_95_QT_001.quadrupole] - - [A1, OCTF2_QCORROCT_95_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN12-AR/EM-OCT/OC.01/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN12-AR/EM-COR/OC.01-CQLN.04/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN12-AR/EM-COR/OC.01-CQLT.02/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF21_HCOR_003 - mapping: - - [B2, SXF21_HCOR_003.sextupole] - - [B0, SXF21_HCOR_003.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN12-AR/EM-SX/SCF.02/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN12-AR/EM-COR/SCF.02-CDLH.03/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_103 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN12-AR/DG-EPOS/BPM.04/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN12-AR/DG-EPOS/BPM.04/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SXD21_VCOR_003 - mapping: - - [B2, SXD21_VCOR_003.sextupole] - - [A0, SXD21_VCOR_003.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN12-AR/EM-SX/SCD.03/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN12-AR/EM-COR/SCD.03-CDLV.03/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_118 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN12-AR/EM-COR/CQLN.05/strength - unit: 1/m -- type: pyaml.magnet.quadrupole - name: QCORR_119 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN12-AR/EM-COR/CQLN.06/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SXD2_003 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN12-AR/EM-SX/SCD.04/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: OCTF2_QCORROCT_96_QT_001 - mapping: - - [B3, OCTF2_QCORROCT_96_QT_001.octupole] - - [B1, OCTF2_QCORROCT_96_QT_001.quadrupole] - - [A1, OCTF2_QCORROCT_96_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN12-AR/EM-OCT/OC.02/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN12-AR/EM-COR/OC.02-CQLN.07/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN12-AR/EM-COR/OC.02-CQLT.03/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF2_HCOR_003 - mapping: - - [B2, SXF2_HCOR_003.sextupole] - - [B0, SXF2_HCOR_003.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN12-AR/EM-SX/SCF.05/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN12-AR/EM-COR/SCF.05-CDLH.04/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_104 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN12-AR/DG-EPOS/BPM.05/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN12-AR/DG-EPOS/BPM.05/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SXD2_VCOR_003 - mapping: - - [B2, SXD2_VCOR_003.sextupole] - - [A0, SXD2_VCOR_003.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN12-AR/EM-SX/SCD.06/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN12-AR/EM-COR/SCD.06-CDLV.04/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_120 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN12-AR/EM-COR/CQLN.08/strength - unit: 1/m -- type: pyaml.magnet.quadrupole - name: QCORR_121 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN12-AR/EM-COR/CQLN.09/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SXD22_003 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN12-AR/EM-SX/SCD.07/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF22_HCOR_003 - mapping: - - [B2, SXF22_HCOR_003.sextupole] - - [B0, SXF22_HCOR_003.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN12-AR/EM-SX/SCF.08/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN12-AR/EM-COR/SCF.08-CDLH.05/strength - unit: '1' -- type: pyaml.magnet.cfm_magnet - name: OCTF2_QCORROCT_97_QT_001 - mapping: - - [B3, OCTF2_QCORROCT_97_QT_001.octupole] - - [B1, OCTF2_QCORROCT_97_QT_001.quadrupole] - - [A1, OCTF2_QCORROCT_97_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN12-AR/EM-OCT/OC.03/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN12-AR/EM-COR/OC.03-CQLN.10/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN12-AR/EM-COR/OC.03-CQLT.04/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXD22_VCOR_003 - mapping: - - [B2, SXD22_VCOR_003.sextupole] - - [A0, SXD22_VCOR_003.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN12-AR/EM-SX/SCD.09/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN12-AR/EM-COR/SCD.09-CDLV.05/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_105 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN12-AR/DG-EPOS/BPM.06/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN12-AR/DG-EPOS/BPM.06/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SH9_COR_009 - mapping: - - [B2, SH9_COR_009.sextupole] - - [B0, SH9_COR_009.hcorrector] - - [A0, SH9_COR_009.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0, A0] - units: [1/m**2, '1', '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN12-AR/EM-SX/SHD.04/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN12-AR/EM-COR/SHD.04-CDLH.06/strength - unit: '1' - - type: tango.pyaml.attribute - attribute: AN12-AR/EM-COR/SHD.04-CDLV.06/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_122 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN12-AR/EM-COR/CQLN.11/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SH8_009 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN12-AR/EM-SX/SHD.05/strength - unit: 1/m**2 -- type: pyaml.magnet.quadrupole - name: QCORR_123 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN12-AR/EM-COR/CQLN.12/strength - unit: 1/m -- type: pyaml.bpm.bpm - name: BPM_106 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN12-AR/DG-EPOS/BPM.07/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN12-AR/DG-EPOS/BPM.07/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SH7_COR_009 - mapping: - - [B2, SH7_COR_009.sextupole] - - [B0, SH7_COR_009.hcorrector] - - [A0, SH7_COR_009.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0, A0] - units: [1/m**2, '1', '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN12-AR/EM-SX/SHF.06/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN12-AR/EM-COR/SHF.06-CDLH.07/strength - unit: '1' - - type: tango.pyaml.attribute - attribute: AN12-AR/EM-COR/SHF.06-CDLV.07/strength - unit: '1' -- type: pyaml.magnet.cfm_magnet - name: OH7_QCORROCT_98_QT_001 - mapping: - - [B3, OH7_QCORROCT_98_QT_001.octupole] - - [B1, OH7_QCORROCT_98_QT_001.quadrupole] - - [A1, OH7_QCORROCT_98_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN12-AR/EM-OCT/OH.03/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN12-AR/EM-COR/OH.03-CQLN.13/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN12-AR/EM-COR/OH.03-CQLT.05/strength - unit: 1/m**2 -- type: pyaml.bpm.bpm - name: BPM_107 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN13-SD/DG-EPOS/BPM.01/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN13-SD/DG-EPOS/BPM.01/y_pos - unit: mm -- type: pyaml.bpm.bpm - name: BPM_108 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN13-SD/DG-EPOS/BPM.02/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN13-SD/DG-EPOS/BPM.02/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: OH7_QCORROCT_99_QT_001 - mapping: - - [B3, OH7_QCORROCT_99_QT_001.octupole] - - [B1, OH7_QCORROCT_99_QT_001.quadrupole] - - [A1, OH7_QCORROCT_99_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN13-AR/EM-OCT/OH.01/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN13-AR/EM-COR/OH.01-CQLN.01/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN13-AR/EM-COR/OH.01-CQLT.01/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SH7_COR_010 - mapping: - - [B2, SH7_COR_010.sextupole] - - [B0, SH7_COR_010.hcorrector] - - [A0, SH7_COR_010.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0, A0] - units: [1/m**2, '1', '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN13-AR/EM-SX/SHF.01/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN13-AR/EM-COR/SHF.01-CDLH.01/strength - unit: '1' - - type: tango.pyaml.attribute - attribute: AN13-AR/EM-COR/SHF.01-CDLV.01/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_109 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN13-AR/DG-EPOS/BPM.03/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN13-AR/DG-EPOS/BPM.03/y_pos - unit: mm -- type: pyaml.magnet.quadrupole - name: QCORR_124 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN13-AR/EM-COR/CQLN.02/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SH8_010 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN13-AR/EM-SX/SHD.02/strength - unit: 1/m**2 -- type: pyaml.magnet.quadrupole - name: QCORR_125 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN13-AR/EM-COR/CQLN.03/strength - unit: 1/m -- type: pyaml.magnet.cfm_magnet - name: SH9_COR_010 - mapping: - - [B2, SH9_COR_010.sextupole] - - [B0, SH9_COR_010.hcorrector] - - [A0, SH9_COR_010.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0, A0] - units: [1/m**2, '1', '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN13-AR/EM-SX/SHD.03/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN13-AR/EM-COR/SHD.03-CDLH.02/strength - unit: '1' - - type: tango.pyaml.attribute - attribute: AN13-AR/EM-COR/SHD.03-CDLV.02/strength - unit: '1' -- type: pyaml.magnet.sextupole - name: SXD31_003 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN13-AR/EM-SX/SCD.01/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: OCTF3_QCORROCT_100_QT_001 - mapping: - - [B3, OCTF3_QCORROCT_100_QT_001.octupole] - - [B1, OCTF3_QCORROCT_100_QT_001.quadrupole] - - [A1, OCTF3_QCORROCT_100_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN13-AR/EM-OCT/OC.01/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN13-AR/EM-COR/OC.01-CQLN.04/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN13-AR/EM-COR/OC.01-CQLT.02/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF31_HCOR_003 - mapping: - - [B2, SXF31_HCOR_003.sextupole] - - [B0, SXF31_HCOR_003.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN13-AR/EM-SX/SCF.02/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN13-AR/EM-COR/SCF.02-CDLH.03/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_110 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN13-AR/DG-EPOS/BPM.04/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN13-AR/DG-EPOS/BPM.04/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SXD31_VCOR_003 - mapping: - - [B2, SXD31_VCOR_003.sextupole] - - [A0, SXD31_VCOR_003.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN13-AR/EM-SX/SCD.03/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN13-AR/EM-COR/SCD.03-CDLV.03/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_126 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN13-AR/EM-COR/CQLN.05/strength - unit: 1/m -- type: pyaml.magnet.quadrupole - name: QCORR_127 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN13-AR/EM-COR/CQLN.06/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SXD3_007 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN13-AR/EM-SX/SCD.04/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: OCTF3_QCORROCT_101_QT_001 - mapping: - - [B3, OCTF3_QCORROCT_101_QT_001.octupole] - - [B1, OCTF3_QCORROCT_101_QT_001.quadrupole] - - [A1, OCTF3_QCORROCT_101_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN13-AR/EM-OCT/OC.02/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN13-AR/EM-COR/OC.02-CQLN.07/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN13-AR/EM-COR/OC.02-CQLT.03/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF3_HCOR_005 - mapping: - - [B2, SXF3_HCOR_005.sextupole] - - [B0, SXF3_HCOR_005.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN13-AR/EM-SX/SCF.05/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN13-AR/EM-COR/SCF.05-CDLH.04/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_111 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN13-AR/DG-EPOS/BPM.05/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN13-AR/DG-EPOS/BPM.05/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SXD3_VCOR_007 - mapping: - - [B2, SXD3_VCOR_007.sextupole] - - [A0, SXD3_VCOR_007.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN13-AR/EM-SX/SCD.06/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN13-AR/EM-COR/SCD.06-CDLV.04/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_128 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN13-AR/EM-COR/CQLN.08/strength - unit: 1/m -- type: pyaml.magnet.quadrupole - name: QCORR_129 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN13-AR/EM-COR/CQLN.09/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SXD3_008 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN13-AR/EM-SX/SCD.07/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: OCTF3_QCORROCT_102_QT_001 - mapping: - - [B3, OCTF3_QCORROCT_102_QT_001.octupole] - - [B1, OCTF3_QCORROCT_102_QT_001.quadrupole] - - [A1, OCTF3_QCORROCT_102_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN13-AR/EM-OCT/OC.03/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN13-AR/EM-COR/OC.03-CQLN.10/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN13-AR/EM-COR/OC.03-CQLT.04/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF33_HCOR_005 - mapping: - - [B2, SXF33_HCOR_005.sextupole] - - [B0, SXF33_HCOR_005.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN13-AR/EM-SX/SCF.08/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN13-AR/EM-COR/SCF.08-CDLH.05/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_112 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN13-AR/DG-EPOS/BPM.06/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN13-AR/DG-EPOS/BPM.06/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SXD33_VCOR_003 - mapping: - - [B2, SXD33_VCOR_003.sextupole] - - [A0, SXD33_VCOR_003.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN13-AR/EM-SX/SCD.09/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN13-AR/EM-COR/SCD.09-CDLV.05/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_130 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN13-AR/EM-COR/CQLN.11/strength - unit: 1/m -- type: pyaml.magnet.quadrupole - name: QCORR_131 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN13-AR/EM-COR/CQLN.12/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SXD33_003 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN13-AR/EM-SX/SCD.10/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF33_HCOR_006 - mapping: - - [B2, SXF33_HCOR_006.sextupole] - - [B0, SXF33_HCOR_006.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN13-AR/EM-SX/SCF.11/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN13-AR/EM-COR/SCF.11-CDLH.06/strength - unit: '1' -- type: pyaml.magnet.cfm_magnet - name: OCTF3_QCORROCT_103_QT_001 - mapping: - - [B3, OCTF3_QCORROCT_103_QT_001.octupole] - - [B1, OCTF3_QCORROCT_103_QT_001.quadrupole] - - [A1, OCTF3_QCORROCT_103_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN13-AR/EM-OCT/OC.04/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN13-AR/EM-COR/OC.04-CQLN.13/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN13-AR/EM-COR/OC.04-CQLT.05/strength - unit: 1/m**2 -- type: pyaml.bpm.bpm - name: BPM_113 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN13-AR/DG-EPOS/BPM.07/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN13-AR/DG-EPOS/BPM.07/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SXD3_VCOR_008 - mapping: - - [B2, SXD3_VCOR_008.sextupole] - - [A0, SXD3_VCOR_008.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN13-AR/EM-SX/SCD.12/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN13-AR/EM-COR/SCD.12-CDLV.06/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_132 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN13-AR/EM-COR/CQLN.14/strength - unit: 1/m -- type: pyaml.magnet.quadrupole - name: QCORR_133 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN13-AR/EM-COR/CQLN.15/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SXD3_009 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN13-AR/EM-SX/SCD.13/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF3_HCOR_006 - mapping: - - [B2, SXF3_HCOR_006.sextupole] - - [B0, SXF3_HCOR_006.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN13-AR/EM-SX/SCF.14/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN13-AR/EM-COR/SCF.14-CDLH.07/strength - unit: '1' -- type: pyaml.magnet.cfm_magnet - name: OCTF3_QCORROCT_104_QT_001 - mapping: - - [B3, OCTF3_QCORROCT_104_QT_001.octupole] - - [B1, OCTF3_QCORROCT_104_QT_001.quadrupole] - - [A1, OCTF3_QCORROCT_104_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN13-AR/EM-OCT/OC.05/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN13-AR/EM-COR/OC.05-CQLN.16/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN13-AR/EM-COR/OC.05-CQLT.06/strength - unit: 1/m**2 -- type: pyaml.bpm.bpm - name: BPM_114 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN13-AR/DG-EPOS/BPM.08/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN13-AR/DG-EPOS/BPM.08/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SXD3_VCOR_009 - mapping: - - [B2, SXD3_VCOR_009.sextupole] - - [A0, SXD3_VCOR_009.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN13-AR/EM-SX/SCD.15/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN13-AR/EM-COR/SCD.15-CDLV.07/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_134 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN13-AR/EM-COR/CQLN.17/strength - unit: 1/m -- type: pyaml.magnet.quadrupole - name: QCORR_135 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN13-AR/EM-COR/CQLN.18/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SXD32_003 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN13-AR/EM-SX/SCD.16/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF32_HCOR_003 - mapping: - - [B2, SXF32_HCOR_003.sextupole] - - [B0, SXF32_HCOR_003.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN13-AR/EM-SX/SCF.17/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN13-AR/EM-COR/SCF.17-CDLH.08/strength - unit: '1' -- type: pyaml.magnet.cfm_magnet - name: OCTF3_QCORROCT_105_QT_001 - mapping: - - [B3, OCTF3_QCORROCT_105_QT_001.octupole] - - [B1, OCTF3_QCORROCT_105_QT_001.quadrupole] - - [A1, OCTF3_QCORROCT_105_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN13-AR/EM-OCT/OC.06/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN13-AR/EM-COR/OC.06-CQLN.19/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN13-AR/EM-COR/OC.06-CQLT.07/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXD32_VCOR_003 - mapping: - - [B2, SXD32_VCOR_003.sextupole] - - [A0, SXD32_VCOR_003.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN13-AR/EM-SX/SCD.18/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN13-AR/EM-COR/SCD.18-CDLV.08/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_115 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN13-AR/DG-EPOS/BPM.09/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN13-AR/DG-EPOS/BPM.09/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SH9_COR_011 - mapping: - - [B2, SH9_COR_011.sextupole] - - [B0, SH9_COR_011.hcorrector] - - [A0, SH9_COR_011.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0, A0] - units: [1/m**2, '1', '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN13-AR/EM-SX/SHD.04/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN13-AR/EM-COR/SHD.04-CDLH.09/strength - unit: '1' - - type: tango.pyaml.attribute - attribute: AN13-AR/EM-COR/SHD.04-CDLV.09/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_136 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN13-AR/EM-COR/CQLN.20/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SH8_011 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN13-AR/EM-SX/SHD.05/strength - unit: 1/m**2 -- type: pyaml.magnet.quadrupole - name: QCORR_137 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN13-AR/EM-COR/CQLN.21/strength - unit: 1/m -- type: pyaml.bpm.bpm - name: BPM_116 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN13-AR/DG-EPOS/BPM.10/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN13-AR/DG-EPOS/BPM.10/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SH7_COR_011 - mapping: - - [B2, SH7_COR_011.sextupole] - - [B0, SH7_COR_011.hcorrector] - - [A0, SH7_COR_011.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0, A0] - units: [1/m**2, '1', '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN13-AR/EM-SX/SHF.06/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN13-AR/EM-COR/SHF.06-CDLH.10/strength - unit: '1' - - type: tango.pyaml.attribute - attribute: AN13-AR/EM-COR/SHF.06-CDLV.10/strength - unit: '1' -- type: pyaml.magnet.cfm_magnet - name: OH7_QCORROCT_106_QT_001 - mapping: - - [B3, OH7_QCORROCT_106_QT_001.octupole] - - [B1, OH7_QCORROCT_106_QT_001.quadrupole] - - [A1, OH7_QCORROCT_106_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN13-AR/EM-OCT/OH.02/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN13-AR/EM-COR/OH.02-CQLN.22/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN13-AR/EM-COR/OH.02-CQLT.08/strength - unit: 1/m**2 -- type: pyaml.bpm.bpm - name: BPM_117 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN14-SD/DG-EPOS/BPM.01/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN14-SD/DG-EPOS/BPM.01/y_pos - unit: mm -- type: pyaml.bpm.bpm - name: BPM_118 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN14-SD/DG-EPOS/BPM.02/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN14-SD/DG-EPOS/BPM.02/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: OH7_QCORROCT_107_QT_001 - mapping: - - [B3, OH7_QCORROCT_107_QT_001.octupole] - - [B1, OH7_QCORROCT_107_QT_001.quadrupole] - - [A1, OH7_QCORROCT_107_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN14-AR/EM-OCT/OH.01/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN14-AR/EM-COR/OH.01-CQLN.01/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN14-AR/EM-COR/OH.01-CQLT.01/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SH7_COR_012 - mapping: - - [B2, SH7_COR_012.sextupole] - - [B0, SH7_COR_012.hcorrector] - - [A0, SH7_COR_012.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0, A0] - units: [1/m**2, '1', '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN14-AR/EM-SX/SHF.01/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN14-AR/EM-COR/SHF.01-CDLH.01/strength - unit: '1' - - type: tango.pyaml.attribute - attribute: AN14-AR/EM-COR/SHF.01-CDLV.01/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_119 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN14-AR/DG-EPOS/BPM.03/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN14-AR/DG-EPOS/BPM.03/y_pos - unit: mm -- type: pyaml.magnet.quadrupole - name: QCORR_138 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN14-AR/EM-COR/CQLN.02/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SH8_012 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN14-AR/EM-SX/SHD.02/strength - unit: 1/m**2 -- type: pyaml.magnet.quadrupole - name: QCORR_139 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN14-AR/EM-COR/CQLN.03/strength - unit: 1/m -- type: pyaml.magnet.cfm_magnet - name: SH9_COR_012 - mapping: - - [B2, SH9_COR_012.sextupole] - - [B0, SH9_COR_012.hcorrector] - - [A0, SH9_COR_012.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0, A0] - units: [1/m**2, '1', '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN14-AR/EM-SX/SHD.03/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN14-AR/EM-COR/SHD.03-CDLH.02/strength - unit: '1' - - type: tango.pyaml.attribute - attribute: AN14-AR/EM-COR/SHD.03-CDLV.02/strength - unit: '1' -- type: pyaml.magnet.sextupole - name: SXD41_003 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN14-AR/EM-SX/SCD.01/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: OCTF4_QCORROCT_108_QT_001 - mapping: - - [B3, OCTF4_QCORROCT_108_QT_001.octupole] - - [B1, OCTF4_QCORROCT_108_QT_001.quadrupole] - - [A1, OCTF4_QCORROCT_108_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN14-AR/EM-OCT/OC.01/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN14-AR/EM-COR/OC.01-CQLN.04/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN14-AR/EM-COR/OC.01-CQLT.02/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF41_HCOR_003 - mapping: - - [B2, SXF41_HCOR_003.sextupole] - - [B0, SXF41_HCOR_003.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN14-AR/EM-SX/SCF.02/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN14-AR/EM-COR/SCF.02-CDLH.03/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_120 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN14-AR/DG-EPOS/BPM.04/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN14-AR/DG-EPOS/BPM.04/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SXD41_VCOR_003 - mapping: - - [B2, SXD41_VCOR_003.sextupole] - - [A0, SXD41_VCOR_003.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN14-AR/EM-SX/SCD.03/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN14-AR/EM-COR/SCD.03-CDLV.03/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_140 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN14-AR/EM-COR/CQLN.05/strength - unit: 1/m -- type: pyaml.magnet.quadrupole - name: QCORR_141 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN14-AR/EM-COR/CQLN.06/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SXD4_003 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN14-AR/EM-SX/SCD.04/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF4_HCOR_003 - mapping: - - [B2, SXF4_HCOR_003.sextupole] - - [B0, SXF4_HCOR_003.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN14-AR/EM-SX/SCF.05/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN14-AR/EM-COR/SCF.05-CDLH.04/strength - unit: '1' -- type: pyaml.magnet.cfm_magnet - name: OCTF4_QCORROCT_109_QT_001 - mapping: - - [B3, OCTF4_QCORROCT_109_QT_001.octupole] - - [B1, OCTF4_QCORROCT_109_QT_001.quadrupole] - - [A1, OCTF4_QCORROCT_109_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN14-AR/EM-OCT/OC.02/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN14-AR/EM-COR/OC.02-CQLN.07/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN14-AR/EM-COR/OC.02-CQLT.03/strength - unit: 1/m**2 -- type: pyaml.bpm.bpm - name: BPM_121 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN14-AR/DG-EPOS/BPM.05/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN14-AR/DG-EPOS/BPM.05/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SXD4_VCOR_003 - mapping: - - [B2, SXD4_VCOR_003.sextupole] - - [A0, SXD4_VCOR_003.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN14-AR/EM-SX/SCD.06/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN14-AR/EM-COR/SCD.06-CDLV.04/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_142 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN14-AR/EM-COR/CQLN.08/strength - unit: 1/m -- type: pyaml.magnet.quadrupole - name: QCORR_143 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN14-AR/EM-COR/CQLN.09/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SXD42_003 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN14-AR/EM-SX/SCD.07/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF42_HCOR_003 - mapping: - - [B2, SXF42_HCOR_003.sextupole] - - [B0, SXF42_HCOR_003.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN14-AR/EM-SX/SCF.08/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN14-AR/EM-COR/SCF.08-CDLH.05/strength - unit: '1' -- type: pyaml.magnet.cfm_magnet - name: OCTF4_QCORROCT_110_QT_001 - mapping: - - [B3, OCTF4_QCORROCT_110_QT_001.octupole] - - [B1, OCTF4_QCORROCT_110_QT_001.quadrupole] - - [A1, OCTF4_QCORROCT_110_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN14-AR/EM-OCT/OC.03/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN14-AR/EM-COR/OC.03-CQLN.10/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN14-AR/EM-COR/OC.03-CQLT.04/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXD42_VCOR_003 - mapping: - - [B2, SXD42_VCOR_003.sextupole] - - [A0, SXD42_VCOR_003.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN14-AR/EM-SX/SCD.09/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN14-AR/EM-COR/SCD.09-CDLV.05/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_122 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN14-AR/DG-EPOS/BPM.06/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN14-AR/DG-EPOS/BPM.06/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SH12_COR_005 - mapping: - - [B2, SH12_COR_005.sextupole] - - [B0, SH12_COR_005.hcorrector] - - [A0, SH12_COR_005.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0, A0] - units: [1/m**2, '1', '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN14-AR/EM-SX/SHD.04/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN14-AR/EM-COR/SHD.04-CDLH.06/strength - unit: '1' - - type: tango.pyaml.attribute - attribute: AN14-AR/EM-COR/SHD.04-CDLV.06/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_144 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN14-AR/EM-COR/CQLN.11/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SH11_005 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN14-AR/EM-SX/SHD.05/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: OH11_QCORROCT_111_001 - mapping: - - [B3, OH11_QCORROCT_111_001.octupole] - - [B1, OH11_QCORROCT_111_001.quadrupole] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1] - units: [1/m**3, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN14-AR/EM-OCT/OH.02/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN14-AR/EM-COR/OH.02-CQLN.12/strength - unit: 1/m**2 -- type: pyaml.bpm.bpm - name: BPM_123 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN14-AR/DG-EPOS/BPM.07/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN14-AR/DG-EPOS/BPM.07/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SH10_COR_005 - mapping: - - [B2, SH10_COR_005.sextupole] - - [B0, SH10_COR_005.hcorrector] - - [A0, SH10_COR_005.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0, A0] - units: [1/m**2, '1', '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN14-AR/EM-SX/SHF.06/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN14-AR/EM-COR/SHF.06-CDLH.07/strength - unit: '1' - - type: tango.pyaml.attribute - attribute: AN14-AR/EM-COR/SHF.06-CDLV.07/strength - unit: '1' -- type: pyaml.magnet.cfm_magnet - name: OH10_QCORROCT_112_QT_001 - mapping: - - [B3, OH10_QCORROCT_112_QT_001.octupole] - - [B1, OH10_QCORROCT_112_QT_001.quadrupole] - - [A1, OH10_QCORROCT_112_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN14-AR/EM-OCT/OH.03/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN14-AR/EM-COR/OH.03-CQLN.13/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN14-AR/EM-COR/OH.03-CQLT.05/strength - unit: 1/m**2 -- type: pyaml.bpm.bpm - name: BPM_124 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN15-SD/DG-EPOS/BPM.01/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN15-SD/DG-EPOS/BPM.01/y_pos - unit: mm -- type: pyaml.bpm.bpm - name: BPM_125 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN15-SD/DG-EPOS/BPM.02/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN15-SD/DG-EPOS/BPM.02/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: OH10_QCORROCT_113_QT_001 - mapping: - - [B3, OH10_QCORROCT_113_QT_001.octupole] - - [B1, OH10_QCORROCT_113_QT_001.quadrupole] - - [A1, OH10_QCORROCT_113_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN15-AR/EM-OCT/OH.01/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN15-AR/EM-COR/OH.01-CQLN.01/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN15-AR/EM-COR/OH.01-CQLT.01/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SH10_COR_006 - mapping: - - [B2, SH10_COR_006.sextupole] - - [B0, SH10_COR_006.hcorrector] - - [A0, SH10_COR_006.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0, A0] - units: [1/m**2, '1', '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN15-AR/EM-SX/SHF.01/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN15-AR/EM-COR/SHF.01-CDLH.01/strength - unit: '1' - - type: tango.pyaml.attribute - attribute: AN15-AR/EM-COR/SHF.01-CDLV.01/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_126 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN15-AR/DG-EPOS/BPM.03/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN15-AR/DG-EPOS/BPM.03/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: OH11_QCORROCT_114_001 - mapping: - - [B3, OH11_QCORROCT_114_001.octupole] - - [B1, OH11_QCORROCT_114_001.quadrupole] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1] - units: [1/m**3, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN15-AR/EM-OCT/OH.02/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN15-AR/EM-COR/OH.02-CQLN.02/strength - unit: 1/m**2 -- type: pyaml.magnet.sextupole - name: SH11_006 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN15-AR/EM-SX/SHD.02/strength - unit: 1/m**2 -- type: pyaml.magnet.quadrupole - name: QCORR_145 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN15-AR/EM-COR/CQLN.03/strength - unit: 1/m -- type: pyaml.magnet.cfm_magnet - name: SH12_COR_006 - mapping: - - [B2, SH12_COR_006.sextupole] - - [B0, SH12_COR_006.hcorrector] - - [A0, SH12_COR_006.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0, A0] - units: [1/m**2, '1', '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN15-AR/EM-SX/SHD.03/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN15-AR/EM-COR/SHD.03-CDLH.02/strength - unit: '1' - - type: tango.pyaml.attribute - attribute: AN15-AR/EM-COR/SHD.03-CDLV.02/strength - unit: '1' -- type: pyaml.magnet.sextupole - name: SXD51_003 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN15-AR/EM-SX/SCD.01/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: OCTF5_QCORROCT_115_QT_001 - mapping: - - [B3, OCTF5_QCORROCT_115_QT_001.octupole] - - [B1, OCTF5_QCORROCT_115_QT_001.quadrupole] - - [A1, OCTF5_QCORROCT_115_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN15-AR/EM-OCT/OC.01/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN15-AR/EM-COR/OC.01-CQLN.04/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN15-AR/EM-COR/OC.01-CQLT.02/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF51_HCOR_003 - mapping: - - [B2, SXF51_HCOR_003.sextupole] - - [B0, SXF51_HCOR_003.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN15-AR/EM-SX/SCF.02/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN15-AR/EM-COR/SCF.02-CDLH.03/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_127 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN15-AR/DG-EPOS/BPM.04/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN15-AR/DG-EPOS/BPM.04/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SXD51_VCOR_003 - mapping: - - [B2, SXD51_VCOR_003.sextupole] - - [A0, SXD51_VCOR_003.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN15-AR/EM-SX/SCD.03/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN15-AR/EM-COR/SCD.03-CDLV.03/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_146 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN15-AR/EM-COR/CQLN.05/strength - unit: 1/m -- type: pyaml.magnet.quadrupole - name: QCORR_147 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN15-AR/EM-COR/CQLN.06/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SXD5_007 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN15-AR/EM-SX/SCD.04/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: OCTF5_QCORROCT_116_QT_001 - mapping: - - [B3, OCTF5_QCORROCT_116_QT_001.octupole] - - [B1, OCTF5_QCORROCT_116_QT_001.quadrupole] - - [A1, OCTF5_QCORROCT_116_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN15-AR/EM-OCT/OC.02/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN15-AR/EM-COR/OC.02-CQLN.07/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN15-AR/EM-COR/OC.02-CQLT.03/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF5_HCOR_005 - mapping: - - [B2, SXF5_HCOR_005.sextupole] - - [B0, SXF5_HCOR_005.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN15-AR/EM-SX/SCF.05/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN15-AR/EM-COR/SCF.05-CDLH.04/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_128 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN15-AR/DG-EPOS/BPM.05/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN15-AR/DG-EPOS/BPM.05/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SXD5_VCOR_007 - mapping: - - [B2, SXD5_VCOR_007.sextupole] - - [A0, SXD5_VCOR_007.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN15-AR/EM-SX/SCD.06/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN15-AR/EM-COR/SCD.06-CDLV.04/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_148 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN15-AR/EM-COR/CQLN.08/strength - unit: 1/m -- type: pyaml.magnet.quadrupole - name: QCORR_149 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN15-AR/EM-COR/CQLN.09/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SXD5_008 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN15-AR/EM-SX/SCD.07/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: OCTF5_QCORROCT_117_QT_001 - mapping: - - [B3, OCTF5_QCORROCT_117_QT_001.octupole] - - [B1, OCTF5_QCORROCT_117_QT_001.quadrupole] - - [A1, OCTF5_QCORROCT_117_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN15-AR/EM-OCT/OC.03/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN15-AR/EM-COR/OC.03-CQLN.10/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN15-AR/EM-COR/OC.03-CQLT.04/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF53_HCOR_005 - mapping: - - [B2, SXF53_HCOR_005.sextupole] - - [B0, SXF53_HCOR_005.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN15-AR/EM-SX/SCF.08/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN15-AR/EM-COR/SCF.08-CDLH.05/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_129 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN15-AR/DG-EPOS/BPM.06/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN15-AR/DG-EPOS/BPM.06/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SXD53_VCOR_003 - mapping: - - [B2, SXD53_VCOR_003.sextupole] - - [A0, SXD53_VCOR_003.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN15-AR/EM-SX/SCD.09/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN15-AR/EM-COR/SCD.09-CDLV.05/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_150 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN15-AR/EM-COR/CQLN.11/strength - unit: 1/m -- type: pyaml.magnet.quadrupole - name: QCORR_151 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN15-AR/EM-COR/CQLN.12/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SXD53_003 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN15-AR/EM-SX/SCD.10/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF53_HCOR_006 - mapping: - - [B2, SXF53_HCOR_006.sextupole] - - [B0, SXF53_HCOR_006.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN15-AR/EM-SX/SCF.11/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN15-AR/EM-COR/SCF.11-CDLH.06/strength - unit: '1' -- type: pyaml.magnet.cfm_magnet - name: OCTF5_QCORROCT_118_QT_001 - mapping: - - [B3, OCTF5_QCORROCT_118_QT_001.octupole] - - [B1, OCTF5_QCORROCT_118_QT_001.quadrupole] - - [A1, OCTF5_QCORROCT_118_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN15-AR/EM-OCT/OC.04/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN15-AR/EM-COR/OC.04-CQLN.13/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN15-AR/EM-COR/OC.04-CQLT.05/strength - unit: 1/m**2 -- type: pyaml.bpm.bpm - name: BPM_130 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN15-AR/DG-EPOS/BPM.07/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN15-AR/DG-EPOS/BPM.07/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SXD5_VCOR_008 - mapping: - - [B2, SXD5_VCOR_008.sextupole] - - [A0, SXD5_VCOR_008.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN15-AR/EM-SX/SCD.12/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN15-AR/EM-COR/SCD.12-CDLV.06/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_152 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN15-AR/EM-COR/CQLN.14/strength - unit: 1/m -- type: pyaml.magnet.quadrupole - name: QCORR_153 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN15-AR/EM-COR/CQLN.15/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SXD5_009 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN15-AR/EM-SX/SCD.13/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF5_HCOR_006 - mapping: - - [B2, SXF5_HCOR_006.sextupole] - - [B0, SXF5_HCOR_006.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN15-AR/EM-SX/SCF.14/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN15-AR/EM-COR/SCF.14-CDLH.07/strength - unit: '1' -- type: pyaml.magnet.cfm_magnet - name: OCTF5_QCORROCT_119_QT_001 - mapping: - - [B3, OCTF5_QCORROCT_119_QT_001.octupole] - - [B1, OCTF5_QCORROCT_119_QT_001.quadrupole] - - [A1, OCTF5_QCORROCT_119_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN15-AR/EM-OCT/OC.05/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN15-AR/EM-COR/OC.05-CQLN.16/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN15-AR/EM-COR/OC.05-CQLT.06/strength - unit: 1/m**2 -- type: pyaml.bpm.bpm - name: BPM_131 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN15-AR/DG-EPOS/BPM.08/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN15-AR/DG-EPOS/BPM.08/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SXD5_VCOR_009 - mapping: - - [B2, SXD5_VCOR_009.sextupole] - - [A0, SXD5_VCOR_009.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN15-AR/EM-SX/SCD.15/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN15-AR/EM-COR/SCD.15-CDLV.07/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_154 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN15-AR/EM-COR/CQLN.17/strength - unit: 1/m -- type: pyaml.magnet.quadrupole - name: QCORR_155 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN15-AR/EM-COR/CQLN.18/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SXD52_003 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN15-AR/EM-SX/SCD.16/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF52_HCOR_003 - mapping: - - [B2, SXF52_HCOR_003.sextupole] - - [B0, SXF52_HCOR_003.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN15-AR/EM-SX/SCF.17/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN15-AR/EM-COR/SCF.17-CDLH.08/strength - unit: '1' -- type: pyaml.magnet.cfm_magnet - name: OCTF5_QCORROCT_120_QT_001 - mapping: - - [B3, OCTF5_QCORROCT_120_QT_001.octupole] - - [B1, OCTF5_QCORROCT_120_QT_001.quadrupole] - - [A1, OCTF5_QCORROCT_120_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN15-AR/EM-OCT/OC.06/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN15-AR/EM-COR/OC.06-CQLN.19/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN15-AR/EM-COR/OC.06-CQLT.07/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXD52_VCOR_003 - mapping: - - [B2, SXD52_VCOR_003.sextupole] - - [A0, SXD52_VCOR_003.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN15-AR/EM-SX/SCD.18/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN15-AR/EM-COR/SCD.18-CDLV.08/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_132 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN15-AR/DG-EPOS/BPM.09/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN15-AR/DG-EPOS/BPM.09/y_pos - unit: mm -- type: pyaml.magnet.quadrupole - name: QCORR_156 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN15-AR/EM-COR/CQLN.20/strength - unit: 1/m -- type: pyaml.magnet.cfm_magnet - name: SH15_VCOR_003 - mapping: - - [B2, SH15_VCOR_003.sextupole] - - [A0, SH15_VCOR_003.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN15-AR/EM-SX/SHD.04/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN15-AR/EM-COR/SHD.04-CDLV.09/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_133 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN15-AR/DG-EPOS/BPM.10/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN15-AR/DG-EPOS/BPM.10/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SH14_HCOR_003 - mapping: - - [B2, SH14_HCOR_003.sextupole] - - [B0, SH14_HCOR_003.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN15-AR/EM-SX/SHD.05/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN15-AR/EM-COR/SHD.05-CDLH.09/strength - unit: '1' -- type: pyaml.magnet.cfm_magnet - name: OH141_QCORROCT_121_001 - mapping: - - [B3, OH141_QCORROCT_121_001.octupole] - - [B1, OH141_QCORROCT_121_001.quadrupole] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1] - units: [1/m**3, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN15-AR/EM-OCT/OH.03/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN15-AR/EM-COR/OH.03-CQLN.21/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SH13_COR_003 - mapping: - - [B2, SH13_COR_003.sextupole] - - [B0, SH13_COR_003.hcorrector] - - [A0, SH13_COR_003.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0, A0] - units: [1/m**2, '1', '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN15-AR/EM-SX/SHF.06/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN15-AR/EM-COR/SHF.06-CDLH.10/strength - unit: '1' - - type: tango.pyaml.attribute - attribute: AN15-AR/EM-COR/SHF.06-CDLV.10/strength - unit: '1' -- type: pyaml.magnet.cfm_magnet - name: OH131_QCORROCT_122_001 - mapping: - - [B3, OH131_QCORROCT_122_001.octupole] - - [B1, OH131_QCORROCT_122_001.quadrupole] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1] - units: [1/m**3, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN15-AR/EM-OCT/OH.04/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN15-AR/EM-COR/OH.04-CQLN.22/strength - unit: 1/m**2 -- type: pyaml.bpm.bpm - name: BPM_134 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN16-SD/DG-EPOS/BPM.01/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN16-SD/DG-EPOS/BPM.01/y_pos - unit: mm -- type: pyaml.bpm.bpm - name: BPM_135 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN16-SD/DG-EPOS/BPM.02/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN16-SD/DG-EPOS/BPM.02/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: OH16_QCORROCT_123_001 - mapping: - - [B3, OH16_QCORROCT_123_001.octupole] - - [B1, OH16_QCORROCT_123_001.quadrupole] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1] - units: [1/m**3, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN16-SD/EM-OCT/OH.01/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN16-SD/EM-COR/OH.01-CQLN.01/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SH16_COR_003 - mapping: - - [B2, SH16_COR_003.sextupole] - - [B0, SH16_COR_003.hcorrector] - - [A0, SH16_COR_003.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0, A0] - units: [1/m**2, '1', '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN16-SD/EM-SX/SHD.01/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN16-SD/EM-COR/SHD.01-CDLH.01/strength - unit: '1' - - type: tango.pyaml.attribute - attribute: AN16-SD/EM-COR/SHD.01-CDLV.01/strength - unit: '1' -- type: pyaml.magnet.cfm_magnet - name: SH16_COR_004 - mapping: - - [B2, SH16_COR_004.sextupole] - - [B0, SH16_COR_004.hcorrector] - - [A0, SH16_COR_004.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0, A0] - units: [1/m**2, '1', '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN16-SD/EM-SX/SHD.02/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN16-SD/EM-COR/SHD.02-CDLH.02/strength - unit: '1' - - type: tango.pyaml.attribute - attribute: AN16-SD/EM-COR/SHD.02-CDLV.02/strength - unit: '1' -- type: pyaml.magnet.cfm_magnet - name: OH16_QCORROCT_124_001 - mapping: - - [B3, OH16_QCORROCT_124_001.octupole] - - [B1, OH16_QCORROCT_124_001.quadrupole] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1] - units: [1/m**3, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN16-SD/EM-OCT/OH.02/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN16-SD/EM-COR/OH.02-CQLN.02/strength - unit: 1/m**2 -- type: pyaml.bpm.bpm - name: BPM_136 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN16-SD/DG-EPOS/BPM.03/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN16-SD/DG-EPOS/BPM.03/y_pos - unit: mm -- type: pyaml.bpm.bpm - name: BPM_137 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN16-SD/DG-EPOS/BPM.04/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN16-SD/DG-EPOS/BPM.04/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: OH132_QCORROCT_125_001 - mapping: - - [B3, OH132_QCORROCT_125_001.octupole] - - [B1, OH132_QCORROCT_125_001.quadrupole] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1] - units: [1/m**3, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN16-AR/EM-OCT/OH.01/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN16-AR/EM-COR/OH.01-CQLN.01/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SH13_COR_004 - mapping: - - [B2, SH13_COR_004.sextupole] - - [B0, SH13_COR_004.hcorrector] - - [A0, SH13_COR_004.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0, A0] - units: [1/m**2, '1', '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN16-AR/EM-SX/SHF.01/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN16-AR/EM-COR/SHF.01-CDLH.03/strength - unit: '1' - - type: tango.pyaml.attribute - attribute: AN16-AR/EM-COR/SHF.01-CDLV.03/strength - unit: '1' -- type: pyaml.magnet.cfm_magnet - name: OH142_QCORROCT_126_001 - mapping: - - [B3, OH142_QCORROCT_126_001.octupole] - - [B1, OH142_QCORROCT_126_001.quadrupole] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1] - units: [1/m**3, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN16-AR/EM-OCT/OH.02/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN16-AR/EM-COR/OH.02-CQLN.02/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SH14_HCOR_004 - mapping: - - [B2, SH14_HCOR_004.sextupole] - - [B0, SH14_HCOR_004.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN16-AR/EM-SX/SHD.02/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN16-AR/EM-COR/SHD.02-CDLH.04/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_138 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN16-AR/DG-EPOS/BPM.05/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN16-AR/DG-EPOS/BPM.05/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SH15_VCOR_004 - mapping: - - [B2, SH15_VCOR_004.sextupole] - - [A0, SH15_VCOR_004.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN16-AR/EM-SX/SHD.03/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN16-AR/EM-COR/SHD.03-CDLV.04/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_157 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN16-AR/EM-COR/CQLN.03/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SXD52_004 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN16-AR/EM-SX/SCD.01/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: OCTF5_QCORROCT_127_QT_001 - mapping: - - [B3, OCTF5_QCORROCT_127_QT_001.octupole] - - [B1, OCTF5_QCORROCT_127_QT_001.quadrupole] - - [A1, OCTF5_QCORROCT_127_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN16-AR/EM-OCT/OC.01/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN16-AR/EM-COR/OC.01-CQLN.04/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN16-AR/EM-COR/OC.01-CQLT.01/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF52_HCOR_004 - mapping: - - [B2, SXF52_HCOR_004.sextupole] - - [B0, SXF52_HCOR_004.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN16-AR/EM-SX/SCF.02/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN16-AR/EM-COR/SCF.02-CDLH.05/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_139 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN16-AR/DG-EPOS/BPM.06/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN16-AR/DG-EPOS/BPM.06/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SXD52_VCOR_004 - mapping: - - [B2, SXD52_VCOR_004.sextupole] - - [A0, SXD52_VCOR_004.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN16-AR/EM-SX/SCD.03/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN16-AR/EM-COR/SCD.03-CDLV.05/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_158 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN16-AR/EM-COR/CQLN.05/strength - unit: 1/m -- type: pyaml.magnet.quadrupole - name: QCORR_159 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN16-AR/EM-COR/CQLN.06/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SXD5_010 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN16-AR/EM-SX/SCD.04/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: OCTF5_QCORROCT_128_QT_001 - mapping: - - [B3, OCTF5_QCORROCT_128_QT_001.octupole] - - [B1, OCTF5_QCORROCT_128_QT_001.quadrupole] - - [A1, OCTF5_QCORROCT_128_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN16-AR/EM-OCT/OC.02/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN16-AR/EM-COR/OC.02-CQLN.07/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN16-AR/EM-COR/OC.02-CQLT.02/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF5_HCOR_007 - mapping: - - [B2, SXF5_HCOR_007.sextupole] - - [B0, SXF5_HCOR_007.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN16-AR/EM-SX/SCF.05/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN16-AR/EM-COR/SCF.05-CDLH.06/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_140 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN16-AR/DG-EPOS/BPM.07/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN16-AR/DG-EPOS/BPM.07/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SXD5_VCOR_010 - mapping: - - [B2, SXD5_VCOR_010.sextupole] - - [A0, SXD5_VCOR_010.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN16-AR/EM-SX/SCD.06/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN16-AR/EM-COR/SCD.06-CDLV.06/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_160 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN16-AR/EM-COR/CQLN.08/strength - unit: 1/m -- type: pyaml.magnet.quadrupole - name: QCORR_161 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN16-AR/EM-COR/CQLN.09/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SXD5_011 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN16-AR/EM-SX/SCD.07/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: OCTF5_QCORROCT_129_QT_001 - mapping: - - [B3, OCTF5_QCORROCT_129_QT_001.octupole] - - [B1, OCTF5_QCORROCT_129_QT_001.quadrupole] - - [A1, OCTF5_QCORROCT_129_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN16-AR/EM-OCT/OC.03/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN16-AR/EM-COR/OC.03-CQLN.10/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN16-AR/EM-COR/OC.03-CQLT.03/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF53_HCOR_007 - mapping: - - [B2, SXF53_HCOR_007.sextupole] - - [B0, SXF53_HCOR_007.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN16-AR/EM-SX/SCF.08/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN16-AR/EM-COR/SCF.08-CDLH.07/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_141 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN16-AR/DG-EPOS/BPM.08/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN16-AR/DG-EPOS/BPM.08/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SXD53_VCOR_004 - mapping: - - [B2, SXD53_VCOR_004.sextupole] - - [A0, SXD53_VCOR_004.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN16-AR/EM-SX/SCD.09/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN16-AR/EM-COR/SCD.09-CDLV.07/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_162 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN16-AR/EM-COR/CQLN.11/strength - unit: 1/m -- type: pyaml.magnet.quadrupole - name: QCORR_163 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN16-AR/EM-COR/CQLN.12/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SXD53_004 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN16-AR/EM-SX/SCD.10/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF53_HCOR_008 - mapping: - - [B2, SXF53_HCOR_008.sextupole] - - [B0, SXF53_HCOR_008.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN16-AR/EM-SX/SCF.11/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN16-AR/EM-COR/SCF.11-CDLH.08/strength - unit: '1' -- type: pyaml.magnet.cfm_magnet - name: OCTF5_QCORROCT_130_QT_001 - mapping: - - [B3, OCTF5_QCORROCT_130_QT_001.octupole] - - [B1, OCTF5_QCORROCT_130_QT_001.quadrupole] - - [A1, OCTF5_QCORROCT_130_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN16-AR/EM-OCT/OC.04/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN16-AR/EM-COR/OC.04-CQLN.13/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN16-AR/EM-COR/OC.04-CQLT.04/strength - unit: 1/m**2 -- type: pyaml.bpm.bpm - name: BPM_142 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN16-AR/DG-EPOS/BPM.09/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN16-AR/DG-EPOS/BPM.09/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SXD5_VCOR_011 - mapping: - - [B2, SXD5_VCOR_011.sextupole] - - [A0, SXD5_VCOR_011.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN16-AR/EM-SX/SCD.12/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN16-AR/EM-COR/SCD.12-CDLV.08/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_164 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN16-AR/EM-COR/CQLN.14/strength - unit: 1/m -- type: pyaml.magnet.quadrupole - name: QCORR_165 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN16-AR/EM-COR/CQLN.15/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SXD5_012 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN16-AR/EM-SX/SCD.13/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF5_HCOR_008 - mapping: - - [B2, SXF5_HCOR_008.sextupole] - - [B0, SXF5_HCOR_008.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN16-AR/EM-SX/SCF.14/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN16-AR/EM-COR/SCF.14-CDLH.09/strength - unit: '1' -- type: pyaml.magnet.cfm_magnet - name: OCTF5_QCORROCT_131_QT_001 - mapping: - - [B3, OCTF5_QCORROCT_131_QT_001.octupole] - - [B1, OCTF5_QCORROCT_131_QT_001.quadrupole] - - [A1, OCTF5_QCORROCT_131_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN16-AR/EM-OCT/OC.05/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN16-AR/EM-COR/OC.05-CQLN.16/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN16-AR/EM-COR/OC.05-CQLT.05/strength - unit: 1/m**2 -- type: pyaml.bpm.bpm - name: BPM_143 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN16-AR/DG-EPOS/BPM.10/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN16-AR/DG-EPOS/BPM.10/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SXD5_VCOR_012 - mapping: - - [B2, SXD5_VCOR_012.sextupole] - - [A0, SXD5_VCOR_012.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN16-AR/EM-SX/SCD.15/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN16-AR/EM-COR/SCD.15-CDLV.09/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_166 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN16-AR/EM-COR/CQLN.17/strength - unit: 1/m -- type: pyaml.magnet.quadrupole - name: QCORR_167 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN16-AR/EM-COR/CQLN.18/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SXD51_004 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN16-AR/EM-SX/SCD.16/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF51_HCOR_004 - mapping: - - [B2, SXF51_HCOR_004.sextupole] - - [B0, SXF51_HCOR_004.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN16-AR/EM-SX/SCF.17/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN16-AR/EM-COR/SCF.17-CDLH.10/strength - unit: '1' -- type: pyaml.magnet.cfm_magnet - name: OCTF5_QCORROCT_132_QT_001 - mapping: - - [B3, OCTF5_QCORROCT_132_QT_001.octupole] - - [B1, OCTF5_QCORROCT_132_QT_001.quadrupole] - - [A1, OCTF5_QCORROCT_132_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN16-AR/EM-OCT/OC.06/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN16-AR/EM-COR/OC.06-CQLN.19/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN16-AR/EM-COR/OC.06-CQLT.06/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXD51_VCOR_004 - mapping: - - [B2, SXD51_VCOR_004.sextupole] - - [A0, SXD51_VCOR_004.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN16-AR/EM-SX/SCD.18/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN16-AR/EM-COR/SCD.18-CDLV.10/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_144 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN16-AR/DG-EPOS/BPM.11/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN16-AR/DG-EPOS/BPM.11/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SH12_COR_007 - mapping: - - [B2, SH12_COR_007.sextupole] - - [B0, SH12_COR_007.hcorrector] - - [A0, SH12_COR_007.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0, A0] - units: [1/m**2, '1', '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN16-AR/EM-SX/SHD.04/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN16-AR/EM-COR/SHD.04-CDLH.11/strength - unit: '1' - - type: tango.pyaml.attribute - attribute: AN16-AR/EM-COR/SHD.04-CDLV.11/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_168 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN16-AR/EM-COR/CQLN.20/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SH11_007 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN16-AR/EM-SX/SHD.05/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: OH11_QCORROCT_133_001 - mapping: - - [B3, OH11_QCORROCT_133_001.octupole] - - [B1, OH11_QCORROCT_133_001.quadrupole] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1] - units: [1/m**3, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN16-AR/EM-OCT/OH.03/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN16-AR/EM-COR/OH.03-CQLN.21/strength - unit: 1/m**2 -- type: pyaml.bpm.bpm - name: BPM_145 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN16-AR/DG-EPOS/BPM.12/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN16-AR/DG-EPOS/BPM.12/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SH10_COR_007 - mapping: - - [B2, SH10_COR_007.sextupole] - - [B0, SH10_COR_007.hcorrector] - - [A0, SH10_COR_007.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0, A0] - units: [1/m**2, '1', '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN16-AR/EM-SX/SHF.06/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN16-AR/EM-COR/SHF.06-CDLH.12/strength - unit: '1' - - type: tango.pyaml.attribute - attribute: AN16-AR/EM-COR/SHF.06-CDLV.12/strength - unit: '1' -- type: pyaml.magnet.cfm_magnet - name: OH10_QCORROCT_134_QT_001 - mapping: - - [B3, OH10_QCORROCT_134_QT_001.octupole] - - [B1, OH10_QCORROCT_134_QT_001.quadrupole] - - [A1, OH10_QCORROCT_134_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN16-AR/EM-OCT/OH.04/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN16-AR/EM-COR/OH.04-CQLN.22/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN16-AR/EM-COR/OH.04-CQLT.07/strength - unit: 1/m**2 -- type: pyaml.bpm.bpm - name: BPM_146 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN17-SD/DG-EPOS/BPM.01/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN17-SD/DG-EPOS/BPM.01/y_pos - unit: mm -- type: pyaml.bpm.bpm - name: BPM_147 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN17-SD/DG-EPOS/BPM.02/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN17-SD/DG-EPOS/BPM.02/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: OH10_QCORROCT_135_QT_001 - mapping: - - [B3, OH10_QCORROCT_135_QT_001.octupole] - - [B1, OH10_QCORROCT_135_QT_001.quadrupole] - - [A1, OH10_QCORROCT_135_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN17-AR/EM-OCT/OH.01/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN17-AR/EM-COR/OH.01-CQLN.01/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN17-AR/EM-COR/OH.01-CQLT.01/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SH10_COR_008 - mapping: - - [B2, SH10_COR_008.sextupole] - - [B0, SH10_COR_008.hcorrector] - - [A0, SH10_COR_008.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0, A0] - units: [1/m**2, '1', '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN17-AR/EM-SX/SHF.01/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN17-AR/EM-COR/SHF.01-CDLH.01/strength - unit: '1' - - type: tango.pyaml.attribute - attribute: AN17-AR/EM-COR/SHF.01-CDLV.01/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_148 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN17-AR/DG-EPOS/BPM.03/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN17-AR/DG-EPOS/BPM.03/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: OH11_QCORROCT_136_001 - mapping: - - [B3, OH11_QCORROCT_136_001.octupole] - - [B1, OH11_QCORROCT_136_001.quadrupole] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1] - units: [1/m**3, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN17-AR/EM-OCT/OH.02/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN17-AR/EM-COR/OH.02-CQLN.02/strength - unit: 1/m**2 -- type: pyaml.magnet.sextupole - name: SH11_008 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN17-AR/EM-SX/SHD.02/strength - unit: 1/m**2 -- type: pyaml.magnet.quadrupole - name: QCORR_169 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN17-AR/EM-COR/CQLN.03/strength - unit: 1/m -- type: pyaml.magnet.cfm_magnet - name: SH12_COR_008 - mapping: - - [B2, SH12_COR_008.sextupole] - - [B0, SH12_COR_008.hcorrector] - - [A0, SH12_COR_008.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0, A0] - units: [1/m**2, '1', '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN17-AR/EM-SX/SHD.03/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN17-AR/EM-COR/SHD.03-CDLH.02/strength - unit: '1' - - type: tango.pyaml.attribute - attribute: AN17-AR/EM-COR/SHD.03-CDLV.02/strength - unit: '1' -- type: pyaml.magnet.sextupole - name: SXD42_004 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN17-AR/EM-SX/SCD.01/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: OCTF4_QCORROCT_137_QT_001 - mapping: - - [B3, OCTF4_QCORROCT_137_QT_001.octupole] - - [B1, OCTF4_QCORROCT_137_QT_001.quadrupole] - - [A1, OCTF4_QCORROCT_137_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN17-AR/EM-OCT/OC.01/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN17-AR/EM-COR/OC.01-CQLN.04/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN17-AR/EM-COR/OC.01-CQLT.02/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF42_HCOR_004 - mapping: - - [B2, SXF42_HCOR_004.sextupole] - - [B0, SXF42_HCOR_004.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN17-AR/EM-SX/SCF.02/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN17-AR/EM-COR/SCF.02-CDLH.03/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_149 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN17-AR/DG-EPOS/BPM.04/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN17-AR/DG-EPOS/BPM.04/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SXD42_VCOR_004 - mapping: - - [B2, SXD42_VCOR_004.sextupole] - - [A0, SXD42_VCOR_004.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN17-AR/EM-SX/SCD.03/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN17-AR/EM-COR/SCD.03-CDLV.03/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_170 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN17-AR/EM-COR/CQLN.05/strength - unit: 1/m -- type: pyaml.magnet.quadrupole - name: QCORR_171 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN17-AR/EM-COR/CQLN.06/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SXD4_004 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN17-AR/EM-SX/SCD.04/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: OCTF4_QCORROCT_138_QT_001 - mapping: - - [B3, OCTF4_QCORROCT_138_QT_001.octupole] - - [B1, OCTF4_QCORROCT_138_QT_001.quadrupole] - - [A1, OCTF4_QCORROCT_138_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN17-AR/EM-OCT/OC.02/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN17-AR/EM-COR/OC.02-CQLN.07/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN17-AR/EM-COR/OC.02-CQLT.03/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF4_HCOR_004 - mapping: - - [B2, SXF4_HCOR_004.sextupole] - - [B0, SXF4_HCOR_004.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN17-AR/EM-SX/SCF.05/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN17-AR/EM-COR/SCF.05-CDLH.04/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_150 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN17-AR/DG-EPOS/BPM.05/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN17-AR/DG-EPOS/BPM.05/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SXD4_VCOR_004 - mapping: - - [B2, SXD4_VCOR_004.sextupole] - - [A0, SXD4_VCOR_004.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN17-AR/EM-SX/SCD.06/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN17-AR/EM-COR/SCD.06-CDLV.04/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_172 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN17-AR/EM-COR/CQLN.08/strength - unit: 1/m -- type: pyaml.magnet.quadrupole - name: QCORR_173 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN17-AR/EM-COR/CQLN.09/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SXD41_004 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN17-AR/EM-SX/SCD.07/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF41_HCOR_004 - mapping: - - [B2, SXF41_HCOR_004.sextupole] - - [B0, SXF41_HCOR_004.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN17-AR/EM-SX/SCF.08/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN17-AR/EM-COR/SCF.08-CDLH.05/strength - unit: '1' -- type: pyaml.magnet.cfm_magnet - name: OCTF4_QCORROCT_139_QT_001 - mapping: - - [B3, OCTF4_QCORROCT_139_QT_001.octupole] - - [B1, OCTF4_QCORROCT_139_QT_001.quadrupole] - - [A1, OCTF4_QCORROCT_139_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN17-AR/EM-OCT/OC.03/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN17-AR/EM-COR/OC.03-CQLN.10/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN17-AR/EM-COR/OC.03-CQLT.04/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXD41_VCOR_004 - mapping: - - [B2, SXD41_VCOR_004.sextupole] - - [A0, SXD41_VCOR_004.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN17-AR/EM-SX/SCD.09/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN17-AR/EM-COR/SCD.09-CDLV.05/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_151 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN17-AR/DG-EPOS/BPM.06/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN17-AR/DG-EPOS/BPM.06/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SH9_COR_013 - mapping: - - [B2, SH9_COR_013.sextupole] - - [B0, SH9_COR_013.hcorrector] - - [A0, SH9_COR_013.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0, A0] - units: [1/m**2, '1', '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN17-AR/EM-SX/SHD.04/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN17-AR/EM-COR/SHD.04-CDLH.06/strength - unit: '1' - - type: tango.pyaml.attribute - attribute: AN17-AR/EM-COR/SHD.04-CDLV.06/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_174 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN17-AR/EM-COR/CQLN.11/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SH8_013 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN17-AR/EM-SX/SHD.05/strength - unit: 1/m**2 -- type: pyaml.magnet.quadrupole - name: QCORR_175 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN17-AR/EM-COR/CQLN.12/strength - unit: 1/m -- type: pyaml.bpm.bpm - name: BPM_152 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN17-AR/DG-EPOS/BPM.07/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN17-AR/DG-EPOS/BPM.07/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SH7_COR_013 - mapping: - - [B2, SH7_COR_013.sextupole] - - [B0, SH7_COR_013.hcorrector] - - [A0, SH7_COR_013.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0, A0] - units: [1/m**2, '1', '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN17-AR/EM-SX/SHF.06/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN17-AR/EM-COR/SHF.06-CDLH.07/strength - unit: '1' - - type: tango.pyaml.attribute - attribute: AN17-AR/EM-COR/SHF.06-CDLV.07/strength - unit: '1' -- type: pyaml.magnet.cfm_magnet - name: OH7_QCORROCT_140_QT_001 - mapping: - - [B3, OH7_QCORROCT_140_QT_001.octupole] - - [B1, OH7_QCORROCT_140_QT_001.quadrupole] - - [A1, OH7_QCORROCT_140_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN17-AR/EM-OCT/OH.03/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN17-AR/EM-COR/OH.03-CQLN.13/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN17-AR/EM-COR/OH.03-CQLT.05/strength - unit: 1/m**2 -- type: pyaml.bpm.bpm - name: BPM_153 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN18-SD/DG-EPOS/BPM.01/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN18-SD/DG-EPOS/BPM.01/y_pos - unit: mm -- type: pyaml.bpm.bpm - name: BPM_154 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN18-SD/DG-EPOS/BPM.02/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN18-SD/DG-EPOS/BPM.02/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: OH7_QCORROCT_141_QT_001 - mapping: - - [B3, OH7_QCORROCT_141_QT_001.octupole] - - [B1, OH7_QCORROCT_141_QT_001.quadrupole] - - [A1, OH7_QCORROCT_141_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN18-AR/EM-OCT/OH.01/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN18-AR/EM-COR/OH.01-CQLN.01/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN18-AR/EM-COR/OH.01-CQLT.01/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SH7_COR_014 - mapping: - - [B2, SH7_COR_014.sextupole] - - [B0, SH7_COR_014.hcorrector] - - [A0, SH7_COR_014.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0, A0] - units: [1/m**2, '1', '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN18-AR/EM-SX/SHF.01/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN18-AR/EM-COR/SHF.01-CDLH.01/strength - unit: '1' - - type: tango.pyaml.attribute - attribute: AN18-AR/EM-COR/SHF.01-CDLV.01/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_155 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN18-AR/DG-EPOS/BPM.03/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN18-AR/DG-EPOS/BPM.03/y_pos - unit: mm -- type: pyaml.magnet.quadrupole - name: QCORR_176 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN18-AR/EM-COR/CQLN.02/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SH8_014 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN18-AR/EM-SX/SHD.02/strength - unit: 1/m**2 -- type: pyaml.magnet.quadrupole - name: QCORR_177 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN18-AR/EM-COR/CQLN.03/strength - unit: 1/m -- type: pyaml.magnet.cfm_magnet - name: SH9_COR_014 - mapping: - - [B2, SH9_COR_014.sextupole] - - [B0, SH9_COR_014.hcorrector] - - [A0, SH9_COR_014.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0, A0] - units: [1/m**2, '1', '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN18-AR/EM-SX/SHD.03/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN18-AR/EM-COR/SHD.03-CDLH.02/strength - unit: '1' - - type: tango.pyaml.attribute - attribute: AN18-AR/EM-COR/SHD.03-CDLV.02/strength - unit: '1' -- type: pyaml.magnet.sextupole - name: SXD32_004 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN18-AR/EM-SX/SCD.01/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: OCTF3_QCORROCT_142_QT_001 - mapping: - - [B3, OCTF3_QCORROCT_142_QT_001.octupole] - - [B1, OCTF3_QCORROCT_142_QT_001.quadrupole] - - [A1, OCTF3_QCORROCT_142_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN18-AR/EM-OCT/OC.01/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN18-AR/EM-COR/OC.01-CQLN.04/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN18-AR/EM-COR/OC.01-CQLT.02/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF32_HCOR_004 - mapping: - - [B2, SXF32_HCOR_004.sextupole] - - [B0, SXF32_HCOR_004.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN18-AR/EM-SX/SCF.02/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN18-AR/EM-COR/SCF.02-CDLH.03/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_156 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN18-AR/DG-EPOS/BPM.04/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN18-AR/DG-EPOS/BPM.04/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SXD32_VCOR_004 - mapping: - - [B2, SXD32_VCOR_004.sextupole] - - [A0, SXD32_VCOR_004.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN18-AR/EM-SX/SCD.03/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN18-AR/EM-COR/SCD.03-CDLV.03/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_178 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN18-AR/EM-COR/CQLN.05/strength - unit: 1/m -- type: pyaml.magnet.quadrupole - name: QCORR_179 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN18-AR/EM-COR/CQLN.06/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SXD3_010 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN18-AR/EM-SX/SCD.04/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: OCTF3_QCORROCT_143_QT_001 - mapping: - - [B3, OCTF3_QCORROCT_143_QT_001.octupole] - - [B1, OCTF3_QCORROCT_143_QT_001.quadrupole] - - [A1, OCTF3_QCORROCT_143_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN18-AR/EM-OCT/OC.02/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN18-AR/EM-COR/OC.02-CQLN.07/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN18-AR/EM-COR/OC.02-CQLT.03/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF3_HCOR_007 - mapping: - - [B2, SXF3_HCOR_007.sextupole] - - [B0, SXF3_HCOR_007.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN18-AR/EM-SX/SCF.05/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN18-AR/EM-COR/SCF.05-CDLH.04/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_157 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN18-AR/DG-EPOS/BPM.05/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN18-AR/DG-EPOS/BPM.05/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SXD3_VCOR_010 - mapping: - - [B2, SXD3_VCOR_010.sextupole] - - [A0, SXD3_VCOR_010.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN18-AR/EM-SX/SCD.06/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN18-AR/EM-COR/SCD.06-CDLV.04/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_180 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN18-AR/EM-COR/CQLN.08/strength - unit: 1/m -- type: pyaml.magnet.quadrupole - name: QCORR_181 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN18-AR/EM-COR/CQLN.09/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SXD3_011 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN18-AR/EM-SX/SCD.07/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: OCTF3_QCORROCT_144_QT_001 - mapping: - - [B3, OCTF3_QCORROCT_144_QT_001.octupole] - - [B1, OCTF3_QCORROCT_144_QT_001.quadrupole] - - [A1, OCTF3_QCORROCT_144_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN18-AR/EM-OCT/OC.03/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN18-AR/EM-COR/OC.03-CQLN.10/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN18-AR/EM-COR/OC.03-CQLT.04/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF33_HCOR_007 - mapping: - - [B2, SXF33_HCOR_007.sextupole] - - [B0, SXF33_HCOR_007.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN18-AR/EM-SX/SCF.08/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN18-AR/EM-COR/SCF.08-CDLH.05/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_158 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN18-AR/DG-EPOS/BPM.06/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN18-AR/DG-EPOS/BPM.06/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SXD33_VCOR_004 - mapping: - - [B2, SXD33_VCOR_004.sextupole] - - [A0, SXD33_VCOR_004.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN18-AR/EM-SX/SCD.09/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN18-AR/EM-COR/SCD.09-CDLV.05/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_182 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN18-AR/EM-COR/CQLN.11/strength - unit: 1/m -- type: pyaml.magnet.quadrupole - name: QCORR_183 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN18-AR/EM-COR/CQLN.12/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SXD33_004 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN18-AR/EM-SX/SCD.10/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF33_HCOR_008 - mapping: - - [B2, SXF33_HCOR_008.sextupole] - - [B0, SXF33_HCOR_008.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN18-AR/EM-SX/SCF.11/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN18-AR/EM-COR/SCF.11-CDLH.06/strength - unit: '1' -- type: pyaml.magnet.cfm_magnet - name: OCTF3_QCORROCT_145_QT_001 - mapping: - - [B3, OCTF3_QCORROCT_145_QT_001.octupole] - - [B1, OCTF3_QCORROCT_145_QT_001.quadrupole] - - [A1, OCTF3_QCORROCT_145_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN18-AR/EM-OCT/OC.04/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN18-AR/EM-COR/OC.04-CQLN.13/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN18-AR/EM-COR/OC.04-CQLT.05/strength - unit: 1/m**2 -- type: pyaml.bpm.bpm - name: BPM_159 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN18-AR/DG-EPOS/BPM.07/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN18-AR/DG-EPOS/BPM.07/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SXD3_VCOR_011 - mapping: - - [B2, SXD3_VCOR_011.sextupole] - - [A0, SXD3_VCOR_011.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN18-AR/EM-SX/SCD.12/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN18-AR/EM-COR/SCD.12-CDLV.06/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_184 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN18-AR/EM-COR/CQLN.14/strength - unit: 1/m -- type: pyaml.magnet.quadrupole - name: QCORR_185 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN18-AR/EM-COR/CQLN.15/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SXD3_012 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN18-AR/EM-SX/SCD.13/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF3_HCOR_008 - mapping: - - [B2, SXF3_HCOR_008.sextupole] - - [B0, SXF3_HCOR_008.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN18-AR/EM-SX/SCF.14/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN18-AR/EM-COR/SCF.14-CDLH.07/strength - unit: '1' -- type: pyaml.magnet.cfm_magnet - name: OCTF3_QCORROCT_146_QT_001 - mapping: - - [B3, OCTF3_QCORROCT_146_QT_001.octupole] - - [B1, OCTF3_QCORROCT_146_QT_001.quadrupole] - - [A1, OCTF3_QCORROCT_146_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN18-AR/EM-OCT/OC.05/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN18-AR/EM-COR/OC.05-CQLN.16/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN18-AR/EM-COR/OC.05-CQLT.06/strength - unit: 1/m**2 -- type: pyaml.bpm.bpm - name: BPM_160 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN18-AR/DG-EPOS/BPM.08/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN18-AR/DG-EPOS/BPM.08/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SXD3_VCOR_012 - mapping: - - [B2, SXD3_VCOR_012.sextupole] - - [A0, SXD3_VCOR_012.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN18-AR/EM-SX/SCD.15/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN18-AR/EM-COR/SCD.15-CDLV.07/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_186 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN18-AR/EM-COR/CQLN.17/strength - unit: 1/m -- type: pyaml.magnet.quadrupole - name: QCORR_187 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN18-AR/EM-COR/CQLN.18/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SXD31_004 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN18-AR/EM-SX/SCD.16/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF31_HCOR_004 - mapping: - - [B2, SXF31_HCOR_004.sextupole] - - [B0, SXF31_HCOR_004.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN18-AR/EM-SX/SCF.17/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN18-AR/EM-COR/SCF.17-CDLH.08/strength - unit: '1' -- type: pyaml.magnet.cfm_magnet - name: OCTF3_QCORROCT_147_QT_001 - mapping: - - [B3, OCTF3_QCORROCT_147_QT_001.octupole] - - [B1, OCTF3_QCORROCT_147_QT_001.quadrupole] - - [A1, OCTF3_QCORROCT_147_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN18-AR/EM-OCT/OC.06/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN18-AR/EM-COR/OC.06-CQLN.19/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN18-AR/EM-COR/OC.06-CQLT.07/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXD31_VCOR_004 - mapping: - - [B2, SXD31_VCOR_004.sextupole] - - [A0, SXD31_VCOR_004.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN18-AR/EM-SX/SCD.18/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN18-AR/EM-COR/SCD.18-CDLV.08/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_161 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN18-AR/DG-EPOS/BPM.09/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN18-AR/DG-EPOS/BPM.09/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SH9_COR_015 - mapping: - - [B2, SH9_COR_015.sextupole] - - [B0, SH9_COR_015.hcorrector] - - [A0, SH9_COR_015.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0, A0] - units: [1/m**2, '1', '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN18-AR/EM-SX/SHD.04/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN18-AR/EM-COR/SHD.04-CDLH.09/strength - unit: '1' - - type: tango.pyaml.attribute - attribute: AN18-AR/EM-COR/SHD.04-CDLV.09/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_188 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN18-AR/EM-COR/CQLN.20/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SH8_015 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN18-AR/EM-SX/SHD.05/strength - unit: 1/m**2 -- type: pyaml.magnet.quadrupole - name: QCORR_189 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN18-AR/EM-COR/CQLN.21/strength - unit: 1/m -- type: pyaml.bpm.bpm - name: BPM_162 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN18-AR/DG-EPOS/BPM.10/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN18-AR/DG-EPOS/BPM.10/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SH7_COR_015 - mapping: - - [B2, SH7_COR_015.sextupole] - - [B0, SH7_COR_015.hcorrector] - - [A0, SH7_COR_015.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0, A0] - units: [1/m**2, '1', '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN18-AR/EM-SX/SHF.06/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN18-AR/EM-COR/SHF.06-CDLH.10/strength - unit: '1' - - type: tango.pyaml.attribute - attribute: AN18-AR/EM-COR/SHF.06-CDLV.10/strength - unit: '1' -- type: pyaml.magnet.cfm_magnet - name: OH7_QCORROCT_148_QT_001 - mapping: - - [B3, OH7_QCORROCT_148_QT_001.octupole] - - [B1, OH7_QCORROCT_148_QT_001.quadrupole] - - [A1, OH7_QCORROCT_148_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN18-AR/EM-OCT/OH.02/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN18-AR/EM-COR/OH.02-CQLN.22/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN18-AR/EM-COR/OH.02-CQLT.08/strength - unit: 1/m**2 -- type: pyaml.bpm.bpm - name: BPM_163 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN19-SD/DG-EPOS/BPM.01/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN19-SD/DG-EPOS/BPM.01/y_pos - unit: mm -- type: pyaml.bpm.bpm - name: BPM_164 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN19-SD/DG-EPOS/BPM.02/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN19-SD/DG-EPOS/BPM.02/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: OH7_QCORROCT_149_QT_001 - mapping: - - [B3, OH7_QCORROCT_149_QT_001.octupole] - - [B1, OH7_QCORROCT_149_QT_001.quadrupole] - - [A1, OH7_QCORROCT_149_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN19-AR/EM-OCT/OH.01/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN19-AR/EM-COR/OH.01-CQLN.01/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN19-AR/EM-COR/OH.01-CQLT.01/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SH7_COR_016 - mapping: - - [B2, SH7_COR_016.sextupole] - - [B0, SH7_COR_016.hcorrector] - - [A0, SH7_COR_016.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0, A0] - units: [1/m**2, '1', '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN19-AR/EM-SX/SHF.01/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN19-AR/EM-COR/SHF.01-CDLH.01/strength - unit: '1' - - type: tango.pyaml.attribute - attribute: AN19-AR/EM-COR/SHF.01-CDLV.01/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_165 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN19-AR/DG-EPOS/BPM.03/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN19-AR/DG-EPOS/BPM.03/y_pos - unit: mm -- type: pyaml.magnet.quadrupole - name: QCORR_190 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN19-AR/EM-COR/CQLN.02/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SH8_016 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN19-AR/EM-SX/SHD.02/strength - unit: 1/m**2 -- type: pyaml.magnet.quadrupole - name: QCORR_191 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN19-AR/EM-COR/CQLN.03/strength - unit: 1/m -- type: pyaml.magnet.cfm_magnet - name: SH9_COR_016 - mapping: - - [B2, SH9_COR_016.sextupole] - - [B0, SH9_COR_016.hcorrector] - - [A0, SH9_COR_016.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0, A0] - units: [1/m**2, '1', '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN19-AR/EM-SX/SHD.03/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN19-AR/EM-COR/SHD.03-CDLH.02/strength - unit: '1' - - type: tango.pyaml.attribute - attribute: AN19-AR/EM-COR/SHD.03-CDLV.02/strength - unit: '1' -- type: pyaml.magnet.sextupole - name: SXD22_004 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN19-AR/EM-SX/SCD.01/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: OCTF2_QCORROCT_150_QT_001 - mapping: - - [B3, OCTF2_QCORROCT_150_QT_001.octupole] - - [B1, OCTF2_QCORROCT_150_QT_001.quadrupole] - - [A1, OCTF2_QCORROCT_150_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN19-AR/EM-OCT/OC.01/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN19-AR/EM-COR/OC.01-CQLN.04/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN19-AR/EM-COR/OC.01-CQLT.02/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF22_HCOR_004 - mapping: - - [B2, SXF22_HCOR_004.sextupole] - - [B0, SXF22_HCOR_004.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN19-AR/EM-SX/SCF.02/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN19-AR/EM-COR/SCF.02-CDLH.03/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_166 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN19-AR/DG-EPOS/BPM.04/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN19-AR/DG-EPOS/BPM.04/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SXD22_VCOR_004 - mapping: - - [B2, SXD22_VCOR_004.sextupole] - - [A0, SXD22_VCOR_004.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN19-AR/EM-SX/SCD.03/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN19-AR/EM-COR/SCD.03-CDLV.03/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_192 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN19-AR/EM-COR/CQLN.05/strength - unit: 1/m -- type: pyaml.magnet.quadrupole - name: QCORR_193 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN19-AR/EM-COR/CQLN.06/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SXD2_004 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN19-AR/EM-SX/SCD.04/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF2_HCOR_004 - mapping: - - [B2, SXF2_HCOR_004.sextupole] - - [B0, SXF2_HCOR_004.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN19-AR/EM-SX/SCF.05/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN19-AR/EM-COR/SCF.05-CDLH.04/strength - unit: '1' -- type: pyaml.magnet.cfm_magnet - name: OCTF2_QCORROCT_151_QT_001 - mapping: - - [B3, OCTF2_QCORROCT_151_QT_001.octupole] - - [B1, OCTF2_QCORROCT_151_QT_001.quadrupole] - - [A1, OCTF2_QCORROCT_151_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN19-AR/EM-OCT/OC.02/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN19-AR/EM-COR/OC.02-CQLN.07/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN19-AR/EM-COR/OC.02-CQLT.03/strength - unit: 1/m**2 -- type: pyaml.bpm.bpm - name: BPM_167 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN19-AR/DG-EPOS/BPM.05/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN19-AR/DG-EPOS/BPM.05/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SXD2_VCOR_004 - mapping: - - [B2, SXD2_VCOR_004.sextupole] - - [A0, SXD2_VCOR_004.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN19-AR/EM-SX/SCD.06/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN19-AR/EM-COR/SCD.06-CDLV.04/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_194 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN19-AR/EM-COR/CQLN.08/strength - unit: 1/m -- type: pyaml.magnet.quadrupole - name: QCORR_195 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN19-AR/EM-COR/CQLN.09/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SXD21_004 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN19-AR/EM-SX/SCD.07/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF21_HCOR_004 - mapping: - - [B2, SXF21_HCOR_004.sextupole] - - [B0, SXF21_HCOR_004.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN19-AR/EM-SX/SCF.08/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN19-AR/EM-COR/SCF.08-CDLH.05/strength - unit: '1' -- type: pyaml.magnet.cfm_magnet - name: OCTF2_QCORROCT_152_QT_001 - mapping: - - [B3, OCTF2_QCORROCT_152_QT_001.octupole] - - [B1, OCTF2_QCORROCT_152_QT_001.quadrupole] - - [A1, OCTF2_QCORROCT_152_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN19-AR/EM-OCT/OC.03/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN19-AR/EM-COR/OC.03-CQLN.10/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN19-AR/EM-COR/OC.03-CQLT.04/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXD21_VCOR_004 - mapping: - - [B2, SXD21_VCOR_004.sextupole] - - [A0, SXD21_VCOR_004.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN19-AR/EM-SX/SCD.09/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN19-AR/EM-COR/SCD.09-CDLV.05/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_168 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN19-AR/DG-EPOS/BPM.06/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN19-AR/DG-EPOS/BPM.06/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SH6_COR_007 - mapping: - - [B2, SH6_COR_007.sextupole] - - [B0, SH6_COR_007.hcorrector] - - [A0, SH6_COR_007.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0, A0] - units: [1/m**2, '1', '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN19-AR/EM-SX/SHD.04/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN19-AR/EM-COR/SHD.04-CDLH.06/strength - unit: '1' - - type: tango.pyaml.attribute - attribute: AN19-AR/EM-COR/SHD.04-CDLV.06/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_196 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN19-AR/EM-COR/CQLN.11/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SH5_007 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN19-AR/EM-SX/SHD.05/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: OH5_QCORROCT_153_001 - mapping: - - [B3, OH5_QCORROCT_153_001.octupole] - - [B1, OH5_QCORROCT_153_001.quadrupole] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1] - units: [1/m**3, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN19-AR/EM-OCT/OH.02/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN19-AR/EM-COR/OH.02-CQLN.12/strength - unit: 1/m**2 -- type: pyaml.bpm.bpm - name: BPM_169 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN19-AR/DG-EPOS/BPM.07/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN19-AR/DG-EPOS/BPM.07/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SH4_COR_007 - mapping: - - [B2, SH4_COR_007.sextupole] - - [B0, SH4_COR_007.hcorrector] - - [A0, SH4_COR_007.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0, A0] - units: [1/m**2, '1', '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN19-AR/EM-SX/SHF.06/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN19-AR/EM-COR/SHF.06-CDLH.07/strength - unit: '1' - - type: tango.pyaml.attribute - attribute: AN19-AR/EM-COR/SHF.06-CDLV.07/strength - unit: '1' -- type: pyaml.magnet.cfm_magnet - name: OH4_QCORROCT_154_QT_001 - mapping: - - [B3, OH4_QCORROCT_154_QT_001.octupole] - - [B1, OH4_QCORROCT_154_QT_001.quadrupole] - - [A1, OH4_QCORROCT_154_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN19-AR/EM-OCT/OH.03/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN19-AR/EM-COR/OH.03-CQLN.13/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN19-AR/EM-COR/OH.03-CQLT.05/strength - unit: 1/m**2 -- type: pyaml.bpm.bpm - name: BPM_170 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN20-SD/DG-EPOS/BPM.01/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN20-SD/DG-EPOS/BPM.01/y_pos - unit: mm -- type: pyaml.bpm.bpm - name: BPM_171 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN20-SD/DG-EPOS/BPM.02/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN20-SD/DG-EPOS/BPM.02/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: OH4_QCORROCT_155_QT_001 - mapping: - - [B3, OH4_QCORROCT_155_QT_001.octupole] - - [B1, OH4_QCORROCT_155_QT_001.quadrupole] - - [A1, OH4_QCORROCT_155_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN20-AR/EM-OCT/OH.01/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN20-AR/EM-COR/OH.01-CQLN.01/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN20-AR/EM-COR/OH.01-CQLT.01/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SH4_COR_008 - mapping: - - [B2, SH4_COR_008.sextupole] - - [B0, SH4_COR_008.hcorrector] - - [A0, SH4_COR_008.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0, A0] - units: [1/m**2, '1', '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN20-AR/EM-SX/SHF.01/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN20-AR/EM-COR/SHF.01-CDLH.01/strength - unit: '1' - - type: tango.pyaml.attribute - attribute: AN20-AR/EM-COR/SHF.01-CDLV.01/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_172 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN20-AR/DG-EPOS/BPM.03/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN20-AR/DG-EPOS/BPM.03/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: OH5_QCORROCT_156_001 - mapping: - - [B3, OH5_QCORROCT_156_001.octupole] - - [B1, OH5_QCORROCT_156_001.quadrupole] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1] - units: [1/m**3, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN20-AR/EM-OCT/OH.02/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN20-AR/EM-COR/OH.02-CQLN.02/strength - unit: 1/m**2 -- type: pyaml.magnet.sextupole - name: SH5_008 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN20-AR/EM-SX/SHD.02/strength - unit: 1/m**2 -- type: pyaml.magnet.quadrupole - name: QCORR_197 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN20-AR/EM-COR/CQLN.03/strength - unit: 1/m -- type: pyaml.magnet.cfm_magnet - name: SH6_COR_008 - mapping: - - [B2, SH6_COR_008.sextupole] - - [B0, SH6_COR_008.hcorrector] - - [A0, SH6_COR_008.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0, A0] - units: [1/m**2, '1', '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN20-AR/EM-SX/SHD.03/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN20-AR/EM-COR/SHD.03-CDLH.02/strength - unit: '1' - - type: tango.pyaml.attribute - attribute: AN20-AR/EM-COR/SHD.03-CDLV.02/strength - unit: '1' -- type: pyaml.magnet.sextupole - name: SXD12_004 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN20-AR/EM-SX/SCD.01/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: OCTF1_QCORROCT_157_QT_001 - mapping: - - [B3, OCTF1_QCORROCT_157_QT_001.octupole] - - [B1, OCTF1_QCORROCT_157_QT_001.quadrupole] - - [A1, OCTF1_QCORROCT_157_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN20-AR/EM-OCT/OC.01/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN20-AR/EM-COR/OC.01-CQLN.04/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN20-AR/EM-COR/OC.01-CQLT.02/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF12_HCOR_004 - mapping: - - [B2, SXF12_HCOR_004.sextupole] - - [B0, SXF12_HCOR_004.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN20-AR/EM-SX/SCF.02/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN20-AR/EM-COR/SCF.02-CDLH.03/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_173 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN20-AR/DG-EPOS/BPM.04/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN20-AR/DG-EPOS/BPM.04/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SXD12_VCOR_004 - mapping: - - [B2, SXD12_VCOR_004.sextupole] - - [A0, SXD12_VCOR_004.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN20-AR/EM-SX/SCD.03/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN20-AR/EM-COR/SCD.03-CDLV.03/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_198 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN20-AR/EM-COR/CQLN.05/strength - unit: 1/m -- type: pyaml.magnet.quadrupole - name: QCORR_199 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN20-AR/EM-COR/CQLN.06/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SXD1_010 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN20-AR/EM-SX/SCD.04/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: OCTF1_QCORROCT_158_QT_001 - mapping: - - [B3, OCTF1_QCORROCT_158_QT_001.octupole] - - [B1, OCTF1_QCORROCT_158_QT_001.quadrupole] - - [A1, OCTF1_QCORROCT_158_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN20-AR/EM-OCT/OC.02/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN20-AR/EM-COR/OC.02-CQLN.07/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN20-AR/EM-COR/OC.02-CQLT.03/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF1_HCOR_007 - mapping: - - [B2, SXF1_HCOR_007.sextupole] - - [B0, SXF1_HCOR_007.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN20-AR/EM-SX/SCF.05/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN20-AR/EM-COR/SCF.05-CDLH.04/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_174 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN20-AR/DG-EPOS/BPM.05/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN20-AR/DG-EPOS/BPM.05/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SXD1_VCOR_010 - mapping: - - [B2, SXD1_VCOR_010.sextupole] - - [A0, SXD1_VCOR_010.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN20-AR/EM-SX/SCD.06/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN20-AR/EM-COR/SCD.06-CDLV.04/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_200 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN20-AR/EM-COR/CQLN.08/strength - unit: 1/m -- type: pyaml.magnet.quadrupole - name: QCORR_201 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN20-AR/EM-COR/CQLN.09/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SXD1_011 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN20-AR/EM-SX/SCD.07/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: OCTF1_QCORROCT_159_QT_001 - mapping: - - [B3, OCTF1_QCORROCT_159_QT_001.octupole] - - [B1, OCTF1_QCORROCT_159_QT_001.quadrupole] - - [A1, OCTF1_QCORROCT_159_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN20-AR/EM-OCT/OC.03/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN20-AR/EM-COR/OC.03-CQLN.10/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN20-AR/EM-COR/OC.03-CQLT.04/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF13_HCOR_007 - mapping: - - [B2, SXF13_HCOR_007.sextupole] - - [B0, SXF13_HCOR_007.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN20-AR/EM-SX/SCF.08/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN20-AR/EM-COR/SCF.08-CDLH.05/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_175 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN20-AR/DG-EPOS/BPM.06/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN20-AR/DG-EPOS/BPM.06/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SXD13_VCOR_004 - mapping: - - [B2, SXD13_VCOR_004.sextupole] - - [A0, SXD13_VCOR_004.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN20-AR/EM-SX/SCD.09/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN20-AR/EM-COR/SCD.09-CDLV.05/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_202 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN20-AR/EM-COR/CQLN.11/strength - unit: 1/m -- type: pyaml.magnet.quadrupole - name: QCORR_203 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN20-AR/EM-COR/CQLN.12/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SXD13_004 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN20-AR/EM-SX/SCD.10/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF13_HCOR_008 - mapping: - - [B2, SXF13_HCOR_008.sextupole] - - [B0, SXF13_HCOR_008.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN20-AR/EM-SX/SCF.11/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN20-AR/EM-COR/SCF.11-CDLH.06/strength - unit: '1' -- type: pyaml.magnet.cfm_magnet - name: OCTF1_QCORROCT_160_QT_001 - mapping: - - [B3, OCTF1_QCORROCT_160_QT_001.octupole] - - [B1, OCTF1_QCORROCT_160_QT_001.quadrupole] - - [A1, OCTF1_QCORROCT_160_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN20-AR/EM-OCT/OC.04/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN20-AR/EM-COR/OC.04-CQLN.13/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN20-AR/EM-COR/OC.04-CQLT.05/strength - unit: 1/m**2 -- type: pyaml.bpm.bpm - name: BPM_176 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN20-AR/DG-EPOS/BPM.07/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN20-AR/DG-EPOS/BPM.07/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SXD1_VCOR_011 - mapping: - - [B2, SXD1_VCOR_011.sextupole] - - [A0, SXD1_VCOR_011.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN20-AR/EM-SX/SCD.12/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN20-AR/EM-COR/SCD.12-CDLV.06/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_204 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN20-AR/EM-COR/CQLN.14/strength - unit: 1/m -- type: pyaml.magnet.quadrupole - name: QCORR_205 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN20-AR/EM-COR/CQLN.15/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SXD1_012 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN20-AR/EM-SX/SCD.13/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF1_HCOR_008 - mapping: - - [B2, SXF1_HCOR_008.sextupole] - - [B0, SXF1_HCOR_008.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN20-AR/EM-SX/SCF.14/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN20-AR/EM-COR/SCF.14-CDLH.07/strength - unit: '1' -- type: pyaml.magnet.cfm_magnet - name: OCTF1_QCORROCT_161_QT_001 - mapping: - - [B3, OCTF1_QCORROCT_161_QT_001.octupole] - - [B1, OCTF1_QCORROCT_161_QT_001.quadrupole] - - [A1, OCTF1_QCORROCT_161_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN20-AR/EM-OCT/OC.05/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN20-AR/EM-COR/OC.05-CQLN.16/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN20-AR/EM-COR/OC.05-CQLT.06/strength - unit: 1/m**2 -- type: pyaml.bpm.bpm - name: BPM_177 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN20-AR/DG-EPOS/BPM.08/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN20-AR/DG-EPOS/BPM.08/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: SXD1_VCOR_012 - mapping: - - [B2, SXD1_VCOR_012.sextupole] - - [A0, SXD1_VCOR_012.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN20-AR/EM-SX/SCD.15/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN20-AR/EM-COR/SCD.15-CDLV.07/strength - unit: '1' -- type: pyaml.magnet.quadrupole - name: QCORR_206 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN20-AR/EM-COR/CQLN.17/strength - unit: 1/m -- type: pyaml.magnet.quadrupole - name: QCORR_207 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN20-AR/EM-COR/CQLN.18/strength - unit: 1/m -- type: pyaml.magnet.sextupole - name: SXD11_004 - model: - type: pyaml.magnet.identity_model - unit: 1/m**2 - physics: - type: tango.pyaml.attribute - attribute: AN20-AR/EM-SX/SCD.16/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXF11_HCOR_004 - mapping: - - [B2, SXF11_HCOR_004.sextupole] - - [B0, SXF11_HCOR_004.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN20-AR/EM-SX/SCF.17/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN20-AR/EM-COR/SCF.17-CDLH.08/strength - unit: '1' -- type: pyaml.magnet.cfm_magnet - name: OCTF1_QCORROCT_162_QT_001 - mapping: - - [B3, OCTF1_QCORROCT_162_QT_001.octupole] - - [B1, OCTF1_QCORROCT_162_QT_001.quadrupole] - - [A1, OCTF1_QCORROCT_162_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN20-AR/EM-OCT/OC.06/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN20-AR/EM-COR/OC.06-CQLN.19/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN20-AR/EM-COR/OC.06-CQLT.07/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SXD11_VCOR_004 - mapping: - - [B2, SXD11_VCOR_004.sextupole] - - [A0, SXD11_VCOR_004.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN20-AR/EM-SX/SCD.18/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN20-AR/EM-COR/SCD.18-CDLV.08/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_178 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN20-AR/DG-EPOS/BPM.09/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN20-AR/DG-EPOS/BPM.09/y_pos - unit: mm -- type: pyaml.magnet.quadrupole - name: QCORR_208 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: AN20-AR/EM-COR/CQLN.20/strength - unit: 1/m -- type: pyaml.magnet.cfm_magnet - name: SH3_VCOR_004 - mapping: - - [B2, SH3_VCOR_004.sextupole] - - [A0, SH3_VCOR_004.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, A0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN20-AR/EM-SX/SHD.04/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN20-AR/EM-COR/SHD.04-CDLV.09/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_179 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN20-AR/DG-EPOS/BPM.10/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN20-AR/DG-EPOS/BPM.10/y_pos - unit: mm -- type: pyaml.magnet.cfm_magnet - name: OH2_QCORROCT_163_001 - mapping: - - [B3, OH2_QCORROCT_163_001.octupole] - - [B1, OH2_QCORROCT_163_001.quadrupole] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1] - units: [1/m**3, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN20-AR/EM-OCT/OH.03/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN20-AR/EM-COR/OH.03-CQLN.21/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SH2_HCOR_004 - mapping: - - [B2, SH2_HCOR_004.sextupole] - - [B0, SH2_HCOR_004.hcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0] - units: [1/m**2, '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN20-AR/EM-SX/SHD.05/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN20-AR/EM-COR/SHD.05-CDLH.09/strength - unit: '1' -- type: pyaml.magnet.cfm_magnet - name: OH1_QCORROCT_164_QT_001 - mapping: - - [B3, OH1_QCORROCT_164_QT_001.octupole] - - [B1, OH1_QCORROCT_164_QT_001.quadrupole] - - [A1, OH1_QCORROCT_164_QT_001.skewquad] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B3, B1, A1] - units: [1/m**3, 1/m**2, 1/m**2] - physics: - - type: tango.pyaml.attribute - attribute: AN20-AR/EM-OCT/OH.04/strength - unit: 1/m**3 - - type: tango.pyaml.attribute - attribute: AN20-AR/EM-COR/OH.04-CQLN.22/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN20-AR/EM-COR/OH.04-CQLT.08/strength - unit: 1/m**2 -- type: pyaml.magnet.cfm_magnet - name: SH1_COR_004 - mapping: - - [B2, SH1_COR_004.sextupole] - - [B0, SH1_COR_004.hcorrector] - - [A0, SH1_COR_004.vcorrector] - model: - type: pyaml.magnet.identity_cfm_model - multipoles: [B2, B0, A0] - units: [1/m**2, '1', '1'] - physics: - - type: tango.pyaml.attribute - attribute: AN20-AR/EM-SX/SHF.06/strength - unit: 1/m**2 - - type: tango.pyaml.attribute - attribute: AN20-AR/EM-COR/SHF.06-CDLH.10/strength - unit: '1' - - type: tango.pyaml.attribute - attribute: AN20-AR/EM-COR/SHF.06-CDLV.10/strength - unit: '1' -- type: pyaml.bpm.bpm - name: BPM_180 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: AN01-SD/DG-EPOS/BPM.01/x_pos - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: AN01-SD/DG-EPOS/BPM.01/y_pos - unit: mm -- type: pyaml.rf.rf_plant - name: RF - masterclock: - type: tango.pyaml.attribute - attribute: simulator/ringsimulator/ringsimulator/RfFrequency - unit: Hz - transmitters: - - type: pyaml.rf.rf_transmitter - name: RFTRA - cavities: [RF_002, RFHARMON_002] - harmonic: 1 - distribution: 1 - voltage: - type: tango.pyaml.attribute - attribute: simulator/ringsimulator/ringsimulator/RfVoltage - unit: V diff --git a/examples/other_examples/ControlSystem/README.md b/examples/other_examples/ControlSystem/README.md new file mode 100644 index 000000000..e5e59de1a --- /dev/null +++ b/examples/other_examples/ControlSystem/README.md @@ -0,0 +1,3 @@ +# Example of simple ControlSystem interface implementations + +This folder provides examples of ControlSystem implementation and configuration. diff --git a/examples/other_examples/ControlSystem/tango/config.yaml b/examples/other_examples/ControlSystem/tango/config.yaml new file mode 100644 index 000000000..22881f758 --- /dev/null +++ b/examples/other_examples/ControlSystem/tango/config.yaml @@ -0,0 +1,14 @@ +type: pyaml.accelerator +facility: ESRF +machine: sr +energy: 6e9 +controls: + - type: tango_controlsystem + prefix: //ebs-simu-3:10000/ + name: live +data_folder: /data/store +devices: +- type: pyaml.bpm.bpm + name: BPM_C01-01 + x_pos: srdiag/bpm/c01-01/SA_HPosition + y_pos: srdiag/bpm/c01-01/SA_VPosition diff --git a/examples/other_examples/ControlSystem/tango/main.py b/examples/other_examples/ControlSystem/tango/main.py new file mode 100644 index 000000000..8fe0782be --- /dev/null +++ b/examples/other_examples/ControlSystem/tango/main.py @@ -0,0 +1,11 @@ +from pyaml.accelerator import Accelerator + +sr = Accelerator.load("config.yaml") + +# print the BPM position +bpm = sr.live.bpm.get("BPM_C01-01") # bpm is a BPM +print(bpm.positions.get()) + +# Direct access to control system +da = sr.live.get_device_access("srdiag/bpm/c01-01/SA_HPosition") # da is a DeviceAccess +print(f"h={da.get()} {da.unit()}") diff --git a/examples/other_examples/ControlSystem/tango/tango_controlsystem.py b/examples/other_examples/ControlSystem/tango/tango_controlsystem.py new file mode 100644 index 000000000..0f4a2e975 --- /dev/null +++ b/examples/other_examples/ControlSystem/tango/tango_controlsystem.py @@ -0,0 +1,124 @@ +# This example show a minimal Tango control system implementation + +import logging + +import tango +from pydantic import BaseModel + +from pyaml.control.controlsystem import ControlSystemAdapter +from pyaml.control.deviceaccess import DeviceAccess + +PYAMLCLASS: str = "MyControlSystem" + +# ---------------------- ControlSystem configuration model ----------------------- + + +class ConfigModel(BaseModel): + """ + Configuration model for an OA Control System. + + Attributes + ---------- + name : str + Name of the control system. + prefix : str + Prefix added to the to name passed to get_device() + """ + + name: str + prefix: str = "" + + +# ---------------------- Hardware access interface ------------------------------- + + +class MyDevice(DeviceAccess): + def __init__(self, name: str): + self._name = self.name + self._proxy = tango.AttributeProxy(name) + att_config = self._proxy.get_config() + self._iswrittable = att_config.writable in [ + tango.AttrWriteType.READ_WRITE, + tango.AttrWriteType.WRITE, + tango.AttrWriteType.READ_WITH_WRITE, + ] + self._unit = att_config.unit + try: + min = float(att_config.min_value) + max = float(att_config.max_value) + self._range = [min, max] + except Exception: + self._range = [None, None] + + def name(self) -> str: + """Return the name of the variable""" + return self._name + + def measure_name(self) -> str: + """Return the name of the measure""" + return self._name + + def set(self, value): + """Write a control system device variable (i.e. a power supply current)""" + self._proxy.write(value) + + def set_and_wait(self, value): + """Write a control system device variable (i.e. a power supply current)""" + pass + + def get(self): + """Return the setpoint(s) of a control system device variable""" + if self._iswrittable: + return self._proxy.read().w_value + else: + return self._proxy.read().value + + def readback(self): + """Return the measured variable""" + return self._proxy.read().value + + def unit(self) -> str: + """Return the variable unit""" + return self._unit + + def get_range(self) -> list[float]: + """ + Get the valid range for the device variable. + + Returns + ------- + list[float] + List containing [min, max] values + """ + return self._range + + def check_device_availability(self) -> bool: + """ + Check if the device is available and accessible. + + Returns + ------- + bool + True if device is available, False otherwise + """ + return self._proxy.ping() + + +# ---------------------- The control system class ------------------------------- + + +class MyControlSystem(ControlSystemAdapter): + def __init__(self, cfg: ConfigModel): + super().__init__() + self._cfg = cfg + + def get_device_access(self, ref: str | BaseModel | None) -> DeviceAccess | None: + if ref is None: + return None + return MyDevice(self._cfg.prefix + ref) + + def name(self) -> str: + return self._cfg.name + + def __repr__(self): + return repr(self._cfg).replace("ConfigModel", self.__class__.__name__) diff --git a/examples/ORM_Tango_server/ORM.py b/examples/other_examples/ORM_Tango_server/ORM.py similarity index 100% rename from examples/ORM_Tango_server/ORM.py rename to examples/other_examples/ORM_Tango_server/ORM.py diff --git a/examples/ORM_Tango_server/README.md b/examples/other_examples/ORM_Tango_server/README.md similarity index 100% rename from examples/ORM_Tango_server/README.md rename to examples/other_examples/ORM_Tango_server/README.md diff --git a/examples/ORM_Tango_server/orm_scan_1.png b/examples/other_examples/ORM_Tango_server/orm_scan_1.png similarity index 100% rename from examples/ORM_Tango_server/orm_scan_1.png rename to examples/other_examples/ORM_Tango_server/orm_scan_1.png diff --git a/examples/ORM_Tango_server/orm_scan_2.png b/examples/other_examples/ORM_Tango_server/orm_scan_2.png similarity index 100% rename from examples/ORM_Tango_server/orm_scan_2.png rename to examples/other_examples/ORM_Tango_server/orm_scan_2.png diff --git a/examples/ORM_Tango_server/orm_scan_3.png b/examples/other_examples/ORM_Tango_server/orm_scan_3.png similarity index 100% rename from examples/ORM_Tango_server/orm_scan_3.png rename to examples/other_examples/ORM_Tango_server/orm_scan_3.png diff --git a/examples/OphydDevice_examples/README.md b/examples/other_examples/OphydDevice_examples/README.md similarity index 100% rename from examples/OphydDevice_examples/README.md rename to examples/other_examples/OphydDevice_examples/README.md diff --git a/examples/OphydDevice_examples/tune_ophyd_device.py b/examples/other_examples/OphydDevice_examples/tune_ophyd_device.py similarity index 100% rename from examples/OphydDevice_examples/tune_ophyd_device.py rename to examples/other_examples/OphydDevice_examples/tune_ophyd_device.py diff --git a/examples/use_cases/01-tune_correction.ipynb b/examples/use_cases/01-tune_correction.ipynb new file mode 100644 index 000000000..de520fbad --- /dev/null +++ b/examples/use_cases/01-tune_correction.ipynb @@ -0,0 +1,588 @@ +{ + "cells": [ + { + "cell_type": "code", + "execution_count": 1, + "id": "a6f35de9", + "metadata": {}, + "outputs": [], + "source": [ + "from pathlib import Path\n", + "\n", + "import matplotlib.pyplot as plt\n", + "import numpy as np\n", + "\n", + "from pyaml.accelerator import Accelerator\n", + "from pyaml.common.constants import Action" + ] + }, + { + "cell_type": "markdown", + "id": "fec1651c", + "metadata": {}, + "source": [ + "## Facility configuration\n", + "\n", + "Edit the `CONFIG_FILE` variable below to select the facility. The rest of the notebook runs unchanged.\n", + "\n", + "| Facility | Config file | Control system | Virtual twin |\n", + "|----------|-------------|----------------|--------------|\n", + "| SOLEIL II | `config/soleil_ii/p.yaml` | TANGO (`tango-pyaml`) | Apptainer container |\n", + "| BESSY2 | `config/bessy2/bessy2.yaml` | EPICS (`pyaml-cs-oa`) | Apptainer container |\n", + "| ESRF EBS | `config/esrf/esrf.yaml` | TANGO (`tango-pyaml`) | Apptainer container |\n", + "\n", + "See `README.md` for installation and virtual accelerator startup instructions." + ] + }, + { + "cell_type": "code", + "execution_count": 2, + "id": "244e23c0", + "metadata": {}, + "outputs": [ + { + "name": "stderr", + "output_type": "stream", + "text": [ + "PyAML Tango control system binding (0.4.0) initialized with name 'live' and TANGO_HOST=ebs-simu-3:10000\n" + ] + }, + { + "name": "stdout", + "output_type": "stream", + "text": [ + "14 Aug 2026, 13:40:30 | WARNING | /home/gubaidulin/codes/operation/pyAML/pyaml/examples/unified_examples/config/esrf/trm.json: file not found\n", + "14 Aug 2026, 13:40:30 | WARNING | /home/gubaidulin/codes/operation/pyAML/pyaml/examples/unified_examples/config/esrf/chroma_resp.json: file not found\n", + "14 Aug 2026, 13:40:30 | WARNING | Loading /home/gubaidulin/codes/operation/pyAML/pyaml/examples/unified_examples/config/esrf/orm.json failed /home/gubaidulin/codes/operation/pyAML/pyaml/examples/unified_examples/config/esrf/orm.json: file not found\n" + ] + }, + { + "data": { + "text/plain": [ + "Accelerator(facility='ESRF', machine='sr', description=None, live=TangoControlSystem(name='live', tango_host='ebs-simu-3:10000', catalog=, debug_level=None, lazy_devices=True, timeout_ms=3000), design=Simulator(name='design', lattice='/home/gubaidulin/codes/operation/pyAML/pyaml/examples/unified_examples/config/esrf/sr/lattices/ebs.mat', mat_key=None, linker=None, description=None), yellow_pages=Controls:\n", + " live\n", + " .\n", + "\n", + "Simulators:\n", + " design\n", + " .\n", + "\n", + "Arrays:\n", + " BPM (pyaml.arrays.bpm_array) size=320\n", + " HCorr (pyaml.arrays.magnet_array) size=288\n", + " VCorr (pyaml.arrays.magnet_array) size=288\n", + " Skews (pyaml.arrays.magnet_array) size=288\n", + " Sext (pyaml.arrays.magnet_array) size=180\n", + " QForTune (pyaml.arrays.magnet_array) size=124\n", + " .\n", + "\n", + "Tools:\n", + " BBA-BPM_C04-04 (pyaml.tuning_tools.bba)\n", + " BBA2-BPM_C04-04 (pyaml.tuning_tools.bba2)\n", + " CHROMATICITY_MONITOR (pyaml.tuning_tools.chromaticity_monitor)\n", + " DEFAULT_TUNE_CORRECTION (pyaml.tuning_tools.tune)\n", + " DEFAULT_TUNE_RESPONSE_MATRIX (pyaml.tuning_tools.tune_response_matrix)\n", + " DEFAULT_CHROMATICITY_RESPONSE_MATRIX (pyaml.tuning_tools.chromaticity_response_matrix)\n", + " DEFAULT_CHROMATICITY_CORRECTION (pyaml.tuning_tools.chromaticity)\n", + " DEFAULT_ORBIT_CORRECTION (pyaml.tuning_tools.orbit)\n", + " DEFAULT_ORBIT_RESPONSE_MATRIX (pyaml.tuning_tools.orbit_response_matrix)\n", + " DEFAULT_DISPERSION (pyaml.tuning_tools.dispersion)\n", + " .\n", + "\n", + "Diagnostics:\n", + " BETATRON_TUNE (pyaml.diagnostics.tune_monitor)\n", + " .)" + ] + }, + "execution_count": 2, + "metadata": {}, + "output_type": "execute_result" + } + ], + "source": [ + "# ── Facility configuration ──────────────────────────────────────────────────\n", + "# Uncomment the facility you want to use:\n", + "\n", + "# CONFIG_FILE = \"config/soleil_ii/p.yaml\"\n", + "# CONFIG_FILE = \"config/bessy2/bessy2.yaml\"\n", + "CONFIG_FILE = \"config/esrf/esrf.yaml\"\n", + "# ────────────────────────────────────────────────────────────────────────────\n", + "\n", + "CONFIG_DIR = Path(CONFIG_FILE).parent\n", + "\n", + "sr = Accelerator.load(CONFIG_FILE)\n", + "sr # string representation" + ] + }, + { + "cell_type": "markdown", + "id": "ff257f23", + "metadata": {}, + "source": [ + "### Virtual accelerator setup\n", + "\n", + "For **live** control mode you need a running control system or emulator. If you want to skip this, run the notebook in **design** mode only.\n", + "\n", + "**SOLEIL II / ESRF (TANGO)**\n", + "```\n", + "apptainer pull virtual-accelerator.sif oras://gitlab-registry.synchrotron-soleil.fr/software-control-system/containers/apptainer/virtual-accelerator:latest\n", + "apptainer run virtual-accelerator.sif\n", + "```\n", + "\n", + "**BESSY2 (EPICS)**\n", + "```\n", + "apptainer run oras://registry.hzdr.de/digital-twins-for-accelerators/containers/pyat-softioc-digital-twin:default-v0-5-1-bessy.2711893\n", + "```\n", + "\n", + "> **Note for BESSY2 live mode:** the PV prefix in `config/bessy2/bessy2.yaml` must match your virtual accelerator instance. Edit the `prefix:` field under `controls:`." + ] + }, + { + "cell_type": "markdown", + "id": "eb26cc8a", + "metadata": {}, + "source": [ + "### Control mode choice\n", + "\n", + "- **`sr.design`** — runs pyAT locally, no control system needed. Set `wait_time = 0.0`.\n", + "- **`sr.live`** — connects to the real machine or virtual twin. Set `wait_time` to allow readback settling (typically 1.5–2 s)." + ] + }, + { + "cell_type": "code", + "execution_count": 3, + "id": "134855a2", + "metadata": {}, + "outputs": [ + { + "data": { + "text/plain": [ + "Simulator(name='design', lattice='/home/gubaidulin/codes/operation/pyAML/pyaml/examples/unified_examples/config/esrf/sr/lattices/ebs.mat', mat_key=None, linker=None, description=None)" + ] + }, + "execution_count": 3, + "metadata": {}, + "output_type": "execute_result" + } + ], + "source": [ + "SR = sr.design\n", + "# SR = sr.live\n", + "\n", + "wait_time = 0.0 if SR == sr.design else 2.0\n", + "SR # string representation" + ] + }, + { + "cell_type": "markdown", + "id": "ebba627e", + "metadata": {}, + "source": [ + "#### Betatron tune monitor\n", + "\n", + "The tune monitor is defined in the configuration file under the name `BETATRON_TUNE`." + ] + }, + { + "cell_type": "code", + "execution_count": 4, + "id": "e028b13f", + "metadata": {}, + "outputs": [ + { + "name": "stdout", + "output_type": "stream", + "text": [ + "Current tune: [0.15999673 0.33999769]\n" + ] + }, + { + "data": { + "text/plain": [ + "BetatronTuneMonitor(tune_h='srdiag/beam-tune/main/Qh', tune_v='srdiag/beam-tune/main/Qv', name='BETATRON_TUNE')" + ] + }, + "execution_count": 4, + "metadata": {}, + "output_type": "execute_result" + } + ], + "source": [ + "tune_monitor = SR.get_betatron_tune_monitor(\"BETATRON_TUNE\")\n", + "print(f\"Current tune: {tune_monitor.tune.get()}\")\n", + "tune_monitor # string representation" + ] + }, + { + "cell_type": "markdown", + "id": "7f60ac56", + "metadata": {}, + "source": [ + "#### Quadrupolar correctors\n", + "\n", + "The `QForTune` array contains the quadrupoles used for tune correction. You can access and set individual corrector strengths." + ] + }, + { + "cell_type": "code", + "execution_count": 5, + "id": "33d2cb2c", + "metadata": {}, + "outputs": [ + { + "name": "stdout", + "output_type": "stream", + "text": [ + "The ring has 124 quadrupolar correctors. First: QD2E-C04\n" + ] + }, + { + "data": { + "text/plain": [ + "Quadrupole(peer='Simulator:design', name='QD2E-C04', model_name='QD2E-C04', magnet_model=LinearMagnetModel(curve=CSVCurve(file='sr/magnet_models/QD2_strength.csv'), powerconverter='srmag/vps-qd2/c04-e/current', calibration_factor=0.999305341, calibration_offset=0.0, crosstalk=0.99912, unit='1/m', hardware_unit='A'))" + ] + }, + "execution_count": 5, + "metadata": {}, + "output_type": "execute_result" + } + ], + "source": [ + "qcorrectors = SR.get_magnets(\"QForTune\")\n", + "first_q = qcorrectors[0]\n", + "print(f\"The ring has {len(qcorrectors)} quadrupolar correctors. First: {first_q.get_name()}\")\n", + "qcorrectors[0] # string representation" + ] + }, + { + "cell_type": "code", + "execution_count": 6, + "id": "704ecb05", + "metadata": {}, + "outputs": [ + { + "name": "stdout", + "output_type": "stream", + "text": [ + "Current strength: qcorrectors[0].strength.get()=-0.6176\n", + "After stepping by 0.002: qcorrectors[0].strength.get()=-0.6156\n", + "Reset to -0.6176\n" + ] + } + ], + "source": [ + "str_before = qcorrectors[0].strength.get()\n", + "print(f\"Current strength: {qcorrectors[0].strength.get()=:.4f}\")\n", + "qcorrectors[0].strength.set(str_before + 0.002)\n", + "print(f\"After stepping by 0.002: {qcorrectors[0].strength.get()=:.4f}\")\n", + "qcorrectors[0].strength.set(str_before)\n", + "print(f\"Reset to {str_before:.4f}\")" + ] + }, + { + "cell_type": "markdown", + "id": "04431246", + "metadata": {}, + "source": [ + "### Standard tune correction tool\n", + "\n", + "`SR.tune` is the `DEFAULT_TUNE_CORRECTION` tool. `SR.trm` is the `DEFAULT_TUNE_RESPONSE_MATRIX` tool.\n", + "\n", + "Before correcting the tune you need a response matrix. It can be measured (below) or loaded from a previously saved file." + ] + }, + { + "cell_type": "code", + "execution_count": 7, + "id": "5c57ef30", + "metadata": {}, + "outputs": [ + { + "data": { + "text/plain": [ + "Tune(peer='Simulator:design', name='DEFAULT_TUNE_CORRECTION', description=None, lattice_names=None, quad_array_name='QForTune', betatron_tune_name='BETATRON_TUNE', response_matrix=None)" + ] + }, + "execution_count": 7, + "metadata": {}, + "output_type": "execute_result" + } + ], + "source": [ + "SR.tune # string representation" + ] + }, + { + "cell_type": "markdown", + "id": "5a699129", + "metadata": {}, + "source": [ + "#### Measuring the tune response matrix\n", + "\n", + "The callback below prints progress during the measurement. The `sleep_between_step` parameter controls the wait time between corrector steps — set it to 0 for design mode.\n", + "\n", + "> **Note:** on some lattices `disable_6d()` is required before measuring in design mode." + ] + }, + { + "cell_type": "code", + "execution_count": 8, + "id": "a1e6ab4c", + "metadata": {}, + "outputs": [], + "source": [ + "# Required on some lattices before measuring the TRM in design mode\n", + "sr.design.get_lattice().disable_6d()\n", + "\n", + "\n", + "def tune_callback(action: int, cb_data: dict):\n", + " if action == Action.MEASURE:\n", + " print(f\"Tune response: #{cb_data['step']} {cb_data['magnet']} {cb_data['tune']}\")\n", + " return True" + ] + }, + { + "cell_type": "code", + "execution_count": 9, + "id": "c81cdb05", + "metadata": {}, + "outputs": [ + { + "name": "stdout", + "output_type": "stream", + "text": [ + "Tune response: #0 QD2E-C04 [0.15998216 0.34012592]\n", + "Tune response: #0 QD2A-C05 [0.15998212 0.34012589]\n", + "Tune response: #0 QD2E-C05 [0.1599821 0.34012584]\n", + "Tune response: #0 QD2A-C06 [0.15998217 0.34012594]\n", + "Tune response: #0 QD2E-C06 [0.15998208 0.34012584]\n", + "Tune response: #0 QD2A-C07 [0.15998213 0.34012602]\n", + "Tune response: #0 QD2E-C07 [0.15998215 0.340126 ]\n", + "Tune response: #0 QD2A-C08 [0.15998206 0.34012578]\n", + "Tune response: #0 QD2E-C08 [0.15998218 0.34012586]\n", + "Tune response: #0 QD2A-C09 [0.15998211 0.34012597]\n", + "Tune response: #0 QD2E-C09 [0.15998211 0.34012589]\n", + "Tune response: #0 QD2A-C10 [0.15998217 0.34012598]\n", + "Tune response: #0 QD2E-C10 [0.15998208 0.34012601]\n", + "Tune response: #0 QD2A-C11 [0.15998214 0.34012583]\n", + "Tune response: #0 QD2E-C11 [0.15998213 0.3401259 ]\n", + "Tune response: #0 QD2A-C12 [0.15998208 0.3401259 ]\n", + "Tune response: #0 QD2E-C12 [0.15998217 0.34012583]\n", + "Tune response: #0 QD2A-C13 [0.1599821 0.34012601]\n", + "Tune response: #0 QD2E-C13 [0.15998212 0.34012598]\n", + "Tune response: #0 QD2A-C14 [0.15998216 0.34012589]\n", + "Tune response: #0 QD2E-C14 [0.15998417 0.34012858]\n", + "Tune response: #0 QD2A-C15 [0.15998426 0.34012844]\n", + "Tune response: #0 QD2E-C15 [0.15998478 0.34012941]\n", + "Tune response: #0 QD2A-C16 [0.15998476 0.34012945]\n", + "Tune response: #0 QD2E-C16 [0.15998218 0.34012588]\n", + "Tune response: #0 QD2A-C17 [0.15998206 0.34012598]\n", + "Tune response: #0 QD2E-C17 [0.15998217 0.34012597]\n", + "Tune response: #0 QD2A-C18 [0.15998213 0.34012588]\n", + "Tune response: #0 QD2E-C18 [0.15998208 0.34012594]\n", + "Tune response: #0 QD2A-C19 [0.15998219 0.34012587]\n", + "Tune response: #0 QD2E-C19 [0.15998207 0.34012585]\n", + "Tune response: #0 QD2A-C20 [0.15998211 0.34012595]\n", + "Tune response: #0 QD2E-C20 [0.15998217 0.34012596]\n", + "Tune response: #0 QD2A-C21 [0.15998206 0.34012594]\n", + "Tune response: #0 QD2E-C21 [0.15998218 0.340126 ]\n", + "Tune response: #0 QD2A-C22 [0.15998212 0.34012583]\n", + "Tune response: #0 QD2E-C22 [0.15998209 0.34012586]\n", + "Tune response: #0 QD2A-C23 [0.15998219 0.34012593]\n", + "Tune response: #0 QD2E-C23 [0.15998206 0.34012584]\n", + "Tune response: #0 QD2A-C24 [0.15998214 0.34012597]\n", + "Tune response: #0 QD2E-C24 [0.15998215 0.3401259 ]\n", + "Tune response: #0 QD2A-C25 [0.15998206 0.34012597]\n", + "Tune response: #0 QD2E-C25 [0.15998219 0.34012598]\n", + "Tune response: #0 QD2A-C26 [0.15998209 0.34012578]\n", + "Tune response: #0 QD2E-C26 [0.15998212 0.34012582]\n", + "Tune response: #0 QD2A-C27 [0.15998218 0.34012602]\n", + "Tune response: #0 QD2E-C27 [0.15998206 0.34012593]\n", + "Tune response: #0 QD2A-C28 [0.15998214 0.34012592]\n", + "Tune response: #0 QD2E-C28 [0.15998214 0.34012605]\n", + "Tune response: #0 QD2A-C29 [0.15998207 0.3401258 ]\n", + "Tune response: #0 QD2E-C29 [0.15998444 0.34012874]\n", + "Tune response: #0 QD2A-C30 [0.15998435 0.34012877]\n", + "Tune response: #0 QD2E-C30 [0.15998212 0.34012589]\n", + "Tune response: #0 QD2A-C31 [0.15998217 0.34012598]\n", + "Tune response: #0 QD2E-C31 [0.15998208 0.34012595]\n", + "Tune response: #0 QD2A-C32 [0.15998213 0.34012582]\n", + "Tune response: #0 QD2E-C32 [0.15998214 0.34012586]\n", + "Tune response: #0 QD2A-C01 [0.15998208 0.34012599]\n", + "Tune response: #0 QD2E-C01 [0.15998217 0.34012592]\n", + "Tune response: #0 QD2A-C02 [0.15998208 0.34012587]\n", + "Tune response: #0 QD2E-C02 [0.15998213 0.34012591]\n", + "Tune response: #0 QD2A-C03 [0.15998216 0.34012595]\n", + "Tune response: #0 QF1E-C04 [0.15994093 0.34004929]\n", + "Tune response: #0 QF1A-C05 [0.15994083 0.34004928]\n", + "Tune response: #0 QF1E-C05 [0.15994074 0.34004926]\n", + "Tune response: #0 QF1A-C06 [0.15994093 0.34004931]\n", + "Tune response: #0 QF1E-C06 [0.15994063 0.34004925]\n", + "Tune response: #0 QF1A-C07 [0.15994075 0.34004933]\n", + "Tune response: #0 QF1E-C07 [0.1599408 0.34004933]\n", + "Tune response: #0 QF1A-C08 [0.15994062 0.34004925]\n", + "Tune response: #0 QF1E-C08 [0.15994094 0.34004926]\n", + "Tune response: #0 QF1A-C09 [0.15994079 0.34004931]\n", + "Tune response: #0 QF1E-C09 [0.15994078 0.34004927]\n", + "Tune response: #0 QF1A-C10 [0.15994094 0.34004931]\n", + "Tune response: #0 QF1E-C10 [0.15994062 0.34004932]\n", + "Tune response: #0 QF1A-C11 [0.15994079 0.34004925]\n", + "Tune response: #0 QF1E-C11 [0.15994076 0.34004929]\n", + "Tune response: #0 QF1A-C12 [0.15994062 0.34004929]\n", + "Tune response: #0 QF1E-C12 [0.15994094 0.34004925]\n", + "Tune response: #0 QF1A-C13 [0.15994075 0.34004932]\n", + "Tune response: #0 QF1E-C13 [0.15994082 0.34004931]\n", + "Tune response: #0 QF1A-C14 [0.15994094 0.34004927]\n", + "Tune response: #0 QF1E-C14 [0.1599476 0.34004944]\n", + "Tune response: #0 QF1A-C15 [0.15994785 0.34004939]\n", + "Tune response: #0 QF1E-C15 [0.15994977 0.34004945]\n", + "Tune response: #0 QF1A-C16 [0.15994975 0.34004947]\n", + "Tune response: #0 QF1E-C16 [0.1599409 0.34004927]\n", + "Tune response: #0 QF1A-C17 [0.15994059 0.34004931]\n", + "Tune response: #0 QF1E-C17 [0.15994098 0.34004931]\n", + "Tune response: #0 QF1A-C18 [0.15994089 0.34004927]\n", + "Tune response: #0 QF1E-C18 [0.15994069 0.3400493 ]\n", + "Tune response: #0 QF1A-C19 [0.15994098 0.34004927]\n", + "Tune response: #0 QF1E-C19 [0.15994058 0.34004926]\n", + "Tune response: #0 QF1A-C20 [0.1599407 0.34004931]\n", + "Tune response: #0 QF1E-C20 [0.15994085 0.34004929]\n", + "Tune response: #0 QF1A-C21 [0.15994057 0.34004929]\n", + "Tune response: #0 QF1E-C21 [0.159941 0.34004932]\n", + "Tune response: #0 QF1A-C22 [0.15994083 0.34004925]\n", + "Tune response: #0 QF1E-C22 [0.15994074 0.34004927]\n", + "Tune response: #0 QF1A-C23 [0.159941 0.3400493]\n", + "Tune response: #0 QF1E-C23 [0.15994056 0.34004926]\n", + "Tune response: #0 QF1A-C24 [0.15994076 0.34004931]\n", + "Tune response: #0 QF1E-C24 [0.15994079 0.34004928]\n", + "Tune response: #0 QF1A-C25 [0.15994056 0.3400493 ]\n", + "Tune response: #0 QF1E-C25 [0.159941 0.34004932]\n", + "Tune response: #0 QF1A-C26 [0.15994078 0.34004925]\n", + "Tune response: #0 QF1E-C26 [0.1599408 0.34004924]\n", + "Tune response: #0 QF1A-C27 [0.159941 0.34004933]\n", + "Tune response: #0 QF1E-C27 [0.15994056 0.34004929]\n", + "Tune response: #0 QF1A-C28 [0.15994081 0.34004929]\n", + "Tune response: #0 QF1E-C28 [0.15994074 0.34004933]\n", + "Tune response: #0 QF1A-C29 [0.15994057 0.34004924]\n", + "Tune response: #0 QF1E-C29 [0.15994855 0.34004941]\n", + "Tune response: #0 QF1A-C30 [0.15994833 0.34004944]\n", + "Tune response: #0 QF1E-C30 [0.1599408 0.34004927]\n", + "Tune response: #0 QF1A-C31 [0.15994094 0.34004931]\n", + "Tune response: #0 QF1E-C31 [0.15994063 0.34004931]\n", + "Tune response: #0 QF1A-C32 [0.1599408 0.34004926]\n", + "Tune response: #0 QF1E-C32 [0.15994075 0.34004926]\n", + "Tune response: #0 QF1A-C01 [0.15994063 0.34004932]\n", + "Tune response: #0 QF1E-C01 [0.15994093 0.34004929]\n", + "Tune response: #0 QF1A-C02 [0.15994074 0.34004928]\n", + "Tune response: #0 QF1E-C02 [0.15994083 0.34004928]\n", + "Tune response: #0 QF1A-C03 [0.15994093 0.3400493 ]\n", + "Response matrix loaded.\n" + ] + }, + { + "data": { + "text/plain": [ + "TuneResponseMatrix(peer='Simulator:design', name='DEFAULT_TUNE_RESPONSE_MATRIX', description=None, lattice_names=None, n_step=1, sleep_between_step=0, n_avg_meas=1, sleep_between_meas=0, quad_array_name='QForTune', betatron_tune_name='BETATRON_TUNE', quad_delta=0.0001)" + ] + }, + "execution_count": 9, + "metadata": {}, + "output_type": "execute_result" + } + ], + "source": [ + "if SR.tune.response_matrix is None:\n", + " SR.trm.measure(sleep_between_step=wait_time, callback=tune_callback)\n", + " SR.trm.save(CONFIG_DIR / \"trm.json\")\n", + "\n", + "SR.tune.load(CONFIG_DIR / \"trm.json\")\n", + "print(\"Response matrix loaded.\")\n", + "SR.trm # string representation" + ] + }, + { + "cell_type": "markdown", + "id": "ef7d7ce4", + "metadata": {}, + "source": [ + "#### Correcting the tune\n", + "\n", + "`SR.tune.set([qx, qy])` runs the correction iteratively. The `iter` parameter controls the number of iterations and `wait_time` the settling time between each iteration." + ] + }, + { + "cell_type": "code", + "execution_count": 10, + "id": "6b8bcf91", + "metadata": {}, + "outputs": [ + { + "name": "stdout", + "output_type": "stream", + "text": [ + "Tune before correction: [0.16000001 0.33999986]\n", + "\n", + "Setting tune to [0.19, 0.28]\n", + "Tune after correction: [0.19 0.28]\n", + "\n", + "Setting tune to [0.21, 0.3]\n", + "Tune after correction: [0.21 0.3 ]\n" + ] + }, + { + "data": { + "text/plain": [ + "Tune(peer='Simulator:design', name='DEFAULT_TUNE_CORRECTION', description=None, lattice_names=None, quad_array_name='QForTune', betatron_tune_name='BETATRON_TUNE', response_matrix=ResponseMatrixData(matrix=[[0.1785312775665071, 0.17890918518254084, 0.17917983711424057, 0.1784306145899417, 0.17932054383273943, 0.17884878472013144, 0.17868979674900975, 0.17950221390589105, 0.17836418103545082, 0.17902879800274496, 0.17907228791497198, 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-0.49446220468818414, -0.4941096561139613, -0.49580432387785756, -0.49525990132137654, -0.495847581273301, -0.4960629050582144, -0.49405329285656663, -0.4945045490734046, -0.4944593030919986, -0.49409568533387294, -0.4943868486234626, -0.4941100382965802, -0.49400608370830934, -0.4944961134639714, -0.49429209945439645, -0.4942981255562362, -0.4945974694420263, -0.4939197575981602, -0.4940787556634296, -0.49437648356964736, -0.4939864595138177, -0.4945109812737325, -0.4941389209023317, -0.49443276362082234, -0.4945754345897502, -0.4938861760950264, -0.4938234754592319, -0.49469773213683954, -0.4942676459879225, -0.4943106724386581, -0.4947356646151091, -0.49380505579399436, -0.49553591837780964, -0.495742188148518, -0.4940722391477692, -0.4944901952558256, -0.4944531012929243, -0.4940232475564299, -0.4939673852005777, -0.4945672189560213, -0.49428634374737435, -0.4942095438964511, -0.4941586272116938, -0.49439460739097996]], variable_names=['QD2E-C04', 'QD2A-C05', 'QD2E-C05', 'QD2A-C06', 'QD2E-C06', 'QD2A-C07', 'QD2E-C07', 'QD2A-C08', 'QD2E-C08', 'QD2A-C09', 'QD2E-C09', 'QD2A-C10', 'QD2E-C10', 'QD2A-C11', 'QD2E-C11', 'QD2A-C12', 'QD2E-C12', 'QD2A-C13', 'QD2E-C13', 'QD2A-C14', 'QD2E-C14', 'QD2A-C15', 'QD2E-C15', 'QD2A-C16', 'QD2E-C16', 'QD2A-C17', 'QD2E-C17', 'QD2A-C18', 'QD2E-C18', 'QD2A-C19', 'QD2E-C19', 'QD2A-C20', 'QD2E-C20', 'QD2A-C21', 'QD2E-C21', 'QD2A-C22', 'QD2E-C22', 'QD2A-C23', 'QD2E-C23', 'QD2A-C24', 'QD2E-C24', 'QD2A-C25', 'QD2E-C25', 'QD2A-C26', 'QD2E-C26', 'QD2A-C27', 'QD2E-C27', 'QD2A-C28', 'QD2E-C28', 'QD2A-C29', 'QD2E-C29', 'QD2A-C30', 'QD2E-C30', 'QD2A-C31', 'QD2E-C31', 'QD2A-C32', 'QD2E-C32', 'QD2A-C01', 'QD2E-C01', 'QD2A-C02', 'QD2E-C02', 'QD2A-C03', 'QF1E-C04', 'QF1A-C05', 'QF1E-C05', 'QF1A-C06', 'QF1E-C06', 'QF1A-C07', 'QF1E-C07', 'QF1A-C08', 'QF1E-C08', 'QF1A-C09', 'QF1E-C09', 'QF1A-C10', 'QF1E-C10', 'QF1A-C11', 'QF1E-C11', 'QF1A-C12', 'QF1E-C12', 'QF1A-C13', 'QF1E-C13', 'QF1A-C14', 'QF1E-C14', 'QF1A-C15', 'QF1E-C15', 'QF1A-C16', 'QF1E-C16', 'QF1A-C17', 'QF1E-C17', 'QF1A-C18', 'QF1E-C18', 'QF1A-C19', 'QF1E-C19', 'QF1A-C20', 'QF1E-C20', 'QF1A-C21', 'QF1E-C21', 'QF1A-C22', 'QF1E-C22', 'QF1A-C23', 'QF1E-C23', 'QF1A-C24', 'QF1E-C24', 'QF1A-C25', 'QF1E-C25', 'QF1A-C26', 'QF1E-C26', 'QF1A-C27', 'QF1E-C27', 'QF1A-C28', 'QF1E-C28', 'QF1A-C29', 'QF1E-C29', 'QF1A-C30', 'QF1E-C30', 'QF1A-C31', 'QF1E-C31', 'QF1A-C32', 'QF1E-C32', 'QF1A-C01', 'QF1E-C01', 'QF1A-C02', 'QF1E-C02', 'QF1A-C03'], observable_names=['BETATRON_TUNE.x', 'BETATRON_TUNE.y']))" + ] + }, + "execution_count": 10, + "metadata": {}, + "output_type": "execute_result" + } + ], + "source": [ + "print(f\"Tune before correction: {SR.tune.readback()}\")\n", + "\n", + "qx, qy = 0.19, 0.28\n", + "print(f\"\\nSetting tune to [{qx}, {qy}]\")\n", + "SR.tune.set([qx, qy], iter=10, wait_time=wait_time)\n", + "print(f\"Tune after correction: {SR.tune.readback()}\")\n", + "\n", + "qx, qy = 0.21, 0.30\n", + "print(f\"\\nSetting tune to [{qx}, {qy}]\")\n", + "SR.tune.set([qx, qy], iter=10, wait_time=wait_time)\n", + "print(f\"Tune after correction: {SR.tune.readback()}\")\n", + "\n", + "SR.tune # string representation" + ] + }, + { + "cell_type": "code", + "execution_count": null, + "id": "29bfad11-3da0-4890-b069-f31cfeaa41bb", + "metadata": {}, + "outputs": [], + "source": [] + } + ], + "metadata": { + "kernelspec": { + "display_name": "Python 3 (ipykernel)", + "language": "python", + "name": "python3" + }, + "language_info": { + "codemirror_mode": { + "name": "ipython", + "version": 3 + }, + "file_extension": ".py", + "mimetype": "text/x-python", + "name": "python", + "nbconvert_exporter": "python", + "pygments_lexer": "ipython3", + "version": "3.12.3" + } + }, + "nbformat": 4, + "nbformat_minor": 5 +} diff --git a/examples/use_cases/01-tune_correction.py b/examples/use_cases/01-tune_correction.py new file mode 100644 index 000000000..959affb65 --- /dev/null +++ b/examples/use_cases/01-tune_correction.py @@ -0,0 +1,180 @@ +#!/usr/bin/env python +# coding: utf-8 + +# In[1]: + + +# ## Facility configuration +# +# Edit the `CONFIG_FILE` variable below to select the facility. The rest of the notebook runs unchanged. +# +# | Facility | Config file | Control system | Virtual twin | +# |----------|-------------|----------------|--------------| +# | SOLEIL II | `config/soleil_ii/p.yaml` | TANGO (`tango-pyaml`) | Apptainer container | +# | BESSY2 | `config/bessy2/bessy2.yaml` | EPICS (`pyaml-cs-oa`) | Apptainer container | +# | ESRF EBS | `config/esrf/esrf.yaml` | TANGO (`tango-pyaml`) | Apptainer container | +# +# See `README.md` for installation and virtual accelerator startup instructions. +# In[2]: +from pathlib import Path + +import matplotlib.pyplot as plt +import numpy as np + +from pyaml.accelerator import Accelerator +from pyaml.common.constants import Action + +# ── Facility configuration ────────────────────────────────────────────────── +# Uncomment the facility you want to use: + +# CONFIG_FILE = "config/soleil_ii/p.yaml" +# CONFIG_FILE = "config/bessy2/bessy2.yaml" +CONFIG_FILE = "config/esrf/esrf.yaml" +# ──────────────────────────────────────────────────────────────────────────── + +CONFIG_DIR = Path(CONFIG_FILE).parent + +sr = Accelerator.load(CONFIG_FILE) +print(sr) # string representation + + +# ### Virtual accelerator setup +# +# For **live** control mode you need a running control system or emulator. +# If you want to skip this, run the notebook in **design** mode only. +# +# **SOLEIL II / ESRF (TANGO)** +# ``` +# apptainer pull virtual-accelerator.sif oras://gitlab-registry.synchrotron-soleil.fr/software-control-system/containers/apptainer/virtual-accelerator:latest +# apptainer run virtual-accelerator.sif +# ``` +# +# **BESSY2 (EPICS)** +# ``` +# apptainer run oras://registry.hzdr.de/digital-twins-for-accelerators/containers/pyat-softioc-digital-twin:default-v0-5-1-bessy.2711893 +# ``` +# +# > **Note for BESSY2 live mode:** the PV prefix in `config/bessy2/bessy2.yaml` must match +# > your virtual accelerator instance. Edit the `prefix:` field under `controls:`. + +# ### Control mode choice +# +# - **`sr.design`** — runs pyAT locally, no control system needed. Set `wait_time = 0.0`. +# - **`sr.live`** — connects to the real machine or virtual twin. Set `wait_time` to allow +# readback settling (typically 1.5–2 s). + +# In[3]: + + +SR = sr.design +# SR = sr.live + +wait_time = 0.0 if SR == sr.design else 2.0 +print(SR) # string representation + + +# #### Betatron tune monitor +# +# The tune monitor is defined in the configuration file under the name `BETATRON_TUNE`. + +# In[4]: + + +tune_monitor = SR.get_betatron_tune_monitor("BETATRON_TUNE") +print(f"Current tune: {tune_monitor.tune.get()}") +print(tune_monitor) # string representation + + +# #### Quadrupolar correctors +# +# The `QForTune` array contains the quadrupoles used for tune correction. +# You can access and set individual corrector strengths. + +# In[5]: + + +qcorrectors = SR.get_magnets("QForTune") +first_q = qcorrectors[0] +print(f"The ring has {len(qcorrectors)} quadrupolar correctors. First: {first_q.get_name()}") +print(qcorrectors[0]) # string representation + + +# In[6]: + + +str_before = qcorrectors[0].strength.get() +print(f"Current strength: {qcorrectors[0].strength.get()=:.4f}") +qcorrectors[0].strength.set(str_before + 0.002) +print(f"After stepping by 0.002: {qcorrectors[0].strength.get()=:.4f}") +qcorrectors[0].strength.set(str_before) +print(f"Reset to {str_before:.4f}") + + +# ### Standard tune correction tool +# +# `SR.tune` is the `DEFAULT_TUNE_CORRECTION` tool. `SR.trm` is the `DEFAULT_TUNE_RESPONSE_MATRIX` tool. +# +# Before correcting the tune you need a response matrix. It can be measured (below) or loaded from a previously saved file. + +# In[7]: + + +print(SR.tune) # string representation + + +# #### Measuring the tune response matrix +# +# The callback below prints progress during the measurement. The `sleep_between_step` +# parameter controls the wait time between corrector steps — set it to 0 for design mode. +# +# > **Note:** on some lattices `disable_6d()` is required before measuring in design mode. + +# In[8]: + + +# Required on some lattices before measuring the TRM in design mode +sr.design.get_lattice().disable_6d() + + +def tune_callback(action: int, cb_data: dict): + if action == Action.MEASURE: + print(f"Tune response: #{cb_data['step']} {cb_data['magnet']} {cb_data['tune']}") + return True + + +# In[9]: + + +if SR.tune.response_matrix is None: + SR.trm.measure(sleep_between_step=wait_time, callback=tune_callback) + SR.trm.save(CONFIG_DIR / "trm.json") + +SR.tune.load(CONFIG_DIR / "trm.json") +print("Response matrix loaded.") +print(SR.trm) # string representation + + +# #### Correcting the tune +# +# `SR.tune.set([qx, qy])` runs the correction iteratively. The `iter` parameter controls +# the number of iterations and `wait_time` the settling time between each iteration. + +# In[10]: + + +print(f"Tune before correction: {SR.tune.readback()}") + +qx, qy = 0.19, 0.28 +print(f"\nSetting tune to [{qx}, {qy}]") +SR.tune.set([qx, qy], iter=10, wait_time=wait_time) +print(f"Tune after correction: {SR.tune.readback()}") + +qx, qy = 0.21, 0.30 +print(f"\nSetting tune to [{qx}, {qy}]") +SR.tune.set([qx, qy], iter=10, wait_time=wait_time) +print(f"Tune after correction: {SR.tune.readback()}") + +print(SR.tune) # string representation + + +# In[ ]: diff --git a/examples/use_cases/02-chromaticity_measurement.ipynb b/examples/use_cases/02-chromaticity_measurement.ipynb new file mode 100644 index 000000000..0b794824c --- /dev/null +++ b/examples/use_cases/02-chromaticity_measurement.ipynb @@ -0,0 +1,326 @@ +{ + "cells": [ + { + "cell_type": "code", + "execution_count": 12, + "id": "45d2462a", + "metadata": {}, + "outputs": [], + "source": [ + "import numpy as np\n", + "\n", + "from pyaml.accelerator import Accelerator\n", + "from pyaml.common.constants import Action" + ] + }, + { + "cell_type": "markdown", + "id": "9ba6385a", + "metadata": {}, + "source": [ + "## Facility configuration\n", + "\n", + "Edit the `CONFIG_FILE` variable below to select the facility. The rest of the notebook runs unchanged.\n", + "\n", + "| Facility | Config file | Control system | Virtual twin |\n", + "|----------|-------------|----------------|--------------|\n", + "| SOLEIL II | `config/soleil_ii/p.yaml` | TANGO (`tango-pyaml`) | Apptainer container |\n", + "| BESSY2 | `config/bessy2/bessy2.yaml` | EPICS (`pyaml-cs-oa`) | Apptainer container |\n", + "| ESRF EBS | `config/esrf/esrf.yaml` | TANGO (`tango-pyaml`) | Apptainer container |\n", + "\n", + "See `README.md` for installation and virtual accelerator startup instructions." + ] + }, + { + "cell_type": "code", + "execution_count": 13, + "id": "bca6435a", + "metadata": {}, + "outputs": [ + { + "name": "stdout", + "output_type": "stream", + "text": [ + "14 Aug 2026, 13:41:08 | WARNING | PyAML Tango control system binding (0.4.0) initialized with name 'live' and TANGO_HOST=ebs-simu-3:10000\n", + "14 Aug 2026, 13:41:10 | WARNING | /home/gubaidulin/codes/operation/pyAML/pyaml/examples/unified_examples/config/esrf/chroma_resp.json: file not found\n", + "14 Aug 2026, 13:41:10 | WARNING | Loading /home/gubaidulin/codes/operation/pyAML/pyaml/examples/unified_examples/config/esrf/orm.json failed /home/gubaidulin/codes/operation/pyAML/pyaml/examples/unified_examples/config/esrf/orm.json: file not found\n" + ] + }, + { + "data": { + "text/plain": [ + "Accelerator(facility='ESRF', machine='sr', description=None, live=TangoControlSystem(name='live', tango_host='ebs-simu-3:10000', catalog=, debug_level=None, lazy_devices=True, timeout_ms=3000), design=Simulator(name='design', lattice='/home/gubaidulin/codes/operation/pyAML/pyaml/examples/unified_examples/config/esrf/sr/lattices/ebs.mat', mat_key=None, linker=None, description=None), yellow_pages=Controls:\n", + " live\n", + " .\n", + "\n", + "Simulators:\n", + " design\n", + " .\n", + "\n", + "Arrays:\n", + " BPM (pyaml.arrays.bpm_array) size=320\n", + " HCorr (pyaml.arrays.magnet_array) size=288\n", + " VCorr (pyaml.arrays.magnet_array) size=288\n", + " Skews (pyaml.arrays.magnet_array) size=288\n", + " Sext (pyaml.arrays.magnet_array) size=180\n", + " QForTune (pyaml.arrays.magnet_array) size=124\n", + " .\n", + "\n", + "Tools:\n", + " BBA-BPM_C04-04 (pyaml.tuning_tools.bba)\n", + " BBA2-BPM_C04-04 (pyaml.tuning_tools.bba2)\n", + " CHROMATICITY_MONITOR (pyaml.tuning_tools.chromaticity_monitor)\n", + " DEFAULT_TUNE_CORRECTION (pyaml.tuning_tools.tune)\n", + " DEFAULT_TUNE_RESPONSE_MATRIX (pyaml.tuning_tools.tune_response_matrix)\n", + " DEFAULT_CHROMATICITY_RESPONSE_MATRIX (pyaml.tuning_tools.chromaticity_response_matrix)\n", + " DEFAULT_CHROMATICITY_CORRECTION (pyaml.tuning_tools.chromaticity)\n", + " DEFAULT_ORBIT_CORRECTION (pyaml.tuning_tools.orbit)\n", + " DEFAULT_ORBIT_RESPONSE_MATRIX (pyaml.tuning_tools.orbit_response_matrix)\n", + " DEFAULT_DISPERSION (pyaml.tuning_tools.dispersion)\n", + " .\n", + "\n", + "Diagnostics:\n", + " BETATRON_TUNE (pyaml.diagnostics.tune_monitor)\n", + " .)" + ] + }, + "execution_count": 13, + "metadata": {}, + "output_type": "execute_result" + } + ], + "source": [ + "# ── Facility configuration ──────────────────────────────────────────────────\n", + "# Uncomment the facility you want to use:\n", + "\n", + "# CONFIG_FILE = \"config/soleil_ii/p.yaml\"\n", + "# CONFIG_FILE = \"config/bessy2/bessy2.yaml\"\n", + "CONFIG_FILE = \"config/esrf/esrf.yaml\"\n", + "# ────────────────────────────────────────────────────────────────────────────\n", + "\n", + "sr = Accelerator.load(CONFIG_FILE)\n", + "sr # string representation" + ] + }, + { + "cell_type": "markdown", + "id": "1e562c84", + "metadata": {}, + "source": [ + "### Virtual accelerator setup\n", + "\n", + "For **live** control mode you need a running control system or emulator. If you want to skip this, run the notebook in **design** mode only.\n", + "\n", + "**SOLEIL II / ESRF (TANGO)**\n", + "```\n", + "apptainer pull virtual-accelerator.sif oras://gitlab-registry.synchrotron-soleil.fr/software-control-system/containers/apptainer/virtual-accelerator:latest\n", + "apptainer run virtual-accelerator.sif\n", + "```\n", + "\n", + "**BESSY2 (EPICS)**\n", + "```\n", + "apptainer run oras://registry.hzdr.de/digital-twins-for-accelerators/containers/pyat-softioc-digital-twin:default-v0-5-1-bessy.2711893\n", + "```\n", + "\n", + "> **Note for BESSY2 live mode:** the PV prefix in `config/bessy2/bessy2.yaml` must match your virtual accelerator instance. Edit the `prefix:` field under `controls:`." + ] + }, + { + "cell_type": "markdown", + "id": "b112b495", + "metadata": {}, + "source": [ + "### Control mode choice\n", + "\n", + "- **`sr.design`** — runs pyAT locally, no control system needed. Set `wait_time = 0.0`.\n", + "- **`sr.live`** — connects to the real machine or virtual twin. Set `wait_time` to allow readback settling (typically 1.5–2 s)." + ] + }, + { + "cell_type": "code", + "execution_count": 14, + "id": "f23b58c7", + "metadata": {}, + "outputs": [ + { + "data": { + "text/plain": [ + "Simulator(name='design', lattice='/home/gubaidulin/codes/operation/pyAML/pyaml/examples/unified_examples/config/esrf/sr/lattices/ebs.mat', mat_key=None, linker=None, description=None)" + ] + }, + "execution_count": 14, + "metadata": {}, + "output_type": "execute_result" + } + ], + "source": [ + "SR = sr.design\n", + "# SR = sr.live\n", + "\n", + "wait_time = 0.0 if SR == sr.design else 2.0\n", + "SR # string representation" + ] + }, + { + "cell_type": "markdown", + "id": "8af61b38", + "metadata": {}, + "source": [ + "### Momentum compaction factor\n", + "\n", + "The momentum compaction factor α_c is needed to convert RF frequency deviation to momentum deviation. It is computed from the lattice model (design mode)." + ] + }, + { + "cell_type": "code", + "execution_count": 15, + "id": "2154aab9", + "metadata": {}, + "outputs": [ + { + "name": "stdout", + "output_type": "stream", + "text": [ + "Momentum compaction factor: αc = 8.623615e-05\n" + ] + } + ], + "source": [ + "sr.design.get_lattice().disable_6d()\n", + "alphac = sr.design.get_lattice().get_mcf()\n", + "sr.design.get_lattice().enable_6d()\n", + "print(f\"Momentum compaction factor: αc = {alphac:.6e}\")" + ] + }, + { + "cell_type": "markdown", + "id": "5d3fc38e", + "metadata": {}, + "source": [ + "### Chromaticity measurement\n", + "\n", + "The chromaticity monitor is named `CHROMATICITY_MONITOR` in the configuration. The measurement sweeps the RF frequency and fits the resulting tune shift.\n", + "\n", + "Parameters:\n", + "- `alphac` — momentum compaction factor (from lattice above)\n", + "- `fit_order` — polynomial fit order (2 = quadratic)\n", + "- `n_step` — number of RF frequency steps\n", + "- `sleep_between_meas` / `sleep_between_step` — settling times (set to `wait_time` for live mode)\n", + "- `do_plot=True` — show the tune vs. δp fit" + ] + }, + { + "cell_type": "code", + "execution_count": 16, + "id": "d80fd338", + "metadata": {}, + "outputs": [], + "source": [ + "def chroma_callback(action: int, cb_data: dict):\n", + " if action == Action.MEASURE:\n", + " print(f\"Chromaticity: #{cb_data['step']} RF={cb_data['rf']:.2f} Hz, Tune={cb_data['tune']}\")\n", + " return True" + ] + }, + { + "cell_type": "code", + "execution_count": 17, + "id": "160e4cf7", + "metadata": {}, + "outputs": [ + { + "name": "stdout", + "output_type": "stream", + "text": [ + "Chromaticity: #0 RF=352372199.79 Hz, Tune=[0.15148296 0.33444759]\n", + "Chromaticity: #1 RF=352372184.59 Hz, Tune=[0.15569448 0.33720674]\n", + "Chromaticity: #2 RF=352372169.40 Hz, Tune=[0.15996911 0.34002636]\n", + "Chromaticity: #3 RF=352372154.21 Hz, Tune=[0.16430419 0.3429056 ]\n", + "Chromaticity: #4 RF=352372139.01 Hz, Tune=[0.16869704 0.34584364]\n" + ] + }, + { + "data": { + "image/png": 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aDiZtRJ1UXl6ecHR0FOvXrzdo++ov0ezs7AbbjRkzRjz66KON2kdZWZlwc3MTq1evNihWan2NPV903Z6oI+NABKJOys7ODi+//DLeeecdzJw5E3J58zziGhERcdd50+5m48aNMDExwezZs5soKmqrmuJ8IeqoOBCBqBNbtGgRkpOTmy1hA4CXX365wcEgupg9ezYuX75c54Sg1LE0xflC1FExaSMiIiJqB2RC3JpinIiIiIjaLF5pIyIiImoHmLQRERERtQMcPWogtVqN69evw8bGptGLVxMREVHnJYRAYWEhPDw8GhwYxqTNQNevX+dSH0RERNRkrly5gq5du9Zbz6TNQDY2NgA0v+CaC+4SERER6aOgoACenp5SblEfJm0Gqr4lamtry6SNiIiIGu1uj1sxaSMiIiKqg0otcDg9F8rCMihszBHm6wgjees9x86kjYiIiOgOO85kYPkvicjIL5PK3O3MsXRcd4zu6d4qMXHKDyIiIqIadpzJwJwtx7USNgDIzC/DnC3HseNMRqvExaSNiIiI6BaVWmD5L4moa7mo6rLlvyRCpW75BaWYtBERERHdsitZWesKW00CQEZ+GQ6n57ZcULfwmTYiIiLq1NJzihGblIWdSVk6J2PKwvoTu+bCpI2IiIg6lSqVGscv50mJWlp2sd77UNiYN0NkDWPSRkRERB1eYVkl9pzLQWxSFuJSlLhZUinVGctlCPdzRFSwKyKDFZj66UFk5pfV+VybDICbnWb6j5bGpI2IiIg6pCu5JYhNykJsshIHL9xApep2GmZnYYLIIBdEhbhiRJALbM1NpLql47pjzpbjkAFaiZusRn1rzNfGpI2IiIg6BLVa4NTVPOxMykJskhLJmYVa9b7OVogOUSAqxBUDvB1gbFT3eMzRPd2xdlq/WvO0ubXyPG1M2oiIiKjdKqmowr7UHMQmKRGbrEROUblUJ5cBA7wdEd1dk6j5u1jrvN/RPd1xb3c3rohAREREZKjM/DLEJmuupu0/n4PyKrVUZ21mjBHdXBDdXYGIbgo4WJka/D5GchkG+zs1RchNgkkbERERtWlCCJy9XoCdt0Z7nrlWoFXf1cEC0SGuiA5xRZivI0yNO+Y0tEzaiIiIqM0pq1QhIe0GdiZl1ZrwViYDQj3tpUStm6s1ZLLWu23ZUpi0ERERUZuQXViOuGQldiZlYW9qDkorVVKdhYkRhgU6I7q7KyKDFHCxMWvFSFsHkzYiIiJqFUIIpGQVIjZJk6idvJIHUWOODTdbc0SFKBDd3RWD/ZxgbmLUesG2AUzaiIiIqMVUVKlxKP2GlKhdvVmqVd+ri50mUQtxRQ8P205x21NXTNqIiIioWd0srkBcihKxSUrsOZeNwvIqqc7MWI57ApwRFaJAVLAr3Oxafnmo9oJJGxERETW5tOwi7EzUTMtx9FIu1DVuezpbmyEqWIGoEAWGBjrD0pTpiC74WyIiIqJGq1KpcfTSTU2ilqxEeo72IuzBbjaIDnFFVIgCfbraQ96Kk9S2V0zaiIiIyCAFZZXYnZKNnUlZiE/JRn7p7UXYTYxkGOTnJCVqXR0sWzHSjoFJGxEREens8o0SaZLbw+m5qKpx39PB0gSRwZpBBMMCnWFTYxF2ajwmbURERFQvlVrg5JWb2JmkRGxSFs5lFWnV+7tYIbq7ZpLbfl4Orbo2Z0fHpI2IiIi0FJdXYW9qNnYmKRGXrMSN4gqpzkguw0AfB2k1Ah9nq1aMtHMxOGmrqKhAeno6/P39YWzM3I+IiKg9u55XitikLOxMUiIh7QYqVLcXYbcxN0ZEkALRIZpF2O0seduzNeidbZWUlGDevHn4/PPPAQDnzp2Dn58f5s2bhy5duuCVV15p8iCJiIioaanVAmeu52NnoiZRS8zQXoTd28lSGkQw0McRJkYdcxH29kTvpG3x4sU4deoU4uPjMXr0aKk8Ojoay5YtY9JGRETURpVWqLD/fA5ikzXzpykLy6U6uQzo5+WAqBBX3NtdAX+XzrEIe3uid9K2bds2bN26FYMGDdI6mD169EBaWlqTBkdERESNoywoQ2yyZhDBvvM5KKu8fdvTytQIw7u5IDrEFZHBCjhambZipHQ3eidt2dnZUCgUtcqLi4uZkRMREbUyIQSSMgqxMykLsUlZOHU1X6u+i72FtLZnuJ8jzIw79yLs7YneSduAAQOwfft2zJs3DwCkRG39+vUYPHhw00ZHREREd1VepcLBC7m3lo3KwvX8Mq36Pp72iA5WILq7K4LdbHiRpZ3SO2l78803MWbMGCQmJqKqqgrvvfceEhMTceDAAezevbs5YiQiIqI73CgqR1xKNmKTsrDnXDaKK1RSnbmJHEMDXBAdosDIYAUUtlyEvSPQO2kbOnQoTp48iZUrV6JXr174448/0K9fPyQkJKBXr17NESMREVGnJ4TAeWWRNMntscs3IWoswu5qa4aRwa6IDlHgngBnmJvwtmdHIxOi5iFveWvWrME777yDzMxM9OnTBx988AHCwsLqbHv27FksWbIEx44dw6VLl7Bq1So8//zztdpdu3YNixYtwm+//YaSkhIEBARg48aNGDBgAADgiSeekKYsqTZq1Cjs2LFD57gLCgpgZ2eH/Px82Nra6t5hIiIiHVWq1DiSnoudSUrsTMrC5dwSrfoeHraa0Z4hrujhYctF2NspXXMKg2bFVavVOH/+PJRKJdRqtVbd8OHDdd7P1q1bsXDhQqxbtw7h4eFYvXo1Ro0ahZSUlDoHO5SUlMDPzw+PPvooFixYUOc+b968iXvuuQeRkZH47bff4OLigtTUVDg4OGi1Gz16NDZu3Ci9NjMz0zluIiKi5pJfUon4c0rsTFIiPkWJwrIqqc7UWI4h/k6ICnFFVLACHvYWrRgptTS9k7aDBw9i6tSpuHTpEu68SCeTyaBSqerZsrZ3330Xs2bNwsyZMwEA69atw/bt2/HZZ5/VOd/bwIEDMXDgQACodz64t956C56enloJma+vb612ZmZmcHNz0znW8vJylJffns+moKCggdZERES6S88pvrUaQRaOXLwJVY1F2J2sTDEyWIGoW4uwW5lxFaLOSu8jP3v2bGkEqbu7u8EjUCoqKnDs2DEsXrxYKpPL5YiOjkZCQoJB+wSAn3/+GaNGjcKjjz6K3bt3o0uXLnj22Wcxa9YsrXbx8fFQKBRwcHDAyJEj8e9//xtOTk717jcmJgbLly83OC4iIqJqVSo1jl/OkxK1tOxirfogVxtEhWgStVBPey7CTgAMSNpSU1Px/fffIyAgoFFvnJOTA5VKBVdXV61yV1dXJCcnG7zfCxcuYO3atVi4cCH++c9/4siRI5g/fz5MTU0xY8YMAJpbow899BB8fX2RlpaGf/7znxgzZgwSEhJgZFT3g5uLFy/GwoULpdcFBQXw9PQ0OE4iImrfVGqBw+m5UBaWQWFjjjBfxwaTq8KySuw5l4PYpCzEpShxs6RSqjOWyxDu5ygtwu7paNkSXaB2Ru+kLTw8HOfPn2900tZc1Go1BgwYgDfffBMA0LdvX5w5cwbr1q2TkrbJkydL7Xv16oXevXvD398f8fHxiIqKqnO/ZmZmfO6NiIgAADvOZGD5L4nIqDEfmrudOZaO647RPd2lsiu5JYhNykJsshIHL9xAper2bU87C5Nbtz0VGN7NBbbmXISdGqZ30jZv3jy88MILyMzMRK9evWBion2S9e7dW6f9ODs7w8jICFlZWVrlWVlZej1rdid3d3d0795dqywkJAQ//PBDvdv4+fnB2dkZ58+frzdpIyIiAjQJ25wtx3Hn1AuZ+WWYveU4Fo0OQlF5FWKTlEjOLNRq4+dshejumkEE/b0dYMxF2EkPeidtDz/8MADgySeflMpkMhmEEHoNRDA1NUX//v0RGxuLCRMmANBcJYuNjcXcuXP1DUtyzz33ICUlRavs3Llz8Pb2rnebq1ev4saNG3B3d6+3DRERkUotsPyXxFoJGwCp7K0dt7+D5DJggI8j7g1xRVSIAn4u1i0SJ3VMeidt6enpTfbmCxcuxIwZMzBgwACEhYVh9erVKC4ulkaTTp8+HV26dEFMTAwAzeCFxMRE6d/Xrl3DyZMnYW1tLd2uXbBgAYYMGYI333wTEydOxOHDh/HJJ5/gk08+AQAUFRVh+fLlePjhh+Hm5oa0tDS8/PLLCAgIwKhRo5qsb0RE1PEcTs/VuiVan0F+jpg80AsRQS6wt+Qi7NQ09E7aGrpipa9JkyYhOzsbS5YsQWZmJkJDQ7Fjxw5pcMLly5chl9++dHz9+nX07dtXev2f//wH//nPfzBixAjEx8cD0EwL8uOPP2Lx4sVYsWIFfH19sXr1ajz22GMAACMjI5w+fRqff/458vLy4OHhgfvuuw+vv/46n1kjIqI6qdUCp67mYeN+3S5cTAnzwgOhXZo5Kups9F4R4Ysvvmiwfvr06Y0KqL3gighERB1bUXkV9p7LRmyyZpLbnKIKnbf9etYgDPavfxopopp0zSn0TtruXFmgsrISJSUlMDU1haWlJXJzcw2LuJ1h0kZE1PFcvlGC2OQs7KpjtKeNuTGGB7pg3/kc5JdW1rm9DICbnTn2LRrJudVIZ822jNXNmzdrlaWmpmLOnDl46aWX9N0dERFRq5EmuU3Owq4kJVKVRVr1vs5WiApWYGSIAgN9HGFiJJdGjwLQGpBQnaItHdedCRs1iyZbMP7o0aOYNm1aoybGbU94pY2IqH3KL6nE7tRs7ErKQvy5bOTVmOTWSC5DmI8jokIUGBlc/2hPXedpI9JFsy4YX+eOjI1x/fr1ptodERFRkxBC4EJOMXYlKRGbXHttT3tLE0QGaZK04d1cYGdx90luR/d0x73d3fRaEYGosfRO2n7++Wet10IIZGRk4MMPP8Q999zTZIEREREZqqJKjaMXc7EzSYldyVm4eKNEq76bqzVGBmvmTuvraW/QJLdGchkHG1CL0jlpMzIyQkZGhjQRbjWZTAYXFxeMHDkS//d//9fU8REREekkt7gC8SlKxCYpsedcNgrLq6Q6UyM5wv0cERWsWYSda3tSe6Rz0lb96JtarW62YIiIiHQlhMC5rCLsTNKM9jx++SZqPqXtbG2KyCDN2p5DA11gbdZkTwQRtQqewURE1G6UVapw8MIN7ErWXFG7lleqVd/d3RZRIZqrab272EHOZ8yoA9EraVu/fj2srRteN23+/PmNCoiIiKgmZWEZ4m4lafvO56Ck4vYa12bGctwT4IyRwZqBBB72Fq0YKVHz0nnKD7lcjq5du8LIyKj+nclkuHDhQpMF15Zxyg8iouYhhMDZ6wWIvTWI4NTVfK16V1szjAx2RXSIAkP8nWFhWv/3ElF70CxTfhw9ehQKhaLRwREREdVUWqHC/vM5iE3WJGpZBeVa9X262iEqxBUjgxXo4WELmYy3Panz0Tlp4/8gRETUlK7nlWJXshK7kpXYfz4H5VW3B7pZmhphaIAzokNcERHsAoWNeStGStQ26D16lIiIyBBqtcCpq3nSIILEjAKt+i72FogOUWBkiCvCfR1hbsLbnkQ16Zy0LV269K6DEIiIiGoqKq/CvtRs7ExSIj5FiZyiCqlOLgP6eTlgZIgCUcGu6OZqzbs6RA1osrVHOxsORCAiqtuV3BLEJmUhNlmJgxduoFJ1+2vGxswYw4NcEBWsQESQAo5Wpq0YKVHb0OJrjxIRUedUpVLjxJU8zSS3SUqkKou06n2cLBEV4oqoYAUG+DjC1Fj/JaOIiEkbEREZIL+0ErvPZWNXUhbiz2Ujr6RSqjOSyzDQxwFRwa4YGaKAvwsfrSFqCkzaiIhIJxeyixCbpERschaOXLwJlfr2bU87CxNEBrlgZIgrRgS6wM7SpBUjJeqYmLQREVGdKlVqHEnPvTV3mhLpOcVa9YEKa2kQQT8vexgb8bYnUXPSKWnr27evziN6jh8/3qiAiIio9eQWVyA+RYnYZCX2pGSjsLxKqjMxkmGQnxNGBmsSNS8ny1aMlKjz0SlpmzBhQjOHQURErUEIgXNZRYhN1gwiOH75Jmrc9YSTlSkigxWIDlFgaKALrM14g4aotXDKDwNxyg8iaq/KKlU4lJ6LXbem5bh6s1SrPsTdFlHBCkSFKNCnqz3kcs6dRtScOOUHERFJlIVliE/Oxs6kLOw7n4OSCpVUZ2osxz3+TtLanh72Fq0YKRHVR++kTaVSYdWqVfj2229x+fJlVFRUaNXn5uY2WXBERGQYIQTOXi9AbJJmAfZTV/O16l1tzTAyWDN32pAAJ1ia8m94orZO7/9Lly9fjvXr1+OFF17Aq6++in/961+4ePEitm3bhiVLljRHjEREpIPSChX2n89BbLIScclKZBaUadX37mqHqGBXRIUo0MPDlktGEbUzej/T5u/vj/fffx/3338/bGxscPLkSans4MGD+Oqrr5or1jaFz7QRUVuQkV9662qaEvvP56C8Si3VWZgYYVigM6JCFIgMUkBha96KkRJRfZrtmbbMzEz06tULAGBtbY38fM0l97/97W947bXXDAyXiIh0oVYLnLqah13JSsQmKZGYUaBV38XeAlEhCowMVmCQnxPMTYxaKVIiamp6J21du3ZFRkYGvLy84O/vjz/++AP9+vXDkSNHYGZm1hwxEhF1akXlVdiXmo3YJCXiUpTIKbr9LLFMBvTzctDMnRaiQJCrDW97EnVQeidtDz74IGJjYxEeHo558+Zh2rRp2LBhAy5fvowFCxY0R4xERJ3OldwSxN6akuPQhVxUqG7f9rQ2M8aIbi4YGaxARJALnKz5BzNRZ9DoedoOHjyIAwcOIDAwEOPGjWuquNo8PtNGRA1RqQUOp+dCWVgGhY05wnwdYdTAfGdVKjVOXMnTrO2ZlIVUZZFWvbeTpTSIYKCPI0yNuWQUUUeha06h9//1e/bsQVXV7WVNBg0ahIULF2LMmDHYs2eP3oGuWbMGPj4+MDc3R3h4OA4fPlxv27Nnz+Lhhx+Gj48PZDIZVq9eXWe7a9euYdq0aXBycoKFhQV69eqFo0ePSvVCCCxZsgTu7u6wsLBAdHQ0UlNT9Y6diKguO85kYOhbuzDl04P4xzcnMeXTgxj61i7sOJOh1S6/tBK/nLqOBVtPYsAbO/HougSs252GVGURjOQyhPs64p9jg7Fz4QjEvxiBJeO6454AZyZsRJ2U3rdHIyMjkZGRAYVCoVWen5+PyMhIqFSqerasbevWrVi4cCHWrVuH8PBwrF69GqNGjUJKSkqt/QNASUkJ/Pz88Oijj9Z7K/bmzZu45557EBkZid9++w0uLi5ITU2Fg4OD1Obtt9/G+++/j88//xy+vr547bXXMGrUKCQmJsLcnKOriMhwO85kYM6W47jzFkZmfhnmbDmOZeO7o1IlsDMpC0cu3oSqxppRdhYmiAi6dduzmwJ2liYtGzwRtWl63x6Vy+XIysqCi4uLVvm5c+cwYMAAFBQU1LNlbeHh4Rg4cCA+/PBDAIBarYanpyfmzZuHV155pcFtfXx88Pzzz+P555/XKn/llVewf/9+7N27t87thBDw8PDACy+8gBdffBGAJuF0dXXFpk2bMHnyZJ1i5+1RIrqTSi0w9K1dyMgvu3vjWwIU1reWjHJFPy97GBvxKhpRZ9PkU3489NBDAACZTIYnnnhCa6SoSqXC6dOnMWTIEJ0DrKiowLFjx7B48WKpTC6XIzo6GgkJCTrv504///wzRo0ahUcffRS7d+9Gly5d8Oyzz2LWrFkAgPT0dGRmZiI6Olraxs7ODuHh4UhISKg3aSsvL0d5ebn0Wp/klIg6h8PpuTolbD272OGhvl0QFaKAt5NVC0RGRB2Bzn/S2dnZwc7ODkII2NjYSK/t7Ozg5uaGp59+Glu2bNH5jXNycqBSqeDq6qpV7urqiszMTN17cIcLFy5g7dq1CAwMxO+//445c+Zg/vz5+PzzzwFA2re+7xsTE6PVZ09PT4NjJKKORQiBM9fysTnhok7tZw3zxZNDfZmwEZFedL7StnHjRgCa25IvvvgirKza5oeNWq3GgAED8OabbwIA+vbtizNnzmDdunWYMWOGwftdvHgxFi5cKL0uKChg4kbUiRWXV2Hf+RzEJWvmTssqKL/7RrcobPjsLBHpT++BCEuXLm2SN3Z2doaRkRGysrK0yrOysuDm5mbwft3d3dG9e3etspCQEPzwww8AIO07KysL7u7uWu8bGhpa737NzMw4eTBRJ3fpRjF2JWuWjLpz7jQLEyPcE+CEIxdzkV9aVef2MgBudprpP4iI9KV30paVlYUXX3wRsbGxUCqVuHMcg66jR01NTdG/f3/ExsZiwoQJADRXyWJjYzF37lx9w5Lcc889SElJ0So7d+4cvL29AQC+vr5wc3NDbGyslKQVFBTg0KFDmDNnjsHvS0QdT0WVGkcv5moStRQlLmQXa9V7OVpiZLACkcEKhPs6wtzESBo9CkBrBGn1DG1Lx3VvcL42IqL66J20PfHEE7h8+TJee+01uLu7N2q5lIULF2LGjBkYMGAAwsLCsHr1ahQXF2PmzJkAgOnTp6NLly6IiYkBoBm8kJiYKP372rVrOHnyJKytrREQEAAAWLBgAYYMGYI333wTEydOxOHDh/HJJ5/gk08+AaAZSPH888/j3//+NwIDA6UpPzw8PKTkkYg6r+zCcsSnaG557j2Xg8Ly21fNjOUyDPDRLBk1MtgV/i5WtT4DR/d0x9pp/bD8l0StQQluduZYOq47Rvd0BxGRIfSe8sPGxgZ79+5t8FaiPj788EO88847yMzMRGhoKN5//32Eh4cDACIiIuDj44NNmzYBAC5evAhfX99a+xgxYgTi4+Ol1//73/+wePFipKamwtfXFwsXLpRGjwKah4aXLl2KTz75BHl5eRg6dCg++ugjdOvWTee4OeUHUcegVgucvV4gXU07fTUPNT8VnaxMMSLIBVHBrhjWzRm25rrNnabvighE1HnpmlPonbR1794dX375Jfr27dvoINszJm1E7ZdmAfYc7ErOQlxKNrILtQcR9Oxii5FBmtuefbraQ85ki4iaUZPP01Zt9erVeOWVV/Dxxx/Dx8enMTESEbWYiznFiE1WIi5ZiUPpN1Cpuv33qqWpEYYGOEvPp7nacnQnEbU9eidtkyZNQklJCfz9/WFpaQkTE+1bBbm5uU0WHBGRoSqq1DhyaxBBXLISF3K0BxF4O1neejZNgTBfR5gZG7VSpEREujHoShsRUVukLCxDfEo2diUpse98DoruGEQQ5usoXU3zc649iICIqC3TO2lrzAS1RERNSa0W+OtavuZqWooSp6/ma9U7W5siIkhzNW1ooO6DCIiI2iK9kzZAMxfbtm3bkJSUBADo0aMHxo8fDyMj3l4gouZVWFZ5axCBEnEp2cgp0h5E0KuLHSKDFYgKVqBXFzsOIiCiDkPvpO38+fMYO3Ysrl27hqCgIACadTk9PT2xfft2+Pv7N3mQRNS5XcguklYiOHIxV2sQgZWpEYYFumBksAIRQS5QcBABEXVQek/5MXbsWAgh8OWXX8LRUbMUy40bNzBt2jTI5XJs3769WQJtazjlB1HzqahS43B6LmKTsxCXrMTFGyVa9b7OVoi8ddtzoK8DBxEQUbvWbFN+7N69GwcPHpQSNgBwcnLCypUrcc899xgWLRF1esqCMsSlaK6m7UvNQXHF7SXxTIw0gwiqEzU/F+tWjJSIqHXonbSZmZmhsLCwVnlRURFMTU2bJCgi6vjUaoHT1YMIkpX469qdgwjMMDJYc9vzngBn2HAQARF1cnonbX/729/w9NNPY8OGDQgLCwMAHDp0CLNnz8b48eObPEAi6jgKbg0iiE1SYvc5JXKKKrTq+3TVDCIYGaxATw8OIiAiqknvpO3999/HjBkzMHjwYGli3aqqKowfP55zuBGRFiEE0rKLEVdjEEGV+vZjtNZmxhgW6IzI6kEENhxEQERUH72TNnt7e/z00084f/68NOVHSEgIAgICmjw4Imp/yqtUOHQhV5o77dIdgwj8nK2klQgG+DjC1FjeSpESEbUveidte/bsQXBwMAICArQStcrKSiQkJGD48OFNGiARtX1ZBWWIS1YiNlmJ/edzUFJjEIGpkRzhfrcHEfg4W7VipERE7ZfeSVtERARcXV3x448/YtCgQVJ5bm4uIiMjoVKpGtiaiDoClVrg1NU86bbn2esFWvUKGzNEBmmWixoa6AxrM4Pm8SYiohoM+iSdPHkyoqKisGbNGjzxxBNSuZ5TvhFRO5JfWom9qdnYlazE7pRs3Ci+PYhAJgN6d7VH1K3bnt3dbTmIgIioiemdtMlkMixevBjDhg3D9OnTcfr0afzf//2fVEdEHYNmEMHtlQiOXrypNYjAxswYw7u5SIMInK3NWjFaIqKOT++krfpq2kMPPQRfX1888MADSExMxHvvvdfkwRFRyyqrVOFQei52JWVhV4oSV3JLter9XTSDCCKDFRjo4wgTIw4iICJqKY160KRv3744fPgwJkyYgKioqKaKiYhaUGZ+mXQ1bf/5HJRW1h5EoLnt6QovJ8tWjJSIqHPTO2mbMWMGLCwspNdubm7YvXs3nn76aezZs6dJgyOipqdSC5y8kieN9kzK0B5E4GprprmaFqRZicCKgwiIiNoEvReMJw0uGE/tSX5JJXanZiMuWYnd57KRe8cgglBPe4y8Ndqzh4ctn08lImpBTbpg/OnTp9GzZ0/I5XKcPn26wba9e/fWL1IianJCCKQqbw8iOHbpJlQ1BxGYawYRRAUrMKKbC5w4iICIqM3TKWkLDQ1FZmYmFAoFQkNDIZPJtKb3qH4tk8k4TxtRKymrVCHhwg1p7rSrN7UHEQQorBF1axBBf28HDiIgImpndEra0tPT4eLiIv2biNqG63mliEtRYleSEvvTclBWqZbqTI3lGOznJC0Z5enIQQRERO2ZTkmbt7c3AM1SVcuXL8drr70GX1/fZg2MiGrTDCK4idgkzdW05MxCrXo3W3NEBisQFazAkAAnWJpyEAERUUeh1ye6iYkJfvjhB7z22mvNFQ9Rp6BSCxxOz4WysAwKG3OE+TrCqJ4VBPJKKrD73O1BBDdLKqU6mQzo62mPqBBXRAYpEOJuw0EEREQdlN5/hk+YMAHbtm3DggULmiMeog5vx5kMLP8lERn5ZVKZu505lo7rjtE93SGEwLms6kEEWTh26SZqjCGArbkxRgQpMDLYBSO6KeBoZdoKvSAiopamd9IWGBiIFStWYP/+/ejfvz+srKy06ufPn99kwRF1NDvOZGDOluO4c56djPwyzN5yHMO7OSNNWYxredqDCLq5WiMyWIGRQZpBBMYcREBE1OnoPU9bQ8+yyWQyXLhwodFBtQecp430pVILDH1rl9YVtvqYGcsx2N8JUcEKRARxEAERUUfWpPO01cTRo0SGOZCWo1PC9tJ9QXhyqC8sTI1aICoiImovGjW0rPoiHR98JqqbsqAM8eeyEZ+iGe2pi66OFkzYiIioFoOSti+++ALvvPMOUlNTAQDdunXDSy+9hMcff7xJgyNqb1RqgVNX8xCfrMSuFCXOXCu4+0Z3UNiYN0NkRETU3un9NPO7776LOXPmYOzYsfj222/x7bffYvTo0Zg9ezZWrVplUBBr1qyBj48PzM3NER4ejsOHD9fb9uzZs3j44Yfh4+MDmUyG1atX12qzbNkyyGQyrZ/g4GCtNhEREbXazJ4926D4qXO7WVyBn05ew/PfnMCAf/+Jhz46gPd3nZcStt5d7fCPqED8d84QuNmaob7r0jJoRpGG+Tq2WOxERNR+6H2l7YMPPsDatWsxffp0qWz8+PHo0aMHli1bpvdUIFu3bsXChQuxbt06hIeHY/Xq1Rg1ahRSUlKgUChqtS8pKYGfnx8effTRBt+rR48e2Llzp/Ta2Lh2V2fNmoUVK1ZIry0t+bA33Z0QAmevFyA+RYm4lGycuKw9JUf1up6RQZp1PV1sbq/ruWx8D8zZchwyQGsEaXUit3Rc93rnayMios5N76QtIyMDQ4YMqVU+ZMgQZGRk6B3Au+++i1mzZmHmzJkAgHXr1mH79u347LPP8Morr9RqP3DgQAwcOBAA6qyvZmxsDDc3twbf29LS8q5tiACgoKwS+1NzEJeiRHxKNpSF5Vr1wW42iAjSLBfVz8u+3ik5Rvd0x9pp/WrN0+ZWY542IiKiuuidtAUEBODbb7/FP//5T63yrVu3IjAwUK99VVRU4NixY1i8eLFUJpfLER0djYSEBH1D05KamgoPDw+Ym5tj8ODBiImJgZeXl1abL7/8Elu2bIGbmxvGjRuH1157rd6rbeXl5Sgvv/1FXVCg/7NK1H4IIXBeWaRZ1zNZiaMXb6KqxuU0S1Mj3BPgjMggBSKCXOBhb6Hzvkf3dMe93d10XhGBiIgIMCBpW758OSZNmoQ9e/bgnnvuAQDs378fsbGx+Pbbb/XaV05ODlQqFVxdXbXKXV1dkZycrG9okvDwcGzatAlBQUHIyMjA8uXLMWzYMJw5cwY2NjYAgKlTp8Lb2xseHh44ffo0Fi1ahJSUFPz3v/+tc58xMTFYvny5wTFR21dSUYWEtBuIS1EiLjm71gS3fs5W0tW0gb4OMDM2fISnkVyGwf5OjQ2ZiIg6Eb2TtocffhiHDh3CqlWrsG3bNgBASEgIDh8+jL59+zZ1fAYZM2aM9O/evXsjPDwc3t7e+Pbbb/HUU08BAJ5++mmpTa9eveDu7o6oqCikpaXB39+/1j4XL16MhQsXSq8LCgrg6enZjL2glnDpRjHikpXYlZKNgxduoKJKLdWZGssx2M8JkUEuiAhSwMfZqoE9ERERNS+Dpvzo378/tmzZ0ug3d3Z2hpGREbKysrTKs7KymvRZM3t7e3Tr1g3nz5+vt014eDgA4Pz583UmbWZmZjAzM6tVTu1LeZUKh9NzEZesmTvtQk6xVn0XewtEBrtgZLACg/2cOV8aERG1GTonbbo+w6XPkk6mpqbo378/YmNjMWHCBACAWq1GbGws5s6dq/N+7qaoqAhpaWkNziN38uRJAIC7Ox8E72iu55VKtzwPpOWgpEIl1RnLZRjo44jIYM1ozwCFNSeLJiKiNknnpM3e3r7BLzMhBGQyGVQqVb1t6rJw4ULMmDEDAwYMQFhYGFavXo3i4mJpNOn06dPRpUsXxMTEANAMXkhMTJT+fe3aNZw8eRLW1tYICAgAALz44osYN24cvL29cf36dSxduhRGRkaYMmUKACAtLQ1fffUVxo4dCycnJ5w+fRoLFizA8OHD0bt3b73ip7anUqXG8Us3EZeiuZqWnFmoVe9iY4bIIM3VtHsCnGFjbtJKkRIREelO56QtLi5O+rcQAmPHjsX69evRpUuXRgUwadIkZGdnY8mSJcjMzERoaCh27NghDU64fPky5PLb0ydcv35d69m5//znP/jPf/6DESNGID4+HgBw9epVTJkyBTdu3ICLiwuGDh2KgwcPwsXFBYDmCt/OnTulBNHT0xMPP/wwXn311Ub1hVpPdmE5dp/LRlyKEnvOZaOwrEqqk8uAvl4O0rNpPTxseTWNiIjaHZmoXkBUTzY2Njh16hT8/PyaOqZ2oaCgAHZ2dsjPz9frljA1DZVa4PTVPOlq2umr+Vr1DpYmiLg1HcfwQBc4WJm2UqREREQN0zWnaNSC8UQtKa+kAntScxCfrET8uWzkFldo1ffqYqe5mhasQJ+u9pz3jIiIOhQmbdRmCSGQmFGA+JRsxCUrcfzO5aLMNMtFRQS5YESQCxdaJyKiDq1RSRufC6KmVlRehX2pObfW9VQiq0B7uaggVxtE3Brp2d/bASb1LBdFRETU0eictD300ENar8vKyjB79mxYWWlPOFrfigJEdRFCIC27CHHJmkEERy7molJ1+3KahYkR7glwQkSQApHBCnTRY7koIiKijkTnpM3Ozk7r9bRp05o8GOocSitUOHjhBnYla66mXb2pvVyUr7MVIoI0V9PCfB1hbsIJbomIiHRO2jZu3NiccVAHd/lGiWaC2xQlEtJuoLzmclFGcoT7OWJksAIRQQr4crkoIiKiWjgQgZpFRZUaRy7mIu7W1bS0bO3lojzszBEZrEBkkAJDApxgacpTkYiIqCH8pqQmk5FfKo303H8+B8U1losyksswwNsBI4M1z6YFcrkoIiIivTBpI4NVqdQ4cSXv1tW0bCRlaK9P62ytWS4qMliBoYHOsOVyUURERAZj0kZ6ySkqx+6U28tFFdRYLkomA0I97THy1kjP7u62kHOCWyIioibBpI0apFYL/HUtXzOIIFmJ09fyUXPhM3tLE4zophnpObybCxy5XBQREVGzYNJGteSXVGJPquZq2u6UbNy4Y7monl1sERmkGekZ6snlooiIiFoCkzaCEALJmYXS1bTjl/OgqrFelLWZMYYFOiMySIERQS5wteVyUURERC2NSVsnVVRehf3nby0XlZyNzIIyrfpAhbU0b1p/bweYGnO5KCIiotbEpK2TEELgQk4x4pKViE/JxqH0G1rLRZmbyHGPvzMighWI6OYCT0fLVoyWiIiI7sSkrQMrq1Qh4cINxN+akuNybolWvZejpTRvWjiXiyIiImrTmLR1MFdySzS3PFOycSAtB2WVtZeLighSIDLIBb7OVpzgloiIqJ1g0tYGqdQCh9NzoSwsg8LGHGG+jvWO0KyoUuPoxdxb63pm47yySKveveZyUf5OsDLjISciImqP+A3exuw4k4HlvyQiI//2wAB3O3MsHdcdo3u6AwCyCsqkAQT7zuegqPz2BLdGchn6ezsgMkiByGAXBLna8GoaERFRB8CkrQ3ZcSYDc7Ych7ijPCO/DLO3HMfonq64fKMUibWWizK9dctTs1yUnQWXiyIiIupomLS1ESq1wPJfEmslbDXtOJMFQLNcVJ+u9tLVtJ4edlwuioiIqINj0tZGHE7P1bolWp9nI/zx1FBfOFmbtUBURERE1FZwxtQ2Qll494QNAILcbJiwERERdUJM2toIhY1uS0Pp2o6IiIg6FiZtbUSYryPc7cxR35NpMmhGkYb5OrZkWERERNRGMGlrI4zkMiwd1x0AaiVu1a+Xjute73xtRERE1LExaWtDRvd0x9pp/eBmp30L1M3OHGun9ZPmaSMiIqLOh6NH25jRPd1xb3c3nVdEICIios6BSZuBhNDMqFZQUHCXlobp4WKCHi6aSXKLiwqb5T2IiIio9VXnEtW5RX2YtBmosFCTSHl6erZyJERERNQRFBYWws7Ort56mbhbWkd1UqvVuH79Omxsmmdtz4KCAnh6euLKlSuwtbVt8v23RZ2tz52tv0Dn63Nn6y/Q+frc2foLdL4+t0R/hRAoLCyEh4cH5PL6hxvwSpuB5HI5unbt2uzvY2tr2yn+p6ips/W5s/UX6Hx97mz9BTpfnztbf4HO1+fm7m9DV9iqcfQoERERUTvApI2IiIioHWDS1kaZmZlh6dKlMDPrPOuMdrY+d7b+Ap2vz52tv0Dn63Nn6y/Q+frclvrLgQhERERE7QCvtBERERG1A0zaiIiIiNoBJm1ERERE7QCTNiIiIqJ2gEkbERERUTvApK2F5Obm4rHHHoOtrS3s7e3x1FNPoaioqMFtPvnkE0RERMDW1hYymQx5eXkG7ff06dMYNmwYzM3N4enpibfffrspu1YvQ/pcVlaG5557Dk5OTrC2tsbDDz+MrKwsqX7Tpk2QyWR1/iiVSgBAfHx8nfWZmZntrr8A6uzLN998o9UmPj4e/fr1g5mZGQICArBp06am7l6dmqPPp06dwpQpU+Dp6QkLCwuEhITgvffe09pHSx3jNWvWwMfHB+bm5ggPD8fhw4cbbP/dd98hODgY5ubm6NWrF3799VeteiEElixZAnd3d1hYWCA6OhqpqalabQz5nTalpuxzZWUlFi1ahF69esHKygoeHh6YPn06rl+/rrUPHx+fWsdy5cqVzdK/OzX1MX7iiSdq9WX06NFabTrSMQbq/oySyWR45513pDbt5RifPXsWDz/8sBTv6tWrDdqnLp/tBhHUIkaPHi369OkjDh48KPbu3SsCAgLElClTGtxm1apVIiYmRsTExAgA4ubNm3rvNz8/X7i6uorHHntMnDlzRnz99dfCwsJCfPzxx03dRb1jq8vs2bOFp6eniI2NFUePHhWDBg0SQ4YMkepLSkpERkaG1s+oUaPEiBEjpDZxcXECgEhJSdFqp1KpmqurQojm6a8QQgAQGzdu1OpLaWmpVH/hwgVhaWkpFi5cKBITE8UHH3wgjIyMxI4dO5qlnzU1R583bNgg5s+fL+Lj40VaWprYvHmzsLCwEB988IHUpiWO8TfffCNMTU3FZ599Js6ePStmzZol7O3tRVZWVp3t9+/fL4yMjMTbb78tEhMTxauvvipMTEzEX3/9JbVZuXKlsLOzE9u2bROnTp0S48ePF76+vlrH05DfaVNp6j7n5eWJ6OhosXXrVpGcnCwSEhJEWFiY6N+/v9Z+vL29xYoVK7SOZVFRUbvrrxBCzJgxQ4wePVqrL7m5uVr76UjHWAhR6zP5s88+EzKZTKSlpUlt2ssxPnz4sHjxxRfF119/Ldzc3MSqVasM2qcun+2GYNLWAhITEwUAceTIEanst99+EzKZTFy7du2u21d/Qd2ZtOmy348++kg4ODiI8vJyqc2iRYtEUFBQI3vVMEP6nJeXJ0xMTMR3330nlSUlJQkAIiEhoc5tlEqlMDExEV988YVUVt/vqzk1Z38BiB9//LHe93755ZdFjx49tMomTZokRo0aZWBvdNNSx1gIIZ599lkRGRkpvW6JYxwWFiaee+456bVKpRIeHh4iJiamzvYTJ04U999/v1ZZeHi4eOaZZ4QQQqjVauHm5ibeeecdqT4vL0+YmZmJr7/+WgjR+M+KxmrqPtfl8OHDAoC4dOmSVObt7V3nl2Nza47+zpgxQzzwwAP1vmdnOMYPPPCAGDlypFZZeznGNdUX8932aejnnC54e7QFJCQkwN7eHgMGDJDKoqOjIZfLcejQoWbdb0JCAoYPHw5TU1OpzahRo5CSkoKbN28a/N5NEdudjh07hsrKSkRHR0tlwcHB8PLyQkJCQp3bfPHFF7C0tMQjjzxSqy40NBTu7u649957sX///kb2qGHN3d/nnnsOzs7OCAsLw2effQZRY07shIQErX0AmmNc3++sqbTUMQaA/Px8ODo61ipvrmNcUVGBY8eOacUpl8sRHR1db5x3Ow7p6enIzMzUamNnZ4fw8HCpTXN9VuiiOfpcl/z8fMhkMtjb22uVr1y5Ek5OTujbty/eeecdVFVVGd4ZHTRnf+Pj46FQKBAUFIQ5c+bgxo0bWvvoyMc4KysL27dvx1NPPVWrrj0c46bYp6Gfc7owbtTWpJPMzEwoFAqtMmNjYzg6OjbqGRxd9puZmQlfX1+tNq6urlKdg4ODwe/f2Njq2sbU1LTWh7mrq2u922zYsAFTp06FhYWFVObu7o5169ZhwIABKC8vx/r16xEREYFDhw6hX79+jetYPZqzvytWrMDIkSNhaWmJP/74A88++yyKioowf/58aT/Vx7TmPgoKClBaWqr1u2lKLXWMDxw4gK1bt2L79u1SWXMf45ycHKhUqjp/r8nJyXVuU99xqPn/YnVZQ22a47NCF83R5zuVlZVh0aJFmDJlCmxtbaXy+fPno1+/fnB0dMSBAwewePFiZGRk4N13321kr+rXXP0dPXo0HnroIfj6+iItLQ3//Oc/MWbMGCQkJMDIyKjDH+PPP/8cNjY2eOihh7TK28sxbop9GvI5pysmbY3wyiuv4K233mqwTVJSUgtF0zLaUp8TEhKQlJSEzZs3a5UHBQUhKChIej1kyBCkpaVh1apVtdreTVvo72uvvSb9u2/fviguLsY777wjJW1NrS30udqZM2fwwAMPYOnSpbjvvvuk8qY8xtQyKisrMXHiRAghsHbtWq26hQsXSv/u3bs3TE1N8cwzzyAmJqZNrPeoj8mTJ0v/7tWrF3r37g1/f3/Ex8cjKiqqFSNrGZ999hkee+wxmJuba5V3pGPcmpi0NcILL7yAJ554osE2fn5+cHNzk0Y2VquqqkJubi7c3NwMfn9d9uvm5lZrxEr1a0Peuzn77ObmhoqKCuTl5Wn9hZKVlVXnNuvXr0doaCj69+9/17jDwsKwb9++u7a7U1vqb7Xw8HC8/vrrKC8vh5mZWb3H2NbW1qCrbG2lz4mJiYiKisLTTz+NV1999a5xG3qM6+Ls7AwjI6M6f68N9a2h9tX/zcrKgru7u1ab0NBQqU1zfFboojn6XK06Ybt06RJ27dqldZWtLuHh4aiqqsLFixe1kvOm1Jz9rcnPzw/Ozs44f/48oqKiOuwxBoC9e/ciJSUFW7duvWssbfUYN8U+Df1s10mjnogjnVQ/eHr06FGp7Pfff2+ygQgN7bd6IEJFRYXUZvHixS02EEGfPlc/vPn9999LZcnJyXU+vFlYWCisra21RhQ2JDo6Wjz44IMG9EQ3zd3fmv79738LBwcH6fXLL78sevbsqdVmypQpLTYQoTn6fObMGaFQKMRLL72kczxNfYzDwsLE3LlzpdcqlUp06dKlwQe2//a3v2mVDR48uNZAhP/85z9SfX5+fp0DEQz9rGispu6zEEJUVFSICRMmiB49egilUqlTHFu2bBFyubzWqMum1hz9vdOVK1eETCYTP/30kxCiYx7jajNmzKg1Mrg+bfUY19TQQISG9mnoZ7sumLS1kNGjR4u+ffuKQ4cOiX379onAwECtId5Xr14VQUFB4tChQ1JZRkaGOHHihPj0008FALFnzx5x4sQJcePGDZ33m5eXJ1xdXcXjjz8uzpw5I7755hthaWnZYlN+6Nvn2bNnCy8vL7Fr1y5x9OhRMXjwYDF48OBa+16/fr0wNzevc/TgqlWrxLZt20Rqaqr466+/xD/+8Q8hl8vFzp07m6Wf1Zqjvz///LP49NNPxV9//SVSU1PFRx99JCwtLcWSJUukNtVTfrz00ksiKSlJrFmzpkWn/GjqPv/111/CxcVFTJs2TWt6gJpf+C1xjL/55hthZmYmNm3aJBITE8XTTz8t7O3tRWZmphBCiMcff1y88sorUvv9+/cLY2Nj8Z///EckJSWJpUuX1jnlh729vfjpp5/E6dOnxQMPPFDnlB8N/U6bU1P3uaKiQowfP1507dpVnDx5Uut4Vo9oP3DggFi1apU4efKkSEtLE1u2bBEuLi5i+vTp7a6/hYWF4sUXXxQJCQkiPT1d7Ny5U/Tr108EBgaKsrIyaT8d6RhXy8/PF5aWlmLt2rW13rM9HePy8nJx4sQJceLECeHu7i5efPFFceLECZGamqrzPoXQ/btMX0zaWsiNGzfElClThLW1tbC1tRUzZ84UhYWFUn16eroAIOLi4qSypUuXCgC1fjZu3KjzfoUQ4tSpU2Lo0KHCzMxMdOnSRaxcubK5u6tTbHX1ubS0VDz77LPCwcFBWFpaigcffFBkZGTU2vfgwYPF1KlT63zft956S/j7+wtzc3Ph6OgoIiIixK5du5q8f3dqjv7+9ttvIjQ0VFhbWwsrKyvRp08fsW7dulrzkcXFxYnQ0FBhamoq/Pz8tM6R5tQcfa7vvPf29pbatNQx/uCDD4SXl5cwNTUVYWFh4uDBg1LdiBEjxIwZM7Taf/vtt6Jbt27C1NRU9OjRQ2zfvl2rXq1Wi9dee024uroKMzMzERUVJVJSUrTa6PL/dHNqyj5XH/+6fqrPiWPHjonw8HBhZ2cnzM3NRUhIiHjzzTe1kpzm1JT9LSkpEffdd59wcXERJiYmwtvbW8yaNUvry1yIjnWMq3388cfCwsJC5OXl1aprT8e4vnO25lygd9unELp/l+lLJkSNuQOIiIiIqE3iPG1ERERE7QCTNiIiIqJ2gEkbERERUTvApI2IiIioHWDSRkRERNQOMGkjIiIiageYtBERERG1A0zaiIiIiNoBJm1ERERE7QCTNiIiIqJ2gEkbERERUTvApI2IiIioHWDSRkRERNQOMGkjIiIiageYtBERERG1A0zaiIiIiNoBJm1ERERE7QCTNiIiIqJ2gEkbEbVb5eXlePLJJ+Hl5QVbW1sMGjQICQkJrR0WEVGzYNJGRO1WVVUVfHx8sG/fPuTl5eH555/HuHHjUFRU1NqhERE1OSZtRJ3Y22+/jeDgYKjV6ru2XbZsGWQyWQtEVdu6devg5eWF8vJyrXIrKyssWbIEXl5ekMvlmDx5MkxNTZGSktIqcdJtrXm+EHVUTNqoXSkqKsLSpUsxevRoODo6QiaTYdOmTQa3q3bs2DGMHj0atra2sLGxwX333YeTJ0/eNZ4jR45g7ty56NGjB6ysrODl5YWJEyfi3LlzWu3i4+Mhk8nq/Dl48KDBsRw/fhzjx4+Ho6MjLC0t0bNnT7z//vt3jRsACgoK8NZbb2HRokWQy1vmo0CtVsPFxQVvv/22Xts98cQTqKiowMcff9xgu9TUVOTm5iIgIKAxYepFn2PbEF2Ppa7nR2pqKiZPnoyuXbvC0tISwcHBWLFiBUpKSrTa6XoOtwZDz5eWUF5ejkWLFsHDwwMWFhYIDw/Hn3/+qdO2Z8+exaOPPgo/Pz9YWlrC2dkZw4cPxy+//HLXbd944w3IZDL07NmzUTE1Jn5qPcatHQCRPnJycrBixQp4eXmhT58+iI+Pb1Q7QPNlOXToUHh6emLp0qVQq9X46KOPMGLECBw+fBhBQUH1bvvWW29h//79ePTRR9G7d29kZmbiww8/RL9+/XDw4MFaH6zz58/HwIEDtcpqJhj6xPLHH39g3Lhx6Nu3L1577TVYW1sjLS0NV69ebeA3eNtnn32GqqoqTJkyRaf2TeHw4cPIycnB/fffr9d25ubmmDFjBt59913Mmzevzis4paWlmDZtGhYvXgw7O7umCllndzu2DdH1WOp6fly5cgVhYWGws7PD3Llz4ejoiISEBCxduhTHjh3DTz/9JO1T33O4JRl6vrSEJ554At9//z2ef/55BAYGYtOmTRg7dizi4uIwdOjQBre9dOkSCgsLMWPGDHh4eKCkpAQ//PADxo8fj48//hhPP/10ndtdvXoVb775JqysrBodU2Pip1YkiNqRsrIykZGRIYQQ4siRIwKA2Lhxo8HthBBi7NixwsHBQeTk5Ehl169fF9bW1uKhhx5qMJ79+/eL8vJyrbJz584JMzMz8dhjj0llcXFxAoD47rvvGtyfrrHk5+cLV1dX8eCDDwqVStXgPuvTu3dvMW3aNJ3bL126VDT2I+O1114T3t7eBm179OhRAUDExsbWqquoqBD333+/mDp1qlCr1Qbtf8SIEWLGjBl6b6frsa2PPsdS1/PjjTfeEADEmTNntLafPn26ACByc3OlMl3PYX219vmiC0OP+aFDhwQA8c4770hlpaWlwt/fXwwePNigWKqqqkSfPn1EUFBQvW0mTZokRo4cKUaMGCF69OhhcEzNET+1DN4epXbFzMwMbm5uTdYOAPbu3Yvo6Gg4OTlJZe7u7hgxYgT+97//NfhQ+5AhQ2BqaqpVFhgYiB49eiApKanObQoLC1FVVdWoWL766itkZWXhjTfegFwuR3FxsU7PpVVLT0/H6dOnER0dXWf9vn37MHDgQJibm8Pf37/O25LVzywlJydj4sSJsLW1hZOTE/7xj3+grKyszv1u375d66qJPvvo378/HB0dta4SAZpbaI8//jhkMhk+//zzVn2OqqFjWx99jqWu50dBQQEAwNXVVWt7d3d3yOVyrXPWkHP4Ti1xvhiyfXP5/vvvYWRkpHVFzNzcHE899RQSEhJw5coVvfdpZGQET09P5OXl1Vm/Z88efP/991i9enWjY2qO+KllMGmjTq+8vBwWFha1yi0tLVFRUYEzZ87otT8hBLKysuDs7FyrbubMmbC1tYW5uTkiIyNx9OhRg2LZuXMnbG1tce3aNQQFBcHa2hq2traYM2eOTl9gBw4cAAD069evVt1ff/2F++67D0qlEsuWLcPMmTOxdOlS/Pjjj3Xua+LEiSgrK0NMTAzGjh2L999/v87bO5mZmThx4gTGjh1r8D769euH/fv3a5U988wzyMjIwHfffQdj49Z74uNux7Y++hxLXc+PiIgIAMBTTz2FkydP4sqVK9i6dSvWrl2L+fPn13t7rVpD5/CdWvp80XX75nTixAl069YNtra2WuVhYWEAoNPzsABQXFyMnJwcpKWlYdWqVfjtt98QFRVVq51KpcK8efPw97//Hb169Wp0TE0VP7WC1r7UR2Sou9321LVdr169RLdu3URVVZVUVl5eLry8vAQA8f333+sV1+bNmwUAsWHDBqls//794uGHHxYbNmwQP/30k4iJiRFOTk7C3NxcHD9+XO9YevfuLSwtLYWlpaWYN2+e+OGHH8S8efMEADF58uS7xvjqq68KAKKwsLBW3YQJE4S5ubm4dOmSVJaYmCiMjIy0bndV3/4aP3681vbPPvusACBOnTqlVb5hwwZhYWEhSkpKDN7H008/LSwsLKTXFy9eFACEubm5sLKykn727Nlz19/BnQy9Vabrsa2PPsdSn3P19ddfFxYWFgKA9POvf/1Lpz7VdQ7Xp6XOF32314Whx7xHjx5i5MiRtcrPnj0rAIh169bptJ9nnnlGOjZyuVw88sgjWreuq3344YfCzs5OKJVKKe47b4/qE1NTxU8tj0kbtVtNlbStXbtWABAzZswQZ8+eFX/99ZeYNGmSMDExEQDE5s2bdY4pKSlJ2NraisGDB2t9sdYlNTVVWFhYiFGjRukdi5+fnwAgZs+erbXP6i+Bc+fONfjec+bMEcbGxrXKq6qqhIWFRZ2J39ixY+v8Ev79999r/Q4AiJiYGK3yhx9+WIwdO1arTN99LFq0SAAQxcXFDfbvbioqKkR2drbWz5AhQ8TkyZNrlRvyzGBdx7Y++hxLfc7VzZs3i1GjRolPPvlE/PDDD+LJJ58UMplMfPDBBw3Go8853JLni77b36kpj7mfn58YM2ZMrfK0tDQBQKxatarB7WvG/ueff4rPP/9c3H///eLBBx8UmZmZWm1ycnKEo6Oj+M9//iOV1ZW06RNTU8VPLY+3R6nTmz17Nv75z3/iq6++Qo8ePdCrVy+kpaXh5ZdfBgBYW1vrtJ/MzEzcf//9sLOzk54ZaUhAQAAeeOABxMXFQaVS6RVL9S2yO0d+Tp06FQAMXhUgOzsbpaWlCAwMrFVX3yjaO9v6+/tDLpfj4sWLUlllZSX+/PPPekcB6rIPQHPbDkCjn1vbv38/XFxctH4OHDiAb775plb55cuX9d5/Xce2PvocS13Pj2+++QZPP/001q9fj1mzZuGhhx7Chg0bMGPGDCxatAg3btyoMxZ9z+HWOF90PVfu1JTH3MLCotacgQCk29l13cKuS3BwMKKjozF9+nTpmcRx48ZJ5zkAvPrqq3B0dMS8efOaLKamip9aHpM2ImjmPsrKysLevXtx+vRpHDlyRHoYvFu3bnfdPj8/H2PGjEFeXh527NgBDw8Pnd7X09MTFRUVKC4u1iuW6v3f+aC5QqEAANy8ebPB93VyckJVVRUKCwt1ilMfdSVU+/btQ0FBQZ3Ps+m6D0DTL0tLy0Z/qfTp0wd//vmn1k/v3r1x33331SrXdUDLneo6tnXR91jqcn589NFH6Nu3L7p27aq17fjx41FSUoITJ07UisPQc7ixGnu+6JrAN+Uxd3d3R0ZGRq3y6jJDf3ePPPIIjhw5Is2Rl5qaik8++QTz58/H9evXcfHiRVy8eBFlZWWorKzExYsXkZubq3dMzRU/NT/O00Z0i4ODg9b8RDt37kTXrl0RHBzc4HZlZWUYN24czp07h507d6J79+46v+eFCxdgbm5e62re3WLp378//vzzT+nh9WrXr18HALi4uDT4vtX7SU9PR+/evaVyFxcXWFhYIDU1tdY29a0ykJqaCl9fX+n1+fPnoVar4ePjI5Vt374d3bt31yrTdx/V8YaEhDTYN104ODjUGjnr4OAAd3f3ekfU6qu+Y3snQ47l3c6PrKwsODg41NqusrISAGqNcDX0HG6N80XXc+VOTXnMQ0NDERcXh4KCAq2H+Q8dOiTVG6K0tBSAJoEGgGvXrkGtVmP+/PmYP39+rfa+vr74xz/+gdWrV+sVU3PFT82PV9qI6rB161YcOXIEzz//vLRaQElJCZKTk5GTkyO1U6lUmDRpEhISEvDdd99h8ODBde4vOzu7VtmpU6fw888/47777mtwRYK6Ypk4cSIAYMOGDVpt169fD2NjY2n0YH2q47xzhKORkRFGjRqFbdu2ad0iSkpKwu+//17nvtasWaP1+oMPPgAAjBkzRir79ddfG5wgVZd9AJrJZYcMGVLvflqDPse2rnOosceyrvOjW7duOHHiRK1VDb7++mvI5XKtRF3Xc7gurXG+6HquNKdHHnkEKpUKn3zyiVRWXl6OjRs3Ijw8HJ6enlJ5XcdcqVTW2mdlZSW++OILWFhYSElzz5498eOPP9b66dGjB7y8vPDjjz/iqaee0jsmfdpS28IrbdTufPjhh8jLy5OuRPzyyy/SzPHz5s2TZsPXtd2ePXuwYsUK3HfffXBycsLBgwexceNGjB49Gv/4xz+k9z18+DAiIyOxdOlSLFu2DADwwgsv4Oeff8a4ceOQm5uLLVu2aMU6bdo0AMCkSZNgYWGBIUOGQKFQIDExEZ988gksLS2xcuVKqb2usfTt2xdPPvmktKrBiBEjEB8fj++++w6LFy++6+0NPz8/9OzZEzt37sSTTz6pVbd8+XLs2LEDw4YNw7PPPouqqip88MEH6NGjB06fPl1rX+np6Rg/fjxGjx6NhIQEbNmyBVOnTkWfPn2k+qSkJKxdu7beeO62D0CzfFNubi4eeOCBBvvW0nQ9tkDd55A+x1LX8+Oll17Cb7/9hmHDhmHu3LlwcnLC//73P/z222/4+9//rrVPXc/h+rT0+aLLudLcwsPD8eijj2Lx4sVQKpUICAjA559/josXL9ZKvus65s888wwKCgowfPhwdOnSBZmZmfjyyy+RnJyM//u//5Ouzjo7O2PChAm13r96rraadfrEpE9bamNaeyQEkb68vb21pjGo+ZOenq53u/Pnz4v77rtPODs7CzMzMxEcHCxiYmJqzRJfPfP90qVLpbIRI0bU+x41//d67733RFhYmHB0dBTGxsbC3d1dTJs2TaSmpmq9h66xCKEZDbds2TLh7e0tTExMREBAgF6jvt59911hbW2tNQVHtd27d4v+/fsLU1NT4efnJ9atW1drhvvq14mJieKRRx4RNjY2wsHBQcydO1eUlpZK7aqnK6isrKz1PrruQwjNyFEvLy+DVzy4G0Onf9D12ApR9zkkhO7HUp/z49ChQ2LMmDHCzc1NmJiYiG7duok33nij1nHQ9RxuSEucL/qcK7oy9JgLoVlB4MUXXxRubm7CzMxMDBw4UOzYsaNWu7qO+ddffy2io6OFq6urMDY2Fg4ODiI6Olr89NNPOsd95+hRfWLSty21HUzaiDqpvLw84ejoKNavX2/Q9tVfotnZ2Q22GzNmjHj00UcbtY+ysjLh5uYmVq9ebVCs1Poae77ouj1RR8bbo0SdlJ2dHV5++WW88847mDlzZoPP1TVGREQEhg0b1qh9bNy4ESYmJpg9e3YTRUVtVVOcL0QdFQciEHViixYtQnJycrMlbADw8ssv6/Vwe11mz56Ny5cvw8zMrImioraqKc4Xoo6KSRsRERFROyATosbUy0RERETUJvFKGxEREVE7wKSNiIiIqB3g6FEDqdVqXL9+HTY2No1evJqIiIg6LyEECgsL4eHh0eDAMCZtBrp+/TqX+iAiIqImc+XKFXTt2rXeeiZtBrKxsQGg+QXXXHCXiIiISB8FBQXw9PSUcov6MGkzUPUtUVtbWyZtREREHZBKLXA4PRfKwjIobMwR5usII3nzPRJ1t8etmLQRERER3WHHmQws/yURGfllUpm7nTmWjuuO0T3dWyUmjh4lIiIiqmHHmQzM2XJcK2EDgMz8MszZchw7zmS0SlxM2oiIiIhuUakFlv+SiLpWHqguW/5LIlTqll+bgEkbERER0S2H03NrXWGrSQDIyC/D4fTclgvqFiZtRERERABKKqqwMylTp7bKwvoTu+bCgQhERETUaWUVlCE2SYmdSVnYdz4HFVVqnbZT2Jg3c2S1MWkjIiKiTkMIgZSsQvx5Ngs7k7Jw6mq+Vn1XBwvkFlegpEJV5/YyAG52muk/WhqTNiIiIurQKlVqHE7PxZ+JmkTt6s1SrfpQT3vc290V0SGu6OZqjd/PZmLOluMAoDUgoXoWtaXjujfrfG31YdJGREREHU5+aSXiU5TYmaREfIoShWVVUp2ZsRxDA5wR3d0VUcEKKGy1b3WO7umOtdP61Zqnza2V52lj0kZEREQdwpXcEuxMysKfiVk4nJ6LqhrTcjhZmSIqRIHoEFcMDXSGpWnDKdDonu64t7tbi66IcDdM2oiIiKhdUqsFTl/Lx85btz2TMwu16gMV1oi+ddsz1NNe74TLSC7DYH+npgy5UdrElB9r1qyBj48PzM3NER4ejsOHD9fb9r///S8GDBgAe3t7WFlZITQ0FJs3b663/ezZsyGTybB69Wqtch8fH8hkMq2flStXNlWXiIiIqBmUVaoQm5SFxf89jfCYWExYsx8fxp1HcmYh5DIg3NcRr94fgrgXI/DnwhFYNDoY/b0dWvUKWVNp9SttW7duxcKFC7Fu3TqEh4dj9erVGDVqFFJSUqBQKGq1d3R0xL/+9S8EBwfD1NQU//vf/zBz5kwoFAqMGjVKq+2PP/6IgwcPwsPDo873XrFiBWbNmiW9trGxadrOERERUaPlFJVjV7ISOxOzsDc1B6WVt0d2WpkaISJIgejuCkR0U8DByrQVI21erZ60vfvuu5g1axZmzpwJAFi3bh22b9+Ozz77DK+88kqt9hEREVqv//GPf+Dzzz/Hvn37tJK2a9euYd68efj9999x//331/neNjY2cHNza7rOEBERUaMJIZCWXYQ/EzXzpx2/fBOixjBODztz6bZnuJ8jzIyNWi/YFtSqSVtFRQWOHTuGxYsXS2VyuRzR0dFISEi46/ZCCOzatQspKSl46623pHK1Wo3HH38cL730Enr06FHv9itXrsTrr78OLy8vTJ06FQsWLICxcd2/kvLycpSXl0uvCwoKdOkiERER6aBKpcaxSzelaTku3ijRqu/ZxRbRIZpErYeHLWSy9n+7U1+tmrTl5ORApVLB1dVVq9zV1RXJycn1bpefn48uXbqgvLwcRkZG+Oijj3DvvfdK9W+99RaMjY0xf/78evcxf/589OvXD46Ojjhw4AAWL16MjIwMvPvuu3W2j4mJwfLly/XsIREREdWnqLwKe85lY2diFnalKJFXUinVmRrJMdjfSZqWw8PeohUjbRta/faoIWxsbHDy5EkUFRUhNjYWCxcuhJ+fHyIiInDs2DG89957OH78eINZ+MKFC6V/9+7dG6ampnjmmWcQExMDMzOzWu0XL16stU1BQQE8PT2btmNEREQd3PW8UsQmZeHPJCUOpt1Aher2slH2liYYGaTAvd1dMaybC6zN2mWa0mxa9bfh7OwMIyMjZGVlaZVnZWU1+KyZXC5HQEAAACA0NBRJSUmIiYlBREQE9u7dC6VSCS8vL6m9SqXCCy+8gNWrV+PixYt17jM8PBxVVVW4ePEigoKCatWbmZnVmcwRERFR/YQQOHu9QJo/7ex17ceLfJwspdUI+ns7wNioTUxs0Sa1atJmamqK/v37IzY2FhMmTACgeR4tNjYWc+fO1Xk/arVaet7s8ccfR3R0tFb9qFGj8Pjjj0uDHepy8uRJyOXyOkesEhERke7Kq1Q4eCFXmj+t5qoCMhnQ38tBGkjg72LVKZ9PM0SrX3dcuHAhZsyYgQEDBiAsLAyrV69GcXGxlGBNnz4dXbp0QUxMDADNs2UDBgyAv78/ysvL8euvv2Lz5s1Yu3YtAMDJyQlOTtoT4ZmYmMDNzU26gpaQkIBDhw4hMjISNjY2SEhIwIIFCzBt2jQ4ODi0YO+JiIg6hpvFFYhL0Yz23J2SjeIaC65bmBhhWKBm2aiRwQo4W/POlSFaPWmbNGkSsrOzsWTJEmRmZiI0NBQ7duyQBidcvnwZcvntS6XFxcV49tlncfXqVVhYWCA4OBhbtmzBpEmTdH5PMzMzfPPNN1i2bBnKy8vh6+uLBQsWaD2zRkRERA27mFMs3fY8eukmVDWWjVLYmCEqxBX3dldgiL8zzE06x7QczUkmRM2ZT0hXBQUFsLOzQ35+PmxtbVs7HCIiomanUgucvHJTmj/tvLJIqz7YzUZ6Pq1XFzvIO8AqBC1B15yi1a+0ERERUdtVUlGFvak5mmk5kpW4UVwh1RnLZQj3c5TmT/N0tGzFSDs+Jm1ERESkRVlQhthby0btO5+D8qrb03LYmBsjMkiB6O6uGNHNBXYWJq0YaefCpI2IiKiTE0IgJasQOxM186edupKnVd/VwQL3dnfFvSGuGOjrCBNOy9EqmLQRERF1QpUqNY6k5+KPW9NyXL1ZqlXfx9Me94ZorqgFudpwWo42gEkbERFRJ5FfWondt5aNiktRorCsSqozM5ZjaICztGyUwta8FSOlujBpIyIi6sCu5JZgZ5LmatqhC7moqjEth5OVKUYGa5aNGhroDEtTpgVtGY8OERFRB6JWC/x1LV+aPy05s1CrPkBhjehb86eFejrAiNNytBtM2oiIiNq5skoVDqTl4M9EJWKTsqAsLJfq5DJgoI8j7u3uiqgQV/g6W7VipNQYTNqIiIjaoZyicuy6NS3H3tQclFbeXjbKytQII4JcEB3iisggBRysTFsxUmoqTNqIiIjaASEE0rI1y0btTMzCscs3UXNNI3c7c80kt91dMcjPEWbGXDaqo2HSRkRE1EZVqdQ4dunmrYEESqTnFGvV9/CwlZaN6uFhy2k5OjiDk7aKigqkp6fD398fxsbM/YiIiJpCUXkV9tyalmNXihJ5JZVSnYmRDIP9nXFviAJRIa7wsLdoxUippemdbZWUlGDevHn4/PPPAQDnzp2Dn58f5s2bhy5duuCVV15p8iCJiIg6soz8UuxM0jyflpB2AxWq28tG2VuaYOStZaOGBTrDxpzLRnVWeidtixcvxqlTpxAfH4/Ro0dL5dHR0Vi2bBmTNiIiorsQQuDs9QJp/rQz1wq06r2dLHFviCvu7e6K/t4OMOayUQQDkrZt27Zh69atGDRokNa98x49eiAtLa1JgyMiImqrVGqBw+m5UBaWQWFjjjBfxwbnPCuvUuHQhVz8mZiF2KQsXM8vk+pkMqCfl4M0f5q/izWfT6Na9E7asrOzoVAoapUXFxfzBCMiok5hx5kMLP8lERk1Ei93O3MsHdcdo3u6S2V5JRWIS1FiZ6ISu89lo6j89rJRFiZGGBaoWTZqZLACztZmLdoHan/0TtoGDBiA7du3Y968eQAgJWrr16/H4MGDmzY6IiKiNmbHmQzM2XIc4o7yzPwyzNlyHMsf6I6KKoE/E7Nw9NJNqGosG+ViY4boEAWiQ1xxT4AzzE04LQfpTu+k7c0338SYMWOQmJiIqqoqvPfee0hMTMSBAwewe/fu5oiRiIioTVCpBZb/klgrYQMglS35KVGrPNjNRpo/rXcXO8i5bBQZSO+kbejQoTh58iRWrlyJXr164Y8//kC/fv2QkJCAXr16NUeMREREbcLh9FytW6L16elhi4f7d0V0iCs8HS1bIDLqDAyaYM3f3x+ffvppU8dCRETUZl29WYLvj13Rqe2s4X54ILRLM0dEnY1BSZtarcb58+ehVCqhVqu16oYPH94kgREREbUmlVrg5JWbiE1SIjZJiZSsQp23VdiYN2Nk1FnpnbQdPHgQU6dOxaVLlyCE9l19mUwGlUpVz5ZERERtW2FZJfam5iA2SYm4FCVyiyukOrkM6O/tgOTMQhSWVdW5vQyAm51m+g+ipqZ30jZ79mxpBKm7uzun+SAionbt8o0SxCZnITZJiUPpN1Cpun1BwsbcGCO6uSA6xBURQS6wtzSVRo8C0BqQUP1tuHRc9wbnayMylEzcebnsLqysrHDq1CkEBAQ0V0ztQkFBAezs7JCfnw9bW9vWDoeIiHRUpVLjxJU87EzKwq4kJVKVRVr1vs5WiApWYGSIAgN9HGFSx2oEus7TRqQLXXMKva+0hYeH4/z5850+aSMiovajoKwSu1OysStZc9uz5iLsRnIZBvo4ICrYFVEhCvi5WN91f6N7uuPe7m56rYhA1Fh6J23z5s3DCy+8gMzMTPTq1QsmJtoL1/bu3bvJgiMiIjJUek4xYpM0tz2PXMxFVY1Jbu0sTBAR5IKoEFeMCHSBnaX+i7AbyWUY7O/UlCETNUjv26Nyee3LxDKZDEKITjUQgbdHiYjaliqVGkcv3dQkaslKXMgu1qr3d7FCdIhmySguwk5tSbPdHk1PT29UYERERE0lv6QS8ec0U3LEpyhRUGNUp7FchnA/R4wMdkVUsAI+zlatGClR4+mdtHl7ezdHHERERHclhMCFGrc971zb08HSBJFBCkSFuGJYN2fYmut/25OordI7afviiy8arJ8+fbrBwRAREd2pUqXGkfRcxCYrEZuUhYs3SrTqu7laY2SwK6JDFOjr5cDBANRh6f1Mm4ODg9bryspKlJSUwNTUFJaWlsjNzW3SANsqPtNGRNR8bhZXIP6cEjuTlNiTko3C8tu3PU2MZBjk56SZliPYFV5OXNuT2rdme6bt5s2btcpSU1MxZ84cvPTSS/rujoiICEIInFcWYWeSEruSs3Ds0k3UuOsJJytTRAYrEBWswLBuLrA2M2gVRqJ2rUnO+sDAQKxcuRLTpk1DcnJyU+ySiIg6uIoqNQ6n52omuU1W4nKu9m3PYDcbRIVonk/r09Wetz2p02uyP1WMjY1x/fr1ptodERF1QDeKyhGXko1dyVnYcy4HRTVue5oayTHY3wlRIQqMDFagqwNvexLVpHfS9vPPP2u9FkIgIyMDH374Ie65554mC4yIiNo/IQRSsgoRm6QZRHDiSh5qPkntbG2GkcGaSW6HBjjDirc9ieql8/8dRkZGyMjIwIQJE7TKZTIZXFxcMHLkSPzf//1fU8dHRETtTHmVCgcv5ErTclzLK9Wq7+5ui+gQBUaGuKJ3FzvIeduTSCc6J23Vg0zVanWzBUNERO1TdmE54pKViE3Owt7UHJRU3F4dx8xYjnsCnDEyWIGoEAXc7SxaMVKi9ovXoYmISG9CCCRlFCI2KQs7k5U4dSVPq15hY6YZRBDsiiEBTrA05dcNUWPp9X/R+vXrYW1t3WCb+fPnNyogIiJqm8oqVUhIu4HY5CzsSlLien6ZVn2vLnZSotbDw5a3PYmamM6T68rlcnTt2hVGRkb170wmw4ULF5osuLaMk+sSUWegLCjDrmTNJLf7z+egtPL2bU9zEzmGBjgj6tYi7K625q0YKVH71SyT6x49ehQKhaLRwRERUdskhMDZ6wXS3Gmnr+Zr1bvbmUvPpg3xd4a5Sf1/yBNR09I5aZPJeJmbiKgjKq1QYf/5HMQma1YjyCoo16rv42mPqFuJWnd3W34fELUSvUePEhFR+5eZX4bYZM2UHPvP56C86vbMABYmRhgW6IzoEFdEBLtAYcPbnkRtgc5J29KlS+86CIGIiNomtVrgr2v5iE3WTHJ79nqBVn0XewtpJYJBfk687UnUBuk8EIG0cSACEbV1JRVV2Jeag9gkJXalKJFdePu2p0wGhHraI/rWIIJgNxve9iRqJc0yEIGIiNq2a3ml2JWUhdhkJQ6k3UBFjdueVqZGGN7NBSODFYgMVsDZ2qwVIyUifTFpIyJqx9RqgZNX87ArSYmdSVlIzizUqu/qYIHoEFdEhSgQ5usIM2Pe9iRqr5i0ERG1M0XlVdiXmo3YJCXiUpTIKaqQ6uQyoJ+XA6JuJWqBCmve9iTqIJi0ERG1A1dyS25NcpuFQxdyUaG6fdvTxswYw7u5ICpEgYggBRytTFsxUiJqLjolbX379tX5L7Xjx483KiAiIgJUaoGTV25iZ5ISu5KUSMnSvu3p7WSJqGDN1bSBPo4wNZa3UqRE1FJ0StomTJjQzGEQEXUsKrXA4fRcKAvLoLAxR5ivI4zushZnYVkl9pzLQWxyFuJTspFbrH3bc4CP461Jbl3h72LF255EnQyn/DAQp/wgovrsOJOB5b8kIqPGguruduZYOq47Rvd012p76UYxYpOUiE3OwuH0XFSqbn8k25gbIyJIgegQBUZ0c4G9JW97EnVEuuYUbeJ6+po1a+Dj4wNzc3OEh4fj8OHD9bb973//iwEDBsDe3h5WVlYIDQ3F5s2b620/e/ZsyGQyrF69Wqs8NzcXjz32GGxtbWFvb4+nnnoKRUVFTdUlIuqkdpzJwJwtx7USNkCzAsGcLcex/fR1HE7PRcxvSYh+dzdGvBOPFf9LxP7zN1CpEvBztsKsYb74etYgHH/tXnwwpS8eCO3ChI2I9B+IoFKpsGrVKnz77be4fPkyKioqtOpzc3P12t/WrVuxcOFCrFu3DuHh4Vi9ejVGjRqFlJSUOhend3R0xL/+9S8EBwfD1NQU//vf/zBz5kwoFAqMGjVKq+2PP/6IgwcPwsPDo9Z+HnvsMWRkZODPP/9EZWUlZs6ciaeffhpfffWVXvETEVVTqQWW/5KIum5fVJfN/foEat7fMJLLMNDHQZrk1s+FK88QUd30vj26ZMkSrF+/Hi+88AJeffVV/Otf/8LFixexbds2LFmyBPPnz9crgPDwcAwcOBAffvghAECtVsPT0xPz5s3DK6+8otM++vXrh/vvvx+vv/66VHbt2jWEh4fj999/x/3334/nn38ezz//PAAgKSkJ3bt3x5EjRzBgwAAAwI4dOzB27FhcvXq1ziTvTrw9SkR3Ski7gSmfHrxrOyszI9wb4oqRIa4Y0c0FdhYmLRAdEbVVzXZ79Msvv8Snn36KF154AcbGxpgyZQrWr1+PJUuW4ODBu39Y1VRRUYFjx44hOjr6dkByOaKjo5GQkHDX7YUQiI2NRUpKCoYPHy6Vq9VqPP7443jppZfQo0ePWtslJCTA3t5eStgAIDo6GnK5HIcOHarzvcrLy1FQUKD1Q0RUraxShd3nlDq1ff2Bnlg9uS/G9/FgwkZEOtP79mhmZiZ69eoFALC2tkZ+fj4A4G9/+xtee+01vfaVk5MDlUoFV1dXrXJXV1ckJyfXu11+fj66dOmC8vJyGBkZ4aOPPsK9994r1b/11lswNjau96pfZmZmrVuvxsbGcHR0RGZmZp3bxMTEYPny5bp2jYg6gYz8UsQlZ2NXshL7z+egtFKl03budhbNHBkRdUR6J21du3ZFRkYGvLy84O/vjz/++AP9+vXDkSNHYGbWMuvY2djY4OTJkygqKkJsbCwWLlwIPz8/RERE4NixY3jvvfdw/PjxJh0Ov3jxYixcuFB6XVBQAE9PzybbPxG1fdVzp+1KVmJXcjaSMrSvuLvamqGgtKre5E0GwM1OM/0HEZG+9E7aHnzwQcTGxiI8PBzz5s3DtGnTsGHDBly+fBkLFizQa1/Ozs4wMjJCVlaWVnlWVhbc3Nzq3U4ulyMgIAAAEBoaiqSkJMTExCAiIgJ79+6FUqmEl5eX1F6lUuGFF17A6tWrcfHiRbi5uUGp1L6NUVVVhdzc3Hrf18zMrMWSUiJqO/JKKrD7XDbikpXYfS4bN0sqpTqZDAj1tMfIIM0C7D08bPH72UzM2aKZZLzmA8PVf0IuHdf9rvO1ERHVRe+kbeXKldK/J02aBG9vbxw4cACBgYEYN26cXvsyNTVF//79ERsbK03gq1arERsbi7lz5+q8H7VajfLycgDA448/rvWMHACMGjUKjz/+OGbOnAkAGDx4MPLy8nDs2DH0798fALBr1y6o1WqEh4fr1Qci6liEEEjOLERcihJxyUocu3QT6hrZl625ZsmokcGaudOcrLX/mBvd0x1rp/WrNU+bWz3ztBER6arRa48OGjQIgwYNMnj7hQsXYsaMGRgwYADCwsKwevVqFBcXSwnW9OnT0aVLF8TExADQPFs2YMAA+Pv7o7y8HL/++is2b96MtWvXAgCcnJzg5OSk9R4mJiZwc3NDUFAQACAkJASjR4/GrFmzsG7dOlRWVmLu3LmYPHmyTiNHiahjKa1QYf/5HOxKUSI+WYnrd8yx1s3VGpHBCowMUqC/twOMjRoewzW6pzvu7e6m94oIREQN0Ttpi4mJgaurK5588kmt8s8++wzZ2dlYtGiRXvubNGkSsrOzsWTJEmRmZiI0NBQ7duyQBidcvnwZcvntD8ji4mI8++yzuHr1KiwsLBAcHIwtW7Zg0qRJer3vl19+iblz5yIqKgpyuRwPP/ww3n//fb32QUTtV/UC7LuSlUi4cAMVVbcXYDczluOeAGdEBrkgMliBrg6Weu/fSC7DYH+nuzckItKR3vO0+fj44KuvvsKQIUO0yg8dOoTJkycjPT29SQNsqzhPG1H7UqlS4+jFm4hL0SRq55XaK6B0sbfAyGAFRgYrMNjfCeYmRq0UKRF1NrrmFAZN+eHuXvuZDBcXF2RkZOi7OyKiZpNTVI74FM0ggj2p2Sgsq5LqjOQy9Pd2kBK1QIU1F2AnojZN76TN09MT+/fvh6+vr1b5/v37+TwYEbUqtVrg7PUCzW3PFCVOX83TWjLK0coUEd00tzyHB7rAzpIT2xJR+6F30jZr1iw8//zzqKysxMiRIwEAsbGxePnll/HCCy80eYBERA0pLKvEvtQczWjPlGxkF5Zr1ffwsMXIYM2UHH262nMwABG1W3onbS+99BJu3LiBZ599Vlos3tzcHIsWLcLixYubPEAiopqEELiQU4y4W4MIjlzMRaXq9uU0S1MjDA1wlhI1V1vzVoyWiKjp6D0QoVpRURGSkpJgYWGBwMDATjfxLAciELWc8ioVDl3Ixa5kJeJSlLh0o0Sr3tfZCpFBmmfTBvo6wMyYgwiIqP1otoEI1aytrTFw4EBDNycialBmfpk00nP/+RyUVNxeGsrESIZwXyfN3GnBCvg6W7VipERELUOnpO2hhx7Cpk2bYGtri4ceeqjBtv/973+bJDAi6lw063rmSbc9E+9Y11NhY4bIW8tFDQ10hrVZo+cGJyJqV3T61LOzs5OGwtva2nJYPBE1ifySSuxOvb2uZ25xhVQnkwF9utpLU3J0d7eFnIMIiKgTM/iZts6Oz7QR6U8IgZSsQsQlaxK1Y5dvQlVjYU+b6nU9gxSICKq9ricRUUfUbM+0jRw5Ev/9739hb29f6w0nTJiAXbt26R0sEXVcpRUqHEjLwa5kJeJTsnEtr1Srvnpdz8hb63qa3GVdTyKizkrvpC0+Pl6a6qOmsrIy7N27t0mCIqL27UpuiTSIICHtBsrvWNdziL8TRgYrEBGkgKej/ut6EhF1RjonbadPn5b+nZiYiMzMTOm1SqXCjh070KVLl6aNjojahUqVGscu3ZQGEaTWsa5nZLCLZl1PP2dYmHJKDiIifemctIWGhkImk0Emk0krIdRkYWGBDz74oEmDI6K268atdT13pSix51wd63p6OUhTcnRz5bqeRESNpXPSlp6eDiEE/Pz8cPjwYbi4uEh1pqamUCgUMDLiX89EHZUQNdb1TFbi1B3rejpYmiDi1pQcI7iuJxFRk9M5afP29kZlZSVmzJgBJycneHt7N2dcRNQGFJVXYV9qtjSIQFnHup7Vc6eFenJdTyKi5qTXQAQTExP8+OOPWLJkSXPFQ0St7EJ2kbRc1OH0+tf1jAhSwM2O63oSEbUUvUePPvDAA9i2bRsWLFjQHPEQUQsrr1LhcPqtdT2Tlbh4x7qePk6W0rNpYb6OXNeTiKiV6J20BQYGYsWKFdi/fz/69+8PKyvtNf/mz5/fZMERUfPIKiiTRnruP5+D4jvW9QzzdZQWYPdzsW7FSImIqJreKyL4+vrWvzOZDBcuXGh0UO0BV0Sg9kSlFjh19fa6nmeva6/r6WJjhsggzZQcQwNduK4nEVELarYVEdLT0xsVGBG1jPzSSuw5p1kuKr6BdT0jgxTo4cF1PYmI2jqD/5yuqKhAeno6/P39YWzMv8qJWpsQAqnKImlKjmOX6l/Xc0SQC5y5ricRUbuid7ZVUlKCefPm4fPPPwcAnDt3Dn5+fpg3bx66dOmCV155pcmDJKK6lVXeXtczLrn2up6BCmvN1bRgrutJRNTe6Z20LV68GKdOnUJ8fDxGjx4tlUdHR2PZsmVM2oia2dWbJdKzaQfqWNdz8K11PSO5ricRUYeid9K2bds2bN26FYMGDdJalqZHjx5IS0tr0uCIOiqVWuBwei6UhWVQ2JgjzNex3olpq26t67krRTMlx7ks7XU9PezMpSk5hvhzXU8ioo5K76QtOzsbCoWiVnlxcTHXFiTSwY4zGVj+SyIy8sukMnc7cywd1x2je7oD0KzrufucZiWCPeeyUVBjXU+5DOjvfXtdzyBXG/6/R0TUCeidtA0YMADbt2/HvHnzAED6sli/fj0GDx7ctNERdTA7zmRgzpbjuHOenYz8Mszechzj+7jjys1SnLzCdT2JiEib3knbm2++iTFjxiAxMRFVVVV47733kJiYiAMHDmD37t3NESNRh6BSCyz/JbFWwlbTz6cypH93d7eVBhFwXU8iItI5aTtz5gx69uyJoUOH4uTJk1i5ciV69eqFP/74A/369UNCQgJ69erVnLEStWuHLtzQuiVan78P88Xfh/pxXU8iItKic9LWu3dvDBw4EH//+98xefJkfPrpp80ZF1GHUFxehQNpNxCfosSvf2XcfQMAvbrYMWEjIqJadE7adu/ejY0bN+KFF17AggUL8Mgjj+Cpp57CsGHDmjM+onZFCIG07CLEp2QjPiUbh9NzUaFS333DGhQ2TNiIiKg2vdceLS4uxrfffotNmzZh7969CAgIwFNPPYUZM2bAzc2tueJsc7j2KFUrqahCQtoNxKUoEZ+Sjas3tSe49XK0RESQC4Z3c8GrP/6FrILyOp9rkwFwszPHvkUj+fwaEVEnomtOoXfSVtP58+exceNGbN68GZmZmRg9ejR+/vlnQ3fXrjBp67yEELiQU3zrapoShy5oX00zNZIj3M8REUEKRAS5wM/ZShplXT16FIBW4ladoq2d1k+a9oOIiDqHFknaAM2Vty+//BKLFy9GXl4eVCpVY3bXbjBp61xKK1RIuJCD+JRsxKUocSVX+2paVwcLRN5K0gb7O8HStP4nD3SZp42IiDoPXXMKg1d637NnDz777DP88MMPkMvlmDhxIp566ilDd0fU5qTnFCMuWYn4c9k4eOEGKqq0r6aF+ToiIsgFEUEK+LtY6TzB7eie7ri3u5vOKyIQEREBeiZt169fx6ZNm7Bp0yacP38eQ4YMwfvvv4+JEyfCysqquWIkahGlFSocvKAZ6Rl/LhuXbpRo1Xext0BEkAsigxQY7O8EKzOD/+aBkVyGwf5OjQ2ZiIg6EZ2/dcaMGYOdO3fC2dkZ06dPx5NPPomgoKDmjI2o2V3MKUZ8ihJxKZqraTUXXzcxkmmupnXT3PYMUFhzuSgiImo1OidtJiYm+P777/G3v/0NRkZckJrap7LK6qtpmkEEF++4muZhZ46IYAUiurlgSIAzrBtxNY2IiKgp6fyN1FlGhVLHc+nG7ZGeCRduoKxS+2raAG9HRAZrnk0L5NU0IiJqo3gZgTqcskoVDqXnIj5Fid0p2biQU6xV725nLg0guIdX04iIqJ3gtxV1CFdyS6TJbQ+k5WhdTTOWyzDAx0GaNy3I1YZX04iIqN1h0kbtUnmVCofTcxGXnI34c0pcyNa+muZqaybNm3ZPgDNszE1aKVIiIqKmwaSN2o0ruSWIP5eN+GQlDqTdQGnl7YmcjeQy9Pd2kBK1YDdeTSMioo6FSRu1WeVVKhxJvynNm3ZeWaRVr7Axk+ZNuyfQGba8mkZERB0YkzZqU67eLLk10lPzbFpJxR1X07wcMOJWohbizqtpRETUeTBpo1ZVUaXG0Yu50iCC1DuuprnYmCGim2ak59BAZ9hZ8GoaERF1TkzaqMVdzyuVFl4/cD4HxTWupsllQD8vB0QGKzCimwu6u9tCzjU5iYiImLRR86uoUuPopVzsvpWoncvSvprmbG2GEd1cEBnsgmEBLrCz5NU0IiKiOzFpo2aRkV8qrUKw//wNFJVXSXVyGdDXy0G67dnDg1fTiIiI7oZJGzWJSpUaxy7dRNytVQiSMwu16p2sTDHi1ioEwwOdYW9p2kqREhERtU9M2shgmfll2H1OibjkbOw/n4PCGlfTZDIg1NNemjetp4cdr6YRERE1ApM20lmlSo3jl24i/lw24pKVta6mOVqZYkQ3F0QEuWB4oAscrHg1jYiIqKkwaaMGZRWUYXeKZqmovak5KCzTvprWp6u9NMFtry68mkZERNRc5K0dAACsWbMGPj4+MDc3R3h4OA4fPlxv2//+978YMGAA7O3tYWVlhdDQUGzevFmrzbJlyxAcHAwrKys4ODggOjoahw4d0mrj4+MDmUym9bNy5cpm6V97UqVS48jFXLy9Ixlj39uL8Ddj8fIPp/HrX5koLKuCg6UJJoR6YPWkUBz9VzS2PXcPno/uhj6e9kzYiIiImlGrX2nbunUrFi5ciHXr1iE8PByrV6/GqFGjkJKSAoVCUau9o6Mj/vWvfyE4OBimpqb43//+h5kzZ0KhUGDUqFEAgG7duuHDDz+En58fSktLsWrVKtx33304f/48XFxcpH2tWLECs2bNkl7b2Ng0f4fbIGXhratpKdnYm5qNgjuupvXuYoeIW8+m9e5qDyMmZ0RERC1OJoQQrRlAeHg4Bg4ciA8//BAAoFar4enpiXnz5uGVV17RaR/9+vXD/fffj9dff73O+oKCAtjZ2WHnzp2IiooCoLnS9vzzz+P55583KO7qfebn58PW1tagfbSWKpUaJ6/kSRPcnr1eoFVvb2mC4YGaedOGB7rAydqslSIlIiLq+HTNKVr1SltFRQWOHTuGxYsXS2VyuRzR0dFISEi46/ZCCOzatQspKSl466236n2PTz75BHZ2dujTp49W3cqVK/H666/Dy8sLU6dOxYIFC2BsXPevpLy8HOXl5dLrgoKCOtu1VdmF5dh9TjNv2t7UHOSXVmrV9+5qh4huLhgRpECoJ6+mERERtTWtmrTl5ORApVLB1dVVq9zV1RXJycn1bpefn48uXbqgvLwcRkZG+Oijj3Dvvfdqtfnf//6HyZMno6SkBO7u7vjzzz/h7Ows1c+fPx/9+vWDo6MjDhw4gMWLFyMjIwPvvvtune8ZExOD5cuXN6K3LUulFjh55aa0+Ppf1/K16u0sTDC8mwsiurlgeDcXuNjwahoREVFb1urPtBnCxsYGJ0+eRFFREWJjY7Fw4UL4+fkhIiJCahMZGYmTJ08iJycHn376KSZOnIhDhw5Jz8ktXLhQatu7d2+YmprimWeeQUxMDMzMaicwixcv1tqmoKAAnp6ezddJA+QUlWPPuWzE3Xo2La9E+2pazy620rxpfbraw9ioTYxDISIiIh20atLm7OwMIyMjZGVlaZVnZWXBzc2t3u3kcjkCAgIAAKGhoUhKSkJMTIxW0mZlZYWAgAAEBARg0KBBCAwMxIYNG7RuxdYUHh6OqqoqXLx4EUFBQbXqzczM6kzmmoNKLXA4PRfKwjIobMwR5utY5+1KlVrg1NU8abmov67lo+YTirbmxhjWTTMdx/BuzlDYmLdI/ERERNT0WjVpMzU1Rf/+/REbG4sJEyYA0AxEiI2Nxdy5c3Xej1qt1nrezJA2J0+ehFwur3PEakvacSYDy39JREZ+mVTmbmeOpeO6Y3RPd9woKseeVM0tzz3nsnHzjqtpPTxspXnTQj15NY2IiKijaPXbowsXLsSMGTMwYMAAhIWFYfXq1SguLsbMmTMBANOnT0eXLl0QExMDQPNs2YABA+Dv74/y8nL8+uuv2Lx5M9auXQsAKC4uxhtvvIHx48fD3d0dOTk5WLNmDa5du4ZHH30UAJCQkIBDhw4hMjISNjY2SEhIwIIFCzBt2jQ4ODi0zi8CmoRtzpbjuHM4b0Z+GWZvOQ4fJ0tcyi3RuppmY26M4YEumnU9u7lAYcuraURERB1RqydtkyZNQnZ2NpYsWYLMzEyEhoZix44d0uCEy5cvQy6/fbWouLgYzz77LK5evQoLCwsEBwdjy5YtmDRpEgDAyMgIycnJ+Pzzz5GTkwMnJycMHDgQe/fuRY8ePQBobnV+8803WLZsGcrLy+Hr64sFCxZoPbPW0lRqgeW/JNZK2Gq6eKMEABDibovIW4uv9/WyhwmvphEREXV4rT5PW3vV1PO0JaTdwJRPD9613Zqp/XB/b/dGvx8RERG1DbrmFLxE00YoC8vu3ghAlVrdzJEQERFRW8SkrY3QdWQnR4ASERF1Tkza2ogwX0e425mjvnUIZNCMIg3zdWzJsIiIiKiNYNLWRhjJZVg6rjsA1Ercql8vHdedy0sRERF1Ukza2pDRPd2xdlo/uNlp3wJ1szPH2mn9MLonByAQERF1Vq0+5QdpG93THfd2d9NpRQQiIiLqPJi0Gah6ppSCgoJm2X8PFxP0cDEBABQXFTbLexAREVHrq84l7jYLG5M2AxUWahKptrZoPBEREbVPhYWFsLOzq7eek+saSK1W4/r167CxsYFM1vS3LgsKCuDp6YkrV640yeS97UFn63Nn6y/Q+frc2foLdL4+d7b+Ap2vzy3RXyEECgsL4eHhobUK1J14pc1AcrkcXbt2bfb3sbW17RT/U9TU2frc2foLdL4+d7b+Ap2vz52tv0Dn63Nz97ehK2zVOHqUiIiIqB1g0kZERETUDjBpa6PMzMywdOlSmJmZtXYoLaaz9bmz9RfofH3ubP0FOl+fO1t/gc7X57bUXw5EICIiImoHeKWNiIiIqB1g0kZERETUDjBpIyIiImoHmLQRERERtQNM2lpIbm4uHnvsMdja2sLe3h5PPfUUioqKGtzmk08+QUREBGxtbSGTyZCXl2fQfk+fPo1hw4bB3Nwcnp6eePvtt5uya/UypM9lZWV47rnn4OTkBGtrazz88MPIysqS6jdt2gSZTFbnj1KpBADEx8fXWZ+Zmdnu+gugzr588803Wm3i4+PRr18/mJmZISAgAJs2bWrq7tWpOfp86tQpTJkyBZ6enrCwsEBISAjee+89rX201DFes2YNfHx8YG5ujvDwcBw+fLjB9t999x2Cg4Nhbm6OXr164ddff9WqF0JgyZIlcHd3h4WFBaKjo5GamqrVxpDfaVNqyj5XVlZi0aJF6NWrF6ysrODh4YHp06fj+vXrWvvw8fGpdSxXrlzZLP27U1Mf4yeeeKJWX0aPHq3VpiMdY6DuzyiZTIZ33nlHatNejvHZs2fx8MMPS/GuXr3aoH3q8tluEEEtYvTo0aJPnz7i4MGDYu/evSIgIEBMmTKlwW1WrVolYmJiRExMjAAgbt68qfd+8/Pzhaurq3jsscfEmTNnxNdffy0sLCzExx9/3NRd1Du2usyePVt4enqK2NhYcfToUTFo0CAxZMgQqb6kpERkZGRo/YwaNUqMGDFCahMXFycAiJSUFK12KpWquboqhGie/gohBACxceNGrb6UlpZK9RcuXBCWlpZi4cKFIjExUXzwwQfCyMhI7Nixo1n6WVNz9HnDhg1i/vz5Ij4+XqSlpYnNmzcLCwsL8cEHH0htWuIYf/PNN8LU1FR89tln4uzZs2LWrFnC3t5eZGVl1dl+//79wsjISLz99tsiMTFRvPrqq8LExET89ddfUpuVK1cKOzs7sW3bNnHq1Ckxfvx44evrq3U8DfmdNpWm7nNeXp6Ijo4WW7duFcnJySIhIUGEhYWJ/v37a+3H29tbrFixQutYFhUVtbv+CiHEjBkzxOjRo7X6kpubq7WfjnSMhRC1PpM/++wzIZPJRFpamtSmvRzjw4cPixdffFF8/fXXws3NTaxatcqgfery2W4IJm0tIDExUQAQR44ckcp+++03IZPJxLVr1+66ffUX1J1Jmy77/eijj4SDg4MoLy+X2ixatEgEBQU1slcNM6TPeXl5wsTERHz33XdSWVJSkgAgEhIS6txGqVQKExMT8cUXX0hl9f2+mlNz9heA+PHHH+t975dffln06NFDq2zSpEli1KhRBvZGNy11jIUQ4tlnnxWRkZHS65Y4xmFhYeK5556TXqtUKuHh4SFiYmLqbD9x4kRx//33a5WFh4eLZ555RgghhFqtFm5ubuKdd96R6vPy8oSZmZn4+uuvhRCN/6xorKbuc10OHz4sAIhLly5JZd7e3nV+OTa35ujvjBkzxAMPPFDve3aGY/zAAw+IkSNHapW1l2NcU30x322fhn7O6YK3R1tAQkIC7O3tMWDAAKksOjoacrkchw4datb9JiQkYPjw4TA1NZXajBo1CikpKbh586bB790Usd3p2LFjqKysRHR0tFQWHBwMLy8vJCQk1LnNF198AUtLSzzyyCO16kJDQ+Hu7o57770X+/fvb2SPGtbc/X3uuefg7OyMsLAwfPbZZxA1pldMSEjQ2gegOcb1/c6aSksdYwDIz8+Ho6NjrfLmOsYVFRU4duyYVpxyuRzR0dH1xnm345Ceno7MzEytNnZ2dggPD5faNNdnhS6ao891yc/Ph0wmg729vVb5ypUr4eTkhL59++Kdd95BVVWV4Z3RQXP2Nz4+HgqFAkFBQZgzZw5u3LihtY+OfIyzsrKwfft2PPXUU7Xq2sMxbop9Gvo5pwsuGN8CMjMzoVAotMqMjY3h6OjYqGdwdNlvZmYmfH19tdq4urpKdQ4ODga/f2Njq2sbU1PTWh/mrq6u9W6zYcMGTJ06FRYWFlKZu7s71q1bhwEDBqC8vBzr169HREQEDh06hH79+jWuY/Vozv6uWLECI0eOhKWlJf744w88++yzKCoqwvz586X9VB/TmvsoKChAaWmp1u+mKbXUMT5w4AC2bt2K7du3S2XNfYxzcnKgUqnq/L0mJyfXuU19x6Hm/4vVZQ21aY7PCl00R5/vVFZW9v/t3XtUjPkfB/D3iJpGpgujIiVUJ91FZC1LLu2ybh2RW2GRy7Hsyt3GwRYitrWxHGpdll33w4njkqyijS10dFGnXHYja5VbTKPP7w9nnl+PLqbpwvB5ndPZeb7Pdz7P9zPfMfPd7/N8n8H8+fMREBAg+uHtWbNmoVOnTjAzM0NSUhIWLlyIgoICrF+/vpZZVa2+8vX19cXw4cNha2uL3NxcLFq0CJ9//jkuXrwIPT29D76PY2Nj0axZMwwfPlxUrit9XBcxtfmc0xQP2mphwYIFWL16dbV1MjIyGqg1DeN9yvnixYvIyMjAzp07ReUODg5wcHAQtrt3747c3FxERkZWqPs270O+S5cuFR57eHjg2bNnWLt2rTBoq2vvQ85q6enpGDJkCEJDQ9G/f3+hvC77mDWM0tJS+Pv7g4gQHR0t2vfNN98Ij11dXaGvr4+pU6ciLCzsvfjpoJoYNWqU8NjFxQWurq5o3749zp07Bx8fn3fYsoaxfft2jBkzBlKpVFT+IfXxu8SDtlr49ttvERQUVG2ddu3awcLCQljZqKZSqfDff//BwsJC6+NrEtfCwqLCihX1tjbHrs+cLSwsoFQqUVRUJPo/lPv371f6nG3btsHd3R2enp5vbbeXlxcuXLjw1npvep/yVevatStWrFiBly9fwsDAoMo+lsvlWs2yvS8537hxAz4+PpgyZQqWLFny1nZr28eVadGiBfT09Cp9XavLrbr66v/ev38flpaWojru7u5Cnfr4rNBEfeSsph6w3bp1C2fPnhXNslWma9euUKlUyM/PFw3O61J95lteu3bt0KJFC+Tk5MDHx+eD7WMA+OOPP5CVlYV9+/a9tS3vax/XRUxtP9s1Uqsr4phG1BeeXr58WSg7efJknS1EqC6ueiGCUqkU6ixcuLDBFiLUJGf1xZv79+8XyjIzMyu9ePPJkydkZGQkWlFYnb59+9KwYcO0yEQz9Z1veStXriRTU1Nhe968eeTs7CyqExAQ0GALEeoj5/T0dGrZsiWFhIRo3J667mMvLy+aOXOmsP3q1Stq3bp1tRdsDxo0SFTm7e1dYSFCRESEsL+4uLjShQjaflbUVl3nTESkVCpp6NCh5OTkRIWFhRq1Y9euXdSoUaMKqy7rWn3k+6Y7d+6QRCKhI0eOENGH2cdqgYGBFVYGV+V97ePyqluIUF1MbT/bNcGDtgbi6+tLHh4elJycTBcuXCA7OzvREu+7d++Sg4MDJScnC2UFBQWUmppKW7duJQB0/vx5Sk1NpYcPH2oct6ioiMzNzWncuHGUnp5Oe/fuJZlM1mC3/KhpzsHBwWRtbU1nz56ly5cvk7e3N3l7e1eIvW3bNpJKpZWuHoyMjKTDhw/TzZs36fr16/T1119To0aN6PTp0/WSp1p95Hv06FHaunUrXb9+nW7evEk//fQTyWQy+u6774Q66lt+hISEUEZGBm3atKlBb/lR1zlfv36dFAoFjR07VnR7gPJf+A3Rx3v37iUDAwOKiYmhGzdu0JQpU8jExITu3btHRETjxo2jBQsWCPUTExOpcePGFBERQRkZGRQaGlrpLT9MTEzoyJEjdO3aNRoyZEilt/yo7jWtT3Wds1KppMGDB5OVlRWlpaWJ+lO9oj0pKYkiIyMpLS2NcnNzadeuXaRQKGj8+PE6l++TJ09o7ty5dPHiRcrLy6PTp09Tp06dyM7Ojl68eCHE+ZD6WK24uJhkMhlFR0dXOKYu9fHLly8pNTWVUlNTydLSkubOnUupqal08+ZNjWMSaf5dVlM8aGsgDx8+pICAADIyMiK5XE4TJkygJ0+eCPvz8vIIAMXHxwtloaGhBKDC344dOzSOS0R09epV6tGjBxkYGFDr1q0pPDy8vtPVqG2V5VxSUkLTp08nU1NTkslkNGzYMCooKKgQ29vbm0aPHl3pcVevXk3t27cnqVRKZmZm9Nlnn9HZs2frPL831Ue+cXFx5O7uTkZGRtS0aVNyc3OjzZs3V7gfWXx8PLm7u5O+vj61a9dO9B6pT/WRc1XvexsbG6FOQ/VxVFQUWVtbk76+Pnl5edGlS5eEfb169aLAwEBR/d9++43s7e1JX1+fnJyc6Pjx46L9ZWVltHTpUjI3NycDAwPy8fGhrKwsUR1N/k3Xp7rMWd3/lf2p3xNXrlyhrl27krGxMUmlUnJ0dKTvv/9eNMipT3WZ7/Pnz6l///6kUCioSZMmZGNjQ5MnTxZ9mRN9WH2stmXLFjI0NKSioqIK+3Spj6t6z5a/F+jbYhJp/l1WUxKicvcOYIwxxhhj7yW+TxtjjDHGmA7gQRtjjDHGmA7gQRtjjDHGmA7gQRtjjDHGmA7gQRtjjDHGmA7gQRtjjDHGmA7gQRtjjDHGmA7gQRtjjDHGmA7gQRtjjNWzoKAgDB06tNo6bdu2xYYNG4Tte/fuoV+/fmjatKnoR6frikQiweHDh+s87tvExMRAIpFAIpFg9uzZtYoVFBQkxHoXuTDW0HjQxthHSP1lFxwcXGHfjBkzIJFIEBQU1PAN08KyZcvg7u7+TtuwdetWuLm5wcjICCYmJvDw8EBYWFiNYqSkpGDKlCnCdmRkJAoKCpCWlobs7GycO3cOEokERUVFddz6mrl16xYMDQ3x9OlTrWPI5XIUFBRgxYoVQllERARatmyJli1bYt26daL6ycnJ8PT0hEqlEpVv3LgRBQUFWreDMV3T+F03gDH2brRp0wZ79+5FZGQkDA0NAQAvXrzAnj17YG1t/Y5bpzu2b9+O2bNn44cffkCvXr3w8uVLXLt2Denp6TWKo1AoRNu5ubnw9PSEnZ0dAODGjRt11ubaOHLkCHr37g0jIyOtY0gkElhYWAjb165dw3fffYdjx46BiDBo0CD0798fLi4uUKlUCA4Oxs8//4zGjcVfWcbGxjA2Nta6HYzpGp5pY+wj1alTJ7Rp0wYHDx4Uyg4ePAhra2t4eHiI6r58+RKzZs1Cy5YtIZVK0aNHD6SkpAj71bNAJ0+ehIeHBwwNDdGnTx8UFhYiLi4Ojo6OkMvlGD16NJ4/fy48r6ysDGFhYbC1tYWhoSHc3Nywf//+CnHPnDmDzp07QyaToXv37sjKygLw+lTb8uXLcfXqVeE0WUxMDPLz8yGRSJCWlibEKioqgkQiwblz52rV5jcdPXoU/v7+mDRpEjp06AAnJycEBARg1apVFepGRETA0tISzZs3x4wZM1BaWirsK396tG3btjhw4AB++eUXYdazd+/eAABTU9Maz4TevHkTPXv2hFQqRceOHXHq1CnRfvXrtXfvXnTv3h1SqRTOzs5ISEioEOvIkSMYPHgwgP+f9l2+fDkUCgXkcjmCg4OhVCo1bhsAZGZmwtXVFX369IGPjw9cXV2RmZkJAFi7di169uyJLl261CgmYx8inmlj7CM2ceJE7NixA2PGjAHwetZowoQJwsBGbd68eThw4ABiY2NhY2ODNWvWYMCAAcjJyYGZmZlQb9myZfjxxx8hk8ng7+8Pf39/GBgYYM+ePXj69CmGDRuGqKgozJ8/HwAQFhaGXbt2YfPmzbCzs8P58+cxduxYKBQK9OrVS4i7ePFirFu3DgqFAsHBwZg4cSISExMxcuRIpKen48SJEzh9+jSA17Mv9+/f1/g1qGmb32RhYYGEhATcunULNjY2VR4nPj4elpaWiI+PR05ODkaOHAl3d3dMnjy5Qt2UlBSMHz8ecrkcGzduhKGhIQYPHgw/Pz9kZWVBLpcLs6NvU1ZWhuHDh8Pc3BzJyckoLi6u8lqykJAQbNiwAR07dsT69evx5ZdfIi8vD82bNwfweuB74cIF7Ny5U3jOmTNnIJVKce7cOeTn52PChAlo3rx5pYPWqri4uCA7Oxu3b98GESE7OxvOzs7Izc3Fjh07cOXKFY1jMfZBI8bYRycwMJCGDBlChYWFZGBgQPn5+ZSfn09SqZQePHhAQ4YMocDAQCIievr0KTVp0oR2794tPF+pVFKrVq1ozZo1REQUHx9PAOj06dNCnbCwMAJAubm5QtnUqVNpwIABRET04sULkslklJSUJGrbpEmTKCAgoMq4x48fJwBUUlJCREShoaHk5uYmipGXl0cAKDU1VSh79OgRAaD4+Hit21yZf/75h7p160YAyN7engIDA2nfvn306tUr0ettY2NDKpVKKBsxYgSNHDlS2LaxsaHIyEhhu3wflG/vo0ePqmxLZU6ePEmNGzemv//+WyiLi4sjAHTo0CEi+v/rFR4eLtQpLS0lKysrWr16tVC2e/du6ty5sygvMzMzevbsmVAWHR1NRkZGovzL27FjBxkbG1coj46OJnt7e7K3t6fo6GgiIvLx8aFDhw7R77//Tk5OTuTu7k4JCQkVnls+F8Y+ZDzTxthHTKFQYODAgYiJiQERYeDAgWjRooWoTm5uLkpLS/HJJ58IZU2aNIGXlxcyMjJEdV1dXYXH5ubmkMlkaNeunajszz//BADk5OTg+fPn6NevnyiGUqmscHq2fFxLS0sAQGFhYZ1ce1eTNlfG0tISFy9eRHp6Os6fP4+kpCQEBgZi27ZtOHHiBBo1en0VipOTE/T09ETPu379eq3b/zYZGRlo06YNWrVqJZR5e3tXWrd8eePGjdG5c2dRH5c/Narm5uYGmUwmivH06VPcuXOn2pnHNwUHB4sWxsTGxqJZs2bw9vaGg4MDUlJScPfuXYwaNQp5eXkwMDDQODZjHwoetDH2kZs4cSJmzpwJANi0aVOtYjVp0kR4LJFIRNvqsrKyMgAQVh8eP34crVu3FtV78wv5zbgAhDiVUQ+UiEgoK3/9mLZtro6zszOcnZ0xffp0BAcH49NPP0VCQoJwLZq2cd8XSqUSJ06cwKJFi+r9WP/++y+WL1+O8+fPIzk5Gfb29rCzs4OdnR1KS0uRnZ0NFxeXem8HY+8bXojA2EfO19cXSqUSpaWlGDBgQIX97du3h76+PhITE4Wy0tJSpKSkoGPHjloft2PHjjAwMMDt27fRoUMH0V+bNm00jqOvr49Xr16JytQrMcvfDqL8ooT6pn5dnj17Vmcx9fX1AaBCrm/j6OiIO3fuiF6LS5cuVVq3fLlKpcKVK1fg6OgI4PXCDVNTU7i5uYmec/XqVZSUlIhiGBkZ1agP3zRnzhzMmTMHVlZWePXqlWjArVKpavwaMPah4Jk2xj5yenp6wimw8qfv1Jo2bYpp06YhJCQEZmZmsLa2xpo1a/D8+XNMmjRJ6+M2a9YMc+fOxZw5c1BWVoYePXqguLgYiYmJkMvlCAwM1ChO27ZtkZeXh7S0NFhZWaFZs2YwNDREt27dEB4eDltbWxQWFmLJkiVat7U606ZNQ6tWrdCnTx9YWVmhoKAAK1euhEKhqPI0pDZsbGwgkUhw7NgxfPHFFzA0NNTotht9+/aFvb09AgMDsXbtWjx+/BiLFy+utO6mTZtgZ2cHR0dHREZG4tGjR5g4cSKA16tk3zw1CryegZs0aRKWLFmC/Px8hIaGYubMmcJsZ02dOnUK2dnZiI2NBQB06dIFmZmZiIuLw507d6CnpwcHBwetYjOm63imjTEGuVwOuVxe5f7w8HD4+flh3Lhx6NSpE3JycnDy5EmYmprW6rgrVqzA0qVLERYWBkdHR/j6+uL48eOwtbXVOIafnx98fX3Ru3dvKBQK/PrrrwBer4RVqVTw9PTE7NmzsXLlylq1tSp9+/bFpUuXMGLECNjb28PPzw9SqRRnzpwRVl3WhdatW2P58uVYsGABzM3NhVPa6l8YqEqjRo1w6NAhlJSUwMvLC1999VWVKzvDw8MRHh4ONzc3XLhwAUePHhWucaxq0Obj4wM7Ozv07NkTI0eOxODBg7Fs2TKtciwpKcHMmTOxZcsWYdBnZWWFqKgoTJgwAatWrUJsbKzGK2cZ+9BIqPxFH4wxxnRKaGgoEhISKtympSby8/Nha2uL1NTUSn9d4q+//kKfPn3w4MED0bV5QUFBKCoqqtFPSMXExGD27Nl1+ssOEokEhw4deutPhTGm63imjTHGdFhcXBzWrFlTr8dQqVSIioqqsJhCW8XFxTAyMqry3neaCg4OrtUvMzCma3imjTHGPnJvm2mrijYzbU+ePBFufmxiYlLhFjM1UVhYiMePHwN4fQuVpk2bah2LMV3AgzbGGGOMMR3Ap0cZY4wxxnQAD9oYY4wxxnQAD9oYY4wxxnQAD9oYY4wxxnQAD9oYY4wxxnQAD9oYY4wxxnQAD9oYY4wxxnQAD9oYY4wxxnTA/wDVNyb8jAupdwAAAABJRU5ErkJggg==", + "text/plain": [ + "
" + ] + }, + "metadata": {}, + "output_type": "display_data" + }, + { + "data": { + "text/plain": [ + "True" + ] + }, + "execution_count": 17, + "metadata": {}, + "output_type": "execute_result" + } + ], + "source": [ + "chroma_monitor = SR.get_chromaticity_monitor(\"CHROMATICITY_MONITOR\")\n", + "\n", + "chroma_monitor.measure(\n", + " callback=chroma_callback,\n", + " do_plot=True,\n", + " alphac=alphac,\n", + " fit_order=2,\n", + " n_step=5,\n", + " sleep_between_meas=wait_time,\n", + " sleep_between_step=wait_time,\n", + ")" + ] + }, + { + "cell_type": "code", + "execution_count": 18, + "id": "cecc48f1", + "metadata": {}, + "outputs": [ + { + "name": "stdout", + "output_type": "stream", + "text": [ + "Measured chromaticity: ξx = 8.608, ξy = 5.698\n" + ] + } + ], + "source": [ + "ksi = chroma_monitor.chromaticity.get()\n", + "print(f\"Measured chromaticity: ξx = {ksi[0]:.3f}, ξy = {ksi[1]:.3f}\")" + ] + }, + { + "cell_type": "code", + "execution_count": null, + "id": "015cb06e-7c70-4300-a043-c7c182bd2411", + "metadata": {}, + "outputs": [], + "source": [] + } + ], + "metadata": { + "kernelspec": { + "display_name": "Python 3 (ipykernel)", + "language": "python", + "name": "python3" + }, + "language_info": { + "codemirror_mode": { + "name": "ipython", + "version": 3 + }, + "file_extension": ".py", + "mimetype": "text/x-python", + "name": "python", + "nbconvert_exporter": "python", + "pygments_lexer": "ipython3", + "version": "3.12.3" + } + }, + "nbformat": 4, + "nbformat_minor": 5 +} diff --git a/examples/use_cases/02-chromaticity_measurement.py b/examples/use_cases/02-chromaticity_measurement.py new file mode 100644 index 000000000..966b23ef3 --- /dev/null +++ b/examples/use_cases/02-chromaticity_measurement.py @@ -0,0 +1,132 @@ +#!/usr/bin/env python +# coding: utf-8 + +# In[12]: + + +import numpy as np + +from pyaml.accelerator import Accelerator +from pyaml.common.constants import Action + +# ## Facility configuration +# +# Edit the `CONFIG_FILE` variable below to select the facility. The rest of the notebook runs unchanged. +# +# | Facility | Config file | Control system | Virtual twin | +# |----------|-------------|----------------|--------------| +# | SOLEIL II | `config/soleil_ii/p.yaml` | TANGO (`tango-pyaml`) | Apptainer container | +# | BESSY2 | `config/bessy2/bessy2.yaml` | EPICS (`pyaml-cs-oa`) | Apptainer container | +# | ESRF EBS | `config/esrf/esrf.yaml` | TANGO (`tango-pyaml`) | Apptainer container | +# +# See `README.md` for installation and virtual accelerator startup instructions. + +# In[13]: + + +# ── Facility configuration ────────────────────────────────────────────────── +# Uncomment the facility you want to use: + +# CONFIG_FILE = "config/soleil_ii/p.yaml" +# CONFIG_FILE = "config/bessy2/bessy2.yaml" +CONFIG_FILE = "config/esrf/esrf.yaml" +# ──────────────────────────────────────────────────────────────────────────── + +sr = Accelerator.load(CONFIG_FILE) +print(sr) # string representation + + +# ### Virtual accelerator setup +# +# For **live** control mode you need a running control system or emulator. +# If you want to skip this, run the notebook in **design** mode only. +# +# **SOLEIL II / ESRF (TANGO)** +# ``` +# apptainer pull virtual-accelerator.sif oras://gitlab-registry.synchrotron-soleil.fr/software-control-system/containers/apptainer/virtual-accelerator:latest +# apptainer run virtual-accelerator.sif +# ``` +# +# **BESSY2 (EPICS)** +# ``` +# apptainer run oras://registry.hzdr.de/digital-twins-for-accelerators/containers/pyat-softioc-digital-twin:default-v0-5-1-bessy.2711893 +# ``` +# +# > **Note for BESSY2 live mode:** the PV prefix in `config/bessy2/bessy2.yaml` must match +# > your virtual accelerator instance. Edit the `prefix:` field under `controls:`. + +# ### Control mode choice +# +# - **`sr.design`** — runs pyAT locally, no control system needed. Set `wait_time = 0.0`. +# - **`sr.live`** — connects to the real machine or virtual twin. Set `wait_time` to allow +# readback settling (typically 1.5–2 s). + +# In[14]: + + +SR = sr.design +# SR = sr.live + +wait_time = 0.0 if SR == sr.design else 2.0 +print(SR) # string representation + + +# ### Momentum compaction factor +# +# The momentum compaction factor α_c is needed to convert RF frequency deviation to +# momentum deviation. It is computed from the lattice model (design mode). + +# In[15]: + + +sr.design.get_lattice().disable_6d() +alphac = sr.design.get_lattice().get_mcf() +sr.design.get_lattice().enable_6d() +print(f"Momentum compaction factor: αc = {alphac:.6e}") + + +# ### Chromaticity measurement +# +# The chromaticity monitor is named `CHROMATICITY_MONITOR` in the configuration. +# The measurement sweeps the RF frequency and fits the resulting tune shift. +# +# Parameters: +# - `alphac` — momentum compaction factor (from lattice above) +# - `fit_order` — polynomial fit order (2 = quadratic) +# - `n_step` — number of RF frequency steps +# - `sleep_between_meas` / `sleep_between_step` — settling times (set to `wait_time` for live mode) +# - `do_plot=True` — show the tune vs. δp fit + +# In[16]: + + +def chroma_callback(action: int, cb_data: dict): + if action == Action.MEASURE: + print(f"Chromaticity: #{cb_data['step']} RF={cb_data['rf']:.2f} Hz, Tune={cb_data['tune']}") + return True + + +# In[17]: + + +chroma_monitor = SR.get_chromaticity_monitor("CHROMATICITY_MONITOR") + +chroma_monitor.measure( + callback=chroma_callback, + do_plot=True, + alphac=alphac, + fit_order=2, + n_step=5, + sleep_between_meas=wait_time, + sleep_between_step=wait_time, +) + + +# In[18]: + + +ksi = chroma_monitor.chromaticity.get() +print(f"Measured chromaticity: ξx = {ksi[0]:.3f}, ξy = {ksi[1]:.3f}") + + +# In[ ]: diff --git a/examples/use_cases/03-orbit_correction.ipynb b/examples/use_cases/03-orbit_correction.ipynb new file mode 100644 index 000000000..301ecbad0 --- /dev/null +++ b/examples/use_cases/03-orbit_correction.ipynb @@ -0,0 +1,659 @@ +{ + "cells": [ + { + "cell_type": "code", + "execution_count": 1, + "id": "beeea64e", + "metadata": {}, + "outputs": [], + "source": [ + "from pathlib import Path\n", + "from time import sleep\n", + "\n", + "import matplotlib.pyplot as plt\n", + "import numpy as np\n", + "\n", + "from pyaml.accelerator import Accelerator\n", + "from pyaml.common.constants import Action" + ] + }, + { + "cell_type": "markdown", + "id": "72c306ec", + "metadata": {}, + "source": [ + "## Facility configuration\n", + "\n", + "Edit the `CONFIG_FILE` variable below to select the facility. The rest of the notebook runs unchanged.\n", + "\n", + "| Facility | Config file | Control system | Virtual twin |\n", + "|----------|-------------|----------------|--------------|\n", + "| SOLEIL II | `config/soleil_ii/p.yaml` | TANGO (`tango-pyaml`) | Apptainer container |\n", + "| BESSY2 | `config/bessy2/bessy2.yaml` | EPICS (`pyaml-cs-oa`) | Apptainer container |\n", + "| ESRF EBS | `config/esrf/esrf.yaml` | TANGO (`tango-pyaml`) | Apptainer container |\n", + "\n", + "See `README.md` for installation and virtual accelerator startup instructions." + ] + }, + { + "cell_type": "code", + "execution_count": 2, + "id": "e86031ad", + "metadata": {}, + "outputs": [ + { + "name": "stderr", + "output_type": "stream", + "text": [ + "PyAML OA control system binding (0.1.2) initialized with name 'live' and prefix='pons:'\n" + ] + }, + { + "name": "stdout", + "output_type": "stream", + "text": [ + "14 Aug 2026, 14:23:11 | WARNING | Loading /home/gubaidulin/codes/operation/pyAML/pyaml/examples/unified_examples/config/bessy2/orm.json failed /home/gubaidulin/codes/operation/pyAML/pyaml/examples/unified_examples/config/bessy2/orm.json: file not found\n" + ] + }, + { + "data": { + "text/plain": [ + "Accelerator(facility='BESSY2', machine='sr', description=None, live=OphydAsyncControlSystem(name='live', prefix='pons:', catalog=, debug_level=None), design=Simulator(name='design', lattice='/home/gubaidulin/codes/operation/pyAML/pyaml/examples/unified_examples/config/bessy2/bessy2_standard_user.mat', mat_key=None, linker=None, description=None), yellow_pages=Controls:\n", + " live\n", + " .\n", + "\n", + "Simulators:\n", + " design\n", + " .\n", + "\n", + "Arrays:\n", + " BPM (pyaml.arrays.bpm_array) size=123\n", + " HCorr (pyaml.arrays.magnet_array) size=48\n", + " VCorr (pyaml.arrays.magnet_array) size=64\n", + " QForTune (pyaml.arrays.magnet_array) size=64\n", + " .\n", + "\n", + "Tools:\n", + " DEFAULT_ORBIT_RESPONSE_MATRIX (pyaml.tuning_tools.orbit_response_matrix)\n", + " DEFAULT_DISPERSION (pyaml.tuning_tools.dispersion)\n", + " DEFAULT_ORBIT_CORRECTION (pyaml.tuning_tools.orbit)\n", + " DEFAULT_TUNE_CORRECTION (pyaml.tuning_tools.tune)\n", + " DEFAULT_TUNE_RESPONSE_MATRIX (pyaml.tuning_tools.tune_response_matrix)\n", + " KSI (pyaml.tuning_tools.chromaticity_monitor)\n", + " CHROMATICITY_MONITOR (pyaml.tuning_tools.chromaticity_monitor)\n", + " .\n", + "\n", + "Diagnostics:\n", + " BETATRON_TUNE (pyaml.diagnostics.tune_monitor)\n", + " .)" + ] + }, + "execution_count": 2, + "metadata": {}, + "output_type": "execute_result" + } + ], + "source": [ + "# ── Facility configuration ──────────────────────────────────────────────────\n", + "# Uncomment the facility you want to use:\n", + "\n", + "# CONFIG_FILE = \"config/soleil_ii/p.yaml\"\n", + "CONFIG_FILE = \"config/bessy2/bessy2.yaml\"\n", + "# CONFIG_FILE = \"config/esrf/esrf.yaml\"\n", + "# ────────────────────────────────────────────────────────────────────────────\n", + "\n", + "CONFIG_DIR = Path(CONFIG_FILE).parent\n", + "\n", + "sr = Accelerator.load(CONFIG_FILE)\n", + "sr # string representation" + ] + }, + { + "cell_type": "markdown", + "id": "fc060e0d", + "metadata": {}, + "source": [ + "### Virtual accelerator setup\n", + "\n", + "For **live** control mode you need a running control system or emulator. If you want to skip this, run the notebook in **design** mode only.\n", + "\n", + "**SOLEIL II / ESRF (TANGO)**\n", + "```\n", + "apptainer pull virtual-accelerator.sif oras://gitlab-registry.synchrotron-soleil.fr/software-control-system/containers/apptainer/virtual-accelerator:latest\n", + "apptainer run virtual-accelerator.sif\n", + "```\n", + "\n", + "**BESSY2 (EPICS)**\n", + "```\n", + "apptainer run oras://registry.hzdr.de/digital-twins-for-accelerators/containers/pyat-softioc-digital-twin:default-v0-5-1-bessy.2711893\n", + "```\n", + "\n", + "> **Note for BESSY2 live mode:** the PV prefix in `config/bessy2/bessy2.yaml` must match your virtual accelerator instance. Edit the `prefix:` field under `controls:`." + ] + }, + { + "cell_type": "markdown", + "id": "c8e07cd2", + "metadata": {}, + "source": [ + "### Control mode choice\n", + "\n", + "- **`sr.design`** runs in simulation, no control system needed. ORM measurement is fast (set `wait_time = 0.0`).\n", + "- **`sr.live`** connects to the real machine or twin. Use `wait_time ≥ 1.5 s` for settling.\n", + "\n", + "> **BESSY2 live note:** BPM readbacks may be in nm. `orbit_correction.correct(gain=1e-9)` compensates for the unit mismatch when using a design-mode ORM to correct on live." + ] + }, + { + "cell_type": "code", + "execution_count": 3, + "id": "0d946122", + "metadata": {}, + "outputs": [ + { + "data": { + "text/plain": [ + "Simulator(name='design', lattice='/home/gubaidulin/codes/operation/pyAML/pyaml/examples/unified_examples/config/bessy2/bessy2_standard_user.mat', mat_key=None, linker=None, description=None)" + ] + }, + "execution_count": 3, + "metadata": {}, + "output_type": "execute_result" + } + ], + "source": [ + "SR = sr.design\n", + "# SR = sr.live\n", + "\n", + "wait_time = 0.0 if SR == sr.design else 2.0\n", + "SR # string representation" + ] + }, + { + "cell_type": "markdown", + "id": "85d74eec", + "metadata": {}, + "source": [ + "#### Orbit diagnostics and correctors" + ] + }, + { + "cell_type": "code", + "execution_count": 4, + "id": "6adb7436", + "metadata": {}, + "outputs": [ + { + "name": "stdout", + "output_type": "stream", + "text": [ + "BPMs: 123, H correctors: 48, V correctors: 64\n" + ] + } + ], + "source": [ + "bpms = SR.get_bpms(\"BPM\")\n", + "hcorr = SR.get_magnets(\"HCorr\")\n", + "vcorr = SR.get_magnets(\"VCorr\")\n", + "print(f\"BPMs: {len(bpms)}, H correctors: {len(hcorr)}, V correctors: {len(vcorr)}\")" + ] + }, + { + "cell_type": "markdown", + "id": "808334df", + "metadata": {}, + "source": [ + "### Orbit response matrix\n", + "\n", + "The ORM can be saved in multiple formats. Load it into `SR.orbit` before correcting." + ] + }, + { + "cell_type": "code", + "execution_count": 5, + "id": "33636af2", + "metadata": {}, + "outputs": [ + { + "data": { + "text/plain": [ + "OrbitResponseMatrix(peer='Simulator:design', name='DEFAULT_ORBIT_RESPONSE_MATRIX', description=None, lattice_names=None, n_step=1, sleep_between_step=0, n_avg_meas=1, sleep_between_meas=0, bpm_array_name='BPM', hcorr_array_name='HCorr', vcorr_array_name='VCorr', corrector_delta=1e-06)" + ] + }, + "execution_count": 5, + "metadata": {}, + "output_type": "execute_result" + } + ], + "source": [ + "SR.orm # string representation" + ] + }, + { + "cell_type": "code", + "execution_count": 6, + "id": "3f9dcb18", + "metadata": {}, + "outputs": [ + { + "name": "stdout", + "output_type": "stream", + "text": [ + "14 Aug 2026, 14:23:14 | INFO | Measuring correctors from the default arrays: HCorr and VCorr.\n", + "14 Aug 2026, 14:23:14 | INFO | Measured response of HS4M2D1R.\n", + "14 Aug 2026, 14:23:14 | INFO | Measured response of HS1MT1R.\n", + "14 Aug 2026, 14:23:14 | INFO | Measured response of HS4M1T1R.\n", + "14 Aug 2026, 14:23:14 | INFO | Measured response of HS4M2T1R.\n", + "14 Aug 2026, 14:23:15 | INFO | Measured response of HS1MD2R.\n", + "14 Aug 2026, 14:23:15 | INFO | Measured response of HS4M1D2R.\n", + "14 Aug 2026, 14:23:15 | INFO | Measured response of HS4M2D2R.\n", + "14 Aug 2026, 14:23:15 | INFO | Measured response of HS1MT2R.\n", + "14 Aug 2026, 14:23:15 | INFO | Measured response of HS4M1T2R.\n", + "14 Aug 2026, 14:23:15 | INFO | Measured response of HS4M2T2R.\n", + "14 Aug 2026, 14:23:15 | INFO | Measured response of HS1MD3R.\n", + "14 Aug 2026, 14:23:16 | INFO | Measured response of HS4M1D3R.\n", + "14 Aug 2026, 14:23:16 | INFO | Measured response of HS4M2D3R.\n", + "14 Aug 2026, 14:23:16 | INFO | Measured response of HS1MT3R.\n", + "14 Aug 2026, 14:23:16 | INFO | Measured response of HS4M1T3R.\n", + "14 Aug 2026, 14:23:16 | INFO | Measured response of HS4M2T3R.\n", + "14 Aug 2026, 14:23:16 | INFO | Measured response of HS1MD4R.\n", + "14 Aug 2026, 14:23:16 | INFO | Measured response of HS4M1D4R.\n", + "14 Aug 2026, 14:23:17 | INFO | Measured response of HS4M2D4R.\n", + "14 Aug 2026, 14:23:17 | INFO | Measured response of HS1MT4R.\n", + "14 Aug 2026, 14:23:17 | INFO | Measured response of HS4M1T4R.\n", + "14 Aug 2026, 14:23:17 | INFO | Measured response of HS4M2T4R.\n", + "14 Aug 2026, 14:23:17 | INFO | Measured response of HS1MD5R.\n", + "14 Aug 2026, 14:23:17 | INFO | Measured response of HS4M1D5R.\n", + "14 Aug 2026, 14:23:17 | INFO | Measured response of HS4M2D5R.\n", + "14 Aug 2026, 14:23:18 | INFO | Measured response of HS1MT5R.\n", + "14 Aug 2026, 14:23:18 | INFO | Measured response of HS4M1T5R.\n", + "14 Aug 2026, 14:23:18 | INFO | Measured response of HS4M2T5R.\n", + "14 Aug 2026, 14:23:18 | INFO | Measured response of HS1MD6R.\n", + "14 Aug 2026, 14:23:18 | INFO | Measured response of HS4M1D6R.\n", + "14 Aug 2026, 14:23:18 | INFO | Measured response of HS4M2D6R.\n", + "14 Aug 2026, 14:23:18 | INFO | Measured response of HS1MT6R.\n", + "14 Aug 2026, 14:23:19 | INFO | Measured response of HS4M1T6R.\n", + "14 Aug 2026, 14:23:19 | INFO | Measured response of HS4M2T6R.\n", + "14 Aug 2026, 14:23:19 | INFO | Measured response of HS1MD7R.\n", + "14 Aug 2026, 14:23:19 | INFO | Measured response of HS4M1D7R.\n", + "14 Aug 2026, 14:23:19 | INFO | Measured response of HS4M2D7R.\n", + "14 Aug 2026, 14:23:19 | INFO | Measured response of HS1MT7R.\n", + "14 Aug 2026, 14:23:19 | INFO | Measured response of HS4M1T7R.\n", + "14 Aug 2026, 14:23:20 | INFO | Measured response of HS4M2T7R.\n", + "14 Aug 2026, 14:23:20 | INFO | Measured response of HS1MD8R.\n", + "14 Aug 2026, 14:23:20 | INFO | Measured response of HS4M1D8R.\n", + "14 Aug 2026, 14:23:20 | INFO | Measured response of HS4M2D8R.\n", + "14 Aug 2026, 14:23:20 | INFO | Measured response of HS1MT8R.\n", + "14 Aug 2026, 14:23:20 | INFO | Measured response of HS4M1T8R.\n", + "14 Aug 2026, 14:23:20 | INFO | Measured response of HS4M2T8R.\n", + "14 Aug 2026, 14:23:21 | INFO | Measured response of HS1MD1R.\n", + "14 Aug 2026, 14:23:21 | INFO | Measured response of HS4M1D1R.\n", + "14 Aug 2026, 14:23:21 | INFO | Measured response of VS3M2D1R.\n", + "14 Aug 2026, 14:23:21 | INFO | Measured response of VS2M2D1R.\n", + "14 Aug 2026, 14:23:21 | INFO | Measured response of VS2M1T1R.\n", + "14 Aug 2026, 14:23:21 | INFO | Measured response of VS3M1T1R.\n", + "14 Aug 2026, 14:23:21 | INFO | Measured response of VS3M2T1R.\n", + "14 Aug 2026, 14:23:22 | INFO | Measured response of VS2M2T1R.\n", + "14 Aug 2026, 14:23:22 | INFO | Measured response of VS2M1D2R.\n", + "14 Aug 2026, 14:23:22 | INFO | Measured response of VS3M1D2R.\n", + "14 Aug 2026, 14:23:22 | INFO | Measured response of VS3M2D2R.\n", + "14 Aug 2026, 14:23:22 | INFO | Measured response of VS2M2D2R.\n", + "14 Aug 2026, 14:23:22 | INFO | Measured response of VS2M1T2R.\n", + "14 Aug 2026, 14:23:22 | INFO | Measured response of VS3M1T2R.\n", + "14 Aug 2026, 14:23:23 | INFO | Measured response of VS3M2T2R.\n", + "14 Aug 2026, 14:23:23 | INFO | Measured response of VS2M2T2R.\n", + "14 Aug 2026, 14:23:23 | INFO | Measured response of VS2M1D3R.\n", + "14 Aug 2026, 14:23:23 | INFO | Measured response of VS3M1D3R.\n", + "14 Aug 2026, 14:23:23 | INFO | Measured response of VS3M2D3R.\n", + "14 Aug 2026, 14:23:23 | INFO | Measured response of VS2M2D3R.\n", + "14 Aug 2026, 14:23:23 | INFO | Measured response of VS2M1T3R.\n", + "14 Aug 2026, 14:23:24 | INFO | Measured response of VS3M1T3R.\n", + "14 Aug 2026, 14:23:24 | INFO | Measured response of VS3M2T3R.\n", + "14 Aug 2026, 14:23:24 | INFO | Measured response of VS2M2T3R.\n", + "14 Aug 2026, 14:23:24 | INFO | Measured response of VS2M1D4R.\n", + "14 Aug 2026, 14:23:24 | INFO | Measured response of VS3M1D4R.\n", + "14 Aug 2026, 14:23:24 | INFO | Measured response of VS3M2D4R.\n", + "14 Aug 2026, 14:23:24 | INFO | Measured response of VS2M2D4R.\n", + "14 Aug 2026, 14:23:25 | INFO | Measured response of VS2M1T4R.\n", + "14 Aug 2026, 14:23:25 | INFO | Measured response of VS3M1T4R.\n", + "14 Aug 2026, 14:23:25 | INFO | Measured response of VS3M2T4R.\n", + "14 Aug 2026, 14:23:25 | INFO | Measured response of VS2M2T4R.\n", + "14 Aug 2026, 14:23:25 | INFO | Measured response of VS2M1D5R.\n", + "14 Aug 2026, 14:23:25 | INFO | Measured response of VS3M1D5R.\n", + "14 Aug 2026, 14:23:25 | INFO | Measured response of VS3M2D5R.\n", + "14 Aug 2026, 14:23:26 | INFO | Measured response of VS2M2D5R.\n", + "14 Aug 2026, 14:23:26 | INFO | Measured response of VS2M1T5R.\n", + "14 Aug 2026, 14:23:26 | INFO | Measured response of VS3M1T5R.\n", + "14 Aug 2026, 14:23:26 | INFO | Measured response of VS3M2T5R.\n", + "14 Aug 2026, 14:23:26 | INFO | Measured response of VS2M2T5R.\n", + "14 Aug 2026, 14:23:26 | INFO | Measured response of VS2M1D6R.\n", + "14 Aug 2026, 14:23:26 | INFO | Measured response of VS3M1D6R.\n", + "14 Aug 2026, 14:23:27 | INFO | Measured response of VS3M2D6R.\n", + "14 Aug 2026, 14:23:27 | INFO | Measured response of VS2M2D6R.\n", + "14 Aug 2026, 14:23:27 | INFO | Measured response of VS2M1T6R.\n", + "14 Aug 2026, 14:23:27 | INFO | Measured response of VS3M1T6R.\n", + "14 Aug 2026, 14:23:27 | INFO | Measured response of VS3M2T6R.\n", + "14 Aug 2026, 14:23:27 | INFO | Measured response of VS2M2T6R.\n", + "14 Aug 2026, 14:23:27 | INFO | Measured response of VS2M1D7R.\n", + "14 Aug 2026, 14:23:28 | INFO | Measured response of VS3M1D7R.\n", + "14 Aug 2026, 14:23:28 | INFO | Measured response of VS3M2D7R.\n", + "14 Aug 2026, 14:23:28 | INFO | Measured response of VS2M2D7R.\n", + "14 Aug 2026, 14:23:28 | INFO | Measured response of VS2M1T7R.\n", + "14 Aug 2026, 14:23:28 | INFO | Measured response of VS3M1T7R.\n", + "14 Aug 2026, 14:23:28 | INFO | Measured response of VS3M2T7R.\n", + "14 Aug 2026, 14:23:28 | INFO | Measured response of VS2M2T7R.\n", + "14 Aug 2026, 14:23:29 | INFO | Measured response of VS2M1D8R.\n", + "14 Aug 2026, 14:23:29 | INFO | Measured response of VS3M1D8R.\n", + "14 Aug 2026, 14:23:29 | INFO | Measured response of VS3M2D8R.\n", + "14 Aug 2026, 14:23:29 | INFO | Measured response of VS2M2D8R.\n", + "14 Aug 2026, 14:23:29 | INFO | Measured response of VS2M1T8R.\n", + "14 Aug 2026, 14:23:29 | INFO | Measured response of VS3M1T8R.\n", + "14 Aug 2026, 14:23:29 | INFO | Measured response of VS3M2T8R.\n", + "14 Aug 2026, 14:23:30 | INFO | Measured response of VS2M2T8R.\n", + "14 Aug 2026, 14:23:30 | INFO | Measured response of VS2M1D1R.\n", + "14 Aug 2026, 14:23:30 | INFO | Measured response of VS3M1D1R.\n", + "ORM measured, saved and loaded.\n" + ] + } + ], + "source": [ + "SR.orm.measure(sleep_between_step=wait_time)\n", + "SR.orm.save(CONFIG_DIR / \"orm.json\")\n", + "SR.orm.save(CONFIG_DIR / \"orm.yaml\", with_type=\"yaml\")\n", + "SR.orm.save(CONFIG_DIR / \"orm.npz\", with_type=\"npz\")\n", + "\n", + "SR.orbit.load(CONFIG_DIR / \"orm.json\")\n", + "print(\"ORM measured, saved and loaded.\")" + ] + }, + { + "cell_type": "markdown", + "id": "ff9a6ca2", + "metadata": {}, + "source": [ + "#### Visualise the orbit response matrix" + ] + }, + { + "cell_type": "code", + "execution_count": 7, + "id": "942f8f3b", + "metadata": {}, + "outputs": [ + { + "data": { + "image/png": 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", + "text/plain": [ + "
" + ] + }, + "metadata": {}, + "output_type": "display_data" + } + ], + "source": [ + "orm_data = SR.orm.get()\n", + "plt.imshow(np.array(orm_data[\"matrix\"]))\n", + "plt.colorbar()\n", + "plt.title(\"Orbit response matrix\")\n", + "plt.xlabel(\"Corrector index\")\n", + "plt.ylabel(\"BPM index\")\n", + "plt.show()" + ] + }, + { + "cell_type": "markdown", + "id": "8239ebda", + "metadata": {}, + "source": [ + "### Dispersion measurement (optional)\n", + "\n", + "The dispersion can be measured and incorporated into the ORM to enable RF-based orbit correction. This is particularly useful for correcting closed-orbit distortions caused by energy errors." + ] + }, + { + "cell_type": "code", + "execution_count": 8, + "id": "693fc409", + "metadata": {}, + "outputs": [], + "source": [ + "# Uncomment to measure and visualise dispersion\n", + "\n", + "# def disp_callback(action: int, cb_data) -> bool:\n", + "# from pyaml.common.constants import Action\n", + "# if action == Action.APPLY:\n", + "# print(\"Changing RF frequency\")\n", + "# elif action == Action.MEASURE:\n", + "# print(\"Reading orbit\")\n", + "# elif action == Action.RESTORE:\n", + "# print(\"Restoring RF frequency\")\n", + "# return True\n", + "\n", + "# SR.dispersion.measure(callback=disp_callback)\n", + "# disp_data = SR.dispersion.get()\n", + "# plt.plot(disp_data[\"frequency_response_x\"], label=\"H dispersion\")\n", + "# plt.plot(disp_data[\"frequency_response_y\"], label=\"V dispersion\")\n", + "# plt.xlabel(\"BPM index\")\n", + "# plt.ylabel(\"Orbit / Δf [m/Hz]\")\n", + "# plt.legend()\n", + "# plt.show()" + ] + }, + { + "cell_type": "markdown", + "id": "874b9cf0", + "metadata": {}, + "source": [ + "### Introduce orbit distortion\n", + "\n", + "Reset correctors to zero, then add small random kicks to simulate a disturbed orbit." + ] + }, + { + "cell_type": "code", + "execution_count": 9, + "id": "1fc925a6", + "metadata": {}, + "outputs": [], + "source": [ + "# Reset correctors to zero\n", + "hcorr.strengths.set(np.zeros(len(hcorr)))\n", + "vcorr.strengths.set(np.zeros(len(vcorr)))\n", + "ref_h, ref_v = SR.get_bpms(\"BPM\").positions.get().T\n", + "reference = np.concatenate((ref_h, ref_v))\n", + "\n", + "# Add random kicks to simulate a distorted orbit\n", + "np.random.seed(1)\n", + "std_kick = 1e-6 # rad\n", + "hcorr.strengths.set(hcorr.strengths.get() + std_kick * np.random.normal(size=len(hcorr)))\n", + "vcorr.strengths.set(vcorr.strengths.get() + std_kick * np.random.normal(size=len(vcorr)))" + ] + }, + { + "cell_type": "code", + "execution_count": 10, + "id": "ca562309", + "metadata": {}, + "outputs": [ + { + "name": "stdout", + "output_type": "stream", + "text": [ + "R.m.s. orbit before correction — H: 81.0 µm, V: 32.8 µm\n" + ] + } + ], + "source": [ + "positions_bc = bpms.positions.get()\n", + "std_bc = np.std(positions_bc, axis=0)\n", + "print(f\"R.m.s. orbit before correction — H: {1e6 * std_bc[0]:.1f} µm, V: {1e6 * std_bc[1]:.1f} µm\")" + ] + }, + { + "cell_type": "markdown", + "id": "5fe60131", + "metadata": {}, + "source": [ + "#### Orbit before correction" + ] + }, + { + "cell_type": "code", + "execution_count": 11, + "id": "b4e335c9", + "metadata": {}, + "outputs": [ + { + "data": { + "image/png": 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", + "text/plain": [ + "
" + ] + }, + "metadata": {}, + "output_type": "display_data" + } + ], + "source": [ + "plt.figure()\n", + "plt.plot(positions_bc[:, 0] * 1e6, label=\"H (before)\", color=\"C0\", ls=\"--\")\n", + "plt.plot(positions_bc[:, 1] * 1e6, label=\"V (before)\", color=\"C1\", ls=\"--\")\n", + "plt.xlabel(\"BPM index\")\n", + "plt.ylabel(\"Position [µm]\")\n", + "plt.legend()\n", + "plt.title(\"Orbit before correction\")\n", + "plt.show()" + ] + }, + { + "cell_type": "markdown", + "id": "cf49c543", + "metadata": {}, + "source": [ + "### Correct the orbit\n", + "\n", + "Standard correction: `SR.orbit.correct(reference=reference)`.\n", + "\n", + "Optional variants (uncomment to use):\n", + "- **Virtual corrector weight**: down-weights correctors that are already at large strengths.\n", + "- **RF correction**: also adjusts the RF frequency to minimise dispersion-driven orbit.\n", + "- **Live unit mismatch**: if BESSY2 BPMs read in nm, pass `gain=1e-9`." + ] + }, + { + "cell_type": "code", + "execution_count": 12, + "id": "93135a4c", + "metadata": {}, + "outputs": [ + { + "name": "stdout", + "output_type": "stream", + "text": [ + "14 Aug 2026, 14:23:32 | INFO | (Re-)Building pseudoinverse RM with method='svd_values', parameter=16, plane='H', virtual=True, rf=False.\n", + "14 Aug 2026, 14:23:32 | INFO | (Re-)Building pseudoinverse RM with method='svd_values', parameter=16, plane='V', virtual=False, rf=False.\n" + ] + } + ], + "source": [ + "# Standard correction\n", + "SR.orbit.correct(reference=reference)\n", + "\n", + "# With virtual corrector weight (ESRF style):\n", + "# SR.orbit.set_virtual_weight(1000)\n", + "# SR.orbit.correct(reference=reference)\n", + "\n", + "# With RF orbit correction (ESRF style, requires dispersion in ORM):\n", + "# SR.orbit.correct(reference=reference, rf=True)\n", + "\n", + "# BESSY2 live mode — BPMs in nm, use gain to compensate unit mismatch:\n", + "# SR.orbit.correct(reference=reference, gain=1e-9)\n", + "\n", + "sleep(wait_time)" + ] + }, + { + "cell_type": "code", + "execution_count": 13, + "id": "2d0253b7", + "metadata": {}, + "outputs": [ + { + "name": "stdout", + "output_type": "stream", + "text": [ + "R.m.s. orbit after correction — H: 7.3 µm, V: 2.2 µm\n" + ] + }, + { + "data": { + "image/png": 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", + "text/plain": [ + "
" + ] + }, + "metadata": {}, + "output_type": "display_data" + } + ], + "source": [ + "positions_ac = bpms.positions.get()\n", + "std_ac = np.std(positions_ac, axis=0)\n", + "print(f\"R.m.s. orbit after correction — H: {1e6 * std_ac[0]:.1f} µm, V: {1e6 * std_ac[1]:.1f} µm\")\n", + "\n", + "fig, axes = plt.subplots(3, 1, figsize=(10, 8))\n", + "\n", + "axes[0].plot(positions_ac[:, 0] * 1e6, label=\"After\", color=\"C0\", ls=\"-\")\n", + "axes[0].plot(positions_bc[:, 0] * 1e6, label=\"Before\", color=\"grey\", ls=\"--\")\n", + "\n", + "axes[0].set_ylabel(\"H position [µm]\")\n", + "axes[0].legend()\n", + "\n", + "axes[1].plot(positions_ac[:, 1] * 1e6, label=\"After\", color=\"C1\", ls=\"-\")\n", + "axes[1].plot(positions_bc[:, 1] * 1e6, label=\"Before\", color=\"grey\", ls=\"--\")\n", + "\n", + "axes[1].set_ylabel(\"V position [µm]\")\n", + "axes[1].legend()\n", + "\n", + "axes[2].plot(hcorr.strengths.get() * 1e6, label=\"H correctors\")\n", + "axes[2].plot(vcorr.strengths.get() * 1e6, label=\"V correctors\")\n", + "axes[2].set_ylabel(\"Strength [µrad]\")\n", + "axes[2].set_xlabel(\"Index\")\n", + "axes[2].legend()\n", + "\n", + "fig.tight_layout()\n", + "plt.show()" + ] + }, + { + "cell_type": "code", + "execution_count": null, + "id": "1d72eed8-df85-4e9d-b313-39fc711d28b7", + "metadata": {}, + "outputs": [], + "source": [] + } + ], + "metadata": { + "kernelspec": { + "display_name": "Python 3 (ipykernel)", + "language": "python", + "name": "python3" + }, + "language_info": { + "codemirror_mode": { + "name": "ipython", + "version": 3 + }, + "file_extension": ".py", + "mimetype": "text/x-python", + "name": "python", + "nbconvert_exporter": "python", + "pygments_lexer": "ipython3", + "version": "3.12.3" + } + }, + "nbformat": 4, + "nbformat_minor": 5 +} diff --git a/examples/use_cases/03-orbit_correction.py b/examples/use_cases/03-orbit_correction.py new file mode 100644 index 000000000..b41ba01fb --- /dev/null +++ b/examples/use_cases/03-orbit_correction.py @@ -0,0 +1,262 @@ +#!/usr/bin/env python +# coding: utf-8 + +# In[1]: + + +from pathlib import Path +from time import sleep + +import matplotlib.pyplot as plt +import numpy as np + +from pyaml.accelerator import Accelerator +from pyaml.common.constants import Action + +# ## Facility configuration +# +# Edit the `CONFIG_FILE` variable below to select the facility. The rest of the notebook runs unchanged. +# +# | Facility | Config file | Control system | Virtual twin | +# |----------|-------------|----------------|--------------| +# | SOLEIL II | `config/soleil_ii/p.yaml` | TANGO (`tango-pyaml`) | Apptainer container | +# | BESSY2 | `config/bessy2/bessy2.yaml` | EPICS (`pyaml-cs-oa`) | Apptainer container | +# | ESRF EBS | `config/esrf/esrf.yaml` | TANGO (`tango-pyaml`) | Apptainer container | +# +# See `README.md` for installation and virtual accelerator startup instructions. + +# In[2]: + + +# ── Facility configuration ────────────────────────────────────────────────── +# Uncomment the facility you want to use: + +# CONFIG_FILE = "config/soleil_ii/p.yaml" +CONFIG_FILE = "config/bessy2/bessy2.yaml" +# CONFIG_FILE = "config/esrf/esrf.yaml" +# ──────────────────────────────────────────────────────────────────────────── + +CONFIG_DIR = Path(CONFIG_FILE).parent + +sr = Accelerator.load(CONFIG_FILE) +print(sr) # string representation + + +# ### Virtual accelerator setup +# +# For **live** control mode you need a running control system or emulator. +# If you want to skip this, run the notebook in **design** mode only. +# +# **SOLEIL II / ESRF (TANGO)** +# ``` +# apptainer pull virtual-accelerator.sif oras://gitlab-registry.synchrotron-soleil.fr/software-control-system/containers/apptainer/virtual-accelerator:latest +# apptainer run virtual-accelerator.sif +# ``` +# +# **BESSY2 (EPICS)** +# ``` +# apptainer run oras://registry.hzdr.de/digital-twins-for-accelerators/containers/pyat-softioc-digital-twin:default-v0-5-1-bessy.2711893 +# ``` +# +# > **Note for BESSY2 live mode:** the PV prefix in `config/bessy2/bessy2.yaml` must match +# > your virtual accelerator instance. Edit the `prefix:` field under `controls:`. + +# ### Control mode choice +# +# - **`sr.design`** runs in simulation, no control system needed. ORM measurement is fast (set `wait_time = 0.0`). +# - **`sr.live`** connects to the real machine or twin. Use `wait_time ≥ 1.5 s` for settling. +# +# > **BESSY2 live note:** BPM readbacks may be in nm. `orbit_correction.correct(gain=1e-9)` +# > compensates for the unit mismatch when using a design-mode ORM to correct on live. + +# In[3]: + + +SR = sr.design +# SR = sr.live + +wait_time = 0.0 if SR == sr.design else 2.0 +print(SR) # string representation + + +# #### Orbit diagnostics and correctors + +# In[4]: + + +bpms = SR.get_bpms("BPM") +hcorr = SR.get_magnets("HCorr") +vcorr = SR.get_magnets("VCorr") +print(f"BPMs: {len(bpms)}, H correctors: {len(hcorr)}, V correctors: {len(vcorr)}") + + +# ### Orbit response matrix +# +# The ORM can be saved in multiple formats. Load it into `SR.orbit` before correcting. + +# In[5]: + + +print(SR.orm) # string representation + + +# In[6]: + + +SR.orm.measure(sleep_between_step=wait_time) +SR.orm.save(CONFIG_DIR / "orm.json") +SR.orm.save(CONFIG_DIR / "orm.yaml", with_type="yaml") +SR.orm.save(CONFIG_DIR / "orm.npz", with_type="npz") + +SR.orbit.load(CONFIG_DIR / "orm.json") +print("ORM measured, saved and loaded.") + + +# #### Visualise the orbit response matrix + +# In[7]: + + +orm_data = SR.orm.get() +plt.imshow(np.array(orm_data["matrix"])) +plt.colorbar() +plt.title("Orbit response matrix") +plt.xlabel("Corrector index") +plt.ylabel("BPM index") +plt.show() + + +# ### Dispersion measurement (optional) +# +# The dispersion can be measured and incorporated into the ORM to enable RF-based orbit +# correction. This is particularly useful for correcting closed-orbit distortions caused +# by energy errors. + +# In[8]: + + +# Uncomment to measure and visualise dispersion + +# def disp_callback(action: int, cb_data) -> bool: +# from pyaml.common.constants import Action +# if action == Action.APPLY: +# print("Changing RF frequency") +# elif action == Action.MEASURE: +# print("Reading orbit") +# elif action == Action.RESTORE: +# print("Restoring RF frequency") +# return True + +# SR.dispersion.measure(callback=disp_callback) +# disp_data = SR.dispersion.get() +# plt.plot(disp_data["frequency_response_x"], label="H dispersion") +# plt.plot(disp_data["frequency_response_y"], label="V dispersion") +# plt.xlabel("BPM index") +# plt.ylabel("Orbit / Δf [m/Hz]") +# plt.legend() +# plt.show() + + +# ### Introduce orbit distortion +# +# Reset correctors to zero, then add small random kicks to simulate a disturbed orbit. + +# In[9]: + + +# Reset correctors to zero +hcorr.strengths.set(np.zeros(len(hcorr))) +vcorr.strengths.set(np.zeros(len(vcorr))) +ref_h, ref_v = SR.get_bpms("BPM").positions.get().T +reference = np.concatenate((ref_h, ref_v)) + +# Add random kicks to simulate a distorted orbit +np.random.seed(1) +std_kick = 1e-6 # rad +hcorr.strengths.set(hcorr.strengths.get() + std_kick * np.random.normal(size=len(hcorr))) +vcorr.strengths.set(vcorr.strengths.get() + std_kick * np.random.normal(size=len(vcorr))) + + +# In[10]: + + +positions_bc = bpms.positions.get() +std_bc = np.std(positions_bc, axis=0) +print(f"R.m.s. orbit before correction — H: {1e6 * std_bc[0]:.1f} µm, V: {1e6 * std_bc[1]:.1f} µm") + + +# #### Orbit before correction + +# In[11]: + + +plt.figure() +plt.plot(positions_bc[:, 0] * 1e6, label="H (before)", color="C0", ls="--") +plt.plot(positions_bc[:, 1] * 1e6, label="V (before)", color="C1", ls="--") +plt.xlabel("BPM index") +plt.ylabel("Position [µm]") +plt.legend() +plt.title("Orbit before correction") +plt.show() + + +# ### Correct the orbit +# +# Standard correction: `SR.orbit.correct(reference=reference)`. +# +# Optional variants (uncomment to use): +# - **Virtual corrector weight**: down-weights correctors that are already at large strengths. +# - **RF correction**: also adjusts the RF frequency to minimise dispersion-driven orbit. +# - **Live unit mismatch**: if BESSY2 BPMs read in nm, pass `gain=1e-9`. + +# In[12]: + + +# Standard correction +SR.orbit.correct(reference=reference) + +# With virtual corrector weight (ESRF style): +# SR.orbit.set_virtual_weight(1000) +# SR.orbit.correct(reference=reference) + +# With RF orbit correction (ESRF style, requires dispersion in ORM): +# SR.orbit.correct(reference=reference, rf=True) + +# BESSY2 live mode — BPMs in nm, use gain to compensate unit mismatch: +# SR.orbit.correct(reference=reference, gain=1e-9) + +sleep(wait_time) + + +# In[13]: + + +positions_ac = bpms.positions.get() +std_ac = np.std(positions_ac, axis=0) +print(f"R.m.s. orbit after correction — H: {1e6 * std_ac[0]:.1f} µm, V: {1e6 * std_ac[1]:.1f} µm") + +fig, axes = plt.subplots(3, 1, figsize=(10, 8)) + +axes[0].plot(positions_ac[:, 0] * 1e6, label="After", color="C0", ls="-") +axes[0].plot(positions_bc[:, 0] * 1e6, label="Before", color="grey", ls="--") + +axes[0].set_ylabel("H position [µm]") +axes[0].legend() + +axes[1].plot(positions_ac[:, 1] * 1e6, label="After", color="C1", ls="-") +axes[1].plot(positions_bc[:, 1] * 1e6, label="Before", color="grey", ls="--") + +axes[1].set_ylabel("V position [µm]") +axes[1].legend() + +axes[2].plot(hcorr.strengths.get() * 1e6, label="H correctors") +axes[2].plot(vcorr.strengths.get() * 1e6, label="V correctors") +axes[2].set_ylabel("Strength [µrad]") +axes[2].set_xlabel("Index") +axes[2].legend() + +fig.tight_layout() +plt.show() + + +# In[ ]: diff --git a/examples/use_cases/README.md b/examples/use_cases/README.md new file mode 100644 index 000000000..ebcfe8c99 --- /dev/null +++ b/examples/use_cases/README.md @@ -0,0 +1,96 @@ +# Unified pyAML Examples + +Three notebooks demonstrating tune correction, chromaticity measurement, and orbit correction. A single configuration variable at the top of each notebook selects the facility — the rest of the code runs unchanged. + +## Notebooks + +| Notebook | Topic | +|----------|-------| +| `01-tune_correction.ipynb` | Measure tune response matrix and correct betatron tune | +| `02-chromaticity_measurement.ipynb` | Measure chromaticity via RF frequency scan | +| `03-orbit_correction.ipynb` | Measure ORM and correct closed orbit | + +## Facility configuration + +Edit the `CONFIG_FILE` variable at the top of each notebook: + +```python +CONFIG_FILE = "config/soleil_ii/p.yaml" # SOLEIL II +# CONFIG_FILE = "config/bessy2/bessy2.yaml" # BESSY2 +# CONFIG_FILE = "config/esrf/esrf.yaml" # ESRF EBS +``` + +## Installation + +### SOLEIL II and ESRF (TANGO) + +```bash +pip install accelerator-middle-layer[tango-pyaml] +``` + +### BESSY2 (EPICS) + +```bash +pip install accelerator-middle-layer[pyaml-cs-oa] +``` + +To support both control systems in the same environment: + +```bash +pip install accelerator-middle-layer[tango-pyaml,pyaml-cs-oa] +``` + +## Starting the virtual accelerator + +### SOLEIL II + +```bash +apptainer pull -F virtual-accelerator.sif oras://gitlab-registry.synchrotron-soleil.fr/software-control-system/containers/apptainer/virtual-accelerator:latest +apptainer run virtual-accelerator.sif +``` + +This starts the TANGO control system twin on `localhost:11000`. + +### BESSY2 + +```bash +apptainer run oras://registry.hzdr.de/digital-twins-for-accelerators/containers/pyat-softioc-digital-twin:default-v0-5-1-bessy.2711893 +``` + +> **BESSY2 PV prefix:** the virtual accelerator assigns a unique PV prefix (usually your username). Edit `config/bessy2/bessy2.yaml` and set `prefix:` under `controls:` to match: +> ```yaml +> controls: +> - type: pyaml_cs_oa.controlsystem +> prefix: "your_prefix:" # ← change this +> ``` + +### ESRF EBS + +Follow the ESRF internal documentation to start the EBS simulator and set `tango_host` in `config/esrf/esrf.yaml`. + +## Control modes + +Each notebook lets you choose between design and live mode: + +```python +SR = sr.design # simulation only — no control system needed +# SR = sr.live # real machine or virtual twin +``` + +In `design` mode all wait times can be set to `0.0`. In `live` mode use `wait_time ≥ 1.5 s` to allow readbacks to settle. + +## Named arrays and tools (canonical names used in all configs) + +| Name | Description | +|------|-------------| +| `QForTune` | Quadrupoles for tune correction | +| `HCorr` | Horizontal orbit correctors | +| `VCorr` | Vertical orbit correctors | +| `BPM` | Beam position monitors | +| `BETATRON_TUNE` | Betatron tune monitor | +| `CHROMATICITY_MONITOR` | Chromaticity monitor | +| `DEFAULT_TUNE_CORRECTION` | Tune correction tool → `SR.tune` | +| `DEFAULT_TUNE_RESPONSE_MATRIX` | Tune response matrix tool → `SR.trm` | +| `DEFAULT_ORBIT_CORRECTION` | Orbit correction tool → `SR.orbit` | +| `DEFAULT_ORBIT_RESPONSE_MATRIX` | Orbit response matrix tool → `SR.orm` | +| `DEFAULT_DISPERSION` | Dispersion measurement tool → `SR.dispersion` | diff --git a/examples/use_cases/config/bessy2/bessy2.yaml b/examples/use_cases/config/bessy2/bessy2.yaml new file mode 100644 index 000000000..c04f66c82 --- /dev/null +++ b/examples/use_cases/config/bessy2/bessy2.yaml @@ -0,0 +1,2462 @@ +class: pyaml.accelerator.Accelerator +machine: sr +facility: BESSY2 +energy: 1.7185e9 +simulators: +- class: pyaml.lattice.simulator.Simulator + lattice: bessy2_standard_user.mat + name: design +controls: +- class: pyaml_cs_oa.controlsystem.OphydAsyncControlSystem + prefix: 'pons:' + name: live + catalog: + class: pyaml_cs_oa.dynamic_catalog.DynamicCatalog + backend: epics +data_folder: /data/store +arrays: +- class: pyaml.arrays.magnet.Magnet + name: HCorr + elements: + - HS4M2D1R + - HS1MT1R + - HS4M1T1R + - HS4M2T1R + - HS1MD2R + - HS4M1D2R + - HS4M2D2R + - HS1MT2R + - HS4M1T2R + - HS4M2T2R + - HS1MD3R + - HS4M1D3R + - HS4M2D3R + - HS1MT3R + - HS4M1T3R + - HS4M2T3R + - HS1MD4R + - HS4M1D4R + - HS4M2D4R + - HS1MT4R + - HS4M1T4R + - HS4M2T4R + - HS1MD5R + - HS4M1D5R + - HS4M2D5R + - HS1MT5R + - HS4M1T5R + - HS4M2T5R + - HS1MD6R + - HS4M1D6R + - HS4M2D6R + - HS1MT6R + - HS4M1T6R + - HS4M2T6R + - HS1MD7R + - HS4M1D7R + - HS4M2D7R + - HS1MT7R + - HS4M1T7R + - HS4M2T7R + - HS1MD8R + - HS4M1D8R + - HS4M2D8R + - HS1MT8R + - HS4M1T8R + - HS4M2T8R + - HS1MD1R + - HS4M1D1R +- class: pyaml.arrays.magnet.Magnet + name: VCorr + elements: + - VS3M2D1R + - VS2M2D1R + - VS2M1T1R + - VS3M1T1R + - VS3M2T1R + - VS2M2T1R + - VS2M1D2R + - VS3M1D2R + - VS3M2D2R + - VS2M2D2R + - VS2M1T2R + - VS3M1T2R + - VS3M2T2R + - VS2M2T2R + - VS2M1D3R + - VS3M1D3R + - VS3M2D3R + - VS2M2D3R + - VS2M1T3R + - VS3M1T3R + - VS3M2T3R + - VS2M2T3R + - VS2M1D4R + - VS3M1D4R + - VS3M2D4R + - VS2M2D4R + - VS2M1T4R + - VS3M1T4R + - VS3M2T4R + - VS2M2T4R + - VS2M1D5R + - VS3M1D5R + - VS3M2D5R + - VS2M2D5R + - VS2M1T5R + - VS3M1T5R + - VS3M2T5R + - VS2M2T5R + - VS2M1D6R + - VS3M1D6R + - VS3M2D6R + - VS2M2D6R + - VS2M1T6R + - VS3M1T6R + - VS3M2T6R + - VS2M2T6R + - VS2M1D7R + - VS3M1D7R + - VS3M2D7R + - VS2M2D7R + - VS2M1T7R + - VS3M1T7R + - VS3M2T7R + - VS2M2T7R + - VS2M1D8R + - VS3M1D8R + - VS3M2D8R + - VS2M2D8R + - VS2M1T8R + - VS3M1T8R + - VS3M2T8R + - VS2M2T8R + - VS2M1D1R + - VS3M1D1R +- class: pyaml.arrays.bpm.BPM + name: BPM + elements: + - BPMZ5D1R + - BPMZ6D1R + - BPMZ7D1R + - BPMZ1T1R + - BPMZ2T1R + - BPMZ3T1R + - BPMZ4T1R + - BPMZ41T1R + - BPMZ5T1R + - BPMZ6T1R + - BPMZ7T1R + - BPMZ1D2R + - BPMZ2D2R + - BPMZ3D2R + - BPMZ4D2R + - BPMZ5D2R + - BPMZ6D2R + - BPMZ7D2R + - BPMZ1T2R + - BPMZ2T2R + - BPMZ3T2R + - BPMZ4T2R + - BPMZ41T2R + - BPMZ42T2R + - BPMZ43T2R + - BPMZ5T2R + - BPMZ6T2R + - BPMZ7T2R + - BPMZ1D3R + - BPMZ2D3R + - BPMZ3D3R + - BPMZ4D3R + - BPMZ5D3R + - BPMZ6D3R + - BPMZ7D3R + - BPMZ1T3R + - BPMZ2T3R + - BPMZ3T3R + - BPMZ4T3R + - BPMZ5T3R + - BPMZ6T3R + - BPMZ7T3R + - BPMZ1D4R + - BPMZ2D4R + - BPMZ3D4R + - BPMZ4D4R + - BPMZ5D4R + - BPMZ6D4R + - BPMZ7D4R + - BPMZ1T4R + - BPMZ2T4R + - BPMZ3T4R + - BPMZ4T4R + - BPMZ5T4R + - BPMZ6T4R + - BPMZ7T4R + - BPMZ1D5R + - BPMZ2D5R + - BPMZ3D5R + - BPMZ4D5R + - BPMZ5D5R + - BPMZ6D5R + - BPMZ7D5R + - BPMZ1T5R + - BPMZ2T5R + - BPMZ3T5R + - BPMZ4T5R + - BPMZ5T5R + - BPMZ6T5R + - BPMZ7T5R + - BPMZ1D6R + - BPMZ2D6R + - BPMZ3D6R + - BPMZ4D6R + - BPMZ41D6R + - BPMZ42D6R + - BPMZ43D6R + - BPMZ44D6R + - BPMZ6D6R + - BPMZ7D6R + - BPMZ1T6R + - BPMZ2T6R + - BPMZ3T6R + - BPMZ4T6R + - BPMZ41T6R + - BPMZ5T6R + - BPMZ6T6R + - BPMZ7T6R + - BPMZ1D7R + - BPMZ2D7R + - BPMZ3D7R + - BPMZ4D7R + - BPMZ5D7R + - BPMZ6D7R + - BPMZ7D7R + - BPMZ1T7R + - BPMZ2T7R + - BPMZ3T7R + - BPMZ4T7R + - BPMZ41T7R + - BPMZ5T7R + - BPMZ6T7R + - BPMZ7T7R + - BPMZ1D8R + - BPMZ2D8R + - BPMZ3D8R + - BPMZ4D8R + - BPMZ5D8R + - BPMZ6D8R + - BPMZ7D8R + - BPMZ1T8R + - BPMZ2T8R + - BPMZ3T8R + - BPMZ4T8R + - BPMZ5T8R + - BPMZ6T8R + - BPMZ7T8R + - BPMZ1D1R + - BPMZ2D1R + - BPMZ3D1R + - BPMZ4D1R + - BPMZ41D1R + - BPMZ42D1R +- class: pyaml.arrays.magnet.Magnet + name: QForTune + elements: + - Q3M2D1R + - Q3M1T1R + - Q3M2T1R + - Q3M1D2R + - Q3M2D2R + - Q3M1T2R + - Q3M2T2R + - Q3M1D3R + - Q3M2D3R + - Q3M1T3R + - Q3M2T3R + - Q3M1D4R + - Q3M2D4R + - Q3M1T4R + - Q3M2T4R + - Q3M1D5R + - Q3M2D5R + - Q3M1T5R + - Q3M2T5R + - Q3M1D6R + - Q3M2D6R + - Q3M1T6R + - Q3M2T6R + - Q3M1D7R + - Q3M2D7R + - Q3M1T7R + - Q3M2T7R + - Q3M1D8R + - Q3M2D8R + - Q3M1T8R + - Q3M2T8R + - Q3M1D1R + - Q4M2D1R + - Q4M1T1R + - Q4M2T1R + - Q4M1D2R + - Q4M2D2R + - Q4M1T2R + - Q4M2T2R + - Q4M1D3R + - Q4M2D3R + - Q4M1T3R + - Q4M2T3R + - Q4M1D4R + - Q4M2D4R + - Q4M1T4R + - Q4M2T4R + - Q4M1D5R + - Q4M2D5R + - Q4M1T5R + - Q4M2T5R + - Q4M1D6R + - Q4M2D6R + - Q4M1T6R + - Q4M2T6R + - Q4M1D7R + - Q4M2D7R + - Q4M1T7R + - Q4M2T7R + - Q4M1D8R + - Q4M2D8R + - Q4M1T8R + - Q4M2T8R + - Q4M1D1R +devices: +- class: pyaml.tuning_tools.orbit_response_matrix.OrbitResponseMatrix + bpm_array_name: BPM + hcorr_array_name: HCorr + vcorr_array_name: VCorr + corrector_delta: 1e-6 + name: DEFAULT_ORBIT_RESPONSE_MATRIX +- class: pyaml.tuning_tools.dispersion.Dispersion + bpm_array_name: BPM + rf_plant_name: RF + frequency_delta: 10 + name: DEFAULT_DISPERSION +- class: pyaml.tuning_tools.orbit.Orbit + bpm_array_name: BPM + hcorr_array_name: HCorr + vcorr_array_name: VCorr + name: DEFAULT_ORBIT_CORRECTION + singular_values: 16 + response_matrix: ${path:orm.json} +- class: pyaml.rf.rf_plant.RFPlant + name: RF + masterclock: (MCLKHX251C:freq)[KHz] +- class: pyaml.magnet.hcorrector.HCorrector + name: HS4M2D1R + lattice_names: S4M2D1R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: -0.0044502 + unit: 1/m + powerconverter: (HS4P2D1R:rdbk, HS4P2D1R:set)[A] + hardware_unit: A +- class: pyaml.magnet.hcorrector.HCorrector + name: HS1MT1R + lattice_names: S1MT1R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: -0.00553438 + unit: 1/m + powerconverter: (HS1PT1R:rdbk, HS1PT1R:set)[A] + hardware_unit: A +- class: pyaml.magnet.hcorrector.HCorrector + name: HS4M1T1R + lattice_names: S4M1T1R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: -0.0044502 + unit: 1/m + powerconverter: (HS4P1T1R:rdbk, HS4P1T1R:set)[A] + hardware_unit: A +- class: pyaml.magnet.hcorrector.HCorrector + name: HS4M2T1R + lattice_names: S4M2T1R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: -0.0044502 + unit: 1/m + powerconverter: (HS4P2T1R:rdbk, HS4P2T1R:set)[A] + hardware_unit: A +- class: pyaml.magnet.hcorrector.HCorrector + name: HS1MD2R + lattice_names: S1MD2R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: -0.00553438 + unit: 1/m + powerconverter: (HS1PD2R:rdbk, HS1PD2R:set)[A] + hardware_unit: A +- class: pyaml.magnet.hcorrector.HCorrector + name: HS4M1D2R + lattice_names: S4M1D2R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: -0.0044502 + unit: 1/m + powerconverter: (HS4P1D2R:rdbk, HS4P1D2R:set)[A] + hardware_unit: A +- class: pyaml.magnet.hcorrector.HCorrector + name: HS4M2D2R + lattice_names: S4M2D2R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: -0.0044502 + unit: 1/m + powerconverter: (HS4P2D2R:rdbk, HS4P2D2R:set)[A] + hardware_unit: A +- class: pyaml.magnet.hcorrector.HCorrector + name: HS1MT2R + lattice_names: S1MT2R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: -0.00553438 + unit: 1/m + powerconverter: (HS1PT2R:rdbk, HS1PT2R:set)[A] + hardware_unit: A +- class: pyaml.magnet.hcorrector.HCorrector + name: HS4M1T2R + lattice_names: S4M1T2R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: -0.0044502 + unit: 1/m + powerconverter: (HS4P1T2R:rdbk, HS4P1T2R:set)[A] + hardware_unit: A +- class: pyaml.magnet.hcorrector.HCorrector + name: HS4M2T2R + lattice_names: S4M2T2R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: -0.0044502 + unit: 1/m + powerconverter: (HS4P2T2R:rdbk, HS4P2T2R:set)[A] + hardware_unit: A +- class: pyaml.magnet.hcorrector.HCorrector + name: HS1MD3R + lattice_names: S1MD3R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: -0.00553438 + unit: 1/m + powerconverter: (HS1PD3R:rdbk, HS1PD3R:set)[A] + hardware_unit: A +- class: pyaml.magnet.hcorrector.HCorrector + name: HS4M1D3R + lattice_names: S4M1D3R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: -0.0044502 + unit: 1/m + powerconverter: (HS4P1D3R:rdbk, HS4P1D3R:set)[A] + hardware_unit: A +- class: pyaml.magnet.hcorrector.HCorrector + name: HS4M2D3R + lattice_names: S4M2D3R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: -0.0044502 + unit: 1/m + powerconverter: (HS4P2D3R:rdbk, HS4P2D3R:set)[A] + hardware_unit: A +- class: pyaml.magnet.hcorrector.HCorrector + name: HS1MT3R + lattice_names: S1MT3R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: -0.00553438 + unit: 1/m + powerconverter: (HS1PT3R:rdbk, HS1PT3R:set)[A] + hardware_unit: A +- class: pyaml.magnet.hcorrector.HCorrector + name: HS4M1T3R + lattice_names: S4M1T3R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: -0.0044502 + unit: 1/m + powerconverter: (HS4P1T3R:rdbk, HS4P1T3R:set)[A] + hardware_unit: A +- class: pyaml.magnet.hcorrector.HCorrector + name: HS4M2T3R + lattice_names: S4M2T3R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: -0.0044502 + unit: 1/m + powerconverter: (HS4P2T3R:rdbk, HS4P2T3R:set)[A] + hardware_unit: A +- class: pyaml.magnet.hcorrector.HCorrector + name: HS1MD4R + lattice_names: S1MD4R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: -0.00553438 + unit: 1/m + powerconverter: (HS1PD4R:rdbk, HS1PD4R:set)[A] + hardware_unit: A +- class: pyaml.magnet.hcorrector.HCorrector + name: HS4M1D4R + lattice_names: S4M1D4R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: -0.0044502 + unit: 1/m + powerconverter: (HS4P1D4R:rdbk, HS4P1D4R:set)[A] + hardware_unit: A +- class: pyaml.magnet.hcorrector.HCorrector + name: HS4M2D4R + lattice_names: S4M2D4R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: -0.0044502 + unit: 1/m + powerconverter: (HS4P2D4R:rdbk, HS4P2D4R:set)[A] + hardware_unit: A +- class: pyaml.magnet.hcorrector.HCorrector + name: HS1MT4R + lattice_names: S1MT4R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: -0.00553438 + unit: 1/m + powerconverter: (HS1PT4R:rdbk, HS1PT4R:set)[A] + hardware_unit: A +- class: pyaml.magnet.hcorrector.HCorrector + name: HS4M1T4R + lattice_names: S4M1T4R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: -0.0044502 + unit: 1/m + powerconverter: (HS4P1T4R:rdbk, HS4P1T4R:set)[A] + hardware_unit: A +- class: pyaml.magnet.hcorrector.HCorrector + name: HS4M2T4R + lattice_names: S4M2T4R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: -0.0044502 + unit: 1/m + powerconverter: (HS4P2T4R:rdbk, HS4P2T4R:set)[A] + hardware_unit: A +- class: pyaml.magnet.hcorrector.HCorrector + name: HS1MD5R + lattice_names: S1MD5R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: -0.00553438 + unit: 1/m + powerconverter: (HS1PD5R:rdbk, HS1PD5R:set)[A] + hardware_unit: A +- class: pyaml.magnet.hcorrector.HCorrector + name: HS4M1D5R + lattice_names: S4M1D5R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: -0.0044502 + unit: 1/m + powerconverter: (HS4P1D5R:rdbk, HS4P1D5R:set)[A] + hardware_unit: A +- class: pyaml.magnet.hcorrector.HCorrector + name: HS4M2D5R + lattice_names: S4M2D5R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: -0.0044502 + unit: 1/m + powerconverter: (HS4P2D5R:rdbk, HS4P2D5R:set)[A] + hardware_unit: A +- class: pyaml.magnet.hcorrector.HCorrector + name: HS1MT5R + lattice_names: S1MT5R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: -0.00553438 + unit: 1/m + powerconverter: (HS1PT5R:rdbk, HS1PT5R:set)[A] + hardware_unit: A +- class: pyaml.magnet.hcorrector.HCorrector + name: HS4M1T5R + lattice_names: S4M1T5R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: -0.0044502 + unit: 1/m + powerconverter: (HS4P1T5R:rdbk, HS4P1T5R:set)[A] + hardware_unit: A +- class: pyaml.magnet.hcorrector.HCorrector + name: HS4M2T5R + lattice_names: S4M2T5R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: -0.0044502 + unit: 1/m + powerconverter: (HS4P2T5R:rdbk, HS4P2T5R:set)[A] + hardware_unit: A +- class: pyaml.magnet.hcorrector.HCorrector + name: HS1MD6R + lattice_names: S1MD6R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: -0.00553438 + unit: 1/m + powerconverter: (HS1PD6R:rdbk, HS1PD6R:set)[A] + hardware_unit: A +- class: pyaml.magnet.hcorrector.HCorrector + name: HS4M1D6R + lattice_names: S4M1D6R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: -0.0044502 + unit: 1/m + powerconverter: (HS4P1D6R:rdbk, HS4P1D6R:set)[A] + hardware_unit: A +- class: pyaml.magnet.hcorrector.HCorrector + name: HS4M2D6R + lattice_names: S4M2D6R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: -0.0044502 + unit: 1/m + powerconverter: (HS4P2D6R:rdbk, HS4P2D6R:set)[A] + hardware_unit: A +- class: pyaml.magnet.hcorrector.HCorrector + name: HS1MT6R + lattice_names: S1MT6R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: -0.00553438 + unit: 1/m + powerconverter: (HS1PT6R:rdbk, HS1PT6R:set)[A] + hardware_unit: A +- class: pyaml.magnet.hcorrector.HCorrector + name: HS4M1T6R + lattice_names: S4M1T6R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: -0.0044502 + unit: 1/m + powerconverter: (HS4P1T6R:rdbk, HS4P1T6R:set)[A] + hardware_unit: A +- class: pyaml.magnet.hcorrector.HCorrector + name: HS4M2T6R + lattice_names: S4M2T6R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: -0.0044502 + unit: 1/m + powerconverter: (HS4P2T6R:rdbk, HS4P2T6R:set)[A] + hardware_unit: A +- class: pyaml.magnet.hcorrector.HCorrector + name: HS1MD7R + lattice_names: S1MD7R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: -0.00553438 + unit: 1/m + powerconverter: (HS1PD7R:rdbk, HS1PD7R:set)[A] + hardware_unit: A +- class: pyaml.magnet.hcorrector.HCorrector + name: HS4M1D7R + lattice_names: S4M1D7R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: -0.0044502 + unit: 1/m + powerconverter: (HS4P1D7R:rdbk, HS4P1D7R:set)[A] + hardware_unit: A +- class: pyaml.magnet.hcorrector.HCorrector + name: HS4M2D7R + lattice_names: S4M2D7R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: -0.0044502 + unit: 1/m + powerconverter: (HS4P2D7R:rdbk, HS4P2D7R:set)[A] + hardware_unit: A +- class: pyaml.magnet.hcorrector.HCorrector + name: HS1MT7R + lattice_names: S1MT7R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: -0.00553438 + unit: 1/m + powerconverter: (HS1PT7R:rdbk, HS1PT7R:set)[A] + hardware_unit: A +- class: pyaml.magnet.hcorrector.HCorrector + name: HS4M1T7R + lattice_names: S4M1T7R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: -0.0044502 + unit: 1/m + powerconverter: (HS4P1T7R:rdbk, HS4P1T7R:set)[A] + hardware_unit: A +- class: pyaml.magnet.hcorrector.HCorrector + name: HS4M2T7R + lattice_names: S4M2T7R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: -0.0044502 + unit: 1/m + powerconverter: (HS4P2T7R:rdbk, HS4P2T7R:set)[A] + hardware_unit: A +- class: pyaml.magnet.hcorrector.HCorrector + name: HS1MD8R + lattice_names: S1MD8R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: -0.00553438 + unit: 1/m + powerconverter: (HS1PD8R:rdbk, HS1PD8R:set)[A] + hardware_unit: A +- class: pyaml.magnet.hcorrector.HCorrector + name: HS4M1D8R + lattice_names: S4M1D8R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: -0.0044502 + unit: 1/m + powerconverter: (HS4P1D8R:rdbk, HS4P1D8R:set)[A] + hardware_unit: A +- class: pyaml.magnet.hcorrector.HCorrector + name: HS4M2D8R + lattice_names: S4M2D8R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: -0.0044502 + unit: 1/m + powerconverter: (HS4P2D8R:rdbk, HS4P2D8R:set)[A] + hardware_unit: A +- class: pyaml.magnet.hcorrector.HCorrector + name: HS1MT8R + lattice_names: S1MT8R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: -0.00553438 + unit: 1/m + powerconverter: (HS1PT8R:rdbk, HS1PT8R:set)[A] + hardware_unit: A +- class: pyaml.magnet.hcorrector.HCorrector + name: HS4M1T8R + lattice_names: S4M1T8R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: -0.0044502 + unit: 1/m + powerconverter: (HS4P1T8R:rdbk, HS4P1T8R:set)[A] + hardware_unit: A +- class: pyaml.magnet.hcorrector.HCorrector + name: HS4M2T8R + lattice_names: S4M2T8R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: -0.0044502 + unit: 1/m + powerconverter: (HS4P2T8R:rdbk, HS4P2T8R:set)[A] + hardware_unit: A +- class: pyaml.magnet.hcorrector.HCorrector + name: HS1MD1R + lattice_names: S1MD1R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: -0.00553438 + unit: 1/m + powerconverter: (HS1PD1R:rdbk, HS1PD1R:set)[A] + hardware_unit: A +- class: pyaml.magnet.hcorrector.HCorrector + name: HS4M1D1R + lattice_names: S4M1D1R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: -0.0044502 + unit: 1/m + powerconverter: (HS4P1D1R:rdbk, HS4P1D1R:set)[A] + hardware_unit: A +- class: pyaml.magnet.vcorrector.VCorrector + name: VS3M2D1R + lattice_names: S3M2D1R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.00297607 + unit: 1/m + powerconverter: (VS3P2D1R:rdbk, VS3P2D1R:set)[A] + hardware_unit: A +- class: pyaml.magnet.vcorrector.VCorrector + name: VS2M2D1R + lattice_names: S2M2D1R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.00297607 + unit: 1/m + powerconverter: (VS2P2D1R:rdbk, VS2P2D1R:set)[A] + hardware_unit: A +- class: pyaml.magnet.vcorrector.VCorrector + name: VS2M1T1R + lattice_names: S2M1T1R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.00297607 + unit: 1/m + powerconverter: (VS2P1T1R:rdbk, VS2P1T1R:set)[A] + hardware_unit: A +- class: pyaml.magnet.vcorrector.VCorrector + name: VS3M1T1R + lattice_names: S3M1T1R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.00297607 + unit: 1/m + powerconverter: (VS3P1T1R:rdbk, VS3P1T1R:set)[A] + hardware_unit: A +- class: pyaml.magnet.vcorrector.VCorrector + name: VS3M2T1R + lattice_names: S3M2T1R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.00297607 + unit: 1/m + powerconverter: (VS3P2T1R:rdbk, VS3P2T1R:set)[A] + hardware_unit: A +- class: pyaml.magnet.vcorrector.VCorrector + name: VS2M2T1R + lattice_names: S2M2T1R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.00297607 + unit: 1/m + powerconverter: (VS2P2T1R:rdbk, VS2P2T1R:set)[A] + hardware_unit: A +- class: pyaml.magnet.vcorrector.VCorrector + name: VS2M1D2R + lattice_names: S2M1D2R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.00297607 + unit: 1/m + powerconverter: (VS2P1D2R:rdbk, VS2P1D2R:set)[A] + hardware_unit: A +- class: pyaml.magnet.vcorrector.VCorrector + name: VS3M1D2R + lattice_names: S3M1D2R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.00297607 + unit: 1/m + powerconverter: (VS3P1D2R:rdbk, VS3P1D2R:set)[A] + hardware_unit: A +- class: pyaml.magnet.vcorrector.VCorrector + name: VS3M2D2R + lattice_names: S3M2D2R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.00297607 + unit: 1/m + powerconverter: (VS3P2D2R:rdbk, VS3P2D2R:set)[A] + hardware_unit: A +- class: pyaml.magnet.vcorrector.VCorrector + name: VS2M2D2R + lattice_names: S2M2D2R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.00297607 + unit: 1/m + powerconverter: (VS2P2D2R:rdbk, VS2P2D2R:set)[A] + hardware_unit: A +- class: pyaml.magnet.vcorrector.VCorrector + name: VS2M1T2R + lattice_names: S2M1T2R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.00297607 + unit: 1/m + powerconverter: (VS2P1T2R:rdbk, VS2P1T2R:set)[A] + hardware_unit: A +- class: pyaml.magnet.vcorrector.VCorrector + name: VS3M1T2R + lattice_names: S3M1T2R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.00297607 + unit: 1/m + powerconverter: (VS3P1T2R:rdbk, VS3P1T2R:set)[A] + hardware_unit: A +- class: pyaml.magnet.vcorrector.VCorrector + name: VS3M2T2R + lattice_names: S3M2T2R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.00297607 + unit: 1/m + powerconverter: (VS3P2T2R:rdbk, VS3P2T2R:set)[A] + hardware_unit: A +- class: pyaml.magnet.vcorrector.VCorrector + name: VS2M2T2R + lattice_names: S2M2T2R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.00297607 + unit: 1/m + powerconverter: (VS2P2T2R:rdbk, VS2P2T2R:set)[A] + hardware_unit: A +- class: pyaml.magnet.vcorrector.VCorrector + name: VS2M1D3R + lattice_names: S2M1D3R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.00297607 + unit: 1/m + powerconverter: (VS2P1D3R:rdbk, VS2P1D3R:set)[A] + hardware_unit: A +- class: pyaml.magnet.vcorrector.VCorrector + name: VS3M1D3R + lattice_names: S3M1D3R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.00297607 + unit: 1/m + powerconverter: (VS3P1D3R:rdbk, VS3P1D3R:set)[A] + hardware_unit: A +- class: pyaml.magnet.vcorrector.VCorrector + name: VS3M2D3R + lattice_names: S3M2D3R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.00297607 + unit: 1/m + powerconverter: (VS3P2D3R:rdbk, VS3P2D3R:set)[A] + hardware_unit: A +- class: pyaml.magnet.vcorrector.VCorrector + name: VS2M2D3R + lattice_names: S2M2D3R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.00297607 + unit: 1/m + powerconverter: (VS2P2D3R:rdbk, VS2P2D3R:set)[A] + hardware_unit: A +- class: pyaml.magnet.vcorrector.VCorrector + name: VS2M1T3R + lattice_names: S2M1T3R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.00297607 + unit: 1/m + powerconverter: (VS2P1T3R:rdbk, VS2P1T3R:set)[A] + hardware_unit: A +- class: pyaml.magnet.vcorrector.VCorrector + name: VS3M1T3R + lattice_names: S3M1T3R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.00297607 + unit: 1/m + powerconverter: (VS3P1T3R:rdbk, VS3P1T3R:set)[A] + hardware_unit: A +- class: pyaml.magnet.vcorrector.VCorrector + name: VS3M2T3R + lattice_names: S3M2T3R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.00297607 + unit: 1/m + powerconverter: (VS3P2T3R:rdbk, VS3P2T3R:set)[A] + hardware_unit: A +- class: pyaml.magnet.vcorrector.VCorrector + name: VS2M2T3R + lattice_names: S2M2T3R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.00297607 + unit: 1/m + powerconverter: (VS2P2T3R:rdbk, VS2P2T3R:set)[A] + hardware_unit: A +- class: pyaml.magnet.vcorrector.VCorrector + name: VS2M1D4R + lattice_names: S2M1D4R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.00297607 + unit: 1/m + powerconverter: (VS2P1D4R:rdbk, VS2P1D4R:set)[A] + hardware_unit: A +- class: pyaml.magnet.vcorrector.VCorrector + name: VS3M1D4R + lattice_names: S3M1D4R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.00297607 + unit: 1/m + powerconverter: (VS3P1D4R:rdbk, VS3P1D4R:set)[A] + hardware_unit: A +- class: pyaml.magnet.vcorrector.VCorrector + name: VS3M2D4R + lattice_names: S3M2D4R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.00297607 + unit: 1/m + powerconverter: (VS3P2D4R:rdbk, VS3P2D4R:set)[A] + hardware_unit: A +- class: pyaml.magnet.vcorrector.VCorrector + name: VS2M2D4R + lattice_names: S2M2D4R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.00297607 + unit: 1/m + powerconverter: (VS2P2D4R:rdbk, VS2P2D4R:set)[A] + hardware_unit: A +- class: pyaml.magnet.vcorrector.VCorrector + name: VS2M1T4R + lattice_names: S2M1T4R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.00297607 + unit: 1/m + powerconverter: (VS2P1T4R:rdbk, VS2P1T4R:set)[A] + hardware_unit: A +- class: pyaml.magnet.vcorrector.VCorrector + name: VS3M1T4R + lattice_names: S3M1T4R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.00297607 + unit: 1/m + powerconverter: (VS3P1T4R:rdbk, VS3P1T4R:set)[A] + hardware_unit: A +- class: pyaml.magnet.vcorrector.VCorrector + name: VS3M2T4R + lattice_names: S3M2T4R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.00297607 + unit: 1/m + powerconverter: (VS3P2T4R:rdbk, VS3P2T4R:set)[A] + hardware_unit: A +- class: pyaml.magnet.vcorrector.VCorrector + name: VS2M2T4R + lattice_names: S2M2T4R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.00297607 + unit: 1/m + powerconverter: (VS2P2T4R:rdbk, VS2P2T4R:set)[A] + hardware_unit: A +- class: pyaml.magnet.vcorrector.VCorrector + name: VS2M1D5R + lattice_names: S2M1D5R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.00297607 + unit: 1/m + powerconverter: (VS2P1D5R:rdbk, VS2P1D5R:set)[A] + hardware_unit: A +- class: pyaml.magnet.vcorrector.VCorrector + name: VS3M1D5R + lattice_names: S3M1D5R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.00297607 + unit: 1/m + powerconverter: (VS3P1D5R:rdbk, VS3P1D5R:set)[A] + hardware_unit: A +- class: pyaml.magnet.vcorrector.VCorrector + name: VS3M2D5R + lattice_names: S3M2D5R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.00297607 + unit: 1/m + powerconverter: (VS3P2D5R:rdbk, VS3P2D5R:set)[A] + hardware_unit: A +- class: pyaml.magnet.vcorrector.VCorrector + name: VS2M2D5R + lattice_names: S2M2D5R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.00297607 + unit: 1/m + powerconverter: (VS2P2D5R:rdbk, VS2P2D5R:set)[A] + hardware_unit: A +- class: pyaml.magnet.vcorrector.VCorrector + name: VS2M1T5R + lattice_names: S2M1T5R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.00297607 + unit: 1/m + powerconverter: (VS2P1T5R:rdbk, VS2P1T5R:set)[A] + hardware_unit: A +- class: pyaml.magnet.vcorrector.VCorrector + name: VS3M1T5R + lattice_names: S3M1T5R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.00297607 + unit: 1/m + powerconverter: (VS3P1T5R:rdbk, VS3P1T5R:set)[A] + hardware_unit: A +- class: pyaml.magnet.vcorrector.VCorrector + name: VS3M2T5R + lattice_names: S3M2T5R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.00297607 + unit: 1/m + powerconverter: (VS3P2T5R:rdbk, VS3P2T5R:set)[A] + hardware_unit: A +- class: pyaml.magnet.vcorrector.VCorrector + name: VS2M2T5R + lattice_names: S2M2T5R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.00297607 + unit: 1/m + powerconverter: (VS2P2T5R:rdbk, VS2P2T5R:set)[A] + hardware_unit: A +- class: pyaml.magnet.vcorrector.VCorrector + name: VS2M1D6R + lattice_names: S2M1D6R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.00297607 + unit: 1/m + powerconverter: (VS2P1D6R:rdbk, VS2P1D6R:set)[A] + hardware_unit: A +- class: pyaml.magnet.vcorrector.VCorrector + name: VS3M1D6R + lattice_names: S3M1D6R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.00297607 + unit: 1/m + powerconverter: (VS3P1D6R:rdbk, VS3P1D6R:set)[A] + hardware_unit: A +- class: pyaml.magnet.vcorrector.VCorrector + name: VS3M2D6R + lattice_names: S3M2D6R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.00297607 + unit: 1/m + powerconverter: (VS3P2D6R:rdbk, VS3P2D6R:set)[A] + hardware_unit: A +- class: pyaml.magnet.vcorrector.VCorrector + name: VS2M2D6R + lattice_names: S2M2D6R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.00297607 + unit: 1/m + powerconverter: (VS2P2D6R:rdbk, VS2P2D6R:set)[A] + hardware_unit: A +- class: pyaml.magnet.vcorrector.VCorrector + name: VS2M1T6R + lattice_names: S2M1T6R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.00297607 + unit: 1/m + powerconverter: (VS2P1T6R:rdbk, VS2P1T6R:set)[A] + hardware_unit: A +- class: pyaml.magnet.vcorrector.VCorrector + name: VS3M1T6R + lattice_names: S3M1T6R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.00297607 + unit: 1/m + powerconverter: (VS3P1T6R:rdbk, VS3P1T6R:set)[A] + hardware_unit: A +- class: pyaml.magnet.vcorrector.VCorrector + name: VS3M2T6R + lattice_names: S3M2T6R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.00297607 + unit: 1/m + powerconverter: (VS3P2T6R:rdbk, VS3P2T6R:set)[A] + hardware_unit: A +- class: pyaml.magnet.vcorrector.VCorrector + name: VS2M2T6R + lattice_names: S2M2T6R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.00297607 + unit: 1/m + powerconverter: (VS2P2T6R:rdbk, VS2P2T6R:set)[A] + hardware_unit: A +- class: pyaml.magnet.vcorrector.VCorrector + name: VS2M1D7R + lattice_names: S2M1D7R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.00297607 + unit: 1/m + powerconverter: (VS2P1D7R:rdbk, VS2P1D7R:set)[A] + hardware_unit: A +- class: pyaml.magnet.vcorrector.VCorrector + name: VS3M1D7R + lattice_names: S3M1D7R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.00297607 + unit: 1/m + powerconverter: (VS3P1D7R:rdbk, VS3P1D7R:set)[A] + hardware_unit: A +- class: pyaml.magnet.vcorrector.VCorrector + name: VS3M2D7R + lattice_names: S3M2D7R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.00297607 + unit: 1/m + powerconverter: (VS3P2D7R:rdbk, VS3P2D7R:set)[A] + hardware_unit: A +- class: pyaml.magnet.vcorrector.VCorrector + name: VS2M2D7R + lattice_names: S2M2D7R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.00297607 + unit: 1/m + powerconverter: (VS2P2D7R:rdbk, VS2P2D7R:set)[A] + hardware_unit: A +- class: pyaml.magnet.vcorrector.VCorrector + name: VS2M1T7R + lattice_names: S2M1T7R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.00297607 + unit: 1/m + powerconverter: (VS2P1T7R:rdbk, VS2P1T7R:set)[A] + hardware_unit: A +- class: pyaml.magnet.vcorrector.VCorrector + name: VS3M1T7R + lattice_names: S3M1T7R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.00297607 + unit: 1/m + powerconverter: (VS3P1T7R:rdbk, VS3P1T7R:set)[A] + hardware_unit: A +- class: pyaml.magnet.vcorrector.VCorrector + name: VS3M2T7R + lattice_names: S3M2T7R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.00297607 + unit: 1/m + powerconverter: (VS3P2T7R:rdbk, VS3P2T7R:set)[A] + hardware_unit: A +- class: pyaml.magnet.vcorrector.VCorrector + name: VS2M2T7R + lattice_names: S2M2T7R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.00297607 + unit: 1/m + powerconverter: (VS2P2T7R:rdbk, VS2P2T7R:set)[A] + hardware_unit: A +- class: pyaml.magnet.vcorrector.VCorrector + name: VS2M1D8R + lattice_names: S2M1D8R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.00297607 + unit: 1/m + powerconverter: (VS2P1D8R:rdbk, VS2P1D8R:set)[A] + hardware_unit: A +- class: pyaml.magnet.vcorrector.VCorrector + name: VS3M1D8R + lattice_names: S3M1D8R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.00297607 + unit: 1/m + powerconverter: (VS3P1D8R:rdbk, VS3P1D8R:set)[A] + hardware_unit: A +- class: pyaml.magnet.vcorrector.VCorrector + name: VS3M2D8R + lattice_names: S3M2D8R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.00297607 + unit: 1/m + powerconverter: (VS3P2D8R:rdbk, VS3P2D8R:set)[A] + hardware_unit: A +- class: pyaml.magnet.vcorrector.VCorrector + name: VS2M2D8R + lattice_names: S2M2D8R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.00297607 + unit: 1/m + powerconverter: (VS2P2D8R:rdbk, VS2P2D8R:set)[A] + hardware_unit: A +- class: pyaml.magnet.vcorrector.VCorrector + name: VS2M1T8R + lattice_names: S2M1T8R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.00297607 + unit: 1/m + powerconverter: (VS2P1T8R:rdbk, VS2P1T8R:set)[A] + hardware_unit: A +- class: pyaml.magnet.vcorrector.VCorrector + name: VS3M1T8R + lattice_names: S3M1T8R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.00297607 + unit: 1/m + powerconverter: (VS3P1T8R:rdbk, VS3P1T8R:set)[A] + hardware_unit: A +- class: pyaml.magnet.vcorrector.VCorrector + name: VS3M2T8R + lattice_names: S3M2T8R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.00297607 + unit: 1/m + powerconverter: (VS3P2T8R:rdbk, VS3P2T8R:set)[A] + hardware_unit: A +- class: pyaml.magnet.vcorrector.VCorrector + name: VS2M2T8R + lattice_names: S2M2T8R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.00297607 + unit: 1/m + powerconverter: (VS2P2T8R:rdbk, VS2P2T8R:set)[A] + hardware_unit: A +- class: pyaml.magnet.vcorrector.VCorrector + name: VS2M1D1R + lattice_names: S2M1D1R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.00297607 + unit: 1/m + powerconverter: (VS2P1D1R:rdbk, VS2P1D1R:set)[A] + hardware_unit: A +- class: pyaml.magnet.vcorrector.VCorrector + name: VS3M1D1R + lattice_names: S3M1D1R@0 + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.00297607 + unit: 1/m + powerconverter: (VS3P1D1R:rdbk, VS3P1D1R:set)[A] + hardware_unit: A +- class: pyaml.bpm.bpm.BPM + name: BPMZ5D1R + x_pos: ORBITCC:rdPos@0 + y_pos: ORBITCC:rdPos@1 +- class: pyaml.bpm.bpm.BPM + name: BPMZ6D1R + x_pos: ORBITCC:rdPos@2 + y_pos: ORBITCC:rdPos@3 +- class: pyaml.bpm.bpm.BPM + name: BPMZ7D1R + x_pos: ORBITCC:rdPos@4 + y_pos: ORBITCC:rdPos@5 +- class: pyaml.bpm.bpm.BPM + name: BPMZ1T1R + x_pos: ORBITCC:rdPos@6 + y_pos: ORBITCC:rdPos@7 +- class: pyaml.bpm.bpm.BPM + name: BPMZ2T1R + x_pos: ORBITCC:rdPos@8 + y_pos: ORBITCC:rdPos@9 +- class: pyaml.bpm.bpm.BPM + name: BPMZ3T1R + x_pos: ORBITCC:rdPos@10 + y_pos: ORBITCC:rdPos@11 +- class: pyaml.bpm.bpm.BPM + name: BPMZ4T1R + x_pos: ORBITCC:rdPos@12 + y_pos: ORBITCC:rdPos@13 +- class: pyaml.bpm.bpm.BPM + name: BPMZ41T1R + x_pos: ORBITCC:rdPos@14 + y_pos: ORBITCC:rdPos@15 +- class: pyaml.bpm.bpm.BPM + name: BPMZ5T1R + x_pos: ORBITCC:rdPos@16 + y_pos: ORBITCC:rdPos@17 +- class: pyaml.bpm.bpm.BPM + name: BPMZ6T1R + x_pos: ORBITCC:rdPos@18 + y_pos: ORBITCC:rdPos@19 +- class: pyaml.bpm.bpm.BPM + name: BPMZ7T1R + x_pos: ORBITCC:rdPos@20 + y_pos: ORBITCC:rdPos@21 +- class: pyaml.bpm.bpm.BPM + name: BPMZ1D2R + x_pos: ORBITCC:rdPos@22 + y_pos: ORBITCC:rdPos@23 +- class: pyaml.bpm.bpm.BPM + name: BPMZ2D2R + x_pos: ORBITCC:rdPos@24 + y_pos: ORBITCC:rdPos@25 +- class: pyaml.bpm.bpm.BPM + name: BPMZ3D2R + x_pos: ORBITCC:rdPos@26 + y_pos: ORBITCC:rdPos@27 +- class: pyaml.bpm.bpm.BPM + name: BPMZ4D2R + x_pos: ORBITCC:rdPos@28 + y_pos: ORBITCC:rdPos@29 +- class: pyaml.bpm.bpm.BPM + name: BPMZ5D2R + x_pos: ORBITCC:rdPos@30 + y_pos: ORBITCC:rdPos@31 +- class: pyaml.bpm.bpm.BPM + name: BPMZ6D2R + x_pos: ORBITCC:rdPos@32 + y_pos: ORBITCC:rdPos@33 +- class: pyaml.bpm.bpm.BPM + name: BPMZ7D2R + x_pos: ORBITCC:rdPos@34 + y_pos: ORBITCC:rdPos@35 +- class: pyaml.bpm.bpm.BPM + name: BPMZ1T2R + x_pos: ORBITCC:rdPos@36 + y_pos: ORBITCC:rdPos@37 +- class: pyaml.bpm.bpm.BPM + name: BPMZ2T2R + x_pos: ORBITCC:rdPos@38 + y_pos: ORBITCC:rdPos@39 +- class: pyaml.bpm.bpm.BPM + name: BPMZ3T2R + x_pos: ORBITCC:rdPos@40 + y_pos: ORBITCC:rdPos@41 +- class: pyaml.bpm.bpm.BPM + name: BPMZ4T2R + x_pos: ORBITCC:rdPos@42 + y_pos: ORBITCC:rdPos@43 +- class: pyaml.bpm.bpm.BPM + name: BPMZ41T2R + x_pos: ORBITCC:rdPos@44 + y_pos: ORBITCC:rdPos@45 +- class: pyaml.bpm.bpm.BPM + name: BPMZ42T2R + x_pos: ORBITCC:rdPos@46 + y_pos: ORBITCC:rdPos@47 +- class: pyaml.bpm.bpm.BPM + name: BPMZ43T2R + x_pos: ORBITCC:rdPos@48 + y_pos: ORBITCC:rdPos@49 +- class: pyaml.bpm.bpm.BPM + name: BPMZ5T2R + x_pos: ORBITCC:rdPos@50 + y_pos: ORBITCC:rdPos@51 +- class: pyaml.bpm.bpm.BPM + name: BPMZ6T2R + x_pos: ORBITCC:rdPos@52 + y_pos: ORBITCC:rdPos@53 +- class: pyaml.bpm.bpm.BPM + name: BPMZ7T2R + x_pos: ORBITCC:rdPos@54 + y_pos: ORBITCC:rdPos@55 +- class: pyaml.bpm.bpm.BPM + name: BPMZ1D3R + x_pos: ORBITCC:rdPos@56 + y_pos: ORBITCC:rdPos@57 +- class: pyaml.bpm.bpm.BPM + name: BPMZ2D3R + x_pos: ORBITCC:rdPos@58 + y_pos: ORBITCC:rdPos@59 +- class: pyaml.bpm.bpm.BPM + name: BPMZ3D3R + x_pos: ORBITCC:rdPos@60 + y_pos: ORBITCC:rdPos@61 +- class: pyaml.bpm.bpm.BPM + name: BPMZ4D3R + x_pos: ORBITCC:rdPos@62 + y_pos: ORBITCC:rdPos@63 +- class: pyaml.bpm.bpm.BPM + name: BPMZ5D3R + x_pos: ORBITCC:rdPos@64 + y_pos: ORBITCC:rdPos@65 +- class: pyaml.bpm.bpm.BPM + name: BPMZ6D3R + x_pos: ORBITCC:rdPos@66 + y_pos: ORBITCC:rdPos@67 +- class: pyaml.bpm.bpm.BPM + name: BPMZ7D3R + x_pos: ORBITCC:rdPos@68 + y_pos: ORBITCC:rdPos@69 +- class: pyaml.bpm.bpm.BPM + name: BPMZ1T3R + x_pos: ORBITCC:rdPos@70 + y_pos: ORBITCC:rdPos@71 +- class: pyaml.bpm.bpm.BPM + name: BPMZ2T3R + x_pos: ORBITCC:rdPos@72 + y_pos: ORBITCC:rdPos@73 +- class: pyaml.bpm.bpm.BPM + name: BPMZ3T3R + x_pos: ORBITCC:rdPos@74 + y_pos: ORBITCC:rdPos@75 +- class: pyaml.bpm.bpm.BPM + name: BPMZ4T3R + x_pos: ORBITCC:rdPos@76 + y_pos: ORBITCC:rdPos@77 +- class: pyaml.bpm.bpm.BPM + name: BPMZ5T3R + x_pos: ORBITCC:rdPos@78 + y_pos: ORBITCC:rdPos@79 +- class: pyaml.bpm.bpm.BPM + name: BPMZ6T3R + x_pos: ORBITCC:rdPos@80 + y_pos: ORBITCC:rdPos@81 +- class: pyaml.bpm.bpm.BPM + name: BPMZ7T3R + x_pos: ORBITCC:rdPos@82 + y_pos: ORBITCC:rdPos@83 +- class: pyaml.bpm.bpm.BPM + name: BPMZ1D4R + x_pos: ORBITCC:rdPos@84 + y_pos: ORBITCC:rdPos@85 +- class: pyaml.bpm.bpm.BPM + name: BPMZ2D4R + x_pos: ORBITCC:rdPos@86 + y_pos: ORBITCC:rdPos@87 +- class: pyaml.bpm.bpm.BPM + name: BPMZ3D4R + x_pos: ORBITCC:rdPos@88 + y_pos: ORBITCC:rdPos@89 +- class: pyaml.bpm.bpm.BPM + name: BPMZ4D4R + x_pos: ORBITCC:rdPos@90 + y_pos: ORBITCC:rdPos@91 +- class: pyaml.bpm.bpm.BPM + name: BPMZ5D4R + x_pos: ORBITCC:rdPos@92 + y_pos: ORBITCC:rdPos@93 +- class: pyaml.bpm.bpm.BPM + name: BPMZ6D4R + x_pos: ORBITCC:rdPos@94 + y_pos: ORBITCC:rdPos@95 +- class: pyaml.bpm.bpm.BPM + name: BPMZ7D4R + x_pos: ORBITCC:rdPos@96 + y_pos: ORBITCC:rdPos@97 +- class: pyaml.bpm.bpm.BPM + name: BPMZ1T4R + x_pos: ORBITCC:rdPos@98 + y_pos: ORBITCC:rdPos@99 +- class: pyaml.bpm.bpm.BPM + name: BPMZ2T4R + x_pos: ORBITCC:rdPos@100 + y_pos: ORBITCC:rdPos@101 +- class: pyaml.bpm.bpm.BPM + name: BPMZ3T4R + x_pos: ORBITCC:rdPos@102 + y_pos: ORBITCC:rdPos@103 +- class: pyaml.bpm.bpm.BPM + name: BPMZ4T4R + x_pos: ORBITCC:rdPos@104 + y_pos: ORBITCC:rdPos@105 +- class: pyaml.bpm.bpm.BPM + name: BPMZ5T4R + x_pos: ORBITCC:rdPos@106 + y_pos: ORBITCC:rdPos@107 +- class: pyaml.bpm.bpm.BPM + name: BPMZ6T4R + x_pos: ORBITCC:rdPos@108 + y_pos: ORBITCC:rdPos@109 +- class: pyaml.bpm.bpm.BPM + name: BPMZ7T4R + x_pos: ORBITCC:rdPos@110 + y_pos: ORBITCC:rdPos@111 +- class: pyaml.bpm.bpm.BPM + name: BPMZ1D5R + x_pos: ORBITCC:rdPos@112 + y_pos: ORBITCC:rdPos@113 +- class: pyaml.bpm.bpm.BPM + name: BPMZ2D5R + x_pos: ORBITCC:rdPos@114 + y_pos: ORBITCC:rdPos@115 +- class: pyaml.bpm.bpm.BPM + name: BPMZ3D5R + x_pos: ORBITCC:rdPos@116 + y_pos: ORBITCC:rdPos@117 +- class: pyaml.bpm.bpm.BPM + name: BPMZ4D5R + x_pos: ORBITCC:rdPos@118 + y_pos: ORBITCC:rdPos@119 +- class: pyaml.bpm.bpm.BPM + name: BPMZ5D5R + x_pos: ORBITCC:rdPos@120 + y_pos: ORBITCC:rdPos@121 +- class: pyaml.bpm.bpm.BPM + name: BPMZ6D5R + x_pos: ORBITCC:rdPos@122 + y_pos: ORBITCC:rdPos@123 +- class: pyaml.bpm.bpm.BPM + name: BPMZ7D5R + x_pos: ORBITCC:rdPos@124 + y_pos: ORBITCC:rdPos@125 +- class: pyaml.bpm.bpm.BPM + name: BPMZ1T5R + x_pos: ORBITCC:rdPos@126 + y_pos: ORBITCC:rdPos@127 +- class: pyaml.bpm.bpm.BPM + name: BPMZ2T5R + x_pos: ORBITCC:rdPos@128 + y_pos: ORBITCC:rdPos@129 +- class: pyaml.bpm.bpm.BPM + name: BPMZ3T5R + x_pos: ORBITCC:rdPos@130 + y_pos: ORBITCC:rdPos@131 +- class: pyaml.bpm.bpm.BPM + name: BPMZ4T5R + x_pos: ORBITCC:rdPos@132 + y_pos: ORBITCC:rdPos@133 +- class: pyaml.bpm.bpm.BPM + name: BPMZ5T5R + x_pos: ORBITCC:rdPos@134 + y_pos: ORBITCC:rdPos@135 +- class: pyaml.bpm.bpm.BPM + name: BPMZ6T5R + x_pos: ORBITCC:rdPos@136 + y_pos: ORBITCC:rdPos@137 +- class: pyaml.bpm.bpm.BPM + name: BPMZ7T5R + x_pos: ORBITCC:rdPos@138 + y_pos: ORBITCC:rdPos@139 +- class: pyaml.bpm.bpm.BPM + name: BPMZ1D6R + x_pos: ORBITCC:rdPos@140 + y_pos: ORBITCC:rdPos@141 +- class: pyaml.bpm.bpm.BPM + name: BPMZ2D6R + x_pos: ORBITCC:rdPos@142 + y_pos: ORBITCC:rdPos@143 +- class: pyaml.bpm.bpm.BPM + name: BPMZ3D6R + x_pos: ORBITCC:rdPos@144 + y_pos: ORBITCC:rdPos@145 +- class: pyaml.bpm.bpm.BPM + name: BPMZ4D6R + x_pos: ORBITCC:rdPos@146 + y_pos: ORBITCC:rdPos@147 +- class: pyaml.bpm.bpm.BPM + name: BPMZ41D6R + x_pos: ORBITCC:rdPos@148 + y_pos: ORBITCC:rdPos@149 +- class: pyaml.bpm.bpm.BPM + name: BPMZ42D6R + x_pos: ORBITCC:rdPos@150 + y_pos: ORBITCC:rdPos@151 +- class: pyaml.bpm.bpm.BPM + name: BPMZ43D6R + x_pos: ORBITCC:rdPos@152 + y_pos: ORBITCC:rdPos@153 +- class: pyaml.bpm.bpm.BPM + name: BPMZ44D6R + x_pos: ORBITCC:rdPos@154 + y_pos: ORBITCC:rdPos@155 +- class: pyaml.bpm.bpm.BPM + name: BPMZ6D6R + x_pos: ORBITCC:rdPos@156 + y_pos: ORBITCC:rdPos@157 +- class: pyaml.bpm.bpm.BPM + name: BPMZ7D6R + x_pos: ORBITCC:rdPos@158 + y_pos: ORBITCC:rdPos@159 +- class: pyaml.bpm.bpm.BPM + name: BPMZ1T6R + x_pos: ORBITCC:rdPos@160 + y_pos: ORBITCC:rdPos@161 +- class: pyaml.bpm.bpm.BPM + name: BPMZ2T6R + x_pos: ORBITCC:rdPos@162 + y_pos: ORBITCC:rdPos@163 +- class: pyaml.bpm.bpm.BPM + name: BPMZ3T6R + x_pos: ORBITCC:rdPos@164 + y_pos: ORBITCC:rdPos@165 +- class: pyaml.bpm.bpm.BPM + name: BPMZ4T6R + x_pos: ORBITCC:rdPos@166 + y_pos: ORBITCC:rdPos@167 +- class: pyaml.bpm.bpm.BPM + name: BPMZ41T6R + x_pos: ORBITCC:rdPos@168 + y_pos: ORBITCC:rdPos@169 +- class: pyaml.bpm.bpm.BPM + name: BPMZ5T6R + x_pos: ORBITCC:rdPos@170 + y_pos: ORBITCC:rdPos@171 +- class: pyaml.bpm.bpm.BPM + name: BPMZ6T6R + x_pos: ORBITCC:rdPos@172 + y_pos: ORBITCC:rdPos@173 +- class: pyaml.bpm.bpm.BPM + name: BPMZ7T6R + x_pos: ORBITCC:rdPos@174 + y_pos: ORBITCC:rdPos@175 +- class: pyaml.bpm.bpm.BPM + name: BPMZ1D7R + x_pos: ORBITCC:rdPos@176 + y_pos: ORBITCC:rdPos@177 +- class: pyaml.bpm.bpm.BPM + name: BPMZ2D7R + x_pos: ORBITCC:rdPos@178 + y_pos: ORBITCC:rdPos@179 +- class: pyaml.bpm.bpm.BPM + name: BPMZ3D7R + x_pos: ORBITCC:rdPos@180 + y_pos: ORBITCC:rdPos@181 +- class: pyaml.bpm.bpm.BPM + name: BPMZ4D7R + x_pos: ORBITCC:rdPos@182 + y_pos: ORBITCC:rdPos@183 +- class: pyaml.bpm.bpm.BPM + name: BPMZ5D7R + x_pos: ORBITCC:rdPos@184 + y_pos: ORBITCC:rdPos@185 +- class: pyaml.bpm.bpm.BPM + name: BPMZ6D7R + x_pos: ORBITCC:rdPos@186 + y_pos: ORBITCC:rdPos@187 +- class: pyaml.bpm.bpm.BPM + name: BPMZ7D7R + x_pos: ORBITCC:rdPos@188 + y_pos: ORBITCC:rdPos@189 +- class: pyaml.bpm.bpm.BPM + name: BPMZ1T7R + x_pos: ORBITCC:rdPos@190 + y_pos: ORBITCC:rdPos@191 +- class: pyaml.bpm.bpm.BPM + name: BPMZ2T7R + x_pos: ORBITCC:rdPos@192 + y_pos: ORBITCC:rdPos@193 +- class: pyaml.bpm.bpm.BPM + name: BPMZ3T7R + x_pos: ORBITCC:rdPos@194 + y_pos: ORBITCC:rdPos@195 +- class: pyaml.bpm.bpm.BPM + name: BPMZ4T7R + x_pos: ORBITCC:rdPos@196 + y_pos: ORBITCC:rdPos@197 +- class: pyaml.bpm.bpm.BPM + name: BPMZ41T7R + x_pos: ORBITCC:rdPos@198 + y_pos: ORBITCC:rdPos@199 +- class: pyaml.bpm.bpm.BPM + name: BPMZ5T7R + x_pos: ORBITCC:rdPos@200 + y_pos: ORBITCC:rdPos@201 +- class: pyaml.bpm.bpm.BPM + name: BPMZ6T7R + x_pos: ORBITCC:rdPos@202 + y_pos: ORBITCC:rdPos@203 +- class: pyaml.bpm.bpm.BPM + name: BPMZ7T7R + x_pos: ORBITCC:rdPos@204 + y_pos: ORBITCC:rdPos@205 +- class: pyaml.bpm.bpm.BPM + name: BPMZ1D8R + x_pos: ORBITCC:rdPos@206 + y_pos: ORBITCC:rdPos@207 +- class: pyaml.bpm.bpm.BPM + name: BPMZ2D8R + x_pos: ORBITCC:rdPos@208 + y_pos: ORBITCC:rdPos@209 +- class: pyaml.bpm.bpm.BPM + name: BPMZ3D8R + x_pos: ORBITCC:rdPos@210 + y_pos: ORBITCC:rdPos@211 +- class: pyaml.bpm.bpm.BPM + name: BPMZ4D8R + x_pos: ORBITCC:rdPos@212 + y_pos: ORBITCC:rdPos@213 +- class: pyaml.bpm.bpm.BPM + name: BPMZ5D8R + x_pos: ORBITCC:rdPos@214 + y_pos: ORBITCC:rdPos@215 +- class: pyaml.bpm.bpm.BPM + name: BPMZ6D8R + x_pos: ORBITCC:rdPos@216 + y_pos: ORBITCC:rdPos@217 +- class: pyaml.bpm.bpm.BPM + name: BPMZ7D8R + x_pos: ORBITCC:rdPos@218 + y_pos: ORBITCC:rdPos@219 +- class: pyaml.bpm.bpm.BPM + name: BPMZ1T8R + x_pos: ORBITCC:rdPos@220 + y_pos: ORBITCC:rdPos@221 +- class: pyaml.bpm.bpm.BPM + name: BPMZ2T8R + x_pos: ORBITCC:rdPos@222 + y_pos: ORBITCC:rdPos@223 +- class: pyaml.bpm.bpm.BPM + name: BPMZ3T8R + x_pos: ORBITCC:rdPos@224 + y_pos: ORBITCC:rdPos@225 +- class: pyaml.bpm.bpm.BPM + name: BPMZ4T8R + x_pos: ORBITCC:rdPos@226 + y_pos: ORBITCC:rdPos@227 +- class: pyaml.bpm.bpm.BPM + name: BPMZ5T8R + x_pos: ORBITCC:rdPos@228 + y_pos: ORBITCC:rdPos@229 +- class: pyaml.bpm.bpm.BPM + name: BPMZ6T8R + x_pos: ORBITCC:rdPos@230 + y_pos: ORBITCC:rdPos@231 +- class: pyaml.bpm.bpm.BPM + name: BPMZ7T8R + x_pos: ORBITCC:rdPos@232 + y_pos: ORBITCC:rdPos@233 +- class: pyaml.bpm.bpm.BPM + name: BPMZ1D1R + x_pos: ORBITCC:rdPos@234 + y_pos: ORBITCC:rdPos@235 +- class: pyaml.bpm.bpm.BPM + name: BPMZ2D1R + x_pos: ORBITCC:rdPos@236 + y_pos: ORBITCC:rdPos@237 +- class: pyaml.bpm.bpm.BPM + name: BPMZ3D1R + x_pos: ORBITCC:rdPos@238 + y_pos: ORBITCC:rdPos@239 +- class: pyaml.bpm.bpm.BPM + name: BPMZ4D1R + x_pos: ORBITCC:rdPos@240 + y_pos: ORBITCC:rdPos@241 +- class: pyaml.bpm.bpm.BPM + name: BPMZ41D1R + x_pos: ORBITCC:rdPos@242 + y_pos: ORBITCC:rdPos@243 +- class: pyaml.bpm.bpm.BPM + name: BPMZ42D1R + x_pos: ORBITCC:rdPos@244 + y_pos: ORBITCC:rdPos@245 +- class: pyaml.magnet.quadrupole.Quadrupole + name: Q3M1D1R + lattice_names: Q3M1D1R + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: -0.0158575 + unit: 1/m + powerconverter: (Q3PD1R:rdbk, Q3PD1R:set)[A] + hardware_unit: A +- class: pyaml.magnet.quadrupole.Quadrupole + name: Q3M2D1R + lattice_names: Q3M2D1R + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: -0.0158575 + unit: 1/m + powerconverter: (Q3PD1R:rdbk, Q3PD1R:set)[A] + hardware_unit: A +- class: pyaml.magnet.quadrupole.Quadrupole + name: Q3M1T1R + lattice_names: Q3M1T1R + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: -0.015735 + unit: 1/m + powerconverter: (Q3P1T1R:rdbk, Q3P1T1R:set)[A] + hardware_unit: A +- class: pyaml.magnet.quadrupole.Quadrupole + name: Q3M2T1R + lattice_names: Q3M2T1R + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: -0.015735 + unit: 1/m + powerconverter: (Q3P2T1R:rdbk, Q3P2T1R:set)[A] + hardware_unit: A +- class: pyaml.magnet.quadrupole.Quadrupole + name: Q3M1D2R + lattice_names: Q3M1D2R + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: -0.0158575 + unit: 1/m + powerconverter: (Q3PD2R:rdbk, Q3PD2R:set)[A] + hardware_unit: A +- class: pyaml.magnet.quadrupole.Quadrupole + name: Q3M2D2R + lattice_names: Q3M2D2R + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: -0.0158575 + unit: 1/m + powerconverter: (Q3PD2R:rdbk, Q3PD2R:set)[A] + hardware_unit: A +- class: pyaml.magnet.quadrupole.Quadrupole + name: Q3M1T2R + lattice_names: Q3M1T2R + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: -0.015735 + unit: 1/m + powerconverter: (Q3PT2R:rdbk, Q3PT2R:set)[A] + hardware_unit: A +- class: pyaml.magnet.quadrupole.Quadrupole + name: Q3M2T2R + lattice_names: Q3M2T2R + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: -0.015735 + unit: 1/m + powerconverter: (Q3PT2R:rdbk, Q3PT2R:set)[A] + hardware_unit: A +- class: pyaml.magnet.quadrupole.Quadrupole + name: Q3M1D3R + lattice_names: Q3M1D3R + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: -0.0158575 + unit: 1/m + powerconverter: (Q3PD3R:rdbk, Q3PD3R:set)[A] + hardware_unit: A +- class: pyaml.magnet.quadrupole.Quadrupole + name: Q3M2D3R + lattice_names: Q3M2D3R + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: -0.0158575 + unit: 1/m + powerconverter: (Q3PD3R:rdbk, Q3PD3R:set)[A] + hardware_unit: A +- class: pyaml.magnet.quadrupole.Quadrupole + name: Q3M1T3R + lattice_names: Q3M1T3R + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: -0.015735 + unit: 1/m + powerconverter: (Q3PT3R:rdbk, Q3PT3R:set)[A] + hardware_unit: A +- class: pyaml.magnet.quadrupole.Quadrupole + name: Q3M2T3R + lattice_names: Q3M2T3R + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: -0.015735 + unit: 1/m + powerconverter: (Q3PT3R:rdbk, Q3PT3R:set)[A] + hardware_unit: A +- class: pyaml.magnet.quadrupole.Quadrupole + name: Q3M1D4R + lattice_names: Q3M1D4R + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: -0.0158575 + unit: 1/m + powerconverter: (Q3PD4R:rdbk, Q3PD4R:set)[A] + hardware_unit: A +- class: pyaml.magnet.quadrupole.Quadrupole + name: Q3M2D4R + lattice_names: Q3M2D4R + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: -0.0158575 + unit: 1/m + powerconverter: (Q3PD4R:rdbk, Q3PD4R:set)[A] + hardware_unit: A +- class: pyaml.magnet.quadrupole.Quadrupole + name: Q3M1T4R + lattice_names: Q3M1T4R + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: -0.015735 + unit: 1/m + powerconverter: (Q3PT4R:rdbk, Q3PT4R:set)[A] + hardware_unit: A +- class: pyaml.magnet.quadrupole.Quadrupole + name: Q3M2T4R + lattice_names: Q3M2T4R + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: -0.015735 + unit: 1/m + powerconverter: (Q3PT4R:rdbk, Q3PT4R:set)[A] + hardware_unit: A +- class: pyaml.magnet.quadrupole.Quadrupole + name: Q3M1D5R + lattice_names: Q3M1D5R + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: -0.0158575 + unit: 1/m + powerconverter: (Q3PD5R:rdbk, Q3PD5R:set)[A] + hardware_unit: A +- class: pyaml.magnet.quadrupole.Quadrupole + name: Q3M2D5R + lattice_names: Q3M2D5R + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: -0.0158575 + unit: 1/m + powerconverter: (Q3PD5R:rdbk, Q3PD5R:set)[A] + hardware_unit: A +- class: pyaml.magnet.quadrupole.Quadrupole + name: Q3M1T5R + lattice_names: Q3M1T5R + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: -0.015735 + unit: 1/m + powerconverter: (Q3PT5R:rdbk, Q3PT5R:set)[A] + hardware_unit: A +- class: pyaml.magnet.quadrupole.Quadrupole + name: Q3M2T5R + lattice_names: Q3M2T5R + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: -0.015735 + unit: 1/m + powerconverter: (Q3PT5R:rdbk, Q3PT5R:set)[A] + hardware_unit: A +- class: pyaml.magnet.quadrupole.Quadrupole + name: Q3M1D6R + lattice_names: Q3M1D6R + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: -0.0158575 + unit: 1/m + powerconverter: (Q3PD6R:rdbk, Q3PD6R:set)[A] + hardware_unit: A +- class: pyaml.magnet.quadrupole.Quadrupole + name: Q3M2D6R + lattice_names: Q3M2D6R + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: -0.0158575 + unit: 1/m + powerconverter: (Q3PD6R:rdbk, Q3PD6R:set)[A] + hardware_unit: A +- class: pyaml.magnet.quadrupole.Quadrupole + name: Q3M1T6R + lattice_names: Q3M1T6R + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: -0.015735 + unit: 1/m + powerconverter: (Q3P1T6R:rdbk, Q3P1T6R:set)[A] + hardware_unit: A +- class: pyaml.magnet.quadrupole.Quadrupole + name: Q3M2T6R + lattice_names: Q3M2T6R + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: -0.015735 + unit: 1/m + powerconverter: (Q3P2T6R:rdbk, Q3P2T6R:set)[A] + hardware_unit: A +- class: pyaml.magnet.quadrupole.Quadrupole + name: Q3M1D7R + lattice_names: Q3M1D7R + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: -0.0158575 + unit: 1/m + powerconverter: (Q3PD7R:rdbk, Q3PD7R:set)[A] + hardware_unit: A +- class: pyaml.magnet.quadrupole.Quadrupole + name: Q3M2D7R + lattice_names: Q3M2D7R + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: -0.0158575 + unit: 1/m + powerconverter: (Q3PD7R:rdbk, Q3PD7R:set)[A] + hardware_unit: A +- class: pyaml.magnet.quadrupole.Quadrupole + name: Q3M1T7R + lattice_names: Q3M1T7R + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: -0.015735 + unit: 1/m + powerconverter: (Q3PT7R:rdbk, Q3PT7R:set)[A] + hardware_unit: A +- class: pyaml.magnet.quadrupole.Quadrupole + name: Q3M2T7R + lattice_names: Q3M2T7R + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: -0.015735 + unit: 1/m + powerconverter: (Q3PT7R:rdbk, Q3PT7R:set)[A] + hardware_unit: A +- class: pyaml.magnet.quadrupole.Quadrupole + name: Q3M1D8R + lattice_names: Q3M1D8R + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: -0.0158575 + unit: 1/m + powerconverter: (Q3PD8R:rdbk, Q3PD8R:set)[A] + hardware_unit: A +- class: pyaml.magnet.quadrupole.Quadrupole + name: Q3M2D8R + lattice_names: Q3M2D8R + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: -0.0158575 + unit: 1/m + powerconverter: (Q3PD8R:rdbk, Q3PD8R:set)[A] + hardware_unit: A +- class: pyaml.magnet.quadrupole.Quadrupole + name: Q3M1T8R + lattice_names: Q3M1T8R + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: -0.015735 + unit: 1/m + powerconverter: (Q3P1T8R:rdbk, Q3P1T8R:set)[A] + hardware_unit: A +- class: pyaml.magnet.quadrupole.Quadrupole + name: Q3M2T8R + lattice_names: Q3M2T8R + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: -0.015735 + unit: 1/m + powerconverter: (Q3P2T8R:rdbk, Q3P2T8R:set)[A] + hardware_unit: A +- class: pyaml.magnet.quadrupole.Quadrupole + name: Q4M1D1R + lattice_names: Q4M1D1R + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.0303165 + unit: 1/m + powerconverter: (Q4PD1R:rdbk, Q4PD1R:set)[A] + hardware_unit: A +- class: pyaml.magnet.quadrupole.Quadrupole + name: Q4M2D1R + lattice_names: Q4M2D1R + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.0303165 + unit: 1/m + powerconverter: (Q4PD1R:rdbk, Q4PD1R:set)[A] + hardware_unit: A +- class: pyaml.magnet.quadrupole.Quadrupole + name: Q4M1T1R + lattice_names: Q4M1T1R + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.0296695 + unit: 1/m + powerconverter: (Q4P1T1R:rdbk, Q4P1T1R:set)[A] + hardware_unit: A +- class: pyaml.magnet.quadrupole.Quadrupole + name: Q4M2T1R + lattice_names: Q4M2T1R + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.0296695 + unit: 1/m + powerconverter: (Q4P2T1R:rdbk, Q4P2T1R:set)[A] + hardware_unit: A +- class: pyaml.magnet.quadrupole.Quadrupole + name: Q4M1D2R + lattice_names: Q4M1D2R + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.0303165 + unit: 1/m + powerconverter: (Q4PD2R:rdbk, Q4PD2R:set)[A] + hardware_unit: A +- class: pyaml.magnet.quadrupole.Quadrupole + name: Q4M2D2R + lattice_names: Q4M2D2R + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.0303165 + unit: 1/m + powerconverter: (Q4PD2R:rdbk, Q4PD2R:set)[A] + hardware_unit: A +- class: pyaml.magnet.quadrupole.Quadrupole + name: Q4M1T2R + lattice_names: Q4M1T2R + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.0296695 + unit: 1/m + powerconverter: (Q4PT2R:rdbk, Q4PT2R:set)[A] + hardware_unit: A +- class: pyaml.magnet.quadrupole.Quadrupole + name: Q4M2T2R + lattice_names: Q4M2T2R + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.0296695 + unit: 1/m + powerconverter: (Q4PT2R:rdbk, Q4PT2R:set)[A] + hardware_unit: A +- class: pyaml.magnet.quadrupole.Quadrupole + name: Q4M1D3R + lattice_names: Q4M1D3R + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.0303165 + unit: 1/m + powerconverter: (Q4PD3R:rdbk, Q4PD3R:set)[A] + hardware_unit: A +- class: pyaml.magnet.quadrupole.Quadrupole + name: Q4M2D3R + lattice_names: Q4M2D3R + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.0303165 + unit: 1/m + powerconverter: (Q4PD3R:rdbk, Q4PD3R:set)[A] + hardware_unit: A +- class: pyaml.magnet.quadrupole.Quadrupole + name: Q4M1T3R + lattice_names: Q4M1T3R + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.0296695 + unit: 1/m + powerconverter: (Q4PT3R:rdbk, Q4PT3R:set)[A] + hardware_unit: A +- class: pyaml.magnet.quadrupole.Quadrupole + name: Q4M2T3R + lattice_names: Q4M2T3R + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.0296695 + unit: 1/m + powerconverter: (Q4PT3R:rdbk, Q4PT3R:set)[A] + hardware_unit: A +- class: pyaml.magnet.quadrupole.Quadrupole + name: Q4M1D4R + lattice_names: Q4M1D4R + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.0303165 + unit: 1/m + powerconverter: (Q4PD4R:rdbk, Q4PD4R:set)[A] + hardware_unit: A +- class: pyaml.magnet.quadrupole.Quadrupole + name: Q4M2D4R + lattice_names: Q4M2D4R + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.0303165 + unit: 1/m + powerconverter: (Q4PD4R:rdbk, Q4PD4R:set)[A] + hardware_unit: A +- class: pyaml.magnet.quadrupole.Quadrupole + name: Q4M1T4R + lattice_names: Q4M1T4R + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.0296695 + unit: 1/m + powerconverter: (Q4PT4R:rdbk, Q4PT4R:set)[A] + hardware_unit: A +- class: pyaml.magnet.quadrupole.Quadrupole + name: Q4M2T4R + lattice_names: Q4M2T4R + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.0296695 + unit: 1/m + powerconverter: (Q4PT4R:rdbk, Q4PT4R:set)[A] + hardware_unit: A +- class: pyaml.magnet.quadrupole.Quadrupole + name: Q4M1D5R + lattice_names: Q4M1D5R + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.0303165 + unit: 1/m + powerconverter: (Q4PD5R:rdbk, Q4PD5R:set)[A] + hardware_unit: A +- class: pyaml.magnet.quadrupole.Quadrupole + name: Q4M2D5R + lattice_names: Q4M2D5R + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.0303165 + unit: 1/m + powerconverter: (Q4PD5R:rdbk, Q4PD5R:set)[A] + hardware_unit: A +- class: pyaml.magnet.quadrupole.Quadrupole + name: Q4M1T5R + lattice_names: Q4M1T5R + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.0296695 + unit: 1/m + powerconverter: (Q4PT5R:rdbk, Q4PT5R:set)[A] + hardware_unit: A +- class: pyaml.magnet.quadrupole.Quadrupole + name: Q4M2T5R + lattice_names: Q4M2T5R + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.0296695 + unit: 1/m + powerconverter: (Q4PT5R:rdbk, Q4PT5R:set)[A] + hardware_unit: A +- class: pyaml.magnet.quadrupole.Quadrupole + name: Q4M1D6R + lattice_names: Q4M1D6R + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.0303165 + unit: 1/m + powerconverter: (Q4PD6R:rdbk, Q4PD6R:set)[A] + hardware_unit: A +- class: pyaml.magnet.quadrupole.Quadrupole + name: Q4M2D6R + lattice_names: Q4M2D6R + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.0303165 + unit: 1/m + powerconverter: (Q4PD6R:rdbk, Q4PD6R:set)[A] + hardware_unit: A +- class: pyaml.magnet.quadrupole.Quadrupole + name: Q4M1T6R + lattice_names: Q4M1T6R + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.0296695 + unit: 1/m + powerconverter: (Q4P1T6R:rdbk, Q4P1T6R:set)[A] + hardware_unit: A +- class: pyaml.magnet.quadrupole.Quadrupole + name: Q4M2T6R + lattice_names: Q4M2T6R + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.0296695 + unit: 1/m + powerconverter: (Q4P2T6R:rdbk, Q4P2T6R:set)[A] + hardware_unit: A +- class: pyaml.magnet.quadrupole.Quadrupole + name: Q4M1D7R + lattice_names: Q4M1D7R + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.0303165 + unit: 1/m + powerconverter: (Q4PD7R:rdbk, Q4PD7R:set)[A] + hardware_unit: A +- class: pyaml.magnet.quadrupole.Quadrupole + name: Q4M2D7R + lattice_names: Q4M2D7R + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.0303165 + unit: 1/m + powerconverter: (Q4PD7R:rdbk, Q4PD7R:set)[A] + hardware_unit: A +- class: pyaml.magnet.quadrupole.Quadrupole + name: Q4M1T7R + lattice_names: Q4M1T7R + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.0296695 + unit: 1/m + powerconverter: (Q4PT7R:rdbk, Q4PT7R:set)[A] + hardware_unit: A +- class: pyaml.magnet.quadrupole.Quadrupole + name: Q4M2T7R + lattice_names: Q4M2T7R + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.0296695 + unit: 1/m + powerconverter: (Q4PT7R:rdbk, Q4PT7R:set)[A] + hardware_unit: A +- class: pyaml.magnet.quadrupole.Quadrupole + name: Q4M1D8R + lattice_names: Q4M1D8R + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.0303165 + unit: 1/m + powerconverter: (Q4PD8R:rdbk, Q4PD8R:set)[A] + hardware_unit: A +- class: pyaml.magnet.quadrupole.Quadrupole + name: Q4M2D8R + lattice_names: Q4M2D8R + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.0303165 + unit: 1/m + powerconverter: (Q4PD8R:rdbk, Q4PD8R:set)[A] + hardware_unit: A +- class: pyaml.magnet.quadrupole.Quadrupole + name: Q4M1T8R + lattice_names: Q4M1T8R + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.0296695 + unit: 1/m + powerconverter: (Q4P1T8R:rdbk, Q4P1T8R:set)[A] + hardware_unit: A +- class: pyaml.magnet.quadrupole.Quadrupole + name: Q4M2T8R + lattice_names: Q4M2T8R + model: + class: pyaml.magnet.linear_model.LinearMagnetModel + calibration_factor: 0.0296695 + unit: 1/m + powerconverter: (Q4P2T8R:rdbk, Q4P2T8R:set)[A] + hardware_unit: A +- class: pyaml.diagnostics.tune_monitor.BetatronTuneMonitor + name: BETATRON_TUNE + tune_h: beam:twiss:x:tune + tune_v: beam:twiss:y:tune +- class: pyaml.tuning_tools.tune.Tune + name: DEFAULT_TUNE_CORRECTION + quad_array_name: QForTune + betatron_tune_name: BETATRON_TUNE + response_matrix: ${path:trm.json} +- class: pyaml.tuning_tools.tune_response_matrix.TuneResponseMatrix + name: DEFAULT_TUNE_RESPONSE_MATRIX + quad_array_name: QForTune + betatron_tune_name: BETATRON_TUNE + quad_delta: 1e-4 +- class: pyaml.tuning_tools.chromaticity_monitor.ChromaticityMonitor + name: KSI + betatron_tune_name: BETATRON_TUNE + rf_plant_name: RF + fit_order: 2 + n_avg_meas: 1 + n_step: 5 + sleep_between_meas: 2 + sleep_between_step: 2 + e_delta: 1e-3 + max_e_delta: 1e-3 +- class: pyaml.tuning_tools.chromaticity_monitor.ChromaticityMonitor + name: CHROMATICITY_MONITOR + betatron_tune_name: BETATRON_TUNE + rf_plant_name: RF + fit_order: 2 + n_avg_meas: 1 + n_step: 5 + sleep_between_meas: 2 + sleep_between_step: 2 + e_delta: 1e-3 + max_e_delta: 1e-3 diff --git a/examples/BESSY2_example/bessy2_standard_user.mat b/examples/use_cases/config/bessy2/bessy2_standard_user.mat similarity index 100% rename from examples/BESSY2_example/bessy2_standard_user.mat rename to examples/use_cases/config/bessy2/bessy2_standard_user.mat diff --git a/examples/use_cases/config/bessy2/orm.json b/examples/use_cases/config/bessy2/orm.json new file mode 100644 index 000000000..e1f9deb66 --- /dev/null +++ b/examples/use_cases/config/bessy2/orm.json @@ -0,0 +1,28774 @@ +{ + "type": "pyaml.tuning_tools.orbit_response_matrix_data", + "matrix": [ + [ + -16.598148463795624, + 18.080575992708052, + -14.989908252591041, + 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HS4M2T4R +- HS1MD5R +- HS4M1D5R +- HS4M2D5R +- HS1MT5R +- HS4M1T5R +- HS4M2T5R +- HS1MD6R +- HS4M1D6R +- HS4M2D6R +- HS1MT6R +- HS4M1T6R +- HS4M2T6R +- HS1MD7R +- HS4M1D7R +- HS4M2D7R +- HS1MT7R +- HS4M1T7R +- HS4M2T7R +- HS1MD8R +- HS4M1D8R +- HS4M2D8R +- HS1MT8R +- HS4M1T8R +- HS4M2T8R +- HS1MD1R +- HS4M1D1R +- VS3M2D1R +- VS2M2D1R +- VS2M1T1R +- VS3M1T1R +- VS3M2T1R +- VS2M2T1R +- VS2M1D2R +- VS3M1D2R +- VS3M2D2R +- VS2M2D2R +- VS2M1T2R +- VS3M1T2R +- VS3M2T2R +- VS2M2T2R +- VS2M1D3R +- VS3M1D3R +- VS3M2D3R +- VS2M2D3R +- VS2M1T3R +- VS3M1T3R +- VS3M2T3R +- VS2M2T3R +- VS2M1D4R +- VS3M1D4R +- VS3M2D4R +- VS2M2D4R +- VS2M1T4R +- VS3M1T4R +- VS3M2T4R +- VS2M2T4R +- VS2M1D5R +- VS3M1D5R +- VS3M2D5R +- VS2M2D5R +- VS2M1T5R +- VS3M1T5R +- VS3M2T5R +- VS2M2T5R +- VS2M1D6R +- VS3M1D6R +- VS3M2D6R +- VS2M2D6R +- VS2M1T6R +- VS3M1T6R +- VS3M2T6R +- VS2M2T6R +- VS2M1D7R +- VS3M1D7R +- VS3M2D7R +- VS2M2D7R +- VS2M1T7R +- VS3M1T7R +- VS3M2T7R +- VS2M2T7R +- VS2M1D8R +- VS3M1D8R +- VS3M2D8R +- VS2M2D8R +- VS2M1T8R +- VS3M1T8R +- VS3M2T8R +- VS2M2T8R +- VS2M1D1R +- VS3M1D1R +variable_planes: +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V diff --git a/examples/use_cases/config/bessy2/trm.json b/examples/use_cases/config/bessy2/trm.json new file mode 100644 index 000000000..fec237467 --- /dev/null +++ b/examples/use_cases/config/bessy2/trm.json @@ -0,0 +1,207 @@ +{ + "type": "pyaml.tuning_tools.response_matrix_data", + "matrix": [ + [ + 0.29477536239053137, + 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tango.pyaml.static_catalog_entry + key: srdiag/bpm/c03-04/SA_VPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c03-04/SA_VPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c03-05/SA_HPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c03-05/SA_HPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c03-05/SA_VPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c03-05/SA_VPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c03-06/SA_HPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c03-06/SA_HPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c03-06/SA_VPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c03-06/SA_VPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c03-07/SA_HPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c03-07/SA_HPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c03-07/SA_VPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c03-07/SA_VPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c03-08/SA_HPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c03-08/SA_HPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c03-08/SA_VPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c03-08/SA_VPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c03-09/SA_HPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c03-09/SA_HPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c03-09/SA_VPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c03-09/SA_VPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c03-10/SA_HPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c03-10/SA_HPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c03-10/SA_VPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c03-10/SA_VPosition + unit: m diff --git a/examples/use_cases/config/esrf/catalogs/ebs_catalogs.yaml b/examples/use_cases/config/esrf/catalogs/ebs_catalogs.yaml new file mode 100644 index 000000000..d15349d6f --- /dev/null +++ b/examples/use_cases/config/esrf/catalogs/ebs_catalogs.yaml @@ -0,0 +1,8 @@ +type: tango.pyaml.static_catalog +entries: + - catalogs/ebs_bpm_catalogs.yaml + - catalogs/ebs_rf_catalogs.yaml + - catalogs/ebs_diag_catalogs.yaml + - catalogs/ebs_magnets_catalogs.yaml + - catalogs/ebs_sh_catalogs.yaml + - catalogs/ebs_sext_catalogs.yaml diff --git a/examples/use_cases/config/esrf/catalogs/ebs_diag_catalogs.yaml b/examples/use_cases/config/esrf/catalogs/ebs_diag_catalogs.yaml new file mode 100644 index 000000000..84e820625 --- /dev/null +++ b/examples/use_cases/config/esrf/catalogs/ebs_diag_catalogs.yaml @@ -0,0 +1,12 @@ +- type: tango.pyaml.static_catalog_entry + key: srdiag/beam-tune/main/Qh + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/beam-tune/main/Qh + unit: "" +- type: tango.pyaml.static_catalog_entry + key: srdiag/beam-tune/main/Qv + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/beam-tune/main/Qv + unit: "" diff --git a/examples/use_cases/config/esrf/catalogs/ebs_magnets_catalogs.yaml b/examples/use_cases/config/esrf/catalogs/ebs_magnets_catalogs.yaml new file mode 100644 index 000000000..79923fd6c --- /dev/null +++ b/examples/use_cases/config/esrf/catalogs/ebs_magnets_catalogs.yaml @@ -0,0 +1,875 @@ +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qf1/c04-e/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qf1/c04-e/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qf1/c05-a/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qf1/c05-a/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qf1/c05-e/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qf1/c05-e/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qf1/c06-a/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qf1/c06-a/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qf1/c06-e/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qf1/c06-e/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qf1/c07-a/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qf1/c07-a/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qf1/c07-e/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qf1/c07-e/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qf1/c08-a/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qf1/c08-a/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qf1/c08-e/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qf1/c08-e/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qf1/c09-a/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qf1/c09-a/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qf1/c09-e/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qf1/c09-e/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qf1/c10-a/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qf1/c10-a/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qf1/c10-e/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qf1/c10-e/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qf1/c11-a/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qf1/c11-a/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qf1/c11-e/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qf1/c11-e/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qf1/c12-a/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qf1/c12-a/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qf1/c12-e/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qf1/c12-e/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qf1/c13-a/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qf1/c13-a/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qf1/c13-e/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qf1/c13-e/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qf1/c14-a/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qf1/c14-a/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qf1/c14-e/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qf1/c14-e/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qf1/c15-a/current + device: + type: tango.pyaml.attribute + attribute: 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tango.pyaml.static_catalog_entry + key: srmag/vps-qd2/c03-a/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qd2/c03-a/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qf6/c04-b/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qf6/c04-b/current + range: [10,109] + unit: A diff --git a/examples/use_cases/config/esrf/catalogs/ebs_rf_catalogs.yaml b/examples/use_cases/config/esrf/catalogs/ebs_rf_catalogs.yaml new file mode 100644 index 000000000..0739d3526 --- /dev/null +++ b/examples/use_cases/config/esrf/catalogs/ebs_rf_catalogs.yaml @@ -0,0 +1,30 @@ +- type: tango.pyaml.static_catalog_entry + key: sys/ringsimulator/ebs/RfVoltage + device: + type: tango.pyaml.attribute + attribute: sys/ringsimulator/ebs/RfVoltage + unit: V +- type: tango.pyaml.static_catalog_entry + key: sy/ms/1/Frequency + device: + type: tango.pyaml.attribute + attribute: sy/ms/1/Frequency + unit: Hz +- type: tango.pyaml.static_catalog_entry + key: sr/tra/1/RfVoltage + device: + type: tango.pyaml.attribute + attribute: sr/tra/1/RfVoltage + unit: V +- type: tango.pyaml.static_catalog_entry + key: sr/tra/2/RfVoltage + device: + type: tango.pyaml.attribute + attribute: sr/tra/2/RfVoltage + unit: V +- type: tango.pyaml.static_catalog_entry + key: sr/tra/harm/RfVoltage + device: + type: tango.pyaml.attribute + attribute: sr/tra/harm/RfVoltage + unit: V diff --git a/examples/use_cases/config/esrf/catalogs/ebs_sext_catalogs.yaml b/examples/use_cases/config/esrf/catalogs/ebs_sext_catalogs.yaml new file mode 100644 index 000000000..d62c07305 --- /dev/null +++ b/examples/use_cases/config/esrf/catalogs/ebs_sext_catalogs.yaml @@ -0,0 +1,4608 @@ +- type: tango.pyaml.static_catalog_entry + key: srmag/m-sd1/c04-a/Strength_H + device: + type: tango.pyaml.attribute + attribute: srmag/m-sd1/c04-a/Strength_H + unit: rad +- type: tango.pyaml.static_catalog_entry + key: srmag/m-sd1/c04-a/Strength_V + device: + 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srmag/m-sd1/c03-b/Strength_SQ + unit: m-1 +- type: tango.pyaml.static_catalog_entry + key: srmag/m-sd1/c03-b/Strength + device: + type: tango.pyaml.attribute + attribute: srmag/m-sd1/c03-b/Strength + unit: m-2 +- type: tango.pyaml.static_catalog_entry + key: srmag/m-sd1/c03-d/Strength_H + device: + type: tango.pyaml.attribute + attribute: srmag/m-sd1/c03-d/Strength_H + unit: rad +- type: tango.pyaml.static_catalog_entry + key: srmag/m-sd1/c03-d/Strength_V + device: + type: tango.pyaml.attribute + attribute: srmag/m-sd1/c03-d/Strength_V + unit: rad +- type: tango.pyaml.static_catalog_entry + key: srmag/m-sd1/c03-d/Strength_SQ + device: + type: tango.pyaml.attribute + attribute: srmag/m-sd1/c03-d/Strength_SQ + unit: m-1 +- type: tango.pyaml.static_catalog_entry + key: srmag/m-sd1/c03-d/Strength + device: + type: tango.pyaml.attribute + attribute: srmag/m-sd1/c03-d/Strength + unit: m-2 +- type: tango.pyaml.static_catalog_entry + key: srmag/m-sf2/c03-e/Strength_H + device: + type: tango.pyaml.attribute + attribute: srmag/m-sf2/c03-e/Strength_H + unit: rad +- type: tango.pyaml.static_catalog_entry + key: srmag/m-sf2/c03-e/Strength_V + device: + type: tango.pyaml.attribute + attribute: srmag/m-sf2/c03-e/Strength_V + unit: rad +- type: tango.pyaml.static_catalog_entry + key: srmag/m-sf2/c03-e/Strength_SQ + device: + type: tango.pyaml.attribute + attribute: srmag/m-sf2/c03-e/Strength_SQ + unit: m-1 +- type: tango.pyaml.static_catalog_entry + key: srmag/m-sf2/c03-e/Strength + device: + type: tango.pyaml.attribute + attribute: srmag/m-sf2/c03-e/Strength + unit: m-2 +- type: tango.pyaml.static_catalog_entry + key: srmag/m-sd1/c03-e/Strength_H + device: + type: tango.pyaml.attribute + attribute: srmag/m-sd1/c03-e/Strength_H + unit: rad +- type: tango.pyaml.static_catalog_entry + key: srmag/m-sd1/c03-e/Strength_V + device: + type: tango.pyaml.attribute + attribute: srmag/m-sd1/c03-e/Strength_V + unit: rad +- type: tango.pyaml.static_catalog_entry + key: srmag/m-sd1/c03-e/Strength_SQ + device: + type: tango.pyaml.attribute + attribute: srmag/m-sd1/c03-e/Strength_SQ + unit: m-1 +- type: tango.pyaml.static_catalog_entry + key: srmag/m-sd1/c03-e/Strength + device: + type: tango.pyaml.attribute + attribute: srmag/m-sd1/c03-e/Strength + unit: m-2 diff --git a/examples/use_cases/config/esrf/catalogs/ebs_sh_catalogs.yaml b/examples/use_cases/config/esrf/catalogs/ebs_sh_catalogs.yaml new file mode 100644 index 000000000..72282b1d7 --- /dev/null +++ b/examples/use_cases/config/esrf/catalogs/ebs_sh_catalogs.yaml @@ -0,0 +1,1752 @@ +- type: tango.pyaml.static_catalog_entry + key: srmag/ps-corr-sh1/c04-a-ch1/current + device: + type: tango.pyaml.attribute + attribute: srmag/ps-corr-sh1/c04-a-ch1/current + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/ps-corr-sh1/c04-a-ch2/current + device: + type: tango.pyaml.attribute + attribute: srmag/ps-corr-sh1/c04-a-ch2/current + unit: A +- type: tango.pyaml.static_catalog_entry + key: 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srmag/ps-corr-sh3/c02-e-ch2/current + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/ps-corr-sh3/c02-e-ch3/current + device: + type: tango.pyaml.attribute + attribute: srmag/ps-corr-sh3/c02-e-ch3/current + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/ps-corr-sh1/c03-a-ch1/current + device: + type: tango.pyaml.attribute + attribute: srmag/ps-corr-sh1/c03-a-ch1/current + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/ps-corr-sh1/c03-a-ch2/current + device: + type: tango.pyaml.attribute + attribute: srmag/ps-corr-sh1/c03-a-ch2/current + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/ps-corr-sh1/c03-a-ch3/current + device: + type: tango.pyaml.attribute + attribute: srmag/ps-corr-sh1/c03-a-ch3/current + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/ps-corr-sh2/c03-b-ch1/current + device: + type: tango.pyaml.attribute + attribute: srmag/ps-corr-sh2/c03-b-ch1/current + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/ps-corr-sh2/c03-b-ch2/current + device: + type: tango.pyaml.attribute + attribute: srmag/ps-corr-sh2/c03-b-ch2/current + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/ps-corr-sh2/c03-b-ch3/current + device: + type: tango.pyaml.attribute + attribute: srmag/ps-corr-sh2/c03-b-ch3/current + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/ps-corr-sh3/c03-e-ch1/current + device: + type: tango.pyaml.attribute + attribute: srmag/ps-corr-sh3/c03-e-ch1/current + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/ps-corr-sh3/c03-e-ch2/current + device: + type: tango.pyaml.attribute + attribute: srmag/ps-corr-sh3/c03-e-ch2/current + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/ps-corr-sh3/c03-e-ch3/current + device: + type: tango.pyaml.attribute + attribute: srmag/ps-corr-sh3/c03-e-ch3/current + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/ps-corr-sh3/c03-e-ch5/current + device: + type: tango.pyaml.attribute + attribute: srmag/ps-corr-sh3/c03-e-ch5/current + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/ps-corr-sh3/c03-e-ch6/current + device: + type: tango.pyaml.attribute + attribute: srmag/ps-corr-sh3/c03-e-ch6/current + unit: A diff --git a/examples/use_cases/config/esrf/catalogs/sr_catalogs.yaml b/examples/use_cases/config/esrf/catalogs/sr_catalogs.yaml new file mode 100644 index 000000000..dc3bc686d --- /dev/null +++ b/examples/use_cases/config/esrf/catalogs/sr_catalogs.yaml @@ -0,0 +1,204 @@ +type: tango.pyaml.static_catalog +entries: + - type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c01-01/SA_HPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c01-01/SA_HPosition + unit: mm + - type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c01-01/SA_VPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c01-01/SA_VPosition + unit: mm + - type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c01-01/HOffset + device: + type: tango.pyaml.attribute + attribute: srdiag/bpm/c01-01/HOffset + unit: mm + - type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c01-01/VOffset + device: + type: tango.pyaml.attribute + attribute: srdiag/bpm/c01-01/VOffset + unit: mm + - type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c01-01/Tilt_Angle + device: + type: tango.pyaml.attribute + attribute: srdiag/bpm/c01-01/Tilt_Angle + unit: rad + - type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c01-02/SA_HPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c01-02/SA_HPosition + unit: mm + - type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c01-02/SA_VPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c01-02/SA_VPosition + unit: mm + - type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c01-03/SA_HPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c01-03/SA_HPosition + unit: mm + - type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c01-03/SA_VPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c01-03/SA_VPosition + unit: mm + - type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c01-04/SA_HPosition + device: + type: tango.pyaml.attribute + attribute: srdiag/bpm/c01-04/Position + index: 0 + unit: mm + - type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c01-04/SA_VPosition + device: + type: tango.pyaml.attribute + attribute: srdiag/bpm/c01-04/Position + index: 1 + unit: mm + - type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c04-01/SA_HPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c04-01/SA_HPosition + unit: m + - type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c04-01/SA_VPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c04-01/SA_VPosition + unit: m + - type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c04-02/SA_HPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c04-02/SA_HPosition + unit: m + - type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c04-02/SA_VPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c04-02/SA_VPosition + unit: m + - type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c04-04/SA_HPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c04-04/SA_HPosition + unit: m + - type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c04-04/SA_VPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c04-04/SA_VPosition + unit: m + - type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c04-05/SA_HPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c04-05/SA_HPosition + unit: m + - type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c04-05/SA_VPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c04-05/SA_VPosition + unit: m + - type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c04-06/SA_HPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c04-06/SA_HPosition + unit: m + - type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c04-06/SA_VPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c04-06/SA_VPosition + unit: m + + - type: tango.pyaml.static_catalog_entry + key: srmag/m-qf1/c01-a/strength + device: + type: tango.pyaml.attribute + attribute: srmag/m-qf1/c01-a/strength + unit: m-1 + + - type: tango.pyaml.static_catalog_entry + key: sr/ps-qf1/c01-a/current + device: + type: tango.pyaml.attribute + attribute: sr/ps-qf1/c01-a/current + unit: A + + - type: tango.pyaml.static_catalog_entry + key: srmag/hst-sh1/c01-a/strength + device: + type: tango.pyaml.attribute + attribute: srmag/hst-sh1/c01-a/strength + unit: rad + - type: tango.pyaml.static_catalog_entry + key: srmag/vst-sh1/c01-a/strength + device: + type: tango.pyaml.attribute + attribute: srmag/vst-sh1/c01-a/strength + unit: rad + - type: tango.pyaml.static_catalog_entry + key: srmag/sqp-sh1/c01-a/strength + device: + type: tango.pyaml.attribute + attribute: srmag/sqp-sh1/c01-a/strength + unit: m-1 + + - type: tango.pyaml.static_catalog_entry + key: srmag/ps-corr-sh1/c01-a-ch1/current + device: + type: tango.pyaml.attribute + attribute: srmag/ps-corr-sh1/c01-a-ch1/current + unit: A + range: [-1.5, 1.5] + - type: tango.pyaml.static_catalog_entry + key: srmag/ps-corr-sh1/c01-a-ch2/current + device: + type: tango.pyaml.attribute + attribute: srmag/ps-corr-sh1/c01-a-ch2/current + unit: A + range: [null, 1.5] + - type: tango.pyaml.static_catalog_entry + key: srmag/ps-corr-sh1/c01-a-ch3/current + device: + type: tango.pyaml.attribute + attribute: srmag/ps-corr-sh1/c01-a-ch3/current + unit: A + range: [-1.5, null] + + - type: tango.pyaml.static_catalog_entry + key: srmag/ps-corr-sh1/c02-a-ch1/current + device: + type: tango.pyaml.attribute + attribute: srmag/ps-corr-sh1/c02-a-ch1/current + unit: A + - type: tango.pyaml.static_catalog_entry + key: srmag/ps-corr-sh1/c02-a-ch2/current + device: + type: tango.pyaml.attribute + attribute: srmag/ps-corr-sh1/c02-a-ch2/current + unit: A + - type: tango.pyaml.static_catalog_entry + key: srmag/ps-corr-sh1/c02-a-ch3/current + device: + type: tango.pyaml.attribute + attribute: srmag/ps-corr-sh1/c02-a-ch3/current + unit: A diff --git a/examples/use_cases/config/esrf/esrf.yaml b/examples/use_cases/config/esrf/esrf.yaml new file mode 100644 index 000000000..a3bdba75a --- /dev/null +++ b/examples/use_cases/config/esrf/esrf.yaml @@ -0,0 +1,8609 @@ +type: pyaml.accelerator +machine: sr +facility: ESRF +energy: 6e9 +alphac: 8.623614679299252e-05 +simulators: + - type: pyaml.lattice.simulator + lattice: sr/lattices/ebs.mat + name: design +controls: + - type: tango.pyaml.controlsystem + tango_host: ebs-simu-3:10000 + name: live + catalog: catalogs/ebs_catalogs.yaml +data_folder: /data/store +arrays: + - type: pyaml.arrays.magnet + name: HCorr + elements: + - S*-H + - type: pyaml.arrays.magnet + name: VCorr + elements: + - S*-V + - type: pyaml.arrays.magnet + name: Skews + elements: + - S*-SQ + - type: pyaml.arrays.magnet + name: Sext + elements: + - SF*-S + - SD*-S + - type: pyaml.arrays.bpm + name: BPM + elements: + - BPM* + - type: pyaml.arrays.magnet + name: QForTune + elements: + - QD2* + - QF1* +devices: +- type: pyaml.tuning_tools.bba + name: BBA-BPM_C04-04 + bpm_array_name: BPM + bpm_name : BPM_C04-04 + hcorr_name : SF2E-C02-H + vcorr_name : SD1A-C26-V + quad_name : QF6B-C04 + n_step: 7 + hcorr_delta : 1e-05 + vcorr_delta : 1e-05 + hquad_delta : 0.005 + vquad_delta : 0.005 +- type: pyaml.tuning_tools.bba2 + name: BBA2-BPM_C04-04 + bpm_array_name: BPM + bpm_name : BPM_C04-04 + hcorr_name : SF2E-C02-H + vcorr_name : SD1A-C26-V + quad_name : QF6B-C04 + tune_correction_name: DEFAULT_TUNE_CORRECTION + hcorr_delta : 1e-05 + vcorr_delta : 1e-05 + quad_delta : 0.005 +- type: pyaml.diagnostics.tune_monitor + name: BETATRON_TUNE + tune_h: srdiag/beam-tune/main/Qh + tune_v: srdiag/beam-tune/main/Qv +- type: pyaml.tuning_tools.chromaticity_monitor + name: CHROMATICITY_MONITOR + betatron_tune_name: BETATRON_TUNE + rf_plant_name: RF + bpm_array_name: BPM + n_step: 5 +- type: pyaml.tuning_tools.tune + name: DEFAULT_TUNE_CORRECTION + quad_array_name: QForTune + betatron_tune_name: BETATRON_TUNE + response_matrix: ${path:trm.json} +- type: pyaml.tuning_tools.tune_response_matrix + name: DEFAULT_TUNE_RESPONSE_MATRIX + quad_array_name: QForTune + betatron_tune_name: BETATRON_TUNE + quad_delta: 1e-4 +- type: pyaml.tuning_tools.chromaticity_response_matrix + name: DEFAULT_CHROMATICITY_RESPONSE_MATRIX + sextu_array_name: Sext + chromaticity_name: CHROMATICITY_MONITOR + sextu_delta: 1e-6 +- type: pyaml.tuning_tools.chromaticity + name: DEFAULT_CHROMATICITY_CORRECTION + chromaticity_monitor_name: CHROMATICITY_MONITOR + sextu_array_name: Sext + response_matrix: ${path:chroma_resp.json} +- type: pyaml.tuning_tools.orbit + bpm_array_name: BPM + hcorr_array_name: HCorr + vcorr_array_name: VCorr + rf_plant_name: RF + name: DEFAULT_ORBIT_CORRECTION + singular_values: 162 + response_matrix: ${path:orm.json} +- type: pyaml.tuning_tools.orbit_response_matrix + bpm_array_name: BPM + hcorr_array_name: HCorr + vcorr_array_name: VCorr + corrector_delta: 1e-6 + name: DEFAULT_ORBIT_RESPONSE_MATRIX +- type: pyaml.tuning_tools.dispersion + bpm_array_name: BPM + rf_plant_name: RF + frequency_delta: 10 + name: DEFAULT_DISPERSION +- type: pyaml.rf.rf_plant + name: RF + masterclock: sy/ms/1/Frequency + transmitters: + - type: pyaml.rf.rf_transmitter + name: RFTRA + cavities: [CAV_C05_01,CAV_C05_02,CAV_C05_03,CAV_C05_04,CAV_C05_05,CAV_C07_01,CAV_C07_02,CAV_C07_03,CAV_C07_04,CAV_C07_05,CAV_C25_01,CAV_C25_02,CAV_C25_03] + harmonic: 1 + distribution: 1 + voltage: sys/ringsimulator/ebs/RfVoltage +- type: pyaml.magnet.quadrupole + name: QF6B-C04 + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.998960997 + crosstalk: 0.99918 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF6_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf6/c04-b/current +- type: pyaml.magnet.cfm_magnet + name: SH1A-C04 + mapping: + - [B0, SH1A-C04-H] + - [A0, SH1A-C04-V] + - [A1, SH1A-C04-SQ] + - [B2, SH1A-C04-S] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1,B2] + pseudo_factors: [1.0,-1.0,-1.0,-1.0] + units: [rad,rad,m-1,m-2] + hardware_units: ["A","A","A","A","A"] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SHI_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SHI_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SHI_sq_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SHI_sext_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SHI_matrix.csv + powerconverters: + - srmag/ps-corr-sh1/c04-a-ch1/current + - srmag/ps-corr-sh1/c04-a-ch2/current + - srmag/ps-corr-sh1/c04-a-ch3/current + - srmag/ps-corr-sh1/c04-a-ch5/current + - srmag/ps-corr-sh1/c04-a-ch6/current +- type: pyaml.magnet.cfm_magnet + name: SJ1A-C04 + mapping: + - [B0, SJ1A-C04-H] + - [A0, SJ1A-C04-V] + - [A1, SJ1A-C04-SQ] + - [B2, SJ1A-C04-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c04-a/Strength_H + - srmag/m-sd1/c04-a/Strength_V + - srmag/m-sd1/c04-a/Strength_SQ + - srmag/m-sd1/c04-a/Strength +- type: pyaml.magnet.cfm_magnet + name: SJ2A-C04 + mapping: + - [B0, SJ2A-C04-H] + - [A0, SJ2A-C04-V] + - [A1, SJ2A-C04-SQ] + - [B2, SJ2A-C04-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sf2/c04-a/Strength_H + - srmag/m-sf2/c04-a/Strength_V + - srmag/m-sf2/c04-a/Strength_SQ + - srmag/m-sf2/c04-a/Strength +- type: pyaml.magnet.cfm_magnet + name: SJ1B-C04 + mapping: + - [B0, SJ1B-C04-H] + - [A0, SJ1B-C04-V] + - [A1, SJ1B-C04-SQ] + - [B2, SJ1B-C04-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c04-b/Strength_H + - srmag/m-sd1/c04-b/Strength_V + - srmag/m-sd1/c04-b/Strength_SQ + - srmag/m-sd1/c04-b/Strength +- type: pyaml.magnet.cfm_magnet + name: SH2B-C04 + mapping: + - [B0, SH2B-C04-H] + - [A0, SH2B-C04-V] + - [A1, SH2B-C04-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh2/c04-b-ch1/current + - srmag/ps-corr-sh2/c04-b-ch2/current + - srmag/ps-corr-sh2/c04-b-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SJ1D-C04 + mapping: + - [B0, SJ1D-C04-H] + - [A0, SJ1D-C04-V] + - [A1, SJ1D-C04-SQ] + - [B2, SJ1D-C04-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c04-d/Strength_H + - srmag/m-sd1/c04-d/Strength_V + - srmag/m-sd1/c04-d/Strength_SQ + - srmag/m-sd1/c04-d/Strength +- type: pyaml.magnet.cfm_magnet + name: SJ2E-C04 + mapping: + - [B0, SJ2E-C04-H] + - [A0, SJ2E-C04-V] + - [A1, SJ2E-C04-SQ] + - [B2, SJ2E-C04-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sf2/c04-e/Strength_H + - srmag/m-sf2/c04-e/Strength_V + - srmag/m-sf2/c04-e/Strength_SQ + - srmag/m-sf2/c04-e/Strength +- type: pyaml.magnet.cfm_magnet + name: SJ1E-C04 + mapping: + - [B0, SJ1E-C04-H] + - [A0, SJ1E-C04-V] + - [A1, SJ1E-C04-SQ] + - [B2, SJ1E-C04-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c04-e/Strength_H + - srmag/m-sd1/c04-e/Strength_V + - srmag/m-sd1/c04-e/Strength_SQ + - srmag/m-sd1/c04-e/Strength +- type: pyaml.magnet.cfm_magnet + name: SH3E-C04 + mapping: + - [B0, SH3E-C04-H] + - [A0, SH3E-C04-V] + - [A1, SH3E-C04-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh3/c04-e-ch1/current + - srmag/ps-corr-sh3/c04-e-ch2/current + - srmag/ps-corr-sh3/c04-e-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SH1A-C05 + mapping: + - [B0, SH1A-C05-H] + - [A0, SH1A-C05-V] + - [A1, SH1A-C05-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh1/c05-a-ch1/current + - srmag/ps-corr-sh1/c05-a-ch2/current + - srmag/ps-corr-sh1/c05-a-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SD1A-C05 + mapping: + - [B0, SD1A-C05-H] + - [A0, SD1A-C05-V] + - [A1, SD1A-C05-SQ] + - [B2, SD1A-C05-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c05-a/Strength_H + - srmag/m-sd1/c05-a/Strength_V + - srmag/m-sd1/c05-a/Strength_SQ + - srmag/m-sd1/c05-a/Strength +- type: pyaml.magnet.cfm_magnet + name: SF2A-C05 + mapping: + - [B0, SF2A-C05-H] + - [A0, SF2A-C05-V] + - [A1, SF2A-C05-SQ] + - [B2, SF2A-C05-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sf2/c05-a/Strength_H + - srmag/m-sf2/c05-a/Strength_V + - srmag/m-sf2/c05-a/Strength_SQ + - srmag/m-sf2/c05-a/Strength +- type: pyaml.magnet.cfm_magnet + name: SD1B-C05 + mapping: + - [B0, SD1B-C05-H] + - [A0, SD1B-C05-V] + - [A1, SD1B-C05-SQ] + - [B2, SD1B-C05-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c05-b/Strength_H + - srmag/m-sd1/c05-b/Strength_V + - srmag/m-sd1/c05-b/Strength_SQ + - srmag/m-sd1/c05-b/Strength +- type: pyaml.magnet.cfm_magnet + name: SH2B-C05 + mapping: + - [B0, SH2B-C05-H] + - [A0, SH2B-C05-V] + - [A1, SH2B-C05-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh2/c05-b-ch1/current + - srmag/ps-corr-sh2/c05-b-ch2/current + - srmag/ps-corr-sh2/c05-b-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SD1D-C05 + mapping: + - [B0, SD1D-C05-H] + - [A0, SD1D-C05-V] + - [A1, SD1D-C05-SQ] + - [B2, SD1D-C05-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c05-d/Strength_H + - srmag/m-sd1/c05-d/Strength_V + - srmag/m-sd1/c05-d/Strength_SQ + - srmag/m-sd1/c05-d/Strength +- type: pyaml.magnet.cfm_magnet + name: SF2E-C05 + mapping: + - [B0, SF2E-C05-H] + - [A0, SF2E-C05-V] + - [A1, SF2E-C05-SQ] + - [B2, SF2E-C05-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sf2/c05-e/Strength_H + - srmag/m-sf2/c05-e/Strength_V + - srmag/m-sf2/c05-e/Strength_SQ + - srmag/m-sf2/c05-e/Strength +- type: pyaml.magnet.cfm_magnet + name: SD1E-C05 + mapping: + - [B0, SD1E-C05-H] + - [A0, SD1E-C05-V] + - [A1, SD1E-C05-SQ] + - [B2, SD1E-C05-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c05-e/Strength_H + - srmag/m-sd1/c05-e/Strength_V + - srmag/m-sd1/c05-e/Strength_SQ + - srmag/m-sd1/c05-e/Strength +- type: pyaml.magnet.cfm_magnet + name: SH3E-C05 + mapping: + - [B0, SH3E-C05-H] + - [A0, SH3E-C05-V] + - [A1, SH3E-C05-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh3/c05-e-ch1/current + - srmag/ps-corr-sh3/c05-e-ch2/current + - srmag/ps-corr-sh3/c05-e-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SH1A-C06 + mapping: + - [B0, SH1A-C06-H] + - [A0, SH1A-C06-V] + - [A1, SH1A-C06-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh1/c06-a-ch1/current + - srmag/ps-corr-sh1/c06-a-ch2/current + - srmag/ps-corr-sh1/c06-a-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SD1A-C06 + mapping: + - [B0, SD1A-C06-H] + - [A0, SD1A-C06-V] + - [A1, SD1A-C06-SQ] + - [B2, SD1A-C06-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c06-a/Strength_H + - srmag/m-sd1/c06-a/Strength_V + - srmag/m-sd1/c06-a/Strength_SQ + - srmag/m-sd1/c06-a/Strength +- type: pyaml.magnet.cfm_magnet + name: SF2A-C06 + mapping: + - [B0, SF2A-C06-H] + - [A0, SF2A-C06-V] + - [A1, SF2A-C06-SQ] + - [B2, SF2A-C06-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sf2/c06-a/Strength_H + - srmag/m-sf2/c06-a/Strength_V + - srmag/m-sf2/c06-a/Strength_SQ + - srmag/m-sf2/c06-a/Strength +- type: pyaml.magnet.cfm_magnet + name: SD1B-C06 + mapping: + - [B0, SD1B-C06-H] + - [A0, SD1B-C06-V] + - [A1, SD1B-C06-SQ] + - [B2, SD1B-C06-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c06-b/Strength_H + - srmag/m-sd1/c06-b/Strength_V + - srmag/m-sd1/c06-b/Strength_SQ + - srmag/m-sd1/c06-b/Strength +- type: pyaml.magnet.cfm_magnet + name: SH2B-C06 + mapping: + - [B0, SH2B-C06-H] + - [A0, SH2B-C06-V] + - [A1, SH2B-C06-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh2/c06-b-ch1/current + - srmag/ps-corr-sh2/c06-b-ch2/current + - srmag/ps-corr-sh2/c06-b-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SD1D-C06 + mapping: + - [B0, SD1D-C06-H] + - [A0, SD1D-C06-V] + - [A1, SD1D-C06-SQ] + - [B2, SD1D-C06-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c06-d/Strength_H + - srmag/m-sd1/c06-d/Strength_V + - srmag/m-sd1/c06-d/Strength_SQ + - srmag/m-sd1/c06-d/Strength +- type: pyaml.magnet.cfm_magnet + name: SF2E-C06 + mapping: + - [B0, SF2E-C06-H] + - [A0, SF2E-C06-V] + - [A1, SF2E-C06-SQ] + - [B2, SF2E-C06-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sf2/c06-e/Strength_H + - srmag/m-sf2/c06-e/Strength_V + - srmag/m-sf2/c06-e/Strength_SQ + - srmag/m-sf2/c06-e/Strength +- type: pyaml.magnet.cfm_magnet + name: SD1E-C06 + mapping: + - [B0, SD1E-C06-H] + - [A0, SD1E-C06-V] + - [A1, SD1E-C06-SQ] + - [B2, SD1E-C06-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c06-e/Strength_H + - srmag/m-sd1/c06-e/Strength_V + - srmag/m-sd1/c06-e/Strength_SQ + - srmag/m-sd1/c06-e/Strength +- type: pyaml.magnet.cfm_magnet + name: SH3E-C06 + mapping: + - [B0, SH3E-C06-H] + - [A0, SH3E-C06-V] + - [A1, SH3E-C06-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh3/c06-e-ch1/current + - srmag/ps-corr-sh3/c06-e-ch2/current + - srmag/ps-corr-sh3/c06-e-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SH1A-C07 + mapping: + - [B0, SH1A-C07-H] + - [A0, SH1A-C07-V] + - [A1, SH1A-C07-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh1/c07-a-ch1/current + - srmag/ps-corr-sh1/c07-a-ch2/current + - srmag/ps-corr-sh1/c07-a-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SD1A-C07 + mapping: + - [B0, SD1A-C07-H] + - [A0, SD1A-C07-V] + - [A1, SD1A-C07-SQ] + - [B2, SD1A-C07-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c07-a/Strength_H + - srmag/m-sd1/c07-a/Strength_V + - srmag/m-sd1/c07-a/Strength_SQ + - srmag/m-sd1/c07-a/Strength +- type: pyaml.magnet.cfm_magnet + name: SF2A-C07 + mapping: + - [B0, SF2A-C07-H] + - [A0, SF2A-C07-V] + - [A1, SF2A-C07-SQ] + - [B2, SF2A-C07-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sf2/c07-a/Strength_H + - srmag/m-sf2/c07-a/Strength_V + - srmag/m-sf2/c07-a/Strength_SQ + - srmag/m-sf2/c07-a/Strength +- type: pyaml.magnet.cfm_magnet + name: SD1B-C07 + mapping: + - [B0, SD1B-C07-H] + - [A0, SD1B-C07-V] + - [A1, SD1B-C07-SQ] + - [B2, SD1B-C07-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c07-b/Strength_H + - srmag/m-sd1/c07-b/Strength_V + - srmag/m-sd1/c07-b/Strength_SQ + - srmag/m-sd1/c07-b/Strength +- type: pyaml.magnet.cfm_magnet + name: SH2B-C07 + mapping: + - [B0, SH2B-C07-H] + - [A0, SH2B-C07-V] + - [A1, SH2B-C07-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh2/c07-b-ch1/current + - srmag/ps-corr-sh2/c07-b-ch2/current + - srmag/ps-corr-sh2/c07-b-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SD1D-C07 + mapping: + - [B0, SD1D-C07-H] + - [A0, SD1D-C07-V] + - [A1, SD1D-C07-SQ] + - [B2, SD1D-C07-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c07-d/Strength_H + - srmag/m-sd1/c07-d/Strength_V + - srmag/m-sd1/c07-d/Strength_SQ + - srmag/m-sd1/c07-d/Strength +- type: pyaml.magnet.cfm_magnet + name: SF2E-C07 + mapping: + - [B0, SF2E-C07-H] + - [A0, SF2E-C07-V] + - [A1, SF2E-C07-SQ] + - [B2, SF2E-C07-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sf2/c07-e/Strength_H + - srmag/m-sf2/c07-e/Strength_V + - srmag/m-sf2/c07-e/Strength_SQ + - srmag/m-sf2/c07-e/Strength +- type: pyaml.magnet.cfm_magnet + name: SD1E-C07 + mapping: + - [B0, SD1E-C07-H] + - [A0, SD1E-C07-V] + - [A1, SD1E-C07-SQ] + - [B2, SD1E-C07-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c07-e/Strength_H + - srmag/m-sd1/c07-e/Strength_V + - srmag/m-sd1/c07-e/Strength_SQ + - srmag/m-sd1/c07-e/Strength +- type: pyaml.magnet.cfm_magnet + name: SH3E-C07 + mapping: + - [B0, SH3E-C07-H] + - [A0, SH3E-C07-V] + - [A1, SH3E-C07-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh3/c07-e-ch1/current + - srmag/ps-corr-sh3/c07-e-ch2/current + - srmag/ps-corr-sh3/c07-e-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SH1A-C08 + mapping: + - [B0, SH1A-C08-H] + - [A0, SH1A-C08-V] + - [A1, SH1A-C08-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh1/c08-a-ch1/current + - srmag/ps-corr-sh1/c08-a-ch2/current + - srmag/ps-corr-sh1/c08-a-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SD1A-C08 + mapping: + - [B0, SD1A-C08-H] + - [A0, SD1A-C08-V] + - [A1, SD1A-C08-SQ] + - [B2, SD1A-C08-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c08-a/Strength_H + - srmag/m-sd1/c08-a/Strength_V + - srmag/m-sd1/c08-a/Strength_SQ + - srmag/m-sd1/c08-a/Strength +- type: pyaml.magnet.cfm_magnet + name: SF2A-C08 + mapping: + - [B0, SF2A-C08-H] + - [A0, SF2A-C08-V] + - [A1, SF2A-C08-SQ] + - [B2, SF2A-C08-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sf2/c08-a/Strength_H + - srmag/m-sf2/c08-a/Strength_V + - srmag/m-sf2/c08-a/Strength_SQ + - srmag/m-sf2/c08-a/Strength +- type: pyaml.magnet.cfm_magnet + name: SD1B-C08 + mapping: + - [B0, SD1B-C08-H] + - [A0, SD1B-C08-V] + - [A1, SD1B-C08-SQ] + - [B2, SD1B-C08-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c08-b/Strength_H + - srmag/m-sd1/c08-b/Strength_V + - srmag/m-sd1/c08-b/Strength_SQ + - srmag/m-sd1/c08-b/Strength +- type: pyaml.magnet.cfm_magnet + name: SH2B-C08 + mapping: + - [B0, SH2B-C08-H] + - [A0, SH2B-C08-V] + - [A1, SH2B-C08-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh2/c08-b-ch1/current + - srmag/ps-corr-sh2/c08-b-ch2/current + - srmag/ps-corr-sh2/c08-b-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SD1D-C08 + mapping: + - [B0, SD1D-C08-H] + - [A0, SD1D-C08-V] + - [A1, SD1D-C08-SQ] + - [B2, SD1D-C08-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c08-d/Strength_H + - srmag/m-sd1/c08-d/Strength_V + - srmag/m-sd1/c08-d/Strength_SQ + - srmag/m-sd1/c08-d/Strength +- type: pyaml.magnet.cfm_magnet + name: SF2E-C08 + mapping: + - [B0, SF2E-C08-H] + - [A0, SF2E-C08-V] + - [A1, SF2E-C08-SQ] + - [B2, SF2E-C08-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sf2/c08-e/Strength_H + - srmag/m-sf2/c08-e/Strength_V + - srmag/m-sf2/c08-e/Strength_SQ + - srmag/m-sf2/c08-e/Strength +- type: pyaml.magnet.cfm_magnet + name: SD1E-C08 + mapping: + - [B0, SD1E-C08-H] + - [A0, SD1E-C08-V] + - [A1, SD1E-C08-SQ] + - [B2, SD1E-C08-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c08-e/Strength_H + - srmag/m-sd1/c08-e/Strength_V + - srmag/m-sd1/c08-e/Strength_SQ + - srmag/m-sd1/c08-e/Strength +- type: pyaml.magnet.cfm_magnet + name: SH3E-C08 + mapping: + - [B0, SH3E-C08-H] + - [A0, SH3E-C08-V] + - [A1, SH3E-C08-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh3/c08-e-ch1/current + - srmag/ps-corr-sh3/c08-e-ch2/current + - srmag/ps-corr-sh3/c08-e-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SH1A-C09 + mapping: + - [B0, SH1A-C09-H] + - [A0, SH1A-C09-V] + - [A1, SH1A-C09-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh1/c09-a-ch1/current + - srmag/ps-corr-sh1/c09-a-ch2/current + - srmag/ps-corr-sh1/c09-a-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SD1A-C09 + mapping: + - [B0, SD1A-C09-H] + - [A0, SD1A-C09-V] + - [A1, SD1A-C09-SQ] + - [B2, SD1A-C09-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c09-a/Strength_H + - srmag/m-sd1/c09-a/Strength_V + - srmag/m-sd1/c09-a/Strength_SQ + - srmag/m-sd1/c09-a/Strength +- type: pyaml.magnet.cfm_magnet + name: SF2A-C09 + mapping: + - [B0, SF2A-C09-H] + - [A0, SF2A-C09-V] + - [A1, SF2A-C09-SQ] + - [B2, SF2A-C09-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sf2/c09-a/Strength_H + - srmag/m-sf2/c09-a/Strength_V + - srmag/m-sf2/c09-a/Strength_SQ + - srmag/m-sf2/c09-a/Strength +- type: pyaml.magnet.cfm_magnet + name: SD1B-C09 + mapping: + - [B0, SD1B-C09-H] + - [A0, SD1B-C09-V] + - [A1, SD1B-C09-SQ] + - [B2, SD1B-C09-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c09-b/Strength_H + - srmag/m-sd1/c09-b/Strength_V + - srmag/m-sd1/c09-b/Strength_SQ + - srmag/m-sd1/c09-b/Strength +- type: pyaml.magnet.cfm_magnet + name: SH2B-C09 + mapping: + - [B0, SH2B-C09-H] + - [A0, SH2B-C09-V] + - [A1, SH2B-C09-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh2/c09-b-ch1/current + - srmag/ps-corr-sh2/c09-b-ch2/current + - srmag/ps-corr-sh2/c09-b-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SD1D-C09 + mapping: + - [B0, SD1D-C09-H] + - [A0, SD1D-C09-V] + - [A1, SD1D-C09-SQ] + - [B2, SD1D-C09-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c09-d/Strength_H + - srmag/m-sd1/c09-d/Strength_V + - srmag/m-sd1/c09-d/Strength_SQ + - srmag/m-sd1/c09-d/Strength +- type: pyaml.magnet.cfm_magnet + name: SF2E-C09 + mapping: + - [B0, SF2E-C09-H] + - [A0, SF2E-C09-V] + - [A1, SF2E-C09-SQ] + - [B2, SF2E-C09-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sf2/c09-e/Strength_H + - srmag/m-sf2/c09-e/Strength_V + - srmag/m-sf2/c09-e/Strength_SQ + - srmag/m-sf2/c09-e/Strength +- type: pyaml.magnet.cfm_magnet + name: SD1E-C09 + mapping: + - [B0, SD1E-C09-H] + - [A0, SD1E-C09-V] + - [A1, SD1E-C09-SQ] + - [B2, SD1E-C09-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c09-e/Strength_H + - srmag/m-sd1/c09-e/Strength_V + - srmag/m-sd1/c09-e/Strength_SQ + - srmag/m-sd1/c09-e/Strength +- type: pyaml.magnet.cfm_magnet + name: SH3E-C09 + mapping: + - [B0, SH3E-C09-H] + - [A0, SH3E-C09-V] + - [A1, SH3E-C09-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh3/c09-e-ch1/current + - srmag/ps-corr-sh3/c09-e-ch2/current + - srmag/ps-corr-sh3/c09-e-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SH1A-C10 + mapping: + - [B0, SH1A-C10-H] + - [A0, SH1A-C10-V] + - [A1, SH1A-C10-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh1/c10-a-ch1/current + - srmag/ps-corr-sh1/c10-a-ch2/current + - srmag/ps-corr-sh1/c10-a-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SD1A-C10 + mapping: + - [B0, SD1A-C10-H] + - [A0, SD1A-C10-V] + - [A1, SD1A-C10-SQ] + - [B2, SD1A-C10-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c10-a/Strength_H + - srmag/m-sd1/c10-a/Strength_V + - srmag/m-sd1/c10-a/Strength_SQ + - srmag/m-sd1/c10-a/Strength +- type: pyaml.magnet.cfm_magnet + name: SF2A-C10 + mapping: + - [B0, SF2A-C10-H] + - [A0, SF2A-C10-V] + - [A1, SF2A-C10-SQ] + - [B2, SF2A-C10-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sf2/c10-a/Strength_H + - srmag/m-sf2/c10-a/Strength_V + - srmag/m-sf2/c10-a/Strength_SQ + - srmag/m-sf2/c10-a/Strength +- type: pyaml.magnet.cfm_magnet + name: SD1B-C10 + mapping: + - [B0, SD1B-C10-H] + - [A0, SD1B-C10-V] + - [A1, SD1B-C10-SQ] + - [B2, SD1B-C10-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c10-b/Strength_H + - srmag/m-sd1/c10-b/Strength_V + - srmag/m-sd1/c10-b/Strength_SQ + - srmag/m-sd1/c10-b/Strength +- type: pyaml.magnet.cfm_magnet + name: SH2B-C10 + mapping: + - [B0, SH2B-C10-H] + - [A0, SH2B-C10-V] + - [A1, SH2B-C10-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh2/c10-b-ch1/current + - srmag/ps-corr-sh2/c10-b-ch2/current + - srmag/ps-corr-sh2/c10-b-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SD1D-C10 + mapping: + - [B0, SD1D-C10-H] + - [A0, SD1D-C10-V] + - [A1, SD1D-C10-SQ] + - [B2, SD1D-C10-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c10-d/Strength_H + - srmag/m-sd1/c10-d/Strength_V + - srmag/m-sd1/c10-d/Strength_SQ + - srmag/m-sd1/c10-d/Strength +- type: pyaml.magnet.cfm_magnet + name: SF2E-C10 + mapping: + - [B0, SF2E-C10-H] + - [A0, SF2E-C10-V] + - [A1, SF2E-C10-SQ] + - [B2, SF2E-C10-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sf2/c10-e/Strength_H + - srmag/m-sf2/c10-e/Strength_V + - srmag/m-sf2/c10-e/Strength_SQ + - srmag/m-sf2/c10-e/Strength +- type: pyaml.magnet.cfm_magnet + name: SD1E-C10 + mapping: + - [B0, SD1E-C10-H] + - [A0, SD1E-C10-V] + - [A1, SD1E-C10-SQ] + - [B2, SD1E-C10-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c10-e/Strength_H + - srmag/m-sd1/c10-e/Strength_V + - srmag/m-sd1/c10-e/Strength_SQ + - srmag/m-sd1/c10-e/Strength +- type: pyaml.magnet.cfm_magnet + name: SH3E-C10 + mapping: + - [B0, SH3E-C10-H] + - [A0, SH3E-C10-V] + - [A1, SH3E-C10-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh3/c10-e-ch1/current + - srmag/ps-corr-sh3/c10-e-ch2/current + - srmag/ps-corr-sh3/c10-e-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SH1A-C11 + mapping: + - [B0, SH1A-C11-H] + - [A0, SH1A-C11-V] + - [A1, SH1A-C11-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh1/c11-a-ch1/current + - srmag/ps-corr-sh1/c11-a-ch2/current + - srmag/ps-corr-sh1/c11-a-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SD1A-C11 + mapping: + - [B0, SD1A-C11-H] + - [A0, SD1A-C11-V] + - [A1, SD1A-C11-SQ] + - [B2, SD1A-C11-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c11-a/Strength_H + - srmag/m-sd1/c11-a/Strength_V + - srmag/m-sd1/c11-a/Strength_SQ + - srmag/m-sd1/c11-a/Strength +- type: pyaml.magnet.cfm_magnet + name: SF2A-C11 + mapping: + - [B0, SF2A-C11-H] + - [A0, SF2A-C11-V] + - [A1, SF2A-C11-SQ] + - [B2, SF2A-C11-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sf2/c11-a/Strength_H + - srmag/m-sf2/c11-a/Strength_V + - srmag/m-sf2/c11-a/Strength_SQ + - srmag/m-sf2/c11-a/Strength +- type: pyaml.magnet.cfm_magnet + name: SD1B-C11 + mapping: + - [B0, SD1B-C11-H] + - [A0, SD1B-C11-V] + - [A1, SD1B-C11-SQ] + - [B2, SD1B-C11-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c11-b/Strength_H + - srmag/m-sd1/c11-b/Strength_V + - srmag/m-sd1/c11-b/Strength_SQ + - srmag/m-sd1/c11-b/Strength +- type: pyaml.magnet.cfm_magnet + name: SH2B-C11 + mapping: + - [B0, SH2B-C11-H] + - [A0, SH2B-C11-V] + - [A1, SH2B-C11-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh2/c11-b-ch1/current + - srmag/ps-corr-sh2/c11-b-ch2/current + - srmag/ps-corr-sh2/c11-b-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SD1D-C11 + mapping: + - [B0, SD1D-C11-H] + - [A0, SD1D-C11-V] + - [A1, SD1D-C11-SQ] + - [B2, SD1D-C11-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c11-d/Strength_H + - srmag/m-sd1/c11-d/Strength_V + - srmag/m-sd1/c11-d/Strength_SQ + - srmag/m-sd1/c11-d/Strength +- type: pyaml.magnet.cfm_magnet + name: SF2E-C11 + mapping: + - [B0, SF2E-C11-H] + - [A0, SF2E-C11-V] + - [A1, SF2E-C11-SQ] + - [B2, SF2E-C11-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sf2/c11-e/Strength_H + - srmag/m-sf2/c11-e/Strength_V + - srmag/m-sf2/c11-e/Strength_SQ + - srmag/m-sf2/c11-e/Strength +- type: pyaml.magnet.cfm_magnet + name: SD1E-C11 + mapping: + - [B0, SD1E-C11-H] + - [A0, SD1E-C11-V] + - [A1, SD1E-C11-SQ] + - [B2, SD1E-C11-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c11-e/Strength_H + - srmag/m-sd1/c11-e/Strength_V + - srmag/m-sd1/c11-e/Strength_SQ + - srmag/m-sd1/c11-e/Strength +- type: pyaml.magnet.cfm_magnet + name: SH3E-C11 + mapping: + - [B0, SH3E-C11-H] + - [A0, SH3E-C11-V] + - [A1, SH3E-C11-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh3/c11-e-ch1/current + - srmag/ps-corr-sh3/c11-e-ch2/current + - srmag/ps-corr-sh3/c11-e-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SH1A-C12 + mapping: + - [B0, SH1A-C12-H] + - [A0, SH1A-C12-V] + - [A1, SH1A-C12-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh1/c12-a-ch1/current + - srmag/ps-corr-sh1/c12-a-ch2/current + - srmag/ps-corr-sh1/c12-a-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SD1A-C12 + mapping: + - [B0, SD1A-C12-H] + - [A0, SD1A-C12-V] + - [A1, SD1A-C12-SQ] + - [B2, SD1A-C12-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c12-a/Strength_H + - srmag/m-sd1/c12-a/Strength_V + - srmag/m-sd1/c12-a/Strength_SQ + - srmag/m-sd1/c12-a/Strength +- type: pyaml.magnet.cfm_magnet + name: SF2A-C12 + mapping: + - [B0, SF2A-C12-H] + - [A0, SF2A-C12-V] + - [A1, SF2A-C12-SQ] + - [B2, SF2A-C12-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sf2/c12-a/Strength_H + - srmag/m-sf2/c12-a/Strength_V + - srmag/m-sf2/c12-a/Strength_SQ + - srmag/m-sf2/c12-a/Strength +- type: pyaml.magnet.cfm_magnet + name: SD1B-C12 + mapping: + - [B0, SD1B-C12-H] + - [A0, SD1B-C12-V] + - [A1, SD1B-C12-SQ] + - [B2, SD1B-C12-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c12-b/Strength_H + - srmag/m-sd1/c12-b/Strength_V + - srmag/m-sd1/c12-b/Strength_SQ + - srmag/m-sd1/c12-b/Strength +- type: pyaml.magnet.cfm_magnet + name: SH2B-C12 + mapping: + - [B0, SH2B-C12-H] + - [A0, SH2B-C12-V] + - [A1, SH2B-C12-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh2/c12-b-ch1/current + - srmag/ps-corr-sh2/c12-b-ch2/current + - srmag/ps-corr-sh2/c12-b-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SD1D-C12 + mapping: + - [B0, SD1D-C12-H] + - [A0, SD1D-C12-V] + - [A1, SD1D-C12-SQ] + - [B2, SD1D-C12-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c12-d/Strength_H + - srmag/m-sd1/c12-d/Strength_V + - srmag/m-sd1/c12-d/Strength_SQ + - srmag/m-sd1/c12-d/Strength +- type: pyaml.magnet.cfm_magnet + name: SF2E-C12 + mapping: + - [B0, SF2E-C12-H] + - [A0, SF2E-C12-V] + - [A1, SF2E-C12-SQ] + - [B2, SF2E-C12-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sf2/c12-e/Strength_H + - srmag/m-sf2/c12-e/Strength_V + - srmag/m-sf2/c12-e/Strength_SQ + - srmag/m-sf2/c12-e/Strength +- type: pyaml.magnet.cfm_magnet + name: SD1E-C12 + mapping: + - [B0, SD1E-C12-H] + - [A0, SD1E-C12-V] + - [A1, SD1E-C12-SQ] + - [B2, SD1E-C12-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c12-e/Strength_H + - srmag/m-sd1/c12-e/Strength_V + - srmag/m-sd1/c12-e/Strength_SQ + - srmag/m-sd1/c12-e/Strength +- type: pyaml.magnet.cfm_magnet + name: SH3E-C12 + mapping: + - [B0, SH3E-C12-H] + - [A0, SH3E-C12-V] + - [A1, SH3E-C12-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh3/c12-e-ch1/current + - srmag/ps-corr-sh3/c12-e-ch2/current + - srmag/ps-corr-sh3/c12-e-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SH1A-C13 + mapping: + - [B0, SH1A-C13-H] + - [A0, SH1A-C13-V] + - [A1, SH1A-C13-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh1/c13-a-ch1/current + - srmag/ps-corr-sh1/c13-a-ch2/current + - srmag/ps-corr-sh1/c13-a-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SD1A-C13 + mapping: + - [B0, SD1A-C13-H] + - [A0, SD1A-C13-V] + - [A1, SD1A-C13-SQ] + - [B2, SD1A-C13-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c13-a/Strength_H + - srmag/m-sd1/c13-a/Strength_V + - srmag/m-sd1/c13-a/Strength_SQ + - srmag/m-sd1/c13-a/Strength +- type: pyaml.magnet.cfm_magnet + name: SF2A-C13 + mapping: + - [B0, SF2A-C13-H] + - [A0, SF2A-C13-V] + - [A1, SF2A-C13-SQ] + - [B2, SF2A-C13-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sf2/c13-a/Strength_H + - srmag/m-sf2/c13-a/Strength_V + - srmag/m-sf2/c13-a/Strength_SQ + - srmag/m-sf2/c13-a/Strength +- type: pyaml.magnet.cfm_magnet + name: SD1B-C13 + mapping: + - [B0, SD1B-C13-H] + - [A0, SD1B-C13-V] + - [A1, SD1B-C13-SQ] + - [B2, SD1B-C13-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c13-b/Strength_H + - srmag/m-sd1/c13-b/Strength_V + - srmag/m-sd1/c13-b/Strength_SQ + - srmag/m-sd1/c13-b/Strength +- type: pyaml.magnet.cfm_magnet + name: SH2B-C13 + mapping: + - [B0, SH2B-C13-H] + - [A0, SH2B-C13-V] + - [A1, SH2B-C13-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh2/c13-b-ch1/current + - srmag/ps-corr-sh2/c13-b-ch2/current + - srmag/ps-corr-sh2/c13-b-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SD1D-C13 + mapping: + - [B0, SD1D-C13-H] + - [A0, SD1D-C13-V] + - [A1, SD1D-C13-SQ] + - [B2, SD1D-C13-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c13-d/Strength_H + - srmag/m-sd1/c13-d/Strength_V + - srmag/m-sd1/c13-d/Strength_SQ + - srmag/m-sd1/c13-d/Strength +- type: pyaml.magnet.cfm_magnet + name: SF2E-C13 + mapping: + - [B0, SF2E-C13-H] + - [A0, SF2E-C13-V] + - [A1, SF2E-C13-SQ] + - [B2, SF2E-C13-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sf2/c13-e/Strength_H + - srmag/m-sf2/c13-e/Strength_V + - srmag/m-sf2/c13-e/Strength_SQ + - srmag/m-sf2/c13-e/Strength +- type: pyaml.magnet.cfm_magnet + name: SD1E-C13 + mapping: + - [B0, SD1E-C13-H] + - [A0, SD1E-C13-V] + - [A1, SD1E-C13-SQ] + - [B2, SD1E-C13-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c13-e/Strength_H + - srmag/m-sd1/c13-e/Strength_V + - srmag/m-sd1/c13-e/Strength_SQ + - srmag/m-sd1/c13-e/Strength +- type: pyaml.magnet.cfm_magnet + name: SH3E-C13 + mapping: + - [B0, SH3E-C13-H] + - [A0, SH3E-C13-V] + - [A1, SH3E-C13-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh3/c13-e-ch1/current + - srmag/ps-corr-sh3/c13-e-ch2/current + - srmag/ps-corr-sh3/c13-e-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SH1A-C14 + mapping: + - [B0, SH1A-C14-H] + - [A0, SH1A-C14-V] + - [A1, SH1A-C14-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh1/c14-a-ch1/current + - srmag/ps-corr-sh1/c14-a-ch2/current + - srmag/ps-corr-sh1/c14-a-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SD1A-C14 + mapping: + - [B0, SD1A-C14-H] + - [A0, SD1A-C14-V] + - [A1, SD1A-C14-SQ] + - [B2, SD1A-C14-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c14-a/Strength_H + - srmag/m-sd1/c14-a/Strength_V + - srmag/m-sd1/c14-a/Strength_SQ + - srmag/m-sd1/c14-a/Strength +- type: pyaml.magnet.cfm_magnet + name: SF2A-C14 + mapping: + - [B0, SF2A-C14-H] + - [A0, SF2A-C14-V] + - [A1, SF2A-C14-SQ] + - [B2, SF2A-C14-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sf2/c14-a/Strength_H + - srmag/m-sf2/c14-a/Strength_V + - srmag/m-sf2/c14-a/Strength_SQ + - srmag/m-sf2/c14-a/Strength +- type: pyaml.magnet.cfm_magnet + name: SD1B-C14 + mapping: + - [B0, SD1B-C14-H] + - [A0, SD1B-C14-V] + - [A1, SD1B-C14-SQ] + - [B2, SD1B-C14-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c14-b/Strength_H + - srmag/m-sd1/c14-b/Strength_V + - srmag/m-sd1/c14-b/Strength_SQ + - srmag/m-sd1/c14-b/Strength +- type: pyaml.magnet.cfm_magnet + name: SH2B-C14 + mapping: + - [B0, SH2B-C14-H] + - [A0, SH2B-C14-V] + - [A1, SH2B-C14-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh2/c14-b-ch1/current + - srmag/ps-corr-sh2/c14-b-ch2/current + - srmag/ps-corr-sh2/c14-b-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SD1D-C14 + mapping: + - [B0, SD1D-C14-H] + - [A0, SD1D-C14-V] + - [A1, SD1D-C14-SQ] + - [B2, SD1D-C14-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c14-d/Strength_H + - srmag/m-sd1/c14-d/Strength_V + - srmag/m-sd1/c14-d/Strength_SQ + - srmag/m-sd1/c14-d/Strength +- type: pyaml.magnet.cfm_magnet + name: SF2E-C14 + mapping: + - [B0, SF2E-C14-H] + - [A0, SF2E-C14-V] + - [A1, SF2E-C14-SQ] + - [B2, SF2E-C14-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sf2/c14-e/Strength_H + - srmag/m-sf2/c14-e/Strength_V + - srmag/m-sf2/c14-e/Strength_SQ + - srmag/m-sf2/c14-e/Strength +- type: pyaml.magnet.cfm_magnet + name: SD1E-C14 + mapping: + - [B0, SD1E-C14-H] + - [A0, SD1E-C14-V] + - [A1, SD1E-C14-SQ] + - [B2, SD1E-C14-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c14-e/Strength_H + - srmag/m-sd1/c14-e/Strength_V + - srmag/m-sd1/c14-e/Strength_SQ + - srmag/m-sd1/c14-e/Strength +- type: pyaml.magnet.cfm_magnet + name: SH3E-C14 + mapping: + - [B0, SH3E-C14-H] + - [A0, SH3E-C14-V] + - [A1, SH3E-C14-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh3/c14-e-ch1/current + - srmag/ps-corr-sh3/c14-e-ch2/current + - srmag/ps-corr-sh3/c14-e-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SH1A-C15 + mapping: + - [B0, SH1A-C15-H] + - [A0, SH1A-C15-V] + - [A1, SH1A-C15-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh1/c15-a-ch1/current + - srmag/ps-corr-sh1/c15-a-ch2/current + - srmag/ps-corr-sh1/c15-a-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SD1A-C15 + mapping: + - [B0, SD1A-C15-H] + - [A0, SD1A-C15-V] + - [A1, SD1A-C15-SQ] + - [B2, SD1A-C15-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c15-a/Strength_H + - srmag/m-sd1/c15-a/Strength_V + - srmag/m-sd1/c15-a/Strength_SQ + - srmag/m-sd1/c15-a/Strength +- type: pyaml.magnet.cfm_magnet + name: SF2A-C15 + mapping: + - [B0, SF2A-C15-H] + - [A0, SF2A-C15-V] + - [A1, SF2A-C15-SQ] + - [B2, SF2A-C15-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sf2/c15-a/Strength_H + - srmag/m-sf2/c15-a/Strength_V + - srmag/m-sf2/c15-a/Strength_SQ + - srmag/m-sf2/c15-a/Strength +- type: pyaml.magnet.cfm_magnet + name: SD1B-C15 + mapping: + - [B0, SD1B-C15-H] + - [A0, SD1B-C15-V] + - [A1, SD1B-C15-SQ] + - [B2, SD1B-C15-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c15-b/Strength_H + - srmag/m-sd1/c15-b/Strength_V + - srmag/m-sd1/c15-b/Strength_SQ + - srmag/m-sd1/c15-b/Strength +- type: pyaml.magnet.cfm_magnet + name: SH2B-C15 + mapping: + - [B0, SH2B-C15-H] + - [A0, SH2B-C15-V] + - [A1, SH2B-C15-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh2/c15-b-ch1/current + - srmag/ps-corr-sh2/c15-b-ch2/current + - srmag/ps-corr-sh2/c15-b-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SD1D-C15 + mapping: + - [B0, SD1D-C15-H] + - [A0, SD1D-C15-V] + - [A1, SD1D-C15-SQ] + - [B2, SD1D-C15-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c15-d/Strength_H + - srmag/m-sd1/c15-d/Strength_V + - srmag/m-sd1/c15-d/Strength_SQ + - srmag/m-sd1/c15-d/Strength +- type: pyaml.magnet.cfm_magnet + name: SF2E-C15 + mapping: + - [B0, SF2E-C15-H] + - [A0, SF2E-C15-V] + - [A1, SF2E-C15-SQ] + - [B2, SF2E-C15-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sf2/c15-e/Strength_H + - srmag/m-sf2/c15-e/Strength_V + - srmag/m-sf2/c15-e/Strength_SQ + - srmag/m-sf2/c15-e/Strength +- type: pyaml.magnet.cfm_magnet + name: SD1E-C15 + mapping: + - [B0, SD1E-C15-H] + - [A0, SD1E-C15-V] + - [A1, SD1E-C15-SQ] + - [B2, SD1E-C15-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c15-e/Strength_H + - srmag/m-sd1/c15-e/Strength_V + - srmag/m-sd1/c15-e/Strength_SQ + - srmag/m-sd1/c15-e/Strength +- type: pyaml.magnet.cfm_magnet + name: SH3E-C15 + mapping: + - [B0, SH3E-C15-H] + - [A0, SH3E-C15-V] + - [A1, SH3E-C15-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh3/c15-e-ch1/current + - srmag/ps-corr-sh3/c15-e-ch2/current + - srmag/ps-corr-sh3/c15-e-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SH1A-C16 + mapping: + - [B0, SH1A-C16-H] + - [A0, SH1A-C16-V] + - [A1, SH1A-C16-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh1/c16-a-ch1/current + - srmag/ps-corr-sh1/c16-a-ch2/current + - srmag/ps-corr-sh1/c16-a-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SD1A-C16 + mapping: + - [B0, SD1A-C16-H] + - [A0, SD1A-C16-V] + - [A1, SD1A-C16-SQ] + - [B2, SD1A-C16-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c16-a/Strength_H + - srmag/m-sd1/c16-a/Strength_V + - srmag/m-sd1/c16-a/Strength_SQ + - srmag/m-sd1/c16-a/Strength +- type: pyaml.magnet.cfm_magnet + name: SF2A-C16 + mapping: + - [B0, SF2A-C16-H] + - [A0, SF2A-C16-V] + - [A1, SF2A-C16-SQ] + - [B2, SF2A-C16-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sf2/c16-a/Strength_H + - srmag/m-sf2/c16-a/Strength_V + - srmag/m-sf2/c16-a/Strength_SQ + - srmag/m-sf2/c16-a/Strength +- type: pyaml.magnet.cfm_magnet + name: SD1B-C16 + mapping: + - [B0, SD1B-C16-H] + - [A0, SD1B-C16-V] + - [A1, SD1B-C16-SQ] + - [B2, SD1B-C16-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c16-b/Strength_H + - srmag/m-sd1/c16-b/Strength_V + - srmag/m-sd1/c16-b/Strength_SQ + - srmag/m-sd1/c16-b/Strength +- type: pyaml.magnet.cfm_magnet + name: SH2B-C16 + mapping: + - [B0, SH2B-C16-H] + - [A0, SH2B-C16-V] + - [A1, SH2B-C16-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh2/c16-b-ch1/current + - srmag/ps-corr-sh2/c16-b-ch2/current + - srmag/ps-corr-sh2/c16-b-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SD1D-C16 + mapping: + - [B0, SD1D-C16-H] + - [A0, SD1D-C16-V] + - [A1, SD1D-C16-SQ] + - [B2, SD1D-C16-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c16-d/Strength_H + - srmag/m-sd1/c16-d/Strength_V + - srmag/m-sd1/c16-d/Strength_SQ + - srmag/m-sd1/c16-d/Strength +- type: pyaml.magnet.cfm_magnet + name: SF2E-C16 + mapping: + - [B0, SF2E-C16-H] + - [A0, SF2E-C16-V] + - [A1, SF2E-C16-SQ] + - [B2, SF2E-C16-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sf2/c16-e/Strength_H + - srmag/m-sf2/c16-e/Strength_V + - srmag/m-sf2/c16-e/Strength_SQ + - srmag/m-sf2/c16-e/Strength +- type: pyaml.magnet.cfm_magnet + name: SD1E-C16 + mapping: + - [B0, SD1E-C16-H] + - [A0, SD1E-C16-V] + - [A1, SD1E-C16-SQ] + - [B2, SD1E-C16-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c16-e/Strength_H + - srmag/m-sd1/c16-e/Strength_V + - srmag/m-sd1/c16-e/Strength_SQ + - srmag/m-sd1/c16-e/Strength +- type: pyaml.magnet.cfm_magnet + name: SH3E-C16 + mapping: + - [B0, SH3E-C16-H] + - [A0, SH3E-C16-V] + - [A1, SH3E-C16-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh3/c16-e-ch1/current + - srmag/ps-corr-sh3/c16-e-ch2/current + - srmag/ps-corr-sh3/c16-e-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SH1A-C17 + mapping: + - [B0, SH1A-C17-H] + - [A0, SH1A-C17-V] + - [A1, SH1A-C17-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh1/c17-a-ch1/current + - srmag/ps-corr-sh1/c17-a-ch2/current + - srmag/ps-corr-sh1/c17-a-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SD1A-C17 + mapping: + - [B0, SD1A-C17-H] + - [A0, SD1A-C17-V] + - [A1, SD1A-C17-SQ] + - [B2, SD1A-C17-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c17-a/Strength_H + - srmag/m-sd1/c17-a/Strength_V + - srmag/m-sd1/c17-a/Strength_SQ + - srmag/m-sd1/c17-a/Strength +- type: pyaml.magnet.cfm_magnet + name: SF2A-C17 + mapping: + - [B0, SF2A-C17-H] + - [A0, SF2A-C17-V] + - [A1, SF2A-C17-SQ] + - [B2, SF2A-C17-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sf2/c17-a/Strength_H + - srmag/m-sf2/c17-a/Strength_V + - srmag/m-sf2/c17-a/Strength_SQ + - srmag/m-sf2/c17-a/Strength +- type: pyaml.magnet.cfm_magnet + name: SD1B-C17 + mapping: + - [B0, SD1B-C17-H] + - [A0, SD1B-C17-V] + - [A1, SD1B-C17-SQ] + - [B2, SD1B-C17-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c17-b/Strength_H + - srmag/m-sd1/c17-b/Strength_V + - srmag/m-sd1/c17-b/Strength_SQ + - srmag/m-sd1/c17-b/Strength +- type: pyaml.magnet.cfm_magnet + name: SH2B-C17 + mapping: + - [B0, SH2B-C17-H] + - [A0, SH2B-C17-V] + - [A1, SH2B-C17-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh2/c17-b-ch1/current + - srmag/ps-corr-sh2/c17-b-ch2/current + - srmag/ps-corr-sh2/c17-b-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SD1D-C17 + mapping: + - [B0, SD1D-C17-H] + - [A0, SD1D-C17-V] + - [A1, SD1D-C17-SQ] + - [B2, SD1D-C17-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c17-d/Strength_H + - srmag/m-sd1/c17-d/Strength_V + - srmag/m-sd1/c17-d/Strength_SQ + - srmag/m-sd1/c17-d/Strength +- type: pyaml.magnet.cfm_magnet + name: SF2E-C17 + mapping: + - [B0, SF2E-C17-H] + - [A0, SF2E-C17-V] + - [A1, SF2E-C17-SQ] + - [B2, SF2E-C17-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sf2/c17-e/Strength_H + - srmag/m-sf2/c17-e/Strength_V + - srmag/m-sf2/c17-e/Strength_SQ + - srmag/m-sf2/c17-e/Strength +- type: pyaml.magnet.cfm_magnet + name: SD1E-C17 + mapping: + - [B0, SD1E-C17-H] + - [A0, SD1E-C17-V] + - [A1, SD1E-C17-SQ] + - [B2, SD1E-C17-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c17-e/Strength_H + - srmag/m-sd1/c17-e/Strength_V + - srmag/m-sd1/c17-e/Strength_SQ + - srmag/m-sd1/c17-e/Strength +- type: pyaml.magnet.cfm_magnet + name: SH3E-C17 + mapping: + - [B0, SH3E-C17-H] + - [A0, SH3E-C17-V] + - [A1, SH3E-C17-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh3/c17-e-ch1/current + - srmag/ps-corr-sh3/c17-e-ch2/current + - srmag/ps-corr-sh3/c17-e-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SH1A-C18 + mapping: + - [B0, SH1A-C18-H] + - [A0, SH1A-C18-V] + - [A1, SH1A-C18-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh1/c18-a-ch1/current + - srmag/ps-corr-sh1/c18-a-ch2/current + - srmag/ps-corr-sh1/c18-a-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SD1A-C18 + mapping: + - [B0, SD1A-C18-H] + - [A0, SD1A-C18-V] + - [A1, SD1A-C18-SQ] + - [B2, SD1A-C18-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c18-a/Strength_H + - srmag/m-sd1/c18-a/Strength_V + - srmag/m-sd1/c18-a/Strength_SQ + - srmag/m-sd1/c18-a/Strength +- type: pyaml.magnet.cfm_magnet + name: SF2A-C18 + mapping: + - [B0, SF2A-C18-H] + - [A0, SF2A-C18-V] + - [A1, SF2A-C18-SQ] + - [B2, SF2A-C18-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sf2/c18-a/Strength_H + - srmag/m-sf2/c18-a/Strength_V + - srmag/m-sf2/c18-a/Strength_SQ + - srmag/m-sf2/c18-a/Strength +- type: pyaml.magnet.cfm_magnet + name: SD1B-C18 + mapping: + - [B0, SD1B-C18-H] + - [A0, SD1B-C18-V] + - [A1, SD1B-C18-SQ] + - [B2, SD1B-C18-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c18-b/Strength_H + - srmag/m-sd1/c18-b/Strength_V + - srmag/m-sd1/c18-b/Strength_SQ + - srmag/m-sd1/c18-b/Strength +- type: pyaml.magnet.cfm_magnet + name: SH2B-C18 + mapping: + - [B0, SH2B-C18-H] + - [A0, SH2B-C18-V] + - [A1, SH2B-C18-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh2/c18-b-ch1/current + - srmag/ps-corr-sh2/c18-b-ch2/current + - srmag/ps-corr-sh2/c18-b-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SD1D-C18 + mapping: + - [B0, SD1D-C18-H] + - [A0, SD1D-C18-V] + - [A1, SD1D-C18-SQ] + - [B2, SD1D-C18-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c18-d/Strength_H + - srmag/m-sd1/c18-d/Strength_V + - srmag/m-sd1/c18-d/Strength_SQ + - srmag/m-sd1/c18-d/Strength +- type: pyaml.magnet.cfm_magnet + name: SF2E-C18 + mapping: + - [B0, SF2E-C18-H] + - [A0, SF2E-C18-V] + - [A1, SF2E-C18-SQ] + - [B2, SF2E-C18-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sf2/c18-e/Strength_H + - srmag/m-sf2/c18-e/Strength_V + - srmag/m-sf2/c18-e/Strength_SQ + - srmag/m-sf2/c18-e/Strength +- type: pyaml.magnet.cfm_magnet + name: SD1E-C18 + mapping: + - [B0, SD1E-C18-H] + - [A0, SD1E-C18-V] + - [A1, SD1E-C18-SQ] + - [B2, SD1E-C18-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c18-e/Strength_H + - srmag/m-sd1/c18-e/Strength_V + - srmag/m-sd1/c18-e/Strength_SQ + - srmag/m-sd1/c18-e/Strength +- type: pyaml.magnet.cfm_magnet + name: SH3E-C18 + mapping: + - [B0, SH3E-C18-H] + - [A0, SH3E-C18-V] + - [A1, SH3E-C18-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh3/c18-e-ch1/current + - srmag/ps-corr-sh3/c18-e-ch2/current + - srmag/ps-corr-sh3/c18-e-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SH1A-C19 + mapping: + - [B0, SH1A-C19-H] + - [A0, SH1A-C19-V] + - [A1, SH1A-C19-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh1/c19-a-ch1/current + - srmag/ps-corr-sh1/c19-a-ch2/current + - srmag/ps-corr-sh1/c19-a-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SD1A-C19 + mapping: + - [B0, SD1A-C19-H] + - [A0, SD1A-C19-V] + - [A1, SD1A-C19-SQ] + - [B2, SD1A-C19-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c19-a/Strength_H + - srmag/m-sd1/c19-a/Strength_V + - srmag/m-sd1/c19-a/Strength_SQ + - srmag/m-sd1/c19-a/Strength +- type: pyaml.magnet.cfm_magnet + name: SF2A-C19 + mapping: + - [B0, SF2A-C19-H] + - [A0, SF2A-C19-V] + - [A1, SF2A-C19-SQ] + - [B2, SF2A-C19-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sf2/c19-a/Strength_H + - srmag/m-sf2/c19-a/Strength_V + - srmag/m-sf2/c19-a/Strength_SQ + - srmag/m-sf2/c19-a/Strength +- type: pyaml.magnet.cfm_magnet + name: SD1B-C19 + mapping: + - [B0, SD1B-C19-H] + - [A0, SD1B-C19-V] + - [A1, SD1B-C19-SQ] + - [B2, SD1B-C19-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c19-b/Strength_H + - srmag/m-sd1/c19-b/Strength_V + - srmag/m-sd1/c19-b/Strength_SQ + - srmag/m-sd1/c19-b/Strength +- type: pyaml.magnet.cfm_magnet + name: SH2B-C19 + mapping: + - [B0, SH2B-C19-H] + - [A0, SH2B-C19-V] + - [A1, SH2B-C19-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh2/c19-b-ch1/current + - srmag/ps-corr-sh2/c19-b-ch2/current + - srmag/ps-corr-sh2/c19-b-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SD1D-C19 + mapping: + - [B0, SD1D-C19-H] + - [A0, SD1D-C19-V] + - [A1, SD1D-C19-SQ] + - [B2, SD1D-C19-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c19-d/Strength_H + - srmag/m-sd1/c19-d/Strength_V + - srmag/m-sd1/c19-d/Strength_SQ + - srmag/m-sd1/c19-d/Strength +- type: pyaml.magnet.cfm_magnet + name: SF2E-C19 + mapping: + - [B0, SF2E-C19-H] + - [A0, SF2E-C19-V] + - [A1, SF2E-C19-SQ] + - [B2, SF2E-C19-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sf2/c19-e/Strength_H + - srmag/m-sf2/c19-e/Strength_V + - srmag/m-sf2/c19-e/Strength_SQ + - srmag/m-sf2/c19-e/Strength +- type: pyaml.magnet.cfm_magnet + name: SD1E-C19 + mapping: + - [B0, SD1E-C19-H] + - [A0, SD1E-C19-V] + - [A1, SD1E-C19-SQ] + - [B2, SD1E-C19-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c19-e/Strength_H + - srmag/m-sd1/c19-e/Strength_V + - srmag/m-sd1/c19-e/Strength_SQ + - srmag/m-sd1/c19-e/Strength +- type: pyaml.magnet.cfm_magnet + name: SH3E-C19 + mapping: + - [B0, SH3E-C19-H] + - [A0, SH3E-C19-V] + - [A1, SH3E-C19-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh3/c19-e-ch1/current + - srmag/ps-corr-sh3/c19-e-ch2/current + - srmag/ps-corr-sh3/c19-e-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SH1A-C20 + mapping: + - [B0, SH1A-C20-H] + - [A0, SH1A-C20-V] + - [A1, SH1A-C20-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh1/c20-a-ch1/current + - srmag/ps-corr-sh1/c20-a-ch2/current + - srmag/ps-corr-sh1/c20-a-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SD1A-C20 + mapping: + - [B0, SD1A-C20-H] + - [A0, SD1A-C20-V] + - [A1, SD1A-C20-SQ] + - [B2, SD1A-C20-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c20-a/Strength_H + - srmag/m-sd1/c20-a/Strength_V + - srmag/m-sd1/c20-a/Strength_SQ + - srmag/m-sd1/c20-a/Strength +- type: pyaml.magnet.cfm_magnet + name: SF2A-C20 + mapping: + - [B0, SF2A-C20-H] + - [A0, SF2A-C20-V] + - [A1, SF2A-C20-SQ] + - [B2, SF2A-C20-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sf2/c20-a/Strength_H + - srmag/m-sf2/c20-a/Strength_V + - srmag/m-sf2/c20-a/Strength_SQ + - srmag/m-sf2/c20-a/Strength +- type: pyaml.magnet.cfm_magnet + name: SD1B-C20 + mapping: + - [B0, SD1B-C20-H] + - [A0, SD1B-C20-V] + - [A1, SD1B-C20-SQ] + - [B2, SD1B-C20-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c20-b/Strength_H + - srmag/m-sd1/c20-b/Strength_V + - srmag/m-sd1/c20-b/Strength_SQ + - srmag/m-sd1/c20-b/Strength +- type: pyaml.magnet.cfm_magnet + name: SH2B-C20 + mapping: + - [B0, SH2B-C20-H] + - [A0, SH2B-C20-V] + - [A1, SH2B-C20-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh2/c20-b-ch1/current + - srmag/ps-corr-sh2/c20-b-ch2/current + - srmag/ps-corr-sh2/c20-b-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SD1D-C20 + mapping: + - [B0, SD1D-C20-H] + - [A0, SD1D-C20-V] + - [A1, SD1D-C20-SQ] + - [B2, SD1D-C20-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c20-d/Strength_H + - srmag/m-sd1/c20-d/Strength_V + - srmag/m-sd1/c20-d/Strength_SQ + - srmag/m-sd1/c20-d/Strength +- type: pyaml.magnet.cfm_magnet + name: SF2E-C20 + mapping: + - [B0, SF2E-C20-H] + - [A0, SF2E-C20-V] + - [A1, SF2E-C20-SQ] + - [B2, SF2E-C20-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sf2/c20-e/Strength_H + - srmag/m-sf2/c20-e/Strength_V + - srmag/m-sf2/c20-e/Strength_SQ + - srmag/m-sf2/c20-e/Strength +- type: pyaml.magnet.cfm_magnet + name: SD1E-C20 + mapping: + - [B0, SD1E-C20-H] + - [A0, SD1E-C20-V] + - [A1, SD1E-C20-SQ] + - [B2, SD1E-C20-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c20-e/Strength_H + - srmag/m-sd1/c20-e/Strength_V + - srmag/m-sd1/c20-e/Strength_SQ + - srmag/m-sd1/c20-e/Strength +- type: pyaml.magnet.cfm_magnet + name: SH3E-C20 + mapping: + - [B0, SH3E-C20-H] + - [A0, SH3E-C20-V] + - [A1, SH3E-C20-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh3/c20-e-ch1/current + - srmag/ps-corr-sh3/c20-e-ch2/current + - srmag/ps-corr-sh3/c20-e-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SH1A-C21 + mapping: + - [B0, SH1A-C21-H] + - [A0, SH1A-C21-V] + - [A1, SH1A-C21-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh1/c21-a-ch1/current + - srmag/ps-corr-sh1/c21-a-ch2/current + - srmag/ps-corr-sh1/c21-a-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SD1A-C21 + mapping: + - [B0, SD1A-C21-H] + - [A0, SD1A-C21-V] + - [A1, SD1A-C21-SQ] + - [B2, SD1A-C21-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c21-a/Strength_H + - srmag/m-sd1/c21-a/Strength_V + - srmag/m-sd1/c21-a/Strength_SQ + - srmag/m-sd1/c21-a/Strength +- type: pyaml.magnet.cfm_magnet + name: SF2A-C21 + mapping: + - [B0, SF2A-C21-H] + - [A0, SF2A-C21-V] + - [A1, SF2A-C21-SQ] + - [B2, SF2A-C21-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sf2/c21-a/Strength_H + - srmag/m-sf2/c21-a/Strength_V + - srmag/m-sf2/c21-a/Strength_SQ + - srmag/m-sf2/c21-a/Strength +- type: pyaml.magnet.cfm_magnet + name: SD1B-C21 + mapping: + - [B0, SD1B-C21-H] + - [A0, SD1B-C21-V] + - [A1, SD1B-C21-SQ] + - [B2, SD1B-C21-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c21-b/Strength_H + - srmag/m-sd1/c21-b/Strength_V + - srmag/m-sd1/c21-b/Strength_SQ + - srmag/m-sd1/c21-b/Strength +- type: pyaml.magnet.cfm_magnet + name: SH2B-C21 + mapping: + - [B0, SH2B-C21-H] + - [A0, SH2B-C21-V] + - [A1, SH2B-C21-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh2/c21-b-ch1/current + - srmag/ps-corr-sh2/c21-b-ch2/current + - srmag/ps-corr-sh2/c21-b-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SD1D-C21 + mapping: + - [B0, SD1D-C21-H] + - [A0, SD1D-C21-V] + - [A1, SD1D-C21-SQ] + - [B2, SD1D-C21-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c21-d/Strength_H + - srmag/m-sd1/c21-d/Strength_V + - srmag/m-sd1/c21-d/Strength_SQ + - srmag/m-sd1/c21-d/Strength +- type: pyaml.magnet.cfm_magnet + name: SF2E-C21 + mapping: + - [B0, SF2E-C21-H] + - [A0, SF2E-C21-V] + - [A1, SF2E-C21-SQ] + - [B2, SF2E-C21-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sf2/c21-e/Strength_H + - srmag/m-sf2/c21-e/Strength_V + - srmag/m-sf2/c21-e/Strength_SQ + - srmag/m-sf2/c21-e/Strength +- type: pyaml.magnet.cfm_magnet + name: SD1E-C21 + mapping: + - [B0, SD1E-C21-H] + - [A0, SD1E-C21-V] + - [A1, SD1E-C21-SQ] + - [B2, SD1E-C21-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c21-e/Strength_H + - srmag/m-sd1/c21-e/Strength_V + - srmag/m-sd1/c21-e/Strength_SQ + - srmag/m-sd1/c21-e/Strength +- type: pyaml.magnet.cfm_magnet + name: SH3E-C21 + mapping: + - [B0, SH3E-C21-H] + - [A0, SH3E-C21-V] + - [A1, SH3E-C21-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh3/c21-e-ch1/current + - srmag/ps-corr-sh3/c21-e-ch2/current + - srmag/ps-corr-sh3/c21-e-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SH1A-C22 + mapping: + - [B0, SH1A-C22-H] + - [A0, SH1A-C22-V] + - [A1, SH1A-C22-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh1/c22-a-ch1/current + - srmag/ps-corr-sh1/c22-a-ch2/current + - srmag/ps-corr-sh1/c22-a-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SD1A-C22 + mapping: + - [B0, SD1A-C22-H] + - [A0, SD1A-C22-V] + - [A1, SD1A-C22-SQ] + - [B2, SD1A-C22-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c22-a/Strength_H + - srmag/m-sd1/c22-a/Strength_V + - srmag/m-sd1/c22-a/Strength_SQ + - srmag/m-sd1/c22-a/Strength +- type: pyaml.magnet.cfm_magnet + name: SF2A-C22 + mapping: + - [B0, SF2A-C22-H] + - [A0, SF2A-C22-V] + - [A1, SF2A-C22-SQ] + - [B2, SF2A-C22-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sf2/c22-a/Strength_H + - srmag/m-sf2/c22-a/Strength_V + - srmag/m-sf2/c22-a/Strength_SQ + - srmag/m-sf2/c22-a/Strength +- type: pyaml.magnet.cfm_magnet + name: SD1B-C22 + mapping: + - [B0, SD1B-C22-H] + - [A0, SD1B-C22-V] + - [A1, SD1B-C22-SQ] + - [B2, SD1B-C22-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c22-b/Strength_H + - srmag/m-sd1/c22-b/Strength_V + - srmag/m-sd1/c22-b/Strength_SQ + - srmag/m-sd1/c22-b/Strength +- type: pyaml.magnet.cfm_magnet + name: SH2B-C22 + mapping: + - [B0, SH2B-C22-H] + - [A0, SH2B-C22-V] + - [A1, SH2B-C22-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh2/c22-b-ch1/current + - srmag/ps-corr-sh2/c22-b-ch2/current + - srmag/ps-corr-sh2/c22-b-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SD1D-C22 + mapping: + - [B0, SD1D-C22-H] + - [A0, SD1D-C22-V] + - [A1, SD1D-C22-SQ] + - [B2, SD1D-C22-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c22-d/Strength_H + - srmag/m-sd1/c22-d/Strength_V + - srmag/m-sd1/c22-d/Strength_SQ + - srmag/m-sd1/c22-d/Strength +- type: pyaml.magnet.cfm_magnet + name: SF2E-C22 + mapping: + - [B0, SF2E-C22-H] + - [A0, SF2E-C22-V] + - [A1, SF2E-C22-SQ] + - [B2, SF2E-C22-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sf2/c22-e/Strength_H + - srmag/m-sf2/c22-e/Strength_V + - srmag/m-sf2/c22-e/Strength_SQ + - srmag/m-sf2/c22-e/Strength +- type: pyaml.magnet.cfm_magnet + name: SD1E-C22 + mapping: + - [B0, SD1E-C22-H] + - [A0, SD1E-C22-V] + - [A1, SD1E-C22-SQ] + - [B2, SD1E-C22-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c22-e/Strength_H + - srmag/m-sd1/c22-e/Strength_V + - srmag/m-sd1/c22-e/Strength_SQ + - srmag/m-sd1/c22-e/Strength +- type: pyaml.magnet.cfm_magnet + name: SH3E-C22 + mapping: + - [B0, SH3E-C22-H] + - [A0, SH3E-C22-V] + - [A1, SH3E-C22-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh3/c22-e-ch1/current + - srmag/ps-corr-sh3/c22-e-ch2/current + - srmag/ps-corr-sh3/c22-e-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SH1A-C23 + mapping: + - [B0, SH1A-C23-H] + - [A0, SH1A-C23-V] + - [A1, SH1A-C23-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh1/c23-a-ch1/current + - srmag/ps-corr-sh1/c23-a-ch2/current + - srmag/ps-corr-sh1/c23-a-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SD1A-C23 + mapping: + - [B0, SD1A-C23-H] + - [A0, SD1A-C23-V] + - [A1, SD1A-C23-SQ] + - [B2, SD1A-C23-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c23-a/Strength_H + - srmag/m-sd1/c23-a/Strength_V + - srmag/m-sd1/c23-a/Strength_SQ + - srmag/m-sd1/c23-a/Strength +- type: pyaml.magnet.cfm_magnet + name: SF2A-C23 + mapping: + - [B0, SF2A-C23-H] + - [A0, SF2A-C23-V] + - [A1, SF2A-C23-SQ] + - [B2, SF2A-C23-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sf2/c23-a/Strength_H + - srmag/m-sf2/c23-a/Strength_V + - srmag/m-sf2/c23-a/Strength_SQ + - srmag/m-sf2/c23-a/Strength +- type: pyaml.magnet.cfm_magnet + name: SD1B-C23 + mapping: + - [B0, SD1B-C23-H] + - [A0, SD1B-C23-V] + - [A1, SD1B-C23-SQ] + - [B2, SD1B-C23-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c23-b/Strength_H + - srmag/m-sd1/c23-b/Strength_V + - srmag/m-sd1/c23-b/Strength_SQ + - srmag/m-sd1/c23-b/Strength +- type: pyaml.magnet.cfm_magnet + name: SH2B-C23 + mapping: + - [B0, SH2B-C23-H] + - [A0, SH2B-C23-V] + - [A1, SH2B-C23-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh2/c23-b-ch1/current + - srmag/ps-corr-sh2/c23-b-ch2/current + - srmag/ps-corr-sh2/c23-b-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SD1D-C23 + mapping: + - [B0, SD1D-C23-H] + - [A0, SD1D-C23-V] + - [A1, SD1D-C23-SQ] + - [B2, SD1D-C23-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c23-d/Strength_H + - srmag/m-sd1/c23-d/Strength_V + - srmag/m-sd1/c23-d/Strength_SQ + - srmag/m-sd1/c23-d/Strength +- type: pyaml.magnet.cfm_magnet + name: SF2E-C23 + mapping: + - [B0, SF2E-C23-H] + - [A0, SF2E-C23-V] + - [A1, SF2E-C23-SQ] + - [B2, SF2E-C23-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sf2/c23-e/Strength_H + - srmag/m-sf2/c23-e/Strength_V + - srmag/m-sf2/c23-e/Strength_SQ + - srmag/m-sf2/c23-e/Strength +- type: pyaml.magnet.cfm_magnet + name: SD1E-C23 + mapping: + - [B0, SD1E-C23-H] + - [A0, SD1E-C23-V] + - [A1, SD1E-C23-SQ] + - [B2, SD1E-C23-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c23-e/Strength_H + - srmag/m-sd1/c23-e/Strength_V + - srmag/m-sd1/c23-e/Strength_SQ + - srmag/m-sd1/c23-e/Strength +- type: pyaml.magnet.cfm_magnet + name: SH3E-C23 + mapping: + - [B0, SH3E-C23-H] + - [A0, SH3E-C23-V] + - [A1, SH3E-C23-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh3/c23-e-ch1/current + - srmag/ps-corr-sh3/c23-e-ch2/current + - srmag/ps-corr-sh3/c23-e-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SH1A-C24 + mapping: + - [B0, SH1A-C24-H] + - [A0, SH1A-C24-V] + - [A1, SH1A-C24-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh1/c24-a-ch1/current + - srmag/ps-corr-sh1/c24-a-ch2/current + - srmag/ps-corr-sh1/c24-a-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SD1A-C24 + mapping: + - [B0, SD1A-C24-H] + - [A0, SD1A-C24-V] + - [A1, SD1A-C24-SQ] + - [B2, SD1A-C24-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c24-a/Strength_H + - srmag/m-sd1/c24-a/Strength_V + - srmag/m-sd1/c24-a/Strength_SQ + - srmag/m-sd1/c24-a/Strength +- type: pyaml.magnet.cfm_magnet + name: SF2A-C24 + mapping: + - [B0, SF2A-C24-H] + - [A0, SF2A-C24-V] + - [A1, SF2A-C24-SQ] + - [B2, SF2A-C24-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sf2/c24-a/Strength_H + - srmag/m-sf2/c24-a/Strength_V + - srmag/m-sf2/c24-a/Strength_SQ + - srmag/m-sf2/c24-a/Strength +- type: pyaml.magnet.cfm_magnet + name: SD1B-C24 + mapping: + - [B0, SD1B-C24-H] + - [A0, SD1B-C24-V] + - [A1, SD1B-C24-SQ] + - [B2, SD1B-C24-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c24-b/Strength_H + - srmag/m-sd1/c24-b/Strength_V + - srmag/m-sd1/c24-b/Strength_SQ + - srmag/m-sd1/c24-b/Strength +- type: pyaml.magnet.cfm_magnet + name: SH2B-C24 + mapping: + - [B0, SH2B-C24-H] + - [A0, SH2B-C24-V] + - [A1, SH2B-C24-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh2/c24-b-ch1/current + - srmag/ps-corr-sh2/c24-b-ch2/current + - srmag/ps-corr-sh2/c24-b-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SD1D-C24 + mapping: + - [B0, SD1D-C24-H] + - [A0, SD1D-C24-V] + - [A1, SD1D-C24-SQ] + - [B2, SD1D-C24-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c24-d/Strength_H + - srmag/m-sd1/c24-d/Strength_V + - srmag/m-sd1/c24-d/Strength_SQ + - srmag/m-sd1/c24-d/Strength +- type: pyaml.magnet.cfm_magnet + name: SF2E-C24 + mapping: + - [B0, SF2E-C24-H] + - [A0, SF2E-C24-V] + - [A1, SF2E-C24-SQ] + - [B2, SF2E-C24-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sf2/c24-e/Strength_H + - srmag/m-sf2/c24-e/Strength_V + - srmag/m-sf2/c24-e/Strength_SQ + - srmag/m-sf2/c24-e/Strength +- type: pyaml.magnet.cfm_magnet + name: SD1E-C24 + mapping: + - [B0, SD1E-C24-H] + - [A0, SD1E-C24-V] + - [A1, SD1E-C24-SQ] + - [B2, SD1E-C24-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c24-e/Strength_H + - srmag/m-sd1/c24-e/Strength_V + - srmag/m-sd1/c24-e/Strength_SQ + - srmag/m-sd1/c24-e/Strength +- type: pyaml.magnet.cfm_magnet + name: SH3E-C24 + mapping: + - [B0, SH3E-C24-H] + - [A0, SH3E-C24-V] + - [A1, SH3E-C24-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh3/c24-e-ch1/current + - srmag/ps-corr-sh3/c24-e-ch2/current + - srmag/ps-corr-sh3/c24-e-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SH1A-C25 + mapping: + - [B0, SH1A-C25-H] + - [A0, SH1A-C25-V] + - [A1, SH1A-C25-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh1/c25-a-ch1/current + - srmag/ps-corr-sh1/c25-a-ch2/current + - srmag/ps-corr-sh1/c25-a-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SD1A-C25 + mapping: + - [B0, SD1A-C25-H] + - [A0, SD1A-C25-V] + - [A1, SD1A-C25-SQ] + - [B2, SD1A-C25-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c25-a/Strength_H + - srmag/m-sd1/c25-a/Strength_V + - srmag/m-sd1/c25-a/Strength_SQ + - srmag/m-sd1/c25-a/Strength +- type: pyaml.magnet.cfm_magnet + name: SF2A-C25 + mapping: + - [B0, SF2A-C25-H] + - [A0, SF2A-C25-V] + - [A1, SF2A-C25-SQ] + - [B2, SF2A-C25-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sf2/c25-a/Strength_H + - srmag/m-sf2/c25-a/Strength_V + - srmag/m-sf2/c25-a/Strength_SQ + - srmag/m-sf2/c25-a/Strength +- type: pyaml.magnet.cfm_magnet + name: SD1B-C25 + mapping: + - [B0, SD1B-C25-H] + - [A0, SD1B-C25-V] + - [A1, SD1B-C25-SQ] + - [B2, SD1B-C25-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c25-b/Strength_H + - srmag/m-sd1/c25-b/Strength_V + - srmag/m-sd1/c25-b/Strength_SQ + - srmag/m-sd1/c25-b/Strength +- type: pyaml.magnet.cfm_magnet + name: SH2B-C25 + mapping: + - [B0, SH2B-C25-H] + - [A0, SH2B-C25-V] + - [A1, SH2B-C25-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh2/c25-b-ch1/current + - srmag/ps-corr-sh2/c25-b-ch2/current + - srmag/ps-corr-sh2/c25-b-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SD1D-C25 + mapping: + - [B0, SD1D-C25-H] + - [A0, SD1D-C25-V] + - [A1, SD1D-C25-SQ] + - [B2, SD1D-C25-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c25-d/Strength_H + - srmag/m-sd1/c25-d/Strength_V + - srmag/m-sd1/c25-d/Strength_SQ + - srmag/m-sd1/c25-d/Strength +- type: pyaml.magnet.cfm_magnet + name: SF2E-C25 + mapping: + - [B0, SF2E-C25-H] + - [A0, SF2E-C25-V] + - [A1, SF2E-C25-SQ] + - [B2, SF2E-C25-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sf2/c25-e/Strength_H + - srmag/m-sf2/c25-e/Strength_V + - srmag/m-sf2/c25-e/Strength_SQ + - srmag/m-sf2/c25-e/Strength +- type: pyaml.magnet.cfm_magnet + name: SD1E-C25 + mapping: + - [B0, SD1E-C25-H] + - [A0, SD1E-C25-V] + - [A1, SD1E-C25-SQ] + - [B2, SD1E-C25-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c25-e/Strength_H + - srmag/m-sd1/c25-e/Strength_V + - srmag/m-sd1/c25-e/Strength_SQ + - srmag/m-sd1/c25-e/Strength +- type: pyaml.magnet.cfm_magnet + name: SH3E-C25 + mapping: + - [B0, SH3E-C25-H] + - [A0, SH3E-C25-V] + - [A1, SH3E-C25-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh3/c25-e-ch1/current + - srmag/ps-corr-sh3/c25-e-ch2/current + - srmag/ps-corr-sh3/c25-e-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SH1A-C26 + mapping: + - [B0, SH1A-C26-H] + - [A0, SH1A-C26-V] + - [A1, SH1A-C26-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh1/c26-a-ch1/current + - srmag/ps-corr-sh1/c26-a-ch2/current + - srmag/ps-corr-sh1/c26-a-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SD1A-C26 + mapping: + - [B0, SD1A-C26-H] + - [A0, SD1A-C26-V] + - [A1, SD1A-C26-SQ] + - [B2, SD1A-C26-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c26-a/Strength_H + - srmag/m-sd1/c26-a/Strength_V + - srmag/m-sd1/c26-a/Strength_SQ + - srmag/m-sd1/c26-a/Strength +- type: pyaml.magnet.cfm_magnet + name: SF2A-C26 + mapping: + - [B0, SF2A-C26-H] + - [A0, SF2A-C26-V] + - [A1, SF2A-C26-SQ] + - [B2, SF2A-C26-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sf2/c26-a/Strength_H + - srmag/m-sf2/c26-a/Strength_V + - srmag/m-sf2/c26-a/Strength_SQ + - srmag/m-sf2/c26-a/Strength +- type: pyaml.magnet.cfm_magnet + name: SD1B-C26 + mapping: + - [B0, SD1B-C26-H] + - [A0, SD1B-C26-V] + - [A1, SD1B-C26-SQ] + - [B2, SD1B-C26-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c26-b/Strength_H + - srmag/m-sd1/c26-b/Strength_V + - srmag/m-sd1/c26-b/Strength_SQ + - srmag/m-sd1/c26-b/Strength +- type: pyaml.magnet.cfm_magnet + name: SH2B-C26 + mapping: + - [B0, SH2B-C26-H] + - [A0, SH2B-C26-V] + - [A1, SH2B-C26-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh2/c26-b-ch1/current + - srmag/ps-corr-sh2/c26-b-ch2/current + - srmag/ps-corr-sh2/c26-b-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SD1D-C26 + mapping: + - [B0, SD1D-C26-H] + - [A0, SD1D-C26-V] + - [A1, SD1D-C26-SQ] + - [B2, SD1D-C26-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c26-d/Strength_H + - srmag/m-sd1/c26-d/Strength_V + - srmag/m-sd1/c26-d/Strength_SQ + - srmag/m-sd1/c26-d/Strength +- type: pyaml.magnet.cfm_magnet + name: SF2E-C26 + mapping: + - [B0, SF2E-C26-H] + - [A0, SF2E-C26-V] + - [A1, SF2E-C26-SQ] + - [B2, SF2E-C26-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sf2/c26-e/Strength_H + - srmag/m-sf2/c26-e/Strength_V + - srmag/m-sf2/c26-e/Strength_SQ + - srmag/m-sf2/c26-e/Strength +- type: pyaml.magnet.cfm_magnet + name: SD1E-C26 + mapping: + - [B0, SD1E-C26-H] + - [A0, SD1E-C26-V] + - [A1, SD1E-C26-SQ] + - [B2, SD1E-C26-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c26-e/Strength_H + - srmag/m-sd1/c26-e/Strength_V + - srmag/m-sd1/c26-e/Strength_SQ + - srmag/m-sd1/c26-e/Strength +- type: pyaml.magnet.cfm_magnet + name: SH3E-C26 + mapping: + - [B0, SH3E-C26-H] + - [A0, SH3E-C26-V] + - [A1, SH3E-C26-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh3/c26-e-ch1/current + - srmag/ps-corr-sh3/c26-e-ch2/current + - srmag/ps-corr-sh3/c26-e-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SH1A-C27 + mapping: + - [B0, SH1A-C27-H] + - [A0, SH1A-C27-V] + - [A1, SH1A-C27-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh1/c27-a-ch1/current + - srmag/ps-corr-sh1/c27-a-ch2/current + - srmag/ps-corr-sh1/c27-a-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SD1A-C27 + mapping: + - [B0, SD1A-C27-H] + - [A0, SD1A-C27-V] + - [A1, SD1A-C27-SQ] + - [B2, SD1A-C27-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c27-a/Strength_H + - srmag/m-sd1/c27-a/Strength_V + - srmag/m-sd1/c27-a/Strength_SQ + - srmag/m-sd1/c27-a/Strength +- type: pyaml.magnet.cfm_magnet + name: SF2A-C27 + mapping: + - [B0, SF2A-C27-H] + - [A0, SF2A-C27-V] + - [A1, SF2A-C27-SQ] + - [B2, SF2A-C27-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sf2/c27-a/Strength_H + - srmag/m-sf2/c27-a/Strength_V + - srmag/m-sf2/c27-a/Strength_SQ + - srmag/m-sf2/c27-a/Strength +- type: pyaml.magnet.cfm_magnet + name: SD1B-C27 + mapping: + - [B0, SD1B-C27-H] + - [A0, SD1B-C27-V] + - [A1, SD1B-C27-SQ] + - [B2, SD1B-C27-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c27-b/Strength_H + - srmag/m-sd1/c27-b/Strength_V + - srmag/m-sd1/c27-b/Strength_SQ + - srmag/m-sd1/c27-b/Strength +- type: pyaml.magnet.cfm_magnet + name: SH2B-C27 + mapping: + - [B0, SH2B-C27-H] + - [A0, SH2B-C27-V] + - [A1, SH2B-C27-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh2/c27-b-ch1/current + - srmag/ps-corr-sh2/c27-b-ch2/current + - srmag/ps-corr-sh2/c27-b-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SD1D-C27 + mapping: + - [B0, SD1D-C27-H] + - [A0, SD1D-C27-V] + - [A1, SD1D-C27-SQ] + - [B2, SD1D-C27-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c27-d/Strength_H + - srmag/m-sd1/c27-d/Strength_V + - srmag/m-sd1/c27-d/Strength_SQ + - srmag/m-sd1/c27-d/Strength +- type: pyaml.magnet.cfm_magnet + name: SF2E-C27 + mapping: + - [B0, SF2E-C27-H] + - [A0, SF2E-C27-V] + - [A1, SF2E-C27-SQ] + - [B2, SF2E-C27-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sf2/c27-e/Strength_H + - srmag/m-sf2/c27-e/Strength_V + - srmag/m-sf2/c27-e/Strength_SQ + - srmag/m-sf2/c27-e/Strength +- type: pyaml.magnet.cfm_magnet + name: SD1E-C27 + mapping: + - [B0, SD1E-C27-H] + - [A0, SD1E-C27-V] + - [A1, SD1E-C27-SQ] + - [B2, SD1E-C27-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c27-e/Strength_H + - srmag/m-sd1/c27-e/Strength_V + - srmag/m-sd1/c27-e/Strength_SQ + - srmag/m-sd1/c27-e/Strength +- type: pyaml.magnet.cfm_magnet + name: SH3E-C27 + mapping: + - [B0, SH3E-C27-H] + - [A0, SH3E-C27-V] + - [A1, SH3E-C27-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh3/c27-e-ch1/current + - srmag/ps-corr-sh3/c27-e-ch2/current + - srmag/ps-corr-sh3/c27-e-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SH1A-C28 + mapping: + - [B0, SH1A-C28-H] + - [A0, SH1A-C28-V] + - [A1, SH1A-C28-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh1/c28-a-ch1/current + - srmag/ps-corr-sh1/c28-a-ch2/current + - srmag/ps-corr-sh1/c28-a-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SD1A-C28 + mapping: + - [B0, SD1A-C28-H] + - [A0, SD1A-C28-V] + - [A1, SD1A-C28-SQ] + - [B2, SD1A-C28-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c28-a/Strength_H + - srmag/m-sd1/c28-a/Strength_V + - srmag/m-sd1/c28-a/Strength_SQ + - srmag/m-sd1/c28-a/Strength +- type: pyaml.magnet.cfm_magnet + name: SF2A-C28 + mapping: + - [B0, SF2A-C28-H] + - [A0, SF2A-C28-V] + - [A1, SF2A-C28-SQ] + - [B2, SF2A-C28-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sf2/c28-a/Strength_H + - srmag/m-sf2/c28-a/Strength_V + - srmag/m-sf2/c28-a/Strength_SQ + - srmag/m-sf2/c28-a/Strength +- type: pyaml.magnet.cfm_magnet + name: SD1B-C28 + mapping: + - [B0, SD1B-C28-H] + - [A0, SD1B-C28-V] + - [A1, SD1B-C28-SQ] + - [B2, SD1B-C28-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c28-b/Strength_H + - srmag/m-sd1/c28-b/Strength_V + - srmag/m-sd1/c28-b/Strength_SQ + - srmag/m-sd1/c28-b/Strength +- type: pyaml.magnet.cfm_magnet + name: SH2B-C28 + mapping: + - [B0, SH2B-C28-H] + - [A0, SH2B-C28-V] + - [A1, SH2B-C28-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh2/c28-b-ch1/current + - srmag/ps-corr-sh2/c28-b-ch2/current + - srmag/ps-corr-sh2/c28-b-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SD1D-C28 + mapping: + - [B0, SD1D-C28-H] + - [A0, SD1D-C28-V] + - [A1, SD1D-C28-SQ] + - [B2, SD1D-C28-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c28-d/Strength_H + - srmag/m-sd1/c28-d/Strength_V + - srmag/m-sd1/c28-d/Strength_SQ + - srmag/m-sd1/c28-d/Strength +- type: pyaml.magnet.cfm_magnet + name: SF2E-C28 + mapping: + - [B0, SF2E-C28-H] + - [A0, SF2E-C28-V] + - [A1, SF2E-C28-SQ] + - [B2, SF2E-C28-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sf2/c28-e/Strength_H + - srmag/m-sf2/c28-e/Strength_V + - srmag/m-sf2/c28-e/Strength_SQ + - srmag/m-sf2/c28-e/Strength +- type: pyaml.magnet.cfm_magnet + name: SD1E-C28 + mapping: + - [B0, SD1E-C28-H] + - [A0, SD1E-C28-V] + - [A1, SD1E-C28-SQ] + - [B2, SD1E-C28-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c28-e/Strength_H + - srmag/m-sd1/c28-e/Strength_V + - srmag/m-sd1/c28-e/Strength_SQ + - srmag/m-sd1/c28-e/Strength +- type: pyaml.magnet.cfm_magnet + name: SH3E-C28 + mapping: + - [B0, SH3E-C28-H] + - [A0, SH3E-C28-V] + - [A1, SH3E-C28-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh3/c28-e-ch1/current + - srmag/ps-corr-sh3/c28-e-ch2/current + - srmag/ps-corr-sh3/c28-e-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SH1A-C29 + mapping: + - [B0, SH1A-C29-H] + - [A0, SH1A-C29-V] + - [A1, SH1A-C29-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh1/c29-a-ch1/current + - srmag/ps-corr-sh1/c29-a-ch2/current + - srmag/ps-corr-sh1/c29-a-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SD1A-C29 + mapping: + - [B0, SD1A-C29-H] + - [A0, SD1A-C29-V] + - [A1, SD1A-C29-SQ] + - [B2, SD1A-C29-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c29-a/Strength_H + - srmag/m-sd1/c29-a/Strength_V + - srmag/m-sd1/c29-a/Strength_SQ + - srmag/m-sd1/c29-a/Strength +- type: pyaml.magnet.cfm_magnet + name: SF2A-C29 + mapping: + - [B0, SF2A-C29-H] + - [A0, SF2A-C29-V] + - [A1, SF2A-C29-SQ] + - [B2, SF2A-C29-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sf2/c29-a/Strength_H + - srmag/m-sf2/c29-a/Strength_V + - srmag/m-sf2/c29-a/Strength_SQ + - srmag/m-sf2/c29-a/Strength +- type: pyaml.magnet.cfm_magnet + name: SD1B-C29 + mapping: + - [B0, SD1B-C29-H] + - [A0, SD1B-C29-V] + - [A1, SD1B-C29-SQ] + - [B2, SD1B-C29-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c29-b/Strength_H + - srmag/m-sd1/c29-b/Strength_V + - srmag/m-sd1/c29-b/Strength_SQ + - srmag/m-sd1/c29-b/Strength +- type: pyaml.magnet.cfm_magnet + name: SH2B-C29 + mapping: + - [B0, SH2B-C29-H] + - [A0, SH2B-C29-V] + - [A1, SH2B-C29-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh2/c29-b-ch1/current + - srmag/ps-corr-sh2/c29-b-ch2/current + - srmag/ps-corr-sh2/c29-b-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SD1D-C29 + mapping: + - [B0, SD1D-C29-H] + - [A0, SD1D-C29-V] + - [A1, SD1D-C29-SQ] + - [B2, SD1D-C29-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c29-d/Strength_H + - srmag/m-sd1/c29-d/Strength_V + - srmag/m-sd1/c29-d/Strength_SQ + - srmag/m-sd1/c29-d/Strength +- type: pyaml.magnet.cfm_magnet + name: SF2E-C29 + mapping: + - [B0, SF2E-C29-H] + - [A0, SF2E-C29-V] + - [A1, SF2E-C29-SQ] + - [B2, SF2E-C29-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sf2/c29-e/Strength_H + - srmag/m-sf2/c29-e/Strength_V + - srmag/m-sf2/c29-e/Strength_SQ + - srmag/m-sf2/c29-e/Strength +- type: pyaml.magnet.cfm_magnet + name: SD1E-C29 + mapping: + - [B0, SD1E-C29-H] + - [A0, SD1E-C29-V] + - [A1, SD1E-C29-SQ] + - [B2, SD1E-C29-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c29-e/Strength_H + - srmag/m-sd1/c29-e/Strength_V + - srmag/m-sd1/c29-e/Strength_SQ + - srmag/m-sd1/c29-e/Strength +- type: pyaml.magnet.cfm_magnet + name: SH3E-C29 + mapping: + - [B0, SH3E-C29-H] + - [A0, SH3E-C29-V] + - [A1, SH3E-C29-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh3/c29-e-ch1/current + - srmag/ps-corr-sh3/c29-e-ch2/current + - srmag/ps-corr-sh3/c29-e-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SH1A-C30 + mapping: + - [B0, SH1A-C30-H] + - [A0, SH1A-C30-V] + - [A1, SH1A-C30-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh1/c30-a-ch1/current + - srmag/ps-corr-sh1/c30-a-ch2/current + - srmag/ps-corr-sh1/c30-a-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SD1A-C30 + mapping: + - [B0, SD1A-C30-H] + - [A0, SD1A-C30-V] + - [A1, SD1A-C30-SQ] + - [B2, SD1A-C30-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c30-a/Strength_H + - srmag/m-sd1/c30-a/Strength_V + - srmag/m-sd1/c30-a/Strength_SQ + - srmag/m-sd1/c30-a/Strength +- type: pyaml.magnet.cfm_magnet + name: SF2A-C30 + mapping: + - [B0, SF2A-C30-H] + - [A0, SF2A-C30-V] + - [A1, SF2A-C30-SQ] + - [B2, SF2A-C30-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sf2/c30-a/Strength_H + - srmag/m-sf2/c30-a/Strength_V + - srmag/m-sf2/c30-a/Strength_SQ + - srmag/m-sf2/c30-a/Strength +- type: pyaml.magnet.cfm_magnet + name: SD1B-C30 + mapping: + - [B0, SD1B-C30-H] + - [A0, SD1B-C30-V] + - [A1, SD1B-C30-SQ] + - [B2, SD1B-C30-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c30-b/Strength_H + - srmag/m-sd1/c30-b/Strength_V + - srmag/m-sd1/c30-b/Strength_SQ + - srmag/m-sd1/c30-b/Strength +- type: pyaml.magnet.cfm_magnet + name: SH2B-C30 + mapping: + - [B0, SH2B-C30-H] + - [A0, SH2B-C30-V] + - [A1, SH2B-C30-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh2/c30-b-ch1/current + - srmag/ps-corr-sh2/c30-b-ch2/current + - srmag/ps-corr-sh2/c30-b-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SD1D-C30 + mapping: + - [B0, SD1D-C30-H] + - [A0, SD1D-C30-V] + - [A1, SD1D-C30-SQ] + - [B2, SD1D-C30-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c30-d/Strength_H + - srmag/m-sd1/c30-d/Strength_V + - srmag/m-sd1/c30-d/Strength_SQ + - srmag/m-sd1/c30-d/Strength +- type: pyaml.magnet.cfm_magnet + name: SF2E-C30 + mapping: + - [B0, SF2E-C30-H] + - [A0, SF2E-C30-V] + - [A1, SF2E-C30-SQ] + - [B2, SF2E-C30-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sf2/c30-e/Strength_H + - srmag/m-sf2/c30-e/Strength_V + - srmag/m-sf2/c30-e/Strength_SQ + - srmag/m-sf2/c30-e/Strength +- type: pyaml.magnet.cfm_magnet + name: SD1E-C30 + mapping: + - [B0, SD1E-C30-H] + - [A0, SD1E-C30-V] + - [A1, SD1E-C30-SQ] + - [B2, SD1E-C30-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c30-e/Strength_H + - srmag/m-sd1/c30-e/Strength_V + - srmag/m-sd1/c30-e/Strength_SQ + - srmag/m-sd1/c30-e/Strength +- type: pyaml.magnet.cfm_magnet + name: SH3E-C30 + mapping: + - [B0, SH3E-C30-H] + - [A0, SH3E-C30-V] + - [A1, SH3E-C30-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh3/c30-e-ch1/current + - srmag/ps-corr-sh3/c30-e-ch2/current + - srmag/ps-corr-sh3/c30-e-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SH1A-C31 + mapping: + - [B0, SH1A-C31-H] + - [A0, SH1A-C31-V] + - [A1, SH1A-C31-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh1/c31-a-ch1/current + - srmag/ps-corr-sh1/c31-a-ch2/current + - srmag/ps-corr-sh1/c31-a-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SD1A-C31 + mapping: + - [B0, SD1A-C31-H] + - [A0, SD1A-C31-V] + - [A1, SD1A-C31-SQ] + - [B2, SD1A-C31-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c31-a/Strength_H + - srmag/m-sd1/c31-a/Strength_V + - srmag/m-sd1/c31-a/Strength_SQ + - srmag/m-sd1/c31-a/Strength +- type: pyaml.magnet.cfm_magnet + name: SF2A-C31 + mapping: + - [B0, SF2A-C31-H] + - [A0, SF2A-C31-V] + - [A1, SF2A-C31-SQ] + - [B2, SF2A-C31-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sf2/c31-a/Strength_H + - srmag/m-sf2/c31-a/Strength_V + - srmag/m-sf2/c31-a/Strength_SQ + - srmag/m-sf2/c31-a/Strength +- type: pyaml.magnet.cfm_magnet + name: SD1B-C31 + mapping: + - [B0, SD1B-C31-H] + - [A0, SD1B-C31-V] + - [A1, SD1B-C31-SQ] + - [B2, SD1B-C31-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c31-b/Strength_H + - srmag/m-sd1/c31-b/Strength_V + - srmag/m-sd1/c31-b/Strength_SQ + - srmag/m-sd1/c31-b/Strength +- type: pyaml.magnet.cfm_magnet + name: SH2B-C31 + mapping: + - [B0, SH2B-C31-H] + - [A0, SH2B-C31-V] + - [A1, SH2B-C31-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh2/c31-b-ch1/current + - srmag/ps-corr-sh2/c31-b-ch2/current + - srmag/ps-corr-sh2/c31-b-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SD1D-C31 + mapping: + - [B0, SD1D-C31-H] + - [A0, SD1D-C31-V] + - [A1, SD1D-C31-SQ] + - [B2, SD1D-C31-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c31-d/Strength_H + - srmag/m-sd1/c31-d/Strength_V + - srmag/m-sd1/c31-d/Strength_SQ + - srmag/m-sd1/c31-d/Strength +- type: pyaml.magnet.cfm_magnet + name: SF2E-C31 + mapping: + - [B0, SF2E-C31-H] + - [A0, SF2E-C31-V] + - [A1, SF2E-C31-SQ] + - [B2, SF2E-C31-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sf2/c31-e/Strength_H + - srmag/m-sf2/c31-e/Strength_V + - srmag/m-sf2/c31-e/Strength_SQ + - srmag/m-sf2/c31-e/Strength +- type: pyaml.magnet.cfm_magnet + name: SD1E-C31 + mapping: + - [B0, SD1E-C31-H] + - [A0, SD1E-C31-V] + - [A1, SD1E-C31-SQ] + - [B2, SD1E-C31-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c31-e/Strength_H + - srmag/m-sd1/c31-e/Strength_V + - srmag/m-sd1/c31-e/Strength_SQ + - srmag/m-sd1/c31-e/Strength +- type: pyaml.magnet.cfm_magnet + name: SH3E-C31 + mapping: + - [B0, SH3E-C31-H] + - [A0, SH3E-C31-V] + - [A1, SH3E-C31-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh3/c31-e-ch1/current + - srmag/ps-corr-sh3/c31-e-ch2/current + - srmag/ps-corr-sh3/c31-e-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SH1A-C32 + mapping: + - [B0, SH1A-C32-H] + - [A0, SH1A-C32-V] + - [A1, SH1A-C32-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh1/c32-a-ch1/current + - srmag/ps-corr-sh1/c32-a-ch2/current + - srmag/ps-corr-sh1/c32-a-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SD1A-C32 + mapping: + - [B0, SD1A-C32-H] + - [A0, SD1A-C32-V] + - [A1, SD1A-C32-SQ] + - [B2, SD1A-C32-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c32-a/Strength_H + - srmag/m-sd1/c32-a/Strength_V + - srmag/m-sd1/c32-a/Strength_SQ + - srmag/m-sd1/c32-a/Strength +- type: pyaml.magnet.cfm_magnet + name: SF2A-C32 + mapping: + - [B0, SF2A-C32-H] + - [A0, SF2A-C32-V] + - [A1, SF2A-C32-SQ] + - [B2, SF2A-C32-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sf2/c32-a/Strength_H + - srmag/m-sf2/c32-a/Strength_V + - srmag/m-sf2/c32-a/Strength_SQ + - srmag/m-sf2/c32-a/Strength +- type: pyaml.magnet.cfm_magnet + name: SD1B-C32 + mapping: + - [B0, SD1B-C32-H] + - [A0, SD1B-C32-V] + - [A1, SD1B-C32-SQ] + - [B2, SD1B-C32-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c32-b/Strength_H + - srmag/m-sd1/c32-b/Strength_V + - srmag/m-sd1/c32-b/Strength_SQ + - srmag/m-sd1/c32-b/Strength +- type: pyaml.magnet.cfm_magnet + name: SH2B-C32 + mapping: + - [B0, SH2B-C32-H] + - [A0, SH2B-C32-V] + - [A1, SH2B-C32-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh2/c32-b-ch1/current + - srmag/ps-corr-sh2/c32-b-ch2/current + - srmag/ps-corr-sh2/c32-b-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SD1D-C32 + mapping: + - [B0, SD1D-C32-H] + - [A0, SD1D-C32-V] + - [A1, SD1D-C32-SQ] + - [B2, SD1D-C32-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c32-d/Strength_H + - srmag/m-sd1/c32-d/Strength_V + - srmag/m-sd1/c32-d/Strength_SQ + - srmag/m-sd1/c32-d/Strength +- type: pyaml.magnet.cfm_magnet + name: SF2E-C32 + mapping: + - [B0, SF2E-C32-H] + - [A0, SF2E-C32-V] + - [A1, SF2E-C32-SQ] + - [B2, SF2E-C32-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sf2/c32-e/Strength_H + - srmag/m-sf2/c32-e/Strength_V + - srmag/m-sf2/c32-e/Strength_SQ + - srmag/m-sf2/c32-e/Strength +- type: pyaml.magnet.cfm_magnet + name: SD1E-C32 + mapping: + - [B0, SD1E-C32-H] + - [A0, SD1E-C32-V] + - [A1, SD1E-C32-SQ] + - [B2, SD1E-C32-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c32-e/Strength_H + - srmag/m-sd1/c32-e/Strength_V + - srmag/m-sd1/c32-e/Strength_SQ + - srmag/m-sd1/c32-e/Strength +- type: pyaml.magnet.cfm_magnet + name: SH3E-C32 + mapping: + - [B0, SH3E-C32-H] + - [A0, SH3E-C32-V] + - [A1, SH3E-C32-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh3/c32-e-ch1/current + - srmag/ps-corr-sh3/c32-e-ch2/current + - srmag/ps-corr-sh3/c32-e-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SH1A-C01 + mapping: + - [B0, SH1A-C01-H] + - [A0, SH1A-C01-V] + - [A1, SH1A-C01-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh1/c01-a-ch1/current + - srmag/ps-corr-sh1/c01-a-ch2/current + - srmag/ps-corr-sh1/c01-a-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SD1A-C01 + mapping: + - [B0, SD1A-C01-H] + - [A0, SD1A-C01-V] + - [A1, SD1A-C01-SQ] + - [B2, SD1A-C01-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c01-a/Strength_H + - srmag/m-sd1/c01-a/Strength_V + - srmag/m-sd1/c01-a/Strength_SQ + - srmag/m-sd1/c01-a/Strength +- type: pyaml.magnet.cfm_magnet + name: SF2A-C01 + mapping: + - [B0, SF2A-C01-H] + - [A0, SF2A-C01-V] + - [A1, SF2A-C01-SQ] + - [B2, SF2A-C01-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sf2/c01-a/Strength_H + - srmag/m-sf2/c01-a/Strength_V + - srmag/m-sf2/c01-a/Strength_SQ + - srmag/m-sf2/c01-a/Strength +- type: pyaml.magnet.cfm_magnet + name: SD1B-C01 + mapping: + - [B0, SD1B-C01-H] + - [A0, SD1B-C01-V] + - [A1, SD1B-C01-SQ] + - [B2, SD1B-C01-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c01-b/Strength_H + - srmag/m-sd1/c01-b/Strength_V + - srmag/m-sd1/c01-b/Strength_SQ + - srmag/m-sd1/c01-b/Strength +- type: pyaml.magnet.cfm_magnet + name: SH2B-C01 + mapping: + - [B0, SH2B-C01-H] + - [A0, SH2B-C01-V] + - [A1, SH2B-C01-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh2/c01-b-ch1/current + - srmag/ps-corr-sh2/c01-b-ch2/current + - srmag/ps-corr-sh2/c01-b-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SD1D-C01 + mapping: + - [B0, SD1D-C01-H] + - [A0, SD1D-C01-V] + - [A1, SD1D-C01-SQ] + - [B2, SD1D-C01-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c01-d/Strength_H + - srmag/m-sd1/c01-d/Strength_V + - srmag/m-sd1/c01-d/Strength_SQ + - srmag/m-sd1/c01-d/Strength +- type: pyaml.magnet.cfm_magnet + name: SF2E-C01 + mapping: + - [B0, SF2E-C01-H] + - [A0, SF2E-C01-V] + - [A1, SF2E-C01-SQ] + - [B2, SF2E-C01-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sf2/c01-e/Strength_H + - srmag/m-sf2/c01-e/Strength_V + - srmag/m-sf2/c01-e/Strength_SQ + - srmag/m-sf2/c01-e/Strength +- type: pyaml.magnet.cfm_magnet + name: SD1E-C01 + mapping: + - [B0, SD1E-C01-H] + - [A0, SD1E-C01-V] + - [A1, SD1E-C01-SQ] + - [B2, SD1E-C01-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c01-e/Strength_H + - srmag/m-sd1/c01-e/Strength_V + - srmag/m-sd1/c01-e/Strength_SQ + - srmag/m-sd1/c01-e/Strength +- type: pyaml.magnet.cfm_magnet + name: SH3E-C01 + mapping: + - [B0, SH3E-C01-H] + - [A0, SH3E-C01-V] + - [A1, SH3E-C01-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh3/c01-e-ch1/current + - srmag/ps-corr-sh3/c01-e-ch2/current + - srmag/ps-corr-sh3/c01-e-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SH1A-C02 + mapping: + - [B0, SH1A-C02-H] + - [A0, SH1A-C02-V] + - [A1, SH1A-C02-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh1/c02-a-ch1/current + - srmag/ps-corr-sh1/c02-a-ch2/current + - srmag/ps-corr-sh1/c02-a-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SD1A-C02 + mapping: + - [B0, SD1A-C02-H] + - [A0, SD1A-C02-V] + - [A1, SD1A-C02-SQ] + - [B2, SD1A-C02-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c02-a/Strength_H + - srmag/m-sd1/c02-a/Strength_V + - srmag/m-sd1/c02-a/Strength_SQ + - srmag/m-sd1/c02-a/Strength +- type: pyaml.magnet.cfm_magnet + name: SF2A-C02 + mapping: + - [B0, SF2A-C02-H] + - [A0, SF2A-C02-V] + - [A1, SF2A-C02-SQ] + - [B2, SF2A-C02-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sf2/c02-a/Strength_H + - srmag/m-sf2/c02-a/Strength_V + - srmag/m-sf2/c02-a/Strength_SQ + - srmag/m-sf2/c02-a/Strength +- type: pyaml.magnet.cfm_magnet + name: SD1B-C02 + mapping: + - [B0, SD1B-C02-H] + - [A0, SD1B-C02-V] + - [A1, SD1B-C02-SQ] + - [B2, SD1B-C02-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c02-b/Strength_H + - srmag/m-sd1/c02-b/Strength_V + - srmag/m-sd1/c02-b/Strength_SQ + - srmag/m-sd1/c02-b/Strength +- type: pyaml.magnet.cfm_magnet + name: SH2B-C02 + mapping: + - [B0, SH2B-C02-H] + - [A0, SH2B-C02-V] + - [A1, SH2B-C02-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh2/c02-b-ch1/current + - srmag/ps-corr-sh2/c02-b-ch2/current + - srmag/ps-corr-sh2/c02-b-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SD1D-C02 + mapping: + - [B0, SD1D-C02-H] + - [A0, SD1D-C02-V] + - [A1, SD1D-C02-SQ] + - [B2, SD1D-C02-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c02-d/Strength_H + - srmag/m-sd1/c02-d/Strength_V + - srmag/m-sd1/c02-d/Strength_SQ + - srmag/m-sd1/c02-d/Strength +- type: pyaml.magnet.cfm_magnet + name: SF2E-C02 + mapping: + - [B0, SF2E-C02-H] + - [A0, SF2E-C02-V] + - [A1, SF2E-C02-SQ] + - [B2, SF2E-C02-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sf2/c02-e/Strength_H + - srmag/m-sf2/c02-e/Strength_V + - srmag/m-sf2/c02-e/Strength_SQ + - srmag/m-sf2/c02-e/Strength +- type: pyaml.magnet.cfm_magnet + name: SD1E-C02 + mapping: + - [B0, SD1E-C02-H] + - [A0, SD1E-C02-V] + - [A1, SD1E-C02-SQ] + - [B2, SD1E-C02-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c02-e/Strength_H + - srmag/m-sd1/c02-e/Strength_V + - srmag/m-sd1/c02-e/Strength_SQ + - srmag/m-sd1/c02-e/Strength +- type: pyaml.magnet.cfm_magnet + name: SH3E-C02 + mapping: + - [B0, SH3E-C02-H] + - [A0, SH3E-C02-V] + - [A1, SH3E-C02-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh3/c02-e-ch1/current + - srmag/ps-corr-sh3/c02-e-ch2/current + - srmag/ps-corr-sh3/c02-e-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SH1A-C03 + mapping: + - [B0, SH1A-C03-H] + - [A0, SH1A-C03-V] + - [A1, SH1A-C03-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH1_SH3_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh1/c03-a-ch1/current + - srmag/ps-corr-sh1/c03-a-ch2/current + - srmag/ps-corr-sh1/c03-a-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SI1A-C03 + mapping: + - [B0, SI1A-C03-H] + - [A0, SI1A-C03-V] + - [A1, SI1A-C03-SQ] + - [B2, SI1A-C03-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c03-a/Strength_H + - srmag/m-sd1/c03-a/Strength_V + - srmag/m-sd1/c03-a/Strength_SQ + - srmag/m-sd1/c03-a/Strength +- type: pyaml.magnet.cfm_magnet + name: SI2A-C03 + mapping: + - [B0, SI2A-C03-H] + - [A0, SI2A-C03-V] + - [A1, SI2A-C03-SQ] + - [B2, SI2A-C03-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sf2/c03-a/Strength_H + - srmag/m-sf2/c03-a/Strength_V + - srmag/m-sf2/c03-a/Strength_SQ + - srmag/m-sf2/c03-a/Strength +- type: pyaml.magnet.cfm_magnet + name: SI1B-C03 + mapping: + - [B0, SI1B-C03-H] + - [A0, SI1B-C03-V] + - [A1, SI1B-C03-SQ] + - [B2, SI1B-C03-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c03-b/Strength_H + - srmag/m-sd1/c03-b/Strength_V + - srmag/m-sd1/c03-b/Strength_SQ + - srmag/m-sd1/c03-b/Strength +- type: pyaml.magnet.cfm_magnet + name: SH2B-C03 + mapping: + - [B0, SH2B-C03-H] + - [A0, SH2B-C03-V] + - [A1, SH2B-C03-SQ] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1] + units: [rad,rad,m-1] + hardware_units: ["A","A","A"] + pseudo_factors: [1.0,-1.0,-1.0] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SH2_sq_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SH_matrix.csv + powerconverters: + - srmag/ps-corr-sh2/c03-b-ch1/current + - srmag/ps-corr-sh2/c03-b-ch2/current + - srmag/ps-corr-sh2/c03-b-ch3/current +- type: pyaml.magnet.cfm_magnet + name: SI1D-C03 + mapping: + - [B0, SI1D-C03-H] + - [A0, SI1D-C03-V] + - [A1, SI1D-C03-SQ] + - [B2, SI1D-C03-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c03-d/Strength_H + - srmag/m-sd1/c03-d/Strength_V + - srmag/m-sd1/c03-d/Strength_SQ + - srmag/m-sd1/c03-d/Strength +- type: pyaml.magnet.cfm_magnet + name: SI2E-C03 + mapping: + - [B0, SI2E-C03-H] + - [A0, SI2E-C03-V] + - [A1, SI2E-C03-SQ] + - [B2, SI2E-C03-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sf2/c03-e/Strength_H + - srmag/m-sf2/c03-e/Strength_V + - srmag/m-sf2/c03-e/Strength_SQ + - srmag/m-sf2/c03-e/Strength +- type: pyaml.magnet.cfm_magnet + name: SI1E-C03 + mapping: + - [B0, SI1E-C03-H] + - [A0, SI1E-C03-V] + - [A1, SI1E-C03-SQ] + - [B2, SI1E-C03-S] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B0,A0,A1,B2] + units: [rad,rad,m-1,m-2] + physics: + - srmag/m-sd1/c03-e/Strength_H + - srmag/m-sd1/c03-e/Strength_V + - srmag/m-sd1/c03-e/Strength_SQ + - srmag/m-sd1/c03-e/Strength +- type: pyaml.magnet.cfm_magnet + name: SH3E-C03 + mapping: + - [B0, SH3E-C03-H] + - [A0, SH3E-C03-V] + - [A1, SH3E-C03-SQ] + - [B2, SH3E-C03-S] + model: + type: pyaml.magnet.linear_cfm_model + multipoles: [B0,A0,A1,B2] + pseudo_factors: [1.0,-1.0,-1.0,-1.0] + units: [rad,rad,m-1,m-2] + hardware_units: ["A","A","A","A","A"] + curves: + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SHI_h_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SHI_v_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SHI_sq_strength.csv + - type: pyaml.magnet.csvcurve + file: sr/magnet_models/SHI_sext_strength.csv + matrix: + type: pyaml.magnet.csvmatrix + file: sr/magnet_models/SHI_matrix.csv + powerconverters: + - srmag/ps-corr-sh3/c03-e-ch1/current + - srmag/ps-corr-sh3/c03-e-ch2/current + - srmag/ps-corr-sh3/c03-e-ch3/current + - srmag/ps-corr-sh3/c03-e-ch5/current + - srmag/ps-corr-sh3/c03-e-ch6/current +- type: pyaml.bpm.bpm + name: BPM_C04-01 + x_pos: srdiag/bpm/c04-01/SA_HPosition + y_pos: srdiag/bpm/c04-01/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C04-02 + x_pos: srdiag/bpm/c04-02/SA_HPosition + y_pos: srdiag/bpm/c04-02/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C04-03 + x_pos: srdiag/bpm/c04-03/SA_HPosition + y_pos: srdiag/bpm/c04-03/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C04-04 + x_pos: srdiag/bpm/c04-04/SA_HPosition + y_pos: srdiag/bpm/c04-04/SA_VPosition + x_offset: srdiag/bpm/c04-04/HOffset + y_offset: srdiag/bpm/c04-04/VOffset +- type: pyaml.bpm.bpm + name: BPM_C04-05 + x_pos: srdiag/bpm/c04-05/SA_HPosition + y_pos: srdiag/bpm/c04-05/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C04-06 + x_pos: srdiag/bpm/c04-06/SA_HPosition + y_pos: srdiag/bpm/c04-06/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C04-07 + x_pos: srdiag/bpm/c04-07/SA_HPosition + y_pos: srdiag/bpm/c04-07/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C04-08 + x_pos: srdiag/bpm/c04-08/SA_HPosition + y_pos: srdiag/bpm/c04-08/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C04-09 + x_pos: srdiag/bpm/c04-09/SA_HPosition + y_pos: srdiag/bpm/c04-09/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C04-10 + x_pos: srdiag/bpm/c04-10/SA_HPosition + y_pos: srdiag/bpm/c04-10/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C05-01 + x_pos: srdiag/bpm/c05-01/SA_HPosition + y_pos: srdiag/bpm/c05-01/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C05-02 + x_pos: srdiag/bpm/c05-02/SA_HPosition + y_pos: srdiag/bpm/c05-02/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C05-03 + x_pos: srdiag/bpm/c05-03/SA_HPosition + y_pos: srdiag/bpm/c05-03/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C05-04 + x_pos: srdiag/bpm/c05-04/SA_HPosition + y_pos: srdiag/bpm/c05-04/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C05-05 + x_pos: srdiag/bpm/c05-05/SA_HPosition + y_pos: srdiag/bpm/c05-05/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C05-06 + x_pos: srdiag/bpm/c05-06/SA_HPosition + y_pos: srdiag/bpm/c05-06/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C05-07 + x_pos: srdiag/bpm/c05-07/SA_HPosition + y_pos: srdiag/bpm/c05-07/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C05-08 + x_pos: srdiag/bpm/c05-08/SA_HPosition + y_pos: srdiag/bpm/c05-08/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C05-09 + x_pos: srdiag/bpm/c05-09/SA_HPosition + y_pos: srdiag/bpm/c05-09/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C05-10 + x_pos: srdiag/bpm/c05-10/SA_HPosition + y_pos: srdiag/bpm/c05-10/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C06-01 + x_pos: srdiag/bpm/c06-01/SA_HPosition + y_pos: srdiag/bpm/c06-01/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C06-02 + x_pos: srdiag/bpm/c06-02/SA_HPosition + y_pos: srdiag/bpm/c06-02/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C06-03 + x_pos: srdiag/bpm/c06-03/SA_HPosition + y_pos: srdiag/bpm/c06-03/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C06-04 + x_pos: srdiag/bpm/c06-04/SA_HPosition + y_pos: srdiag/bpm/c06-04/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C06-05 + x_pos: srdiag/bpm/c06-05/SA_HPosition + y_pos: srdiag/bpm/c06-05/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C06-06 + x_pos: srdiag/bpm/c06-06/SA_HPosition + y_pos: srdiag/bpm/c06-06/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C06-07 + x_pos: srdiag/bpm/c06-07/SA_HPosition + y_pos: srdiag/bpm/c06-07/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C06-08 + x_pos: srdiag/bpm/c06-08/SA_HPosition + y_pos: srdiag/bpm/c06-08/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C06-09 + x_pos: srdiag/bpm/c06-09/SA_HPosition + y_pos: srdiag/bpm/c06-09/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C06-10 + x_pos: srdiag/bpm/c06-10/SA_HPosition + y_pos: srdiag/bpm/c06-10/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C07-01 + x_pos: srdiag/bpm/c07-01/SA_HPosition + y_pos: srdiag/bpm/c07-01/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C07-02 + x_pos: srdiag/bpm/c07-02/SA_HPosition + y_pos: srdiag/bpm/c07-02/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C07-03 + x_pos: srdiag/bpm/c07-03/SA_HPosition + y_pos: srdiag/bpm/c07-03/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C07-04 + x_pos: srdiag/bpm/c07-04/SA_HPosition + y_pos: srdiag/bpm/c07-04/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C07-05 + x_pos: srdiag/bpm/c07-05/SA_HPosition + y_pos: srdiag/bpm/c07-05/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C07-06 + x_pos: srdiag/bpm/c07-06/SA_HPosition + y_pos: srdiag/bpm/c07-06/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C07-07 + x_pos: srdiag/bpm/c07-07/SA_HPosition + y_pos: srdiag/bpm/c07-07/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C07-08 + x_pos: srdiag/bpm/c07-08/SA_HPosition + y_pos: srdiag/bpm/c07-08/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C07-09 + x_pos: srdiag/bpm/c07-09/SA_HPosition + y_pos: srdiag/bpm/c07-09/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C07-10 + x_pos: srdiag/bpm/c07-10/SA_HPosition + y_pos: srdiag/bpm/c07-10/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C08-01 + x_pos: srdiag/bpm/c08-01/SA_HPosition + y_pos: srdiag/bpm/c08-01/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C08-02 + x_pos: srdiag/bpm/c08-02/SA_HPosition + y_pos: srdiag/bpm/c08-02/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C08-03 + x_pos: srdiag/bpm/c08-03/SA_HPosition + y_pos: srdiag/bpm/c08-03/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C08-04 + x_pos: srdiag/bpm/c08-04/SA_HPosition + y_pos: srdiag/bpm/c08-04/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C08-05 + x_pos: srdiag/bpm/c08-05/SA_HPosition + y_pos: srdiag/bpm/c08-05/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C08-06 + x_pos: srdiag/bpm/c08-06/SA_HPosition + y_pos: srdiag/bpm/c08-06/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C08-07 + x_pos: srdiag/bpm/c08-07/SA_HPosition + y_pos: srdiag/bpm/c08-07/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C08-08 + x_pos: srdiag/bpm/c08-08/SA_HPosition + y_pos: srdiag/bpm/c08-08/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C08-09 + x_pos: srdiag/bpm/c08-09/SA_HPosition + y_pos: srdiag/bpm/c08-09/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C08-10 + x_pos: srdiag/bpm/c08-10/SA_HPosition + y_pos: srdiag/bpm/c08-10/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C09-01 + x_pos: srdiag/bpm/c09-01/SA_HPosition + y_pos: srdiag/bpm/c09-01/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C09-02 + x_pos: srdiag/bpm/c09-02/SA_HPosition + y_pos: srdiag/bpm/c09-02/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C09-03 + x_pos: srdiag/bpm/c09-03/SA_HPosition + y_pos: srdiag/bpm/c09-03/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C09-04 + x_pos: srdiag/bpm/c09-04/SA_HPosition + y_pos: srdiag/bpm/c09-04/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C09-05 + x_pos: srdiag/bpm/c09-05/SA_HPosition + y_pos: srdiag/bpm/c09-05/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C09-06 + x_pos: srdiag/bpm/c09-06/SA_HPosition + y_pos: srdiag/bpm/c09-06/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C09-07 + x_pos: 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srdiag/bpm/c30-05/SA_HPosition + y_pos: srdiag/bpm/c30-05/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C30-06 + x_pos: srdiag/bpm/c30-06/SA_HPosition + y_pos: srdiag/bpm/c30-06/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C30-07 + x_pos: srdiag/bpm/c30-07/SA_HPosition + y_pos: srdiag/bpm/c30-07/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C30-08 + x_pos: srdiag/bpm/c30-08/SA_HPosition + y_pos: srdiag/bpm/c30-08/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C30-09 + x_pos: srdiag/bpm/c30-09/SA_HPosition + y_pos: srdiag/bpm/c30-09/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C30-10 + x_pos: srdiag/bpm/c30-10/SA_HPosition + y_pos: srdiag/bpm/c30-10/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C31-01 + x_pos: srdiag/bpm/c31-01/SA_HPosition + y_pos: srdiag/bpm/c31-01/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C31-02 + x_pos: srdiag/bpm/c31-02/SA_HPosition + y_pos: srdiag/bpm/c31-02/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C31-03 + x_pos: srdiag/bpm/c31-03/SA_HPosition + y_pos: srdiag/bpm/c31-03/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C31-04 + x_pos: srdiag/bpm/c31-04/SA_HPosition + y_pos: srdiag/bpm/c31-04/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C31-05 + x_pos: srdiag/bpm/c31-05/SA_HPosition + y_pos: srdiag/bpm/c31-05/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C31-06 + x_pos: srdiag/bpm/c31-06/SA_HPosition + y_pos: srdiag/bpm/c31-06/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C31-07 + x_pos: srdiag/bpm/c31-07/SA_HPosition + y_pos: srdiag/bpm/c31-07/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C31-08 + x_pos: srdiag/bpm/c31-08/SA_HPosition + y_pos: srdiag/bpm/c31-08/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C31-09 + x_pos: srdiag/bpm/c31-09/SA_HPosition + y_pos: srdiag/bpm/c31-09/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C31-10 + x_pos: srdiag/bpm/c31-10/SA_HPosition + y_pos: srdiag/bpm/c31-10/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C32-01 + x_pos: srdiag/bpm/c32-01/SA_HPosition + y_pos: srdiag/bpm/c32-01/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C32-02 + x_pos: srdiag/bpm/c32-02/SA_HPosition + y_pos: srdiag/bpm/c32-02/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C32-03 + x_pos: srdiag/bpm/c32-03/SA_HPosition + y_pos: srdiag/bpm/c32-03/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C32-04 + x_pos: srdiag/bpm/c32-04/SA_HPosition + y_pos: srdiag/bpm/c32-04/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C32-05 + x_pos: srdiag/bpm/c32-05/SA_HPosition + y_pos: srdiag/bpm/c32-05/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C32-06 + x_pos: srdiag/bpm/c32-06/SA_HPosition + y_pos: srdiag/bpm/c32-06/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C32-07 + x_pos: srdiag/bpm/c32-07/SA_HPosition + y_pos: srdiag/bpm/c32-07/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C32-08 + x_pos: srdiag/bpm/c32-08/SA_HPosition + y_pos: srdiag/bpm/c32-08/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C32-09 + x_pos: srdiag/bpm/c32-09/SA_HPosition + y_pos: srdiag/bpm/c32-09/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C32-10 + x_pos: srdiag/bpm/c32-10/SA_HPosition + y_pos: srdiag/bpm/c32-10/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C01-01 + x_pos: srdiag/bpm/c01-01/SA_HPosition + y_pos: srdiag/bpm/c01-01/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C01-02 + x_pos: srdiag/bpm/c01-02/SA_HPosition + y_pos: srdiag/bpm/c01-02/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C01-03 + x_pos: srdiag/bpm/c01-03/SA_HPosition + y_pos: srdiag/bpm/c01-03/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C01-04 + x_pos: srdiag/bpm/c01-04/SA_HPosition + y_pos: srdiag/bpm/c01-04/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C01-05 + x_pos: srdiag/bpm/c01-05/SA_HPosition + y_pos: srdiag/bpm/c01-05/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C01-06 + x_pos: srdiag/bpm/c01-06/SA_HPosition + y_pos: srdiag/bpm/c01-06/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C01-07 + x_pos: srdiag/bpm/c01-07/SA_HPosition + y_pos: srdiag/bpm/c01-07/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C01-08 + x_pos: srdiag/bpm/c01-08/SA_HPosition + y_pos: srdiag/bpm/c01-08/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C01-09 + x_pos: srdiag/bpm/c01-09/SA_HPosition + y_pos: srdiag/bpm/c01-09/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C01-10 + x_pos: srdiag/bpm/c01-10/SA_HPosition + y_pos: srdiag/bpm/c01-10/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C02-01 + x_pos: srdiag/bpm/c02-01/SA_HPosition + y_pos: srdiag/bpm/c02-01/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C02-02 + x_pos: srdiag/bpm/c02-02/SA_HPosition + y_pos: srdiag/bpm/c02-02/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C02-03 + x_pos: srdiag/bpm/c02-03/SA_HPosition + y_pos: srdiag/bpm/c02-03/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C02-04 + x_pos: srdiag/bpm/c02-04/SA_HPosition + y_pos: srdiag/bpm/c02-04/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C02-05 + x_pos: srdiag/bpm/c02-05/SA_HPosition + y_pos: srdiag/bpm/c02-05/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C02-06 + x_pos: srdiag/bpm/c02-06/SA_HPosition + y_pos: srdiag/bpm/c02-06/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C02-07 + x_pos: srdiag/bpm/c02-07/SA_HPosition + y_pos: srdiag/bpm/c02-07/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C02-08 + x_pos: srdiag/bpm/c02-08/SA_HPosition + y_pos: srdiag/bpm/c02-08/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C02-09 + x_pos: srdiag/bpm/c02-09/SA_HPosition + y_pos: srdiag/bpm/c02-09/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C02-10 + x_pos: srdiag/bpm/c02-10/SA_HPosition + y_pos: srdiag/bpm/c02-10/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C03-01 + x_pos: srdiag/bpm/c03-01/SA_HPosition + y_pos: srdiag/bpm/c03-01/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C03-02 + x_pos: srdiag/bpm/c03-02/SA_HPosition + y_pos: srdiag/bpm/c03-02/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C03-03 + x_pos: srdiag/bpm/c03-03/SA_HPosition + y_pos: srdiag/bpm/c03-03/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C03-04 + x_pos: srdiag/bpm/c03-04/SA_HPosition + y_pos: srdiag/bpm/c03-04/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C03-05 + x_pos: srdiag/bpm/c03-05/SA_HPosition + y_pos: srdiag/bpm/c03-05/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C03-06 + x_pos: srdiag/bpm/c03-06/SA_HPosition + y_pos: srdiag/bpm/c03-06/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C03-07 + x_pos: srdiag/bpm/c03-07/SA_HPosition + y_pos: srdiag/bpm/c03-07/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C03-08 + x_pos: srdiag/bpm/c03-08/SA_HPosition + y_pos: srdiag/bpm/c03-08/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C03-09 + x_pos: srdiag/bpm/c03-09/SA_HPosition + y_pos: srdiag/bpm/c03-09/SA_VPosition +- type: pyaml.bpm.bpm + name: BPM_C03-10 + x_pos: srdiag/bpm/c03-10/SA_HPosition + y_pos: srdiag/bpm/c03-10/SA_VPosition +- type: pyaml.magnet.quadrupole + name: QF1E-C04 + description: "QF1E-C04 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.00054 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c04-e/current +- type: pyaml.magnet.quadrupole + name: QF1A-C05 + description: "QF1A-C05 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.996841 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c05-a/current +- type: pyaml.magnet.quadrupole + name: QF1E-C05 + description: "QF1E-C05 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.00191 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c05-e/current +- type: pyaml.magnet.quadrupole + name: QF1A-C06 + description: "QF1A-C06 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.0003 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c06-a/current +- type: pyaml.magnet.quadrupole + name: QF1E-C06 + description: "QF1E-C06 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.997615 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c06-e/current +- type: pyaml.magnet.quadrupole + name: QF1A-C07 + description: "QF1A-C07 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.998152 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c07-a/current +- type: pyaml.magnet.quadrupole + name: QF1E-C07 + description: "QF1E-C07 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.00262 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c07-e/current +- type: pyaml.magnet.quadrupole + name: QF1A-C08 + description: "QF1A-C08 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.00319 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c08-a/current +- type: pyaml.magnet.quadrupole + name: QF1E-C08 + description: "QF1E-C08 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.996180929 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c08-e/current +- type: pyaml.magnet.quadrupole + name: QF1A-C09 + description: "QF1A-C09 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.00206 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c09-a/current +- type: pyaml.magnet.quadrupole + name: QF1E-C09 + description: "QF1E-C09 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.999285 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c09-e/current +- type: pyaml.magnet.quadrupole + name: QF1A-C10 + description: "QF1A-C10 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.00232 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c10-a/current +- type: pyaml.magnet.quadrupole + name: QF1E-C10 + description: "QF1E-C10 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.998212 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c10-e/current +- type: pyaml.magnet.quadrupole + name: QF1A-C11 + description: "QF1A-C11 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.999225 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c11-a/current +- type: pyaml.magnet.quadrupole + name: QF1E-C11 + description: "QF1E-C11 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.998033 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c11-e/current +- type: pyaml.magnet.quadrupole + name: QF1A-C12 + description: "QF1A-C12 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.998748 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c12-a/current +- type: pyaml.magnet.quadrupole + name: QF1E-C12 + description: "QF1E-C12 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.0023 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c12-e/current +- type: pyaml.magnet.quadrupole + name: QF1A-C13 + description: "QF1A-C13 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.00337 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c13-a/current +- type: pyaml.magnet.quadrupole + name: QF1E-C13 + description: "QF1E-C13 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.00403 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c13-e/current +- type: pyaml.magnet.quadrupole + name: QF1A-C14 + description: "QF1A-C14 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.00182 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c14-a/current +- type: pyaml.magnet.quadrupole + name: QF1E-C14 + description: "QF1E-C14 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.998303 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c14-e/current +- type: pyaml.magnet.quadrupole + name: QF1A-C15 + description: "QF1A-C15 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.998748 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c15-a/current +- type: pyaml.magnet.quadrupole + name: QF1E-C15 + description: "QF1E-C15 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.994098 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c15-e/current +- type: pyaml.magnet.quadrupole + name: QF1A-C16 + description: "QF1A-C16 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.00232 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c16-a/current +- type: pyaml.magnet.quadrupole + name: QF1E-C16 + description: "QF1E-C16 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.99884 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c16-e/current +- type: pyaml.magnet.quadrupole + name: QF1A-C17 + description: "QF1A-C17 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.0079 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c17-a/current +- type: pyaml.magnet.quadrupole + name: QF1E-C17 + description: "QF1E-C17 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.999523 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c17-e/current +- type: pyaml.magnet.quadrupole + name: QF1A-C18 + description: "QF1A-C18 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c18-a/current +- type: pyaml.magnet.quadrupole + name: QF1E-C18 + description: "QF1E-C18 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.999854 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c18-e/current +- type: pyaml.magnet.quadrupole + name: QF1A-C19 + description: "QF1A-C19 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.99845 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c19-a/current +- type: pyaml.magnet.quadrupole + name: QF1E-C19 + description: "QF1E-C19 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c19-e/current +- type: pyaml.magnet.quadrupole + name: QF1A-C20 + description: "QF1A-C20 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.00095 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c20-a/current +- type: pyaml.magnet.quadrupole + name: QF1E-C20 + description: "QF1E-C20 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.996753 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c20-e/current +- type: pyaml.magnet.quadrupole + name: QF1A-C21 + description: "QF1A-C21 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.00334 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c21-a/current +- type: pyaml.magnet.quadrupole + name: QF1E-C21 + description: "QF1E-C21 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.997707 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c21-e/current +- type: pyaml.magnet.quadrupole + name: QF1A-C22 + description: "QF1A-C22 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.00152 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c22-a/current +- type: pyaml.magnet.quadrupole + name: QF1E-C22 + description: "QF1E-C22 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.998124 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c22-e/current +- type: pyaml.magnet.quadrupole + name: QF1A-C23 + description: "QF1A-C23 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.996662 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c23-a/current +- type: pyaml.magnet.quadrupole + name: QF1E-C23 + description: "QF1E-C23 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.0017 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c23-e/current +- type: pyaml.magnet.quadrupole + name: QF1A-C24 + description: "QF1A-C24 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.999642 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c24-a/current +- type: pyaml.magnet.quadrupole + name: QF1E-C24 + description: "QF1E-C24 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.00042 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c24-e/current +- type: pyaml.magnet.quadrupole + name: QF1A-C25 + description: "QF1A-C25 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.00471 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c25-a/current +- type: pyaml.magnet.quadrupole + name: QF1E-C25 + description: "QF1E-C25 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.00393 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c25-e/current +- type: pyaml.magnet.quadrupole + name: QF1A-C26 + description: "QF1A-C26 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.992906 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c26-a/current +- type: pyaml.magnet.quadrupole + name: QF1E-C26 + description: "QF1E-C26 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.00268 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c26-e/current +- type: pyaml.magnet.quadrupole + name: QF1A-C27 + description: "QF1A-C27 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.00248 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c27-a/current +- type: pyaml.magnet.quadrupole + name: QF1E-C27 + description: "QF1E-C27 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.00203 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c27-e/current +- type: pyaml.magnet.quadrupole + name: QF1A-C28 + description: "QF1A-C28 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.998030791 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c28-a/current +- type: pyaml.magnet.quadrupole + name: QF1E-C28 + description: "QF1E-C28 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.00232 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c28-e/current +- type: pyaml.magnet.quadrupole + name: QF1A-C29 + description: "QF1A-C29 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.995052 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c29-a/current +- type: pyaml.magnet.quadrupole + name: QF1E-C29 + description: "QF1E-C29 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.00155 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c29-e/current +- type: pyaml.magnet.quadrupole + name: QF1A-C30 + description: "QF1A-C30 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.998271 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c30-a/current +- type: pyaml.magnet.quadrupole + name: QF1E-C30 + description: "QF1E-C30 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.999702 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c30-e/current +- type: pyaml.magnet.quadrupole + name: QF1A-C31 + description: "QF1A-C31 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.998005 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c31-a/current +- type: pyaml.magnet.quadrupole + name: QF1E-C31 + description: "QF1E-C31 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.999463 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c31-e/current +- type: pyaml.magnet.quadrupole + name: QF1A-C32 + description: "QF1A-C32 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.997794 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c32-a/current +- type: pyaml.magnet.quadrupole + name: QF1E-C32 + description: "QF1E-C32 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.00203 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c32-e/current +- type: pyaml.magnet.quadrupole + name: QF1A-C01 + description: "QF1A-C01 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.00504 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c01-a/current +- type: pyaml.magnet.quadrupole + name: QF1E-C01 + description: "QF1E-C01 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.998212 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c01-e/current +- type: pyaml.magnet.quadrupole + name: QF1A-C02 + description: "QF1A-C02 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.0037 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c02-a/current +- type: pyaml.magnet.quadrupole + name: QF1E-C02 + description: "QF1E-C02 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.00093 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c02-e/current +- type: pyaml.magnet.quadrupole + name: QF1A-C03 + description: "QF1A-C03 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.0025 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c03-a/current +- type: pyaml.magnet.quadrupole + name: QD2E-C04 + description: "QD2E-C04 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.999305341 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c04-e/current +- type: pyaml.magnet.quadrupole + name: QD2A-C05 + description: "QD2A-C05 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.997452918 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c05-a/current +- type: pyaml.magnet.quadrupole + name: QD2E-C05 + description: "QD2E-C05 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.997993208 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c05-e/current +- type: pyaml.magnet.quadrupole + name: QD2A-C06 + description: "QD2A-C06 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.006031322 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c06-a/current +- type: pyaml.magnet.quadrupole + name: QD2E-C06 + description: "QD2E-C06 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.998547233 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c06-e/current +- type: pyaml.magnet.quadrupole + name: QD2A-C07 + description: "QD2A-C07 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.002327856 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c07-a/current +- type: pyaml.magnet.quadrupole + name: QD2E-C07 + description: "QD2E-C07 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.000154369 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c07-e/current +- type: pyaml.magnet.quadrupole + name: QD2A-C08 + description: "QD2A-C08 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.009580478 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c08-a/current +- type: pyaml.magnet.quadrupole + name: QD2E-C08 + description: "QD2E-C08 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.00447669 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c08-e/current +- type: pyaml.magnet.quadrupole + name: QD2A-C09 + description: "QD2A-C09 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.0015563 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c09-a/current +- type: pyaml.magnet.quadrupole + name: QD2E-C09 + description: "QD2E-C09 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.997221365 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c09-e/current +- type: pyaml.magnet.quadrupole + name: QD2A-C10 + description: "QD2A-C10 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.005954167 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c10-a/current +- type: pyaml.magnet.quadrupole + name: QD2E-C10 + description: "QD2E-C10 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.006725723 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c10-e/current +- type: pyaml.magnet.quadrupole + name: QD2A-C11 + description: "QD2A-C11 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.994535144 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c11-a/current +- type: pyaml.magnet.quadrupole + name: QD2E-C11 + description: "QD2E-C11 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.999550256 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c11-e/current +- type: pyaml.magnet.quadrupole + name: QD2A-C12 + description: "QD2A-C12 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.001479145 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c12-a/current +- type: pyaml.magnet.quadrupole + name: QD2E-C12 + description: "QD2E-C12 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.000321811 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c12-e/current +- type: pyaml.magnet.quadrupole + name: QD2A-C13 + description: "QD2A-C13 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.006715036 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c13-a/current +- type: pyaml.magnet.quadrupole + name: QD2E-C13 + description: "QD2E-C13 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.0036395 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c13-e/current +- type: pyaml.magnet.quadrupole + name: QD2A-C14 + description: "QD2A-C14 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.997684471 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c14-a/current +- type: pyaml.magnet.quadrupole + name: QD2E-C14 + description: "QD2E-C14 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.000385922 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c14-e/current +- type: pyaml.magnet.quadrupole + name: QD2A-C15 + description: "QD2A-C15 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.999010167 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c15-a/current +- type: pyaml.magnet.quadrupole + name: QD2E-C15 + description: "QD2E-C15 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.998392922 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c15-e/current +- type: pyaml.magnet.quadrupole + name: QD2A-C16 + description: "QD2A-C16 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.999318789 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c16-a/current +- type: pyaml.magnet.quadrupole + name: QD2E-C16 + description: "QD2E-C16 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.996926967 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c16-e/current +- type: pyaml.magnet.quadrupole + name: QD2A-C17 + description: "QD2A-C17 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.000849027 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c17-a/current +- type: pyaml.magnet.quadrupole + name: QD2E-C17 + description: "QD2E-C17 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.003392444 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c17-e/current +- type: pyaml.magnet.quadrupole + name: QD2A-C18 + description: "QD2A-C18 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.001312133 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c18-a/current +- type: pyaml.magnet.quadrupole + name: QD2E-C18 + description: "QD2E-C18 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.005402902 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c18-e/current +- type: pyaml.magnet.quadrupole + name: QD2A-C19 + description: "QD2A-C19 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.995846789 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c19-a/current +- type: pyaml.magnet.quadrupole + name: QD2E-C19 + description: "QD2E-C19 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.005877011 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c19-e/current +- type: pyaml.magnet.quadrupole + name: QD2A-C20 + description: "QD2A-C20 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.001016211 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c20-a/current +- type: pyaml.magnet.quadrupole + name: QD2E-C20 + description: "QD2E-C20 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.999010167 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c20-e/current +- type: pyaml.magnet.quadrupole + name: QD2A-C21 + description: "QD2A-C21 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.007265811 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c21-a/current +- type: pyaml.magnet.quadrupole + name: QD2E-C21 + description: "QD2E-C21 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.998238611 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c21-e/current +- type: pyaml.magnet.quadrupole + name: QD2A-C22 + description: "QD2A-C22 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.998161456 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c22-a/current +- type: pyaml.magnet.quadrupole + name: QD2E-C22 + description: "QD2E-C22 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.004642522 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c22-e/current +- type: pyaml.magnet.quadrupole + name: QD2A-C23 + description: "QD2A-C23 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.001479145 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c23-a/current +- type: pyaml.magnet.quadrupole + name: QD2E-C23 + description: "QD2E-C23 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.001942078 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c23-e/current +- type: pyaml.magnet.quadrupole + name: QD2A-C24 + description: "QD2A-C24 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.999087322 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c24-a/current +- type: pyaml.magnet.quadrupole + name: QD2E-C24 + description: "QD2E-C24 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.998547233 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c24-e/current +- type: pyaml.magnet.quadrupole + name: QD2A-C25 + description: "QD2A-C25 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.001698055 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c25-a/current +- type: pyaml.magnet.quadrupole + name: QD2E-C25 + description: "QD2E-C25 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.999704567 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c25-e/current +- type: pyaml.magnet.quadrupole + name: QD2A-C26 + description: "QD2A-C26 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.999164478 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c26-a/current +- type: pyaml.magnet.quadrupole + name: QD2E-C26 + description: "QD2E-C26 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.000694659 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c26-e/current +- type: pyaml.magnet.quadrupole + name: QD2A-C27 + description: "QD2A-C27 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.99945971 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c27-a/current +- type: pyaml.magnet.quadrupole + name: QD2E-C27 + description: "QD2E-C27 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.999922816 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c27-e/current +- type: pyaml.magnet.quadrupole + name: QD2A-C28 + description: "QD2A-C28 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.999922816 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c28-a/current +- type: pyaml.magnet.quadrupole + name: QD2E-C28 + description: "QD2E-C28 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.997838839 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c28-e/current +- type: pyaml.magnet.quadrupole + name: QD2A-C29 + description: "QD2A-C29 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.003318926 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c29-a/current +- type: pyaml.magnet.quadrupole + name: QD2E-C29 + description: "QD2E-C29 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.004179589 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c29-e/current +- type: pyaml.magnet.quadrupole + name: QD2A-C30 + description: "QD2A-C30 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.999010167 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c30-a/current +- type: pyaml.magnet.quadrupole + name: QD2E-C30 + description: "QD2E-C30 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.9987787 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c30-e/current +- type: pyaml.magnet.quadrupole + name: QD2A-C31 + description: "QD2A-C31 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.004411056 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c31-a/current +- type: pyaml.magnet.quadrupole + name: QD2E-C31 + description: "QD2E-C31 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.0029451 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c31-e/current +- type: pyaml.magnet.quadrupole + name: QD2A-C32 + description: "QD2A-C32 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.009426167 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c32-a/current +- type: pyaml.magnet.quadrupole + name: QD2E-C32 + description: "QD2E-C32 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.0050283 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c32-e/current +- type: pyaml.magnet.quadrupole + name: QD2A-C01 + description: "QD2A-C01 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.998533498 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c01-a/current +- type: pyaml.magnet.quadrupole + name: QD2E-C01 + description: "QD2E-C01 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.003485189 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c01-e/current +- type: pyaml.magnet.quadrupole + name: QD2A-C02 + description: "QD2A-C02 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.001389318 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c02-a/current +- type: pyaml.magnet.quadrupole + name: QD2E-C02 + description: "QD2E-C02 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.006108478 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c02-e/current +- type: pyaml.magnet.quadrupole + name: QD2A-C03 + description: "QD2A-C03 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.002096389 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c03-a/current diff --git a/examples/use_cases/config/esrf/sr/lattices/ebs.mat b/examples/use_cases/config/esrf/sr/lattices/ebs.mat new file mode 100644 index 000000000..157489629 Binary files /dev/null and b/examples/use_cases/config/esrf/sr/lattices/ebs.mat differ diff --git a/examples/use_cases/config/esrf/sr/magnet_models/QD2_strength.csv b/examples/use_cases/config/esrf/sr/magnet_models/QD2_strength.csv new file mode 100644 index 000000000..f61fae5e1 --- /dev/null +++ b/examples/use_cases/config/esrf/sr/magnet_models/QD2_strength.csv @@ -0,0 +1,101 @@ + 0, 0 + 10, -1.5344273 +11.01010101, -1.680715587 +12.02020202, -1.827007776 +13.03030303, -1.973307772 +14.04040404, -2.119619478 +15.05050505, -2.265946797 +16.06060606, -2.412291425 +17.07070707, -2.558647463 +18.08080808, -2.705007376 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b/examples/use_cases/config/esrf/sr/magnet_models/SH1_SH3_sq_strength.csv new file mode 100644 index 000000000..0372cffb1 --- /dev/null +++ b/examples/use_cases/config/esrf/sr/magnet_models/SH1_SH3_sq_strength.csv @@ -0,0 +1,17 @@ +-4.2667,-0.53024685 +-3.7333,-0.49480939 +-3.2,-0.45147696 +-2.6667,-0.39314961 +-2.1333,-0.31870389 +-1.6,-0.24073587 +-1.0667,-0.16134213 +-0.53333,-0.081016541 +0.0,0.0 +0.53333,0.081016541 +1.0667,0.16134213 +1.6,0.24073587 +2.1333,0.31870389 +2.6667,0.39314961 +3.2,0.45147696 +3.7333,0.49480939 +4.2667,0.53024685 diff --git a/examples/use_cases/config/esrf/sr/magnet_models/SH1_SH3_v_strength.csv b/examples/use_cases/config/esrf/sr/magnet_models/SH1_SH3_v_strength.csv new file mode 100644 index 000000000..c29ae483d --- /dev/null +++ b/examples/use_cases/config/esrf/sr/magnet_models/SH1_SH3_v_strength.csv @@ -0,0 +1,19 @@ +-4.8,-0.011256173 +-4.2667,-0.010400214 +-3.7333,-0.009291842 +-3.2,-0.008060268 +-2.6667,-0.006750694 +-2.1333,-0.005414052 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b/examples/use_cases/config/esrf/sr/magnet_models/SH2_sq_strength.csv new file mode 100644 index 000000000..5a162df13 --- /dev/null +++ b/examples/use_cases/config/esrf/sr/magnet_models/SH2_sq_strength.csv @@ -0,0 +1,17 @@ +-4.2667,-0.523618764 +-3.7333,-0.488624273 +-3.2,-0.445833498 +-2.6667,-0.38823524 +-2.1333,-0.314720091 +-1.6,-0.237726672 +-1.0667,-0.159325353 +-0.53333,-0.080003834 +0.0,0.0 +0.53333,0.080003834 +1.0667,0.159325353 +1.6,0.237726672 +2.1333,0.314720091 +2.6667,0.38823524 +3.2,0.445833498 +3.7333,0.488624273 +4.2667,0.523618764 diff --git a/examples/use_cases/config/esrf/sr/magnet_models/SH2_v_strength.csv b/examples/use_cases/config/esrf/sr/magnet_models/SH2_v_strength.csv new file mode 100644 index 000000000..ee54f295b --- /dev/null +++ b/examples/use_cases/config/esrf/sr/magnet_models/SH2_v_strength.csv @@ -0,0 +1,19 @@ +-4.8,-0.011115471 +-4.2667,-0.010270211 +-3.7333,-0.009175693 +-3.2,-0.007959515 +-2.6667,-0.00666631 +-2.1333,-0.005346376 +-1.6,-0.004016278 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000000000..ca893a254 --- /dev/null +++ b/examples/use_cases/config/esrf/sr/magnet_models/SHI_matrix.csv @@ -0,0 +1,4 @@ +1,-0.0886,0.0493,0.0886,-0.0493 +0,1,-1,1,-1 +0,1,1,1,1 +-0.35,-1.31,1,1.31,-1 diff --git a/examples/use_cases/config/esrf/sr/magnet_models/SHI_sext_strength.csv b/examples/use_cases/config/esrf/sr/magnet_models/SHI_sext_strength.csv new file mode 100644 index 000000000..8bce6bc23 --- /dev/null +++ b/examples/use_cases/config/esrf/sr/magnet_models/SHI_sext_strength.csv @@ -0,0 +1,21 @@ +-10.0,-27.5725 +-9.0,-25.8065 +-8.0,-23.6602 +-7.0,-20.97822704 +-6.0,-17.98133746 +-5.0,-14.98444789 +-4.0,-11.987558 +-3.0,-8.990668 +-2.0,-5.993779154 +-1.0,-2.996889577 +0.0,0.0 +1.0,2.996889577 +2.0,5.993779154 +3.0,8.990668 +4.0,11.987558 +5.0,14.98444789 +6.0,17.98133746 +7.0,20.97822704 +8.0,23.6602 +9.0,25.8065 +10.0,27.5725 diff --git a/examples/use_cases/config/esrf/sr/magnet_models/SHI_sq_strength.csv b/examples/use_cases/config/esrf/sr/magnet_models/SHI_sq_strength.csv new file mode 100644 index 000000000..7370225b3 --- /dev/null +++ b/examples/use_cases/config/esrf/sr/magnet_models/SHI_sq_strength.csv @@ -0,0 +1,19 @@ +-9.59999,-0.53335905 +-8.53333,-0.5026322 +-7.46666,-0.4659577 +-6.39999,-0.41839668 +-5.33333,-0.35644257 +-4.26666,-0.28783524 +-3.19999,-0.21716061 +-2.13333,-0.14531671 +-1.06666,-0.072921909 +0.0,0.0 +1.06666,0.072921909 +2.13333,0.14531671 +3.19999,0.21716061 +4.26666,0.28783524 +5.33333,0.35644257 +6.39999,0.41839668 +7.46666,0.4659577 +8.53333,0.5026322 +9.59999,0.53335905 diff --git a/examples/use_cases/config/esrf/sr/magnet_models/SHI_v_strength.csv b/examples/use_cases/config/esrf/sr/magnet_models/SHI_v_strength.csv new file mode 100644 index 000000000..8d5d2eadf --- /dev/null +++ b/examples/use_cases/config/esrf/sr/magnet_models/SHI_v_strength.csv @@ -0,0 +1,19 @@ +-9.59999,-0.010499059 +-8.53333,-0.0095203075 +-7.46666,-0.0084496508 +-6.39999,-0.0072807183 +-5.33333,-0.0060823154 +-4.26666,-0.0048763485 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+ "QD2E-C18", + "QD2A-C19", + "QD2E-C19", + "QD2A-C20", + "QD2E-C20", + "QD2A-C21", + "QD2E-C21", + "QD2A-C22", + "QD2E-C22", + "QD2A-C23", + "QD2E-C23", + "QD2A-C24", + "QD2E-C24", + "QD2A-C25", + "QD2E-C25", + "QD2A-C26", + "QD2E-C26", + "QD2A-C27", + "QD2E-C27", + "QD2A-C28", + "QD2E-C28", + "QD2A-C29", + "QD2E-C29", + "QD2A-C30", + "QD2E-C30", + "QD2A-C31", + "QD2E-C31", + "QD2A-C32", + "QD2E-C32", + "QD2A-C01", + "QD2E-C01", + "QD2A-C02", + "QD2E-C02", + "QD2A-C03", + "QF1E-C04", + "QF1A-C05", + "QF1E-C05", + "QF1A-C06", + "QF1E-C06", + "QF1A-C07", + "QF1E-C07", + "QF1A-C08", + "QF1E-C08", + "QF1A-C09", + "QF1E-C09", + "QF1A-C10", + "QF1E-C10", + "QF1A-C11", + "QF1E-C11", + "QF1A-C12", + "QF1E-C12", + "QF1A-C13", + "QF1E-C13", + "QF1A-C14", + "QF1E-C14", + "QF1A-C15", + "QF1E-C15", + "QF1A-C16", + "QF1E-C16", + "QF1A-C17", + "QF1E-C17", + "QF1A-C18", + "QF1E-C18", + "QF1A-C19", + "QF1E-C19", + "QF1A-C20", + "QF1E-C20", + "QF1A-C21", + "QF1E-C21", + "QF1A-C22", + "QF1E-C22", + "QF1A-C23", + "QF1E-C23", + "QF1A-C24", + "QF1E-C24", + "QF1A-C25", + "QF1E-C25", + "QF1A-C26", + "QF1E-C26", + "QF1A-C27", + "QF1E-C27", + "QF1A-C28", + "QF1E-C28", + "QF1A-C29", + "QF1E-C29", + "QF1A-C30", + "QF1E-C30", + "QF1A-C31", + "QF1E-C31", + "QF1A-C32", + "QF1E-C32", + "QF1A-C01", + "QF1E-C01", + "QF1A-C02", + "QF1E-C02", + "QF1A-C03" + ], + "observable_names": [ + "BETATRON_TUNE.x", + "BETATRON_TUNE.y" + ] +} diff --git a/examples/SOLEIL_examples/SOLEIL_II_V3631_sym1_V001_database_rf.m b/examples/use_cases/config/soleil_ii/SOLEIL_II_V3631_sym1_V001_database_rf.m similarity index 100% rename from examples/SOLEIL_examples/SOLEIL_II_V3631_sym1_V001_database_rf.m rename to examples/use_cases/config/soleil_ii/SOLEIL_II_V3631_sym1_V001_database_rf.m diff --git a/examples/SOLEIL_examples/arrays.yaml b/examples/use_cases/config/soleil_ii/arrays.yaml similarity index 90% rename from examples/SOLEIL_examples/arrays.yaml rename to examples/use_cases/config/soleil_ii/arrays.yaml index 510d1579c..67c7f3273 100644 --- a/examples/SOLEIL_examples/arrays.yaml +++ b/examples/use_cases/config/soleil_ii/arrays.yaml @@ -1,369 +1,369 @@ - type: pyaml.arrays.magnet name: HCORR - elements: - - SH1_COR_001.hcorrector - - SH2_HCOR_001.hcorrector - - SXF11_HCOR_001.hcorrector - - SXF1_HCOR_001.hcorrector - - SXF13_HCOR_001.hcorrector - - SXF13_HCOR_002.hcorrector - - SXF1_HCOR_002.hcorrector - - SXF12_HCOR_001.hcorrector - - SH6_COR_001.hcorrector - - SH4_COR_001.hcorrector - - SH4_COR_002.hcorrector - - SH6_COR_002.hcorrector - - SXF21_HCOR_001.hcorrector - - SXF2_HCOR_001.hcorrector - - SXF22_HCOR_001.hcorrector - - SH9_COR_001.hcorrector - - SH7_COR_001.hcorrector - - SH7_COR_002.hcorrector - - SH9_COR_002.hcorrector - - SXF31_HCOR_001.hcorrector - - SXF3_HCOR_001.hcorrector - - SXF33_HCOR_001.hcorrector - - SXF33_HCOR_002.hcorrector - - SXF3_HCOR_002.hcorrector - - SXF32_HCOR_001.hcorrector - - SH9_COR_003.hcorrector - - SH7_COR_003.hcorrector - - SH7_COR_004.hcorrector - - SH9_COR_004.hcorrector - - SXF41_HCOR_001.hcorrector - - SXF4_HCOR_001.hcorrector - - SXF42_HCOR_001.hcorrector - - SH12_COR_001.hcorrector - - SH10_COR_001.hcorrector - - SH10_COR_002.hcorrector - - SH12_COR_002.hcorrector - - SXF51_HCOR_001.hcorrector - - SXF5_HCOR_001.hcorrector - - SXF53_HCOR_001.hcorrector - - SXF53_HCOR_002.hcorrector - - SXF5_HCOR_002.hcorrector - - SXF52_HCOR_001.hcorrector - - SH14_HCOR_001.hcorrector - - SH13_COR_001.hcorrector - - SH16_COR_001.hcorrector - - SH16_COR_002.hcorrector - - SH13_COR_002.hcorrector - - SH14_HCOR_002.hcorrector - - SXF52_HCOR_002.hcorrector - - SXF5_HCOR_003.hcorrector - - SXF53_HCOR_003.hcorrector - - SXF53_HCOR_004.hcorrector - - SXF5_HCOR_004.hcorrector - - SXF51_HCOR_002.hcorrector - - SH12_COR_003.hcorrector - - SH10_COR_003.hcorrector - - SH10_COR_004.hcorrector - - SH12_COR_004.hcorrector - - SXF42_HCOR_002.hcorrector - - SXF4_HCOR_002.hcorrector - - SXF41_HCOR_002.hcorrector - - SH9_COR_005.hcorrector - - SH7_COR_005.hcorrector - - SH7_COR_006.hcorrector - - SH9_COR_006.hcorrector - - SXF32_HCOR_002.hcorrector - - SXF3_HCOR_003.hcorrector - - SXF33_HCOR_003.hcorrector - - SXF33_HCOR_004.hcorrector - - SXF3_HCOR_004.hcorrector - - SXF31_HCOR_002.hcorrector - - SH9_COR_007.hcorrector - - SH7_COR_007.hcorrector - - SH7_COR_008.hcorrector - - SH9_COR_008.hcorrector - - SXF22_HCOR_002.hcorrector - - SXF2_HCOR_002.hcorrector - - SXF21_HCOR_002.hcorrector - - SH6_COR_003.hcorrector - - SH4_COR_003.hcorrector - - SH4_COR_004.hcorrector - - SH6_COR_004.hcorrector - - SXF12_HCOR_002.hcorrector - - SXF1_HCOR_003.hcorrector - - SXF13_HCOR_003.hcorrector - - SXF13_HCOR_004.hcorrector - - SXF1_HCOR_004.hcorrector - - SXF11_HCOR_002.hcorrector - - SH2_HCOR_002.hcorrector - - SH1_COR_002.hcorrector - - SH1_COR_003.hcorrector - - SH2_HCOR_003.hcorrector - - SXF11_HCOR_003.hcorrector - - SXF1_HCOR_005.hcorrector - - SXF13_HCOR_005.hcorrector - - SXF13_HCOR_006.hcorrector - - SXF1_HCOR_006.hcorrector - - SXF12_HCOR_003.hcorrector - - SH6_COR_005.hcorrector - - SH4_COR_005.hcorrector - - SH4_COR_006.hcorrector - - SH6_COR_006.hcorrector - - SXF21_HCOR_003.hcorrector - - SXF2_HCOR_003.hcorrector - - SXF22_HCOR_003.hcorrector - - SH9_COR_009.hcorrector - - SH7_COR_009.hcorrector - - SH7_COR_010.hcorrector - - SH9_COR_010.hcorrector - - SXF31_HCOR_003.hcorrector - - SXF3_HCOR_005.hcorrector - - SXF33_HCOR_005.hcorrector - - SXF33_HCOR_006.hcorrector - - SXF3_HCOR_006.hcorrector - - SXF32_HCOR_003.hcorrector - - SH9_COR_011.hcorrector - - SH7_COR_011.hcorrector - - SH7_COR_012.hcorrector - - SH9_COR_012.hcorrector - - SXF41_HCOR_003.hcorrector - - SXF4_HCOR_003.hcorrector - - SXF42_HCOR_003.hcorrector - - SH12_COR_005.hcorrector - - SH10_COR_005.hcorrector - - SH10_COR_006.hcorrector - - SH12_COR_006.hcorrector - - SXF51_HCOR_003.hcorrector - - SXF5_HCOR_005.hcorrector - - SXF53_HCOR_005.hcorrector - - SXF53_HCOR_006.hcorrector - - SXF5_HCOR_006.hcorrector - - SXF52_HCOR_003.hcorrector - - SH14_HCOR_003.hcorrector - - SH13_COR_003.hcorrector - - SH16_COR_003.hcorrector - - SH16_COR_004.hcorrector - - SH13_COR_004.hcorrector - - SH14_HCOR_004.hcorrector - - SXF52_HCOR_004.hcorrector - - SXF5_HCOR_007.hcorrector - - SXF53_HCOR_007.hcorrector - - SXF53_HCOR_008.hcorrector - - SXF5_HCOR_008.hcorrector - - SXF51_HCOR_004.hcorrector - - SH12_COR_007.hcorrector - - SH10_COR_007.hcorrector - - SH10_COR_008.hcorrector - - SH12_COR_008.hcorrector - - SXF42_HCOR_004.hcorrector - - SXF4_HCOR_004.hcorrector - - SXF41_HCOR_004.hcorrector - - SH9_COR_013.hcorrector - - SH7_COR_013.hcorrector - - SH7_COR_014.hcorrector - - SH9_COR_014.hcorrector - - SXF32_HCOR_004.hcorrector - - SXF3_HCOR_007.hcorrector - - SXF33_HCOR_007.hcorrector - - SXF33_HCOR_008.hcorrector - - SXF3_HCOR_008.hcorrector - - SXF31_HCOR_004.hcorrector - - SH9_COR_015.hcorrector - - SH7_COR_015.hcorrector - - SH7_COR_016.hcorrector - - SH9_COR_016.hcorrector - - SXF22_HCOR_004.hcorrector - - SXF2_HCOR_004.hcorrector - - SXF21_HCOR_004.hcorrector - - SH6_COR_007.hcorrector - - SH4_COR_007.hcorrector - - SH4_COR_008.hcorrector - - SH6_COR_008.hcorrector - - SXF12_HCOR_004.hcorrector - - SXF1_HCOR_007.hcorrector - - SXF13_HCOR_007.hcorrector - - SXF13_HCOR_008.hcorrector - - SXF1_HCOR_008.hcorrector - - SXF11_HCOR_004.hcorrector - - SH2_HCOR_004.hcorrector - - SH1_COR_004.hcorrector + elements: &id001 + - SH1_COR_001.hcorrector + - SH2_HCOR_001.hcorrector + - SXF11_HCOR_001.hcorrector + - SXF1_HCOR_001.hcorrector + - SXF13_HCOR_001.hcorrector + - SXF13_HCOR_002.hcorrector + - SXF1_HCOR_002.hcorrector + - SXF12_HCOR_001.hcorrector + - SH6_COR_001.hcorrector + - SH4_COR_001.hcorrector + - SH4_COR_002.hcorrector + - SH6_COR_002.hcorrector + - SXF21_HCOR_001.hcorrector + - SXF2_HCOR_001.hcorrector + - SXF22_HCOR_001.hcorrector + - SH9_COR_001.hcorrector + - SH7_COR_001.hcorrector + - SH7_COR_002.hcorrector + - SH9_COR_002.hcorrector + - SXF31_HCOR_001.hcorrector + - SXF3_HCOR_001.hcorrector + - SXF33_HCOR_001.hcorrector + - SXF33_HCOR_002.hcorrector + - SXF3_HCOR_002.hcorrector + - SXF32_HCOR_001.hcorrector + - SH9_COR_003.hcorrector + - SH7_COR_003.hcorrector + - SH7_COR_004.hcorrector + - SH9_COR_004.hcorrector + - SXF41_HCOR_001.hcorrector + - SXF4_HCOR_001.hcorrector + - SXF42_HCOR_001.hcorrector + - SH12_COR_001.hcorrector + - SH10_COR_001.hcorrector + - SH10_COR_002.hcorrector + - SH12_COR_002.hcorrector + - SXF51_HCOR_001.hcorrector + - SXF5_HCOR_001.hcorrector + - SXF53_HCOR_001.hcorrector + - SXF53_HCOR_002.hcorrector + - SXF5_HCOR_002.hcorrector + - SXF52_HCOR_001.hcorrector + - SH14_HCOR_001.hcorrector + - SH13_COR_001.hcorrector + - SH16_COR_001.hcorrector + - SH16_COR_002.hcorrector + - SH13_COR_002.hcorrector + - SH14_HCOR_002.hcorrector + - SXF52_HCOR_002.hcorrector + - SXF5_HCOR_003.hcorrector + - SXF53_HCOR_003.hcorrector + - SXF53_HCOR_004.hcorrector + - SXF5_HCOR_004.hcorrector + - SXF51_HCOR_002.hcorrector + - SH12_COR_003.hcorrector + - SH10_COR_003.hcorrector + - SH10_COR_004.hcorrector + - SH12_COR_004.hcorrector + - SXF42_HCOR_002.hcorrector + - SXF4_HCOR_002.hcorrector + - SXF41_HCOR_002.hcorrector + - SH9_COR_005.hcorrector + - SH7_COR_005.hcorrector + - SH7_COR_006.hcorrector + - SH9_COR_006.hcorrector + - SXF32_HCOR_002.hcorrector + - SXF3_HCOR_003.hcorrector + - SXF33_HCOR_003.hcorrector + - SXF33_HCOR_004.hcorrector + - SXF3_HCOR_004.hcorrector + - SXF31_HCOR_002.hcorrector + - SH9_COR_007.hcorrector + - SH7_COR_007.hcorrector + - SH7_COR_008.hcorrector + - SH9_COR_008.hcorrector + - SXF22_HCOR_002.hcorrector + - SXF2_HCOR_002.hcorrector + - SXF21_HCOR_002.hcorrector + - SH6_COR_003.hcorrector + - SH4_COR_003.hcorrector + - SH4_COR_004.hcorrector + - SH6_COR_004.hcorrector + - SXF12_HCOR_002.hcorrector + - SXF1_HCOR_003.hcorrector + - SXF13_HCOR_003.hcorrector + - SXF13_HCOR_004.hcorrector + - SXF1_HCOR_004.hcorrector + - SXF11_HCOR_002.hcorrector + - SH2_HCOR_002.hcorrector + - SH1_COR_002.hcorrector + - SH1_COR_003.hcorrector + - SH2_HCOR_003.hcorrector + - SXF11_HCOR_003.hcorrector + - SXF1_HCOR_005.hcorrector + - SXF13_HCOR_005.hcorrector + - SXF13_HCOR_006.hcorrector + - SXF1_HCOR_006.hcorrector + - SXF12_HCOR_003.hcorrector + - SH6_COR_005.hcorrector + - SH4_COR_005.hcorrector + - SH4_COR_006.hcorrector + - SH6_COR_006.hcorrector + - SXF21_HCOR_003.hcorrector + - SXF2_HCOR_003.hcorrector + - SXF22_HCOR_003.hcorrector + - SH9_COR_009.hcorrector + - SH7_COR_009.hcorrector + - SH7_COR_010.hcorrector + - SH9_COR_010.hcorrector + - SXF31_HCOR_003.hcorrector + - SXF3_HCOR_005.hcorrector + - SXF33_HCOR_005.hcorrector + - SXF33_HCOR_006.hcorrector + - SXF3_HCOR_006.hcorrector + - SXF32_HCOR_003.hcorrector + - SH9_COR_011.hcorrector + - SH7_COR_011.hcorrector + - SH7_COR_012.hcorrector + - SH9_COR_012.hcorrector + - SXF41_HCOR_003.hcorrector + - SXF4_HCOR_003.hcorrector + - SXF42_HCOR_003.hcorrector + - SH12_COR_005.hcorrector + - SH10_COR_005.hcorrector + - SH10_COR_006.hcorrector + - SH12_COR_006.hcorrector + - SXF51_HCOR_003.hcorrector + - SXF5_HCOR_005.hcorrector + - SXF53_HCOR_005.hcorrector + - SXF53_HCOR_006.hcorrector + - SXF5_HCOR_006.hcorrector + - SXF52_HCOR_003.hcorrector + - SH14_HCOR_003.hcorrector + - SH13_COR_003.hcorrector + - SH16_COR_003.hcorrector + - SH16_COR_004.hcorrector + - SH13_COR_004.hcorrector + - SH14_HCOR_004.hcorrector + - SXF52_HCOR_004.hcorrector + - SXF5_HCOR_007.hcorrector + - SXF53_HCOR_007.hcorrector + - SXF53_HCOR_008.hcorrector + - SXF5_HCOR_008.hcorrector + - SXF51_HCOR_004.hcorrector + - SH12_COR_007.hcorrector + - SH10_COR_007.hcorrector + - SH10_COR_008.hcorrector + - SH12_COR_008.hcorrector + - SXF42_HCOR_004.hcorrector + - SXF4_HCOR_004.hcorrector + - SXF41_HCOR_004.hcorrector + - SH9_COR_013.hcorrector + - SH7_COR_013.hcorrector + - SH7_COR_014.hcorrector + - SH9_COR_014.hcorrector + - SXF32_HCOR_004.hcorrector + - SXF3_HCOR_007.hcorrector + - SXF33_HCOR_007.hcorrector + - SXF33_HCOR_008.hcorrector + - SXF3_HCOR_008.hcorrector + - SXF31_HCOR_004.hcorrector + - SH9_COR_015.hcorrector + - SH7_COR_015.hcorrector + - SH7_COR_016.hcorrector + - SH9_COR_016.hcorrector + - SXF22_HCOR_004.hcorrector + - SXF2_HCOR_004.hcorrector + - SXF21_HCOR_004.hcorrector + - SH6_COR_007.hcorrector + - SH4_COR_007.hcorrector + - SH4_COR_008.hcorrector + - SH6_COR_008.hcorrector + - SXF12_HCOR_004.hcorrector + - SXF1_HCOR_007.hcorrector + - SXF13_HCOR_007.hcorrector + - SXF13_HCOR_008.hcorrector + - SXF1_HCOR_008.hcorrector + - SXF11_HCOR_004.hcorrector + - SH2_HCOR_004.hcorrector + - SH1_COR_004.hcorrector - type: pyaml.arrays.magnet name: VCORR - elements: - - SH1_COR_001.vcorrector - - SH3_VCOR_001.vcorrector - - SXD11_VCOR_001.vcorrector - - SXD1_VCOR_001.vcorrector - - SXD13_VCOR_001.vcorrector - - SXD1_VCOR_002.vcorrector - - SXD1_VCOR_003.vcorrector - - SXD12_VCOR_001.vcorrector - - SH6_COR_001.vcorrector - - SH4_COR_001.vcorrector - - SH4_COR_002.vcorrector - - SH6_COR_002.vcorrector - - SXD21_VCOR_001.vcorrector - - SXD2_VCOR_001.vcorrector - - SXD22_VCOR_001.vcorrector - - SH9_COR_001.vcorrector - - SH7_COR_001.vcorrector - - SH7_COR_002.vcorrector - - SH9_COR_002.vcorrector - - SXD31_VCOR_001.vcorrector - - SXD3_VCOR_001.vcorrector - - SXD33_VCOR_001.vcorrector - - SXD3_VCOR_002.vcorrector - - SXD3_VCOR_003.vcorrector - - SXD32_VCOR_001.vcorrector - - SH9_COR_003.vcorrector - - SH7_COR_003.vcorrector - - SH7_COR_004.vcorrector - - SH9_COR_004.vcorrector - - SXD41_VCOR_001.vcorrector - - SXD4_VCOR_001.vcorrector - - SXD42_VCOR_001.vcorrector - - SH12_COR_001.vcorrector - - SH10_COR_001.vcorrector - - SH10_COR_002.vcorrector - - SH12_COR_002.vcorrector - - SXD51_VCOR_001.vcorrector - - SXD5_VCOR_001.vcorrector - - SXD53_VCOR_001.vcorrector - - SXD5_VCOR_002.vcorrector - - SXD5_VCOR_003.vcorrector - - SXD52_VCOR_001.vcorrector - - SH15_VCOR_001.vcorrector - - SH13_COR_001.vcorrector - - SH16_COR_001.vcorrector - - SH16_COR_002.vcorrector - - SH13_COR_002.vcorrector - - SH15_VCOR_002.vcorrector - - SXD52_VCOR_002.vcorrector - - SXD5_VCOR_004.vcorrector - - SXD53_VCOR_002.vcorrector - - SXD5_VCOR_005.vcorrector - - SXD5_VCOR_006.vcorrector - - SXD51_VCOR_002.vcorrector - - SH12_COR_003.vcorrector - - SH10_COR_003.vcorrector - - SH10_COR_004.vcorrector - - SH12_COR_004.vcorrector - - SXD42_VCOR_002.vcorrector - - SXD4_VCOR_002.vcorrector - - SXD41_VCOR_002.vcorrector - - SH9_COR_005.vcorrector - - SH7_COR_005.vcorrector - - SH7_COR_006.vcorrector - - SH9_COR_006.vcorrector - - SXD32_VCOR_002.vcorrector - - SXD3_VCOR_004.vcorrector - - SXD33_VCOR_002.vcorrector - - SXD3_VCOR_005.vcorrector - - SXD3_VCOR_006.vcorrector - - SXD31_VCOR_002.vcorrector - - SH9_COR_007.vcorrector - - SH7_COR_007.vcorrector - - SH7_COR_008.vcorrector - - SH9_COR_008.vcorrector - - SXD22_VCOR_002.vcorrector - - SXD2_VCOR_002.vcorrector - - SXD21_VCOR_002.vcorrector - - SH6_COR_003.vcorrector - - SH4_COR_003.vcorrector - - SH4_COR_004.vcorrector - - SH6_COR_004.vcorrector - - SXD12_VCOR_002.vcorrector - - SXD1_VCOR_004.vcorrector - - SXD13_VCOR_002.vcorrector - - SXD1_VCOR_005.vcorrector - - SXD1_VCOR_006.vcorrector - - SXD11_VCOR_002.vcorrector - - SH3_VCOR_002.vcorrector - - SH1_COR_002.vcorrector - - SH1_COR_003.vcorrector - - SH3_VCOR_003.vcorrector - - SXD11_VCOR_003.vcorrector - - SXD1_VCOR_007.vcorrector - - SXD13_VCOR_003.vcorrector - - SXD1_VCOR_008.vcorrector - - SXD1_VCOR_009.vcorrector - - SXD12_VCOR_003.vcorrector - - SH6_COR_005.vcorrector - - SH4_COR_005.vcorrector - - SH4_COR_006.vcorrector - - SH6_COR_006.vcorrector - - SXD21_VCOR_003.vcorrector - - SXD2_VCOR_003.vcorrector - - SXD22_VCOR_003.vcorrector - - SH9_COR_009.vcorrector - - SH7_COR_009.vcorrector - - SH7_COR_010.vcorrector - - SH9_COR_010.vcorrector - - SXD31_VCOR_003.vcorrector - - SXD3_VCOR_007.vcorrector - - SXD33_VCOR_003.vcorrector - - SXD3_VCOR_008.vcorrector - - SXD3_VCOR_009.vcorrector - - SXD32_VCOR_003.vcorrector - - SH9_COR_011.vcorrector - - SH7_COR_011.vcorrector - - SH7_COR_012.vcorrector - - SH9_COR_012.vcorrector - - SXD41_VCOR_003.vcorrector - - SXD4_VCOR_003.vcorrector - - SXD42_VCOR_003.vcorrector - - SH12_COR_005.vcorrector - - SH10_COR_005.vcorrector - - SH10_COR_006.vcorrector - - SH12_COR_006.vcorrector - - SXD51_VCOR_003.vcorrector - - SXD5_VCOR_007.vcorrector - - SXD53_VCOR_003.vcorrector - - SXD5_VCOR_008.vcorrector - - SXD5_VCOR_009.vcorrector - - SXD52_VCOR_003.vcorrector - - SH15_VCOR_003.vcorrector - - SH13_COR_003.vcorrector - - SH16_COR_003.vcorrector - - SH16_COR_004.vcorrector - - SH13_COR_004.vcorrector - - SH15_VCOR_004.vcorrector - - SXD52_VCOR_004.vcorrector - - SXD5_VCOR_010.vcorrector - - SXD53_VCOR_004.vcorrector - - SXD5_VCOR_011.vcorrector - - SXD5_VCOR_012.vcorrector - - SXD51_VCOR_004.vcorrector - - SH12_COR_007.vcorrector - - SH10_COR_007.vcorrector - - SH10_COR_008.vcorrector - - SH12_COR_008.vcorrector - - SXD42_VCOR_004.vcorrector - - SXD4_VCOR_004.vcorrector - - SXD41_VCOR_004.vcorrector - - SH9_COR_013.vcorrector - - SH7_COR_013.vcorrector - - SH7_COR_014.vcorrector - - SH9_COR_014.vcorrector - - SXD32_VCOR_004.vcorrector - - SXD3_VCOR_010.vcorrector - - SXD33_VCOR_004.vcorrector - - SXD3_VCOR_011.vcorrector - - SXD3_VCOR_012.vcorrector - - SXD31_VCOR_004.vcorrector - - SH9_COR_015.vcorrector - - SH7_COR_015.vcorrector - - SH7_COR_016.vcorrector - - SH9_COR_016.vcorrector - - SXD22_VCOR_004.vcorrector - - SXD2_VCOR_004.vcorrector - - SXD21_VCOR_004.vcorrector - - SH6_COR_007.vcorrector - - SH4_COR_007.vcorrector - - SH4_COR_008.vcorrector - - SH6_COR_008.vcorrector - - SXD12_VCOR_004.vcorrector - - SXD1_VCOR_010.vcorrector - - SXD13_VCOR_004.vcorrector - - SXD1_VCOR_011.vcorrector - - SXD1_VCOR_012.vcorrector - - SXD11_VCOR_004.vcorrector - - SH3_VCOR_004.vcorrector - - SH1_COR_004.vcorrector + elements: &id002 + - SH1_COR_001.vcorrector + - SH3_VCOR_001.vcorrector + - SXD11_VCOR_001.vcorrector + - SXD1_VCOR_001.vcorrector + - SXD13_VCOR_001.vcorrector + - SXD1_VCOR_002.vcorrector + - SXD1_VCOR_003.vcorrector + - SXD12_VCOR_001.vcorrector + - SH6_COR_001.vcorrector + - SH4_COR_001.vcorrector + - SH4_COR_002.vcorrector + - SH6_COR_002.vcorrector + - SXD21_VCOR_001.vcorrector + - SXD2_VCOR_001.vcorrector + - SXD22_VCOR_001.vcorrector + - SH9_COR_001.vcorrector + - SH7_COR_001.vcorrector + - SH7_COR_002.vcorrector + - SH9_COR_002.vcorrector + - SXD31_VCOR_001.vcorrector + - SXD3_VCOR_001.vcorrector + - SXD33_VCOR_001.vcorrector + - SXD3_VCOR_002.vcorrector + - SXD3_VCOR_003.vcorrector + - SXD32_VCOR_001.vcorrector + - SH9_COR_003.vcorrector + - SH7_COR_003.vcorrector + - SH7_COR_004.vcorrector + - SH9_COR_004.vcorrector + - SXD41_VCOR_001.vcorrector + - SXD4_VCOR_001.vcorrector + - SXD42_VCOR_001.vcorrector + - SH12_COR_001.vcorrector + - SH10_COR_001.vcorrector + - SH10_COR_002.vcorrector + - SH12_COR_002.vcorrector + - SXD51_VCOR_001.vcorrector + - SXD5_VCOR_001.vcorrector + - SXD53_VCOR_001.vcorrector + - SXD5_VCOR_002.vcorrector + - SXD5_VCOR_003.vcorrector + - SXD52_VCOR_001.vcorrector + - SH15_VCOR_001.vcorrector + - SH13_COR_001.vcorrector + - SH16_COR_001.vcorrector + - SH16_COR_002.vcorrector + - SH13_COR_002.vcorrector + - SH15_VCOR_002.vcorrector + - SXD52_VCOR_002.vcorrector + - SXD5_VCOR_004.vcorrector + - SXD53_VCOR_002.vcorrector + - SXD5_VCOR_005.vcorrector + - SXD5_VCOR_006.vcorrector + - SXD51_VCOR_002.vcorrector + - SH12_COR_003.vcorrector + - SH10_COR_003.vcorrector + - SH10_COR_004.vcorrector + - SH12_COR_004.vcorrector + - SXD42_VCOR_002.vcorrector + - SXD4_VCOR_002.vcorrector + - SXD41_VCOR_002.vcorrector + - SH9_COR_005.vcorrector + - SH7_COR_005.vcorrector + - SH7_COR_006.vcorrector + - SH9_COR_006.vcorrector + - SXD32_VCOR_002.vcorrector + - SXD3_VCOR_004.vcorrector + - SXD33_VCOR_002.vcorrector + - SXD3_VCOR_005.vcorrector + - SXD3_VCOR_006.vcorrector + - SXD31_VCOR_002.vcorrector + - SH9_COR_007.vcorrector + - SH7_COR_007.vcorrector + - SH7_COR_008.vcorrector + - SH9_COR_008.vcorrector + - SXD22_VCOR_002.vcorrector + - SXD2_VCOR_002.vcorrector + - SXD21_VCOR_002.vcorrector + - SH6_COR_003.vcorrector + - SH4_COR_003.vcorrector + - SH4_COR_004.vcorrector + - SH6_COR_004.vcorrector + - SXD12_VCOR_002.vcorrector + - SXD1_VCOR_004.vcorrector + - SXD13_VCOR_002.vcorrector + - SXD1_VCOR_005.vcorrector + - SXD1_VCOR_006.vcorrector + - SXD11_VCOR_002.vcorrector + - SH3_VCOR_002.vcorrector + - SH1_COR_002.vcorrector + - SH1_COR_003.vcorrector + - SH3_VCOR_003.vcorrector + - SXD11_VCOR_003.vcorrector + - SXD1_VCOR_007.vcorrector + - SXD13_VCOR_003.vcorrector + - SXD1_VCOR_008.vcorrector + - SXD1_VCOR_009.vcorrector + - SXD12_VCOR_003.vcorrector + - SH6_COR_005.vcorrector + - SH4_COR_005.vcorrector + - SH4_COR_006.vcorrector + - SH6_COR_006.vcorrector + - SXD21_VCOR_003.vcorrector + - SXD2_VCOR_003.vcorrector + - SXD22_VCOR_003.vcorrector + - SH9_COR_009.vcorrector + - SH7_COR_009.vcorrector + - SH7_COR_010.vcorrector + - SH9_COR_010.vcorrector + - SXD31_VCOR_003.vcorrector + - SXD3_VCOR_007.vcorrector + - SXD33_VCOR_003.vcorrector + - SXD3_VCOR_008.vcorrector + - SXD3_VCOR_009.vcorrector + - SXD32_VCOR_003.vcorrector + - SH9_COR_011.vcorrector + - SH7_COR_011.vcorrector + - SH7_COR_012.vcorrector + - SH9_COR_012.vcorrector + - SXD41_VCOR_003.vcorrector + - SXD4_VCOR_003.vcorrector + - SXD42_VCOR_003.vcorrector + - SH12_COR_005.vcorrector + - SH10_COR_005.vcorrector + - SH10_COR_006.vcorrector + - SH12_COR_006.vcorrector + - SXD51_VCOR_003.vcorrector + - SXD5_VCOR_007.vcorrector + - SXD53_VCOR_003.vcorrector + - SXD5_VCOR_008.vcorrector + - SXD5_VCOR_009.vcorrector + - SXD52_VCOR_003.vcorrector + - SH15_VCOR_003.vcorrector + - SH13_COR_003.vcorrector + - SH16_COR_003.vcorrector + - SH16_COR_004.vcorrector + - SH13_COR_004.vcorrector + - SH15_VCOR_004.vcorrector + - SXD52_VCOR_004.vcorrector + - SXD5_VCOR_010.vcorrector + - SXD53_VCOR_004.vcorrector + - SXD5_VCOR_011.vcorrector + - SXD5_VCOR_012.vcorrector + - SXD51_VCOR_004.vcorrector + - SH12_COR_007.vcorrector + - SH10_COR_007.vcorrector + - SH10_COR_008.vcorrector + - SH12_COR_008.vcorrector + - SXD42_VCOR_004.vcorrector + - SXD4_VCOR_004.vcorrector + - SXD41_VCOR_004.vcorrector + - SH9_COR_013.vcorrector + - SH7_COR_013.vcorrector + - SH7_COR_014.vcorrector + - SH9_COR_014.vcorrector + - SXD32_VCOR_004.vcorrector + - SXD3_VCOR_010.vcorrector + - SXD33_VCOR_004.vcorrector + - SXD3_VCOR_011.vcorrector + - SXD3_VCOR_012.vcorrector + - SXD31_VCOR_004.vcorrector + - SH9_COR_015.vcorrector + - SH7_COR_015.vcorrector + - SH7_COR_016.vcorrector + - SH9_COR_016.vcorrector + - SXD22_VCOR_004.vcorrector + - SXD2_VCOR_004.vcorrector + - SXD21_VCOR_004.vcorrector + - SH6_COR_007.vcorrector + - SH4_COR_007.vcorrector + - SH4_COR_008.vcorrector + - SH6_COR_008.vcorrector + - SXD12_VCOR_004.vcorrector + - SXD1_VCOR_010.vcorrector + - SXD13_VCOR_004.vcorrector + - SXD1_VCOR_011.vcorrector + - SXD1_VCOR_012.vcorrector + - SXD11_VCOR_004.vcorrector + - SH3_VCOR_004.vcorrector + - SH1_COR_004.vcorrector - type: pyaml.arrays.bpm name: BPM elements: @@ -721,7 +721,7 @@ - SH3_VCOR_004.vcorrector - type: pyaml.arrays.magnet name: QCORR - elements: + elements: &id003 - QCORR_001 - QCORR_002 - QCORR_003 @@ -4824,3 +4824,12 @@ - OH1_QCORROCT_164_QT_001.octupole - OH1_QCORROCT_164_QT_001.quadrupole - OH1_QCORROCT_164_QT_001.skewquad +- type: pyaml.arrays.magnet + name: HCorr + elements: *id001 +- type: pyaml.arrays.magnet + name: VCorr + elements: *id002 +- type: pyaml.arrays.magnet + name: QForTune + elements: *id003 diff --git a/examples/use_cases/config/soleil_ii/catalogs.yaml b/examples/use_cases/config/soleil_ii/catalogs.yaml new file mode 100644 index 000000000..696587335 --- /dev/null +++ b/examples/use_cases/config/soleil_ii/catalogs.yaml @@ -0,0 +1,10836 @@ +type: tango.pyaml.static_catalog +entries: +- type: tango.pyaml.static_catalog_entry + key: AN01-SD/DG-EPOS/BPM.02/x_pos + device: + type: tango.pyaml.attribute_read_only + attribute: AN01-SD/DG-EPOS/BPM.02/x_pos + unit: mm +- type: tango.pyaml.static_catalog_entry + key: AN01-SD/DG-EPOS/BPM.02/y_pos + device: + type: tango.pyaml.attribute_read_only + attribute: AN01-SD/DG-EPOS/BPM.02/y_pos + unit: mm +- type: tango.pyaml.static_catalog_entry + key: AN01-AR/DG-EPOS/BPM.03/x_pos + device: + type: tango.pyaml.attribute_read_only + attribute: AN01-AR/DG-EPOS/BPM.03/x_pos + unit: mm +- type: tango.pyaml.static_catalog_entry + key: AN01-AR/DG-EPOS/BPM.03/y_pos + device: + type: tango.pyaml.attribute_read_only + attribute: AN01-AR/DG-EPOS/BPM.03/y_pos + unit: mm +- type: tango.pyaml.static_catalog_entry + key: AN01-AR/DG-EPOS/BPM.04/x_pos + device: + type: tango.pyaml.attribute_read_only + attribute: AN01-AR/DG-EPOS/BPM.04/x_pos + unit: mm +- type: tango.pyaml.static_catalog_entry + key: AN01-AR/DG-EPOS/BPM.04/y_pos + device: + type: tango.pyaml.attribute_read_only + attribute: AN01-AR/DG-EPOS/BPM.04/y_pos + unit: mm +- type: tango.pyaml.static_catalog_entry + key: AN01-AR/DG-EPOS/BPM.05/x_pos + device: + type: tango.pyaml.attribute_read_only + attribute: AN01-AR/DG-EPOS/BPM.05/x_pos + unit: mm +- type: tango.pyaml.static_catalog_entry + key: AN01-AR/DG-EPOS/BPM.05/y_pos + device: + type: tango.pyaml.attribute_read_only + attribute: AN01-AR/DG-EPOS/BPM.05/y_pos + unit: mm +- type: tango.pyaml.static_catalog_entry + key: AN01-AR/DG-EPOS/BPM.06/x_pos + device: + type: tango.pyaml.attribute_read_only + attribute: AN01-AR/DG-EPOS/BPM.06/x_pos + unit: mm +- type: tango.pyaml.static_catalog_entry + key: AN01-AR/DG-EPOS/BPM.06/y_pos + device: + type: tango.pyaml.attribute_read_only + attribute: AN01-AR/DG-EPOS/BPM.06/y_pos + unit: mm +- type: tango.pyaml.static_catalog_entry + key: AN01-AR/DG-EPOS/BPM.07/x_pos + device: + type: tango.pyaml.attribute_read_only + attribute: AN01-AR/DG-EPOS/BPM.07/x_pos + unit: mm +- type: tango.pyaml.static_catalog_entry + key: AN01-AR/DG-EPOS/BPM.07/y_pos + device: + type: tango.pyaml.attribute_read_only + attribute: AN01-AR/DG-EPOS/BPM.07/y_pos + unit: mm +- type: tango.pyaml.static_catalog_entry + key: AN01-AR/DG-EPOS/BPM.08/x_pos + device: + type: tango.pyaml.attribute_read_only + attribute: AN01-AR/DG-EPOS/BPM.08/x_pos + unit: mm +- type: tango.pyaml.static_catalog_entry + key: AN01-AR/DG-EPOS/BPM.08/y_pos + device: + type: tango.pyaml.attribute_read_only + attribute: AN01-AR/DG-EPOS/BPM.08/y_pos + unit: mm +- type: tango.pyaml.static_catalog_entry + key: AN01-AR/DG-EPOS/BPM.09/x_pos + device: + type: tango.pyaml.attribute_read_only + attribute: AN01-AR/DG-EPOS/BPM.09/x_pos + unit: mm +- type: tango.pyaml.static_catalog_entry + key: AN01-AR/DG-EPOS/BPM.09/y_pos + device: + type: tango.pyaml.attribute_read_only + attribute: AN01-AR/DG-EPOS/BPM.09/y_pos + unit: mm +- type: tango.pyaml.static_catalog_entry + key: AN01-AR/DG-EPOS/BPM.10/x_pos + device: + type: tango.pyaml.attribute_read_only + attribute: AN01-AR/DG-EPOS/BPM.10/x_pos + unit: mm +- type: tango.pyaml.static_catalog_entry + key: AN01-AR/DG-EPOS/BPM.10/y_pos + device: + type: tango.pyaml.attribute_read_only + attribute: AN01-AR/DG-EPOS/BPM.10/y_pos + unit: mm +- type: tango.pyaml.static_catalog_entry + key: AN02-SD/DG-EPOS/BPM.01/x_pos + device: + type: tango.pyaml.attribute_read_only + attribute: AN02-SD/DG-EPOS/BPM.01/x_pos + unit: mm +- type: tango.pyaml.static_catalog_entry + key: AN02-SD/DG-EPOS/BPM.01/y_pos + device: + type: tango.pyaml.attribute_read_only + attribute: AN02-SD/DG-EPOS/BPM.01/y_pos + unit: mm +- type: tango.pyaml.static_catalog_entry + key: AN02-SD/DG-EPOS/BPM.02/x_pos + device: + type: tango.pyaml.attribute_read_only + attribute: AN02-SD/DG-EPOS/BPM.02/x_pos + unit: mm +- type: tango.pyaml.static_catalog_entry + key: AN02-SD/DG-EPOS/BPM.02/y_pos + device: + type: tango.pyaml.attribute_read_only + attribute: AN02-SD/DG-EPOS/BPM.02/y_pos + unit: mm +- type: tango.pyaml.static_catalog_entry + key: AN02-AR/DG-EPOS/BPM.03/x_pos + device: + type: tango.pyaml.attribute_read_only + attribute: AN02-AR/DG-EPOS/BPM.03/x_pos + unit: mm +- type: tango.pyaml.static_catalog_entry + key: AN02-AR/DG-EPOS/BPM.03/y_pos + device: + type: tango.pyaml.attribute_read_only + attribute: AN02-AR/DG-EPOS/BPM.03/y_pos + unit: mm +- type: tango.pyaml.static_catalog_entry + key: AN02-AR/DG-EPOS/BPM.04/x_pos + device: + type: tango.pyaml.attribute_read_only + attribute: AN02-AR/DG-EPOS/BPM.04/x_pos + unit: mm +- type: tango.pyaml.static_catalog_entry + key: AN02-AR/DG-EPOS/BPM.04/y_pos + device: + type: tango.pyaml.attribute_read_only + attribute: AN02-AR/DG-EPOS/BPM.04/y_pos + unit: mm +- type: tango.pyaml.static_catalog_entry + key: AN02-AR/DG-EPOS/BPM.05/x_pos + device: + type: tango.pyaml.attribute_read_only + attribute: AN02-AR/DG-EPOS/BPM.05/x_pos + unit: mm +- type: tango.pyaml.static_catalog_entry + key: AN02-AR/DG-EPOS/BPM.05/y_pos + device: + type: tango.pyaml.attribute_read_only + attribute: AN02-AR/DG-EPOS/BPM.05/y_pos + unit: mm +- type: tango.pyaml.static_catalog_entry + key: AN02-AR/DG-EPOS/BPM.06/x_pos + device: + type: tango.pyaml.attribute_read_only + attribute: AN02-AR/DG-EPOS/BPM.06/x_pos + unit: mm +- type: tango.pyaml.static_catalog_entry + key: AN02-AR/DG-EPOS/BPM.06/y_pos + device: + type: tango.pyaml.attribute_read_only + attribute: AN02-AR/DG-EPOS/BPM.06/y_pos + unit: mm +- type: tango.pyaml.static_catalog_entry + key: AN02-AR/DG-EPOS/BPM.07/x_pos + device: + type: tango.pyaml.attribute_read_only + attribute: AN02-AR/DG-EPOS/BPM.07/x_pos + unit: mm +- type: tango.pyaml.static_catalog_entry + key: AN02-AR/DG-EPOS/BPM.07/y_pos + device: + type: tango.pyaml.attribute_read_only + attribute: AN02-AR/DG-EPOS/BPM.07/y_pos + unit: mm +- type: tango.pyaml.static_catalog_entry + key: AN03-SD/DG-EPOS/BPM.01/x_pos + device: + type: tango.pyaml.attribute_read_only + attribute: AN03-SD/DG-EPOS/BPM.01/x_pos + unit: mm +- type: tango.pyaml.static_catalog_entry + key: AN03-SD/DG-EPOS/BPM.01/y_pos + device: + type: tango.pyaml.attribute_read_only + attribute: AN03-SD/DG-EPOS/BPM.01/y_pos + unit: mm +- type: tango.pyaml.static_catalog_entry + key: AN03-SD/DG-EPOS/BPM.02/x_pos + device: + type: tango.pyaml.attribute_read_only + attribute: AN03-SD/DG-EPOS/BPM.02/x_pos + unit: mm +- type: tango.pyaml.static_catalog_entry + key: AN03-SD/DG-EPOS/BPM.02/y_pos + device: + type: tango.pyaml.attribute_read_only + attribute: AN03-SD/DG-EPOS/BPM.02/y_pos + unit: mm +- type: tango.pyaml.static_catalog_entry + key: AN03-AR/DG-EPOS/BPM.03/x_pos + device: + type: tango.pyaml.attribute_read_only + attribute: AN03-AR/DG-EPOS/BPM.03/x_pos + unit: mm +- type: tango.pyaml.static_catalog_entry + key: AN03-AR/DG-EPOS/BPM.03/y_pos + device: + type: tango.pyaml.attribute_read_only + attribute: AN03-AR/DG-EPOS/BPM.03/y_pos + unit: mm +- type: tango.pyaml.static_catalog_entry + key: AN03-AR/DG-EPOS/BPM.04/x_pos + device: + type: tango.pyaml.attribute_read_only + attribute: AN03-AR/DG-EPOS/BPM.04/x_pos + unit: mm +- type: tango.pyaml.static_catalog_entry + key: AN03-AR/DG-EPOS/BPM.04/y_pos + device: + type: tango.pyaml.attribute_read_only + attribute: AN03-AR/DG-EPOS/BPM.04/y_pos + unit: mm +- type: tango.pyaml.static_catalog_entry + key: AN03-AR/DG-EPOS/BPM.05/x_pos + device: + type: tango.pyaml.attribute_read_only + attribute: AN03-AR/DG-EPOS/BPM.05/x_pos + unit: mm +- type: tango.pyaml.static_catalog_entry + key: AN03-AR/DG-EPOS/BPM.05/y_pos + device: + type: tango.pyaml.attribute_read_only + attribute: AN03-AR/DG-EPOS/BPM.05/y_pos + unit: mm +- type: tango.pyaml.static_catalog_entry + key: AN03-AR/DG-EPOS/BPM.06/x_pos + device: + type: tango.pyaml.attribute_read_only + attribute: AN03-AR/DG-EPOS/BPM.06/x_pos + unit: mm +- type: tango.pyaml.static_catalog_entry + key: AN03-AR/DG-EPOS/BPM.06/y_pos + device: + type: tango.pyaml.attribute_read_only + attribute: AN03-AR/DG-EPOS/BPM.06/y_pos + unit: mm +- type: tango.pyaml.static_catalog_entry + key: AN03-AR/DG-EPOS/BPM.07/x_pos + device: + type: tango.pyaml.attribute_read_only + attribute: AN03-AR/DG-EPOS/BPM.07/x_pos + unit: mm +- type: tango.pyaml.static_catalog_entry + key: AN03-AR/DG-EPOS/BPM.07/y_pos + device: + type: tango.pyaml.attribute_read_only + attribute: AN03-AR/DG-EPOS/BPM.07/y_pos + unit: mm +- type: tango.pyaml.static_catalog_entry + key: AN03-AR/DG-EPOS/BPM.08/x_pos + device: + type: tango.pyaml.attribute_read_only + attribute: AN03-AR/DG-EPOS/BPM.08/x_pos + unit: mm +- type: tango.pyaml.static_catalog_entry + key: AN03-AR/DG-EPOS/BPM.08/y_pos + device: + type: tango.pyaml.attribute_read_only + attribute: AN03-AR/DG-EPOS/BPM.08/y_pos + unit: mm +- type: tango.pyaml.static_catalog_entry + key: AN03-AR/DG-EPOS/BPM.09/x_pos + device: + type: tango.pyaml.attribute_read_only + attribute: AN03-AR/DG-EPOS/BPM.09/x_pos + unit: mm +- type: tango.pyaml.static_catalog_entry + key: AN03-AR/DG-EPOS/BPM.09/y_pos + device: + type: tango.pyaml.attribute_read_only + attribute: AN03-AR/DG-EPOS/BPM.09/y_pos + unit: mm +- type: tango.pyaml.static_catalog_entry + key: AN03-AR/DG-EPOS/BPM.10/x_pos + device: + type: tango.pyaml.attribute_read_only + attribute: AN03-AR/DG-EPOS/BPM.10/x_pos + unit: mm +- type: tango.pyaml.static_catalog_entry + key: AN03-AR/DG-EPOS/BPM.10/y_pos + device: + type: tango.pyaml.attribute_read_only + attribute: AN03-AR/DG-EPOS/BPM.10/y_pos + unit: mm +- type: tango.pyaml.static_catalog_entry + key: AN04-SD/DG-EPOS/BPM.01/x_pos + device: + type: tango.pyaml.attribute_read_only + attribute: AN04-SD/DG-EPOS/BPM.01/x_pos + unit: mm +- type: tango.pyaml.static_catalog_entry + key: AN04-SD/DG-EPOS/BPM.01/y_pos + device: + type: tango.pyaml.attribute_read_only + attribute: AN04-SD/DG-EPOS/BPM.01/y_pos + unit: mm +- type: tango.pyaml.static_catalog_entry + key: AN04-SD/DG-EPOS/BPM.02/x_pos + device: + type: tango.pyaml.attribute_read_only + attribute: AN04-SD/DG-EPOS/BPM.02/x_pos + unit: mm +- type: tango.pyaml.static_catalog_entry + key: AN04-SD/DG-EPOS/BPM.02/y_pos + device: + type: tango.pyaml.attribute_read_only + attribute: AN04-SD/DG-EPOS/BPM.02/y_pos + unit: mm +- type: tango.pyaml.static_catalog_entry + key: AN04-AR/DG-EPOS/BPM.03/x_pos + device: + type: tango.pyaml.attribute_read_only + attribute: AN04-AR/DG-EPOS/BPM.03/x_pos + unit: mm +- type: tango.pyaml.static_catalog_entry + key: AN04-AR/DG-EPOS/BPM.03/y_pos + device: + type: tango.pyaml.attribute_read_only + attribute: AN04-AR/DG-EPOS/BPM.03/y_pos + unit: mm +- type: tango.pyaml.static_catalog_entry + key: AN04-AR/DG-EPOS/BPM.04/x_pos + device: + type: tango.pyaml.attribute_read_only + attribute: AN04-AR/DG-EPOS/BPM.04/x_pos + unit: mm +- type: tango.pyaml.static_catalog_entry + key: AN04-AR/DG-EPOS/BPM.04/y_pos + device: + type: tango.pyaml.attribute_read_only + attribute: AN04-AR/DG-EPOS/BPM.04/y_pos + unit: mm +- type: tango.pyaml.static_catalog_entry + key: AN04-AR/DG-EPOS/BPM.05/x_pos + device: + type: tango.pyaml.attribute_read_only + attribute: AN04-AR/DG-EPOS/BPM.05/x_pos + unit: mm +- type: tango.pyaml.static_catalog_entry + key: AN04-AR/DG-EPOS/BPM.05/y_pos + device: + type: tango.pyaml.attribute_read_only + attribute: AN04-AR/DG-EPOS/BPM.05/y_pos + unit: mm +- type: tango.pyaml.static_catalog_entry + key: AN04-AR/DG-EPOS/BPM.06/x_pos + device: + type: tango.pyaml.attribute_read_only + attribute: AN04-AR/DG-EPOS/BPM.06/x_pos + unit: mm +- type: tango.pyaml.static_catalog_entry + key: AN04-AR/DG-EPOS/BPM.06/y_pos + device: + type: tango.pyaml.attribute_read_only + attribute: AN04-AR/DG-EPOS/BPM.06/y_pos + unit: mm +- type: tango.pyaml.static_catalog_entry + key: AN04-AR/DG-EPOS/BPM.07/x_pos + device: + type: tango.pyaml.attribute_read_only + attribute: AN04-AR/DG-EPOS/BPM.07/x_pos + unit: mm +- type: tango.pyaml.static_catalog_entry + key: AN04-AR/DG-EPOS/BPM.07/y_pos + device: + type: tango.pyaml.attribute_read_only + attribute: AN04-AR/DG-EPOS/BPM.07/y_pos + unit: mm +- type: tango.pyaml.static_catalog_entry + key: AN05-SD/DG-EPOS/BPM.01/x_pos + device: + type: tango.pyaml.attribute_read_only + attribute: 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tango.pyaml.static_catalog_entry + key: AN20-AR/EM-COR/OH.04-CQLN.22/strength + device: + type: tango.pyaml.attribute + attribute: AN20-AR/EM-COR/OH.04-CQLN.22/strength + unit: 1/m**2 +- type: tango.pyaml.static_catalog_entry + key: AN20-AR/EM-COR/OH.04-CQLT.08/strength + device: + type: tango.pyaml.attribute + attribute: AN20-AR/EM-COR/OH.04-CQLT.08/strength + unit: 1/m**2 +- type: tango.pyaml.static_catalog_entry + key: AN20-AR/EM-SX/SHF.06/strength + device: + type: tango.pyaml.attribute + attribute: AN20-AR/EM-SX/SHF.06/strength + unit: 1/m**2 +- type: tango.pyaml.static_catalog_entry + key: AN20-AR/EM-COR/SHF.06-CDLH.10/strength + device: + type: tango.pyaml.attribute + attribute: AN20-AR/EM-COR/SHF.06-CDLH.10/strength + unit: '1' +- type: tango.pyaml.static_catalog_entry + key: AN20-AR/EM-COR/SHF.06-CDLV.10/strength + device: + type: tango.pyaml.attribute + attribute: AN20-AR/EM-COR/SHF.06-CDLV.10/strength + unit: '1' diff --git a/examples/use_cases/config/soleil_ii/devices.yaml b/examples/use_cases/config/soleil_ii/devices.yaml new file mode 100644 index 000000000..e75b0954a --- /dev/null +++ b/examples/use_cases/config/soleil_ii/devices.yaml @@ -0,0 +1,8542 @@ +- type: pyaml.bpm.bpm + name: BPM_001 + x_pos: AN01-SD/DG-EPOS/BPM.02/x_pos + y_pos: AN01-SD/DG-EPOS/BPM.02/y_pos +- type: pyaml.magnet.cfm_magnet + name: SH1_COR_001 + mapping: + - [B2, SH1_COR_001.sextupole] + - [B0, SH1_COR_001.hcorrector] + - [A0, SH1_COR_001.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0, A0] + units: [1/m**2, '1', '1'] + physics: + - AN01-AR/EM-SX/SHF.01/strength + - AN01-AR/EM-COR/SHF.01-CDLH.01/strength + - AN01-AR/EM-COR/SHF.01-CDLV.01/strength +- type: pyaml.magnet.cfm_magnet + name: OH1_QCORROCT_1_QT_001 + mapping: + - [B3, OH1_QCORROCT_1_QT_001.octupole] + - [B1, OH1_QCORROCT_1_QT_001.quadrupole] + - [A1, OH1_QCORROCT_1_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN01-AR/EM-OCT/OH.01/strength + - AN01-AR/EM-COR/OH.01-CQLN.01/strength + - AN01-AR/EM-COR/OH.01-CQLT.01/strength +- type: pyaml.magnet.cfm_magnet + name: SH2_HCOR_001 + mapping: + - [B2, SH2_HCOR_001.sextupole] + - [B0, SH2_HCOR_001.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN01-AR/EM-SX/SHD.02/strength + - AN01-AR/EM-COR/SHD.02-CDLH.02/strength +- type: pyaml.magnet.cfm_magnet + name: OH2_QCORROCT_2_001 + mapping: + - [B3, OH2_QCORROCT_2_001.octupole] + - [B1, OH2_QCORROCT_2_001.quadrupole] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1] + units: [1/m**3, 1/m**2] + physics: + - AN01-AR/EM-OCT/OH.02/strength + - AN01-AR/EM-COR/OH.02-CQLN.02/strength +- type: pyaml.bpm.bpm + name: BPM_002 + x_pos: AN01-AR/DG-EPOS/BPM.03/x_pos + y_pos: AN01-AR/DG-EPOS/BPM.03/y_pos +- type: pyaml.magnet.cfm_magnet + name: SH3_VCOR_001 + mapping: + - [B2, SH3_VCOR_001.sextupole] + - [A0, SH3_VCOR_001.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN01-AR/EM-SX/SHD.03/strength + - AN01-AR/EM-COR/SHD.03-CDLV.02/strength +- type: pyaml.magnet.quadrupole + name: QCORR_001 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN01-AR/EM-COR/CQLN.03/strength +- type: pyaml.magnet.sextupole + name: SXD11_001 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN01-AR/EM-SX/SCD.01/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF1_QCORROCT_3_QT_001 + mapping: + - [B3, OCTF1_QCORROCT_3_QT_001.octupole] + - [B1, OCTF1_QCORROCT_3_QT_001.quadrupole] + - [A1, OCTF1_QCORROCT_3_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN01-AR/EM-OCT/OC.01/strength + - AN01-AR/EM-COR/OC.01-CQLN.04/strength + - AN01-AR/EM-COR/OC.01-CQLT.02/strength +- type: pyaml.magnet.cfm_magnet + name: SXF11_HCOR_001 + mapping: + - [B2, SXF11_HCOR_001.sextupole] + - [B0, SXF11_HCOR_001.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN01-AR/EM-SX/SCF.02/strength + - AN01-AR/EM-COR/SCF.02-CDLH.03/strength +- type: pyaml.bpm.bpm + name: BPM_003 + x_pos: AN01-AR/DG-EPOS/BPM.04/x_pos + y_pos: AN01-AR/DG-EPOS/BPM.04/y_pos +- type: pyaml.magnet.cfm_magnet + name: SXD11_VCOR_001 + mapping: + - [B2, SXD11_VCOR_001.sextupole] + - [A0, SXD11_VCOR_001.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN01-AR/EM-SX/SCD.03/strength + - AN01-AR/EM-COR/SCD.03-CDLV.03/strength +- type: pyaml.magnet.quadrupole + name: QCORR_002 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN01-AR/EM-COR/CQLN.05/strength +- type: pyaml.magnet.quadrupole + name: QCORR_003 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN01-AR/EM-COR/CQLN.06/strength +- type: pyaml.magnet.sextupole + name: SXD1_001 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN01-AR/EM-SX/SCD.04/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF1_QCORROCT_4_QT_001 + mapping: + - [B3, OCTF1_QCORROCT_4_QT_001.octupole] + - [B1, OCTF1_QCORROCT_4_QT_001.quadrupole] + - [A1, OCTF1_QCORROCT_4_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN01-AR/EM-OCT/OC.02/strength + - AN01-AR/EM-COR/OC.02-CQLN.07/strength + - AN01-AR/EM-COR/OC.02-CQLT.03/strength +- type: pyaml.magnet.cfm_magnet + name: SXF1_HCOR_001 + mapping: + - [B2, SXF1_HCOR_001.sextupole] + - [B0, SXF1_HCOR_001.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN01-AR/EM-SX/SCF.05/strength + - AN01-AR/EM-COR/SCF.05-CDLH.04/strength +- type: pyaml.bpm.bpm + name: BPM_004 + x_pos: AN01-AR/DG-EPOS/BPM.05/x_pos + y_pos: AN01-AR/DG-EPOS/BPM.05/y_pos +- type: pyaml.magnet.cfm_magnet + name: SXD1_VCOR_001 + mapping: + - [B2, SXD1_VCOR_001.sextupole] + - [A0, SXD1_VCOR_001.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN01-AR/EM-SX/SCD.06/strength + - AN01-AR/EM-COR/SCD.06-CDLV.04/strength +- type: pyaml.magnet.quadrupole + name: QCORR_004 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN01-AR/EM-COR/CQLN.08/strength +- type: pyaml.magnet.quadrupole + name: QCORR_005 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN01-AR/EM-COR/CQLN.09/strength +- type: pyaml.magnet.sextupole + name: SXD1_002 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN01-AR/EM-SX/SCD.07/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF1_QCORROCT_5_QT_001 + mapping: + - [B3, OCTF1_QCORROCT_5_QT_001.octupole] + - [B1, OCTF1_QCORROCT_5_QT_001.quadrupole] + - [A1, OCTF1_QCORROCT_5_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN01-AR/EM-OCT/OC.03/strength + - AN01-AR/EM-COR/OC.03-CQLN.10/strength + - AN01-AR/EM-COR/OC.03-CQLT.04/strength +- type: pyaml.magnet.cfm_magnet + name: SXF13_HCOR_001 + mapping: + - [B2, SXF13_HCOR_001.sextupole] + - [B0, SXF13_HCOR_001.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN01-AR/EM-SX/SCF.08/strength + - AN01-AR/EM-COR/SCF.08-CDLH.05/strength +- type: pyaml.bpm.bpm + name: BPM_005 + x_pos: AN01-AR/DG-EPOS/BPM.06/x_pos + y_pos: AN01-AR/DG-EPOS/BPM.06/y_pos +- type: pyaml.magnet.cfm_magnet + name: SXD13_VCOR_001 + mapping: + - [B2, SXD13_VCOR_001.sextupole] + - [A0, SXD13_VCOR_001.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN01-AR/EM-SX/SCD.09/strength + - AN01-AR/EM-COR/SCD.09-CDLV.05/strength +- type: pyaml.magnet.quadrupole + name: QCORR_006 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN01-AR/EM-COR/CQLN.11/strength +- type: pyaml.magnet.quadrupole + name: QCORR_007 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN01-AR/EM-COR/CQLN.12/strength +- type: pyaml.magnet.sextupole + name: SXD13_001 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN01-AR/EM-SX/SCD.10/strength +- type: pyaml.magnet.cfm_magnet + name: SXF13_HCOR_002 + mapping: + - [B2, SXF13_HCOR_002.sextupole] + - [B0, SXF13_HCOR_002.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN01-AR/EM-SX/SCF.11/strength + - AN01-AR/EM-COR/SCF.11-CDLH.06/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF1_QCORROCT_6_QT_001 + mapping: + - [B3, OCTF1_QCORROCT_6_QT_001.octupole] + - [B1, OCTF1_QCORROCT_6_QT_001.quadrupole] + - [A1, OCTF1_QCORROCT_6_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN01-AR/EM-OCT/OC.04/strength + - AN01-AR/EM-COR/OC.04-CQLN.13/strength + - AN01-AR/EM-COR/OC.04-CQLT.05/strength +- type: pyaml.bpm.bpm + name: BPM_006 + x_pos: AN01-AR/DG-EPOS/BPM.07/x_pos + y_pos: AN01-AR/DG-EPOS/BPM.07/y_pos +- type: pyaml.magnet.cfm_magnet + name: SXD1_VCOR_002 + mapping: + - [B2, SXD1_VCOR_002.sextupole] + - [A0, SXD1_VCOR_002.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN01-AR/EM-SX/SCD.12/strength + - AN01-AR/EM-COR/SCD.12-CDLV.06/strength +- type: pyaml.magnet.quadrupole + name: QCORR_008 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN01-AR/EM-COR/CQLN.14/strength +- type: pyaml.magnet.quadrupole + name: QCORR_009 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN01-AR/EM-COR/CQLN.15/strength +- type: pyaml.magnet.sextupole + name: SXD1_003 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN01-AR/EM-SX/SCD.13/strength +- type: pyaml.magnet.cfm_magnet + name: SXF1_HCOR_002 + mapping: + - [B2, SXF1_HCOR_002.sextupole] + - [B0, SXF1_HCOR_002.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN01-AR/EM-SX/SCF.14/strength + - AN01-AR/EM-COR/SCF.14-CDLH.07/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF1_QCORROCT_7_QT_001 + mapping: + - [B3, OCTF1_QCORROCT_7_QT_001.octupole] + - [B1, OCTF1_QCORROCT_7_QT_001.quadrupole] + - [A1, OCTF1_QCORROCT_7_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN01-AR/EM-OCT/OC.05/strength + - AN01-AR/EM-COR/OC.05-CQLN.16/strength + - AN01-AR/EM-COR/OC.05-CQLT.06/strength +- type: pyaml.bpm.bpm + name: BPM_007 + x_pos: AN01-AR/DG-EPOS/BPM.08/x_pos + y_pos: AN01-AR/DG-EPOS/BPM.08/y_pos +- type: pyaml.magnet.cfm_magnet + name: SXD1_VCOR_003 + mapping: + - [B2, SXD1_VCOR_003.sextupole] + - [A0, SXD1_VCOR_003.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN01-AR/EM-SX/SCD.15/strength + - AN01-AR/EM-COR/SCD.15-CDLV.07/strength +- type: pyaml.magnet.quadrupole + name: QCORR_010 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN01-AR/EM-COR/CQLN.17/strength +- type: pyaml.magnet.quadrupole + name: QCORR_011 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN01-AR/EM-COR/CQLN.18/strength +- type: pyaml.magnet.sextupole + name: SXD12_001 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN01-AR/EM-SX/SCD.16/strength +- type: pyaml.magnet.cfm_magnet + name: SXF12_HCOR_001 + mapping: + - [B2, SXF12_HCOR_001.sextupole] + - [B0, SXF12_HCOR_001.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN01-AR/EM-SX/SCF.17/strength + - AN01-AR/EM-COR/SCF.17-CDLH.08/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF1_QCORROCT_8_QT_001 + mapping: + - [B3, OCTF1_QCORROCT_8_QT_001.octupole] + - [B1, OCTF1_QCORROCT_8_QT_001.quadrupole] + - [A1, OCTF1_QCORROCT_8_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN01-AR/EM-OCT/OC.06/strength + - AN01-AR/EM-COR/OC.06-CQLN.19/strength + - AN01-AR/EM-COR/OC.06-CQLT.07/strength +- type: pyaml.magnet.cfm_magnet + name: SXD12_VCOR_001 + mapping: + - [B2, SXD12_VCOR_001.sextupole] + - [A0, SXD12_VCOR_001.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN01-AR/EM-SX/SCD.18/strength + - AN01-AR/EM-COR/SCD.18-CDLV.08/strength +- type: pyaml.bpm.bpm + name: BPM_008 + x_pos: AN01-AR/DG-EPOS/BPM.09/x_pos + y_pos: AN01-AR/DG-EPOS/BPM.09/y_pos +- type: pyaml.magnet.cfm_magnet + name: SH6_COR_001 + mapping: + - [B2, SH6_COR_001.sextupole] + - [B0, SH6_COR_001.hcorrector] + - [A0, SH6_COR_001.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0, A0] + units: [1/m**2, '1', '1'] + physics: + - AN01-AR/EM-SX/SHD.04/strength + - AN01-AR/EM-COR/SHD.04-CDLH.09/strength + - AN01-AR/EM-COR/SHD.04-CDLV.09/strength +- type: pyaml.magnet.quadrupole + name: QCORR_012 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN01-AR/EM-COR/CQLN.20/strength +- type: pyaml.magnet.sextupole + name: SH5_001 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN01-AR/EM-SX/SHD.05/strength +- type: pyaml.magnet.cfm_magnet + name: OH5_QCORROCT_9_001 + mapping: + - [B3, OH5_QCORROCT_9_001.octupole] + - [B1, OH5_QCORROCT_9_001.quadrupole] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1] + units: [1/m**3, 1/m**2] + physics: + - AN01-AR/EM-OCT/OH.03/strength + - AN01-AR/EM-COR/OH.03-CQLN.21/strength +- type: pyaml.bpm.bpm + name: BPM_009 + x_pos: AN01-AR/DG-EPOS/BPM.10/x_pos + y_pos: AN01-AR/DG-EPOS/BPM.10/y_pos +- type: pyaml.magnet.cfm_magnet + name: SH4_COR_001 + mapping: + - [B2, SH4_COR_001.sextupole] + - [B0, SH4_COR_001.hcorrector] + - [A0, SH4_COR_001.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0, A0] + units: [1/m**2, '1', '1'] + physics: + - AN01-AR/EM-SX/SHF.06/strength + - AN01-AR/EM-COR/SHF.06-CDLH.10/strength + - AN01-AR/EM-COR/SHF.06-CDLV.10/strength +- type: pyaml.magnet.cfm_magnet + name: OH4_QCORROCT_10_QT_001 + mapping: + - [B3, OH4_QCORROCT_10_QT_001.octupole] + - [B1, OH4_QCORROCT_10_QT_001.quadrupole] + - [A1, OH4_QCORROCT_10_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN01-AR/EM-OCT/OH.04/strength + - AN01-AR/EM-COR/OH.04-CQLN.22/strength + - AN01-AR/EM-COR/OH.04-CQLT.08/strength +- type: pyaml.bpm.bpm + name: BPM_010 + x_pos: AN02-SD/DG-EPOS/BPM.01/x_pos + y_pos: AN02-SD/DG-EPOS/BPM.01/y_pos +- type: pyaml.bpm.bpm + name: BPM_011 + x_pos: AN02-SD/DG-EPOS/BPM.02/x_pos + y_pos: AN02-SD/DG-EPOS/BPM.02/y_pos +- type: pyaml.magnet.cfm_magnet + name: OH4_QCORROCT_11_QT_001 + mapping: + - [B3, OH4_QCORROCT_11_QT_001.octupole] + - [B1, OH4_QCORROCT_11_QT_001.quadrupole] + - [A1, OH4_QCORROCT_11_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN02-AR/EM-OCT/OH.01/strength + - AN02-AR/EM-COR/OH.01-CQLN.01/strength + - AN02-AR/EM-COR/OH.01-CQLT.01/strength +- type: pyaml.magnet.cfm_magnet + name: SH4_COR_002 + mapping: + - [B2, SH4_COR_002.sextupole] + - [B0, SH4_COR_002.hcorrector] + - [A0, SH4_COR_002.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0, A0] + units: [1/m**2, '1', '1'] + physics: + - AN02-AR/EM-SX/SHF.01/strength + - AN02-AR/EM-COR/SHF.01-CDLH.01/strength + - AN02-AR/EM-COR/SHF.01-CDLV.01/strength +- type: pyaml.bpm.bpm + name: BPM_012 + x_pos: AN02-AR/DG-EPOS/BPM.03/x_pos + y_pos: AN02-AR/DG-EPOS/BPM.03/y_pos +- type: pyaml.magnet.cfm_magnet + name: OH5_QCORROCT_12_001 + mapping: + - [B3, OH5_QCORROCT_12_001.octupole] + - [B1, OH5_QCORROCT_12_001.quadrupole] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1] + units: [1/m**3, 1/m**2] + physics: + - AN02-AR/EM-OCT/OH.02/strength + - AN02-AR/EM-COR/OH.02-CQLN.02/strength +- type: pyaml.magnet.sextupole + name: SH5_002 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN02-AR/EM-SX/SHD.02/strength +- type: pyaml.magnet.quadrupole + name: QCORR_013 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN02-AR/EM-COR/CQLN.03/strength +- type: pyaml.magnet.cfm_magnet + name: SH6_COR_002 + mapping: + - [B2, SH6_COR_002.sextupole] + - [B0, SH6_COR_002.hcorrector] + - [A0, SH6_COR_002.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0, A0] + units: [1/m**2, '1', '1'] + physics: + - AN02-AR/EM-SX/SHD.03/strength + - AN02-AR/EM-COR/SHD.03-CDLH.02/strength + - AN02-AR/EM-COR/SHD.03-CDLV.02/strength +- type: pyaml.magnet.sextupole + name: SXD21_001 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN02-AR/EM-SX/SCD.01/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF2_QCORROCT_13_QT_001 + mapping: + - [B3, OCTF2_QCORROCT_13_QT_001.octupole] + - [B1, OCTF2_QCORROCT_13_QT_001.quadrupole] + - [A1, OCTF2_QCORROCT_13_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN02-AR/EM-OCT/OC.01/strength + - AN02-AR/EM-COR/OC.01-CQLN.04/strength + - AN02-AR/EM-COR/OC.01-CQLT.02/strength +- type: pyaml.magnet.cfm_magnet + name: SXF21_HCOR_001 + mapping: + - [B2, SXF21_HCOR_001.sextupole] + - [B0, SXF21_HCOR_001.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN02-AR/EM-SX/SCF.02/strength + - AN02-AR/EM-COR/SCF.02-CDLH.03/strength +- type: pyaml.bpm.bpm + name: BPM_013 + x_pos: AN02-AR/DG-EPOS/BPM.04/x_pos + y_pos: AN02-AR/DG-EPOS/BPM.04/y_pos +- type: pyaml.magnet.cfm_magnet + name: SXD21_VCOR_001 + mapping: + - [B2, SXD21_VCOR_001.sextupole] + - [A0, SXD21_VCOR_001.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN02-AR/EM-SX/SCD.03/strength + - AN02-AR/EM-COR/SCD.03-CDLV.03/strength +- type: pyaml.magnet.quadrupole + name: QCORR_014 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN02-AR/EM-COR/CQLN.05/strength +- type: pyaml.magnet.quadrupole + name: QCORR_015 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN02-AR/EM-COR/CQLN.06/strength +- type: pyaml.magnet.sextupole + name: SXD2_001 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN02-AR/EM-SX/SCD.04/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF2_QCORROCT_14_QT_001 + mapping: + - [B3, OCTF2_QCORROCT_14_QT_001.octupole] + - [B1, OCTF2_QCORROCT_14_QT_001.quadrupole] + - [A1, OCTF2_QCORROCT_14_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN02-AR/EM-OCT/OC.02/strength + - AN02-AR/EM-COR/OC.02-CQLN.07/strength + - AN02-AR/EM-COR/OC.02-CQLT.03/strength +- type: pyaml.magnet.cfm_magnet + name: SXF2_HCOR_001 + mapping: + - [B2, SXF2_HCOR_001.sextupole] + - [B0, SXF2_HCOR_001.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN02-AR/EM-SX/SCF.05/strength + - AN02-AR/EM-COR/SCF.05-CDLH.04/strength +- type: pyaml.bpm.bpm + name: BPM_014 + x_pos: AN02-AR/DG-EPOS/BPM.05/x_pos + y_pos: AN02-AR/DG-EPOS/BPM.05/y_pos +- type: pyaml.magnet.cfm_magnet + name: SXD2_VCOR_001 + mapping: + - [B2, SXD2_VCOR_001.sextupole] + - [A0, SXD2_VCOR_001.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN02-AR/EM-SX/SCD.06/strength + - AN02-AR/EM-COR/SCD.06-CDLV.04/strength +- type: pyaml.magnet.quadrupole + name: QCORR_016 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN02-AR/EM-COR/CQLN.08/strength +- type: pyaml.magnet.quadrupole + name: QCORR_017 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN02-AR/EM-COR/CQLN.09/strength +- type: pyaml.magnet.sextupole + name: SXD22_001 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN02-AR/EM-SX/SCD.07/strength +- type: pyaml.magnet.cfm_magnet + name: SXF22_HCOR_001 + mapping: + - [B2, SXF22_HCOR_001.sextupole] + - [B0, SXF22_HCOR_001.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN02-AR/EM-SX/SCF.08/strength + - AN02-AR/EM-COR/SCF.08-CDLH.05/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF2_QCORROCT_15_QT_001 + mapping: + - [B3, OCTF2_QCORROCT_15_QT_001.octupole] + - [B1, OCTF2_QCORROCT_15_QT_001.quadrupole] + - [A1, OCTF2_QCORROCT_15_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN02-AR/EM-OCT/OC.03/strength + - AN02-AR/EM-COR/OC.03-CQLN.10/strength + - AN02-AR/EM-COR/OC.03-CQLT.04/strength +- type: pyaml.magnet.cfm_magnet + name: SXD22_VCOR_001 + mapping: + - [B2, SXD22_VCOR_001.sextupole] + - [A0, SXD22_VCOR_001.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN02-AR/EM-SX/SCD.09/strength + - AN02-AR/EM-COR/SCD.09-CDLV.05/strength +- type: pyaml.bpm.bpm + name: BPM_015 + x_pos: AN02-AR/DG-EPOS/BPM.06/x_pos + y_pos: AN02-AR/DG-EPOS/BPM.06/y_pos +- type: pyaml.magnet.cfm_magnet + name: SH9_COR_001 + mapping: + - [B2, SH9_COR_001.sextupole] + - [B0, SH9_COR_001.hcorrector] + - [A0, SH9_COR_001.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0, A0] + units: [1/m**2, '1', '1'] + physics: + - AN02-AR/EM-SX/SHD.04/strength + - AN02-AR/EM-COR/SHD.04-CDLH.06/strength + - AN02-AR/EM-COR/SHD.04-CDLV.06/strength +- type: pyaml.magnet.quadrupole + name: QCORR_018 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN02-AR/EM-COR/CQLN.11/strength +- type: pyaml.magnet.sextupole + name: SH8_001 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN02-AR/EM-SX/SHD.05/strength +- type: pyaml.magnet.quadrupole + name: QCORR_019 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN02-AR/EM-COR/CQLN.12/strength +- type: pyaml.bpm.bpm + name: BPM_016 + x_pos: AN02-AR/DG-EPOS/BPM.07/x_pos + y_pos: AN02-AR/DG-EPOS/BPM.07/y_pos +- type: pyaml.magnet.cfm_magnet + name: SH7_COR_001 + mapping: + - [B2, SH7_COR_001.sextupole] + - [B0, SH7_COR_001.hcorrector] + - [A0, SH7_COR_001.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0, A0] + units: [1/m**2, '1', '1'] + physics: + - AN02-AR/EM-SX/SHF.06/strength + - AN02-AR/EM-COR/SHF.06-CDLH.07/strength + - AN02-AR/EM-COR/SHF.06-CDLV.07/strength +- type: pyaml.magnet.cfm_magnet + name: OH7_QCORROCT_16_QT_001 + mapping: + - [B3, OH7_QCORROCT_16_QT_001.octupole] + - [B1, OH7_QCORROCT_16_QT_001.quadrupole] + - [A1, OH7_QCORROCT_16_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN02-AR/EM-OCT/OH.03/strength + - AN02-AR/EM-COR/OH.03-CQLN.13/strength + - AN02-AR/EM-COR/OH.03-CQLT.05/strength +- type: pyaml.bpm.bpm + name: BPM_017 + x_pos: AN03-SD/DG-EPOS/BPM.01/x_pos + y_pos: AN03-SD/DG-EPOS/BPM.01/y_pos +- type: pyaml.bpm.bpm + name: BPM_018 + x_pos: AN03-SD/DG-EPOS/BPM.02/x_pos + y_pos: AN03-SD/DG-EPOS/BPM.02/y_pos +- type: pyaml.magnet.cfm_magnet + name: OH7_QCORROCT_17_QT_001 + mapping: + - [B3, OH7_QCORROCT_17_QT_001.octupole] + - [B1, OH7_QCORROCT_17_QT_001.quadrupole] + - [A1, OH7_QCORROCT_17_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN03-AR/EM-OCT/OH.01/strength + - AN03-AR/EM-COR/OH.01-CQLN.01/strength + - AN03-AR/EM-COR/OH.01-CQLT.01/strength +- type: pyaml.magnet.cfm_magnet + name: SH7_COR_002 + mapping: + - [B2, SH7_COR_002.sextupole] + - [B0, SH7_COR_002.hcorrector] + - [A0, SH7_COR_002.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0, A0] + units: [1/m**2, '1', '1'] + physics: + - AN03-AR/EM-SX/SHF.01/strength + - AN03-AR/EM-COR/SHF.01-CDLH.01/strength + - AN03-AR/EM-COR/SHF.01-CDLV.01/strength +- type: pyaml.bpm.bpm + name: BPM_019 + x_pos: AN03-AR/DG-EPOS/BPM.03/x_pos + y_pos: AN03-AR/DG-EPOS/BPM.03/y_pos +- type: pyaml.magnet.quadrupole + name: QCORR_020 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN03-AR/EM-COR/CQLN.02/strength +- type: pyaml.magnet.sextupole + name: SH8_002 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN03-AR/EM-SX/SHD.02/strength +- type: pyaml.magnet.quadrupole + name: QCORR_021 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN03-AR/EM-COR/CQLN.03/strength +- type: pyaml.magnet.cfm_magnet + name: SH9_COR_002 + mapping: + - [B2, SH9_COR_002.sextupole] + - [B0, SH9_COR_002.hcorrector] + - [A0, SH9_COR_002.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0, A0] + units: [1/m**2, '1', '1'] + physics: + - AN03-AR/EM-SX/SHD.03/strength + - AN03-AR/EM-COR/SHD.03-CDLH.02/strength + - AN03-AR/EM-COR/SHD.03-CDLV.02/strength +- type: pyaml.magnet.sextupole + name: SXD31_001 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN03-AR/EM-SX/SCD.01/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF3_QCORROCT_18_QT_001 + mapping: + - [B3, OCTF3_QCORROCT_18_QT_001.octupole] + - [B1, OCTF3_QCORROCT_18_QT_001.quadrupole] + - [A1, OCTF3_QCORROCT_18_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN03-AR/EM-OCT/OC.01/strength + - AN03-AR/EM-COR/OC.01-CQLN.04/strength + - AN03-AR/EM-COR/OC.01-CQLT.02/strength +- type: pyaml.magnet.cfm_magnet + name: SXF31_HCOR_001 + mapping: + - [B2, SXF31_HCOR_001.sextupole] + - [B0, SXF31_HCOR_001.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN03-AR/EM-SX/SCF.02/strength + - AN03-AR/EM-COR/SCF.02-CDLH.03/strength +- type: pyaml.bpm.bpm + name: BPM_020 + x_pos: AN03-AR/DG-EPOS/BPM.04/x_pos + y_pos: AN03-AR/DG-EPOS/BPM.04/y_pos +- type: pyaml.magnet.cfm_magnet + name: SXD31_VCOR_001 + mapping: + - [B2, SXD31_VCOR_001.sextupole] + - [A0, SXD31_VCOR_001.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN03-AR/EM-SX/SCD.03/strength + - AN03-AR/EM-COR/SCD.03-CDLV.03/strength +- type: pyaml.magnet.quadrupole + name: QCORR_022 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN03-AR/EM-COR/CQLN.05/strength +- type: pyaml.magnet.quadrupole + name: QCORR_023 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN03-AR/EM-COR/CQLN.06/strength +- type: pyaml.magnet.sextupole + name: SXD3_001 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN03-AR/EM-SX/SCD.04/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF3_QCORROCT_19_QT_001 + mapping: + - [B3, OCTF3_QCORROCT_19_QT_001.octupole] + - [B1, OCTF3_QCORROCT_19_QT_001.quadrupole] + - [A1, OCTF3_QCORROCT_19_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN03-AR/EM-OCT/OC.02/strength + - AN03-AR/EM-COR/OC.02-CQLN.07/strength + - AN03-AR/EM-COR/OC.02-CQLT.03/strength +- type: pyaml.magnet.cfm_magnet + name: SXF3_HCOR_001 + mapping: + - [B2, SXF3_HCOR_001.sextupole] + - [B0, SXF3_HCOR_001.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN03-AR/EM-SX/SCF.05/strength + - AN03-AR/EM-COR/SCF.05-CDLH.04/strength +- type: pyaml.bpm.bpm + name: BPM_021 + x_pos: AN03-AR/DG-EPOS/BPM.05/x_pos + y_pos: AN03-AR/DG-EPOS/BPM.05/y_pos +- type: pyaml.magnet.cfm_magnet + name: SXD3_VCOR_001 + mapping: + - [B2, SXD3_VCOR_001.sextupole] + - [A0, SXD3_VCOR_001.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN03-AR/EM-SX/SCD.06/strength + - AN03-AR/EM-COR/SCD.06-CDLV.04/strength +- type: pyaml.magnet.quadrupole + name: QCORR_024 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN03-AR/EM-COR/CQLN.08/strength +- type: pyaml.magnet.quadrupole + name: QCORR_025 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN03-AR/EM-COR/CQLN.09/strength +- type: pyaml.magnet.sextupole + name: SXD3_002 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN03-AR/EM-SX/SCD.07/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF3_QCORROCT_20_QT_001 + mapping: + - [B3, OCTF3_QCORROCT_20_QT_001.octupole] + - [B1, OCTF3_QCORROCT_20_QT_001.quadrupole] + - [A1, OCTF3_QCORROCT_20_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN03-AR/EM-OCT/OC.03/strength + - AN03-AR/EM-COR/OC.03-CQLN.10/strength + - AN03-AR/EM-COR/OC.03-CQLT.04/strength +- type: pyaml.magnet.cfm_magnet + name: SXF33_HCOR_001 + mapping: + - [B2, SXF33_HCOR_001.sextupole] + - [B0, SXF33_HCOR_001.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN03-AR/EM-SX/SCF.08/strength + - AN03-AR/EM-COR/SCF.08-CDLH.05/strength +- type: pyaml.bpm.bpm + name: BPM_022 + x_pos: AN03-AR/DG-EPOS/BPM.06/x_pos + y_pos: AN03-AR/DG-EPOS/BPM.06/y_pos +- type: pyaml.magnet.cfm_magnet + name: SXD33_VCOR_001 + mapping: + - [B2, SXD33_VCOR_001.sextupole] + - [A0, SXD33_VCOR_001.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN03-AR/EM-SX/SCD.09/strength + - AN03-AR/EM-COR/SCD.09-CDLV.05/strength +- type: pyaml.magnet.quadrupole + name: QCORR_026 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN03-AR/EM-COR/CQLN.11/strength +- type: pyaml.magnet.quadrupole + name: QCORR_027 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN03-AR/EM-COR/CQLN.12/strength +- type: pyaml.magnet.sextupole + name: SXD33_001 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN03-AR/EM-SX/SCD.10/strength +- type: pyaml.magnet.cfm_magnet + name: SXF33_HCOR_002 + mapping: + - [B2, SXF33_HCOR_002.sextupole] + - [B0, SXF33_HCOR_002.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN03-AR/EM-SX/SCF.11/strength + - AN03-AR/EM-COR/SCF.11-CDLH.06/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF3_QCORROCT_21_QT_001 + mapping: + - [B3, OCTF3_QCORROCT_21_QT_001.octupole] + - [B1, OCTF3_QCORROCT_21_QT_001.quadrupole] + - [A1, OCTF3_QCORROCT_21_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN03-AR/EM-OCT/OC.04/strength + - AN03-AR/EM-COR/OC.04-CQLN.13/strength + - AN03-AR/EM-COR/OC.04-CQLT.05/strength +- type: pyaml.bpm.bpm + name: BPM_023 + x_pos: AN03-AR/DG-EPOS/BPM.07/x_pos + y_pos: AN03-AR/DG-EPOS/BPM.07/y_pos +- type: pyaml.magnet.cfm_magnet + name: SXD3_VCOR_002 + mapping: + - [B2, SXD3_VCOR_002.sextupole] + - [A0, SXD3_VCOR_002.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN03-AR/EM-SX/SCD.12/strength + - AN03-AR/EM-COR/SCD.12-CDLV.06/strength +- type: pyaml.magnet.quadrupole + name: QCORR_028 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN03-AR/EM-COR/CQLN.14/strength +- type: pyaml.magnet.quadrupole + name: QCORR_029 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN03-AR/EM-COR/CQLN.15/strength +- type: pyaml.magnet.sextupole + name: SXD3_003 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN03-AR/EM-SX/SCD.13/strength +- type: pyaml.magnet.cfm_magnet + name: SXF3_HCOR_002 + mapping: + - [B2, SXF3_HCOR_002.sextupole] + - [B0, SXF3_HCOR_002.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN03-AR/EM-SX/SCF.14/strength + - AN03-AR/EM-COR/SCF.14-CDLH.07/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF3_QCORROCT_22_QT_001 + mapping: + - [B3, OCTF3_QCORROCT_22_QT_001.octupole] + - [B1, OCTF3_QCORROCT_22_QT_001.quadrupole] + - [A1, OCTF3_QCORROCT_22_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN03-AR/EM-OCT/OC.05/strength + - AN03-AR/EM-COR/OC.05-CQLN.16/strength + - AN03-AR/EM-COR/OC.05-CQLT.06/strength +- type: pyaml.bpm.bpm + name: BPM_024 + x_pos: AN03-AR/DG-EPOS/BPM.08/x_pos + y_pos: AN03-AR/DG-EPOS/BPM.08/y_pos +- type: pyaml.magnet.cfm_magnet + name: SXD3_VCOR_003 + mapping: + - [B2, SXD3_VCOR_003.sextupole] + - [A0, SXD3_VCOR_003.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN03-AR/EM-SX/SCD.15/strength + - AN03-AR/EM-COR/SCD.15-CDLV.07/strength +- type: pyaml.magnet.quadrupole + name: QCORR_030 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN03-AR/EM-COR/CQLN.17/strength +- type: pyaml.magnet.quadrupole + name: QCORR_031 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN03-AR/EM-COR/CQLN.18/strength +- type: pyaml.magnet.sextupole + name: SXD32_001 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN03-AR/EM-SX/SCD.16/strength +- type: pyaml.magnet.cfm_magnet + name: SXF32_HCOR_001 + mapping: + - [B2, SXF32_HCOR_001.sextupole] + - [B0, SXF32_HCOR_001.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN03-AR/EM-SX/SCF.17/strength + - AN03-AR/EM-COR/SCF.17-CDLH.08/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF3_QCORROCT_23_QT_001 + mapping: + - [B3, OCTF3_QCORROCT_23_QT_001.octupole] + - [B1, OCTF3_QCORROCT_23_QT_001.quadrupole] + - [A1, OCTF3_QCORROCT_23_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN03-AR/EM-OCT/OC.06/strength + - AN03-AR/EM-COR/OC.06-CQLN.19/strength + - AN03-AR/EM-COR/OC.06-CQLT.07/strength +- type: pyaml.magnet.cfm_magnet + name: SXD32_VCOR_001 + mapping: + - [B2, SXD32_VCOR_001.sextupole] + - [A0, SXD32_VCOR_001.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN03-AR/EM-SX/SCD.18/strength + - AN03-AR/EM-COR/SCD.18-CDLV.08/strength +- type: pyaml.bpm.bpm + name: BPM_025 + x_pos: AN03-AR/DG-EPOS/BPM.09/x_pos + y_pos: AN03-AR/DG-EPOS/BPM.09/y_pos +- type: pyaml.magnet.cfm_magnet + name: SH9_COR_003 + mapping: + - [B2, SH9_COR_003.sextupole] + - [B0, SH9_COR_003.hcorrector] + - [A0, SH9_COR_003.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0, A0] + units: [1/m**2, '1', '1'] + physics: + - AN03-AR/EM-SX/SHD.04/strength + - AN03-AR/EM-COR/SHD.04-CDLH.09/strength + - AN03-AR/EM-COR/SHD.04-CDLV.09/strength +- type: pyaml.magnet.quadrupole + name: QCORR_032 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN03-AR/EM-COR/CQLN.20/strength +- type: pyaml.magnet.sextupole + name: SH8_003 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN03-AR/EM-SX/SHD.05/strength +- type: pyaml.magnet.quadrupole + name: QCORR_033 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN03-AR/EM-COR/CQLN.21/strength +- type: pyaml.bpm.bpm + name: BPM_026 + x_pos: AN03-AR/DG-EPOS/BPM.10/x_pos + y_pos: AN03-AR/DG-EPOS/BPM.10/y_pos +- type: pyaml.magnet.cfm_magnet + name: SH7_COR_003 + mapping: + - [B2, SH7_COR_003.sextupole] + - [B0, SH7_COR_003.hcorrector] + - [A0, SH7_COR_003.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0, A0] + units: [1/m**2, '1', '1'] + physics: + - AN03-AR/EM-SX/SHF.06/strength + - AN03-AR/EM-COR/SHF.06-CDLH.10/strength + - AN03-AR/EM-COR/SHF.06-CDLV.10/strength +- type: pyaml.magnet.cfm_magnet + name: OH7_QCORROCT_24_QT_001 + mapping: + - [B3, OH7_QCORROCT_24_QT_001.octupole] + - [B1, OH7_QCORROCT_24_QT_001.quadrupole] + - [A1, OH7_QCORROCT_24_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN03-AR/EM-OCT/OH.02/strength + - AN03-AR/EM-COR/OH.02-CQLN.22/strength + - AN03-AR/EM-COR/OH.02-CQLT.08/strength +- type: pyaml.bpm.bpm + name: BPM_027 + x_pos: AN04-SD/DG-EPOS/BPM.01/x_pos + y_pos: AN04-SD/DG-EPOS/BPM.01/y_pos +- type: pyaml.bpm.bpm + name: BPM_028 + x_pos: AN04-SD/DG-EPOS/BPM.02/x_pos + y_pos: AN04-SD/DG-EPOS/BPM.02/y_pos +- type: pyaml.magnet.cfm_magnet + name: OH7_QCORROCT_25_QT_001 + mapping: + - [B3, OH7_QCORROCT_25_QT_001.octupole] + - [B1, OH7_QCORROCT_25_QT_001.quadrupole] + - [A1, OH7_QCORROCT_25_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN04-AR/EM-OCT/OH.01/strength + - AN04-AR/EM-COR/OH.01-CQLN.01/strength + - AN04-AR/EM-COR/OH.01-CQLT.01/strength +- type: pyaml.magnet.cfm_magnet + name: SH7_COR_004 + mapping: + - [B2, SH7_COR_004.sextupole] + - [B0, SH7_COR_004.hcorrector] + - [A0, SH7_COR_004.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0, A0] + units: [1/m**2, '1', '1'] + physics: + - AN04-AR/EM-SX/SHF.01/strength + - AN04-AR/EM-COR/SHF.01-CDLH.01/strength + - AN04-AR/EM-COR/SHF.01-CDLV.01/strength +- type: pyaml.bpm.bpm + name: BPM_029 + x_pos: AN04-AR/DG-EPOS/BPM.03/x_pos + y_pos: AN04-AR/DG-EPOS/BPM.03/y_pos +- type: pyaml.magnet.quadrupole + name: QCORR_034 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN04-AR/EM-COR/CQLN.02/strength +- type: pyaml.magnet.sextupole + name: SH8_004 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN04-AR/EM-SX/SHD.02/strength +- type: pyaml.magnet.quadrupole + name: QCORR_035 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN04-AR/EM-COR/CQLN.03/strength +- type: pyaml.magnet.cfm_magnet + name: SH9_COR_004 + mapping: + - [B2, SH9_COR_004.sextupole] + - [B0, SH9_COR_004.hcorrector] + - [A0, SH9_COR_004.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0, A0] + units: [1/m**2, '1', '1'] + physics: + - AN04-AR/EM-SX/SHD.03/strength + - AN04-AR/EM-COR/SHD.03-CDLH.02/strength + - AN04-AR/EM-COR/SHD.03-CDLV.02/strength +- type: pyaml.magnet.sextupole + name: SXD41_001 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN04-AR/EM-SX/SCD.01/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF4_QCORROCT_26_QT_001 + mapping: + - [B3, OCTF4_QCORROCT_26_QT_001.octupole] + - [B1, OCTF4_QCORROCT_26_QT_001.quadrupole] + - [A1, OCTF4_QCORROCT_26_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN04-AR/EM-OCT/OC.01/strength + - AN04-AR/EM-COR/OC.01-CQLN.04/strength + - AN04-AR/EM-COR/OC.01-CQLT.02/strength +- type: pyaml.magnet.cfm_magnet + name: SXF41_HCOR_001 + mapping: + - [B2, SXF41_HCOR_001.sextupole] + - [B0, SXF41_HCOR_001.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN04-AR/EM-SX/SCF.02/strength + - AN04-AR/EM-COR/SCF.02-CDLH.03/strength +- type: pyaml.bpm.bpm + name: BPM_030 + x_pos: AN04-AR/DG-EPOS/BPM.04/x_pos + y_pos: AN04-AR/DG-EPOS/BPM.04/y_pos +- type: pyaml.magnet.cfm_magnet + name: SXD41_VCOR_001 + mapping: + - [B2, SXD41_VCOR_001.sextupole] + - [A0, SXD41_VCOR_001.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN04-AR/EM-SX/SCD.03/strength + - AN04-AR/EM-COR/SCD.03-CDLV.03/strength +- type: pyaml.magnet.quadrupole + name: QCORR_036 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN04-AR/EM-COR/CQLN.05/strength +- type: pyaml.magnet.quadrupole + name: QCORR_037 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN04-AR/EM-COR/CQLN.06/strength +- type: pyaml.magnet.sextupole + name: SXD4_001 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN04-AR/EM-SX/SCD.04/strength +- type: pyaml.magnet.cfm_magnet + name: SXF4_HCOR_001 + mapping: + - [B2, SXF4_HCOR_001.sextupole] + - [B0, SXF4_HCOR_001.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN04-AR/EM-SX/SCF.05/strength + - AN04-AR/EM-COR/SCF.05-CDLH.04/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF4_QCORROCT_27_QT_001 + mapping: + - [B3, OCTF4_QCORROCT_27_QT_001.octupole] + - [B1, OCTF4_QCORROCT_27_QT_001.quadrupole] + - [A1, OCTF4_QCORROCT_27_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN04-AR/EM-OCT/OC.02/strength + - AN04-AR/EM-COR/OC.02-CQLN.07/strength + - AN04-AR/EM-COR/OC.02-CQLT.03/strength +- type: pyaml.bpm.bpm + name: BPM_031 + x_pos: AN04-AR/DG-EPOS/BPM.05/x_pos + y_pos: AN04-AR/DG-EPOS/BPM.05/y_pos +- type: pyaml.magnet.cfm_magnet + name: SXD4_VCOR_001 + mapping: + - [B2, SXD4_VCOR_001.sextupole] + - [A0, SXD4_VCOR_001.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN04-AR/EM-SX/SCD.06/strength + - AN04-AR/EM-COR/SCD.06-CDLV.04/strength +- type: pyaml.magnet.quadrupole + name: QCORR_038 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN04-AR/EM-COR/CQLN.08/strength +- type: pyaml.magnet.quadrupole + name: QCORR_039 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN04-AR/EM-COR/CQLN.09/strength +- type: pyaml.magnet.sextupole + name: SXD42_001 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN04-AR/EM-SX/SCD.07/strength +- type: pyaml.magnet.cfm_magnet + name: SXF42_HCOR_001 + mapping: + - [B2, SXF42_HCOR_001.sextupole] + - [B0, SXF42_HCOR_001.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN04-AR/EM-SX/SCF.08/strength + - AN04-AR/EM-COR/SCF.08-CDLH.05/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF4_QCORROCT_28_QT_001 + mapping: + - [B3, OCTF4_QCORROCT_28_QT_001.octupole] + - [B1, OCTF4_QCORROCT_28_QT_001.quadrupole] + - [A1, OCTF4_QCORROCT_28_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN04-AR/EM-OCT/OC.03/strength + - AN04-AR/EM-COR/OC.03-CQLN.10/strength + - AN04-AR/EM-COR/OC.03-CQLT.04/strength +- type: pyaml.magnet.cfm_magnet + name: SXD42_VCOR_001 + mapping: + - [B2, SXD42_VCOR_001.sextupole] + - [A0, SXD42_VCOR_001.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN04-AR/EM-SX/SCD.09/strength + - AN04-AR/EM-COR/SCD.09-CDLV.05/strength +- type: pyaml.bpm.bpm + name: BPM_032 + x_pos: AN04-AR/DG-EPOS/BPM.06/x_pos + y_pos: AN04-AR/DG-EPOS/BPM.06/y_pos +- type: pyaml.magnet.cfm_magnet + name: SH12_COR_001 + mapping: + - [B2, SH12_COR_001.sextupole] + - [B0, SH12_COR_001.hcorrector] + - [A0, SH12_COR_001.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0, A0] + units: [1/m**2, '1', '1'] + physics: + - AN04-AR/EM-SX/SHD.04/strength + - AN04-AR/EM-COR/SHD.04-CDLH.06/strength + - AN04-AR/EM-COR/SHD.04-CDLV.06/strength +- type: pyaml.magnet.quadrupole + name: QCORR_040 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN04-AR/EM-COR/CQLN.11/strength +- type: pyaml.magnet.sextupole + name: SH11_001 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN04-AR/EM-SX/SHD.05/strength +- type: pyaml.magnet.cfm_magnet + name: OH11_QCORROCT_29_001 + mapping: + - [B3, OH11_QCORROCT_29_001.octupole] + - [B1, OH11_QCORROCT_29_001.quadrupole] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1] + units: [1/m**3, 1/m**2] + physics: + - AN04-AR/EM-OCT/OH.02/strength + - AN04-AR/EM-COR/OH.02-CQLN.12/strength +- type: pyaml.bpm.bpm + name: BPM_033 + x_pos: AN04-AR/DG-EPOS/BPM.07/x_pos + y_pos: AN04-AR/DG-EPOS/BPM.07/y_pos +- type: pyaml.magnet.cfm_magnet + name: SH10_COR_001 + mapping: + - [B2, SH10_COR_001.sextupole] + - [B0, SH10_COR_001.hcorrector] + - [A0, SH10_COR_001.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0, A0] + units: [1/m**2, '1', '1'] + physics: + - AN04-AR/EM-SX/SHF.06/strength + - AN04-AR/EM-COR/SHF.06-CDLH.07/strength + - AN04-AR/EM-COR/SHF.06-CDLV.07/strength +- type: pyaml.magnet.cfm_magnet + name: OH10_QCORROCT_30_QT_001 + mapping: + - [B3, OH10_QCORROCT_30_QT_001.octupole] + - [B1, OH10_QCORROCT_30_QT_001.quadrupole] + - [A1, OH10_QCORROCT_30_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN04-AR/EM-OCT/OH.03/strength + - AN04-AR/EM-COR/OH.03-CQLN.13/strength + - AN04-AR/EM-COR/OH.03-CQLT.05/strength +- type: pyaml.bpm.bpm + name: BPM_034 + x_pos: AN05-SD/DG-EPOS/BPM.01/x_pos + y_pos: AN05-SD/DG-EPOS/BPM.01/y_pos +- type: pyaml.bpm.bpm + name: BPM_035 + x_pos: AN05-SD/DG-EPOS/BPM.02/x_pos + y_pos: AN05-SD/DG-EPOS/BPM.02/y_pos +- type: pyaml.magnet.cfm_magnet + name: OH10_QCORROCT_31_QT_001 + mapping: + - [B3, OH10_QCORROCT_31_QT_001.octupole] + - [B1, OH10_QCORROCT_31_QT_001.quadrupole] + - [A1, OH10_QCORROCT_31_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN05-AR/EM-OCT/OH.01/strength + - AN05-AR/EM-COR/OH.01-CQLN.01/strength + - AN05-AR/EM-COR/OH.01-CQLT.01/strength +- type: pyaml.magnet.cfm_magnet + name: SH10_COR_002 + mapping: + - [B2, SH10_COR_002.sextupole] + - [B0, SH10_COR_002.hcorrector] + - [A0, SH10_COR_002.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0, A0] + units: [1/m**2, '1', '1'] + physics: + - AN05-AR/EM-SX/SHF.01/strength + - AN05-AR/EM-COR/SHF.01-CDLH.01/strength + - AN05-AR/EM-COR/SHF.01-CDLV.01/strength +- type: pyaml.bpm.bpm + name: BPM_036 + x_pos: AN05-AR/DG-EPOS/BPM.03/x_pos + y_pos: AN05-AR/DG-EPOS/BPM.03/y_pos +- type: pyaml.magnet.cfm_magnet + name: OH11_QCORROCT_32_001 + mapping: + - [B3, OH11_QCORROCT_32_001.octupole] + - [B1, OH11_QCORROCT_32_001.quadrupole] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1] + units: [1/m**3, 1/m**2] + physics: + - AN05-AR/EM-OCT/OH.02/strength + - AN05-AR/EM-COR/OH.02-CQLN.02/strength +- type: pyaml.magnet.sextupole + name: SH11_002 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN05-AR/EM-SX/SHD.02/strength +- type: pyaml.magnet.quadrupole + name: QCORR_041 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN05-AR/EM-COR/CQLN.03/strength +- type: pyaml.magnet.cfm_magnet + name: SH12_COR_002 + mapping: + - [B2, SH12_COR_002.sextupole] + - [B0, SH12_COR_002.hcorrector] + - [A0, SH12_COR_002.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0, A0] + units: [1/m**2, '1', '1'] + physics: + - AN05-AR/EM-SX/SHD.03/strength + - AN05-AR/EM-COR/SHD.03-CDLH.02/strength + - AN05-AR/EM-COR/SHD.03-CDLV.02/strength +- type: pyaml.magnet.sextupole + name: SXD51_001 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN05-AR/EM-SX/SCD.01/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF5_QCORROCT_33_QT_001 + mapping: + - [B3, OCTF5_QCORROCT_33_QT_001.octupole] + - [B1, OCTF5_QCORROCT_33_QT_001.quadrupole] + - [A1, OCTF5_QCORROCT_33_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN05-AR/EM-OCT/OC.01/strength + - AN05-AR/EM-COR/OC.01-CQLN.04/strength + - AN05-AR/EM-COR/OC.01-CQLT.02/strength +- type: pyaml.magnet.cfm_magnet + name: SXF51_HCOR_001 + mapping: + - [B2, SXF51_HCOR_001.sextupole] + - [B0, SXF51_HCOR_001.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN05-AR/EM-SX/SCF.02/strength + - AN05-AR/EM-COR/SCF.02-CDLH.03/strength +- type: pyaml.bpm.bpm + name: BPM_037 + x_pos: AN05-AR/DG-EPOS/BPM.04/x_pos + y_pos: AN05-AR/DG-EPOS/BPM.04/y_pos +- type: pyaml.magnet.cfm_magnet + name: SXD51_VCOR_001 + mapping: + - [B2, SXD51_VCOR_001.sextupole] + - [A0, SXD51_VCOR_001.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN05-AR/EM-SX/SCD.03/strength + - AN05-AR/EM-COR/SCD.03-CDLV.03/strength +- type: pyaml.magnet.quadrupole + name: QCORR_042 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN05-AR/EM-COR/CQLN.05/strength +- type: pyaml.magnet.quadrupole + name: QCORR_043 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN05-AR/EM-COR/CQLN.06/strength +- type: pyaml.magnet.sextupole + name: SXD5_001 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN05-AR/EM-SX/SCD.04/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF5_QCORROCT_34_QT_001 + mapping: + - [B3, OCTF5_QCORROCT_34_QT_001.octupole] + - [B1, OCTF5_QCORROCT_34_QT_001.quadrupole] + - [A1, OCTF5_QCORROCT_34_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN05-AR/EM-OCT/OC.02/strength + - AN05-AR/EM-COR/OC.02-CQLN.07/strength + - AN05-AR/EM-COR/OC.02-CQLT.03/strength +- type: pyaml.magnet.cfm_magnet + name: SXF5_HCOR_001 + mapping: + - [B2, SXF5_HCOR_001.sextupole] + - [B0, SXF5_HCOR_001.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN05-AR/EM-SX/SCF.05/strength + - AN05-AR/EM-COR/SCF.05-CDLH.04/strength +- type: pyaml.bpm.bpm + name: BPM_038 + x_pos: AN05-AR/DG-EPOS/BPM.05/x_pos + y_pos: AN05-AR/DG-EPOS/BPM.05/y_pos +- type: pyaml.magnet.cfm_magnet + name: SXD5_VCOR_001 + mapping: + - [B2, SXD5_VCOR_001.sextupole] + - [A0, SXD5_VCOR_001.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN05-AR/EM-SX/SCD.06/strength + - AN05-AR/EM-COR/SCD.06-CDLV.04/strength +- type: pyaml.magnet.quadrupole + name: QCORR_044 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN05-AR/EM-COR/CQLN.08/strength +- type: pyaml.magnet.quadrupole + name: QCORR_045 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN05-AR/EM-COR/CQLN.09/strength +- type: pyaml.magnet.sextupole + name: SXD5_002 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN05-AR/EM-SX/SCD.07/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF5_QCORROCT_35_QT_001 + mapping: + - [B3, OCTF5_QCORROCT_35_QT_001.octupole] + - [B1, OCTF5_QCORROCT_35_QT_001.quadrupole] + - [A1, OCTF5_QCORROCT_35_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN05-AR/EM-OCT/OC.03/strength + - AN05-AR/EM-COR/OC.03-CQLN.10/strength + - AN05-AR/EM-COR/OC.03-CQLT.04/strength +- type: pyaml.magnet.cfm_magnet + name: SXF53_HCOR_001 + mapping: + - [B2, SXF53_HCOR_001.sextupole] + - [B0, SXF53_HCOR_001.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN05-AR/EM-SX/SCF.08/strength + - AN05-AR/EM-COR/SCF.08-CDLH.05/strength +- type: pyaml.bpm.bpm + name: BPM_039 + x_pos: AN05-AR/DG-EPOS/BPM.06/x_pos + y_pos: AN05-AR/DG-EPOS/BPM.06/y_pos +- type: pyaml.magnet.cfm_magnet + name: SXD53_VCOR_001 + mapping: + - [B2, SXD53_VCOR_001.sextupole] + - [A0, SXD53_VCOR_001.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN05-AR/EM-SX/SCD.09/strength + - AN05-AR/EM-COR/SCD.09-CDLV.05/strength +- type: pyaml.magnet.quadrupole + name: QCORR_046 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN05-AR/EM-COR/CQLN.11/strength +- type: pyaml.magnet.quadrupole + name: QCORR_047 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN05-AR/EM-COR/CQLN.12/strength +- type: pyaml.magnet.sextupole + name: SXD53_001 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN05-AR/EM-SX/SCD.10/strength +- type: pyaml.magnet.cfm_magnet + name: SXF53_HCOR_002 + mapping: + - [B2, SXF53_HCOR_002.sextupole] + - [B0, SXF53_HCOR_002.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN05-AR/EM-SX/SCF.11/strength + - AN05-AR/EM-COR/SCF.11-CDLH.06/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF5_QCORROCT_36_QT_001 + mapping: + - [B3, OCTF5_QCORROCT_36_QT_001.octupole] + - [B1, OCTF5_QCORROCT_36_QT_001.quadrupole] + - [A1, OCTF5_QCORROCT_36_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN05-AR/EM-OCT/OC.04/strength + - AN05-AR/EM-COR/OC.04-CQLN.13/strength + - AN05-AR/EM-COR/OC.04-CQLT.05/strength +- type: pyaml.bpm.bpm + name: BPM_040 + x_pos: AN05-AR/DG-EPOS/BPM.07/x_pos + y_pos: AN05-AR/DG-EPOS/BPM.07/y_pos +- type: pyaml.magnet.cfm_magnet + name: SXD5_VCOR_002 + mapping: + - [B2, SXD5_VCOR_002.sextupole] + - [A0, SXD5_VCOR_002.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN05-AR/EM-SX/SCD.12/strength + - AN05-AR/EM-COR/SCD.12-CDLV.06/strength +- type: pyaml.magnet.quadrupole + name: QCORR_048 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN05-AR/EM-COR/CQLN.14/strength +- type: pyaml.magnet.quadrupole + name: QCORR_049 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN05-AR/EM-COR/CQLN.15/strength +- type: pyaml.magnet.sextupole + name: SXD5_003 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN05-AR/EM-SX/SCD.13/strength +- type: pyaml.magnet.cfm_magnet + name: SXF5_HCOR_002 + mapping: + - [B2, SXF5_HCOR_002.sextupole] + - [B0, SXF5_HCOR_002.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN05-AR/EM-SX/SCF.14/strength + - AN05-AR/EM-COR/SCF.14-CDLH.07/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF5_QCORROCT_37_QT_001 + mapping: + - [B3, OCTF5_QCORROCT_37_QT_001.octupole] + - [B1, OCTF5_QCORROCT_37_QT_001.quadrupole] + - [A1, OCTF5_QCORROCT_37_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN05-AR/EM-OCT/OC.05/strength + - AN05-AR/EM-COR/OC.05-CQLN.16/strength + - AN05-AR/EM-COR/OC.05-CQLT.06/strength +- type: pyaml.bpm.bpm + name: BPM_041 + x_pos: AN05-AR/DG-EPOS/BPM.08/x_pos + y_pos: AN05-AR/DG-EPOS/BPM.08/y_pos +- type: pyaml.magnet.cfm_magnet + name: SXD5_VCOR_003 + mapping: + - [B2, SXD5_VCOR_003.sextupole] + - [A0, SXD5_VCOR_003.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN05-AR/EM-SX/SCD.15/strength + - AN05-AR/EM-COR/SCD.15-CDLV.07/strength +- type: pyaml.magnet.quadrupole + name: QCORR_050 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN05-AR/EM-COR/CQLN.17/strength +- type: pyaml.magnet.quadrupole + name: QCORR_051 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN05-AR/EM-COR/CQLN.18/strength +- type: pyaml.magnet.sextupole + name: SXD52_001 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN05-AR/EM-SX/SCD.16/strength +- type: pyaml.magnet.cfm_magnet + name: SXF52_HCOR_001 + mapping: + - [B2, SXF52_HCOR_001.sextupole] + - [B0, SXF52_HCOR_001.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN05-AR/EM-SX/SCF.17/strength + - AN05-AR/EM-COR/SCF.17-CDLH.08/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF5_QCORROCT_38_QT_001 + mapping: + - [B3, OCTF5_QCORROCT_38_QT_001.octupole] + - [B1, OCTF5_QCORROCT_38_QT_001.quadrupole] + - [A1, OCTF5_QCORROCT_38_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN05-AR/EM-OCT/OC.06/strength + - AN05-AR/EM-COR/OC.06-CQLN.19/strength + - AN05-AR/EM-COR/OC.06-CQLT.07/strength +- type: pyaml.magnet.cfm_magnet + name: SXD52_VCOR_001 + mapping: + - [B2, SXD52_VCOR_001.sextupole] + - [A0, SXD52_VCOR_001.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN05-AR/EM-SX/SCD.18/strength + - AN05-AR/EM-COR/SCD.18-CDLV.08/strength +- type: pyaml.bpm.bpm + name: BPM_042 + x_pos: AN05-AR/DG-EPOS/BPM.09/x_pos + y_pos: AN05-AR/DG-EPOS/BPM.09/y_pos +- type: pyaml.magnet.quadrupole + name: QCORR_052 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN05-AR/EM-COR/CQLN.20/strength +- type: pyaml.magnet.cfm_magnet + name: SH15_VCOR_001 + mapping: + - [B2, SH15_VCOR_001.sextupole] + - [A0, SH15_VCOR_001.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN05-AR/EM-SX/SHD.04/strength + - AN05-AR/EM-COR/SHD.04-CDLV.09/strength +- type: pyaml.bpm.bpm + name: BPM_043 + x_pos: AN05-AR/DG-EPOS/BPM.10/x_pos + y_pos: AN05-AR/DG-EPOS/BPM.10/y_pos +- type: pyaml.magnet.cfm_magnet + name: SH14_HCOR_001 + mapping: + - [B2, SH14_HCOR_001.sextupole] + - [B0, SH14_HCOR_001.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN05-AR/EM-SX/SHD.05/strength + - AN05-AR/EM-COR/SHD.05-CDLH.09/strength +- type: pyaml.magnet.cfm_magnet + name: OH14_QCORROCT_39_001 + mapping: + - [B3, OH14_QCORROCT_39_001.octupole] + - [B1, OH14_QCORROCT_39_001.quadrupole] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1] + units: [1/m**3, 1/m**2] + physics: + - AN05-AR/EM-OCT/OH.03/strength + - AN05-AR/EM-COR/OH.03-CQLN.21/strength +- type: pyaml.magnet.cfm_magnet + name: SH13_COR_001 + mapping: + - [B2, SH13_COR_001.sextupole] + - [B0, SH13_COR_001.hcorrector] + - [A0, SH13_COR_001.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0, A0] + units: [1/m**2, '1', '1'] + physics: + - AN05-AR/EM-SX/SHF.06/strength + - AN05-AR/EM-COR/SHF.06-CDLH.10/strength + - AN05-AR/EM-COR/SHF.06-CDLV.10/strength +- type: pyaml.magnet.cfm_magnet + name: OH13_QCORROCT_40_QT_001 + mapping: + - [B3, OH13_QCORROCT_40_QT_001.octupole] + - [B1, OH13_QCORROCT_40_QT_001.quadrupole] + - [A1, OH13_QCORROCT_40_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN05-AR/EM-OCT/OH.04/strength + - AN05-AR/EM-COR/OH.04-CQLN.22/strength + - AN05-AR/EM-COR/OH.04-CQLT.08/strength +- type: pyaml.bpm.bpm + name: BPM_044 + x_pos: AN06-SD/DG-EPOS/BPM.01/x_pos + y_pos: AN06-SD/DG-EPOS/BPM.01/y_pos +- type: pyaml.bpm.bpm + name: BPM_045 + x_pos: AN06-SD/DG-EPOS/BPM.02/x_pos + y_pos: AN06-SD/DG-EPOS/BPM.02/y_pos +- type: pyaml.magnet.cfm_magnet + name: OH16_QCORROCT_41_001 + mapping: + - [B3, OH16_QCORROCT_41_001.octupole] + - [B1, OH16_QCORROCT_41_001.quadrupole] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1] + units: [1/m**3, 1/m**2] + physics: + - AN06-SD/EM-OCT/OH.01/strength + - AN06-SD/EM-COR/OH.01-CQLN.01/strength +- type: pyaml.magnet.cfm_magnet + name: SH16_COR_001 + mapping: + - [B2, SH16_COR_001.sextupole] + - [B0, SH16_COR_001.hcorrector] + - [A0, SH16_COR_001.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0, A0] + units: [1/m**2, '1', '1'] + physics: + - AN06-SD/EM-SX/SHD.01/strength + - AN06-SD/EM-COR/SHD.01-CDLH.01/strength + - AN06-SD/EM-COR/SHD.01-CDLV.01/strength +- type: pyaml.magnet.cfm_magnet + name: SH16_COR_002 + mapping: + - [B2, SH16_COR_002.sextupole] + - [B0, SH16_COR_002.hcorrector] + - [A0, SH16_COR_002.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0, A0] + units: [1/m**2, '1', '1'] + physics: + - AN06-SD/EM-SX/SHD.02/strength + - AN06-SD/EM-COR/SHD.02-CDLH.02/strength + - AN06-SD/EM-COR/SHD.02-CDLV.02/strength +- type: pyaml.magnet.cfm_magnet + name: OH16_QCORROCT_42_001 + mapping: + - [B3, OH16_QCORROCT_42_001.octupole] + - [B1, OH16_QCORROCT_42_001.quadrupole] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1] + units: [1/m**3, 1/m**2] + physics: + - AN06-SD/EM-OCT/OH.02/strength + - AN06-SD/EM-COR/OH.02-CQLN.02/strength +- type: pyaml.bpm.bpm + name: BPM_046 + x_pos: AN06-SD/DG-EPOS/BPM.03/x_pos + y_pos: AN06-SD/DG-EPOS/BPM.03/y_pos +- type: pyaml.bpm.bpm + name: BPM_047 + x_pos: AN06-SD/DG-EPOS/BPM.04/x_pos + y_pos: AN06-SD/DG-EPOS/BPM.04/y_pos +- type: pyaml.magnet.cfm_magnet + name: OH13_QCORROCT_43_QT_001 + mapping: + - [B3, OH13_QCORROCT_43_QT_001.octupole] + - [B1, OH13_QCORROCT_43_QT_001.quadrupole] + - [A1, OH13_QCORROCT_43_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN06-AR/EM-OCT/OH.01/strength + - AN06-AR/EM-COR/OH.01-CQLN.01/strength + - AN06-AR/EM-COR/OH.01-CQLT.01/strength +- type: pyaml.magnet.cfm_magnet + name: SH13_COR_002 + mapping: + - [B2, SH13_COR_002.sextupole] + - [B0, SH13_COR_002.hcorrector] + - [A0, SH13_COR_002.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0, A0] + units: [1/m**2, '1', '1'] + physics: + - AN06-AR/EM-SX/SHF.01/strength + - AN06-AR/EM-COR/SHF.01-CDLH.03/strength + - AN06-AR/EM-COR/SHF.01-CDLV.03/strength +- type: pyaml.magnet.cfm_magnet + name: OH14_QCORROCT_44_001 + mapping: + - [B3, OH14_QCORROCT_44_001.octupole] + - [B1, OH14_QCORROCT_44_001.quadrupole] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1] + units: [1/m**3, 1/m**2] + physics: + - AN06-AR/EM-OCT/OH.02/strength + - AN06-AR/EM-COR/OH.02-CQLN.02/strength +- type: pyaml.magnet.cfm_magnet + name: SH14_HCOR_002 + mapping: + - [B2, SH14_HCOR_002.sextupole] + - [B0, SH14_HCOR_002.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN06-AR/EM-SX/SHD.02/strength + - AN06-AR/EM-COR/SHD.02-CDLH.04/strength +- type: pyaml.bpm.bpm + name: BPM_048 + x_pos: AN06-AR/DG-EPOS/BPM.05/x_pos + y_pos: AN06-AR/DG-EPOS/BPM.05/y_pos +- type: pyaml.magnet.cfm_magnet + name: SH15_VCOR_002 + mapping: + - [B2, SH15_VCOR_002.sextupole] + - [A0, SH15_VCOR_002.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN06-AR/EM-SX/SHD.03/strength + - AN06-AR/EM-COR/SHD.03-CDLV.04/strength +- type: pyaml.magnet.quadrupole + name: QCORR_053 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN06-AR/EM-COR/CQLN.03/strength +- type: pyaml.magnet.sextupole + name: SXD52_002 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN06-AR/EM-SX/SCD.01/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF5_QCORROCT_45_QT_001 + mapping: + - [B3, OCTF5_QCORROCT_45_QT_001.octupole] + - [B1, OCTF5_QCORROCT_45_QT_001.quadrupole] + - [A1, OCTF5_QCORROCT_45_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN06-AR/EM-OCT/OC.01/strength + - AN06-AR/EM-COR/OC.01-CQLN.04/strength + - AN06-AR/EM-COR/OC.01-CQLT.02/strength +- type: pyaml.magnet.cfm_magnet + name: SXF52_HCOR_002 + mapping: + - [B2, SXF52_HCOR_002.sextupole] + - [B0, SXF52_HCOR_002.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN06-AR/EM-SX/SCF.02/strength + - AN06-AR/EM-COR/SCF.02-CDLH.05/strength +- type: pyaml.bpm.bpm + name: BPM_049 + x_pos: AN06-AR/DG-EPOS/BPM.06/x_pos + y_pos: AN06-AR/DG-EPOS/BPM.06/y_pos +- type: pyaml.magnet.cfm_magnet + name: SXD52_VCOR_002 + mapping: + - [B2, SXD52_VCOR_002.sextupole] + - [A0, SXD52_VCOR_002.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN06-AR/EM-SX/SCD.03/strength + - AN06-AR/EM-COR/SCD.03-CDLV.05/strength +- type: pyaml.magnet.quadrupole + name: QCORR_054 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN06-AR/EM-COR/CQLN.05/strength +- type: pyaml.magnet.quadrupole + name: QCORR_055 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN06-AR/EM-COR/CQLN.06/strength +- type: pyaml.magnet.sextupole + name: SXD5_004 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN06-AR/EM-SX/SCD.04/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF5_QCORROCT_46_QT_001 + mapping: + - [B3, OCTF5_QCORROCT_46_QT_001.octupole] + - [B1, OCTF5_QCORROCT_46_QT_001.quadrupole] + - [A1, OCTF5_QCORROCT_46_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN06-AR/EM-OCT/OC.02/strength + - AN06-AR/EM-COR/OC.02-CQLN.07/strength + - AN06-AR/EM-COR/OC.02-CQLT.03/strength +- type: pyaml.magnet.cfm_magnet + name: SXF5_HCOR_003 + mapping: + - [B2, SXF5_HCOR_003.sextupole] + - [B0, SXF5_HCOR_003.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN06-AR/EM-SX/SCF.05/strength + - AN06-AR/EM-COR/SCF.05-CDLH.06/strength +- type: pyaml.bpm.bpm + name: BPM_050 + x_pos: AN06-AR/DG-EPOS/BPM.07/x_pos + y_pos: AN06-AR/DG-EPOS/BPM.07/y_pos +- type: pyaml.magnet.cfm_magnet + name: SXD5_VCOR_004 + mapping: + - [B2, SXD5_VCOR_004.sextupole] + - [A0, SXD5_VCOR_004.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN06-AR/EM-SX/SCD.06/strength + - AN06-AR/EM-COR/SCD.06-CDLV.06/strength +- type: pyaml.magnet.quadrupole + name: QCORR_056 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN06-AR/EM-COR/CQLN.08/strength +- type: pyaml.magnet.quadrupole + name: QCORR_057 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN06-AR/EM-COR/CQLN.09/strength +- type: pyaml.magnet.sextupole + name: SXD5_005 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN06-AR/EM-SX/SCD.07/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF5_QCORROCT_47_QT_001 + mapping: + - [B3, OCTF5_QCORROCT_47_QT_001.octupole] + - [B1, OCTF5_QCORROCT_47_QT_001.quadrupole] + - [A1, OCTF5_QCORROCT_47_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN06-AR/EM-OCT/OC.03/strength + - AN06-AR/EM-COR/OC.03-CQLN.10/strength + - AN06-AR/EM-COR/OC.03-CQLT.04/strength +- type: pyaml.magnet.cfm_magnet + name: SXF53_HCOR_003 + mapping: + - [B2, SXF53_HCOR_003.sextupole] + - [B0, SXF53_HCOR_003.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN06-AR/EM-SX/SCF.08/strength + - AN06-AR/EM-COR/SCF.08-CDLH.07/strength +- type: pyaml.bpm.bpm + name: BPM_051 + x_pos: AN06-AR/DG-EPOS/BPM.08/x_pos + y_pos: AN06-AR/DG-EPOS/BPM.08/y_pos +- type: pyaml.magnet.cfm_magnet + name: SXD53_VCOR_002 + mapping: + - [B2, SXD53_VCOR_002.sextupole] + - [A0, SXD53_VCOR_002.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN06-AR/EM-SX/SCD.09/strength + - AN06-AR/EM-COR/SCD.09-CDLV.07/strength +- type: pyaml.magnet.quadrupole + name: QCORR_058 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN06-AR/EM-COR/CQLN.11/strength +- type: pyaml.magnet.quadrupole + name: QCORR_059 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN06-AR/EM-COR/CQLN.12/strength +- type: pyaml.magnet.sextupole + name: SXD53_002 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN06-AR/EM-SX/SCD.10/strength +- type: pyaml.magnet.cfm_magnet + name: SXF53_HCOR_004 + mapping: + - [B2, SXF53_HCOR_004.sextupole] + - [B0, SXF53_HCOR_004.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN06-AR/EM-SX/SCF.11/strength + - AN06-AR/EM-COR/SCF.11-CDLH.08/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF5_QCORROCT_48_QT_001 + mapping: + - [B3, OCTF5_QCORROCT_48_QT_001.octupole] + - [B1, OCTF5_QCORROCT_48_QT_001.quadrupole] + - [A1, OCTF5_QCORROCT_48_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN06-AR/EM-OCT/OC.04/strength + - AN06-AR/EM-COR/OC.04-CQLN.13/strength + - AN06-AR/EM-COR/OC.04-CQLT.05/strength +- type: pyaml.bpm.bpm + name: BPM_052 + x_pos: AN06-AR/DG-EPOS/BPM.09/x_pos + y_pos: AN06-AR/DG-EPOS/BPM.09/y_pos +- type: pyaml.magnet.cfm_magnet + name: SXD5_VCOR_005 + mapping: + - [B2, SXD5_VCOR_005.sextupole] + - [A0, SXD5_VCOR_005.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN06-AR/EM-SX/SCD.12/strength + - AN06-AR/EM-COR/SCD.12-CDLV.08/strength +- type: pyaml.magnet.quadrupole + name: QCORR_060 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN06-AR/EM-COR/CQLN.14/strength +- type: pyaml.magnet.quadrupole + name: QCORR_061 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN06-AR/EM-COR/CQLN.15/strength +- type: pyaml.magnet.sextupole + name: SXD5_006 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN06-AR/EM-SX/SCD.13/strength +- type: pyaml.magnet.cfm_magnet + name: SXF5_HCOR_004 + mapping: + - [B2, SXF5_HCOR_004.sextupole] + - [B0, SXF5_HCOR_004.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN06-AR/EM-SX/SCF.14/strength + - AN06-AR/EM-COR/SCF.14-CDLH.09/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF5_QCORROCT_49_QT_001 + mapping: + - [B3, OCTF5_QCORROCT_49_QT_001.octupole] + - [B1, OCTF5_QCORROCT_49_QT_001.quadrupole] + - [A1, OCTF5_QCORROCT_49_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN06-AR/EM-OCT/OC.05/strength + - AN06-AR/EM-COR/OC.05-CQLN.16/strength + - AN06-AR/EM-COR/OC.05-CQLT.06/strength +- type: pyaml.bpm.bpm + name: BPM_053 + x_pos: AN06-AR/DG-EPOS/BPM.10/x_pos + y_pos: AN06-AR/DG-EPOS/BPM.10/y_pos +- type: pyaml.magnet.cfm_magnet + name: SXD5_VCOR_006 + mapping: + - [B2, SXD5_VCOR_006.sextupole] + - [A0, SXD5_VCOR_006.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN06-AR/EM-SX/SCD.15/strength + - AN06-AR/EM-COR/SCD.15-CDLV.09/strength +- type: pyaml.magnet.quadrupole + name: QCORR_062 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN06-AR/EM-COR/CQLN.17/strength +- type: pyaml.magnet.quadrupole + name: QCORR_063 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN06-AR/EM-COR/CQLN.18/strength +- type: pyaml.magnet.sextupole + name: SXD51_002 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN06-AR/EM-SX/SCD.16/strength +- type: pyaml.magnet.cfm_magnet + name: SXF51_HCOR_002 + mapping: + - [B2, SXF51_HCOR_002.sextupole] + - [B0, SXF51_HCOR_002.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN06-AR/EM-SX/SCF.17/strength + - AN06-AR/EM-COR/SCF.17-CDLH.10/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF5_QCORROCT_50_QT_001 + mapping: + - [B3, OCTF5_QCORROCT_50_QT_001.octupole] + - [B1, OCTF5_QCORROCT_50_QT_001.quadrupole] + - [A1, OCTF5_QCORROCT_50_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN06-AR/EM-OCT/OC.06/strength + - AN06-AR/EM-COR/OC.06-CQLN.19/strength + - AN06-AR/EM-COR/OC.06-CQLT.07/strength +- type: pyaml.magnet.cfm_magnet + name: SXD51_VCOR_002 + mapping: + - [B2, SXD51_VCOR_002.sextupole] + - [A0, SXD51_VCOR_002.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN06-AR/EM-SX/SCD.18/strength + - AN06-AR/EM-COR/SCD.18-CDLV.10/strength +- type: pyaml.bpm.bpm + name: BPM_054 + x_pos: AN06-AR/DG-EPOS/BPM.11/x_pos + y_pos: AN06-AR/DG-EPOS/BPM.11/y_pos +- type: pyaml.magnet.cfm_magnet + name: SH12_COR_003 + mapping: + - [B2, SH12_COR_003.sextupole] + - [B0, SH12_COR_003.hcorrector] + - [A0, SH12_COR_003.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0, A0] + units: [1/m**2, '1', '1'] + physics: + - AN06-AR/EM-SX/SHD.04/strength + - AN06-AR/EM-COR/SHD.04-CDLH.11/strength + - AN06-AR/EM-COR/SHD.04-CDLV.11/strength +- type: pyaml.magnet.quadrupole + name: QCORR_064 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN06-AR/EM-COR/CQLN.20/strength +- type: pyaml.magnet.sextupole + name: SH11_003 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN06-AR/EM-SX/SHD.05/strength +- type: pyaml.magnet.cfm_magnet + name: OH11_QCORROCT_51_001 + mapping: + - [B3, OH11_QCORROCT_51_001.octupole] + - [B1, OH11_QCORROCT_51_001.quadrupole] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1] + units: [1/m**3, 1/m**2] + physics: + - AN06-AR/EM-OCT/OH.03/strength + - AN06-AR/EM-COR/OH.03-CQLN.21/strength +- type: pyaml.bpm.bpm + name: BPM_055 + x_pos: AN06-AR/DG-EPOS/BPM.12/x_pos + y_pos: AN06-AR/DG-EPOS/BPM.12/y_pos +- type: pyaml.magnet.cfm_magnet + name: SH10_COR_003 + mapping: + - [B2, SH10_COR_003.sextupole] + - [B0, SH10_COR_003.hcorrector] + - [A0, SH10_COR_003.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0, A0] + units: [1/m**2, '1', '1'] + physics: + - AN06-AR/EM-SX/SHF.06/strength + - AN06-AR/EM-COR/SHF.06-CDLH.12/strength + - AN06-AR/EM-COR/SHF.06-CDLV.12/strength +- type: pyaml.magnet.cfm_magnet + name: OH10_QCORROCT_52_QT_001 + mapping: + - [B3, OH10_QCORROCT_52_QT_001.octupole] + - [B1, OH10_QCORROCT_52_QT_001.quadrupole] + - [A1, OH10_QCORROCT_52_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN06-AR/EM-OCT/OH.04/strength + - AN06-AR/EM-COR/OH.04-CQLN.22/strength + - AN06-AR/EM-COR/OH.04-CQLT.08/strength +- type: pyaml.bpm.bpm + name: BPM_056 + x_pos: AN07-SD/DG-EPOS/BPM.01/x_pos + y_pos: AN07-SD/DG-EPOS/BPM.01/y_pos +- type: pyaml.bpm.bpm + name: BPM_057 + x_pos: AN07-SD/DG-EPOS/BPM.02/x_pos + y_pos: AN07-SD/DG-EPOS/BPM.02/y_pos +- type: pyaml.magnet.cfm_magnet + name: OH10_QCORROCT_53_QT_001 + mapping: + - [B3, OH10_QCORROCT_53_QT_001.octupole] + - [B1, OH10_QCORROCT_53_QT_001.quadrupole] + - [A1, OH10_QCORROCT_53_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN07-AR/EM-OCT/OH.01/strength + - AN07-AR/EM-COR/OH.01-CQLN.01/strength + - AN07-AR/EM-COR/OH.01-CQLT.01/strength +- type: pyaml.magnet.cfm_magnet + name: SH10_COR_004 + mapping: + - [B2, SH10_COR_004.sextupole] + - [B0, SH10_COR_004.hcorrector] + - [A0, SH10_COR_004.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0, A0] + units: [1/m**2, '1', '1'] + physics: + - AN07-AR/EM-SX/SHF.01/strength + - AN07-AR/EM-COR/SHF.01-CDLH.01/strength + - AN07-AR/EM-COR/SHF.01-CDLV.01/strength +- type: pyaml.bpm.bpm + name: BPM_058 + x_pos: AN07-AR/DG-EPOS/BPM.03/x_pos + y_pos: AN07-AR/DG-EPOS/BPM.03/y_pos +- type: pyaml.magnet.cfm_magnet + name: OH11_QCORROCT_54_001 + mapping: + - [B3, OH11_QCORROCT_54_001.octupole] + - [B1, OH11_QCORROCT_54_001.quadrupole] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1] + units: [1/m**3, 1/m**2] + physics: + - AN07-AR/EM-OCT/OH.02/strength + - AN07-AR/EM-COR/OH.02-CQLN.02/strength +- type: pyaml.magnet.sextupole + name: SH11_004 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN07-AR/EM-SX/SHD.02/strength +- type: pyaml.magnet.quadrupole + name: QCORR_065 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN07-AR/EM-COR/CQLN.03/strength +- type: pyaml.magnet.cfm_magnet + name: SH12_COR_004 + mapping: + - [B2, SH12_COR_004.sextupole] + - [B0, SH12_COR_004.hcorrector] + - [A0, SH12_COR_004.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0, A0] + units: [1/m**2, '1', '1'] + physics: + - AN07-AR/EM-SX/SHD.03/strength + - AN07-AR/EM-COR/SHD.03-CDLH.02/strength + - AN07-AR/EM-COR/SHD.03-CDLV.02/strength +- type: pyaml.magnet.sextupole + name: SXD42_002 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN07-AR/EM-SX/SCD.01/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF4_QCORROCT_55_QT_001 + mapping: + - [B3, OCTF4_QCORROCT_55_QT_001.octupole] + - [B1, OCTF4_QCORROCT_55_QT_001.quadrupole] + - [A1, OCTF4_QCORROCT_55_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN07-AR/EM-OCT/OC.01/strength + - AN07-AR/EM-COR/OC.01-CQLN.04/strength + - AN07-AR/EM-COR/OC.01-CQLT.02/strength +- type: pyaml.magnet.cfm_magnet + name: SXF42_HCOR_002 + mapping: + - [B2, SXF42_HCOR_002.sextupole] + - [B0, SXF42_HCOR_002.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN07-AR/EM-SX/SCF.02/strength + - AN07-AR/EM-COR/SCF.02-CDLH.03/strength +- type: pyaml.bpm.bpm + name: BPM_059 + x_pos: AN07-AR/DG-EPOS/BPM.04/x_pos + y_pos: AN07-AR/DG-EPOS/BPM.04/y_pos +- type: pyaml.magnet.cfm_magnet + name: SXD42_VCOR_002 + mapping: + - [B2, SXD42_VCOR_002.sextupole] + - [A0, SXD42_VCOR_002.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN07-AR/EM-SX/SCD.03/strength + - AN07-AR/EM-COR/SCD.03-CDLV.03/strength +- type: pyaml.magnet.quadrupole + name: QCORR_066 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN07-AR/EM-COR/CQLN.05/strength +- type: pyaml.magnet.quadrupole + name: QCORR_067 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN07-AR/EM-COR/CQLN.06/strength +- type: pyaml.magnet.sextupole + name: SXD4_002 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN07-AR/EM-SX/SCD.04/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF4_QCORROCT_56_QT_001 + mapping: + - [B3, OCTF4_QCORROCT_56_QT_001.octupole] + - [B1, OCTF4_QCORROCT_56_QT_001.quadrupole] + - [A1, OCTF4_QCORROCT_56_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN07-AR/EM-OCT/OC.02/strength + - AN07-AR/EM-COR/OC.02-CQLN.07/strength + - AN07-AR/EM-COR/OC.02-CQLT.03/strength +- type: pyaml.magnet.cfm_magnet + name: SXF4_HCOR_002 + mapping: + - [B2, SXF4_HCOR_002.sextupole] + - [B0, SXF4_HCOR_002.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN07-AR/EM-SX/SCF.05/strength + - AN07-AR/EM-COR/SCF.05-CDLH.04/strength +- type: pyaml.bpm.bpm + name: BPM_060 + x_pos: AN07-AR/DG-EPOS/BPM.05/x_pos + y_pos: AN07-AR/DG-EPOS/BPM.05/y_pos +- type: pyaml.magnet.cfm_magnet + name: SXD4_VCOR_002 + mapping: + - [B2, SXD4_VCOR_002.sextupole] + - [A0, SXD4_VCOR_002.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN07-AR/EM-SX/SCD.06/strength + - AN07-AR/EM-COR/SCD.06-CDLV.04/strength +- type: pyaml.magnet.quadrupole + name: QCORR_068 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN07-AR/EM-COR/CQLN.08/strength +- type: pyaml.magnet.quadrupole + name: QCORR_069 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN07-AR/EM-COR/CQLN.09/strength +- type: pyaml.magnet.sextupole + name: SXD41_002 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN07-AR/EM-SX/SCD.07/strength +- type: pyaml.magnet.cfm_magnet + name: SXF41_HCOR_002 + mapping: + - [B2, SXF41_HCOR_002.sextupole] + - [B0, SXF41_HCOR_002.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN07-AR/EM-SX/SCF.08/strength + - AN07-AR/EM-COR/SCF.08-CDLH.05/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF4_QCORROCT_57_QT_001 + mapping: + - [B3, OCTF4_QCORROCT_57_QT_001.octupole] + - [B1, OCTF4_QCORROCT_57_QT_001.quadrupole] + - [A1, OCTF4_QCORROCT_57_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN07-AR/EM-OCT/OC.03/strength + - AN07-AR/EM-COR/OC.03-CQLN.10/strength + - AN07-AR/EM-COR/OC.03-CQLT.04/strength +- type: pyaml.magnet.cfm_magnet + name: SXD41_VCOR_002 + mapping: + - [B2, SXD41_VCOR_002.sextupole] + - [A0, SXD41_VCOR_002.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN07-AR/EM-SX/SCD.09/strength + - AN07-AR/EM-COR/SCD.09-CDLV.05/strength +- type: pyaml.bpm.bpm + name: BPM_061 + x_pos: AN07-AR/DG-EPOS/BPM.06/x_pos + y_pos: AN07-AR/DG-EPOS/BPM.06/y_pos +- type: pyaml.magnet.cfm_magnet + name: SH9_COR_005 + mapping: + - [B2, SH9_COR_005.sextupole] + - [B0, SH9_COR_005.hcorrector] + - [A0, SH9_COR_005.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0, A0] + units: [1/m**2, '1', '1'] + physics: + - AN07-AR/EM-SX/SHD.04/strength + - AN07-AR/EM-COR/SHD.04-CDLH.06/strength + - AN07-AR/EM-COR/SHD.04-CDLV.06/strength +- type: pyaml.magnet.quadrupole + name: QCORR_070 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN07-AR/EM-COR/CQLN.11/strength +- type: pyaml.magnet.sextupole + name: SH8_005 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN07-AR/EM-SX/SHD.05/strength +- type: pyaml.magnet.quadrupole + name: QCORR_071 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN07-AR/EM-COR/CQLN.12/strength +- type: pyaml.bpm.bpm + name: BPM_062 + x_pos: AN07-AR/DG-EPOS/BPM.07/x_pos + y_pos: AN07-AR/DG-EPOS/BPM.07/y_pos +- type: pyaml.magnet.cfm_magnet + name: SH7_COR_005 + mapping: + - [B2, SH7_COR_005.sextupole] + - [B0, SH7_COR_005.hcorrector] + - [A0, SH7_COR_005.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0, A0] + units: [1/m**2, '1', '1'] + physics: + - AN07-AR/EM-SX/SHF.06/strength + - AN07-AR/EM-COR/SHF.06-CDLH.07/strength + - AN07-AR/EM-COR/SHF.06-CDLV.07/strength +- type: pyaml.magnet.cfm_magnet + name: OH7_QCORROCT_58_QT_001 + mapping: + - [B3, OH7_QCORROCT_58_QT_001.octupole] + - [B1, OH7_QCORROCT_58_QT_001.quadrupole] + - [A1, OH7_QCORROCT_58_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN07-AR/EM-OCT/OH.03/strength + - AN07-AR/EM-COR/OH.03-CQLN.13/strength + - AN07-AR/EM-COR/OH.03-CQLT.05/strength +- type: pyaml.bpm.bpm + name: BPM_063 + x_pos: AN08-SD/DG-EPOS/BPM.01/x_pos + y_pos: AN08-SD/DG-EPOS/BPM.01/y_pos +- type: pyaml.bpm.bpm + name: BPM_064 + x_pos: AN08-SD/DG-EPOS/BPM.02/x_pos + y_pos: AN08-SD/DG-EPOS/BPM.02/y_pos +- type: pyaml.magnet.cfm_magnet + name: OH7_QCORROCT_59_QT_001 + mapping: + - [B3, OH7_QCORROCT_59_QT_001.octupole] + - [B1, OH7_QCORROCT_59_QT_001.quadrupole] + - [A1, OH7_QCORROCT_59_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN08-AR/EM-OCT/OH.01/strength + - AN08-AR/EM-COR/OH.01-CQLN.01/strength + - AN08-AR/EM-COR/OH.01-CQLT.01/strength +- type: pyaml.magnet.cfm_magnet + name: SH7_COR_006 + mapping: + - [B2, SH7_COR_006.sextupole] + - [B0, SH7_COR_006.hcorrector] + - [A0, SH7_COR_006.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0, A0] + units: [1/m**2, '1', '1'] + physics: + - AN08-AR/EM-SX/SHF.01/strength + - AN08-AR/EM-COR/SHF.01-CDLH.01/strength + - AN08-AR/EM-COR/SHF.01-CDLV.01/strength +- type: pyaml.bpm.bpm + name: BPM_065 + x_pos: AN08-AR/DG-EPOS/BPM.03/x_pos + y_pos: AN08-AR/DG-EPOS/BPM.03/y_pos +- type: pyaml.magnet.quadrupole + name: QCORR_072 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN08-AR/EM-COR/CQLN.02/strength +- type: pyaml.magnet.sextupole + name: SH8_006 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN08-AR/EM-SX/SHD.02/strength +- type: pyaml.magnet.quadrupole + name: QCORR_073 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN08-AR/EM-COR/CQLN.03/strength +- type: pyaml.magnet.cfm_magnet + name: SH9_COR_006 + mapping: + - [B2, SH9_COR_006.sextupole] + - [B0, SH9_COR_006.hcorrector] + - [A0, SH9_COR_006.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0, A0] + units: [1/m**2, '1', '1'] + physics: + - AN08-AR/EM-SX/SHD.03/strength + - AN08-AR/EM-COR/SHD.03-CDLH.02/strength + - AN08-AR/EM-COR/SHD.03-CDLV.02/strength +- type: pyaml.magnet.sextupole + name: SXD32_002 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN08-AR/EM-SX/SCD.01/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF3_QCORROCT_60_QT_001 + mapping: + - [B3, OCTF3_QCORROCT_60_QT_001.octupole] + - [B1, OCTF3_QCORROCT_60_QT_001.quadrupole] + - [A1, OCTF3_QCORROCT_60_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN08-AR/EM-OCT/OC.01/strength + - AN08-AR/EM-COR/OC.01-CQLN.04/strength + - AN08-AR/EM-COR/OC.01-CQLT.02/strength +- type: pyaml.magnet.cfm_magnet + name: SXF32_HCOR_002 + mapping: + - [B2, SXF32_HCOR_002.sextupole] + - [B0, SXF32_HCOR_002.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN08-AR/EM-SX/SCF.02/strength + - AN08-AR/EM-COR/SCF.02-CDLH.03/strength +- type: pyaml.bpm.bpm + name: BPM_066 + x_pos: AN08-AR/DG-EPOS/BPM.04/x_pos + y_pos: AN08-AR/DG-EPOS/BPM.04/y_pos +- type: pyaml.magnet.cfm_magnet + name: SXD32_VCOR_002 + mapping: + - [B2, SXD32_VCOR_002.sextupole] + - [A0, SXD32_VCOR_002.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN08-AR/EM-SX/SCD.03/strength + - AN08-AR/EM-COR/SCD.03-CDLV.03/strength +- type: pyaml.magnet.quadrupole + name: QCORR_074 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN08-AR/EM-COR/CQLN.05/strength +- type: pyaml.magnet.quadrupole + name: QCORR_075 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN08-AR/EM-COR/CQLN.06/strength +- type: pyaml.magnet.sextupole + name: SXD3_004 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN08-AR/EM-SX/SCD.04/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF3_QCORROCT_61_QT_001 + mapping: + - [B3, OCTF3_QCORROCT_61_QT_001.octupole] + - [B1, OCTF3_QCORROCT_61_QT_001.quadrupole] + - [A1, OCTF3_QCORROCT_61_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN08-AR/EM-OCT/OC.02/strength + - AN08-AR/EM-COR/OC.02-CQLN.07/strength + - AN08-AR/EM-COR/OC.02-CQLT.03/strength +- type: pyaml.magnet.cfm_magnet + name: SXF3_HCOR_003 + mapping: + - [B2, SXF3_HCOR_003.sextupole] + - [B0, SXF3_HCOR_003.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN08-AR/EM-SX/SCF.05/strength + - AN08-AR/EM-COR/SCF.05-CDLH.04/strength +- type: pyaml.bpm.bpm + name: BPM_067 + x_pos: AN08-AR/DG-EPOS/BPM.05/x_pos + y_pos: AN08-AR/DG-EPOS/BPM.05/y_pos +- type: pyaml.magnet.cfm_magnet + name: SXD3_VCOR_004 + mapping: + - [B2, SXD3_VCOR_004.sextupole] + - [A0, SXD3_VCOR_004.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN08-AR/EM-SX/SCD.06/strength + - AN08-AR/EM-COR/SCD.06-CDLV.04/strength +- type: pyaml.magnet.quadrupole + name: QCORR_076 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN08-AR/EM-COR/CQLN.08/strength +- type: pyaml.magnet.quadrupole + name: QCORR_077 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN08-AR/EM-COR/CQLN.09/strength +- type: pyaml.magnet.sextupole + name: SXD3_005 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN08-AR/EM-SX/SCD.07/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF3_QCORROCT_62_QT_001 + mapping: + - [B3, OCTF3_QCORROCT_62_QT_001.octupole] + - [B1, OCTF3_QCORROCT_62_QT_001.quadrupole] + - [A1, OCTF3_QCORROCT_62_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN08-AR/EM-OCT/OC.03/strength + - AN08-AR/EM-COR/OC.03-CQLN.10/strength + - AN08-AR/EM-COR/OC.03-CQLT.04/strength +- type: pyaml.magnet.cfm_magnet + name: SXF33_HCOR_003 + mapping: + - [B2, SXF33_HCOR_003.sextupole] + - [B0, SXF33_HCOR_003.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN08-AR/EM-SX/SCF.08/strength + - AN08-AR/EM-COR/SCF.08-CDLH.05/strength +- type: pyaml.bpm.bpm + name: BPM_068 + x_pos: AN08-AR/DG-EPOS/BPM.06/x_pos + y_pos: AN08-AR/DG-EPOS/BPM.06/y_pos +- type: pyaml.magnet.cfm_magnet + name: SXD33_VCOR_002 + mapping: + - [B2, SXD33_VCOR_002.sextupole] + - [A0, SXD33_VCOR_002.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN08-AR/EM-SX/SCD.09/strength + - AN08-AR/EM-COR/SCD.09-CDLV.05/strength +- type: pyaml.magnet.quadrupole + name: QCORR_078 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN08-AR/EM-COR/CQLN.11/strength +- type: pyaml.magnet.quadrupole + name: QCORR_079 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN08-AR/EM-COR/CQLN.12/strength +- type: pyaml.magnet.sextupole + name: SXD33_002 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN08-AR/EM-SX/SCD.10/strength +- type: pyaml.magnet.cfm_magnet + name: SXF33_HCOR_004 + mapping: + - [B2, SXF33_HCOR_004.sextupole] + - [B0, SXF33_HCOR_004.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN08-AR/EM-SX/SCF.11/strength + - AN08-AR/EM-COR/SCF.11-CDLH.06/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF3_QCORROCT_63_QT_001 + mapping: + - [B3, OCTF3_QCORROCT_63_QT_001.octupole] + - [B1, OCTF3_QCORROCT_63_QT_001.quadrupole] + - [A1, OCTF3_QCORROCT_63_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN08-AR/EM-OCT/OC.04/strength + - AN08-AR/EM-COR/OC.04-CQLN.13/strength + - AN08-AR/EM-COR/OC.04-CQLT.05/strength +- type: pyaml.bpm.bpm + name: BPM_069 + x_pos: AN08-AR/DG-EPOS/BPM.07/x_pos + y_pos: AN08-AR/DG-EPOS/BPM.07/y_pos +- type: pyaml.magnet.cfm_magnet + name: SXD3_VCOR_005 + mapping: + - [B2, SXD3_VCOR_005.sextupole] + - [A0, SXD3_VCOR_005.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN08-AR/EM-SX/SCD.12/strength + - AN08-AR/EM-COR/SCD.12-CDLV.06/strength +- type: pyaml.magnet.quadrupole + name: QCORR_080 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN08-AR/EM-COR/CQLN.14/strength +- type: pyaml.magnet.quadrupole + name: QCORR_081 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN08-AR/EM-COR/CQLN.15/strength +- type: pyaml.magnet.sextupole + name: SXD3_006 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN08-AR/EM-SX/SCD.13/strength +- type: pyaml.magnet.cfm_magnet + name: SXF3_HCOR_004 + mapping: + - [B2, SXF3_HCOR_004.sextupole] + - [B0, SXF3_HCOR_004.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN08-AR/EM-SX/SCF.14/strength + - AN08-AR/EM-COR/SCF.14-CDLH.07/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF3_QCORROCT_64_QT_001 + mapping: + - [B3, OCTF3_QCORROCT_64_QT_001.octupole] + - [B1, OCTF3_QCORROCT_64_QT_001.quadrupole] + - [A1, OCTF3_QCORROCT_64_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN08-AR/EM-OCT/OC.05/strength + - AN08-AR/EM-COR/OC.05-CQLN.16/strength + - AN08-AR/EM-COR/OC.05-CQLT.06/strength +- type: pyaml.bpm.bpm + name: BPM_070 + x_pos: AN08-AR/DG-EPOS/BPM.08/x_pos + y_pos: AN08-AR/DG-EPOS/BPM.08/y_pos +- type: pyaml.magnet.cfm_magnet + name: SXD3_VCOR_006 + mapping: + - [B2, SXD3_VCOR_006.sextupole] + - [A0, SXD3_VCOR_006.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN08-AR/EM-SX/SCD.15/strength + - AN08-AR/EM-COR/SCD.15-CDLV.07/strength +- type: pyaml.magnet.quadrupole + name: QCORR_082 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN08-AR/EM-COR/CQLN.17/strength +- type: pyaml.magnet.quadrupole + name: QCORR_083 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN08-AR/EM-COR/CQLN.18/strength +- type: pyaml.magnet.sextupole + name: SXD31_002 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN08-AR/EM-SX/SCD.16/strength +- type: pyaml.magnet.cfm_magnet + name: SXF31_HCOR_002 + mapping: + - [B2, SXF31_HCOR_002.sextupole] + - [B0, SXF31_HCOR_002.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN08-AR/EM-SX/SCF.17/strength + - AN08-AR/EM-COR/SCF.17-CDLH.08/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF3_QCORROCT_65_QT_001 + mapping: + - [B3, OCTF3_QCORROCT_65_QT_001.octupole] + - [B1, OCTF3_QCORROCT_65_QT_001.quadrupole] + - [A1, OCTF3_QCORROCT_65_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN08-AR/EM-OCT/OC.06/strength + - AN08-AR/EM-COR/OC.06-CQLN.19/strength + - AN08-AR/EM-COR/OC.06-CQLT.07/strength +- type: pyaml.magnet.cfm_magnet + name: SXD31_VCOR_002 + mapping: + - [B2, SXD31_VCOR_002.sextupole] + - [A0, SXD31_VCOR_002.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN08-AR/EM-SX/SCD.18/strength + - AN08-AR/EM-COR/SCD.18-CDLV.08/strength +- type: pyaml.bpm.bpm + name: BPM_071 + x_pos: AN08-AR/DG-EPOS/BPM.09/x_pos + y_pos: AN08-AR/DG-EPOS/BPM.09/y_pos +- type: pyaml.magnet.cfm_magnet + name: SH9_COR_007 + mapping: + - [B2, SH9_COR_007.sextupole] + - [B0, SH9_COR_007.hcorrector] + - [A0, SH9_COR_007.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0, A0] + units: [1/m**2, '1', '1'] + physics: + - AN08-AR/EM-SX/SHD.04/strength + - AN08-AR/EM-COR/SHD.04-CDLH.09/strength + - AN08-AR/EM-COR/SHD.04-CDLV.09/strength +- type: pyaml.magnet.quadrupole + name: QCORR_084 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN08-AR/EM-COR/CQLN.20/strength +- type: pyaml.magnet.sextupole + name: SH8_007 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN08-AR/EM-SX/SHD.05/strength +- type: pyaml.magnet.quadrupole + name: QCORR_085 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN08-AR/EM-COR/CQLN.21/strength +- type: pyaml.bpm.bpm + name: BPM_072 + x_pos: AN08-AR/DG-EPOS/BPM.10/x_pos + y_pos: AN08-AR/DG-EPOS/BPM.10/y_pos +- type: pyaml.magnet.cfm_magnet + name: SH7_COR_007 + mapping: + - [B2, SH7_COR_007.sextupole] + - [B0, SH7_COR_007.hcorrector] + - [A0, SH7_COR_007.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0, A0] + units: [1/m**2, '1', '1'] + physics: + - AN08-AR/EM-SX/SHF.06/strength + - AN08-AR/EM-COR/SHF.06-CDLH.10/strength + - AN08-AR/EM-COR/SHF.06-CDLV.10/strength +- type: pyaml.magnet.cfm_magnet + name: OH7_QCORROCT_66_QT_001 + mapping: + - [B3, OH7_QCORROCT_66_QT_001.octupole] + - [B1, OH7_QCORROCT_66_QT_001.quadrupole] + - [A1, OH7_QCORROCT_66_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN08-AR/EM-OCT/OH.02/strength + - AN08-AR/EM-COR/OH.02-CQLN.22/strength + - AN08-AR/EM-COR/OH.02-CQLT.08/strength +- type: pyaml.bpm.bpm + name: BPM_073 + x_pos: AN09-SD/DG-EPOS/BPM.01/x_pos + y_pos: AN09-SD/DG-EPOS/BPM.01/y_pos +- type: pyaml.bpm.bpm + name: BPM_074 + x_pos: AN09-SD/DG-EPOS/BPM.02/x_pos + y_pos: AN09-SD/DG-EPOS/BPM.02/y_pos +- type: pyaml.magnet.cfm_magnet + name: OH7_QCORROCT_67_QT_001 + mapping: + - [B3, OH7_QCORROCT_67_QT_001.octupole] + - [B1, OH7_QCORROCT_67_QT_001.quadrupole] + - [A1, OH7_QCORROCT_67_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN09-AR/EM-OCT/OH.01/strength + - AN09-AR/EM-COR/OH.01-CQLN.01/strength + - AN09-AR/EM-COR/OH.01-CQLT.01/strength +- type: pyaml.magnet.cfm_magnet + name: SH7_COR_008 + mapping: + - [B2, SH7_COR_008.sextupole] + - [B0, SH7_COR_008.hcorrector] + - [A0, SH7_COR_008.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0, A0] + units: [1/m**2, '1', '1'] + physics: + - AN09-AR/EM-SX/SHF.01/strength + - AN09-AR/EM-COR/SHF.01-CDLH.01/strength + - AN09-AR/EM-COR/SHF.01-CDLV.01/strength +- type: pyaml.bpm.bpm + name: BPM_075 + x_pos: AN09-AR/DG-EPOS/BPM.03/x_pos + y_pos: AN09-AR/DG-EPOS/BPM.03/y_pos +- type: pyaml.magnet.quadrupole + name: QCORR_086 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN09-AR/EM-COR/CQLN.02/strength +- type: pyaml.magnet.sextupole + name: SH8_008 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN09-AR/EM-SX/SHD.02/strength +- type: pyaml.magnet.quadrupole + name: QCORR_087 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN09-AR/EM-COR/CQLN.03/strength +- type: pyaml.magnet.cfm_magnet + name: SH9_COR_008 + mapping: + - [B2, SH9_COR_008.sextupole] + - [B0, SH9_COR_008.hcorrector] + - [A0, SH9_COR_008.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0, A0] + units: [1/m**2, '1', '1'] + physics: + - AN09-AR/EM-SX/SHD.03/strength + - AN09-AR/EM-COR/SHD.03-CDLH.02/strength + - AN09-AR/EM-COR/SHD.03-CDLV.02/strength +- type: pyaml.magnet.sextupole + name: SXD22_002 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN09-AR/EM-SX/SCD.01/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF2_QCORROCT_68_QT_001 + mapping: + - [B3, OCTF2_QCORROCT_68_QT_001.octupole] + - [B1, OCTF2_QCORROCT_68_QT_001.quadrupole] + - [A1, OCTF2_QCORROCT_68_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN09-AR/EM-OCT/OC.01/strength + - AN09-AR/EM-COR/OC.01-CQLN.04/strength + - AN09-AR/EM-COR/OC.01-CQLT.02/strength +- type: pyaml.magnet.cfm_magnet + name: SXF22_HCOR_002 + mapping: + - [B2, SXF22_HCOR_002.sextupole] + - [B0, SXF22_HCOR_002.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN09-AR/EM-SX/SCF.02/strength + - AN09-AR/EM-COR/SCF.02-CDLH.03/strength +- type: pyaml.bpm.bpm + name: BPM_076 + x_pos: AN09-AR/DG-EPOS/BPM.04/x_pos + y_pos: AN09-AR/DG-EPOS/BPM.04/y_pos +- type: pyaml.magnet.cfm_magnet + name: SXD22_VCOR_002 + mapping: + - [B2, SXD22_VCOR_002.sextupole] + - [A0, SXD22_VCOR_002.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN09-AR/EM-SX/SCD.03/strength + - AN09-AR/EM-COR/SCD.03-CDLV.03/strength +- type: pyaml.magnet.quadrupole + name: QCORR_088 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN09-AR/EM-COR/CQLN.05/strength +- type: pyaml.magnet.quadrupole + name: QCORR_089 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN09-AR/EM-COR/CQLN.06/strength +- type: pyaml.magnet.sextupole + name: SXD2_002 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN09-AR/EM-SX/SCD.04/strength +- type: pyaml.magnet.cfm_magnet + name: SXF2_HCOR_002 + mapping: + - [B2, SXF2_HCOR_002.sextupole] + - [B0, SXF2_HCOR_002.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN09-AR/EM-SX/SCF.05/strength + - AN09-AR/EM-COR/SCF.05-CDLH.04/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF2_QCORROCT_69_QT_001 + mapping: + - [B3, OCTF2_QCORROCT_69_QT_001.octupole] + - [B1, OCTF2_QCORROCT_69_QT_001.quadrupole] + - [A1, OCTF2_QCORROCT_69_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN09-AR/EM-OCT/OC.02/strength + - AN09-AR/EM-COR/OC.02-CQLN.07/strength + - AN09-AR/EM-COR/OC.02-CQLT.03/strength +- type: pyaml.bpm.bpm + name: BPM_077 + x_pos: AN09-AR/DG-EPOS/BPM.05/x_pos + y_pos: AN09-AR/DG-EPOS/BPM.05/y_pos +- type: pyaml.magnet.cfm_magnet + name: SXD2_VCOR_002 + mapping: + - [B2, SXD2_VCOR_002.sextupole] + - [A0, SXD2_VCOR_002.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN09-AR/EM-SX/SCD.06/strength + - AN09-AR/EM-COR/SCD.06-CDLV.04/strength +- type: pyaml.magnet.quadrupole + name: QCORR_090 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN09-AR/EM-COR/CQLN.08/strength +- type: pyaml.magnet.quadrupole + name: QCORR_091 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN09-AR/EM-COR/CQLN.09/strength +- type: pyaml.magnet.sextupole + name: SXD21_002 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN09-AR/EM-SX/SCD.07/strength +- type: pyaml.magnet.cfm_magnet + name: SXF21_HCOR_002 + mapping: + - [B2, SXF21_HCOR_002.sextupole] + - [B0, SXF21_HCOR_002.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN09-AR/EM-SX/SCF.08/strength + - AN09-AR/EM-COR/SCF.08-CDLH.05/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF2_QCORROCT_70_QT_001 + mapping: + - [B3, OCTF2_QCORROCT_70_QT_001.octupole] + - [B1, OCTF2_QCORROCT_70_QT_001.quadrupole] + - [A1, OCTF2_QCORROCT_70_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN09-AR/EM-OCT/OC.03/strength + - AN09-AR/EM-COR/OC.03-CQLN.10/strength + - AN09-AR/EM-COR/OC.03-CQLT.04/strength +- type: pyaml.magnet.cfm_magnet + name: SXD21_VCOR_002 + mapping: + - [B2, SXD21_VCOR_002.sextupole] + - [A0, SXD21_VCOR_002.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN09-AR/EM-SX/SCD.09/strength + - AN09-AR/EM-COR/SCD.09-CDLV.05/strength +- type: pyaml.bpm.bpm + name: BPM_078 + x_pos: AN09-AR/DG-EPOS/BPM.06/x_pos + y_pos: AN09-AR/DG-EPOS/BPM.06/y_pos +- type: pyaml.magnet.cfm_magnet + name: SH6_COR_003 + mapping: + - [B2, SH6_COR_003.sextupole] + - [B0, SH6_COR_003.hcorrector] + - [A0, SH6_COR_003.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0, A0] + units: [1/m**2, '1', '1'] + physics: + - AN09-AR/EM-SX/SHD.04/strength + - AN09-AR/EM-COR/SHD.04-CDLH.06/strength + - AN09-AR/EM-COR/SHD.04-CDLV.06/strength +- type: pyaml.magnet.quadrupole + name: QCORR_092 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN09-AR/EM-COR/CQLN.11/strength +- type: pyaml.magnet.sextupole + name: SH5_003 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN09-AR/EM-SX/SHD.05/strength +- type: pyaml.magnet.cfm_magnet + name: OH5_QCORROCT_71_001 + mapping: + - [B3, OH5_QCORROCT_71_001.octupole] + - [B1, OH5_QCORROCT_71_001.quadrupole] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1] + units: [1/m**3, 1/m**2] + physics: + - AN09-AR/EM-OCT/OH.02/strength + - AN09-AR/EM-COR/OH.02-CQLN.12/strength +- type: pyaml.bpm.bpm + name: BPM_079 + x_pos: AN09-AR/DG-EPOS/BPM.07/x_pos + y_pos: AN09-AR/DG-EPOS/BPM.07/y_pos +- type: pyaml.magnet.cfm_magnet + name: SH4_COR_003 + mapping: + - [B2, SH4_COR_003.sextupole] + - [B0, SH4_COR_003.hcorrector] + - [A0, SH4_COR_003.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0, A0] + units: [1/m**2, '1', '1'] + physics: + - AN09-AR/EM-SX/SHF.06/strength + - AN09-AR/EM-COR/SHF.06-CDLH.07/strength + - AN09-AR/EM-COR/SHF.06-CDLV.07/strength +- type: pyaml.magnet.cfm_magnet + name: OH4_QCORROCT_72_QT_001 + mapping: + - [B3, OH4_QCORROCT_72_QT_001.octupole] + - [B1, OH4_QCORROCT_72_QT_001.quadrupole] + - [A1, OH4_QCORROCT_72_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN09-AR/EM-OCT/OH.03/strength + - AN09-AR/EM-COR/OH.03-CQLN.13/strength + - AN09-AR/EM-COR/OH.03-CQLT.05/strength +- type: pyaml.bpm.bpm + name: BPM_080 + x_pos: AN10-SD/DG-EPOS/BPM.01/x_pos + y_pos: AN10-SD/DG-EPOS/BPM.01/y_pos +- type: pyaml.bpm.bpm + name: BPM_081 + x_pos: AN10-SD/DG-EPOS/BPM.02/x_pos + y_pos: AN10-SD/DG-EPOS/BPM.02/y_pos +- type: pyaml.magnet.cfm_magnet + name: OH4_QCORROCT_73_QT_001 + mapping: + - [B3, OH4_QCORROCT_73_QT_001.octupole] + - [B1, OH4_QCORROCT_73_QT_001.quadrupole] + - [A1, OH4_QCORROCT_73_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN10-AR/EM-OCT/OH.01/strength + - AN10-AR/EM-COR/OH.01-CQLN.01/strength + - AN10-AR/EM-COR/OH.01-CQLT.01/strength +- type: pyaml.magnet.cfm_magnet + name: SH4_COR_004 + mapping: + - [B2, SH4_COR_004.sextupole] + - [B0, SH4_COR_004.hcorrector] + - [A0, SH4_COR_004.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0, A0] + units: [1/m**2, '1', '1'] + physics: + - AN10-AR/EM-SX/SHF.01/strength + - AN10-AR/EM-COR/SHF.01-CDLH.01/strength + - AN10-AR/EM-COR/SHF.01-CDLV.01/strength +- type: pyaml.bpm.bpm + name: BPM_082 + x_pos: AN10-AR/DG-EPOS/BPM.03/x_pos + y_pos: AN10-AR/DG-EPOS/BPM.03/y_pos +- type: pyaml.magnet.cfm_magnet + name: OH5_QCORROCT_74_001 + mapping: + - [B3, OH5_QCORROCT_74_001.octupole] + - [B1, OH5_QCORROCT_74_001.quadrupole] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1] + units: [1/m**3, 1/m**2] + physics: + - AN10-AR/EM-OCT/OH.02/strength + - AN10-AR/EM-COR/OH.02-CQLN.02/strength +- type: pyaml.magnet.sextupole + name: SH5_004 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN10-AR/EM-SX/SHD.02/strength +- type: pyaml.magnet.quadrupole + name: QCORR_093 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN10-AR/EM-COR/CQLN.03/strength +- type: pyaml.magnet.cfm_magnet + name: SH6_COR_004 + mapping: + - [B2, SH6_COR_004.sextupole] + - [B0, SH6_COR_004.hcorrector] + - [A0, SH6_COR_004.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0, A0] + units: [1/m**2, '1', '1'] + physics: + - AN10-AR/EM-SX/SHD.03/strength + - AN10-AR/EM-COR/SHD.03-CDLH.02/strength + - AN10-AR/EM-COR/SHD.03-CDLV.02/strength +- type: pyaml.magnet.sextupole + name: SXD12_002 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN10-AR/EM-SX/SCD.01/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF1_QCORROCT_75_QT_001 + mapping: + - [B3, OCTF1_QCORROCT_75_QT_001.octupole] + - [B1, OCTF1_QCORROCT_75_QT_001.quadrupole] + - [A1, OCTF1_QCORROCT_75_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN10-AR/EM-OCT/OC.01/strength + - AN10-AR/EM-COR/OC.01-CQLN.04/strength + - AN10-AR/EM-COR/OC.01-CQLT.02/strength +- type: pyaml.magnet.cfm_magnet + name: SXF12_HCOR_002 + mapping: + - [B2, SXF12_HCOR_002.sextupole] + - [B0, SXF12_HCOR_002.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN10-AR/EM-SX/SCF.02/strength + - AN10-AR/EM-COR/SCF.02-CDLH.03/strength +- type: pyaml.bpm.bpm + name: BPM_083 + x_pos: AN10-AR/DG-EPOS/BPM.04/x_pos + y_pos: AN10-AR/DG-EPOS/BPM.04/y_pos +- type: pyaml.magnet.cfm_magnet + name: SXD12_VCOR_002 + mapping: + - [B2, SXD12_VCOR_002.sextupole] + - [A0, SXD12_VCOR_002.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN10-AR/EM-SX/SCD.03/strength + - AN10-AR/EM-COR/SCD.03-CDLV.03/strength +- type: pyaml.magnet.quadrupole + name: QCORR_094 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN10-AR/EM-COR/CQLN.05/strength +- type: pyaml.magnet.quadrupole + name: QCORR_095 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN10-AR/EM-COR/CQLN.06/strength +- type: pyaml.magnet.sextupole + name: SXD1_004 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN10-AR/EM-SX/SCD.04/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF1_QCORROCT_76_QT_001 + mapping: + - [B3, OCTF1_QCORROCT_76_QT_001.octupole] + - [B1, OCTF1_QCORROCT_76_QT_001.quadrupole] + - [A1, OCTF1_QCORROCT_76_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN10-AR/EM-OCT/OC.02/strength + - AN10-AR/EM-COR/OC.02-CQLN.07/strength + - AN10-AR/EM-COR/OC.02-CQLT.03/strength +- type: pyaml.magnet.cfm_magnet + name: SXF1_HCOR_003 + mapping: + - [B2, SXF1_HCOR_003.sextupole] + - [B0, SXF1_HCOR_003.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN10-AR/EM-SX/SCF.05/strength + - AN10-AR/EM-COR/SCF.05-CDLH.04/strength +- type: pyaml.bpm.bpm + name: BPM_084 + x_pos: AN10-AR/DG-EPOS/BPM.05/x_pos + y_pos: AN10-AR/DG-EPOS/BPM.05/y_pos +- type: pyaml.magnet.cfm_magnet + name: SXD1_VCOR_004 + mapping: + - [B2, SXD1_VCOR_004.sextupole] + - [A0, SXD1_VCOR_004.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN10-AR/EM-SX/SCD.06/strength + - AN10-AR/EM-COR/SCD.06-CDLV.04/strength +- type: pyaml.magnet.quadrupole + name: QCORR_096 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN10-AR/EM-COR/CQLN.08/strength +- type: pyaml.magnet.quadrupole + name: QCORR_097 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN10-AR/EM-COR/CQLN.09/strength +- type: pyaml.magnet.sextupole + name: SXD1_005 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN10-AR/EM-SX/SCD.07/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF1_QCORROCT_77_QT_001 + mapping: + - [B3, OCTF1_QCORROCT_77_QT_001.octupole] + - [B1, OCTF1_QCORROCT_77_QT_001.quadrupole] + - [A1, OCTF1_QCORROCT_77_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN10-AR/EM-OCT/OC.03/strength + - AN10-AR/EM-COR/OC.03-CQLN.10/strength + - AN10-AR/EM-COR/OC.03-CQLT.04/strength +- type: pyaml.magnet.cfm_magnet + name: SXF13_HCOR_003 + mapping: + - [B2, SXF13_HCOR_003.sextupole] + - [B0, SXF13_HCOR_003.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN10-AR/EM-SX/SCF.08/strength + - AN10-AR/EM-COR/SCF.08-CDLH.05/strength +- type: pyaml.bpm.bpm + name: BPM_085 + x_pos: AN10-AR/DG-EPOS/BPM.06/x_pos + y_pos: AN10-AR/DG-EPOS/BPM.06/y_pos +- type: pyaml.magnet.cfm_magnet + name: SXD13_VCOR_002 + mapping: + - [B2, SXD13_VCOR_002.sextupole] + - [A0, SXD13_VCOR_002.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN10-AR/EM-SX/SCD.09/strength + - AN10-AR/EM-COR/SCD.09-CDLV.05/strength +- type: pyaml.magnet.quadrupole + name: QCORR_098 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN10-AR/EM-COR/CQLN.11/strength +- type: pyaml.magnet.quadrupole + name: QCORR_099 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN10-AR/EM-COR/CQLN.12/strength +- type: pyaml.magnet.sextupole + name: SXD13_002 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN10-AR/EM-SX/SCD.10/strength +- type: pyaml.magnet.cfm_magnet + name: SXF13_HCOR_004 + mapping: + - [B2, SXF13_HCOR_004.sextupole] + - [B0, SXF13_HCOR_004.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN10-AR/EM-SX/SCF.11/strength + - AN10-AR/EM-COR/SCF.11-CDLH.06/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF1_QCORROCT_78_QT_001 + mapping: + - [B3, OCTF1_QCORROCT_78_QT_001.octupole] + - [B1, OCTF1_QCORROCT_78_QT_001.quadrupole] + - [A1, OCTF1_QCORROCT_78_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN10-AR/EM-OCT/OC.04/strength + - AN10-AR/EM-COR/OC.04-CQLN.13/strength + - AN10-AR/EM-COR/OC.04-CQLT.05/strength +- type: pyaml.bpm.bpm + name: BPM_086 + x_pos: AN10-AR/DG-EPOS/BPM.07/x_pos + y_pos: AN10-AR/DG-EPOS/BPM.07/y_pos +- type: pyaml.magnet.cfm_magnet + name: SXD1_VCOR_005 + mapping: + - [B2, SXD1_VCOR_005.sextupole] + - [A0, SXD1_VCOR_005.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN10-AR/EM-SX/SCD.12/strength + - AN10-AR/EM-COR/SCD.12-CDLV.06/strength +- type: pyaml.magnet.quadrupole + name: QCORR_100 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN10-AR/EM-COR/CQLN.14/strength +- type: pyaml.magnet.quadrupole + name: QCORR_101 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN10-AR/EM-COR/CQLN.15/strength +- type: pyaml.magnet.sextupole + name: SXD1_006 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN10-AR/EM-SX/SCD.13/strength +- type: pyaml.magnet.cfm_magnet + name: SXF1_HCOR_004 + mapping: + - [B2, SXF1_HCOR_004.sextupole] + - [B0, SXF1_HCOR_004.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN10-AR/EM-SX/SCF.14/strength + - AN10-AR/EM-COR/SCF.14-CDLH.07/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF1_QCORROCT_79_QT_001 + mapping: + - [B3, OCTF1_QCORROCT_79_QT_001.octupole] + - [B1, OCTF1_QCORROCT_79_QT_001.quadrupole] + - [A1, OCTF1_QCORROCT_79_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN10-AR/EM-OCT/OC.05/strength + - AN10-AR/EM-COR/OC.05-CQLN.16/strength + - AN10-AR/EM-COR/OC.05-CQLT.06/strength +- type: pyaml.bpm.bpm + name: BPM_087 + x_pos: AN10-AR/DG-EPOS/BPM.08/x_pos + y_pos: AN10-AR/DG-EPOS/BPM.08/y_pos +- type: pyaml.magnet.cfm_magnet + name: SXD1_VCOR_006 + mapping: + - [B2, SXD1_VCOR_006.sextupole] + - [A0, SXD1_VCOR_006.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN10-AR/EM-SX/SCD.15/strength + - AN10-AR/EM-COR/SCD.15-CDLV.07/strength +- type: pyaml.magnet.quadrupole + name: QCORR_102 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN10-AR/EM-COR/CQLN.17/strength +- type: pyaml.magnet.quadrupole + name: QCORR_103 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN10-AR/EM-COR/CQLN.18/strength +- type: pyaml.magnet.sextupole + name: SXD11_002 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN10-AR/EM-SX/SCD.16/strength +- type: pyaml.magnet.cfm_magnet + name: SXF11_HCOR_002 + mapping: + - [B2, SXF11_HCOR_002.sextupole] + - [B0, SXF11_HCOR_002.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN10-AR/EM-SX/SCF.17/strength + - AN10-AR/EM-COR/SCF.17-CDLH.08/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF1_QCORROCT_80_QT_001 + mapping: + - [B3, OCTF1_QCORROCT_80_QT_001.octupole] + - [B1, OCTF1_QCORROCT_80_QT_001.quadrupole] + - [A1, OCTF1_QCORROCT_80_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN10-AR/EM-OCT/OC.06/strength + - AN10-AR/EM-COR/OC.06-CQLN.19/strength + - AN10-AR/EM-COR/OC.06-CQLT.07/strength +- type: pyaml.magnet.cfm_magnet + name: SXD11_VCOR_002 + mapping: + - [B2, SXD11_VCOR_002.sextupole] + - [A0, SXD11_VCOR_002.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN10-AR/EM-SX/SCD.18/strength + - AN10-AR/EM-COR/SCD.18-CDLV.08/strength +- type: pyaml.bpm.bpm + name: BPM_088 + x_pos: AN10-AR/DG-EPOS/BPM.09/x_pos + y_pos: AN10-AR/DG-EPOS/BPM.09/y_pos +- type: pyaml.magnet.quadrupole + name: QCORR_104 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN10-AR/EM-COR/CQLN.20/strength +- type: pyaml.magnet.cfm_magnet + name: SH3_VCOR_002 + mapping: + - [B2, SH3_VCOR_002.sextupole] + - [A0, SH3_VCOR_002.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN10-AR/EM-SX/SHD.04/strength + - AN10-AR/EM-COR/SHD.04-CDLV.09/strength +- type: pyaml.bpm.bpm + name: BPM_089 + x_pos: AN10-AR/DG-EPOS/BPM.10/x_pos + y_pos: AN10-AR/DG-EPOS/BPM.10/y_pos +- type: pyaml.magnet.cfm_magnet + name: OH2_QCORROCT_81_001 + mapping: + - [B3, OH2_QCORROCT_81_001.octupole] + - [B1, OH2_QCORROCT_81_001.quadrupole] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1] + units: [1/m**3, 1/m**2] + physics: + - AN10-AR/EM-OCT/OH.03/strength + - AN10-AR/EM-COR/OH.03-CQLN.21/strength +- type: pyaml.magnet.cfm_magnet + name: SH2_HCOR_002 + mapping: + - [B2, SH2_HCOR_002.sextupole] + - [B0, SH2_HCOR_002.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN10-AR/EM-SX/SHD.05/strength + - AN10-AR/EM-COR/SHD.05-CDLH.09/strength +- type: pyaml.magnet.cfm_magnet + name: OH1_QCORROCT_82_QT_001 + mapping: + - [B3, OH1_QCORROCT_82_QT_001.octupole] + - [B1, OH1_QCORROCT_82_QT_001.quadrupole] + - [A1, OH1_QCORROCT_82_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN10-AR/EM-OCT/OH.04/strength + - AN10-AR/EM-COR/OH.04-CQLN.22/strength + - AN10-AR/EM-COR/OH.04-CQLT.08/strength +- type: pyaml.magnet.cfm_magnet + name: SH1_COR_002 + mapping: + - [B2, SH1_COR_002.sextupole] + - [B0, SH1_COR_002.hcorrector] + - [A0, SH1_COR_002.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0, A0] + units: [1/m**2, '1', '1'] + physics: + - AN10-AR/EM-SX/SHF.06/strength + - AN10-AR/EM-COR/SHF.06-CDLH.10/strength + - AN10-AR/EM-COR/SHF.06-CDLV.10/strength +- type: pyaml.bpm.bpm + name: BPM_090 + x_pos: AN11-SD/DG-EPOS/BPM.01/x_pos + y_pos: AN11-SD/DG-EPOS/BPM.01/y_pos +- type: pyaml.bpm.bpm + name: BPM_091 + x_pos: AN11-SD/DG-EPOS/BPM.02/x_pos + y_pos: AN11-SD/DG-EPOS/BPM.02/y_pos +- type: pyaml.magnet.cfm_magnet + name: SH1_COR_003 + mapping: + - [B2, SH1_COR_003.sextupole] + - [B0, SH1_COR_003.hcorrector] + - [A0, SH1_COR_003.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0, A0] + units: [1/m**2, '1', '1'] + physics: + - AN11-AR/EM-SX/SHF.01/strength + - AN11-AR/EM-COR/SHF.01-CDLH.01/strength + - AN11-AR/EM-COR/SHF.01-CDLV.01/strength +- type: pyaml.magnet.cfm_magnet + name: OH1_QCORROCT_83_QT_001 + mapping: + - [B3, OH1_QCORROCT_83_QT_001.octupole] + - [B1, OH1_QCORROCT_83_QT_001.quadrupole] + - [A1, OH1_QCORROCT_83_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN11-AR/EM-OCT/OH.01/strength + - AN11-AR/EM-COR/OH.01-CQLN.01/strength + - AN11-AR/EM-COR/OH.01-CQLT.01/strength +- type: pyaml.magnet.cfm_magnet + name: SH2_HCOR_003 + mapping: + - [B2, SH2_HCOR_003.sextupole] + - [B0, SH2_HCOR_003.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN11-AR/EM-SX/SHD.02/strength + - AN11-AR/EM-COR/SHD.02-CDLH.02/strength +- type: pyaml.magnet.cfm_magnet + name: OH2_QCORROCT_84_001 + mapping: + - [B3, OH2_QCORROCT_84_001.octupole] + - [B1, OH2_QCORROCT_84_001.quadrupole] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1] + units: [1/m**3, 1/m**2] + physics: + - AN11-AR/EM-OCT/OH.02/strength + - AN11-AR/EM-COR/OH.02-CQLN.02/strength +- type: pyaml.bpm.bpm + name: BPM_092 + x_pos: AN11-AR/DG-EPOS/BPM.03/x_pos + y_pos: AN11-AR/DG-EPOS/BPM.03/y_pos +- type: pyaml.magnet.cfm_magnet + name: SH3_VCOR_003 + mapping: + - [B2, SH3_VCOR_003.sextupole] + - [A0, SH3_VCOR_003.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN11-AR/EM-SX/SHD.03/strength + - AN11-AR/EM-COR/SHD.03-CDLV.02/strength +- type: pyaml.magnet.quadrupole + name: QCORR_105 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN11-AR/EM-COR/CQLN.03/strength +- type: pyaml.magnet.sextupole + name: SXD11_003 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN11-AR/EM-SX/SCD.01/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF1_QCORROCT_85_QT_001 + mapping: + - [B3, OCTF1_QCORROCT_85_QT_001.octupole] + - [B1, OCTF1_QCORROCT_85_QT_001.quadrupole] + - [A1, OCTF1_QCORROCT_85_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN11-AR/EM-OCT/OC.01/strength + - AN11-AR/EM-COR/OC.01-CQLN.04/strength + - AN11-AR/EM-COR/OC.01-CQLT.02/strength +- type: pyaml.magnet.cfm_magnet + name: SXF11_HCOR_003 + mapping: + - [B2, SXF11_HCOR_003.sextupole] + - [B0, SXF11_HCOR_003.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN11-AR/EM-SX/SCF.02/strength + - AN11-AR/EM-COR/SCF.02-CDLH.03/strength +- type: pyaml.bpm.bpm + name: BPM_093 + x_pos: AN11-AR/DG-EPOS/BPM.04/x_pos + y_pos: AN11-AR/DG-EPOS/BPM.04/y_pos +- type: pyaml.magnet.cfm_magnet + name: SXD11_VCOR_003 + mapping: + - [B2, SXD11_VCOR_003.sextupole] + - [A0, SXD11_VCOR_003.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN11-AR/EM-SX/SCD.03/strength + - AN11-AR/EM-COR/SCD.03-CDLV.03/strength +- type: pyaml.magnet.quadrupole + name: QCORR_106 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN11-AR/EM-COR/CQLN.05/strength +- type: pyaml.magnet.quadrupole + name: QCORR_107 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN11-AR/EM-COR/CQLN.06/strength +- type: pyaml.magnet.sextupole + name: SXD1_007 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN11-AR/EM-SX/SCD.04/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF1_QCORROCT_86_QT_001 + mapping: + - [B3, OCTF1_QCORROCT_86_QT_001.octupole] + - [B1, OCTF1_QCORROCT_86_QT_001.quadrupole] + - [A1, OCTF1_QCORROCT_86_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN11-AR/EM-OCT/OC.02/strength + - AN11-AR/EM-COR/OC.02-CQLN.07/strength + - AN11-AR/EM-COR/OC.02-CQLT.03/strength +- type: pyaml.magnet.cfm_magnet + name: SXF1_HCOR_005 + mapping: + - [B2, SXF1_HCOR_005.sextupole] + - [B0, SXF1_HCOR_005.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN11-AR/EM-SX/SCF.05/strength + - AN11-AR/EM-COR/SCF.05-CDLH.04/strength +- type: pyaml.bpm.bpm + name: BPM_094 + x_pos: AN11-AR/DG-EPOS/BPM.05/x_pos + y_pos: AN11-AR/DG-EPOS/BPM.05/y_pos +- type: pyaml.magnet.cfm_magnet + name: SXD1_VCOR_007 + mapping: + - [B2, SXD1_VCOR_007.sextupole] + - [A0, SXD1_VCOR_007.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN11-AR/EM-SX/SCD.06/strength + - AN11-AR/EM-COR/SCD.06-CDLV.04/strength +- type: pyaml.magnet.quadrupole + name: QCORR_108 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN11-AR/EM-COR/CQLN.08/strength +- type: pyaml.magnet.quadrupole + name: QCORR_109 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN11-AR/EM-COR/CQLN.09/strength +- type: pyaml.magnet.sextupole + name: SXD1_008 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN11-AR/EM-SX/SCD.07/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF1_QCORROCT_87_QT_001 + mapping: + - [B3, OCTF1_QCORROCT_87_QT_001.octupole] + - [B1, OCTF1_QCORROCT_87_QT_001.quadrupole] + - [A1, OCTF1_QCORROCT_87_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN11-AR/EM-OCT/OC.03/strength + - AN11-AR/EM-COR/OC.03-CQLN.10/strength + - AN11-AR/EM-COR/OC.03-CQLT.04/strength +- type: pyaml.magnet.cfm_magnet + name: SXF13_HCOR_005 + mapping: + - [B2, SXF13_HCOR_005.sextupole] + - [B0, SXF13_HCOR_005.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN11-AR/EM-SX/SCF.08/strength + - AN11-AR/EM-COR/SCF.08-CDLH.05/strength +- type: pyaml.bpm.bpm + name: BPM_095 + x_pos: AN11-AR/DG-EPOS/BPM.06/x_pos + y_pos: AN11-AR/DG-EPOS/BPM.06/y_pos +- type: pyaml.magnet.cfm_magnet + name: SXD13_VCOR_003 + mapping: + - [B2, SXD13_VCOR_003.sextupole] + - [A0, SXD13_VCOR_003.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN11-AR/EM-SX/SCD.09/strength + - AN11-AR/EM-COR/SCD.09-CDLV.05/strength +- type: pyaml.magnet.quadrupole + name: QCORR_110 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN11-AR/EM-COR/CQLN.11/strength +- type: pyaml.magnet.quadrupole + name: QCORR_111 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN11-AR/EM-COR/CQLN.12/strength +- type: pyaml.magnet.sextupole + name: SXD13_003 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN11-AR/EM-SX/SCD.10/strength +- type: pyaml.magnet.cfm_magnet + name: SXF13_HCOR_006 + mapping: + - [B2, SXF13_HCOR_006.sextupole] + - [B0, SXF13_HCOR_006.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN11-AR/EM-SX/SCF.11/strength + - AN11-AR/EM-COR/SCF.11-CDLH.06/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF1_QCORROCT_88_QT_001 + mapping: + - [B3, OCTF1_QCORROCT_88_QT_001.octupole] + - [B1, OCTF1_QCORROCT_88_QT_001.quadrupole] + - [A1, OCTF1_QCORROCT_88_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN11-AR/EM-OCT/OC.04/strength + - AN11-AR/EM-COR/OC.04-CQLN.13/strength + - AN11-AR/EM-COR/OC.04-CQLT.05/strength +- type: pyaml.bpm.bpm + name: BPM_096 + x_pos: AN11-AR/DG-EPOS/BPM.07/x_pos + y_pos: AN11-AR/DG-EPOS/BPM.07/y_pos +- type: pyaml.magnet.cfm_magnet + name: SXD1_VCOR_008 + mapping: + - [B2, SXD1_VCOR_008.sextupole] + - [A0, SXD1_VCOR_008.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN11-AR/EM-SX/SCD.12/strength + - AN11-AR/EM-COR/SCD.12-CDLV.06/strength +- type: pyaml.magnet.quadrupole + name: QCORR_112 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN11-AR/EM-COR/CQLN.14/strength +- type: pyaml.magnet.quadrupole + name: QCORR_113 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN11-AR/EM-COR/CQLN.15/strength +- type: pyaml.magnet.sextupole + name: SXD1_009 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN11-AR/EM-SX/SCD.13/strength +- type: pyaml.magnet.cfm_magnet + name: SXF1_HCOR_006 + mapping: + - [B2, SXF1_HCOR_006.sextupole] + - [B0, SXF1_HCOR_006.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN11-AR/EM-SX/SCF.14/strength + - AN11-AR/EM-COR/SCF.14-CDLH.07/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF1_QCORROCT_89_QT_001 + mapping: + - [B3, OCTF1_QCORROCT_89_QT_001.octupole] + - [B1, OCTF1_QCORROCT_89_QT_001.quadrupole] + - [A1, OCTF1_QCORROCT_89_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN11-AR/EM-OCT/OC.05/strength + - AN11-AR/EM-COR/OC.05-CQLN.16/strength + - AN11-AR/EM-COR/OC.05-CQLT.06/strength +- type: pyaml.bpm.bpm + name: BPM_097 + x_pos: AN11-AR/DG-EPOS/BPM.08/x_pos + y_pos: AN11-AR/DG-EPOS/BPM.08/y_pos +- type: pyaml.magnet.cfm_magnet + name: SXD1_VCOR_009 + mapping: + - [B2, SXD1_VCOR_009.sextupole] + - [A0, SXD1_VCOR_009.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN11-AR/EM-SX/SCD.15/strength + - AN11-AR/EM-COR/SCD.15-CDLV.07/strength +- type: pyaml.magnet.quadrupole + name: QCORR_114 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN11-AR/EM-COR/CQLN.17/strength +- type: pyaml.magnet.quadrupole + name: QCORR_115 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN11-AR/EM-COR/CQLN.18/strength +- type: pyaml.magnet.sextupole + name: SXD12_003 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN11-AR/EM-SX/SCD.16/strength +- type: pyaml.magnet.cfm_magnet + name: SXF12_HCOR_003 + mapping: + - [B2, SXF12_HCOR_003.sextupole] + - [B0, SXF12_HCOR_003.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN11-AR/EM-SX/SCF.17/strength + - AN11-AR/EM-COR/SCF.17-CDLH.08/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF1_QCORROCT_90_QT_001 + mapping: + - [B3, OCTF1_QCORROCT_90_QT_001.octupole] + - [B1, OCTF1_QCORROCT_90_QT_001.quadrupole] + - [A1, OCTF1_QCORROCT_90_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN11-AR/EM-OCT/OC.06/strength + - AN11-AR/EM-COR/OC.06-CQLN.19/strength + - AN11-AR/EM-COR/OC.06-CQLT.07/strength +- type: pyaml.magnet.cfm_magnet + name: SXD12_VCOR_003 + mapping: + - [B2, SXD12_VCOR_003.sextupole] + - [A0, SXD12_VCOR_003.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN11-AR/EM-SX/SCD.18/strength + - AN11-AR/EM-COR/SCD.18-CDLV.08/strength +- type: pyaml.bpm.bpm + name: BPM_098 + x_pos: AN11-AR/DG-EPOS/BPM.09/x_pos + y_pos: AN11-AR/DG-EPOS/BPM.09/y_pos +- type: pyaml.magnet.cfm_magnet + name: SH6_COR_005 + mapping: + - [B2, SH6_COR_005.sextupole] + - [B0, SH6_COR_005.hcorrector] + - [A0, SH6_COR_005.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0, A0] + units: [1/m**2, '1', '1'] + physics: + - AN11-AR/EM-SX/SHD.04/strength + - AN11-AR/EM-COR/SHD.04-CDLH.09/strength + - AN11-AR/EM-COR/SHD.04-CDLV.09/strength +- type: pyaml.magnet.quadrupole + name: QCORR_116 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN11-AR/EM-COR/CQLN.20/strength +- type: pyaml.magnet.sextupole + name: SH5_005 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN11-AR/EM-SX/SHD.05/strength +- type: pyaml.magnet.cfm_magnet + name: OH5_QCORROCT_91_001 + mapping: + - [B3, OH5_QCORROCT_91_001.octupole] + - [B1, OH5_QCORROCT_91_001.quadrupole] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1] + units: [1/m**3, 1/m**2] + physics: + - AN11-AR/EM-OCT/OH.03/strength + - AN11-AR/EM-COR/OH.03-CQLN.21/strength +- type: pyaml.bpm.bpm + name: BPM_099 + x_pos: AN11-AR/DG-EPOS/BPM.10/x_pos + y_pos: AN11-AR/DG-EPOS/BPM.10/y_pos +- type: pyaml.magnet.cfm_magnet + name: SH4_COR_005 + mapping: + - [B2, SH4_COR_005.sextupole] + - [B0, SH4_COR_005.hcorrector] + - [A0, SH4_COR_005.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0, A0] + units: [1/m**2, '1', '1'] + physics: + - AN11-AR/EM-SX/SHF.06/strength + - AN11-AR/EM-COR/SHF.06-CDLH.10/strength + - AN11-AR/EM-COR/SHF.06-CDLV.10/strength +- type: pyaml.magnet.cfm_magnet + name: OH4_QCORROCT_92_QT_001 + mapping: + - [B3, OH4_QCORROCT_92_QT_001.octupole] + - [B1, OH4_QCORROCT_92_QT_001.quadrupole] + - [A1, OH4_QCORROCT_92_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN11-AR/EM-OCT/OH.04/strength + - AN11-AR/EM-COR/OH.04-CQLN.22/strength + - AN11-AR/EM-COR/OH.04-CQLT.08/strength +- type: pyaml.bpm.bpm + name: BPM_100 + x_pos: AN12-SD/DG-EPOS/BPM.01/x_pos + y_pos: AN12-SD/DG-EPOS/BPM.01/y_pos +- type: pyaml.bpm.bpm + name: BPM_101 + x_pos: AN12-SD/DG-EPOS/BPM.02/x_pos + y_pos: AN12-SD/DG-EPOS/BPM.02/y_pos +- type: pyaml.magnet.cfm_magnet + name: OH4_QCORROCT_93_QT_001 + mapping: + - [B3, OH4_QCORROCT_93_QT_001.octupole] + - [B1, OH4_QCORROCT_93_QT_001.quadrupole] + - [A1, OH4_QCORROCT_93_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN12-AR/EM-OCT/OH.01/strength + - AN12-AR/EM-COR/OH.01-CQLN.01/strength + - AN12-AR/EM-COR/OH.01-CQLT.01/strength +- type: pyaml.magnet.cfm_magnet + name: SH4_COR_006 + mapping: + - [B2, SH4_COR_006.sextupole] + - [B0, SH4_COR_006.hcorrector] + - [A0, SH4_COR_006.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0, A0] + units: [1/m**2, '1', '1'] + physics: + - AN12-AR/EM-SX/SHF.01/strength + - AN12-AR/EM-COR/SHF.01-CDLH.01/strength + - AN12-AR/EM-COR/SHF.01-CDLV.01/strength +- type: pyaml.bpm.bpm + name: BPM_102 + x_pos: AN12-AR/DG-EPOS/BPM.03/x_pos + y_pos: AN12-AR/DG-EPOS/BPM.03/y_pos +- type: pyaml.magnet.cfm_magnet + name: OH5_QCORROCT_94_001 + mapping: + - [B3, OH5_QCORROCT_94_001.octupole] + - [B1, OH5_QCORROCT_94_001.quadrupole] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1] + units: [1/m**3, 1/m**2] + physics: + - AN12-AR/EM-OCT/OH.02/strength + - AN12-AR/EM-COR/OH.02-CQLN.02/strength +- type: pyaml.magnet.sextupole + name: SH5_006 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN12-AR/EM-SX/SHD.02/strength +- type: pyaml.magnet.quadrupole + name: QCORR_117 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN12-AR/EM-COR/CQLN.03/strength +- type: pyaml.magnet.cfm_magnet + name: SH6_COR_006 + mapping: + - [B2, SH6_COR_006.sextupole] + - [B0, SH6_COR_006.hcorrector] + - [A0, SH6_COR_006.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0, A0] + units: [1/m**2, '1', '1'] + physics: + - AN12-AR/EM-SX/SHD.03/strength + - AN12-AR/EM-COR/SHD.03-CDLH.02/strength + - AN12-AR/EM-COR/SHD.03-CDLV.02/strength +- type: pyaml.magnet.sextupole + name: SXD21_003 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN12-AR/EM-SX/SCD.01/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF2_QCORROCT_95_QT_001 + mapping: + - [B3, OCTF2_QCORROCT_95_QT_001.octupole] + - [B1, OCTF2_QCORROCT_95_QT_001.quadrupole] + - [A1, OCTF2_QCORROCT_95_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN12-AR/EM-OCT/OC.01/strength + - AN12-AR/EM-COR/OC.01-CQLN.04/strength + - AN12-AR/EM-COR/OC.01-CQLT.02/strength +- type: pyaml.magnet.cfm_magnet + name: SXF21_HCOR_003 + mapping: + - [B2, SXF21_HCOR_003.sextupole] + - [B0, SXF21_HCOR_003.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN12-AR/EM-SX/SCF.02/strength + - AN12-AR/EM-COR/SCF.02-CDLH.03/strength +- type: pyaml.bpm.bpm + name: BPM_103 + x_pos: AN12-AR/DG-EPOS/BPM.04/x_pos + y_pos: AN12-AR/DG-EPOS/BPM.04/y_pos +- type: pyaml.magnet.cfm_magnet + name: SXD21_VCOR_003 + mapping: + - [B2, SXD21_VCOR_003.sextupole] + - [A0, SXD21_VCOR_003.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN12-AR/EM-SX/SCD.03/strength + - AN12-AR/EM-COR/SCD.03-CDLV.03/strength +- type: pyaml.magnet.quadrupole + name: QCORR_118 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN12-AR/EM-COR/CQLN.05/strength +- type: pyaml.magnet.quadrupole + name: QCORR_119 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN12-AR/EM-COR/CQLN.06/strength +- type: pyaml.magnet.sextupole + name: SXD2_003 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN12-AR/EM-SX/SCD.04/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF2_QCORROCT_96_QT_001 + mapping: + - [B3, OCTF2_QCORROCT_96_QT_001.octupole] + - [B1, OCTF2_QCORROCT_96_QT_001.quadrupole] + - [A1, OCTF2_QCORROCT_96_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN12-AR/EM-OCT/OC.02/strength + - AN12-AR/EM-COR/OC.02-CQLN.07/strength + - AN12-AR/EM-COR/OC.02-CQLT.03/strength +- type: pyaml.magnet.cfm_magnet + name: SXF2_HCOR_003 + mapping: + - [B2, SXF2_HCOR_003.sextupole] + - [B0, SXF2_HCOR_003.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN12-AR/EM-SX/SCF.05/strength + - AN12-AR/EM-COR/SCF.05-CDLH.04/strength +- type: pyaml.bpm.bpm + name: BPM_104 + x_pos: AN12-AR/DG-EPOS/BPM.05/x_pos + y_pos: AN12-AR/DG-EPOS/BPM.05/y_pos +- type: pyaml.magnet.cfm_magnet + name: SXD2_VCOR_003 + mapping: + - [B2, SXD2_VCOR_003.sextupole] + - [A0, SXD2_VCOR_003.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN12-AR/EM-SX/SCD.06/strength + - AN12-AR/EM-COR/SCD.06-CDLV.04/strength +- type: pyaml.magnet.quadrupole + name: QCORR_120 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN12-AR/EM-COR/CQLN.08/strength +- type: pyaml.magnet.quadrupole + name: QCORR_121 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN12-AR/EM-COR/CQLN.09/strength +- type: pyaml.magnet.sextupole + name: SXD22_003 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN12-AR/EM-SX/SCD.07/strength +- type: pyaml.magnet.cfm_magnet + name: SXF22_HCOR_003 + mapping: + - [B2, SXF22_HCOR_003.sextupole] + - [B0, SXF22_HCOR_003.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN12-AR/EM-SX/SCF.08/strength + - AN12-AR/EM-COR/SCF.08-CDLH.05/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF2_QCORROCT_97_QT_001 + mapping: + - [B3, OCTF2_QCORROCT_97_QT_001.octupole] + - [B1, OCTF2_QCORROCT_97_QT_001.quadrupole] + - [A1, OCTF2_QCORROCT_97_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN12-AR/EM-OCT/OC.03/strength + - AN12-AR/EM-COR/OC.03-CQLN.10/strength + - AN12-AR/EM-COR/OC.03-CQLT.04/strength +- type: pyaml.magnet.cfm_magnet + name: SXD22_VCOR_003 + mapping: + - [B2, SXD22_VCOR_003.sextupole] + - [A0, SXD22_VCOR_003.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN12-AR/EM-SX/SCD.09/strength + - AN12-AR/EM-COR/SCD.09-CDLV.05/strength +- type: pyaml.bpm.bpm + name: BPM_105 + x_pos: AN12-AR/DG-EPOS/BPM.06/x_pos + y_pos: AN12-AR/DG-EPOS/BPM.06/y_pos +- type: pyaml.magnet.cfm_magnet + name: SH9_COR_009 + mapping: + - [B2, SH9_COR_009.sextupole] + - [B0, SH9_COR_009.hcorrector] + - [A0, SH9_COR_009.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0, A0] + units: [1/m**2, '1', '1'] + physics: + - AN12-AR/EM-SX/SHD.04/strength + - AN12-AR/EM-COR/SHD.04-CDLH.06/strength + - AN12-AR/EM-COR/SHD.04-CDLV.06/strength +- type: pyaml.magnet.quadrupole + name: QCORR_122 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN12-AR/EM-COR/CQLN.11/strength +- type: pyaml.magnet.sextupole + name: SH8_009 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN12-AR/EM-SX/SHD.05/strength +- type: pyaml.magnet.quadrupole + name: QCORR_123 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN12-AR/EM-COR/CQLN.12/strength +- type: pyaml.bpm.bpm + name: BPM_106 + x_pos: AN12-AR/DG-EPOS/BPM.07/x_pos + y_pos: AN12-AR/DG-EPOS/BPM.07/y_pos +- type: pyaml.magnet.cfm_magnet + name: SH7_COR_009 + mapping: + - [B2, SH7_COR_009.sextupole] + - [B0, SH7_COR_009.hcorrector] + - [A0, SH7_COR_009.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0, A0] + units: [1/m**2, '1', '1'] + physics: + - AN12-AR/EM-SX/SHF.06/strength + - AN12-AR/EM-COR/SHF.06-CDLH.07/strength + - AN12-AR/EM-COR/SHF.06-CDLV.07/strength +- type: pyaml.magnet.cfm_magnet + name: OH7_QCORROCT_98_QT_001 + mapping: + - [B3, OH7_QCORROCT_98_QT_001.octupole] + - [B1, OH7_QCORROCT_98_QT_001.quadrupole] + - [A1, OH7_QCORROCT_98_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN12-AR/EM-OCT/OH.03/strength + - AN12-AR/EM-COR/OH.03-CQLN.13/strength + - AN12-AR/EM-COR/OH.03-CQLT.05/strength +- type: pyaml.bpm.bpm + name: BPM_107 + x_pos: AN13-SD/DG-EPOS/BPM.01/x_pos + y_pos: AN13-SD/DG-EPOS/BPM.01/y_pos +- type: pyaml.bpm.bpm + name: BPM_108 + x_pos: AN13-SD/DG-EPOS/BPM.02/x_pos + y_pos: AN13-SD/DG-EPOS/BPM.02/y_pos +- type: pyaml.magnet.cfm_magnet + name: OH7_QCORROCT_99_QT_001 + mapping: + - [B3, OH7_QCORROCT_99_QT_001.octupole] + - [B1, OH7_QCORROCT_99_QT_001.quadrupole] + - [A1, OH7_QCORROCT_99_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN13-AR/EM-OCT/OH.01/strength + - AN13-AR/EM-COR/OH.01-CQLN.01/strength + - AN13-AR/EM-COR/OH.01-CQLT.01/strength +- type: pyaml.magnet.cfm_magnet + name: SH7_COR_010 + mapping: + - [B2, SH7_COR_010.sextupole] + - [B0, SH7_COR_010.hcorrector] + - [A0, SH7_COR_010.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0, A0] + units: [1/m**2, '1', '1'] + physics: + - AN13-AR/EM-SX/SHF.01/strength + - AN13-AR/EM-COR/SHF.01-CDLH.01/strength + - AN13-AR/EM-COR/SHF.01-CDLV.01/strength +- type: pyaml.bpm.bpm + name: BPM_109 + x_pos: AN13-AR/DG-EPOS/BPM.03/x_pos + y_pos: AN13-AR/DG-EPOS/BPM.03/y_pos +- type: pyaml.magnet.quadrupole + name: QCORR_124 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN13-AR/EM-COR/CQLN.02/strength +- type: pyaml.magnet.sextupole + name: SH8_010 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN13-AR/EM-SX/SHD.02/strength +- type: pyaml.magnet.quadrupole + name: QCORR_125 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN13-AR/EM-COR/CQLN.03/strength +- type: pyaml.magnet.cfm_magnet + name: SH9_COR_010 + mapping: + - [B2, SH9_COR_010.sextupole] + - [B0, SH9_COR_010.hcorrector] + - [A0, SH9_COR_010.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0, A0] + units: [1/m**2, '1', '1'] + physics: + - AN13-AR/EM-SX/SHD.03/strength + - AN13-AR/EM-COR/SHD.03-CDLH.02/strength + - AN13-AR/EM-COR/SHD.03-CDLV.02/strength +- type: pyaml.magnet.sextupole + name: SXD31_003 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN13-AR/EM-SX/SCD.01/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF3_QCORROCT_100_QT_001 + mapping: + - [B3, OCTF3_QCORROCT_100_QT_001.octupole] + - [B1, OCTF3_QCORROCT_100_QT_001.quadrupole] + - [A1, OCTF3_QCORROCT_100_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN13-AR/EM-OCT/OC.01/strength + - AN13-AR/EM-COR/OC.01-CQLN.04/strength + - AN13-AR/EM-COR/OC.01-CQLT.02/strength +- type: pyaml.magnet.cfm_magnet + name: SXF31_HCOR_003 + mapping: + - [B2, SXF31_HCOR_003.sextupole] + - [B0, SXF31_HCOR_003.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN13-AR/EM-SX/SCF.02/strength + - AN13-AR/EM-COR/SCF.02-CDLH.03/strength +- type: pyaml.bpm.bpm + name: BPM_110 + x_pos: AN13-AR/DG-EPOS/BPM.04/x_pos + y_pos: AN13-AR/DG-EPOS/BPM.04/y_pos +- type: pyaml.magnet.cfm_magnet + name: SXD31_VCOR_003 + mapping: + - [B2, SXD31_VCOR_003.sextupole] + - [A0, SXD31_VCOR_003.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN13-AR/EM-SX/SCD.03/strength + - AN13-AR/EM-COR/SCD.03-CDLV.03/strength +- type: pyaml.magnet.quadrupole + name: QCORR_126 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN13-AR/EM-COR/CQLN.05/strength +- type: pyaml.magnet.quadrupole + name: QCORR_127 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN13-AR/EM-COR/CQLN.06/strength +- type: pyaml.magnet.sextupole + name: SXD3_007 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN13-AR/EM-SX/SCD.04/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF3_QCORROCT_101_QT_001 + mapping: + - [B3, OCTF3_QCORROCT_101_QT_001.octupole] + - [B1, OCTF3_QCORROCT_101_QT_001.quadrupole] + - [A1, OCTF3_QCORROCT_101_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN13-AR/EM-OCT/OC.02/strength + - AN13-AR/EM-COR/OC.02-CQLN.07/strength + - AN13-AR/EM-COR/OC.02-CQLT.03/strength +- type: pyaml.magnet.cfm_magnet + name: SXF3_HCOR_005 + mapping: + - [B2, SXF3_HCOR_005.sextupole] + - [B0, SXF3_HCOR_005.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN13-AR/EM-SX/SCF.05/strength + - AN13-AR/EM-COR/SCF.05-CDLH.04/strength +- type: pyaml.bpm.bpm + name: BPM_111 + x_pos: AN13-AR/DG-EPOS/BPM.05/x_pos + y_pos: AN13-AR/DG-EPOS/BPM.05/y_pos +- type: pyaml.magnet.cfm_magnet + name: SXD3_VCOR_007 + mapping: + - [B2, SXD3_VCOR_007.sextupole] + - [A0, SXD3_VCOR_007.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN13-AR/EM-SX/SCD.06/strength + - AN13-AR/EM-COR/SCD.06-CDLV.04/strength +- type: pyaml.magnet.quadrupole + name: QCORR_128 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN13-AR/EM-COR/CQLN.08/strength +- type: pyaml.magnet.quadrupole + name: QCORR_129 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN13-AR/EM-COR/CQLN.09/strength +- type: pyaml.magnet.sextupole + name: SXD3_008 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN13-AR/EM-SX/SCD.07/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF3_QCORROCT_102_QT_001 + mapping: + - [B3, OCTF3_QCORROCT_102_QT_001.octupole] + - [B1, OCTF3_QCORROCT_102_QT_001.quadrupole] + - [A1, OCTF3_QCORROCT_102_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN13-AR/EM-OCT/OC.03/strength + - AN13-AR/EM-COR/OC.03-CQLN.10/strength + - AN13-AR/EM-COR/OC.03-CQLT.04/strength +- type: pyaml.magnet.cfm_magnet + name: SXF33_HCOR_005 + mapping: + - [B2, SXF33_HCOR_005.sextupole] + - [B0, SXF33_HCOR_005.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN13-AR/EM-SX/SCF.08/strength + - AN13-AR/EM-COR/SCF.08-CDLH.05/strength +- type: pyaml.bpm.bpm + name: BPM_112 + x_pos: AN13-AR/DG-EPOS/BPM.06/x_pos + y_pos: AN13-AR/DG-EPOS/BPM.06/y_pos +- type: pyaml.magnet.cfm_magnet + name: SXD33_VCOR_003 + mapping: + - [B2, SXD33_VCOR_003.sextupole] + - [A0, SXD33_VCOR_003.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN13-AR/EM-SX/SCD.09/strength + - AN13-AR/EM-COR/SCD.09-CDLV.05/strength +- type: pyaml.magnet.quadrupole + name: QCORR_130 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN13-AR/EM-COR/CQLN.11/strength +- type: pyaml.magnet.quadrupole + name: QCORR_131 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN13-AR/EM-COR/CQLN.12/strength +- type: pyaml.magnet.sextupole + name: SXD33_003 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN13-AR/EM-SX/SCD.10/strength +- type: pyaml.magnet.cfm_magnet + name: SXF33_HCOR_006 + mapping: + - [B2, SXF33_HCOR_006.sextupole] + - [B0, SXF33_HCOR_006.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN13-AR/EM-SX/SCF.11/strength + - AN13-AR/EM-COR/SCF.11-CDLH.06/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF3_QCORROCT_103_QT_001 + mapping: + - [B3, OCTF3_QCORROCT_103_QT_001.octupole] + - [B1, OCTF3_QCORROCT_103_QT_001.quadrupole] + - [A1, OCTF3_QCORROCT_103_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN13-AR/EM-OCT/OC.04/strength + - AN13-AR/EM-COR/OC.04-CQLN.13/strength + - AN13-AR/EM-COR/OC.04-CQLT.05/strength +- type: pyaml.bpm.bpm + name: BPM_113 + x_pos: AN13-AR/DG-EPOS/BPM.07/x_pos + y_pos: AN13-AR/DG-EPOS/BPM.07/y_pos +- type: pyaml.magnet.cfm_magnet + name: SXD3_VCOR_008 + mapping: + - [B2, SXD3_VCOR_008.sextupole] + - [A0, SXD3_VCOR_008.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN13-AR/EM-SX/SCD.12/strength + - AN13-AR/EM-COR/SCD.12-CDLV.06/strength +- type: pyaml.magnet.quadrupole + name: QCORR_132 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN13-AR/EM-COR/CQLN.14/strength +- type: pyaml.magnet.quadrupole + name: QCORR_133 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN13-AR/EM-COR/CQLN.15/strength +- type: pyaml.magnet.sextupole + name: SXD3_009 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN13-AR/EM-SX/SCD.13/strength +- type: pyaml.magnet.cfm_magnet + name: SXF3_HCOR_006 + mapping: + - [B2, SXF3_HCOR_006.sextupole] + - [B0, SXF3_HCOR_006.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN13-AR/EM-SX/SCF.14/strength + - AN13-AR/EM-COR/SCF.14-CDLH.07/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF3_QCORROCT_104_QT_001 + mapping: + - [B3, OCTF3_QCORROCT_104_QT_001.octupole] + - [B1, OCTF3_QCORROCT_104_QT_001.quadrupole] + - [A1, OCTF3_QCORROCT_104_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN13-AR/EM-OCT/OC.05/strength + - AN13-AR/EM-COR/OC.05-CQLN.16/strength + - AN13-AR/EM-COR/OC.05-CQLT.06/strength +- type: pyaml.bpm.bpm + name: BPM_114 + x_pos: AN13-AR/DG-EPOS/BPM.08/x_pos + y_pos: AN13-AR/DG-EPOS/BPM.08/y_pos +- type: pyaml.magnet.cfm_magnet + name: SXD3_VCOR_009 + mapping: + - [B2, SXD3_VCOR_009.sextupole] + - [A0, SXD3_VCOR_009.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN13-AR/EM-SX/SCD.15/strength + - AN13-AR/EM-COR/SCD.15-CDLV.07/strength +- type: pyaml.magnet.quadrupole + name: QCORR_134 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN13-AR/EM-COR/CQLN.17/strength +- type: pyaml.magnet.quadrupole + name: QCORR_135 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN13-AR/EM-COR/CQLN.18/strength +- type: pyaml.magnet.sextupole + name: SXD32_003 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN13-AR/EM-SX/SCD.16/strength +- type: pyaml.magnet.cfm_magnet + name: SXF32_HCOR_003 + mapping: + - [B2, SXF32_HCOR_003.sextupole] + - [B0, SXF32_HCOR_003.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN13-AR/EM-SX/SCF.17/strength + - AN13-AR/EM-COR/SCF.17-CDLH.08/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF3_QCORROCT_105_QT_001 + mapping: + - [B3, OCTF3_QCORROCT_105_QT_001.octupole] + - [B1, OCTF3_QCORROCT_105_QT_001.quadrupole] + - [A1, OCTF3_QCORROCT_105_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN13-AR/EM-OCT/OC.06/strength + - AN13-AR/EM-COR/OC.06-CQLN.19/strength + - AN13-AR/EM-COR/OC.06-CQLT.07/strength +- type: pyaml.magnet.cfm_magnet + name: SXD32_VCOR_003 + mapping: + - [B2, SXD32_VCOR_003.sextupole] + - [A0, SXD32_VCOR_003.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN13-AR/EM-SX/SCD.18/strength + - AN13-AR/EM-COR/SCD.18-CDLV.08/strength +- type: pyaml.bpm.bpm + name: BPM_115 + x_pos: AN13-AR/DG-EPOS/BPM.09/x_pos + y_pos: AN13-AR/DG-EPOS/BPM.09/y_pos +- type: pyaml.magnet.cfm_magnet + name: SH9_COR_011 + mapping: + - [B2, SH9_COR_011.sextupole] + - [B0, SH9_COR_011.hcorrector] + - [A0, SH9_COR_011.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0, A0] + units: [1/m**2, '1', '1'] + physics: + - AN13-AR/EM-SX/SHD.04/strength + - AN13-AR/EM-COR/SHD.04-CDLH.09/strength + - AN13-AR/EM-COR/SHD.04-CDLV.09/strength +- type: pyaml.magnet.quadrupole + name: QCORR_136 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN13-AR/EM-COR/CQLN.20/strength +- type: pyaml.magnet.sextupole + name: SH8_011 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN13-AR/EM-SX/SHD.05/strength +- type: pyaml.magnet.quadrupole + name: QCORR_137 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN13-AR/EM-COR/CQLN.21/strength +- type: pyaml.bpm.bpm + name: BPM_116 + x_pos: AN13-AR/DG-EPOS/BPM.10/x_pos + y_pos: AN13-AR/DG-EPOS/BPM.10/y_pos +- type: pyaml.magnet.cfm_magnet + name: SH7_COR_011 + mapping: + - [B2, SH7_COR_011.sextupole] + - [B0, SH7_COR_011.hcorrector] + - [A0, SH7_COR_011.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0, A0] + units: [1/m**2, '1', '1'] + physics: + - AN13-AR/EM-SX/SHF.06/strength + - AN13-AR/EM-COR/SHF.06-CDLH.10/strength + - AN13-AR/EM-COR/SHF.06-CDLV.10/strength +- type: pyaml.magnet.cfm_magnet + name: OH7_QCORROCT_106_QT_001 + mapping: + - [B3, OH7_QCORROCT_106_QT_001.octupole] + - [B1, OH7_QCORROCT_106_QT_001.quadrupole] + - [A1, OH7_QCORROCT_106_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN13-AR/EM-OCT/OH.02/strength + - AN13-AR/EM-COR/OH.02-CQLN.22/strength + - AN13-AR/EM-COR/OH.02-CQLT.08/strength +- type: pyaml.bpm.bpm + name: BPM_117 + x_pos: AN14-SD/DG-EPOS/BPM.01/x_pos + y_pos: AN14-SD/DG-EPOS/BPM.01/y_pos +- type: pyaml.bpm.bpm + name: BPM_118 + x_pos: AN14-SD/DG-EPOS/BPM.02/x_pos + y_pos: AN14-SD/DG-EPOS/BPM.02/y_pos +- type: pyaml.magnet.cfm_magnet + name: OH7_QCORROCT_107_QT_001 + mapping: + - [B3, OH7_QCORROCT_107_QT_001.octupole] + - [B1, OH7_QCORROCT_107_QT_001.quadrupole] + - [A1, OH7_QCORROCT_107_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN14-AR/EM-OCT/OH.01/strength + - AN14-AR/EM-COR/OH.01-CQLN.01/strength + - AN14-AR/EM-COR/OH.01-CQLT.01/strength +- type: pyaml.magnet.cfm_magnet + name: SH7_COR_012 + mapping: + - [B2, SH7_COR_012.sextupole] + - [B0, SH7_COR_012.hcorrector] + - [A0, SH7_COR_012.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0, A0] + units: [1/m**2, '1', '1'] + physics: + - AN14-AR/EM-SX/SHF.01/strength + - AN14-AR/EM-COR/SHF.01-CDLH.01/strength + - AN14-AR/EM-COR/SHF.01-CDLV.01/strength +- type: pyaml.bpm.bpm + name: BPM_119 + x_pos: AN14-AR/DG-EPOS/BPM.03/x_pos + y_pos: AN14-AR/DG-EPOS/BPM.03/y_pos +- type: pyaml.magnet.quadrupole + name: QCORR_138 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN14-AR/EM-COR/CQLN.02/strength +- type: pyaml.magnet.sextupole + name: SH8_012 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN14-AR/EM-SX/SHD.02/strength +- type: pyaml.magnet.quadrupole + name: QCORR_139 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN14-AR/EM-COR/CQLN.03/strength +- type: pyaml.magnet.cfm_magnet + name: SH9_COR_012 + mapping: + - [B2, SH9_COR_012.sextupole] + - [B0, SH9_COR_012.hcorrector] + - [A0, SH9_COR_012.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0, A0] + units: [1/m**2, '1', '1'] + physics: + - AN14-AR/EM-SX/SHD.03/strength + - AN14-AR/EM-COR/SHD.03-CDLH.02/strength + - AN14-AR/EM-COR/SHD.03-CDLV.02/strength +- type: pyaml.magnet.sextupole + name: SXD41_003 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN14-AR/EM-SX/SCD.01/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF4_QCORROCT_108_QT_001 + mapping: + - [B3, OCTF4_QCORROCT_108_QT_001.octupole] + - [B1, OCTF4_QCORROCT_108_QT_001.quadrupole] + - [A1, OCTF4_QCORROCT_108_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN14-AR/EM-OCT/OC.01/strength + - AN14-AR/EM-COR/OC.01-CQLN.04/strength + - AN14-AR/EM-COR/OC.01-CQLT.02/strength +- type: pyaml.magnet.cfm_magnet + name: SXF41_HCOR_003 + mapping: + - [B2, SXF41_HCOR_003.sextupole] + - [B0, SXF41_HCOR_003.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN14-AR/EM-SX/SCF.02/strength + - AN14-AR/EM-COR/SCF.02-CDLH.03/strength +- type: pyaml.bpm.bpm + name: BPM_120 + x_pos: AN14-AR/DG-EPOS/BPM.04/x_pos + y_pos: AN14-AR/DG-EPOS/BPM.04/y_pos +- type: pyaml.magnet.cfm_magnet + name: SXD41_VCOR_003 + mapping: + - [B2, SXD41_VCOR_003.sextupole] + - [A0, SXD41_VCOR_003.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN14-AR/EM-SX/SCD.03/strength + - AN14-AR/EM-COR/SCD.03-CDLV.03/strength +- type: pyaml.magnet.quadrupole + name: QCORR_140 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN14-AR/EM-COR/CQLN.05/strength +- type: pyaml.magnet.quadrupole + name: QCORR_141 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN14-AR/EM-COR/CQLN.06/strength +- type: pyaml.magnet.sextupole + name: SXD4_003 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN14-AR/EM-SX/SCD.04/strength +- type: pyaml.magnet.cfm_magnet + name: SXF4_HCOR_003 + mapping: + - [B2, SXF4_HCOR_003.sextupole] + - [B0, SXF4_HCOR_003.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN14-AR/EM-SX/SCF.05/strength + - AN14-AR/EM-COR/SCF.05-CDLH.04/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF4_QCORROCT_109_QT_001 + mapping: + - [B3, OCTF4_QCORROCT_109_QT_001.octupole] + - [B1, OCTF4_QCORROCT_109_QT_001.quadrupole] + - [A1, OCTF4_QCORROCT_109_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN14-AR/EM-OCT/OC.02/strength + - AN14-AR/EM-COR/OC.02-CQLN.07/strength + - AN14-AR/EM-COR/OC.02-CQLT.03/strength +- type: pyaml.bpm.bpm + name: BPM_121 + x_pos: AN14-AR/DG-EPOS/BPM.05/x_pos + y_pos: AN14-AR/DG-EPOS/BPM.05/y_pos +- type: pyaml.magnet.cfm_magnet + name: SXD4_VCOR_003 + mapping: + - [B2, SXD4_VCOR_003.sextupole] + - [A0, SXD4_VCOR_003.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN14-AR/EM-SX/SCD.06/strength + - AN14-AR/EM-COR/SCD.06-CDLV.04/strength +- type: pyaml.magnet.quadrupole + name: QCORR_142 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN14-AR/EM-COR/CQLN.08/strength +- type: pyaml.magnet.quadrupole + name: QCORR_143 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN14-AR/EM-COR/CQLN.09/strength +- type: pyaml.magnet.sextupole + name: SXD42_003 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN14-AR/EM-SX/SCD.07/strength +- type: pyaml.magnet.cfm_magnet + name: SXF42_HCOR_003 + mapping: + - [B2, SXF42_HCOR_003.sextupole] + - [B0, SXF42_HCOR_003.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN14-AR/EM-SX/SCF.08/strength + - AN14-AR/EM-COR/SCF.08-CDLH.05/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF4_QCORROCT_110_QT_001 + mapping: + - [B3, OCTF4_QCORROCT_110_QT_001.octupole] + - [B1, OCTF4_QCORROCT_110_QT_001.quadrupole] + - [A1, OCTF4_QCORROCT_110_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN14-AR/EM-OCT/OC.03/strength + - AN14-AR/EM-COR/OC.03-CQLN.10/strength + - AN14-AR/EM-COR/OC.03-CQLT.04/strength +- type: pyaml.magnet.cfm_magnet + name: SXD42_VCOR_003 + mapping: + - [B2, SXD42_VCOR_003.sextupole] + - [A0, SXD42_VCOR_003.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN14-AR/EM-SX/SCD.09/strength + - AN14-AR/EM-COR/SCD.09-CDLV.05/strength +- type: pyaml.bpm.bpm + name: BPM_122 + x_pos: AN14-AR/DG-EPOS/BPM.06/x_pos + y_pos: AN14-AR/DG-EPOS/BPM.06/y_pos +- type: pyaml.magnet.cfm_magnet + name: SH12_COR_005 + mapping: + - [B2, SH12_COR_005.sextupole] + - [B0, SH12_COR_005.hcorrector] + - [A0, SH12_COR_005.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0, A0] + units: [1/m**2, '1', '1'] + physics: + - AN14-AR/EM-SX/SHD.04/strength + - AN14-AR/EM-COR/SHD.04-CDLH.06/strength + - AN14-AR/EM-COR/SHD.04-CDLV.06/strength +- type: pyaml.magnet.quadrupole + name: QCORR_144 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN14-AR/EM-COR/CQLN.11/strength +- type: pyaml.magnet.sextupole + name: SH11_005 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN14-AR/EM-SX/SHD.05/strength +- type: pyaml.magnet.cfm_magnet + name: OH11_QCORROCT_111_001 + mapping: + - [B3, OH11_QCORROCT_111_001.octupole] + - [B1, OH11_QCORROCT_111_001.quadrupole] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1] + units: [1/m**3, 1/m**2] + physics: + - AN14-AR/EM-OCT/OH.02/strength + - AN14-AR/EM-COR/OH.02-CQLN.12/strength +- type: pyaml.bpm.bpm + name: BPM_123 + x_pos: AN14-AR/DG-EPOS/BPM.07/x_pos + y_pos: AN14-AR/DG-EPOS/BPM.07/y_pos +- type: pyaml.magnet.cfm_magnet + name: SH10_COR_005 + mapping: + - [B2, SH10_COR_005.sextupole] + - [B0, SH10_COR_005.hcorrector] + - [A0, SH10_COR_005.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0, A0] + units: [1/m**2, '1', '1'] + physics: + - AN14-AR/EM-SX/SHF.06/strength + - AN14-AR/EM-COR/SHF.06-CDLH.07/strength + - AN14-AR/EM-COR/SHF.06-CDLV.07/strength +- type: pyaml.magnet.cfm_magnet + name: OH10_QCORROCT_112_QT_001 + mapping: + - [B3, OH10_QCORROCT_112_QT_001.octupole] + - [B1, OH10_QCORROCT_112_QT_001.quadrupole] + - [A1, OH10_QCORROCT_112_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN14-AR/EM-OCT/OH.03/strength + - AN14-AR/EM-COR/OH.03-CQLN.13/strength + - AN14-AR/EM-COR/OH.03-CQLT.05/strength +- type: pyaml.bpm.bpm + name: BPM_124 + x_pos: AN15-SD/DG-EPOS/BPM.01/x_pos + y_pos: AN15-SD/DG-EPOS/BPM.01/y_pos +- type: pyaml.bpm.bpm + name: BPM_125 + x_pos: AN15-SD/DG-EPOS/BPM.02/x_pos + y_pos: AN15-SD/DG-EPOS/BPM.02/y_pos +- type: pyaml.magnet.cfm_magnet + name: OH10_QCORROCT_113_QT_001 + mapping: + - [B3, OH10_QCORROCT_113_QT_001.octupole] + - [B1, OH10_QCORROCT_113_QT_001.quadrupole] + - [A1, OH10_QCORROCT_113_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN15-AR/EM-OCT/OH.01/strength + - AN15-AR/EM-COR/OH.01-CQLN.01/strength + - AN15-AR/EM-COR/OH.01-CQLT.01/strength +- type: pyaml.magnet.cfm_magnet + name: SH10_COR_006 + mapping: + - [B2, SH10_COR_006.sextupole] + - [B0, SH10_COR_006.hcorrector] + - [A0, SH10_COR_006.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0, A0] + units: [1/m**2, '1', '1'] + physics: + - AN15-AR/EM-SX/SHF.01/strength + - AN15-AR/EM-COR/SHF.01-CDLH.01/strength + - AN15-AR/EM-COR/SHF.01-CDLV.01/strength +- type: pyaml.bpm.bpm + name: BPM_126 + x_pos: AN15-AR/DG-EPOS/BPM.03/x_pos + y_pos: AN15-AR/DG-EPOS/BPM.03/y_pos +- type: pyaml.magnet.cfm_magnet + name: OH11_QCORROCT_114_001 + mapping: + - [B3, OH11_QCORROCT_114_001.octupole] + - [B1, OH11_QCORROCT_114_001.quadrupole] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1] + units: [1/m**3, 1/m**2] + physics: + - AN15-AR/EM-OCT/OH.02/strength + - AN15-AR/EM-COR/OH.02-CQLN.02/strength +- type: pyaml.magnet.sextupole + name: SH11_006 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN15-AR/EM-SX/SHD.02/strength +- type: pyaml.magnet.quadrupole + name: QCORR_145 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN15-AR/EM-COR/CQLN.03/strength +- type: pyaml.magnet.cfm_magnet + name: SH12_COR_006 + mapping: + - [B2, SH12_COR_006.sextupole] + - [B0, SH12_COR_006.hcorrector] + - [A0, SH12_COR_006.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0, A0] + units: [1/m**2, '1', '1'] + physics: + - AN15-AR/EM-SX/SHD.03/strength + - AN15-AR/EM-COR/SHD.03-CDLH.02/strength + - AN15-AR/EM-COR/SHD.03-CDLV.02/strength +- type: pyaml.magnet.sextupole + name: SXD51_003 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN15-AR/EM-SX/SCD.01/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF5_QCORROCT_115_QT_001 + mapping: + - [B3, OCTF5_QCORROCT_115_QT_001.octupole] + - [B1, OCTF5_QCORROCT_115_QT_001.quadrupole] + - [A1, OCTF5_QCORROCT_115_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN15-AR/EM-OCT/OC.01/strength + - AN15-AR/EM-COR/OC.01-CQLN.04/strength + - AN15-AR/EM-COR/OC.01-CQLT.02/strength +- type: pyaml.magnet.cfm_magnet + name: SXF51_HCOR_003 + mapping: + - [B2, SXF51_HCOR_003.sextupole] + - [B0, SXF51_HCOR_003.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN15-AR/EM-SX/SCF.02/strength + - AN15-AR/EM-COR/SCF.02-CDLH.03/strength +- type: pyaml.bpm.bpm + name: BPM_127 + x_pos: AN15-AR/DG-EPOS/BPM.04/x_pos + y_pos: AN15-AR/DG-EPOS/BPM.04/y_pos +- type: pyaml.magnet.cfm_magnet + name: SXD51_VCOR_003 + mapping: + - [B2, SXD51_VCOR_003.sextupole] + - [A0, SXD51_VCOR_003.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN15-AR/EM-SX/SCD.03/strength + - AN15-AR/EM-COR/SCD.03-CDLV.03/strength +- type: pyaml.magnet.quadrupole + name: QCORR_146 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN15-AR/EM-COR/CQLN.05/strength +- type: pyaml.magnet.quadrupole + name: QCORR_147 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN15-AR/EM-COR/CQLN.06/strength +- type: pyaml.magnet.sextupole + name: SXD5_007 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN15-AR/EM-SX/SCD.04/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF5_QCORROCT_116_QT_001 + mapping: + - [B3, OCTF5_QCORROCT_116_QT_001.octupole] + - [B1, OCTF5_QCORROCT_116_QT_001.quadrupole] + - [A1, OCTF5_QCORROCT_116_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN15-AR/EM-OCT/OC.02/strength + - AN15-AR/EM-COR/OC.02-CQLN.07/strength + - AN15-AR/EM-COR/OC.02-CQLT.03/strength +- type: pyaml.magnet.cfm_magnet + name: SXF5_HCOR_005 + mapping: + - [B2, SXF5_HCOR_005.sextupole] + - [B0, SXF5_HCOR_005.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN15-AR/EM-SX/SCF.05/strength + - AN15-AR/EM-COR/SCF.05-CDLH.04/strength +- type: pyaml.bpm.bpm + name: BPM_128 + x_pos: AN15-AR/DG-EPOS/BPM.05/x_pos + y_pos: AN15-AR/DG-EPOS/BPM.05/y_pos +- type: pyaml.magnet.cfm_magnet + name: SXD5_VCOR_007 + mapping: + - [B2, SXD5_VCOR_007.sextupole] + - [A0, SXD5_VCOR_007.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN15-AR/EM-SX/SCD.06/strength + - AN15-AR/EM-COR/SCD.06-CDLV.04/strength +- type: pyaml.magnet.quadrupole + name: QCORR_148 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN15-AR/EM-COR/CQLN.08/strength +- type: pyaml.magnet.quadrupole + name: QCORR_149 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN15-AR/EM-COR/CQLN.09/strength +- type: pyaml.magnet.sextupole + name: SXD5_008 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN15-AR/EM-SX/SCD.07/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF5_QCORROCT_117_QT_001 + mapping: + - [B3, OCTF5_QCORROCT_117_QT_001.octupole] + - [B1, OCTF5_QCORROCT_117_QT_001.quadrupole] + - [A1, OCTF5_QCORROCT_117_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN15-AR/EM-OCT/OC.03/strength + - AN15-AR/EM-COR/OC.03-CQLN.10/strength + - AN15-AR/EM-COR/OC.03-CQLT.04/strength +- type: pyaml.magnet.cfm_magnet + name: SXF53_HCOR_005 + mapping: + - [B2, SXF53_HCOR_005.sextupole] + - [B0, SXF53_HCOR_005.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN15-AR/EM-SX/SCF.08/strength + - AN15-AR/EM-COR/SCF.08-CDLH.05/strength +- type: pyaml.bpm.bpm + name: BPM_129 + x_pos: AN15-AR/DG-EPOS/BPM.06/x_pos + y_pos: AN15-AR/DG-EPOS/BPM.06/y_pos +- type: pyaml.magnet.cfm_magnet + name: SXD53_VCOR_003 + mapping: + - [B2, SXD53_VCOR_003.sextupole] + - [A0, SXD53_VCOR_003.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN15-AR/EM-SX/SCD.09/strength + - AN15-AR/EM-COR/SCD.09-CDLV.05/strength +- type: pyaml.magnet.quadrupole + name: QCORR_150 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN15-AR/EM-COR/CQLN.11/strength +- type: pyaml.magnet.quadrupole + name: QCORR_151 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN15-AR/EM-COR/CQLN.12/strength +- type: pyaml.magnet.sextupole + name: SXD53_003 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN15-AR/EM-SX/SCD.10/strength +- type: pyaml.magnet.cfm_magnet + name: SXF53_HCOR_006 + mapping: + - [B2, SXF53_HCOR_006.sextupole] + - [B0, SXF53_HCOR_006.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN15-AR/EM-SX/SCF.11/strength + - AN15-AR/EM-COR/SCF.11-CDLH.06/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF5_QCORROCT_118_QT_001 + mapping: + - [B3, OCTF5_QCORROCT_118_QT_001.octupole] + - [B1, OCTF5_QCORROCT_118_QT_001.quadrupole] + - [A1, OCTF5_QCORROCT_118_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN15-AR/EM-OCT/OC.04/strength + - AN15-AR/EM-COR/OC.04-CQLN.13/strength + - AN15-AR/EM-COR/OC.04-CQLT.05/strength +- type: pyaml.bpm.bpm + name: BPM_130 + x_pos: AN15-AR/DG-EPOS/BPM.07/x_pos + y_pos: AN15-AR/DG-EPOS/BPM.07/y_pos +- type: pyaml.magnet.cfm_magnet + name: SXD5_VCOR_008 + mapping: + - [B2, SXD5_VCOR_008.sextupole] + - [A0, SXD5_VCOR_008.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN15-AR/EM-SX/SCD.12/strength + - AN15-AR/EM-COR/SCD.12-CDLV.06/strength +- type: pyaml.magnet.quadrupole + name: QCORR_152 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN15-AR/EM-COR/CQLN.14/strength +- type: pyaml.magnet.quadrupole + name: QCORR_153 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN15-AR/EM-COR/CQLN.15/strength +- type: pyaml.magnet.sextupole + name: SXD5_009 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN15-AR/EM-SX/SCD.13/strength +- type: pyaml.magnet.cfm_magnet + name: SXF5_HCOR_006 + mapping: + - [B2, SXF5_HCOR_006.sextupole] + - [B0, SXF5_HCOR_006.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN15-AR/EM-SX/SCF.14/strength + - AN15-AR/EM-COR/SCF.14-CDLH.07/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF5_QCORROCT_119_QT_001 + mapping: + - [B3, OCTF5_QCORROCT_119_QT_001.octupole] + - [B1, OCTF5_QCORROCT_119_QT_001.quadrupole] + - [A1, OCTF5_QCORROCT_119_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN15-AR/EM-OCT/OC.05/strength + - AN15-AR/EM-COR/OC.05-CQLN.16/strength + - AN15-AR/EM-COR/OC.05-CQLT.06/strength +- type: pyaml.bpm.bpm + name: BPM_131 + x_pos: AN15-AR/DG-EPOS/BPM.08/x_pos + y_pos: AN15-AR/DG-EPOS/BPM.08/y_pos +- type: pyaml.magnet.cfm_magnet + name: SXD5_VCOR_009 + mapping: + - [B2, SXD5_VCOR_009.sextupole] + - [A0, SXD5_VCOR_009.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN15-AR/EM-SX/SCD.15/strength + - AN15-AR/EM-COR/SCD.15-CDLV.07/strength +- type: pyaml.magnet.quadrupole + name: QCORR_154 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN15-AR/EM-COR/CQLN.17/strength +- type: pyaml.magnet.quadrupole + name: QCORR_155 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN15-AR/EM-COR/CQLN.18/strength +- type: pyaml.magnet.sextupole + name: SXD52_003 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN15-AR/EM-SX/SCD.16/strength +- type: pyaml.magnet.cfm_magnet + name: SXF52_HCOR_003 + mapping: + - [B2, SXF52_HCOR_003.sextupole] + - [B0, SXF52_HCOR_003.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN15-AR/EM-SX/SCF.17/strength + - AN15-AR/EM-COR/SCF.17-CDLH.08/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF5_QCORROCT_120_QT_001 + mapping: + - [B3, OCTF5_QCORROCT_120_QT_001.octupole] + - [B1, OCTF5_QCORROCT_120_QT_001.quadrupole] + - [A1, OCTF5_QCORROCT_120_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN15-AR/EM-OCT/OC.06/strength + - AN15-AR/EM-COR/OC.06-CQLN.19/strength + - AN15-AR/EM-COR/OC.06-CQLT.07/strength +- type: pyaml.magnet.cfm_magnet + name: SXD52_VCOR_003 + mapping: + - [B2, SXD52_VCOR_003.sextupole] + - [A0, SXD52_VCOR_003.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN15-AR/EM-SX/SCD.18/strength + - AN15-AR/EM-COR/SCD.18-CDLV.08/strength +- type: pyaml.bpm.bpm + name: BPM_132 + x_pos: AN15-AR/DG-EPOS/BPM.09/x_pos + y_pos: AN15-AR/DG-EPOS/BPM.09/y_pos +- type: pyaml.magnet.quadrupole + name: QCORR_156 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN15-AR/EM-COR/CQLN.20/strength +- type: pyaml.magnet.cfm_magnet + name: SH15_VCOR_003 + mapping: + - [B2, SH15_VCOR_003.sextupole] + - [A0, SH15_VCOR_003.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN15-AR/EM-SX/SHD.04/strength + - AN15-AR/EM-COR/SHD.04-CDLV.09/strength +- type: pyaml.bpm.bpm + name: BPM_133 + x_pos: AN15-AR/DG-EPOS/BPM.10/x_pos + y_pos: AN15-AR/DG-EPOS/BPM.10/y_pos +- type: pyaml.magnet.cfm_magnet + name: SH14_HCOR_003 + mapping: + - [B2, SH14_HCOR_003.sextupole] + - [B0, SH14_HCOR_003.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN15-AR/EM-SX/SHD.05/strength + - AN15-AR/EM-COR/SHD.05-CDLH.09/strength +- type: pyaml.magnet.cfm_magnet + name: OH141_QCORROCT_121_001 + mapping: + - [B3, OH141_QCORROCT_121_001.octupole] + - [B1, OH141_QCORROCT_121_001.quadrupole] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1] + units: [1/m**3, 1/m**2] + physics: + - AN15-AR/EM-OCT/OH.03/strength + - AN15-AR/EM-COR/OH.03-CQLN.21/strength +- type: pyaml.magnet.cfm_magnet + name: SH13_COR_003 + mapping: + - [B2, SH13_COR_003.sextupole] + - [B0, SH13_COR_003.hcorrector] + - [A0, SH13_COR_003.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0, A0] + units: [1/m**2, '1', '1'] + physics: + - AN15-AR/EM-SX/SHF.06/strength + - AN15-AR/EM-COR/SHF.06-CDLH.10/strength + - AN15-AR/EM-COR/SHF.06-CDLV.10/strength +- type: pyaml.magnet.cfm_magnet + name: OH131_QCORROCT_122_001 + mapping: + - [B3, OH131_QCORROCT_122_001.octupole] + - [B1, OH131_QCORROCT_122_001.quadrupole] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1] + units: [1/m**3, 1/m**2] + physics: + - AN15-AR/EM-OCT/OH.04/strength + - AN15-AR/EM-COR/OH.04-CQLN.22/strength +- type: pyaml.bpm.bpm + name: BPM_134 + x_pos: AN16-SD/DG-EPOS/BPM.01/x_pos + y_pos: AN16-SD/DG-EPOS/BPM.01/y_pos +- type: pyaml.bpm.bpm + name: BPM_135 + x_pos: AN16-SD/DG-EPOS/BPM.02/x_pos + y_pos: AN16-SD/DG-EPOS/BPM.02/y_pos +- type: pyaml.magnet.cfm_magnet + name: OH16_QCORROCT_123_001 + mapping: + - [B3, OH16_QCORROCT_123_001.octupole] + - [B1, OH16_QCORROCT_123_001.quadrupole] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1] + units: [1/m**3, 1/m**2] + physics: + - AN16-SD/EM-OCT/OH.01/strength + - AN16-SD/EM-COR/OH.01-CQLN.01/strength +- type: pyaml.magnet.cfm_magnet + name: SH16_COR_003 + mapping: + - [B2, SH16_COR_003.sextupole] + - [B0, SH16_COR_003.hcorrector] + - [A0, SH16_COR_003.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0, A0] + units: [1/m**2, '1', '1'] + physics: + - AN16-SD/EM-SX/SHD.01/strength + - AN16-SD/EM-COR/SHD.01-CDLH.01/strength + - AN16-SD/EM-COR/SHD.01-CDLV.01/strength +- type: pyaml.magnet.cfm_magnet + name: SH16_COR_004 + mapping: + - [B2, SH16_COR_004.sextupole] + - [B0, SH16_COR_004.hcorrector] + - [A0, SH16_COR_004.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0, A0] + units: [1/m**2, '1', '1'] + physics: + - AN16-SD/EM-SX/SHD.02/strength + - AN16-SD/EM-COR/SHD.02-CDLH.02/strength + - AN16-SD/EM-COR/SHD.02-CDLV.02/strength +- type: pyaml.magnet.cfm_magnet + name: OH16_QCORROCT_124_001 + mapping: + - [B3, OH16_QCORROCT_124_001.octupole] + - [B1, OH16_QCORROCT_124_001.quadrupole] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1] + units: [1/m**3, 1/m**2] + physics: + - AN16-SD/EM-OCT/OH.02/strength + - AN16-SD/EM-COR/OH.02-CQLN.02/strength +- type: pyaml.bpm.bpm + name: BPM_136 + x_pos: AN16-SD/DG-EPOS/BPM.03/x_pos + y_pos: AN16-SD/DG-EPOS/BPM.03/y_pos +- type: pyaml.bpm.bpm + name: BPM_137 + x_pos: AN16-SD/DG-EPOS/BPM.04/x_pos + y_pos: AN16-SD/DG-EPOS/BPM.04/y_pos +- type: pyaml.magnet.cfm_magnet + name: OH132_QCORROCT_125_001 + mapping: + - [B3, OH132_QCORROCT_125_001.octupole] + - [B1, OH132_QCORROCT_125_001.quadrupole] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1] + units: [1/m**3, 1/m**2] + physics: + - AN16-AR/EM-OCT/OH.01/strength + - AN16-AR/EM-COR/OH.01-CQLN.01/strength +- type: pyaml.magnet.cfm_magnet + name: SH13_COR_004 + mapping: + - [B2, SH13_COR_004.sextupole] + - [B0, SH13_COR_004.hcorrector] + - [A0, SH13_COR_004.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0, A0] + units: [1/m**2, '1', '1'] + physics: + - AN16-AR/EM-SX/SHF.01/strength + - AN16-AR/EM-COR/SHF.01-CDLH.03/strength + - AN16-AR/EM-COR/SHF.01-CDLV.03/strength +- type: pyaml.magnet.cfm_magnet + name: OH142_QCORROCT_126_001 + mapping: + - [B3, OH142_QCORROCT_126_001.octupole] + - [B1, OH142_QCORROCT_126_001.quadrupole] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1] + units: [1/m**3, 1/m**2] + physics: + - AN16-AR/EM-OCT/OH.02/strength + - AN16-AR/EM-COR/OH.02-CQLN.02/strength +- type: pyaml.magnet.cfm_magnet + name: SH14_HCOR_004 + mapping: + - [B2, SH14_HCOR_004.sextupole] + - [B0, SH14_HCOR_004.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN16-AR/EM-SX/SHD.02/strength + - AN16-AR/EM-COR/SHD.02-CDLH.04/strength +- type: pyaml.bpm.bpm + name: BPM_138 + x_pos: AN16-AR/DG-EPOS/BPM.05/x_pos + y_pos: AN16-AR/DG-EPOS/BPM.05/y_pos +- type: pyaml.magnet.cfm_magnet + name: SH15_VCOR_004 + mapping: + - [B2, SH15_VCOR_004.sextupole] + - [A0, SH15_VCOR_004.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN16-AR/EM-SX/SHD.03/strength + - AN16-AR/EM-COR/SHD.03-CDLV.04/strength +- type: pyaml.magnet.quadrupole + name: QCORR_157 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN16-AR/EM-COR/CQLN.03/strength +- type: pyaml.magnet.sextupole + name: SXD52_004 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN16-AR/EM-SX/SCD.01/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF5_QCORROCT_127_QT_001 + mapping: + - [B3, OCTF5_QCORROCT_127_QT_001.octupole] + - [B1, OCTF5_QCORROCT_127_QT_001.quadrupole] + - [A1, OCTF5_QCORROCT_127_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN16-AR/EM-OCT/OC.01/strength + - AN16-AR/EM-COR/OC.01-CQLN.04/strength + - AN16-AR/EM-COR/OC.01-CQLT.01/strength +- type: pyaml.magnet.cfm_magnet + name: SXF52_HCOR_004 + mapping: + - [B2, SXF52_HCOR_004.sextupole] + - [B0, SXF52_HCOR_004.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN16-AR/EM-SX/SCF.02/strength + - AN16-AR/EM-COR/SCF.02-CDLH.05/strength +- type: pyaml.bpm.bpm + name: BPM_139 + x_pos: AN16-AR/DG-EPOS/BPM.06/x_pos + y_pos: AN16-AR/DG-EPOS/BPM.06/y_pos +- type: pyaml.magnet.cfm_magnet + name: SXD52_VCOR_004 + mapping: + - [B2, SXD52_VCOR_004.sextupole] + - [A0, SXD52_VCOR_004.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN16-AR/EM-SX/SCD.03/strength + - AN16-AR/EM-COR/SCD.03-CDLV.05/strength +- type: pyaml.magnet.quadrupole + name: QCORR_158 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN16-AR/EM-COR/CQLN.05/strength +- type: pyaml.magnet.quadrupole + name: QCORR_159 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN16-AR/EM-COR/CQLN.06/strength +- type: pyaml.magnet.sextupole + name: SXD5_010 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN16-AR/EM-SX/SCD.04/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF5_QCORROCT_128_QT_001 + mapping: + - [B3, OCTF5_QCORROCT_128_QT_001.octupole] + - [B1, OCTF5_QCORROCT_128_QT_001.quadrupole] + - [A1, OCTF5_QCORROCT_128_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN16-AR/EM-OCT/OC.02/strength + - AN16-AR/EM-COR/OC.02-CQLN.07/strength + - AN16-AR/EM-COR/OC.02-CQLT.02/strength +- type: pyaml.magnet.cfm_magnet + name: SXF5_HCOR_007 + mapping: + - [B2, SXF5_HCOR_007.sextupole] + - [B0, SXF5_HCOR_007.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN16-AR/EM-SX/SCF.05/strength + - AN16-AR/EM-COR/SCF.05-CDLH.06/strength +- type: pyaml.bpm.bpm + name: BPM_140 + x_pos: AN16-AR/DG-EPOS/BPM.07/x_pos + y_pos: AN16-AR/DG-EPOS/BPM.07/y_pos +- type: pyaml.magnet.cfm_magnet + name: SXD5_VCOR_010 + mapping: + - [B2, SXD5_VCOR_010.sextupole] + - [A0, SXD5_VCOR_010.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN16-AR/EM-SX/SCD.06/strength + - AN16-AR/EM-COR/SCD.06-CDLV.06/strength +- type: pyaml.magnet.quadrupole + name: QCORR_160 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN16-AR/EM-COR/CQLN.08/strength +- type: pyaml.magnet.quadrupole + name: QCORR_161 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN16-AR/EM-COR/CQLN.09/strength +- type: pyaml.magnet.sextupole + name: SXD5_011 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN16-AR/EM-SX/SCD.07/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF5_QCORROCT_129_QT_001 + mapping: + - [B3, OCTF5_QCORROCT_129_QT_001.octupole] + - [B1, OCTF5_QCORROCT_129_QT_001.quadrupole] + - [A1, OCTF5_QCORROCT_129_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN16-AR/EM-OCT/OC.03/strength + - AN16-AR/EM-COR/OC.03-CQLN.10/strength + - AN16-AR/EM-COR/OC.03-CQLT.03/strength +- type: pyaml.magnet.cfm_magnet + name: SXF53_HCOR_007 + mapping: + - [B2, SXF53_HCOR_007.sextupole] + - [B0, SXF53_HCOR_007.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN16-AR/EM-SX/SCF.08/strength + - AN16-AR/EM-COR/SCF.08-CDLH.07/strength +- type: pyaml.bpm.bpm + name: BPM_141 + x_pos: AN16-AR/DG-EPOS/BPM.08/x_pos + y_pos: AN16-AR/DG-EPOS/BPM.08/y_pos +- type: pyaml.magnet.cfm_magnet + name: SXD53_VCOR_004 + mapping: + - [B2, SXD53_VCOR_004.sextupole] + - [A0, SXD53_VCOR_004.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN16-AR/EM-SX/SCD.09/strength + - AN16-AR/EM-COR/SCD.09-CDLV.07/strength +- type: pyaml.magnet.quadrupole + name: QCORR_162 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN16-AR/EM-COR/CQLN.11/strength +- type: pyaml.magnet.quadrupole + name: QCORR_163 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN16-AR/EM-COR/CQLN.12/strength +- type: pyaml.magnet.sextupole + name: SXD53_004 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN16-AR/EM-SX/SCD.10/strength +- type: pyaml.magnet.cfm_magnet + name: SXF53_HCOR_008 + mapping: + - [B2, SXF53_HCOR_008.sextupole] + - [B0, SXF53_HCOR_008.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN16-AR/EM-SX/SCF.11/strength + - AN16-AR/EM-COR/SCF.11-CDLH.08/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF5_QCORROCT_130_QT_001 + mapping: + - [B3, OCTF5_QCORROCT_130_QT_001.octupole] + - [B1, OCTF5_QCORROCT_130_QT_001.quadrupole] + - [A1, OCTF5_QCORROCT_130_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN16-AR/EM-OCT/OC.04/strength + - AN16-AR/EM-COR/OC.04-CQLN.13/strength + - AN16-AR/EM-COR/OC.04-CQLT.04/strength +- type: pyaml.bpm.bpm + name: BPM_142 + x_pos: AN16-AR/DG-EPOS/BPM.09/x_pos + y_pos: AN16-AR/DG-EPOS/BPM.09/y_pos +- type: pyaml.magnet.cfm_magnet + name: SXD5_VCOR_011 + mapping: + - [B2, SXD5_VCOR_011.sextupole] + - [A0, SXD5_VCOR_011.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN16-AR/EM-SX/SCD.12/strength + - AN16-AR/EM-COR/SCD.12-CDLV.08/strength +- type: pyaml.magnet.quadrupole + name: QCORR_164 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN16-AR/EM-COR/CQLN.14/strength +- type: pyaml.magnet.quadrupole + name: QCORR_165 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN16-AR/EM-COR/CQLN.15/strength +- type: pyaml.magnet.sextupole + name: SXD5_012 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN16-AR/EM-SX/SCD.13/strength +- type: pyaml.magnet.cfm_magnet + name: SXF5_HCOR_008 + mapping: + - [B2, SXF5_HCOR_008.sextupole] + - [B0, SXF5_HCOR_008.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN16-AR/EM-SX/SCF.14/strength + - AN16-AR/EM-COR/SCF.14-CDLH.09/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF5_QCORROCT_131_QT_001 + mapping: + - [B3, OCTF5_QCORROCT_131_QT_001.octupole] + - [B1, OCTF5_QCORROCT_131_QT_001.quadrupole] + - [A1, OCTF5_QCORROCT_131_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN16-AR/EM-OCT/OC.05/strength + - AN16-AR/EM-COR/OC.05-CQLN.16/strength + - AN16-AR/EM-COR/OC.05-CQLT.05/strength +- type: pyaml.bpm.bpm + name: BPM_143 + x_pos: AN16-AR/DG-EPOS/BPM.10/x_pos + y_pos: AN16-AR/DG-EPOS/BPM.10/y_pos +- type: pyaml.magnet.cfm_magnet + name: SXD5_VCOR_012 + mapping: + - [B2, SXD5_VCOR_012.sextupole] + - [A0, SXD5_VCOR_012.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN16-AR/EM-SX/SCD.15/strength + - AN16-AR/EM-COR/SCD.15-CDLV.09/strength +- type: pyaml.magnet.quadrupole + name: QCORR_166 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN16-AR/EM-COR/CQLN.17/strength +- type: pyaml.magnet.quadrupole + name: QCORR_167 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN16-AR/EM-COR/CQLN.18/strength +- type: pyaml.magnet.sextupole + name: SXD51_004 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN16-AR/EM-SX/SCD.16/strength +- type: pyaml.magnet.cfm_magnet + name: SXF51_HCOR_004 + mapping: + - [B2, SXF51_HCOR_004.sextupole] + - [B0, SXF51_HCOR_004.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN16-AR/EM-SX/SCF.17/strength + - AN16-AR/EM-COR/SCF.17-CDLH.10/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF5_QCORROCT_132_QT_001 + mapping: + - [B3, OCTF5_QCORROCT_132_QT_001.octupole] + - [B1, OCTF5_QCORROCT_132_QT_001.quadrupole] + - [A1, OCTF5_QCORROCT_132_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN16-AR/EM-OCT/OC.06/strength + - AN16-AR/EM-COR/OC.06-CQLN.19/strength + - AN16-AR/EM-COR/OC.06-CQLT.06/strength +- type: pyaml.magnet.cfm_magnet + name: SXD51_VCOR_004 + mapping: + - [B2, SXD51_VCOR_004.sextupole] + - [A0, SXD51_VCOR_004.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN16-AR/EM-SX/SCD.18/strength + - AN16-AR/EM-COR/SCD.18-CDLV.10/strength +- type: pyaml.bpm.bpm + name: BPM_144 + x_pos: AN16-AR/DG-EPOS/BPM.11/x_pos + y_pos: AN16-AR/DG-EPOS/BPM.11/y_pos +- type: pyaml.magnet.cfm_magnet + name: SH12_COR_007 + mapping: + - [B2, SH12_COR_007.sextupole] + - [B0, SH12_COR_007.hcorrector] + - [A0, SH12_COR_007.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0, A0] + units: [1/m**2, '1', '1'] + physics: + - AN16-AR/EM-SX/SHD.04/strength + - AN16-AR/EM-COR/SHD.04-CDLH.11/strength + - AN16-AR/EM-COR/SHD.04-CDLV.11/strength +- type: pyaml.magnet.quadrupole + name: QCORR_168 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN16-AR/EM-COR/CQLN.20/strength +- type: pyaml.magnet.sextupole + name: SH11_007 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN16-AR/EM-SX/SHD.05/strength +- type: pyaml.magnet.cfm_magnet + name: OH11_QCORROCT_133_001 + mapping: + - [B3, OH11_QCORROCT_133_001.octupole] + - [B1, OH11_QCORROCT_133_001.quadrupole] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1] + units: [1/m**3, 1/m**2] + physics: + - AN16-AR/EM-OCT/OH.03/strength + - AN16-AR/EM-COR/OH.03-CQLN.21/strength +- type: pyaml.bpm.bpm + name: BPM_145 + x_pos: AN16-AR/DG-EPOS/BPM.12/x_pos + y_pos: AN16-AR/DG-EPOS/BPM.12/y_pos +- type: pyaml.magnet.cfm_magnet + name: SH10_COR_007 + mapping: + - [B2, SH10_COR_007.sextupole] + - [B0, SH10_COR_007.hcorrector] + - [A0, SH10_COR_007.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0, A0] + units: [1/m**2, '1', '1'] + physics: + - AN16-AR/EM-SX/SHF.06/strength + - AN16-AR/EM-COR/SHF.06-CDLH.12/strength + - AN16-AR/EM-COR/SHF.06-CDLV.12/strength +- type: pyaml.magnet.cfm_magnet + name: OH10_QCORROCT_134_QT_001 + mapping: + - [B3, OH10_QCORROCT_134_QT_001.octupole] + - [B1, OH10_QCORROCT_134_QT_001.quadrupole] + - [A1, OH10_QCORROCT_134_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN16-AR/EM-OCT/OH.04/strength + - AN16-AR/EM-COR/OH.04-CQLN.22/strength + - AN16-AR/EM-COR/OH.04-CQLT.07/strength +- type: pyaml.bpm.bpm + name: BPM_146 + x_pos: AN17-SD/DG-EPOS/BPM.01/x_pos + y_pos: AN17-SD/DG-EPOS/BPM.01/y_pos +- type: pyaml.bpm.bpm + name: BPM_147 + x_pos: AN17-SD/DG-EPOS/BPM.02/x_pos + y_pos: AN17-SD/DG-EPOS/BPM.02/y_pos +- type: pyaml.magnet.cfm_magnet + name: OH10_QCORROCT_135_QT_001 + mapping: + - [B3, OH10_QCORROCT_135_QT_001.octupole] + - [B1, OH10_QCORROCT_135_QT_001.quadrupole] + - [A1, OH10_QCORROCT_135_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN17-AR/EM-OCT/OH.01/strength + - AN17-AR/EM-COR/OH.01-CQLN.01/strength + - AN17-AR/EM-COR/OH.01-CQLT.01/strength +- type: pyaml.magnet.cfm_magnet + name: SH10_COR_008 + mapping: + - [B2, SH10_COR_008.sextupole] + - [B0, SH10_COR_008.hcorrector] + - [A0, SH10_COR_008.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0, A0] + units: [1/m**2, '1', '1'] + physics: + - AN17-AR/EM-SX/SHF.01/strength + - AN17-AR/EM-COR/SHF.01-CDLH.01/strength + - AN17-AR/EM-COR/SHF.01-CDLV.01/strength +- type: pyaml.bpm.bpm + name: BPM_148 + x_pos: AN17-AR/DG-EPOS/BPM.03/x_pos + y_pos: AN17-AR/DG-EPOS/BPM.03/y_pos +- type: pyaml.magnet.cfm_magnet + name: OH11_QCORROCT_136_001 + mapping: + - [B3, OH11_QCORROCT_136_001.octupole] + - [B1, OH11_QCORROCT_136_001.quadrupole] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1] + units: [1/m**3, 1/m**2] + physics: + - AN17-AR/EM-OCT/OH.02/strength + - AN17-AR/EM-COR/OH.02-CQLN.02/strength +- type: pyaml.magnet.sextupole + name: SH11_008 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN17-AR/EM-SX/SHD.02/strength +- type: pyaml.magnet.quadrupole + name: QCORR_169 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN17-AR/EM-COR/CQLN.03/strength +- type: pyaml.magnet.cfm_magnet + name: SH12_COR_008 + mapping: + - [B2, SH12_COR_008.sextupole] + - [B0, SH12_COR_008.hcorrector] + - [A0, SH12_COR_008.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0, A0] + units: [1/m**2, '1', '1'] + physics: + - AN17-AR/EM-SX/SHD.03/strength + - AN17-AR/EM-COR/SHD.03-CDLH.02/strength + - AN17-AR/EM-COR/SHD.03-CDLV.02/strength +- type: pyaml.magnet.sextupole + name: SXD42_004 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN17-AR/EM-SX/SCD.01/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF4_QCORROCT_137_QT_001 + mapping: + - [B3, OCTF4_QCORROCT_137_QT_001.octupole] + - [B1, OCTF4_QCORROCT_137_QT_001.quadrupole] + - [A1, OCTF4_QCORROCT_137_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN17-AR/EM-OCT/OC.01/strength + - AN17-AR/EM-COR/OC.01-CQLN.04/strength + - AN17-AR/EM-COR/OC.01-CQLT.02/strength +- type: pyaml.magnet.cfm_magnet + name: SXF42_HCOR_004 + mapping: + - [B2, SXF42_HCOR_004.sextupole] + - [B0, SXF42_HCOR_004.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN17-AR/EM-SX/SCF.02/strength + - AN17-AR/EM-COR/SCF.02-CDLH.03/strength +- type: pyaml.bpm.bpm + name: BPM_149 + x_pos: AN17-AR/DG-EPOS/BPM.04/x_pos + y_pos: AN17-AR/DG-EPOS/BPM.04/y_pos +- type: pyaml.magnet.cfm_magnet + name: SXD42_VCOR_004 + mapping: + - [B2, SXD42_VCOR_004.sextupole] + - [A0, SXD42_VCOR_004.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN17-AR/EM-SX/SCD.03/strength + - AN17-AR/EM-COR/SCD.03-CDLV.03/strength +- type: pyaml.magnet.quadrupole + name: QCORR_170 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN17-AR/EM-COR/CQLN.05/strength +- type: pyaml.magnet.quadrupole + name: QCORR_171 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN17-AR/EM-COR/CQLN.06/strength +- type: pyaml.magnet.sextupole + name: SXD4_004 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN17-AR/EM-SX/SCD.04/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF4_QCORROCT_138_QT_001 + mapping: + - [B3, OCTF4_QCORROCT_138_QT_001.octupole] + - [B1, OCTF4_QCORROCT_138_QT_001.quadrupole] + - [A1, OCTF4_QCORROCT_138_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN17-AR/EM-OCT/OC.02/strength + - AN17-AR/EM-COR/OC.02-CQLN.07/strength + - AN17-AR/EM-COR/OC.02-CQLT.03/strength +- type: pyaml.magnet.cfm_magnet + name: SXF4_HCOR_004 + mapping: + - [B2, SXF4_HCOR_004.sextupole] + - [B0, SXF4_HCOR_004.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN17-AR/EM-SX/SCF.05/strength + - AN17-AR/EM-COR/SCF.05-CDLH.04/strength +- type: pyaml.bpm.bpm + name: BPM_150 + x_pos: AN17-AR/DG-EPOS/BPM.05/x_pos + y_pos: AN17-AR/DG-EPOS/BPM.05/y_pos +- type: pyaml.magnet.cfm_magnet + name: SXD4_VCOR_004 + mapping: + - [B2, SXD4_VCOR_004.sextupole] + - [A0, SXD4_VCOR_004.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN17-AR/EM-SX/SCD.06/strength + - AN17-AR/EM-COR/SCD.06-CDLV.04/strength +- type: pyaml.magnet.quadrupole + name: QCORR_172 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN17-AR/EM-COR/CQLN.08/strength +- type: pyaml.magnet.quadrupole + name: QCORR_173 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN17-AR/EM-COR/CQLN.09/strength +- type: pyaml.magnet.sextupole + name: SXD41_004 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN17-AR/EM-SX/SCD.07/strength +- type: pyaml.magnet.cfm_magnet + name: SXF41_HCOR_004 + mapping: + - [B2, SXF41_HCOR_004.sextupole] + - [B0, SXF41_HCOR_004.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN17-AR/EM-SX/SCF.08/strength + - AN17-AR/EM-COR/SCF.08-CDLH.05/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF4_QCORROCT_139_QT_001 + mapping: + - [B3, OCTF4_QCORROCT_139_QT_001.octupole] + - [B1, OCTF4_QCORROCT_139_QT_001.quadrupole] + - [A1, OCTF4_QCORROCT_139_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN17-AR/EM-OCT/OC.03/strength + - AN17-AR/EM-COR/OC.03-CQLN.10/strength + - AN17-AR/EM-COR/OC.03-CQLT.04/strength +- type: pyaml.magnet.cfm_magnet + name: SXD41_VCOR_004 + mapping: + - [B2, SXD41_VCOR_004.sextupole] + - [A0, SXD41_VCOR_004.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN17-AR/EM-SX/SCD.09/strength + - AN17-AR/EM-COR/SCD.09-CDLV.05/strength +- type: pyaml.bpm.bpm + name: BPM_151 + x_pos: AN17-AR/DG-EPOS/BPM.06/x_pos + y_pos: AN17-AR/DG-EPOS/BPM.06/y_pos +- type: pyaml.magnet.cfm_magnet + name: SH9_COR_013 + mapping: + - [B2, SH9_COR_013.sextupole] + - [B0, SH9_COR_013.hcorrector] + - [A0, SH9_COR_013.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0, A0] + units: [1/m**2, '1', '1'] + physics: + - AN17-AR/EM-SX/SHD.04/strength + - AN17-AR/EM-COR/SHD.04-CDLH.06/strength + - AN17-AR/EM-COR/SHD.04-CDLV.06/strength +- type: pyaml.magnet.quadrupole + name: QCORR_174 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN17-AR/EM-COR/CQLN.11/strength +- type: pyaml.magnet.sextupole + name: SH8_013 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN17-AR/EM-SX/SHD.05/strength +- type: pyaml.magnet.quadrupole + name: QCORR_175 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN17-AR/EM-COR/CQLN.12/strength +- type: pyaml.bpm.bpm + name: BPM_152 + x_pos: AN17-AR/DG-EPOS/BPM.07/x_pos + y_pos: AN17-AR/DG-EPOS/BPM.07/y_pos +- type: pyaml.magnet.cfm_magnet + name: SH7_COR_013 + mapping: + - [B2, SH7_COR_013.sextupole] + - [B0, SH7_COR_013.hcorrector] + - [A0, SH7_COR_013.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0, A0] + units: [1/m**2, '1', '1'] + physics: + - AN17-AR/EM-SX/SHF.06/strength + - AN17-AR/EM-COR/SHF.06-CDLH.07/strength + - AN17-AR/EM-COR/SHF.06-CDLV.07/strength +- type: pyaml.magnet.cfm_magnet + name: OH7_QCORROCT_140_QT_001 + mapping: + - [B3, OH7_QCORROCT_140_QT_001.octupole] + - [B1, OH7_QCORROCT_140_QT_001.quadrupole] + - [A1, OH7_QCORROCT_140_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN17-AR/EM-OCT/OH.03/strength + - AN17-AR/EM-COR/OH.03-CQLN.13/strength + - AN17-AR/EM-COR/OH.03-CQLT.05/strength +- type: pyaml.bpm.bpm + name: BPM_153 + x_pos: AN18-SD/DG-EPOS/BPM.01/x_pos + y_pos: AN18-SD/DG-EPOS/BPM.01/y_pos +- type: pyaml.bpm.bpm + name: BPM_154 + x_pos: AN18-SD/DG-EPOS/BPM.02/x_pos + y_pos: AN18-SD/DG-EPOS/BPM.02/y_pos +- type: pyaml.magnet.cfm_magnet + name: OH7_QCORROCT_141_QT_001 + mapping: + - [B3, OH7_QCORROCT_141_QT_001.octupole] + - [B1, OH7_QCORROCT_141_QT_001.quadrupole] + - [A1, OH7_QCORROCT_141_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN18-AR/EM-OCT/OH.01/strength + - AN18-AR/EM-COR/OH.01-CQLN.01/strength + - AN18-AR/EM-COR/OH.01-CQLT.01/strength +- type: pyaml.magnet.cfm_magnet + name: SH7_COR_014 + mapping: + - [B2, SH7_COR_014.sextupole] + - [B0, SH7_COR_014.hcorrector] + - [A0, SH7_COR_014.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0, A0] + units: [1/m**2, '1', '1'] + physics: + - AN18-AR/EM-SX/SHF.01/strength + - AN18-AR/EM-COR/SHF.01-CDLH.01/strength + - AN18-AR/EM-COR/SHF.01-CDLV.01/strength +- type: pyaml.bpm.bpm + name: BPM_155 + x_pos: AN18-AR/DG-EPOS/BPM.03/x_pos + y_pos: AN18-AR/DG-EPOS/BPM.03/y_pos +- type: pyaml.magnet.quadrupole + name: QCORR_176 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN18-AR/EM-COR/CQLN.02/strength +- type: pyaml.magnet.sextupole + name: SH8_014 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN18-AR/EM-SX/SHD.02/strength +- type: pyaml.magnet.quadrupole + name: QCORR_177 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN18-AR/EM-COR/CQLN.03/strength +- type: pyaml.magnet.cfm_magnet + name: SH9_COR_014 + mapping: + - [B2, SH9_COR_014.sextupole] + - [B0, SH9_COR_014.hcorrector] + - [A0, SH9_COR_014.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0, A0] + units: [1/m**2, '1', '1'] + physics: + - AN18-AR/EM-SX/SHD.03/strength + - AN18-AR/EM-COR/SHD.03-CDLH.02/strength + - AN18-AR/EM-COR/SHD.03-CDLV.02/strength +- type: pyaml.magnet.sextupole + name: SXD32_004 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN18-AR/EM-SX/SCD.01/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF3_QCORROCT_142_QT_001 + mapping: + - [B3, OCTF3_QCORROCT_142_QT_001.octupole] + - [B1, OCTF3_QCORROCT_142_QT_001.quadrupole] + - [A1, OCTF3_QCORROCT_142_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN18-AR/EM-OCT/OC.01/strength + - AN18-AR/EM-COR/OC.01-CQLN.04/strength + - AN18-AR/EM-COR/OC.01-CQLT.02/strength +- type: pyaml.magnet.cfm_magnet + name: SXF32_HCOR_004 + mapping: + - [B2, SXF32_HCOR_004.sextupole] + - [B0, SXF32_HCOR_004.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN18-AR/EM-SX/SCF.02/strength + - AN18-AR/EM-COR/SCF.02-CDLH.03/strength +- type: pyaml.bpm.bpm + name: BPM_156 + x_pos: AN18-AR/DG-EPOS/BPM.04/x_pos + y_pos: AN18-AR/DG-EPOS/BPM.04/y_pos +- type: pyaml.magnet.cfm_magnet + name: SXD32_VCOR_004 + mapping: + - [B2, SXD32_VCOR_004.sextupole] + - [A0, SXD32_VCOR_004.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN18-AR/EM-SX/SCD.03/strength + - AN18-AR/EM-COR/SCD.03-CDLV.03/strength +- type: pyaml.magnet.quadrupole + name: QCORR_178 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN18-AR/EM-COR/CQLN.05/strength +- type: pyaml.magnet.quadrupole + name: QCORR_179 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN18-AR/EM-COR/CQLN.06/strength +- type: pyaml.magnet.sextupole + name: SXD3_010 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN18-AR/EM-SX/SCD.04/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF3_QCORROCT_143_QT_001 + mapping: + - [B3, OCTF3_QCORROCT_143_QT_001.octupole] + - [B1, OCTF3_QCORROCT_143_QT_001.quadrupole] + - [A1, OCTF3_QCORROCT_143_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN18-AR/EM-OCT/OC.02/strength + - AN18-AR/EM-COR/OC.02-CQLN.07/strength + - AN18-AR/EM-COR/OC.02-CQLT.03/strength +- type: pyaml.magnet.cfm_magnet + name: SXF3_HCOR_007 + mapping: + - [B2, SXF3_HCOR_007.sextupole] + - [B0, SXF3_HCOR_007.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN18-AR/EM-SX/SCF.05/strength + - AN18-AR/EM-COR/SCF.05-CDLH.04/strength +- type: pyaml.bpm.bpm + name: BPM_157 + x_pos: AN18-AR/DG-EPOS/BPM.05/x_pos + y_pos: AN18-AR/DG-EPOS/BPM.05/y_pos +- type: pyaml.magnet.cfm_magnet + name: SXD3_VCOR_010 + mapping: + - [B2, SXD3_VCOR_010.sextupole] + - [A0, SXD3_VCOR_010.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN18-AR/EM-SX/SCD.06/strength + - AN18-AR/EM-COR/SCD.06-CDLV.04/strength +- type: pyaml.magnet.quadrupole + name: QCORR_180 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN18-AR/EM-COR/CQLN.08/strength +- type: pyaml.magnet.quadrupole + name: QCORR_181 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN18-AR/EM-COR/CQLN.09/strength +- type: pyaml.magnet.sextupole + name: SXD3_011 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN18-AR/EM-SX/SCD.07/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF3_QCORROCT_144_QT_001 + mapping: + - [B3, OCTF3_QCORROCT_144_QT_001.octupole] + - [B1, OCTF3_QCORROCT_144_QT_001.quadrupole] + - [A1, OCTF3_QCORROCT_144_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN18-AR/EM-OCT/OC.03/strength + - AN18-AR/EM-COR/OC.03-CQLN.10/strength + - AN18-AR/EM-COR/OC.03-CQLT.04/strength +- type: pyaml.magnet.cfm_magnet + name: SXF33_HCOR_007 + mapping: + - [B2, SXF33_HCOR_007.sextupole] + - [B0, SXF33_HCOR_007.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN18-AR/EM-SX/SCF.08/strength + - AN18-AR/EM-COR/SCF.08-CDLH.05/strength +- type: pyaml.bpm.bpm + name: BPM_158 + x_pos: AN18-AR/DG-EPOS/BPM.06/x_pos + y_pos: AN18-AR/DG-EPOS/BPM.06/y_pos +- type: pyaml.magnet.cfm_magnet + name: SXD33_VCOR_004 + mapping: + - [B2, SXD33_VCOR_004.sextupole] + - [A0, SXD33_VCOR_004.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN18-AR/EM-SX/SCD.09/strength + - AN18-AR/EM-COR/SCD.09-CDLV.05/strength +- type: pyaml.magnet.quadrupole + name: QCORR_182 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN18-AR/EM-COR/CQLN.11/strength +- type: pyaml.magnet.quadrupole + name: QCORR_183 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN18-AR/EM-COR/CQLN.12/strength +- type: pyaml.magnet.sextupole + name: SXD33_004 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN18-AR/EM-SX/SCD.10/strength +- type: pyaml.magnet.cfm_magnet + name: SXF33_HCOR_008 + mapping: + - [B2, SXF33_HCOR_008.sextupole] + - [B0, SXF33_HCOR_008.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN18-AR/EM-SX/SCF.11/strength + - AN18-AR/EM-COR/SCF.11-CDLH.06/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF3_QCORROCT_145_QT_001 + mapping: + - [B3, OCTF3_QCORROCT_145_QT_001.octupole] + - [B1, OCTF3_QCORROCT_145_QT_001.quadrupole] + - [A1, OCTF3_QCORROCT_145_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN18-AR/EM-OCT/OC.04/strength + - AN18-AR/EM-COR/OC.04-CQLN.13/strength + - AN18-AR/EM-COR/OC.04-CQLT.05/strength +- type: pyaml.bpm.bpm + name: BPM_159 + x_pos: AN18-AR/DG-EPOS/BPM.07/x_pos + y_pos: AN18-AR/DG-EPOS/BPM.07/y_pos +- type: pyaml.magnet.cfm_magnet + name: SXD3_VCOR_011 + mapping: + - [B2, SXD3_VCOR_011.sextupole] + - [A0, SXD3_VCOR_011.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN18-AR/EM-SX/SCD.12/strength + - AN18-AR/EM-COR/SCD.12-CDLV.06/strength +- type: pyaml.magnet.quadrupole + name: QCORR_184 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN18-AR/EM-COR/CQLN.14/strength +- type: pyaml.magnet.quadrupole + name: QCORR_185 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN18-AR/EM-COR/CQLN.15/strength +- type: pyaml.magnet.sextupole + name: SXD3_012 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN18-AR/EM-SX/SCD.13/strength +- type: pyaml.magnet.cfm_magnet + name: SXF3_HCOR_008 + mapping: + - [B2, SXF3_HCOR_008.sextupole] + - [B0, SXF3_HCOR_008.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN18-AR/EM-SX/SCF.14/strength + - AN18-AR/EM-COR/SCF.14-CDLH.07/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF3_QCORROCT_146_QT_001 + mapping: + - [B3, OCTF3_QCORROCT_146_QT_001.octupole] + - [B1, OCTF3_QCORROCT_146_QT_001.quadrupole] + - [A1, OCTF3_QCORROCT_146_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN18-AR/EM-OCT/OC.05/strength + - AN18-AR/EM-COR/OC.05-CQLN.16/strength + - AN18-AR/EM-COR/OC.05-CQLT.06/strength +- type: pyaml.bpm.bpm + name: BPM_160 + x_pos: AN18-AR/DG-EPOS/BPM.08/x_pos + y_pos: AN18-AR/DG-EPOS/BPM.08/y_pos +- type: pyaml.magnet.cfm_magnet + name: SXD3_VCOR_012 + mapping: + - [B2, SXD3_VCOR_012.sextupole] + - [A0, SXD3_VCOR_012.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN18-AR/EM-SX/SCD.15/strength + - AN18-AR/EM-COR/SCD.15-CDLV.07/strength +- type: pyaml.magnet.quadrupole + name: QCORR_186 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN18-AR/EM-COR/CQLN.17/strength +- type: pyaml.magnet.quadrupole + name: QCORR_187 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN18-AR/EM-COR/CQLN.18/strength +- type: pyaml.magnet.sextupole + name: SXD31_004 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN18-AR/EM-SX/SCD.16/strength +- type: pyaml.magnet.cfm_magnet + name: SXF31_HCOR_004 + mapping: + - [B2, SXF31_HCOR_004.sextupole] + - [B0, SXF31_HCOR_004.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN18-AR/EM-SX/SCF.17/strength + - AN18-AR/EM-COR/SCF.17-CDLH.08/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF3_QCORROCT_147_QT_001 + mapping: + - [B3, OCTF3_QCORROCT_147_QT_001.octupole] + - [B1, OCTF3_QCORROCT_147_QT_001.quadrupole] + - [A1, OCTF3_QCORROCT_147_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN18-AR/EM-OCT/OC.06/strength + - AN18-AR/EM-COR/OC.06-CQLN.19/strength + - AN18-AR/EM-COR/OC.06-CQLT.07/strength +- type: pyaml.magnet.cfm_magnet + name: SXD31_VCOR_004 + mapping: + - [B2, SXD31_VCOR_004.sextupole] + - [A0, SXD31_VCOR_004.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN18-AR/EM-SX/SCD.18/strength + - AN18-AR/EM-COR/SCD.18-CDLV.08/strength +- type: pyaml.bpm.bpm + name: BPM_161 + x_pos: AN18-AR/DG-EPOS/BPM.09/x_pos + y_pos: AN18-AR/DG-EPOS/BPM.09/y_pos +- type: pyaml.magnet.cfm_magnet + name: SH9_COR_015 + mapping: + - [B2, SH9_COR_015.sextupole] + - [B0, SH9_COR_015.hcorrector] + - [A0, SH9_COR_015.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0, A0] + units: [1/m**2, '1', '1'] + physics: + - AN18-AR/EM-SX/SHD.04/strength + - AN18-AR/EM-COR/SHD.04-CDLH.09/strength + - AN18-AR/EM-COR/SHD.04-CDLV.09/strength +- type: pyaml.magnet.quadrupole + name: QCORR_188 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN18-AR/EM-COR/CQLN.20/strength +- type: pyaml.magnet.sextupole + name: SH8_015 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN18-AR/EM-SX/SHD.05/strength +- type: pyaml.magnet.quadrupole + name: QCORR_189 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN18-AR/EM-COR/CQLN.21/strength +- type: pyaml.bpm.bpm + name: BPM_162 + x_pos: AN18-AR/DG-EPOS/BPM.10/x_pos + y_pos: AN18-AR/DG-EPOS/BPM.10/y_pos +- type: pyaml.magnet.cfm_magnet + name: SH7_COR_015 + mapping: + - [B2, SH7_COR_015.sextupole] + - [B0, SH7_COR_015.hcorrector] + - [A0, SH7_COR_015.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0, A0] + units: [1/m**2, '1', '1'] + physics: + - AN18-AR/EM-SX/SHF.06/strength + - AN18-AR/EM-COR/SHF.06-CDLH.10/strength + - AN18-AR/EM-COR/SHF.06-CDLV.10/strength +- type: pyaml.magnet.cfm_magnet + name: OH7_QCORROCT_148_QT_001 + mapping: + - [B3, OH7_QCORROCT_148_QT_001.octupole] + - [B1, OH7_QCORROCT_148_QT_001.quadrupole] + - [A1, OH7_QCORROCT_148_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN18-AR/EM-OCT/OH.02/strength + - AN18-AR/EM-COR/OH.02-CQLN.22/strength + - AN18-AR/EM-COR/OH.02-CQLT.08/strength +- type: pyaml.bpm.bpm + name: BPM_163 + x_pos: AN19-SD/DG-EPOS/BPM.01/x_pos + y_pos: AN19-SD/DG-EPOS/BPM.01/y_pos +- type: pyaml.bpm.bpm + name: BPM_164 + x_pos: AN19-SD/DG-EPOS/BPM.02/x_pos + y_pos: AN19-SD/DG-EPOS/BPM.02/y_pos +- type: pyaml.magnet.cfm_magnet + name: OH7_QCORROCT_149_QT_001 + mapping: + - [B3, OH7_QCORROCT_149_QT_001.octupole] + - [B1, OH7_QCORROCT_149_QT_001.quadrupole] + - [A1, OH7_QCORROCT_149_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN19-AR/EM-OCT/OH.01/strength + - AN19-AR/EM-COR/OH.01-CQLN.01/strength + - AN19-AR/EM-COR/OH.01-CQLT.01/strength +- type: pyaml.magnet.cfm_magnet + name: SH7_COR_016 + mapping: + - [B2, SH7_COR_016.sextupole] + - [B0, SH7_COR_016.hcorrector] + - [A0, SH7_COR_016.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0, A0] + units: [1/m**2, '1', '1'] + physics: + - AN19-AR/EM-SX/SHF.01/strength + - AN19-AR/EM-COR/SHF.01-CDLH.01/strength + - AN19-AR/EM-COR/SHF.01-CDLV.01/strength +- type: pyaml.bpm.bpm + name: BPM_165 + x_pos: AN19-AR/DG-EPOS/BPM.03/x_pos + y_pos: AN19-AR/DG-EPOS/BPM.03/y_pos +- type: pyaml.magnet.quadrupole + name: QCORR_190 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN19-AR/EM-COR/CQLN.02/strength +- type: pyaml.magnet.sextupole + name: SH8_016 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN19-AR/EM-SX/SHD.02/strength +- type: pyaml.magnet.quadrupole + name: QCORR_191 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN19-AR/EM-COR/CQLN.03/strength +- type: pyaml.magnet.cfm_magnet + name: SH9_COR_016 + mapping: + - [B2, SH9_COR_016.sextupole] + - [B0, SH9_COR_016.hcorrector] + - [A0, SH9_COR_016.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0, A0] + units: [1/m**2, '1', '1'] + physics: + - AN19-AR/EM-SX/SHD.03/strength + - AN19-AR/EM-COR/SHD.03-CDLH.02/strength + - AN19-AR/EM-COR/SHD.03-CDLV.02/strength +- type: pyaml.magnet.sextupole + name: SXD22_004 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN19-AR/EM-SX/SCD.01/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF2_QCORROCT_150_QT_001 + mapping: + - [B3, OCTF2_QCORROCT_150_QT_001.octupole] + - [B1, OCTF2_QCORROCT_150_QT_001.quadrupole] + - [A1, OCTF2_QCORROCT_150_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN19-AR/EM-OCT/OC.01/strength + - AN19-AR/EM-COR/OC.01-CQLN.04/strength + - AN19-AR/EM-COR/OC.01-CQLT.02/strength +- type: pyaml.magnet.cfm_magnet + name: SXF22_HCOR_004 + mapping: + - [B2, SXF22_HCOR_004.sextupole] + - [B0, SXF22_HCOR_004.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN19-AR/EM-SX/SCF.02/strength + - AN19-AR/EM-COR/SCF.02-CDLH.03/strength +- type: pyaml.bpm.bpm + name: BPM_166 + x_pos: AN19-AR/DG-EPOS/BPM.04/x_pos + y_pos: AN19-AR/DG-EPOS/BPM.04/y_pos +- type: pyaml.magnet.cfm_magnet + name: SXD22_VCOR_004 + mapping: + - [B2, SXD22_VCOR_004.sextupole] + - [A0, SXD22_VCOR_004.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN19-AR/EM-SX/SCD.03/strength + - AN19-AR/EM-COR/SCD.03-CDLV.03/strength +- type: pyaml.magnet.quadrupole + name: QCORR_192 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN19-AR/EM-COR/CQLN.05/strength +- type: pyaml.magnet.quadrupole + name: QCORR_193 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN19-AR/EM-COR/CQLN.06/strength +- type: pyaml.magnet.sextupole + name: SXD2_004 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN19-AR/EM-SX/SCD.04/strength +- type: pyaml.magnet.cfm_magnet + name: SXF2_HCOR_004 + mapping: + - [B2, SXF2_HCOR_004.sextupole] + - [B0, SXF2_HCOR_004.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN19-AR/EM-SX/SCF.05/strength + - AN19-AR/EM-COR/SCF.05-CDLH.04/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF2_QCORROCT_151_QT_001 + mapping: + - [B3, OCTF2_QCORROCT_151_QT_001.octupole] + - [B1, OCTF2_QCORROCT_151_QT_001.quadrupole] + - [A1, OCTF2_QCORROCT_151_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN19-AR/EM-OCT/OC.02/strength + - AN19-AR/EM-COR/OC.02-CQLN.07/strength + - AN19-AR/EM-COR/OC.02-CQLT.03/strength +- type: pyaml.bpm.bpm + name: BPM_167 + x_pos: AN19-AR/DG-EPOS/BPM.05/x_pos + y_pos: AN19-AR/DG-EPOS/BPM.05/y_pos +- type: pyaml.magnet.cfm_magnet + name: SXD2_VCOR_004 + mapping: + - [B2, SXD2_VCOR_004.sextupole] + - [A0, SXD2_VCOR_004.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN19-AR/EM-SX/SCD.06/strength + - AN19-AR/EM-COR/SCD.06-CDLV.04/strength +- type: pyaml.magnet.quadrupole + name: QCORR_194 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN19-AR/EM-COR/CQLN.08/strength +- type: pyaml.magnet.quadrupole + name: QCORR_195 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN19-AR/EM-COR/CQLN.09/strength +- type: pyaml.magnet.sextupole + name: SXD21_004 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN19-AR/EM-SX/SCD.07/strength +- type: pyaml.magnet.cfm_magnet + name: SXF21_HCOR_004 + mapping: + - [B2, SXF21_HCOR_004.sextupole] + - [B0, SXF21_HCOR_004.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN19-AR/EM-SX/SCF.08/strength + - AN19-AR/EM-COR/SCF.08-CDLH.05/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF2_QCORROCT_152_QT_001 + mapping: + - [B3, OCTF2_QCORROCT_152_QT_001.octupole] + - [B1, OCTF2_QCORROCT_152_QT_001.quadrupole] + - [A1, OCTF2_QCORROCT_152_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN19-AR/EM-OCT/OC.03/strength + - AN19-AR/EM-COR/OC.03-CQLN.10/strength + - AN19-AR/EM-COR/OC.03-CQLT.04/strength +- type: pyaml.magnet.cfm_magnet + name: SXD21_VCOR_004 + mapping: + - [B2, SXD21_VCOR_004.sextupole] + - [A0, SXD21_VCOR_004.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN19-AR/EM-SX/SCD.09/strength + - AN19-AR/EM-COR/SCD.09-CDLV.05/strength +- type: pyaml.bpm.bpm + name: BPM_168 + x_pos: AN19-AR/DG-EPOS/BPM.06/x_pos + y_pos: AN19-AR/DG-EPOS/BPM.06/y_pos +- type: pyaml.magnet.cfm_magnet + name: SH6_COR_007 + mapping: + - [B2, SH6_COR_007.sextupole] + - [B0, SH6_COR_007.hcorrector] + - [A0, SH6_COR_007.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0, A0] + units: [1/m**2, '1', '1'] + physics: + - AN19-AR/EM-SX/SHD.04/strength + - AN19-AR/EM-COR/SHD.04-CDLH.06/strength + - AN19-AR/EM-COR/SHD.04-CDLV.06/strength +- type: pyaml.magnet.quadrupole + name: QCORR_196 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN19-AR/EM-COR/CQLN.11/strength +- type: pyaml.magnet.sextupole + name: SH5_007 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN19-AR/EM-SX/SHD.05/strength +- type: pyaml.magnet.cfm_magnet + name: OH5_QCORROCT_153_001 + mapping: + - [B3, OH5_QCORROCT_153_001.octupole] + - [B1, OH5_QCORROCT_153_001.quadrupole] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1] + units: [1/m**3, 1/m**2] + physics: + - AN19-AR/EM-OCT/OH.02/strength + - AN19-AR/EM-COR/OH.02-CQLN.12/strength +- type: pyaml.bpm.bpm + name: BPM_169 + x_pos: AN19-AR/DG-EPOS/BPM.07/x_pos + y_pos: AN19-AR/DG-EPOS/BPM.07/y_pos +- type: pyaml.magnet.cfm_magnet + name: SH4_COR_007 + mapping: + - [B2, SH4_COR_007.sextupole] + - [B0, SH4_COR_007.hcorrector] + - [A0, SH4_COR_007.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0, A0] + units: [1/m**2, '1', '1'] + physics: + - AN19-AR/EM-SX/SHF.06/strength + - AN19-AR/EM-COR/SHF.06-CDLH.07/strength + - AN19-AR/EM-COR/SHF.06-CDLV.07/strength +- type: pyaml.magnet.cfm_magnet + name: OH4_QCORROCT_154_QT_001 + mapping: + - [B3, OH4_QCORROCT_154_QT_001.octupole] + - [B1, OH4_QCORROCT_154_QT_001.quadrupole] + - [A1, OH4_QCORROCT_154_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN19-AR/EM-OCT/OH.03/strength + - AN19-AR/EM-COR/OH.03-CQLN.13/strength + - AN19-AR/EM-COR/OH.03-CQLT.05/strength +- type: pyaml.bpm.bpm + name: BPM_170 + x_pos: AN20-SD/DG-EPOS/BPM.01/x_pos + y_pos: AN20-SD/DG-EPOS/BPM.01/y_pos +- type: pyaml.bpm.bpm + name: BPM_171 + x_pos: AN20-SD/DG-EPOS/BPM.02/x_pos + y_pos: AN20-SD/DG-EPOS/BPM.02/y_pos +- type: pyaml.magnet.cfm_magnet + name: OH4_QCORROCT_155_QT_001 + mapping: + - [B3, OH4_QCORROCT_155_QT_001.octupole] + - [B1, OH4_QCORROCT_155_QT_001.quadrupole] + - [A1, OH4_QCORROCT_155_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN20-AR/EM-OCT/OH.01/strength + - AN20-AR/EM-COR/OH.01-CQLN.01/strength + - AN20-AR/EM-COR/OH.01-CQLT.01/strength +- type: pyaml.magnet.cfm_magnet + name: SH4_COR_008 + mapping: + - [B2, SH4_COR_008.sextupole] + - [B0, SH4_COR_008.hcorrector] + - [A0, SH4_COR_008.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0, A0] + units: [1/m**2, '1', '1'] + physics: + - AN20-AR/EM-SX/SHF.01/strength + - AN20-AR/EM-COR/SHF.01-CDLH.01/strength + - AN20-AR/EM-COR/SHF.01-CDLV.01/strength +- type: pyaml.bpm.bpm + name: BPM_172 + x_pos: AN20-AR/DG-EPOS/BPM.03/x_pos + y_pos: AN20-AR/DG-EPOS/BPM.03/y_pos +- type: pyaml.magnet.cfm_magnet + name: OH5_QCORROCT_156_001 + mapping: + - [B3, OH5_QCORROCT_156_001.octupole] + - [B1, OH5_QCORROCT_156_001.quadrupole] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1] + units: [1/m**3, 1/m**2] + physics: + - AN20-AR/EM-OCT/OH.02/strength + - AN20-AR/EM-COR/OH.02-CQLN.02/strength +- type: pyaml.magnet.sextupole + name: SH5_008 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN20-AR/EM-SX/SHD.02/strength +- type: pyaml.magnet.quadrupole + name: QCORR_197 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN20-AR/EM-COR/CQLN.03/strength +- type: pyaml.magnet.cfm_magnet + name: SH6_COR_008 + mapping: + - [B2, SH6_COR_008.sextupole] + - [B0, SH6_COR_008.hcorrector] + - [A0, SH6_COR_008.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0, A0] + units: [1/m**2, '1', '1'] + physics: + - AN20-AR/EM-SX/SHD.03/strength + - AN20-AR/EM-COR/SHD.03-CDLH.02/strength + - AN20-AR/EM-COR/SHD.03-CDLV.02/strength +- type: pyaml.magnet.sextupole + name: SXD12_004 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN20-AR/EM-SX/SCD.01/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF1_QCORROCT_157_QT_001 + mapping: + - [B3, OCTF1_QCORROCT_157_QT_001.octupole] + - [B1, OCTF1_QCORROCT_157_QT_001.quadrupole] + - [A1, OCTF1_QCORROCT_157_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN20-AR/EM-OCT/OC.01/strength + - AN20-AR/EM-COR/OC.01-CQLN.04/strength + - AN20-AR/EM-COR/OC.01-CQLT.02/strength +- type: pyaml.magnet.cfm_magnet + name: SXF12_HCOR_004 + mapping: + - [B2, SXF12_HCOR_004.sextupole] + - [B0, SXF12_HCOR_004.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN20-AR/EM-SX/SCF.02/strength + - AN20-AR/EM-COR/SCF.02-CDLH.03/strength +- type: pyaml.bpm.bpm + name: BPM_173 + x_pos: AN20-AR/DG-EPOS/BPM.04/x_pos + y_pos: AN20-AR/DG-EPOS/BPM.04/y_pos +- type: pyaml.magnet.cfm_magnet + name: SXD12_VCOR_004 + mapping: + - [B2, SXD12_VCOR_004.sextupole] + - [A0, SXD12_VCOR_004.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN20-AR/EM-SX/SCD.03/strength + - AN20-AR/EM-COR/SCD.03-CDLV.03/strength +- type: pyaml.magnet.quadrupole + name: QCORR_198 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN20-AR/EM-COR/CQLN.05/strength +- type: pyaml.magnet.quadrupole + name: QCORR_199 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN20-AR/EM-COR/CQLN.06/strength +- type: pyaml.magnet.sextupole + name: SXD1_010 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN20-AR/EM-SX/SCD.04/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF1_QCORROCT_158_QT_001 + mapping: + - [B3, OCTF1_QCORROCT_158_QT_001.octupole] + - [B1, OCTF1_QCORROCT_158_QT_001.quadrupole] + - [A1, OCTF1_QCORROCT_158_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN20-AR/EM-OCT/OC.02/strength + - AN20-AR/EM-COR/OC.02-CQLN.07/strength + - AN20-AR/EM-COR/OC.02-CQLT.03/strength +- type: pyaml.magnet.cfm_magnet + name: SXF1_HCOR_007 + mapping: + - [B2, SXF1_HCOR_007.sextupole] + - [B0, SXF1_HCOR_007.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN20-AR/EM-SX/SCF.05/strength + - AN20-AR/EM-COR/SCF.05-CDLH.04/strength +- type: pyaml.bpm.bpm + name: BPM_174 + x_pos: AN20-AR/DG-EPOS/BPM.05/x_pos + y_pos: AN20-AR/DG-EPOS/BPM.05/y_pos +- type: pyaml.magnet.cfm_magnet + name: SXD1_VCOR_010 + mapping: + - [B2, SXD1_VCOR_010.sextupole] + - [A0, SXD1_VCOR_010.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN20-AR/EM-SX/SCD.06/strength + - AN20-AR/EM-COR/SCD.06-CDLV.04/strength +- type: pyaml.magnet.quadrupole + name: QCORR_200 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN20-AR/EM-COR/CQLN.08/strength +- type: pyaml.magnet.quadrupole + name: QCORR_201 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN20-AR/EM-COR/CQLN.09/strength +- type: pyaml.magnet.sextupole + name: SXD1_011 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN20-AR/EM-SX/SCD.07/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF1_QCORROCT_159_QT_001 + mapping: + - [B3, OCTF1_QCORROCT_159_QT_001.octupole] + - [B1, OCTF1_QCORROCT_159_QT_001.quadrupole] + - [A1, OCTF1_QCORROCT_159_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN20-AR/EM-OCT/OC.03/strength + - AN20-AR/EM-COR/OC.03-CQLN.10/strength + - AN20-AR/EM-COR/OC.03-CQLT.04/strength +- type: pyaml.magnet.cfm_magnet + name: SXF13_HCOR_007 + mapping: + - [B2, SXF13_HCOR_007.sextupole] + - [B0, SXF13_HCOR_007.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN20-AR/EM-SX/SCF.08/strength + - AN20-AR/EM-COR/SCF.08-CDLH.05/strength +- type: pyaml.bpm.bpm + name: BPM_175 + x_pos: AN20-AR/DG-EPOS/BPM.06/x_pos + y_pos: AN20-AR/DG-EPOS/BPM.06/y_pos +- type: pyaml.magnet.cfm_magnet + name: SXD13_VCOR_004 + mapping: + - [B2, SXD13_VCOR_004.sextupole] + - [A0, SXD13_VCOR_004.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN20-AR/EM-SX/SCD.09/strength + - AN20-AR/EM-COR/SCD.09-CDLV.05/strength +- type: pyaml.magnet.quadrupole + name: QCORR_202 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN20-AR/EM-COR/CQLN.11/strength +- type: pyaml.magnet.quadrupole + name: QCORR_203 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN20-AR/EM-COR/CQLN.12/strength +- type: pyaml.magnet.sextupole + name: SXD13_004 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN20-AR/EM-SX/SCD.10/strength +- type: pyaml.magnet.cfm_magnet + name: SXF13_HCOR_008 + mapping: + - [B2, SXF13_HCOR_008.sextupole] + - [B0, SXF13_HCOR_008.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN20-AR/EM-SX/SCF.11/strength + - AN20-AR/EM-COR/SCF.11-CDLH.06/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF1_QCORROCT_160_QT_001 + mapping: + - [B3, OCTF1_QCORROCT_160_QT_001.octupole] + - [B1, OCTF1_QCORROCT_160_QT_001.quadrupole] + - [A1, OCTF1_QCORROCT_160_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN20-AR/EM-OCT/OC.04/strength + - AN20-AR/EM-COR/OC.04-CQLN.13/strength + - AN20-AR/EM-COR/OC.04-CQLT.05/strength +- type: pyaml.bpm.bpm + name: BPM_176 + x_pos: AN20-AR/DG-EPOS/BPM.07/x_pos + y_pos: AN20-AR/DG-EPOS/BPM.07/y_pos +- type: pyaml.magnet.cfm_magnet + name: SXD1_VCOR_011 + mapping: + - [B2, SXD1_VCOR_011.sextupole] + - [A0, SXD1_VCOR_011.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN20-AR/EM-SX/SCD.12/strength + - AN20-AR/EM-COR/SCD.12-CDLV.06/strength +- type: pyaml.magnet.quadrupole + name: QCORR_204 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN20-AR/EM-COR/CQLN.14/strength +- type: pyaml.magnet.quadrupole + name: QCORR_205 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN20-AR/EM-COR/CQLN.15/strength +- type: pyaml.magnet.sextupole + name: SXD1_012 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN20-AR/EM-SX/SCD.13/strength +- type: pyaml.magnet.cfm_magnet + name: SXF1_HCOR_008 + mapping: + - [B2, SXF1_HCOR_008.sextupole] + - [B0, SXF1_HCOR_008.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN20-AR/EM-SX/SCF.14/strength + - AN20-AR/EM-COR/SCF.14-CDLH.07/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF1_QCORROCT_161_QT_001 + mapping: + - [B3, OCTF1_QCORROCT_161_QT_001.octupole] + - [B1, OCTF1_QCORROCT_161_QT_001.quadrupole] + - [A1, OCTF1_QCORROCT_161_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN20-AR/EM-OCT/OC.05/strength + - AN20-AR/EM-COR/OC.05-CQLN.16/strength + - AN20-AR/EM-COR/OC.05-CQLT.06/strength +- type: pyaml.bpm.bpm + name: BPM_177 + x_pos: AN20-AR/DG-EPOS/BPM.08/x_pos + y_pos: AN20-AR/DG-EPOS/BPM.08/y_pos +- type: pyaml.magnet.cfm_magnet + name: SXD1_VCOR_012 + mapping: + - [B2, SXD1_VCOR_012.sextupole] + - [A0, SXD1_VCOR_012.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN20-AR/EM-SX/SCD.15/strength + - AN20-AR/EM-COR/SCD.15-CDLV.07/strength +- type: pyaml.magnet.quadrupole + name: QCORR_206 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN20-AR/EM-COR/CQLN.17/strength +- type: pyaml.magnet.quadrupole + name: QCORR_207 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN20-AR/EM-COR/CQLN.18/strength +- type: pyaml.magnet.sextupole + name: SXD11_004 + model: + type: pyaml.magnet.identity_model + unit: 1/m**2 + physics: AN20-AR/EM-SX/SCD.16/strength +- type: pyaml.magnet.cfm_magnet + name: SXF11_HCOR_004 + mapping: + - [B2, SXF11_HCOR_004.sextupole] + - [B0, SXF11_HCOR_004.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN20-AR/EM-SX/SCF.17/strength + - AN20-AR/EM-COR/SCF.17-CDLH.08/strength +- type: pyaml.magnet.cfm_magnet + name: OCTF1_QCORROCT_162_QT_001 + mapping: + - [B3, OCTF1_QCORROCT_162_QT_001.octupole] + - [B1, OCTF1_QCORROCT_162_QT_001.quadrupole] + - [A1, OCTF1_QCORROCT_162_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN20-AR/EM-OCT/OC.06/strength + - AN20-AR/EM-COR/OC.06-CQLN.19/strength + - AN20-AR/EM-COR/OC.06-CQLT.07/strength +- type: pyaml.magnet.cfm_magnet + name: SXD11_VCOR_004 + mapping: + - [B2, SXD11_VCOR_004.sextupole] + - [A0, SXD11_VCOR_004.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN20-AR/EM-SX/SCD.18/strength + - AN20-AR/EM-COR/SCD.18-CDLV.08/strength +- type: pyaml.bpm.bpm + name: BPM_178 + x_pos: AN20-AR/DG-EPOS/BPM.09/x_pos + y_pos: AN20-AR/DG-EPOS/BPM.09/y_pos +- type: pyaml.magnet.quadrupole + name: QCORR_208 + model: + type: pyaml.magnet.identity_model + unit: 1/m + physics: AN20-AR/EM-COR/CQLN.20/strength +- type: pyaml.magnet.cfm_magnet + name: SH3_VCOR_004 + mapping: + - [B2, SH3_VCOR_004.sextupole] + - [A0, SH3_VCOR_004.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, A0] + units: [1/m**2, '1'] + physics: + - AN20-AR/EM-SX/SHD.04/strength + - AN20-AR/EM-COR/SHD.04-CDLV.09/strength +- type: pyaml.bpm.bpm + name: BPM_179 + x_pos: AN20-AR/DG-EPOS/BPM.10/x_pos + y_pos: AN20-AR/DG-EPOS/BPM.10/y_pos +- type: pyaml.magnet.cfm_magnet + name: OH2_QCORROCT_163_001 + mapping: + - [B3, OH2_QCORROCT_163_001.octupole] + - [B1, OH2_QCORROCT_163_001.quadrupole] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1] + units: [1/m**3, 1/m**2] + physics: + - AN20-AR/EM-OCT/OH.03/strength + - AN20-AR/EM-COR/OH.03-CQLN.21/strength +- type: pyaml.magnet.cfm_magnet + name: SH2_HCOR_004 + mapping: + - [B2, SH2_HCOR_004.sextupole] + - [B0, SH2_HCOR_004.hcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0] + units: [1/m**2, '1'] + physics: + - AN20-AR/EM-SX/SHD.05/strength + - AN20-AR/EM-COR/SHD.05-CDLH.09/strength +- type: pyaml.magnet.cfm_magnet + name: OH1_QCORROCT_164_QT_001 + mapping: + - [B3, OH1_QCORROCT_164_QT_001.octupole] + - [B1, OH1_QCORROCT_164_QT_001.quadrupole] + - [A1, OH1_QCORROCT_164_QT_001.skewquad] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B3, B1, A1] + units: [1/m**3, 1/m**2, 1/m**2] + physics: + - AN20-AR/EM-OCT/OH.04/strength + - AN20-AR/EM-COR/OH.04-CQLN.22/strength + - AN20-AR/EM-COR/OH.04-CQLT.08/strength +- type: pyaml.magnet.cfm_magnet + name: SH1_COR_004 + mapping: + - [B2, SH1_COR_004.sextupole] + - [B0, SH1_COR_004.hcorrector] + - [A0, SH1_COR_004.vcorrector] + model: + type: pyaml.magnet.identity_cfm_model + multipoles: [B2, B0, A0] + units: [1/m**2, '1', '1'] + physics: + - AN20-AR/EM-SX/SHF.06/strength + - AN20-AR/EM-COR/SHF.06-CDLH.10/strength + - AN20-AR/EM-COR/SHF.06-CDLV.10/strength +- type: pyaml.bpm.bpm + name: BPM_180 + x_pos: AN01-SD/DG-EPOS/BPM.01/x_pos + y_pos: AN01-SD/DG-EPOS/BPM.01/y_pos +- type: pyaml.rf.rf_plant + name: RF + masterclock: simulator/ringsimulator/ringsimulator/RfFrequency + transmitters: + - type: pyaml.rf.rf_transmitter + name: RFTRA + cavities: [RF_002, RFHARMON_002] + harmonic: 1 + distribution: 1 + voltage: 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"SH4_COR_004.vcorrector", + "SH6_COR_004.vcorrector", + "SXD12_VCOR_002.vcorrector", + "SXD1_VCOR_004.vcorrector", + "SXD13_VCOR_002.vcorrector", + "SXD1_VCOR_005.vcorrector", + "SXD1_VCOR_006.vcorrector", + "SXD11_VCOR_002.vcorrector", + "SH3_VCOR_002.vcorrector", + "SH1_COR_002.vcorrector", + "SH1_COR_003.vcorrector", + "SH3_VCOR_003.vcorrector", + "SXD11_VCOR_003.vcorrector", + "SXD1_VCOR_007.vcorrector", + "SXD13_VCOR_003.vcorrector", + "SXD1_VCOR_008.vcorrector", + "SXD1_VCOR_009.vcorrector", + "SXD12_VCOR_003.vcorrector", + "SH6_COR_005.vcorrector", + "SH4_COR_005.vcorrector", + "SH4_COR_006.vcorrector", + "SH6_COR_006.vcorrector", + "SXD21_VCOR_003.vcorrector", + "SXD2_VCOR_003.vcorrector", + "SXD22_VCOR_003.vcorrector", + "SH9_COR_009.vcorrector", + "SH7_COR_009.vcorrector", + "SH7_COR_010.vcorrector", + "SH9_COR_010.vcorrector", + "SXD31_VCOR_003.vcorrector", + "SXD3_VCOR_007.vcorrector", + "SXD33_VCOR_003.vcorrector", + "SXD3_VCOR_008.vcorrector", + "SXD3_VCOR_009.vcorrector", + "SXD32_VCOR_003.vcorrector", + "SH9_COR_011.vcorrector", + "SH7_COR_011.vcorrector", + "SH7_COR_012.vcorrector", + "SH9_COR_012.vcorrector", + "SXD41_VCOR_003.vcorrector", + "SXD4_VCOR_003.vcorrector", + "SXD42_VCOR_003.vcorrector", + "SH12_COR_005.vcorrector", + "SH10_COR_005.vcorrector", + "SH10_COR_006.vcorrector", + "SH12_COR_006.vcorrector", + "SXD51_VCOR_003.vcorrector", + "SXD5_VCOR_007.vcorrector", + "SXD53_VCOR_003.vcorrector", + "SXD5_VCOR_008.vcorrector", + "SXD5_VCOR_009.vcorrector", + "SXD52_VCOR_003.vcorrector", + "SH15_VCOR_003.vcorrector", + "SH13_COR_003.vcorrector", + "SH16_COR_003.vcorrector", + "SH16_COR_004.vcorrector", + "SH13_COR_004.vcorrector", + "SH15_VCOR_004.vcorrector", + "SXD52_VCOR_004.vcorrector", + "SXD5_VCOR_010.vcorrector", + "SXD53_VCOR_004.vcorrector", + "SXD5_VCOR_011.vcorrector", + "SXD5_VCOR_012.vcorrector", + "SXD51_VCOR_004.vcorrector", + "SH12_COR_007.vcorrector", + "SH10_COR_007.vcorrector", + "SH10_COR_008.vcorrector", + "SH12_COR_008.vcorrector", + "SXD42_VCOR_004.vcorrector", + "SXD4_VCOR_004.vcorrector", + "SXD41_VCOR_004.vcorrector", + "SH9_COR_013.vcorrector", + "SH7_COR_013.vcorrector", + "SH7_COR_014.vcorrector", + "SH9_COR_014.vcorrector", + "SXD32_VCOR_004.vcorrector", + "SXD3_VCOR_010.vcorrector", + "SXD33_VCOR_004.vcorrector", + "SXD3_VCOR_011.vcorrector", + "SXD3_VCOR_012.vcorrector", + "SXD31_VCOR_004.vcorrector", + "SH9_COR_015.vcorrector", + "SH7_COR_015.vcorrector", + "SH7_COR_016.vcorrector", + "SH9_COR_016.vcorrector", + "SXD22_VCOR_004.vcorrector", + "SXD2_VCOR_004.vcorrector", + "SXD21_VCOR_004.vcorrector", + "SH6_COR_007.vcorrector", + "SH4_COR_007.vcorrector", + "SH4_COR_008.vcorrector", + "SH6_COR_008.vcorrector", + "SXD12_VCOR_004.vcorrector", + "SXD1_VCOR_010.vcorrector", + "SXD13_VCOR_004.vcorrector", + "SXD1_VCOR_011.vcorrector", + "SXD1_VCOR_012.vcorrector", + "SXD11_VCOR_004.vcorrector", + "SH3_VCOR_004.vcorrector", + "SH1_COR_004.vcorrector" + ], + "observable_names": [ + "BPM_001", + "BPM_002", + "BPM_003", + "BPM_004", + "BPM_005", + "BPM_006", + "BPM_007", + "BPM_008", + "BPM_009", + "BPM_010", + "BPM_011", + "BPM_012", + "BPM_013", + "BPM_014", + "BPM_015", + "BPM_016", + "BPM_017", + "BPM_018", + "BPM_019", + "BPM_020", + "BPM_021", + "BPM_022", + "BPM_023", + "BPM_024", + "BPM_025", + "BPM_026", + "BPM_027", + "BPM_028", + "BPM_029", + "BPM_030", + "BPM_031", + "BPM_032", + "BPM_033", + "BPM_034", + "BPM_035", + "BPM_036", + "BPM_037", + "BPM_038", + "BPM_039", + "BPM_040", + "BPM_041", + "BPM_042", + "BPM_043", + "BPM_044", + "BPM_045", + "BPM_046", + "BPM_047", + "BPM_048", + "BPM_049", + "BPM_050", + "BPM_051", + "BPM_052", + "BPM_053", + "BPM_054", + "BPM_055", + "BPM_056", + "BPM_057", + "BPM_058", + "BPM_059", + "BPM_060", + "BPM_061", + "BPM_062", + "BPM_063", + "BPM_064", + "BPM_065", + "BPM_066", + "BPM_067", + "BPM_068", + "BPM_069", + "BPM_070", + "BPM_071", + "BPM_072", + "BPM_073", + "BPM_074", + "BPM_075", + "BPM_076", + "BPM_077", + "BPM_078", + "BPM_079", + "BPM_080", + "BPM_081", + "BPM_082", + "BPM_083", + "BPM_084", + "BPM_085", + "BPM_086", + "BPM_087", + "BPM_088", + "BPM_089", + "BPM_090", + "BPM_091", + "BPM_092", + "BPM_093", + "BPM_094", + "BPM_095", + "BPM_096", + "BPM_097", + "BPM_098", + "BPM_099", + "BPM_100", + "BPM_101", + "BPM_102", + "BPM_103", + "BPM_104", + "BPM_105", + "BPM_106", + "BPM_107", + "BPM_108", + "BPM_109", + "BPM_110", + "BPM_111", + "BPM_112", + "BPM_113", + "BPM_114", + "BPM_115", + "BPM_116", + "BPM_117", + "BPM_118", + "BPM_119", + "BPM_120", + "BPM_121", + "BPM_122", + "BPM_123", + "BPM_124", + "BPM_125", + "BPM_126", + "BPM_127", + "BPM_128", + "BPM_129", + "BPM_130", + "BPM_131", + "BPM_132", + "BPM_133", + "BPM_134", + "BPM_135", + "BPM_136", + "BPM_137", + "BPM_138", + "BPM_139", + "BPM_140", + "BPM_141", + "BPM_142", + "BPM_143", + "BPM_144", + "BPM_145", + "BPM_146", + "BPM_147", + "BPM_148", + "BPM_149", + "BPM_150", + "BPM_151", + "BPM_152", + "BPM_153", + "BPM_154", + "BPM_155", + "BPM_156", + "BPM_157", + "BPM_158", + "BPM_159", + "BPM_160", + "BPM_161", + "BPM_162", + "BPM_163", + "BPM_164", + "BPM_165", + "BPM_166", + "BPM_167", + "BPM_168", + "BPM_169", + "BPM_170", + "BPM_171", + "BPM_172", + "BPM_173", + "BPM_174", + "BPM_175", + "BPM_176", + "BPM_177", + "BPM_178", + "BPM_179", + "BPM_180", + "BPM_001", + "BPM_002", + "BPM_003", + "BPM_004", + "BPM_005", + "BPM_006", + "BPM_007", + "BPM_008", + "BPM_009", + "BPM_010", + "BPM_011", + "BPM_012", + "BPM_013", + "BPM_014", + "BPM_015", + "BPM_016", + "BPM_017", + "BPM_018", + "BPM_019", + "BPM_020", + "BPM_021", + "BPM_022", + "BPM_023", + "BPM_024", + "BPM_025", + "BPM_026", + "BPM_027", + "BPM_028", + "BPM_029", + "BPM_030", + "BPM_031", + "BPM_032", + "BPM_033", + "BPM_034", + "BPM_035", + "BPM_036", + "BPM_037", + "BPM_038", + "BPM_039", + "BPM_040", + "BPM_041", + "BPM_042", + "BPM_043", + "BPM_044", + "BPM_045", + "BPM_046", + "BPM_047", + "BPM_048", + "BPM_049", + "BPM_050", + "BPM_051", + "BPM_052", + "BPM_053", + "BPM_054", + "BPM_055", + "BPM_056", + "BPM_057", + "BPM_058", + "BPM_059", + "BPM_060", + "BPM_061", + "BPM_062", + "BPM_063", + "BPM_064", + "BPM_065", + "BPM_066", + "BPM_067", + "BPM_068", + "BPM_069", + "BPM_070", + "BPM_071", + "BPM_072", + "BPM_073", + "BPM_074", + "BPM_075", + "BPM_076", + "BPM_077", + "BPM_078", + "BPM_079", + "BPM_080", + "BPM_081", + "BPM_082", + "BPM_083", + "BPM_084", + "BPM_085", + "BPM_086", + "BPM_087", + "BPM_088", + "BPM_089", + "BPM_090", + "BPM_091", + "BPM_092", + "BPM_093", + "BPM_094", + "BPM_095", + "BPM_096", + "BPM_097", + "BPM_098", + "BPM_099", + "BPM_100", + "BPM_101", + "BPM_102", + "BPM_103", + "BPM_104", + "BPM_105", + "BPM_106", + "BPM_107", + "BPM_108", + "BPM_109", + "BPM_110", + "BPM_111", + "BPM_112", + "BPM_113", + "BPM_114", + "BPM_115", + "BPM_116", + "BPM_117", + "BPM_118", + "BPM_119", + "BPM_120", + "BPM_121", + "BPM_122", + "BPM_123", + "BPM_124", + "BPM_125", + "BPM_126", + "BPM_127", + "BPM_128", + "BPM_129", + "BPM_130", + "BPM_131", + "BPM_132", + "BPM_133", + "BPM_134", + "BPM_135", + "BPM_136", + "BPM_137", + "BPM_138", + "BPM_139", + "BPM_140", + "BPM_141", + "BPM_142", + "BPM_143", + "BPM_144", + "BPM_145", + "BPM_146", + "BPM_147", + "BPM_148", + "BPM_149", + "BPM_150", + "BPM_151", + "BPM_152", + "BPM_153", + "BPM_154", + "BPM_155", + "BPM_156", + "BPM_157", + "BPM_158", + "BPM_159", + "BPM_160", + "BPM_161", + "BPM_162", + "BPM_163", + "BPM_164", + "BPM_165", + "BPM_166", + "BPM_167", + "BPM_168", + "BPM_169", + "BPM_170", + "BPM_171", + "BPM_172", + "BPM_173", + "BPM_174", + "BPM_175", + "BPM_176", + "BPM_177", + "BPM_178", + "BPM_179", + "BPM_180" + ], + "rf_response": null, + "variable_planes": [ + "H", + "H", + "H", + "H", + "H", + "H", + "H", + "H", + "H", + "H", + "H", + "H", + "H", + "H", + "H", + "H", + "H", + "H", + "H", + "H", + "H", + "H", + "H", + "H", + "H", + "H", + "H", + "H", + "H", + "H", + "H", + "H", + "H", + "H", 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+- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +rf_response: null +type: pyaml.tuning_tools.orbit_response_matrix_data +variable_names: +- SH1_COR_001.hcorrector +- SH2_HCOR_001.hcorrector +- SXF11_HCOR_001.hcorrector +- SXF1_HCOR_001.hcorrector +- SXF13_HCOR_001.hcorrector +- SXF13_HCOR_002.hcorrector +- SXF1_HCOR_002.hcorrector +- SXF12_HCOR_001.hcorrector +- SH6_COR_001.hcorrector +- SH4_COR_001.hcorrector +- SH4_COR_002.hcorrector +- SH6_COR_002.hcorrector +- SXF21_HCOR_001.hcorrector +- SXF2_HCOR_001.hcorrector +- SXF22_HCOR_001.hcorrector +- SH9_COR_001.hcorrector +- SH7_COR_001.hcorrector +- SH7_COR_002.hcorrector +- SH9_COR_002.hcorrector +- SXF31_HCOR_001.hcorrector +- SXF3_HCOR_001.hcorrector +- SXF33_HCOR_001.hcorrector +- SXF33_HCOR_002.hcorrector +- SXF3_HCOR_002.hcorrector +- SXF32_HCOR_001.hcorrector +- SH9_COR_003.hcorrector +- SH7_COR_003.hcorrector +- SH7_COR_004.hcorrector +- SH9_COR_004.hcorrector +- SXF41_HCOR_001.hcorrector +- SXF4_HCOR_001.hcorrector +- SXF42_HCOR_001.hcorrector +- SH12_COR_001.hcorrector +- SH10_COR_001.hcorrector +- SH10_COR_002.hcorrector +- SH12_COR_002.hcorrector +- SXF51_HCOR_001.hcorrector +- SXF5_HCOR_001.hcorrector +- SXF53_HCOR_001.hcorrector +- SXF53_HCOR_002.hcorrector +- SXF5_HCOR_002.hcorrector +- SXF52_HCOR_001.hcorrector +- SH14_HCOR_001.hcorrector +- SH13_COR_001.hcorrector +- SH16_COR_001.hcorrector +- SH16_COR_002.hcorrector +- SH13_COR_002.hcorrector +- SH14_HCOR_002.hcorrector +- SXF52_HCOR_002.hcorrector +- SXF5_HCOR_003.hcorrector +- SXF53_HCOR_003.hcorrector +- SXF53_HCOR_004.hcorrector +- SXF5_HCOR_004.hcorrector +- SXF51_HCOR_002.hcorrector +- SH12_COR_003.hcorrector +- SH10_COR_003.hcorrector +- SH10_COR_004.hcorrector +- SH12_COR_004.hcorrector +- SXF42_HCOR_002.hcorrector +- SXF4_HCOR_002.hcorrector +- SXF41_HCOR_002.hcorrector +- SH9_COR_005.hcorrector +- SH7_COR_005.hcorrector +- SH7_COR_006.hcorrector +- SH9_COR_006.hcorrector +- SXF32_HCOR_002.hcorrector +- SXF3_HCOR_003.hcorrector +- SXF33_HCOR_003.hcorrector +- SXF33_HCOR_004.hcorrector +- SXF3_HCOR_004.hcorrector +- SXF31_HCOR_002.hcorrector +- SH9_COR_007.hcorrector +- SH7_COR_007.hcorrector +- SH7_COR_008.hcorrector +- SH9_COR_008.hcorrector +- SXF22_HCOR_002.hcorrector +- SXF2_HCOR_002.hcorrector +- SXF21_HCOR_002.hcorrector +- SH6_COR_003.hcorrector +- SH4_COR_003.hcorrector +- SH4_COR_004.hcorrector +- SH6_COR_004.hcorrector +- SXF12_HCOR_002.hcorrector +- SXF1_HCOR_003.hcorrector +- SXF13_HCOR_003.hcorrector +- SXF13_HCOR_004.hcorrector +- SXF1_HCOR_004.hcorrector +- SXF11_HCOR_002.hcorrector +- SH2_HCOR_002.hcorrector +- SH1_COR_002.hcorrector +- SH1_COR_003.hcorrector +- SH2_HCOR_003.hcorrector +- SXF11_HCOR_003.hcorrector +- SXF1_HCOR_005.hcorrector +- SXF13_HCOR_005.hcorrector +- SXF13_HCOR_006.hcorrector +- SXF1_HCOR_006.hcorrector +- SXF12_HCOR_003.hcorrector +- SH6_COR_005.hcorrector +- SH4_COR_005.hcorrector +- SH4_COR_006.hcorrector +- SH6_COR_006.hcorrector +- SXF21_HCOR_003.hcorrector +- SXF2_HCOR_003.hcorrector +- SXF22_HCOR_003.hcorrector +- SH9_COR_009.hcorrector +- SH7_COR_009.hcorrector +- SH7_COR_010.hcorrector +- SH9_COR_010.hcorrector +- SXF31_HCOR_003.hcorrector +- SXF3_HCOR_005.hcorrector +- SXF33_HCOR_005.hcorrector +- SXF33_HCOR_006.hcorrector +- SXF3_HCOR_006.hcorrector +- SXF32_HCOR_003.hcorrector +- SH9_COR_011.hcorrector +- SH7_COR_011.hcorrector +- SH7_COR_012.hcorrector +- SH9_COR_012.hcorrector +- SXF41_HCOR_003.hcorrector +- SXF4_HCOR_003.hcorrector +- SXF42_HCOR_003.hcorrector +- SH12_COR_005.hcorrector +- SH10_COR_005.hcorrector +- SH10_COR_006.hcorrector +- SH12_COR_006.hcorrector +- SXF51_HCOR_003.hcorrector +- SXF5_HCOR_005.hcorrector +- SXF53_HCOR_005.hcorrector +- SXF53_HCOR_006.hcorrector +- SXF5_HCOR_006.hcorrector +- SXF52_HCOR_003.hcorrector +- SH14_HCOR_003.hcorrector +- SH13_COR_003.hcorrector +- SH16_COR_003.hcorrector +- SH16_COR_004.hcorrector +- SH13_COR_004.hcorrector +- SH14_HCOR_004.hcorrector +- SXF52_HCOR_004.hcorrector +- SXF5_HCOR_007.hcorrector +- SXF53_HCOR_007.hcorrector +- SXF53_HCOR_008.hcorrector +- SXF5_HCOR_008.hcorrector +- SXF51_HCOR_004.hcorrector +- SH12_COR_007.hcorrector +- SH10_COR_007.hcorrector +- SH10_COR_008.hcorrector +- SH12_COR_008.hcorrector +- SXF42_HCOR_004.hcorrector +- SXF4_HCOR_004.hcorrector +- SXF41_HCOR_004.hcorrector +- SH9_COR_013.hcorrector +- SH7_COR_013.hcorrector +- SH7_COR_014.hcorrector +- SH9_COR_014.hcorrector +- SXF32_HCOR_004.hcorrector +- SXF3_HCOR_007.hcorrector +- SXF33_HCOR_007.hcorrector +- SXF33_HCOR_008.hcorrector +- SXF3_HCOR_008.hcorrector +- SXF31_HCOR_004.hcorrector +- SH9_COR_015.hcorrector +- SH7_COR_015.hcorrector +- SH7_COR_016.hcorrector +- SH9_COR_016.hcorrector +- SXF22_HCOR_004.hcorrector +- SXF2_HCOR_004.hcorrector +- SXF21_HCOR_004.hcorrector +- SH6_COR_007.hcorrector +- SH4_COR_007.hcorrector +- SH4_COR_008.hcorrector +- SH6_COR_008.hcorrector +- SXF12_HCOR_004.hcorrector +- SXF1_HCOR_007.hcorrector +- SXF13_HCOR_007.hcorrector +- SXF13_HCOR_008.hcorrector +- SXF1_HCOR_008.hcorrector +- SXF11_HCOR_004.hcorrector +- SH2_HCOR_004.hcorrector +- SH1_COR_004.hcorrector +- SH1_COR_001.vcorrector +- SH3_VCOR_001.vcorrector +- SXD11_VCOR_001.vcorrector +- SXD1_VCOR_001.vcorrector +- SXD13_VCOR_001.vcorrector +- SXD1_VCOR_002.vcorrector +- SXD1_VCOR_003.vcorrector +- SXD12_VCOR_001.vcorrector +- SH6_COR_001.vcorrector +- SH4_COR_001.vcorrector +- SH4_COR_002.vcorrector +- SH6_COR_002.vcorrector +- SXD21_VCOR_001.vcorrector +- SXD2_VCOR_001.vcorrector +- SXD22_VCOR_001.vcorrector +- SH9_COR_001.vcorrector +- SH7_COR_001.vcorrector +- SH7_COR_002.vcorrector +- SH9_COR_002.vcorrector +- SXD31_VCOR_001.vcorrector +- SXD3_VCOR_001.vcorrector +- SXD33_VCOR_001.vcorrector +- SXD3_VCOR_002.vcorrector +- SXD3_VCOR_003.vcorrector +- SXD32_VCOR_001.vcorrector +- SH9_COR_003.vcorrector +- SH7_COR_003.vcorrector +- SH7_COR_004.vcorrector +- SH9_COR_004.vcorrector +- SXD41_VCOR_001.vcorrector +- SXD4_VCOR_001.vcorrector +- SXD42_VCOR_001.vcorrector +- SH12_COR_001.vcorrector +- SH10_COR_001.vcorrector +- SH10_COR_002.vcorrector +- SH12_COR_002.vcorrector +- SXD51_VCOR_001.vcorrector +- SXD5_VCOR_001.vcorrector +- SXD53_VCOR_001.vcorrector +- SXD5_VCOR_002.vcorrector +- SXD5_VCOR_003.vcorrector +- SXD52_VCOR_001.vcorrector +- SH15_VCOR_001.vcorrector +- SH13_COR_001.vcorrector +- SH16_COR_001.vcorrector +- SH16_COR_002.vcorrector +- SH13_COR_002.vcorrector +- SH15_VCOR_002.vcorrector +- SXD52_VCOR_002.vcorrector +- SXD5_VCOR_004.vcorrector +- SXD53_VCOR_002.vcorrector +- SXD5_VCOR_005.vcorrector +- SXD5_VCOR_006.vcorrector +- SXD51_VCOR_002.vcorrector +- SH12_COR_003.vcorrector +- SH10_COR_003.vcorrector +- SH10_COR_004.vcorrector +- SH12_COR_004.vcorrector +- SXD42_VCOR_002.vcorrector +- SXD4_VCOR_002.vcorrector +- SXD41_VCOR_002.vcorrector +- SH9_COR_005.vcorrector +- SH7_COR_005.vcorrector +- SH7_COR_006.vcorrector +- SH9_COR_006.vcorrector +- SXD32_VCOR_002.vcorrector +- SXD3_VCOR_004.vcorrector +- SXD33_VCOR_002.vcorrector +- SXD3_VCOR_005.vcorrector +- SXD3_VCOR_006.vcorrector +- SXD31_VCOR_002.vcorrector +- SH9_COR_007.vcorrector +- SH7_COR_007.vcorrector +- SH7_COR_008.vcorrector +- SH9_COR_008.vcorrector +- SXD22_VCOR_002.vcorrector +- SXD2_VCOR_002.vcorrector +- SXD21_VCOR_002.vcorrector +- SH6_COR_003.vcorrector +- SH4_COR_003.vcorrector +- SH4_COR_004.vcorrector +- SH6_COR_004.vcorrector +- SXD12_VCOR_002.vcorrector +- SXD1_VCOR_004.vcorrector +- SXD13_VCOR_002.vcorrector +- SXD1_VCOR_005.vcorrector +- SXD1_VCOR_006.vcorrector +- SXD11_VCOR_002.vcorrector +- SH3_VCOR_002.vcorrector +- SH1_COR_002.vcorrector +- SH1_COR_003.vcorrector +- SH3_VCOR_003.vcorrector +- SXD11_VCOR_003.vcorrector +- SXD1_VCOR_007.vcorrector +- SXD13_VCOR_003.vcorrector +- SXD1_VCOR_008.vcorrector +- SXD1_VCOR_009.vcorrector +- SXD12_VCOR_003.vcorrector +- SH6_COR_005.vcorrector +- SH4_COR_005.vcorrector +- SH4_COR_006.vcorrector +- SH6_COR_006.vcorrector +- SXD21_VCOR_003.vcorrector +- SXD2_VCOR_003.vcorrector +- SXD22_VCOR_003.vcorrector +- SH9_COR_009.vcorrector +- SH7_COR_009.vcorrector +- SH7_COR_010.vcorrector +- SH9_COR_010.vcorrector +- SXD31_VCOR_003.vcorrector +- SXD3_VCOR_007.vcorrector +- SXD33_VCOR_003.vcorrector +- SXD3_VCOR_008.vcorrector +- SXD3_VCOR_009.vcorrector +- SXD32_VCOR_003.vcorrector +- SH9_COR_011.vcorrector +- SH7_COR_011.vcorrector +- SH7_COR_012.vcorrector +- SH9_COR_012.vcorrector +- SXD41_VCOR_003.vcorrector +- SXD4_VCOR_003.vcorrector +- SXD42_VCOR_003.vcorrector +- SH12_COR_005.vcorrector +- SH10_COR_005.vcorrector +- SH10_COR_006.vcorrector +- SH12_COR_006.vcorrector +- SXD51_VCOR_003.vcorrector +- SXD5_VCOR_007.vcorrector +- SXD53_VCOR_003.vcorrector +- SXD5_VCOR_008.vcorrector +- SXD5_VCOR_009.vcorrector +- SXD52_VCOR_003.vcorrector +- SH15_VCOR_003.vcorrector +- SH13_COR_003.vcorrector +- SH16_COR_003.vcorrector +- SH16_COR_004.vcorrector +- SH13_COR_004.vcorrector +- SH15_VCOR_004.vcorrector +- SXD52_VCOR_004.vcorrector +- SXD5_VCOR_010.vcorrector +- SXD53_VCOR_004.vcorrector +- SXD5_VCOR_011.vcorrector +- SXD5_VCOR_012.vcorrector +- SXD51_VCOR_004.vcorrector +- SH12_COR_007.vcorrector +- SH10_COR_007.vcorrector +- SH10_COR_008.vcorrector +- SH12_COR_008.vcorrector +- SXD42_VCOR_004.vcorrector +- SXD4_VCOR_004.vcorrector +- SXD41_VCOR_004.vcorrector +- SH9_COR_013.vcorrector +- SH7_COR_013.vcorrector +- SH7_COR_014.vcorrector +- SH9_COR_014.vcorrector +- SXD32_VCOR_004.vcorrector +- SXD3_VCOR_010.vcorrector +- SXD33_VCOR_004.vcorrector +- SXD3_VCOR_011.vcorrector +- SXD3_VCOR_012.vcorrector +- SXD31_VCOR_004.vcorrector +- SH9_COR_015.vcorrector +- SH7_COR_015.vcorrector +- SH7_COR_016.vcorrector +- SH9_COR_016.vcorrector +- SXD22_VCOR_004.vcorrector +- SXD2_VCOR_004.vcorrector +- SXD21_VCOR_004.vcorrector +- SH6_COR_007.vcorrector +- SH4_COR_007.vcorrector +- SH4_COR_008.vcorrector +- SH6_COR_008.vcorrector +- SXD12_VCOR_004.vcorrector +- SXD1_VCOR_010.vcorrector +- SXD13_VCOR_004.vcorrector +- SXD1_VCOR_011.vcorrector +- SXD1_VCOR_012.vcorrector +- SXD11_VCOR_004.vcorrector +- SH3_VCOR_004.vcorrector +- SH1_COR_004.vcorrector +variable_planes: +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- H +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V +- V diff --git a/examples/SOLEIL_examples/p.yaml b/examples/use_cases/config/soleil_ii/p.yaml similarity index 94% rename from examples/SOLEIL_examples/p.yaml rename to examples/use_cases/config/soleil_ii/p.yaml index 270842a75..d8829096d 100644 --- a/examples/SOLEIL_examples/p.yaml +++ b/examples/use_cases/config/soleil_ii/p.yaml @@ -14,6 +14,7 @@ controls: - type: tango.pyaml.controlsystem name: live tango_host: localhost:11000 + catalog: catalogs.yaml arrays: arrays.yaml devices: - devices.yaml diff --git a/examples/use_cases/config/soleil_ii/trm.json b/examples/use_cases/config/soleil_ii/trm.json new file mode 100644 index 000000000..426def208 --- /dev/null +++ b/examples/use_cases/config/soleil_ii/trm.json @@ -0,0 +1,639 @@ +{ + "type": "pyaml.tuning_tools.response_matrix_data", + "matrix": [ + [ + 0.14112466920759847, + 0.12508652345369353, + 0.12508453275505982, + 0.12514074167291334, + 0.1249331279032928, + 0.12183144072930308, + 0.12167340868193821, + 0.12489224133035992, + 0.12497108739886742, + 0.12489106642790682, + 0.1251106206791308, + 0.2525778989868055, + 0.2521967843216455, + 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"QCORR_174", + "QCORR_175", + "QCORR_176", + "QCORR_177", + "QCORR_178", + "QCORR_179", + "QCORR_180", + "QCORR_181", + "QCORR_182", + "QCORR_183", + "QCORR_184", + "QCORR_185", + "QCORR_186", + "QCORR_187", + "QCORR_188", + "QCORR_189", + "QCORR_190", + "QCORR_191", + "QCORR_192", + "QCORR_193", + "QCORR_194", + "QCORR_195", + "QCORR_196", + "QCORR_197", + "QCORR_198", + "QCORR_199", + "QCORR_200", + "QCORR_201", + "QCORR_202", + "QCORR_203", + "QCORR_204", + "QCORR_205", + "QCORR_206", + "QCORR_207", + "QCORR_208" + ], + "observable_names": [ + "BETATRON_TUNE.x", + "BETATRON_TUNE.y" + ] +} diff --git a/examples/SOLEIL_examples/tuning_tools.yaml b/examples/use_cases/config/soleil_ii/tuning_tools.yaml similarity index 61% rename from examples/SOLEIL_examples/tuning_tools.yaml rename to examples/use_cases/config/soleil_ii/tuning_tools.yaml index 295b9d767..5d67c0f29 100644 --- a/examples/SOLEIL_examples/tuning_tools.yaml +++ b/examples/use_cases/config/soleil_ii/tuning_tools.yaml @@ -1,23 +1,19 @@ - type: pyaml.diagnostics.tune_monitor name: BETATRON_TUNE - tune_h: - type: tango.pyaml.attribute_read_only - attribute: simulator/ringsimulator/ringsimulator/Tune_h - tune_v: - type: tango.pyaml.attribute_read_only - attribute: simulator/ringsimulator/ringsimulator/Tune_v + tune_h: simulator/ringsimulator/ringsimulator/Tune_h + tune_v: simulator/ringsimulator/ringsimulator/Tune_v - type: pyaml.tuning_tools.tune name: DEFAULT_TUNE_CORRECTION - quad_array_name: QCORR + quad_array_name: QForTune betatron_tune_name: BETATRON_TUNE - response_matrix: file:trm.json + response_matrix: ${path:trm.json} - type: pyaml.tuning_tools.tune_response_matrix name: DEFAULT_TUNE_RESPONSE_MATRIX - quad_array_name: QCORR + quad_array_name: QForTune betatron_tune_name: BETATRON_TUNE quad_delta: 1e-3 -- type: pyaml.diagnostics.chromaticity_monitor - name: DEFAULT_CHROMATICITY_MEASUREMENT +- type: pyaml.tuning_tools.chromaticity_monitor + name: CHROMATICITY_MONITOR betatron_tune_name: BETATRON_TUNE rf_plant_name: RF fit_order: 2 @@ -29,8 +25,8 @@ max_e_delta: 5e-2 - type: pyaml.tuning_tools.orbit_response_matrix bpm_array_name: BPM - hcorr_array_name: HCORR - vcorr_array_name: VCORR + hcorr_array_name: HCorr + vcorr_array_name: VCorr corrector_delta: 1e-5 name: DEFAULT_ORBIT_RESPONSE_MATRIX - type: pyaml.tuning_tools.dispersion @@ -40,8 +36,8 @@ name: DEFAULT_DISPERSION - type: pyaml.tuning_tools.orbit bpm_array_name: BPM - hcorr_array_name: HCORR - vcorr_array_name: VCORR + hcorr_array_name: HCorr + vcorr_array_name: VCorr name: DEFAULT_ORBIT_CORRECTION singular_values: 16 - response_matrix: file:orm.json + response_matrix: ${path:orm.json} diff --git a/examples/use_cases/orbit_correction.png b/examples/use_cases/orbit_correction.png new file mode 100644 index 000000000..748ae689e Binary files /dev/null and b/examples/use_cases/orbit_correction.png differ diff --git a/pyaml/__init__.py b/pyaml/__init__.py index 65050bc04..0bb1c8b0b 100644 --- a/pyaml/__init__.py +++ b/pyaml/__init__.py @@ -16,9 +16,10 @@ import logging.config import os +from pyaml.common.element import ReprOptions, set_repr_options from pyaml.common.exception import PyAMLConfigException, PyAMLException -__all__ = ["PyAMLException", "PyAMLConfigException"] +__all__ = ["PyAMLException", "PyAMLConfigException", "ReprOptions", "set_repr_options"] config_file = os.getenv("PYAML_LOG_CONFIG", "pyaml_logging.conf") diff --git a/pyaml/accelerator.py b/pyaml/accelerator.py index 2af928af5..0bc273018 100644 --- a/pyaml/accelerator.py +++ b/pyaml/accelerator.py @@ -2,118 +2,176 @@ Accelerator class """ -from pydantic import BaseModel, ConfigDict, Field +import warnings from .arrays.array import ArrayConfig -from .common.element import Element -from .common.element_holder import ElementHolder +from .common.element import Element, __pyaml_repr__ from .common.exception import PyAMLConfigException +from .common.holders.element_holder import ElementHolder from .configuration import ConfigurationManager, UnsupportedConfigurationRootError from .configuration.factory import Factory from .control.controlsystem import ControlSystem from .lattice.simulator import Simulator +from .validation import DynamicValidation, SchemaValidator, register_schema from .yellow_pages import YellowPages # Define the main class name for this module PYAMLCLASS = "Accelerator" -class ConfigModel(BaseModel): +@register_schema +class Accelerator(DynamicValidation): """ - Configuration model for Accelerator + Top-level accelerator object. + + An Accelerator represents a complete accelerator model, including its + machine-wide properties, devices, arrays, control systems, and simulators. + It serves as the main entry point for loading, constructing, and interacting + with an accelerator configuration. Parameters ---------- facility : str - Facility name + Facility name. machine : str - Accelerator name + Accelerator name. energy : float - Accelerator nominal energy. For ramped machine, - this value can be dynamically set + Nominal accelerator energy. alphac : float, optional - Moment compaction factor. - harmonic_number: int, optional - Number of bucket + Momentum compaction factor. + harmonic_number : int, optional + Harmonic number. controls : list[ControlSystem], optional - List of control system used. An accelerator - can access several control systems + Control systems associated with the accelerator. simulators : list[Simulator], optional - Simulator list - data_folder : str - Data folder + Simulators associated with the accelerator. arrays : list[ArrayConfig], optional - Element family - description : str , optional - Acceleration description - devices : list[.common.element.Element] - Element list + Array configurations. + devices : list[Element], optional + Accelerator devices. + data_folder : str, optional + Path to the accelerator data directory. + description : str, optional + Human-readable description of the accelerator. + + Attributes + ---------- + live + Control system named ``live``, if one is configured. + design + Simulator named ``design``, if one is configured. + yellow_pages + Discovery service over the arrays, tools and diagnostics of every mode. + + Methods + ------- + set_energy(E) + Set the energy for all simulators and control systems. + set_mcf(alphac) + Set the moment compaction factor for all simulators and control systems. + set_harmonic_number(h) + Set the number of bucket. + add_device(config, ignore_external=False) + Dynamically add a device to this accelerator. + post_init() + Method triggered after all initialisations are done + get_description() + Returns the description of the accelerator + simulators() + Return all registered simulator modes. + controls() + Return all registered control modes. + modes() + Return all registered control and simulator modes. + from_dict(config_dict, ignore_external=False, validate=False) + Construct an accelerator from a dictionary. + load(filename, include_locations=False, ignore_external=False, validate=False) + Load an accelerator from a config file. + + Notes + ----- + Control systems and simulators are registered by name and are exposed as + attributes of the accelerator instance. The control system named ``"live"`` + and the simulator named ``"design"`` are additionally available through the + :attr:`live` and :attr:`design` properties. """ - model_config = ConfigDict(arbitrary_types_allowed=True, extra="forbid") + __pyaml_repr_exclude__ = ("description", "yellow_pages") + + def __init__( + self, + facility: str, + machine: str, + energy: float, + alphac: float | None = None, + harmonic_number: int | None = None, + controls: list[ControlSystem] | None = None, + simulators: list[Simulator] | None = None, + arrays: list[ArrayConfig] | None = None, + devices: list[Element] | None = None, + data_folder: str | None = None, + description: str | None = None, + ): + """ + Initialize the Accelerator. + """ + self.facility = facility + self.machine = machine + self._data_folder = data_folder + self.description = description - facility: str - machine: str - energy: float - alphac: float | None = None - harmonic_number: int | None = None - controls: list[ControlSystem] = None - simulators: list[Simulator] = None - data_folder: str - description: str | None = None - arrays: list[ArrayConfig] = Field(default=None, repr=False) - devices: list[Element] = Field(repr=False) + self._energy = float(energy) if energy is not None else None + self._alphac = float(alphac) if alphac is not None else None + self._harmonic_number = int(harmonic_number) if harmonic_number is not None else None + self._arrays = arrays + self._devices = devices -class Accelerator(object): - """PyAML top level class""" + self.__design = None + self.__live = None - def __init__(self, cfg: ConfigModel): - self._cfg = cfg - __design = None - __live = None self._controls: dict[str, ElementHolder] = {} self._simulators: dict[str, ElementHolder] = {} - if cfg.controls is not None: - for c in cfg.controls: + if controls is not None: + for c in controls: if c.name() == "live": self.__live = c else: # Add as dynamic attribute setattr(self, c.name(), c) - c.fill_device(cfg.devices) + c.fill_device(self._devices) c._peer = self self._controls[c.name()] = c - if cfg.simulators is not None: - for s in cfg.simulators: + if simulators is not None: + for s in simulators: if s.name() == "design": self.__design = s else: # Add as dynamic attribute setattr(self, s.name(), s) - s.fill_device(cfg.devices) + s.fill_device(self._devices) s._peer = self self._simulators[s.name()] = s - if cfg.arrays is not None: - for a in cfg.arrays: - if cfg.simulators is not None: - for s in cfg.simulators: + if arrays is not None: + for a in self._arrays: + if self._simulators is not None: + for s in self._simulators.values(): a.fill_array(s) - if cfg.controls is not None: - for c in cfg.controls: + if self._controls is not None: + for c in self._controls.values(): a.fill_array(c) - if cfg.energy is not None: - self.set_energy(cfg.energy) + if self._energy is not None: + self.set_energy(self._energy) - if cfg.alphac is not None: - self.set_mcf(cfg.alphac) + if self._alphac is not None: + self.set_mcf(self._alphac) - if cfg.harmonic_number is not None: - self.set_harmonic_number(cfg.harmonic_number) + if self._harmonic_number is not None: + self.set_harmonic_number(self._harmonic_number) self._yellow_pages = YellowPages(self) @@ -121,12 +179,22 @@ def __init__(self, cfg: ConfigModel): def _set_properties(self, method: str, value): # Sets global property - if self._cfg.simulators is not None: - for s in self._cfg.simulators: + """ + Propagate a machine-wide property to every element of every mode. + + Parameters + ---------- + method : str + Name of the element setter to call, for example ``"set_energy"``. + value : object + Value passed to that setter on every element. + """ + if self._simulators is not None: + for s in self._simulators.values(): m = getattr(s, method) m(value) - if self._cfg.controls is not None: - for c in self._cfg.controls: + if self._controls is not None: + for c in self._controls.values(): m = getattr(c, method) m(value) @@ -165,46 +233,48 @@ def set_harmonic_number(self, h: int): def add_device(self, config: dict, ignore_external=False): """ - Dynamically add a device to this accelerator + Dynamically add a device to this accelerator. - config_dict : str - Dictionary containing accelerator config - ignore_external: bool - Ignore external modules and return None for object that - cannot be created. pydantic schema that support that an - object is not created should handle None fields. + Parameters + ---------- + config : dict + Configuration dictionary describing the device to add. + ignore_external : bool + Ignore external modules and return ``None`` for objects that + cannot be created. Pydantic schemas that support an absent object + should declare the corresponding fields as optional. """ - dev = Factory.depth_first_build(config, ignore_external) + dev = Factory.build(config, ignore_external) if not isinstance(dev, Element): raise PyAMLConfigException( "Invalid device type, Element or sub classes of Element expected " + f"but got {dev.__class__.__name__}" ) - self._cfg.devices.append(dev) - if self._cfg.controls is not None: - for c in self._cfg.controls: + self._devices.append(dev) + if self._controls is not None: + for c in self._controls: c.fill_device([dev]) - if self._cfg.simulators is not None: - for s in self._cfg.simulators: + if self._simulators is not None: + for s in self._simulators: s.fill_device([dev]) def post_init(self): """ Method triggered after all initialisations are done """ - if self._cfg.simulators is not None: - for s in self._cfg.simulators: + if self._simulators is not None: + for s in self._simulators.values(): s.post_init() - if self._cfg.controls is not None: - for c in self._cfg.controls: + if self._controls is not None: + for c in self._controls.values(): c.post_init() def get_description(self) -> str: """ Returns the description of the accelerator """ - return self._cfg.description + return self.description @property def live(self) -> ControlSystem: @@ -232,6 +302,7 @@ def design(self) -> Simulator: @property def yellow_pages(self) -> YellowPages: + """Return the yellow pages.""" return self._yellow_pages def simulators(self) -> dict[str, "ElementHolder"]: @@ -249,33 +320,57 @@ def modes(self) -> dict[str, "ElementHolder"]: modes.update(self._controls) return modes + def _pyaml_repr_fields(self) -> dict[str, object]: + return { + "facility": self.facility, + "machine": self.machine, + "simulators": list(self._simulators), + "controls": list(self._controls), + } + def __repr__(self): - return repr(self._cfg).replace("ConfigModel", self.__class__.__name__) + """ + Implement the __repr__ string. + """ + return __pyaml_repr__(self) @staticmethod - def from_dict(config_dict: dict, ignore_external=False) -> "Accelerator": + def from_dict(config_dict: dict, ignore_external: bool = False, validate: bool = False) -> "Accelerator": """ Construct an accelerator from a dictionary. Parameters ---------- - config_dict : str - Dictionary containing accelerator config - ignore_external: bool - Ignore external modules and return None for object that - cannot be created. pydantic schema that support that an - object is not created should handle None fields. + config_dict : dict + Dictionary containing the accelerator configuration. + ignore_external : bool + Ignore external modules and return ``None`` for objects that + cannot be created. Pydantic schemas that support an absent object + should declare the corresponding fields as optional. + validate : bool + Validate the configuration dictionary against the registered + Pydantic schemas before constructing the accelerator. If ``True``, + validation errors are raised before the factory builds the object. + + Returns + ------- + Accelerator + Constructed accelerator instance. """ if ignore_external: # control systems are external, so remove controls field config_dict.pop("controls", None) + + if validate: + config_dict = SchemaValidator.validate_to_dict(config_dict) + # Ensure factory is clean before building a new accelerator Factory.clear() - return Factory.depth_first_build(config_dict, ignore_external) + return Factory.build(config_dict, ignore_external) @staticmethod - def load(filename: str, use_fast_loader: bool = False, ignore_external=False) -> "Accelerator": + def load(filename: str, include_locations: bool = False, ignore_external=False, validate: bool = False) -> "Accelerator": """ Load an accelerator from a config file. @@ -283,22 +378,35 @@ def load(filename: str, use_fast_loader: bool = False, ignore_external=False) -> ---------- filename : str Configuration file name, yaml or json. - use_fast_loader : bool - Use fast yaml loader. When specified, - no line number are reported in case of error, + include_locations : bool + When False, use faster loader but no line number + are reported in case of error, only the element name that triggered the error - will be reported in the exception) + will be reported in the exception ignore_external : bool Ignore external modules and return None for object that cannot be created. pydantic schema that support that an object is not created should handle None fields. + validate : bool + Validate the loaded data """ + manager = ConfigurationManager() + + if not validate and include_locations: + warnings.warn( + "'include_locations=True' is ignored when 'validate=False'. " + "Source-location metadata is only needed for validation.", + UserWarning, + stacklevel=2, + ) + include_locations = False + try: - manager.add(filename, use_fast_loader=use_fast_loader) + manager.add(filename, include_locations=include_locations) except UnsupportedConfigurationRootError as ex: raise PyAMLConfigException( "Accelerator.load() expects a 'pyaml.accelerator' root configuration. " "Use the factory APIs to build sub-elements directly." ) from ex - return manager.build(ignore_external=ignore_external) + return manager.build(ignore_external=ignore_external, validate=validate) diff --git a/pyaml/apidoc/gen_api.py b/pyaml/apidoc/gen_api.py index 148e68733..e2b05a8ae 100644 --- a/pyaml/apidoc/gen_api.py +++ b/pyaml/apidoc/gen_api.py @@ -1,7 +1,6 @@ import importlib import inspect import sys -from pathlib import Path # List of PyAML modules to include in the API reference # for i in `find . | grep ".py" | grep -v "cache" | grep -v "__init__"`; @@ -22,74 +21,85 @@ "pyaml.arrays.serialized_magnet", "pyaml.arrays.serialized_magnet_array", "pyaml.bpm.bpm", - "pyaml.bpm.bpm_model", - "pyaml.bpm.bpm_simple_model", - "pyaml.bpm.bpm_tiltoffset_model", "pyaml.common.abstract", "pyaml.common.abstract_aggregator", "pyaml.common.constants", "pyaml.common.element", - "pyaml.common.element_holder", "pyaml.common.exception", - "pyaml.configuration.csvcurve", - "pyaml.configuration.csvmatrix", - "pyaml.configuration.curve", + "pyaml.common.holders.element_holder", + "pyaml.common.holders.sub_holders", + "pyaml.common.holders.rf_holder", "pyaml.configuration.factory", "pyaml.configuration.fileloader", - "pyaml.configuration.inline_curve", - "pyaml.configuration.inline_matrix", "pyaml.configuration.manager", - "pyaml.configuration.matrix", + "pyaml.configuration.restfetcher", + "pyaml.configuration.unbound_element", "pyaml.control.abstract_impl", "pyaml.control.controlsystem", "pyaml.control.deviceaccess", "pyaml.control.deviceaccesslist", "pyaml.control.readback_value", - "pyaml.diagnostics.chromaticity_monitor", + "pyaml.diagnostics.atune_monitor", "pyaml.diagnostics.tune_monitor", "pyaml.external.pySC_interface", "pyaml.lattice.abstract_impl", "pyaml.lattice.attribute_linker", - "pyaml.lattice.element", "pyaml.lattice.lattice_elements_linker", "pyaml.lattice.polynom_info", "pyaml.lattice.simulator", "pyaml.magnet.cfm_magnet", "pyaml.magnet.corrector", + "pyaml.magnet.linear_cfm_model", + "pyaml.magnet.linear_model", + "pyaml.magnet.linear_serialized_model", "pyaml.magnet.function_mapping", "pyaml.magnet.hcorrector", "pyaml.magnet.identity_cfm_model", "pyaml.magnet.identity_model", - "pyaml.magnet.linear_cfm_model", - "pyaml.magnet.linear_model", - "pyaml.magnet.linear_serialized_model", "pyaml.magnet.magnet", + "pyaml.magnet.serialized_magnet", + "pyaml.magnet.spline_model", "pyaml.magnet.model", "pyaml.magnet.octupole", "pyaml.magnet.quadrupole", - "pyaml.magnet.serialized_magnet", "pyaml.magnet.sextupole", "pyaml.magnet.skewoctu", "pyaml.magnet.skewquad", "pyaml.magnet.skewsext", - "pyaml.magnet.spline_model", "pyaml.magnet.vcorrector", + "pyaml.magnet.csvcurve", + "pyaml.magnet.csvmatrix", + "pyaml.magnet.curve", + "pyaml.magnet.inline_curve", + "pyaml.magnet.inline_matrix", + "pyaml.magnet.matrix", "pyaml.rf.rf_plant", "pyaml.rf.rf_transmitter", # "pyaml.tuning_tools.LOCO.loco", # "pyaml.tuning_tools.SOFB.sofb", + "pyaml.tuning_tools.chromaticity", + "pyaml.tuning_tools.measurement_tool", + "pyaml.tuning_tools.chromaticity_response_matrix", "pyaml.tuning_tools.dispersion", + "pyaml.tuning_tools.response_matrix_data", "pyaml.tuning_tools.orbit", "pyaml.tuning_tools.orbit_response_matrix", - "pyaml.tuning_tools.chromaticity", - "pyaml.tuning_tools.tune", - "pyaml.tuning_tools.chromaticity_response_matrix", - "pyaml.tuning_tools.measurement_tool", "pyaml.tuning_tools.orbit_response_matrix_data", - "pyaml.tuning_tools.response_matrix_data", + "pyaml.tuning_tools.chromaticity_monitor", + "pyaml.tuning_tools.tune", "pyaml.tuning_tools.tune_response_matrix", "pyaml.tuning_tools.tuning_tool", + "pyaml.tuning_tools.bba", + "pyaml.tuning_tools.bba2", "pyaml.yellow_pages", + "pyaml._version", + "pyaml.validation.configuration_models", + "pyaml.validation.errors", + "pyaml.validation.generator", + "pyaml.validation.registry", + "pyaml.validation.schema_builder", + "pyaml.validation.validation_models", + "pyaml.validation.validator", ] @@ -126,7 +136,7 @@ def generate_selective_module(m): if m in ["pyaml.arrays.element_array"]: # Include special members for operator overloading file.write(" :special-members: __add__, __and__, __or__, __sub__ \n") - if m in ["pyaml.yellow_pages", "pyaml.configuration.manager"]: + if m in ["pyaml.yellow_pages", "pyaml.magnet.manager"]: # Include special members for exploratory overloading file.write(" :special-members: __dir__, __getattr__, __getitem__, __repr__, __str__ \n") file.write(" :exclude-members: model_config\n") diff --git a/pyaml/arrays/__init__.py b/pyaml/arrays/__init__.py new file mode 100644 index 000000000..e69de29bb diff --git a/pyaml/arrays/array.py b/pyaml/arrays/array.py index e3b59b73d..64af7470e 100644 --- a/pyaml/arrays/array.py +++ b/pyaml/arrays/array.py @@ -2,18 +2,17 @@ Array configuration """ -from pydantic import BaseModel, ConfigDict - from pyaml.common.exception import PyAMLException -from ..common.element_holder import ElementHolder +from ..common.element import __pyaml_repr__ +from ..common.holders.element_holder import ElementHolder +from ..validation import DynamicValidation, register_schema -class ArrayConfigModel(BaseModel): +@register_schema +class ArrayConfig(DynamicValidation): """ - Base class for configuration of array of :py:class:`~pyaml.arrays.element.Element`, - :py:class:`~pyaml.arrays.bpm.BPM`, :py:class:`~pyaml.arrays.magnet.Magnet` or - :py:class:`~pyaml.arrays.cfm_magnet.CombinedFunctionMagnet`. + Base class for configuration of arrays (families). Parameters ---------- @@ -21,21 +20,36 @@ class ArrayConfigModel(BaseModel): Name of the array elements : list[str] List of pyaml element names - """ - model_config = ConfigDict(arbitrary_types_allowed=True, extra="forbid") + Attributes + ---------- + name + Return the name. + elements + Return the elements. - name: str - elements: list[str] + Methods + ------- + fill_array(holder) + Fill array with elements from the holder and add the array to the holder. + """ + def __init__(self, name: str, elements: list[str]): + """ + Initialize the ArrayConfig. + """ + self._name = name + self._elements = elements -class ArrayConfig(object): - """ - Base class that implements configuration for access to arrays (families) - """ + @property + def name(self): + """Return the name.""" + return self._name - def __init__(self, cfg: ArrayConfigModel): - self._cfg = cfg + @property + def elements(self): + """Return the elements.""" + return self._elements def fill_array(self, holder: ElementHolder): """ @@ -57,6 +71,7 @@ def fill_array(self, holder: ElementHolder): raise PyAMLException("Array.fill_array() is not subclassed") def __repr__(self): - # ArrayConfigModel is a super class - # ConfigModel is expected from sub classes - return repr(self._cfg).replace("ConfigModel", self.__class__.__name__) + """ + Implement the ``__repr__`` string. + """ + return __pyaml_repr__(self) diff --git a/pyaml/arrays/bpm.py b/pyaml/arrays/bpm.py index 0883a378a..4ea849271 100644 --- a/pyaml/arrays/bpm.py +++ b/pyaml/arrays/bpm.py @@ -1,20 +1,40 @@ -from ..common.element_holder import ElementHolder -from .array import ArrayConfig, ArrayConfigModel +""" +BPM module. -# Define the main class name for this module -PYAMLCLASS = "BPM" +This module provides BPM functionality for the PyAML accelerator middle layer. +""" +from ..common.holders.element_holder import ElementHolder +from ..validation import DynamicValidation, register_schema +from .array import ArrayConfig -class ConfigModel(ArrayConfigModel): - """Configuration model for :py:class:`.BPMArray`.""" +# Define the main class name for this module +PYAMLCLASS = "BPM" -class BPM(ArrayConfig): +@register_schema +class BPM(ArrayConfig, DynamicValidation): """ :py:class:`.BPMArray` configuration. - Example + Parameters + ---------- + name : str + Name under which the array is registered and later looked up. + elements : list[str] + Element name patterns making up the array: literal names, ``fnmatch`` wildcards, or ``re:`` regular + expressions. + + Methods ------- + fill_array(holder) + Fill the :py:class:`.BPMArray` using element holder (:py:class:`~pyaml.lattice.simulator.Simulator` or + :py:class:`~pyaml.control.controlsystem.ControlSystem`) and add the array to the holder. This method is + called when an :py:class:`~pyaml.accelerator.Accelerator` is loaded but can be used to create arrays by + code as shown bellow: + + Examples + -------- Here is an example using a yaml configuration file: .. code-block:: yaml @@ -37,11 +57,13 @@ class BPM(ArrayConfig): name="BPM", elements=["BPM_C04-01","BPM_C04-02","BPM_C04-03"] )) - """ - def __init__(self, cfg: ArrayConfigModel): - super().__init__(cfg) + def __init__(self, name: str, elements: list[str]): + """ + Initialize the BPM. + """ + super().__init__(name, elements) def fill_array(self, holder: ElementHolder): """ @@ -66,4 +88,4 @@ def fill_array(self, holder: ElementHolder): holder : ElementHolder The element holder to populate the :py:class:`.BPMArray` with. """ - holder.fill_bpm_array(self._cfg.name, self._cfg.elements) + holder.bpms.add(self._name, self._elements) diff --git a/pyaml/arrays/bpm_array.py b/pyaml/arrays/bpm_array.py index ea44abb65..9006af38c 100644 --- a/pyaml/arrays/bpm_array.py +++ b/pyaml/arrays/bpm_array.py @@ -1,3 +1,9 @@ +""" +BPM Array module. + +This module provides bpm array functionality for the PyAML accelerator middle layer. +""" + import numpy as np from ..bpm.bpm import BPM @@ -20,9 +26,21 @@ class RWBPMPosition(ReadFloatArray): Name of the position accessor bpms : list[pyaml.bpm.bpm.BPM] List of BPM objects to access + + Methods + ------- + get() + Get BPM positions. + unit() + Get the units for BPM positions. + set_aggregator(agg) + Set the device access list aggregator for improved performance. """ def __init__(self, name: str, bpms: list[BPM]): + """ + Initialize the RWBPMPosition. + """ self.__bpms = bpms self.__name = name self.__aggregator: DeviceAccessList = None @@ -84,9 +102,21 @@ class RWBPMSinglePosition(ReadFloatArray): List of BPM objects to access idx : int Index for the position axis (0 for horizontal, 1 for vertical) + + Methods + ------- + get() + Get single axis BPM positions. + unit() + Get the units for BPM positions. + set_aggregator(agg) + Set the device access list aggregator for improved performance. """ def __init__(self, name: str, bpms: list[BPM], idx: int): + """ + Initialize the RWBPMSinglePosition. + """ self.__bpms = bpms self.__name = name self.__idx = idx @@ -145,11 +175,20 @@ class BPMArray(ElementArray): either a (:py:class:`~pyaml.lattice.simulator.Simulator` or a :py:class:`~pyaml.control.controlsystem.ControlSystem`). use_aggregator : bool - Use aggregator to increase performance by using paralell + Use aggregator to increase performance by using parallel access to underlying devices. - Example - ------- + Attributes + ---------- + positions + Returns position of each bpm of this array + h + Returns horizontal position of each bpm of this array + v + Returns vertical position of each bpm of this array + + Examples + -------- An array can be retrieved from the configuration as in the following example: @@ -161,10 +200,12 @@ class BPMArray(ElementArray): >>> orbit = bpms.positions.get() # Get the orbit or can be created by code using :py:class:`pyaml.arrays.bpm.BPM`. - """ def __init__(self, arrayName: str, bpms: list[BPM], use_aggregator=True): + """ + Initialize the BPMArray. + """ super().__init__(arrayName, bpms, use_aggregator) self.__hvpos = RWBPMPosition(arrayName, bpms) diff --git a/pyaml/arrays/cfm_magnet.py b/pyaml/arrays/cfm_magnet.py index f69ce658d..5526ed966 100644 --- a/pyaml/arrays/cfm_magnet.py +++ b/pyaml/arrays/cfm_magnet.py @@ -1,22 +1,37 @@ -from ..common.element_holder import ElementHolder -from .array import ArrayConfig, ArrayConfigModel - -# Define the main class name for this module -PYAMLCLASS = "CombinedFunctionMagnet" +""" +Cfm Magnet module. +This module provides cfm magnet functionality for the PyAML accelerator middle layer. +""" -class ConfigModel(ArrayConfigModel): - """Configuration model for Combined Function Magnet array.""" +from ..common.holders.element_holder import ElementHolder +from ..validation import DynamicValidation, register_schema +from .array import ArrayConfig - ... +# Define the main class name for this module +PYAMLCLASS = "CombinedFunctionMagnet" -class CombinedFunctionMagnet(ArrayConfig): +@register_schema +class CombinedFunctionMagnet(ArrayConfig, DynamicValidation): """ - Combined function magnet array confirguration + :py:class:`.CombinedFunctionMagnetArray` configuration. - Example + Parameters + ---------- + name : str + Name under which the array is registered and later looked up. + elements : list[str] + Element name patterns making up the array: literal names, ``fnmatch`` wildcards, or ``re:`` regular + expressions. + + Methods ------- + fill_array(holder) + Fill the combined function magnet array in the element holder. + + Examples + -------- A magnet array configuration can also be created by code using the following example:: @@ -28,8 +43,11 @@ class CombinedFunctionMagnet(ArrayConfig): ) """ - def __init__(self, cfg: ArrayConfigModel): - super().__init__(cfg) + def __init__(self, name: str, elements: list[str]): + """ + Initialize the CombinedFunctionMagnet. + """ + super().__init__(name, elements) def fill_array(self, holder: ElementHolder): """ @@ -40,4 +58,4 @@ def fill_array(self, holder: ElementHolder): holder : ElementHolder The element holder to populate with combined function magnet array """ - holder.fill_cfm_magnet_array(self._cfg.name, self._cfg.elements) + holder.combined_function_magnets.add(self._name, self._elements) diff --git a/pyaml/arrays/cfm_magnet_array.py b/pyaml/arrays/cfm_magnet_array.py index 539b6de5b..fcedc5b64 100644 --- a/pyaml/arrays/cfm_magnet_array.py +++ b/pyaml/arrays/cfm_magnet_array.py @@ -1,3 +1,9 @@ +""" +Combined function magnet array module. + +This module provides combined function magnet array functionality. +""" + import numpy as np from ..common.abstract import ReadWriteFloatArray @@ -9,13 +15,39 @@ class RWMagnetStrengths(ReadWriteFloatArray): + """ + Array accessor for the multipole strengths of combined-function magnets. + + Parameters + ---------- + name : str + Name of the array, used when the accessor is reported or logged. + magnets : list[CombinedFunctionMagnet] + Combined-function magnets making up the array; each contributes one entry per multipole. + + Methods + ------- + get() + Return the strength of every multipole, concatenated over the magnets. + set(value) + Set the strength of every multipole, concatenated over the magnets. + set_and_wait(value) + Set every multipole strength and wait for the readbacks to converge. + unit() + Return the strength unit of every multipole. + """ + def __init__(self, name: str, magnets: list[CombinedFunctionMagnet]): + """ + Initialize the RWMagnetStrengths. + """ self.__name = name self.__magnets = magnets self.__nb = sum(m.nb_multipole() for m in magnets) # Gets the values def get(self) -> np.array: + """Return the strength of every multipole, concatenated over the magnets.""" r = np.zeros(self.__nb) idx = 0 for m in self.__magnets: @@ -25,6 +57,14 @@ def get(self) -> np.array: # Sets the values def set(self, value: np.array): + """ + Set the strength of every multipole, concatenated over the magnets. + + Parameters + ---------- + value : np.array + Strength of every multipole, concatenated magnet by magnet. A scalar is broadcast to all of them. + """ nvalue = np.ones(self.__nb) * value if isinstance(value, float) else value idx = 0 for m in self.__magnets: @@ -33,10 +73,24 @@ def set(self, value: np.array): # Sets the values and waits that the read values reach their setpoint def set_and_wait(self, value: np.array): + """ + Set every multipole strength and wait for the readbacks to converge. + + Parameters + ---------- + value : np.array + Strength of every multipole, concatenated magnet by magnet. A scalar is broadcast to all of them. + + Raises + ------ + NotImplementedError + Waiting for readback convergence is not implemented for this accessor. + """ raise NotImplementedError("Not implemented yet.") # Gets the unit of the values def unit(self) -> list[str]: + """Return the strength unit of every multipole.""" r = [] for m in self.__magnets: r.extend(m.strengths.unit()) @@ -44,13 +98,39 @@ def unit(self) -> list[str]: class RWMagnetHardwares(ReadWriteFloatArray): + """ + Array accessor for the hardware values of combined-function magnets. + + Parameters + ---------- + name : str + Name of the array, used when the accessor is reported or logged. + magnets : list[CombinedFunctionMagnet] + Combined-function magnets making up the array; each contributes one entry per multipole. + + Methods + ------- + get() + Return the hardware value of every multipole, concatenated over the magnets. + set(value) + Set the hardware value of every multipole, concatenated over the magnets. + set_and_wait(value) + Set every hardware value and wait for the readbacks to converge. + unit() + Return the hardware unit of every multipole. + """ + def __init__(self, name: str, magnets: list[CombinedFunctionMagnet]): + """ + Initialize the RWMagnetHardwares. + """ self.__name = name self.__magnets = magnets self.__nb = sum(m.nb_multipole() for m in magnets) # Gets the values def get(self) -> np.array: + """Return the hardware value of every multipole, concatenated over the magnets.""" r = np.zeros(self.__nb) idx = 0 for m in self.__magnets: @@ -60,6 +140,14 @@ def get(self) -> np.array: # Sets the values def set(self, value: np.array): + """ + Set the hardware value of every multipole, concatenated over the magnets. + + Parameters + ---------- + value : np.array + Hardware value of every multipole, concatenated magnet by magnet. A scalar is broadcast to all of them. + """ nvalue = np.ones(self.__nb) * value if isinstance(value, float) else value idx = 0 for m in self.__magnets: @@ -68,10 +156,24 @@ def set(self, value: np.array): # Sets the values and waits that the read values reach their setpoint def set_and_wait(self, value: np.array): + """ + Set every hardware value and wait for the readbacks to converge. + + Parameters + ---------- + value : np.array + Hardware value of every multipole, concatenated magnet by magnet. A scalar is broadcast to all of them. + + Raises + ------ + NotImplementedError + Waiting for readback convergence is not implemented for this accessor. + """ raise NotImplementedError("Not implemented yet.") # Gets the unit of the values def unit(self) -> list[str]: + """Return the hardware unit of every multipole.""" r = [] for m in self.__magnets: r.extend(m.hardwares.unit()) @@ -86,12 +188,19 @@ class CombinedFunctionMagnetArray(ElementArray): ---------- arrayName : str Array name - magnets : list[Magnet] + magnets : list[CombinedFunctionMagnet] Magnet list, all elements must be attached to the same instance of either a Simulator or a ControlSystem. use_aggregator : bool - Use aggregator to increase performance by using paralell + Use aggregator to increase performance by using parallel access to underlying devices. + + Attributes + ---------- + strengths + Give access to strength of each magnet of this array + hardwares + Give access to hardware value of each magnet of this array """ def __init__( @@ -100,6 +209,9 @@ def __init__( magnets: list[CombinedFunctionMagnet], use_aggregator=False, ): + """ + Initialize the CombinedFunctionMagnetArray. + """ super().__init__(arrayName, magnets, use_aggregator) self.__rwstrengths = RWMagnetStrengths(arrayName, magnets) diff --git a/pyaml/arrays/element.py b/pyaml/arrays/element.py index 6a40d0275..6483f03de 100644 --- a/pyaml/arrays/element.py +++ b/pyaml/arrays/element.py @@ -1,20 +1,40 @@ -from ..common.element_holder import ElementHolder -from .array import ArrayConfig, ArrayConfigModel +""" +Element module. -# Define the main class name for this module -PYAMLCLASS = "Element" +This module provides element functionality. +""" +from ..common.holders.element_holder import ElementHolder +from ..validation import DynamicValidation, register_schema +from .array import ArrayConfig -class ConfigModel(ArrayConfigModel): - """Configuration model for :py:class:`.ElementArray`.""" +# Define the main class name for this module +PYAMLCLASS = "Element" -class Element(ArrayConfig): +@register_schema +class Element(ArrayConfig, DynamicValidation): """ :py:class:`.ElementArray` configuration. - Example + Parameters + ---------- + name : str + Name under which the array is registered and later looked up. + elements : list[str] + Element name patterns making up the array: literal names, ``fnmatch`` wildcards, or ``re:`` regular + expressions. + + Methods ------- + fill_array(holder) + Fill the :py:class:`.ElementArray` using element holder (:py:class:`~pyaml.lattice.simulator.Simulator` or + :py:class:`~pyaml.control.controlsystem.ControlSystem`) and add the array to the holder. This method is + called when an :py:class:`~pyaml.accelerator.Accelerator` is loaded but can be used to create arrays by + code as shown bellow: + + Examples + -------- An element array configuration can also be created by code using the following example: @@ -25,16 +45,16 @@ class Element(ArrayConfig): elt_cfg = Element( ElementArrayConfigModel(name="MyArray", elements=["BPM_C04-01","SH1A-C04-H"]) ) - - """ - def __init__(self, cfg: ArrayConfigModel): - super().__init__(cfg) + def __init__(self, name: str, elements: list[str]): + """ + Initialize the Element. + """ + super().__init__(name, elements) def fill_array(self, holder: ElementHolder): """ - Fill the :py:class:`.ElementArray` using element holder (:py:class:`~pyaml.lattice.simulator.Simulator` or :py:class:`~pyaml.control.controlsystem.ControlSystem`) @@ -54,4 +74,4 @@ def fill_array(self, holder: ElementHolder): holder : ElementHolder The element holder to populate with element array """ - holder.fill_element_array(self._cfg.name, self._cfg.elements) + holder.fill_element_array(self._name, self._elements) diff --git a/pyaml/arrays/element_array.py b/pyaml/arrays/element_array.py index 8ffae693b..26b7ce260 100644 --- a/pyaml/arrays/element_array.py +++ b/pyaml/arrays/element_array.py @@ -1,20 +1,29 @@ +""" +Element Array module. + +This module provides element array functionality. +""" + import fnmatch import importlib -from typing import Sequence +from typing import TYPE_CHECKING, Sequence import numpy as np from ..bpm.bpm import BPM -from ..common.element import Element +from ..common.element import Element, __pyaml_repr__ from ..common.exception import PyAMLException from ..magnet.cfm_magnet import CombinedFunctionMagnet from ..magnet.magnet import Magnet from ..magnet.serialized_magnet import SerializedMagnets +if TYPE_CHECKING: + from ..common.holders.element_holder import ElementHolder + class ElementArray(list[Element]): """ - Class that implements access to an element array + Class that implements access to an element array. Parameters ---------- @@ -24,11 +33,27 @@ class ElementArray(list[Element]): Element list, all elements must be attached to the same instance of either a Simulator or a ControlSystem. use_aggregator : bool - Use aggregator to increase performance by using paralell + Use aggregator to increase performance by using parallel access to underlying devices. - Example + Methods ------- + get_peer() + Returns the peer (:py:class:`~pyaml.lattice.simulator.Simulator` or + :py:class:`~pyaml.control.controlsystem.ControlSystem`) of an element list + get_name() + Returns the array name + names() + Returns the element names + mask_by_type(element_type) + Return a boolean mask indicating which elements are instances of the given type. + of_type(element_type) + Return a new array containing only elements of the given type. + exclude_type(element_type) + Return a copy of the array without the elements of a given type. + + Examples + -------- An array can be retrieved from the configuration as in the following example: @@ -36,10 +61,12 @@ class ElementArray(list[Element]): >>> sr = Accelerator.load("acc.yaml") >>> elements = sr.design.get_elements("QuadForTune") - """ def __init__(self, array_name: str, elements: list[Element], use_aggregator=True): + """ + Initialize the ElementArray. + """ super().__init__(i for i in elements) self.__name = array_name self.__peer = None @@ -53,7 +80,7 @@ def __init__(self, array_name: str, elements: list[Element], use_aggregator=True "of either a Simulator or a ControlSystem" ) - def get_peer(self): + def get_peer(self) -> "ElementHolder": """ Returns the peer (:py:class:`~pyaml.lattice.simulator.Simulator` or :py:class:`~pyaml.control.controlsystem.ControlSystem`) of @@ -73,7 +100,30 @@ def names(self) -> list[str]: """ return [e.get_name() for e in self] + def _pyaml_repr_fields(self) -> dict[str, object]: + return { + "name": self.get_name(), + "size": len(self), + "peer": self.get_peer(), + "elements": self.names(), + } + + def __repr__(self): + return __pyaml_repr__(self) + def __create_array(self, array_name: str, element_type: type, elements: list): + """ + Implement the __create_array protocol operation. + + Parameters + ---------- + array_name : str + Name given to the newly created array. + element_type : type + Common element type of ``elements``, used to pick the matching array class. + elements : list + Elements to place in the new array. + """ if element_type is None: element_type = Element @@ -99,6 +149,21 @@ def __create_array(self, array_name: str, element_type: type, elements: list): raise PyAMLException(f"Unsupported sliced array for type {str(element_type)}") def __eval_field(self, attribute_name: str, element: Element) -> str: + """ + Implement the __eval_field protocol operation. + + Parameters + ---------- + attribute_name : str + Attribute to read, resolved through the element's ``get_`` method. + element : Element + Element to read the attribute from. + + Returns + ------- + str + Attribute value, or ``None`` if the element has no such getter. + """ function_name = "get_" + attribute_name func = getattr(element, function_name, None) return func() if func is not None else "" @@ -117,7 +182,8 @@ def __ensure_compatible_operand(self, other: object) -> "ElementArray": return other def __auto_array(self, elements: list[Element]): - """Create the most specific array type for the given element list. + """ + Create the most specific array type for the given element list. The target element type is the most specific common base class (nearest common ancestor) of all elements. This supports heterogeneous subclasses (e.g., @@ -127,10 +193,30 @@ def __auto_array(self, elements: list[Element]): if len(elements) == 0: return [] + return self._typed_array(elements) + + def _typed_array(self, elements: list[Element]) -> "ElementArray": + """Build a collection using the most specific compatible array type. + + Parameters + ---------- + elements : list[Element] + Selected references, in their desired order. + + Returns + ------- + ElementArray + Specialized array when possible, otherwise a generic array. + An empty selection returns an empty generic array. + """ + if not elements: + return self.__create_array("", Element, elements) + import inspect def mro_as_list(cls: type) -> list[type]: # inspect.getmro returns (cls, ..., object) + """Return the class MRO, most specific first.""" return list(inspect.getmro(cls)) # Start from the first element MRO as reference order (most specific first). @@ -154,6 +240,22 @@ def mro_as_list(cls: type) -> list[type]: return self.__create_array("", chosen, elements) + def _select_names(self, pattern: str) -> "ElementArray": + """Select names without interpreting field selectors. + + Parameters + ---------- + pattern : str + A fnmatch pattern applied to each element name. + + Returns + ------- + ElementArray + Typed selection in the original order, including an empty array + when no names match. + """ + return self._typed_array([element for element in self if fnmatch.fnmatch(element.get_name(), pattern)]) + def __is_bool_mask(self, other: object) -> bool: """Return True if 'other' looks like a boolean mask (list or numpy array).""" # --- numpy boolean array --- @@ -216,7 +318,6 @@ def __and__(self, other: object): :py:class:`.CombinedFunctionMagnetArray` or :py:class:`.SerializedMagnetsArray` or :py:class:`.ElementArray`. - """ # --- mask filtering --- if self.__is_bool_mask(other): @@ -237,6 +338,14 @@ def __and__(self, other: object): def __rand__(self, other: object): # Support "array on the right" for array operands; for masks, we don't enforce # commutativity. + """ + Implement the __rand__ protocol operation. + + Parameters + ---------- + other : object + Left-hand operand, evaluated when it does not implement the operation itself. + """ if isinstance(other, ElementArray): return other.__and__(self) return NotImplemented @@ -281,7 +390,6 @@ def __sub__(self, other: object): :py:class:`.CombinedFunctionMagnetArray` or :py:class:`.SerializedMagnetsArray` or :py:class:`.ElementArray`. - """ # --- mask removal --- if self.__is_bool_mask(other): @@ -307,14 +415,10 @@ def __or__(self, other: object): Order is stable: elements from ``self`` first, followed by elements from ``other`` that are not already present. - Example - ------- - - .. code-block:: python - - >>> hcorr = sr.live.get_magnets("HCORR") - >>> vcorr = sr.live.get_magnets("VCORR") - >>> all_corr = hcorr | vcorr + Parameters + ---------- + other : ElementArray or list[Element] + Array whose elements are combined with this one. Returns ------- @@ -327,6 +431,14 @@ def __or__(self, other: object): :py:class:`.SerializedMagnetsArray` or :py:class:`.ElementArray`. + Examples + -------- + + .. code-block:: python + + >>> hcorr = sr.live.get_magnets("HCORR") + >>> vcorr = sr.live.get_magnets("VCORR") + >>> all_corr = hcorr | vcorr """ other_arr = self.__ensure_compatible_operand(other) @@ -348,6 +460,14 @@ def __or__(self, other: object): return self.__auto_array(res) def __ror__(self, other: object): + """ + Implement the __ror__ protocol operation. + + Parameters + ---------- + other : object + Left-hand operand, evaluated when it does not implement the operation itself. + """ if isinstance(other, ElementArray): return other.__or__(self) return NotImplemented @@ -356,12 +476,10 @@ def __add__(self, other: object): """ Alias for the union operator ``|``. - Example - ------- - - .. code-block:: python - - >>> all_corr = hcorr + vcorr + Parameters + ---------- + other : ElementArray or list[Element] + Array whose elements are combined with this one. Returns ------- @@ -374,16 +492,31 @@ def __add__(self, other: object): :py:class:`.SerializedMagnetsArray` or :py:class:`.ElementArray`. + Examples + -------- + + .. code-block:: python + + >>> all_corr = hcorr + vcorr """ return self.__or__(other) def __radd__(self, other: object): + """ + Implement the __radd__ protocol operation. + + Parameters + ---------- + other : object + Left-hand operand, evaluated when it does not implement the operation itself. + """ if isinstance(other, ElementArray): return other.__add__(self) return NotImplemented def mask_by_type(self, element_type: type) -> list[bool]: - """Return a boolean mask indicating which elements are instances of the given + """ + Return a boolean mask indicating which elements are instances of the given type. Parameters @@ -403,7 +536,8 @@ def mask_by_type(self, element_type: type) -> list[bool]: return [isinstance(e, element_type) for e in self] def of_type(self, element_type: type): - """Return a new array containing only elements of the given type. + """ + Return a new array containing only elements of the given type. The resulting array is automatically typed according to the most specific common base class of the filtered elements. @@ -426,51 +560,62 @@ def of_type(self, element_type: type): return self.__auto_array(filtered) def exclude_type(self, element_type): + """ + Return a copy of the array without the elements of a given type. + + Parameters + ---------- + element_type : object + Element type to drop; instances of its subclasses are dropped as well. + """ mask = self.mask_by_type(element_type) return self - mask def __getitem__(self, key): + """Return an element or a selection typed by its common element class. + + Parameters + ---------- + key : int, slice or str + Element index, slice, name pattern, or existing field selector. + + Returns + ------- + Element or ElementArray + Indexed element or an array inferred from all selected elements. + Different Magnet subclasses produce a MagnetArray; mixed element + families produce an ElementArray. Empty selections return an + empty ElementArray. + + Examples + -------- + >>> magnets = sr.design.magnets.get() + >>> subset = magnets[:] # MagnetArray, including mixed magnet classes + >>> correctors = magnets["SH*"] # MagnetArray + """ if isinstance(key, slice): # Slicing - element_type = None - r = [] - for i in range(*key.indices(len(self))): - if element_type is None: - element_type = type(self[i]) - elif not isinstance(self[i], element_type): - element_type = Element # Fall back to element - r.append(self[i]) - return self.__create_array("", element_type, r) + r = super().__getitem__(key) elif isinstance(key, str): fields = key.split(":") if len(fields) <= 1: # Selection by name - element_type = None r = [] for e in self: if fnmatch.fnmatch(e.get_name(), key): - if element_type is None: - element_type = type(e) - elif not isinstance(e, element_type): - element_type = Element # Fall back to element r.append(e) else: # Selection by fields - element_type = None r = [] for e in self: txt = self.__eval_field(fields[0], e) if fnmatch.fnmatch(txt, fields[1]): - if element_type is None: - element_type = type(e) - elif not isinstance(e, element_type): - element_type = Element # Fall back to element r.append(e) - return self.__create_array("", element_type, r) - else: # Default to super selection return super().__getitem__(key) + + return self.__auto_array(r) if r else self.__create_array("", Element, r) diff --git a/pyaml/arrays/magnet.py b/pyaml/arrays/magnet.py index d65282cd6..c37d21693 100644 --- a/pyaml/arrays/magnet.py +++ b/pyaml/arrays/magnet.py @@ -1,22 +1,37 @@ -from ..common.element_holder import ElementHolder -from .array import ArrayConfig, ArrayConfigModel - -# Define the main class name for this module -PYAMLCLASS = "Magnet" +""" +Magnet module. +This module provides magnet functionality for the PyAML accelerator middle layer. +""" -class ConfigModel(ArrayConfigModel): - """Configuration model for Magnet array.""" +from ..common.holders.element_holder import ElementHolder +from ..validation import DynamicValidation, register_schema +from .array import ArrayConfig - ... +# Define the main class name for this module +PYAMLCLASS = "Magnet" -class Magnet(ArrayConfig): +@register_schema +class Magnet(ArrayConfig, DynamicValidation): """ - Magnet array confirguration + :py:class:`.MagnetArray` configuration. - Example + Parameters + ---------- + name : str + Name under which the array is registered and later looked up. + elements : list[str] + Element name patterns making up the array: literal names, ``fnmatch`` wildcards, or ``re:`` regular + expressions. + + Methods ------- + fill_array(holder) + Fill the magnet array in the element holder. + + Examples + -------- A magnet array configuration can also be created by code using the following example:: @@ -27,8 +42,11 @@ class Magnet(ArrayConfig): ) """ - def __init__(self, cfg: ArrayConfigModel): - super().__init__(cfg) + def __init__(self, name: str, elements: list[str]): + """ + Initialize the Magnet. + """ + super().__init__(name, elements) def fill_array(self, holder: ElementHolder): """ @@ -39,4 +57,4 @@ def fill_array(self, holder: ElementHolder): holder : ElementHolder The element holder to populate with magnet array """ - holder.fill_magnet_array(self._cfg.name, self._cfg.elements) + holder.magnets.add(self._name, self._elements) diff --git a/pyaml/arrays/magnet_array.py b/pyaml/arrays/magnet_array.py index 5c7f65044..b24a956f4 100644 --- a/pyaml/arrays/magnet_array.py +++ b/pyaml/arrays/magnet_array.py @@ -1,3 +1,9 @@ +""" +Magnet Array module. + +This module provides magnet array functionality for the PyAML accelerator middle layer. +""" + import numpy as np from ..common.abstract import ReadWriteFloatArray @@ -7,7 +13,34 @@ class RWMagnetStrength(ReadWriteFloatArray): + """ + Array accessor for the strengths of a magnet family. + + Parameters + ---------- + name : str + Name of the array, used when the accessor is reported or logged. + magnets : list[Magnet] + Magnets making up the array, in the order their values are read and written. + + Methods + ------- + get() + Return the strength of every magnet in the array. + set(value) + Set the strength of every magnet in the array. + set_and_wait(value) + Set every strength and wait for the readbacks to converge. + unit() + Return the strength unit of every magnet in the array. + set_aggregator(agg) + Install an aggregator so the array is read and written in a single call. + """ + def __init__(self, name: str, magnets: list[Magnet]): + """ + Initialize the RWMagnetStrength. + """ self.__name = name self.__magnets = magnets self.__nb = len(self.__magnets) @@ -15,6 +48,7 @@ def __init__(self, name: str, magnets: list[Magnet]): # Gets the values def get(self) -> np.array: + """Return the strength of every magnet in the array.""" if not self.__aggregator: return np.array([m.strength.get() for m in self.__magnets]) else: @@ -22,6 +56,14 @@ def get(self) -> np.array: # Sets the values def set(self, value: np.array): + """ + Set the strength of every magnet in the array. + + Parameters + ---------- + value : np.array + Strength for each magnet, ordered like the array. A scalar is broadcast to every magnet. + """ nvalue = np.ones(self.__nb) * value if isinstance(value, float) else value if not self.__aggregator: for idx, m in enumerate(self.__magnets): @@ -31,19 +73,69 @@ def set(self, value: np.array): # Sets the values and waits that the read values reach their setpoint def set_and_wait(self, value: np.array): + """ + Set every strength and wait for the readbacks to converge. + + Parameters + ---------- + value : np.array + Strength for each magnet, ordered like the array. A scalar is broadcast to every magnet. + + Raises + ------ + NotImplementedError + Waiting for readback convergence is not implemented for this accessor. + """ raise NotImplementedError("Not implemented yet.") # Gets the unit of the values def unit(self) -> list[str]: + """Return the strength unit of every magnet in the array.""" return [m.strength.unit() for m in self.__magnets] # Set the aggregator (Control system only) def set_aggregator(self, agg: ScalarAggregator): + """ + Install an aggregator so the array is read and written in a single call. + + Parameters + ---------- + agg : ScalarAggregator + Aggregator performing grouped device access. Only available on the control-system side; ``None`` + restores per-magnet access. + """ self.__aggregator = agg class RWMagnetHardware(ReadWriteFloatArray): + """ + Array accessor for the hardware values of a magnet family. + + Parameters + ---------- + name : str + Name of the array, used when the accessor is reported or logged. + magnets : list[Magnet] + Magnets making up the array, in the order their values are read and written. + + Methods + ------- + get() + Return the hardware value of every magnet in the array. + set(value) + Set the hardware value of every magnet in the array. + set_and_wait(value) + Set every hardware value and wait for the readbacks to converge. + unit() + Return the hardware unit of every magnet in the array. + set_aggregator(agg) + Install an aggregator so the array is read and written in a single call. + """ + def __init__(self, name: str, magnets: list[Magnet]): + """ + Initialize the RWMagnetHardware. + """ self.__name = name self.__magnets = magnets self.__nb = len(self.__magnets) @@ -51,6 +143,7 @@ def __init__(self, name: str, magnets: list[Magnet]): # Gets the values def get(self) -> np.array: + """Return the hardware value of every magnet in the array.""" if not self.__aggregator: return np.array([m.hardware.get() for m in self.__magnets]) else: @@ -58,6 +151,14 @@ def get(self) -> np.array: # Sets the values def set(self, value: np.array): + """ + Set the hardware value of every magnet in the array. + + Parameters + ---------- + value : np.array + Hardware value for each magnet, ordered like the array. A scalar is broadcast to every magnet. + """ nvalue = np.ones(self.__nb) * value if isinstance(value, float) else value if not self.__aggregator: for idx, m in enumerate(self.__magnets): @@ -67,20 +168,43 @@ def set(self, value: np.array): # Sets the values and waits that the read values reach their setpoint def set_and_wait(self, value: np.array): + """ + Set every hardware value and wait for the readbacks to converge. + + Parameters + ---------- + value : np.array + Hardware value for each magnet, ordered like the array. A scalar is broadcast to every magnet. + + Raises + ------ + NotImplementedError + Waiting for readback convergence is not implemented for this accessor. + """ raise NotImplementedError("Not implemented yet.") # Gets the unit of the values def unit(self) -> list[str]: + """Return the hardware unit of every magnet in the array.""" return [m.hardware.unit() for m in self.__magnets] # Set the aggregator def set_aggregator(self, agg: ScalarAggregator): + """ + Install an aggregator so the array is read and written in a single call. + + Parameters + ---------- + agg : ScalarAggregator + Aggregator performing grouped device access. Only available on the control-system side; ``None`` + restores per-magnet access. + """ self.__aggregator = agg class MagnetArray(ElementArray): """ - Class that implements access to a magnet array + Class that implements access to a magnet array. Parameters ---------- @@ -91,19 +215,28 @@ class MagnetArray(ElementArray): either a Simulator or a ControlSystem. use_aggregator : bool Use aggregator to increase performance by using - paralell access to underlying devices. + parallel access to underlying devices. - Example - ------- + Attributes + ---------- + strengths + Give access to strength of each magnet of this array + hardwares + Give access to hardware value of each magnet of this array + + Examples + -------- An array can be retrieved from the configuration as in the following example:: sr = Accelerator.load("acc.yaml") quads = sr.design.get_magnets("QuadForTune") - """ def __init__(self, arrayName: str, magnets: list[Magnet], use_aggregator=True): + """ + Initialize the MagnetArray. + """ super().__init__(arrayName, magnets, use_aggregator) self.__rwstrengths = RWMagnetStrength(arrayName, magnets) diff --git a/pyaml/arrays/serialized_magnet.py b/pyaml/arrays/serialized_magnet.py index fd4124036..5f3c07a3a 100644 --- a/pyaml/arrays/serialized_magnet.py +++ b/pyaml/arrays/serialized_magnet.py @@ -1,22 +1,37 @@ -from ..common.element_holder import ElementHolder -from .array import ArrayConfig, ArrayConfigModel - -# Define the main class name for this module -PYAMLCLASS = "SerializedMagnets" +""" +Serialized Magnet module. +This module provides serialized magnet functionality. +""" -class ConfigModel(ArrayConfigModel): - """Configuration model for Serialized Magnets array.""" +from ..common.holders.element_holder import ElementHolder +from ..validation import DynamicValidation, register_schema +from .array import ArrayConfig - ... +# Define the main class name for this module +PYAMLCLASS = "SerializedMagnets" -class SerializedMagnets(ArrayConfig): +@register_schema +class SerializedMagnets(ArrayConfig, DynamicValidation): """ - Serialized magnets array configuration + Serialized magnets array configuration. - Example + Parameters + ---------- + name : str + Name under which the array is registered and later looked up. + elements : list[str] + Element name patterns making up the array: literal names, ``fnmatch`` wildcards, or ``re:`` regular + expressions. + + Methods ------- + fill_array(holder) + Fill the serialized magnet array in the element holder. + + Examples + -------- A magnet array configuration can also be created by code using the following example:: @@ -28,8 +43,11 @@ class SerializedMagnets(ArrayConfig): ) """ - def __init__(self, cfg: ArrayConfigModel): - super().__init__(cfg) + def __init__(self, name: str, elements: list[str]): + """ + Initialize the SerializedMagnets. + """ + super().__init__(name, elements) def fill_array(self, holder: ElementHolder): """ @@ -40,4 +58,4 @@ def fill_array(self, holder: ElementHolder): holder : ElementHolder The element holder to populate with serialized magnet array """ - holder.fill_serialized_magnet_array(self._cfg.name, self._cfg.elements) + holder.serialized_magnets.add(self._name, self._elements) diff --git a/pyaml/arrays/serialized_magnet_array.py b/pyaml/arrays/serialized_magnet_array.py index c436e0164..c891e5c6a 100644 --- a/pyaml/arrays/serialized_magnet_array.py +++ b/pyaml/arrays/serialized_magnet_array.py @@ -1,3 +1,9 @@ +""" +Serialized Magnet Array module. + +This module provides serialized magnet array functionality. +""" + import numpy as np from ..common.abstract import ReadWriteFloatArray @@ -9,27 +15,75 @@ class RWMagnetStrengths(ReadWriteFloatArray): + """ + Array accessor for the strengths of serialized magnet groups. + + Parameters + ---------- + name : str + Name of the array, used when the accessor is reported or logged. + magnets : list[SerializedMagnets] + Serialized magnet groups making up the array, in the order their values are read and written. + + Methods + ------- + get() + Return the shared strength of every serialized group. + set(value) + Set the shared strength of every serialized group. + set_and_wait(value) + Set every shared strength and wait for the readbacks to converge. + unit() + Return the strength unit of every serialized group. + """ + def __init__(self, name: str, magnets: list[SerializedMagnets]): + """ + Initialize the RWMagnetStrengths. + """ self.__name = name self.__magnets = magnets self.__nb = sum(m.get_nb_magnets() for m in magnets) # Gets the values def get(self) -> np.array: + """Return the shared strength of every serialized group.""" return np.array([m.strength.get() for m in self.__magnets]) # Sets the values def set(self, value: np.array): + """ + Set the shared strength of every serialized group. + + Parameters + ---------- + value : np.array + Shared strength for each serialized group, ordered like the array. + """ nvalue = np.ones(len(self.__magnets)) * value if isinstance(value, float) else value for value, m in zip(nvalue, self.__magnets, strict=True): m.strength.set(value) # Sets the values and waits that the read values reach their setpoint def set_and_wait(self, value: np.array): + """ + Set every shared strength and wait for the readbacks to converge. + + Parameters + ---------- + value : np.array + Shared strength for each serialized group, ordered like the array. + + Raises + ------ + NotImplementedError + Waiting for readback convergence is not implemented for this accessor. + """ raise NotImplementedError("Not implemented yet.") # Gets the unit of the values def unit(self) -> list[str]: + """Return the strength unit of every serialized group.""" r = [] for m in self.__magnets: r.extend(m.strength.unit()) @@ -37,27 +91,75 @@ def unit(self) -> list[str]: class RWMagnetHardwares(ReadWriteFloatArray): + """ + Array accessor for the hardware values of serialized magnet groups. + + Parameters + ---------- + name : str + Name of the array, used when the accessor is reported or logged. + magnets : list[SerializedMagnets] + Serialized magnet groups making up the array, in the order their values are read and written. + + Methods + ------- + get() + Return the shared hardware value of every serialized group. + set(value) + Set the shared hardware value of every serialized group. + set_and_wait(value) + Set every shared hardware value and wait for the readbacks to converge. + unit() + Return the hardware unit of every serialized group. + """ + def __init__(self, name: str, magnets: list[SerializedMagnets]): + """ + Initialize the RWMagnetHardwares. + """ self.__name = name self.__magnets = magnets self.__nb = sum(m.get_nb_magnets() for m in magnets) # Gets the values def get(self) -> np.array: + """Return the shared hardware value of every serialized group.""" return np.array([m.hardware.get() for m in self.__magnets]) # Sets the values def set(self, value: np.array): + """ + Set the shared hardware value of every serialized group. + + Parameters + ---------- + value : np.array + Shared hardware value for each serialized group, ordered like the array. + """ nvalue = np.ones(len(self.__magnets)) * value if isinstance(value, float) else value for value, m in zip(nvalue, self.__magnets, strict=True): m.hardware.set(value) # Sets the values and waits that the read values reach their setpoint def set_and_wait(self, value: np.array): + """ + Set every shared hardware value and wait for the readbacks to converge. + + Parameters + ---------- + value : np.array + Shared hardware value for each serialized group, ordered like the array. + + Raises + ------ + NotImplementedError + Waiting for readback convergence is not implemented for this accessor. + """ raise NotImplementedError("Not implemented yet.") # Gets the unit of the values def unit(self) -> list[str]: + """Return the hardware unit of every serialized group.""" r = [] for m in self.__magnets: r.extend(m.hardware.unit()) @@ -72,12 +174,19 @@ class SerializedMagnetsArray(ElementArray): ---------- arrayName : str Array name - magnets : list[Magnet] + magnets : list[SerializedMagnets] Magnet list, all elements must be attached to the same instance of either a Simulator or a ControlSystem. use_aggregator : bool Use aggregator to increase performance by using parallel access to underlying devices. + + Attributes + ---------- + strengths + Give access to strength of each magnet of this array + hardwares + Give access to hardware value of each magnet of this array """ def __init__( @@ -86,6 +195,9 @@ def __init__( magnets: list[SerializedMagnets], use_aggregator=False, ): + """ + Initialize the SerializedMagnetsArray. + """ super().__init__(arrayName, magnets, use_aggregator) self.__rwstrengths = RWMagnetStrengths(arrayName, magnets) diff --git a/pyaml/bpm/__init__.py b/pyaml/bpm/__init__.py new file mode 100644 index 000000000..e69de29bb diff --git a/pyaml/bpm/bpm.py b/pyaml/bpm/bpm.py index 1a14f4b9b..dd7015c2e 100644 --- a/pyaml/bpm/bpm.py +++ b/pyaml/bpm/bpm.py @@ -1,129 +1,155 @@ -from ..bpm.bpm_model import BPMModel -from ..common.element import Element, ElementConfigModel +"""Beam-position monitor elements and their runtime interfaces.""" + +import copy +from typing import TYPE_CHECKING, Self + +from ..common.abstract import ReadFloatArray, ReadWriteFloatArray, ReadWriteFloatScalar +from ..common.element import Element, __pyaml_repr__ from ..common.exception import PyAMLException -from ..lattice.abstract_impl import RBpmArray, RWBpmOffsetArray, RWBpmTiltScalar +from ..validation import DynamicValidation, register_schema -try: - from typing import Self # Python 3.11+ -except ImportError: - from typing_extensions import Self # Python 3.10 and earlier +if TYPE_CHECKING: + from ..common.holders.element_holder import ElementHolder PYAMLCLASS = "BPM" -class ConfigModel(ElementConfigModel): - """ - Configuration model for BPM element. - - Attributes - ---------- - model : BPMModel or None, optional - Object in charge of BPM modeling +@register_schema +class BPM(Element, DynamicValidation): """ + Beam position monitor (BPM) element. - model: BPMModel | None = None + Represents a BPM in the accelerator lattice and provides access to its + associated readback signals, including horizontal and vertical beam + positions, calibration offsets, and mechanical tilt. + Parameters + ---------- + name : str + Name of the BPM. + lattice_names : str | None, optional + Lattice-specific name or names identifying the BPM. + description : str | None, optional + Description of the BPM. + x_pos : str | None, optional + Device catalog key for the horizontal beam position. + y_pos : str | None, optional + Device catalog key for the vertical beam position. + x_offset : str | None, optional + Device catalog key for the horizontal BPM offset. + y_offset : str | None, optional + Device catalog key for the vertical BPM offset. + tilt : str | None, optional + Device catalog key for the BPM tilt. -class BPM(Element): - """ - Class providing access to one BPM of a physical or simulated lattice + Attributes + ---------- + positions + Read accessor for the horizontal and vertical beam positions, in metres. + offset + Read/write accessor for the two calibration offsets, in metres. + tilt + Read/write accessor for the mechanical tilt, in radians. + + Methods + ------- + attach(peer, positions, offset, tilt) + Attach BPM attributes to a peer. + get_pos_devices() + Return configured device keys used for position readback. + get_tilt_device() + Return the configured device key used for tilt access. + get_offset_devices() + Return configured device keys used for offset control. """ - def __init__(self, cfg: ConfigModel): - """ - Construct a BPM - - Parameters - ---------- - name : str - Element name - model : BPMModel - BPM model in charge of computing beam position - """ - - super().__init__(cfg.name) - - self.__model = cfg.model if hasattr(cfg, "model") else None - self._cfg = cfg - self.__positions = None - self.__offset = None - self.__tilt = None - - @property - def model(self) -> BPMModel: + def __init__( + self, + name: str, + lattice_names: str | None = None, + description: str | None = None, + x_pos: str | None = None, + y_pos: str | None = None, + x_offset: str | None = None, + y_offset: str | None = None, + tilt: str | None = None, + ): """ - Get the BPM model. - - Returns - ------- - BPMModel - The BPM model instance + Initialize a beam-position monitor configuration. """ - return self.__model + super().__init__(name, lattice_names, description) + self.x_pos = x_pos + self.y_pos = y_pos + self.x_offset = x_offset + self.y_offset = y_offset + self.tilt_name = tilt + self._positions = None + self._offset = None + self._tilt = None @property - def positions(self) -> RBpmArray: + def positions(self) -> ReadFloatArray: """ Get the BPM position readings. Returns ------- - RBpmArray - BPM position array containing horizontal and vertical positions + ReadFloatArray + Read-only array containing horizontal and vertical positions. Raises ------ PyAMLException If positions have not been attached """ - if self.__positions is None: + if self._positions is None: raise PyAMLException(f"{str(self)} has no attached positions") - return self.__positions + return self._positions @property - def offset(self) -> RWBpmOffsetArray: + def offset(self) -> ReadWriteFloatArray: """ Get the BPM offset values. Returns ------- - RWBpmOffsetArray - BPM offset array for position correction + ReadWriteFloatArray + Read/write array containing horizontal and vertical offsets. Raises ------ PyAMLException If offset has not been attached """ - if self.__offset is None: + if self._offset is None: raise PyAMLException(f"{str(self)} has no attached offset") - return self.__offset + return self._offset @property - def tilt(self) -> RWBpmTiltScalar: + def tilt(self) -> ReadWriteFloatScalar: """ Get the BPM tilt angle. Returns ------- - RWBpmTiltScalar - BPM tilt angle for rotation correction + ReadWriteFloatScalar + Read/write BPM tilt angle used for rotation correction. Raises ------ PyAMLException If tilt has not been attached """ - if self.__tilt is None: + if self._tilt is None: raise PyAMLException(f"{str(self)} has no attached tilt") - return self.__tilt + return self._tilt def attach( self, peer, - positions: RBpmArray, - offset: RWBpmOffsetArray, - tilt: RWBpmTiltScalar, + positions: ReadFloatArray, + offset: ReadWriteFloatArray, + tilt: ReadWriteFloatScalar, ) -> Self: """ Attach BPM attributes to a peer. @@ -131,25 +157,66 @@ def attach( Parameters ---------- peer : object - The peer object (simulator or control system) + Simulator or control-system peer. positions : RBpmArray - BPM position readings + Read-only horizontal and vertical position interface. offset : RWBpmOffsetArray - BPM offset values for correction + Read/write horizontal and vertical offset interface. tilt : RWBpmTiltScalar - BPM tilt angle for rotation correction + Read/write tilt interface. Returns ------- Self - A new attached instance of BPM + Shallow copy of this BPM bound to ``peer`` and its interfaces. """ # Attach positions, offset and tilt attributes and returns a new # reference - obj = self.__class__(self._cfg) - obj.__model = self.__model - obj.__positions = positions - obj.__offset = offset - obj.__tilt = tilt + obj = copy.copy(self) + obj._positions = positions + obj._offset = offset + obj._tilt = tilt obj._peer = peer return obj + + def _fill_device(self, holder: "ElementHolder") -> None: + holder._fill_bpm(self) + + def get_pos_devices(self) -> list[str | None]: + """ + Return configured device keys used for position readback. + + Returns + ------- + list of str or None + Horizontal and vertical position device keys. + """ + return [self.x_pos, self.y_pos] + + def get_tilt_device(self) -> str | None: + """ + Return the configured device key used for tilt access. + + Returns + ------- + str or None + Tilt device key. + """ + return self.tilt_name + + def get_offset_devices(self) -> list[str | None]: + """ + Return configured device keys used for offset control. + + Returns + ------- + list of str or None + Horizontal and vertical offset device keys. + """ + return [self.x_offset, self.y_offset] + + def __repr__(self): + """ + Implement the ``__repr__`` string. + """ + return __pyaml_repr__(self, exclude=["positions", "offset", "tilt"]) diff --git a/pyaml/bpm/bpm_model.py b/pyaml/bpm/bpm_model.py deleted file mode 100644 index e00c2aa3b..000000000 --- a/pyaml/bpm/bpm_model.py +++ /dev/null @@ -1,147 +0,0 @@ -from abc import ABCMeta, abstractmethod - -import numpy as np -from numpy.typing import NDArray - -from ..control.deviceaccess import DeviceAccess - - -class BPMModel(metaclass=ABCMeta): - """ - Abstract class providing interface to accessing BPM positions, offsets, - tilts. - """ - - @abstractmethod - def get_pos_devices(self) -> list[DeviceAccess | None]: - """ - Get device handles used for position reading - - Returns - ------- - list[DeviceAccess] - h and v position devices - """ - pass - - @abstractmethod - def get_tilt_device(self) -> DeviceAccess | None: - """ - Get device handle used for tilt access - - Returns - ------- - list[DeviceAccess] - tilt device - """ - pass - - @abstractmethod - def get_offset_devices(self) -> list[DeviceAccess | None]: - """ - Get device handles used for offset access - - Returns - ------- - list[DeviceAccess] - h and v offset devices - """ - pass - - def x_pos_index(self) -> int | None: - """ - Returns the index of the horizontal position in - an array, otherwise a scalar value is expected from the - corresponding DeviceAccess - - Returns - ------- - int - Index in the array, None for a scalar value - """ - return None - - def y_pos_index(self) -> int | None: - """ - Returns the index of the veritcal position in - an array, otherwise a scalar value is expected from the - corresponding DeviceAccess - - Returns - ------- - int - Index in the array, None for a scalar value - """ - return None - - def is_pos_indexed(self) -> bool: - """ - Check if position values are indexed (array-based). - - Returns - ------- - bool - True if both x and y positions are indexed, False otherwise - """ - return self.x_pos_index() is not None and self.y_pos_index() is not None - - def tilt_index(self) -> int | None: - """ - Returns the index of the tilt angle in - an array, otherwise a scalar value is expected from the - corresponding DeviceAccess - - Returns - ------- - int - Index in the array, None for a scalar value - """ - return None - - def is_tilt_indexed(self) -> bool: - """ - Check if tilt value is indexed (array-based). - - Returns - ------- - bool - True if tilt is indexed, False otherwise - """ - return self.tilt_index() is not None - - def x_offset_index(self) -> int | None: - """ - Returns the index of the horizontal offset in - an array, otherwise a scalar value is expected from the - corresponding DeviceAccess - - Returns - ------- - int - Index in the array, None for a scalar value - """ - return None - - def y_offset_index(self) -> int | None: - """ - Returns the index of the veritcal offset in - an array, otherwise a scalar value is expected from the - corresponding DeviceAccess - - Returns - ------- - int - Index in the array, None for a scalar value - """ - return None - - def is_offset_indexed(self) -> bool: - """ - Check if offset values are indexed (array-based). - - Returns - ------- - bool - True if both x and y offsets are indexed, False otherwise - """ - return self.x_offset_index() is not None and self.y_offset_index() is not None diff --git a/pyaml/bpm/bpm_simple_model.py b/pyaml/bpm/bpm_simple_model.py deleted file mode 100644 index 582a60254..000000000 --- a/pyaml/bpm/bpm_simple_model.py +++ /dev/null @@ -1,111 +0,0 @@ -import numpy as np -from numpy.typing import NDArray -from pydantic import BaseModel, ConfigDict - -from pyaml.bpm.bpm_model import BPMModel - -from ..common.element import __pyaml_repr__ -from ..control.deviceaccess import DeviceAccess - -# Define the main class name for this module -PYAMLCLASS = "BPMSimpleModel" - - -class ConfigModel(BaseModel): - """ - Configuration model for BPM simple model - - Parameters - ---------- - x_pos : DeviceAccess, optional - Horizontal position device - y_pos : DeviceAccess, optional - Vertical position device - x_pos_index : int, optional - Index in the array when specified, otherwise scalar - value is expected - y_pos_index : int, optional - Index in the array when specified, otherwise scalar - value is expected - """ - - model_config = ConfigDict(arbitrary_types_allowed=True, extra="forbid") - - x_pos: DeviceAccess | None - y_pos: DeviceAccess | None - x_pos_index: int | None = None - y_pos_index: int | None = None - - -class BPMSimpleModel(BPMModel): - """ - Concrete implementation of BPMModel that simulates a BPM with tilt and - offset values. - """ - - def __init__(self, cfg: ConfigModel): - self._cfg = cfg - self.__x_pos = cfg.x_pos - self.__y_pos = cfg.y_pos - - def get_pos_devices(self) -> list[DeviceAccess | None]: - """ - Get device handles used for position reading - - Returns - ------- - list[DeviceAccess] - Array of DeviceAcess - """ - return [self.__x_pos, self.__y_pos] - - def get_tilt_device(self) -> DeviceAccess | None: - """ - Get device handle used for tilt access - - Returns - ------- - list[DeviceAccess] - Array of DeviceAcess - """ - return None - - def get_offset_devices(self) -> list[DeviceAccess | None]: - """ - Get device handles used for offset access - - Returns - ------- - list[DeviceAccess] - Array of DeviceAcess - """ - return [None, None] - - def x_pos_index(self) -> int | None: - """ - Returns the index of the horizontal position in - an array, otherwise a scalar value is expected from the - corresponding DeviceAccess - - Returns - ------- - int - Index in the array, None for a scalar value - """ - return self._cfg.x_pos_index - - def y_pos_index(self) -> int | None: - """ - Returns the index of the veritcal position in - an array, otherwise a scalar value is expected from the - corresponding DeviceAccess - - Returns - ------- - int - Index in the array, None for a scalar value - """ - return self._cfg.y_pos_index - - def __repr__(self): - return __pyaml_repr__(self) diff --git a/pyaml/bpm/bpm_tiltoffset_model.py b/pyaml/bpm/bpm_tiltoffset_model.py deleted file mode 100644 index 6bccbd8cf..000000000 --- a/pyaml/bpm/bpm_tiltoffset_model.py +++ /dev/null @@ -1,94 +0,0 @@ -import numpy as np -from numpy.typing import NDArray -from pydantic import BaseModel, ConfigDict - -from pyaml.bpm.bpm_model import BPMModel -from pyaml.bpm.bpm_simple_model import BPMSimpleModel - -from ..common.element import __pyaml_repr__ -from ..control.deviceaccess import DeviceAccess - -# Define the main class name for this module -PYAMLCLASS = "BPMTiltOffsetModel" - -# TODO: Implepement indexed offset and tilt - - -class ConfigModel(BaseModel): - """ - Configuration model for BPM with tilt and offset - - Parameters - ---------- - x_pos : DeviceAccess, optional - Horizontal position device - y_pos : DeviceAccess, optional - Vertical position device - x_offset : DeviceAccess, optional - Horizontal BPM offset device - y_offset : DeviceAccess, optional - Vertical BPM offset device - tilt : DeviceAccess, optional - BPM tilt device - """ - - model_config = ConfigDict(arbitrary_types_allowed=True, extra="forbid") - - x_pos: DeviceAccess | None - y_pos: DeviceAccess | None - x_pos_index: int | None = None - y_pos_index: int | None = None - x_offset: DeviceAccess | None - y_offset: DeviceAccess | None - tilt: DeviceAccess | None - - -class BPMTiltOffsetModel(BPMSimpleModel): - """ - Concrete implementation of BPMModel that simulates a BPM with tilt and - offset values. - """ - - def __init__(self, cfg: ConfigModel): - super().__init__(cfg) - self.__x_pos = cfg.x_pos - self.__y_pos = cfg.y_pos - self.__x_offset = cfg.x_offset - self.__y_offset = cfg.y_offset - self.__tilt = cfg.tilt - - def get_pos_devices(self) -> list[DeviceAccess | None]: - """ - Get device handles used for position reading - - Returns - ------- - list[DeviceAccess] - Array of DeviceAcess - """ - return [self.__x_pos, self.__y_pos] - - def get_tilt_device(self) -> DeviceAccess | None: - """ - Get device handle used for tilt access - - Returns - ------- - DeviceAccess - DeviceAcess - """ - return self.__tilt - - def get_offset_devices(self) -> list[DeviceAccess | None]: - """ - Get device handles used for offset access - - Returns - ------- - list[DeviceAccess] - Array of DeviceAcess - """ - return [self.__x_offset, self.__y_offset] - - def __repr__(self): - return __pyaml_repr__(self) diff --git a/pyaml/common/abstract.py b/pyaml/common/abstract.py index 3eb1989b2..39805038c 100644 --- a/pyaml/common/abstract.py +++ b/pyaml/common/abstract.py @@ -1,3 +1,11 @@ +""" +Abstract read/write interfaces for scalar and array values. + +The interfaces define the small protocol used by PyAML runtime elements to +read values, write setpoints, report units, and map scalar channels onto +array-backed data. +""" + from abc import ABCMeta, abstractmethod from numpy import array, double @@ -7,76 +15,169 @@ class ReadFloatScalar(metaclass=ABCMeta): """ - Abstract class providing read access to a scalar double + Define read-only access to one floating-point value. + + Methods + ------- + get() + Return the current scalar value. + unit() + Return the physical unit of the scalar value. """ @abstractmethod def get(self) -> double: - """Get the value""" + """ + Return the current scalar value. + + Returns + ------- + float + Current value. + """ pass @abstractmethod def unit(self) -> str: - """Get the unit of the value""" + """ + Return the physical unit of the scalar value. + + Returns + ------- + str + Unit label. + """ pass class ReadWriteFloatScalar(ReadFloatScalar): """ - Abstract class providing read write access to a scalar double + Define read/write access to one floating-point value. + + Methods + ------- + set(value) + Write a scalar setpoint. + set_and_wait(value) + Write a setpoint and wait for readback confirmation. """ @abstractmethod def set(self, value: double): - """Set the value""" + """ + Write a scalar setpoint. + + Parameters + ---------- + value : float + Value to write. + """ pass # Sets the value and wait that the read value reach the setpoint @abstractmethod def set_and_wait(self, value: double): - """Set the value and wait that setpoint is reached""" + """ + Write a setpoint and wait for readback confirmation. + + Parameters + ---------- + value : float + Target value. + """ pass class ReadFloatArray(metaclass=ABCMeta): """ - Abstract class providing read access to a vector of float + Define read-only access to an array of floating-point values. + + Methods + ------- + get() + Return the current values as an array. + unit() + Return the units associated with the array values. """ @abstractmethod def get(self) -> array: - """Get the value""" + """Return the current values as an array.""" pass @abstractmethod def unit(self) -> list[str]: - """Get the unit of the values""" + """Return the units associated with the array values.""" pass class ReadWriteFloatArray(ReadFloatScalar): """ - Abstract class providing read write access to a vector of double + Define read/write access to an array of floating-point values. + + Methods + ------- + set(value) + Write array values in the interface's defined order. + set_and_wait(value) + Write array values and wait for readback confirmation. """ @abstractmethod def set(self, value: array): - """Set the values""" + """ + Write array values in the interface's defined order. + + Parameters + ---------- + value : numpy.ndarray + Values to write. + """ pass # Sets the value and waits that the read value reach the setpoint @abstractmethod def set_and_wait(self, value: array): - """Set the values and wait that setpoints are reached""" + """ + Write array values and wait for readback confirmation. + + Parameters + ---------- + value : numpy.ndarray + Target values. + """ pass class RWMapper(ReadWriteFloatScalar): """ - Class mapping a scalar to an element of an array + Expose one array element through a scalar read/write interface. + + Parameters + ---------- + bind : ReadWriteFloatArray + Array interface containing the mapped value. + idx : int + Zero-based index of the mapped element. + + Methods + ------- + get() + Get the value at the mapped index. + set(value) + Set the value at the mapped index. + set_and_wait(value) + Set the value and wait for it to reach the setpoint. + unit() + Get the unit for the value. + index() + Get the mapped array index. """ def __init__(self, bind, idx: int): + """ + Initialize the RWMapper. + """ self.bind = bind self.idx = idx diff --git a/pyaml/common/abstract_aggregator.py b/pyaml/common/abstract_aggregator.py index 65ddb7cb6..7a80d6440 100644 --- a/pyaml/common/abstract_aggregator.py +++ b/pyaml/common/abstract_aggregator.py @@ -1,3 +1,9 @@ +""" +Abstract Aggregator module. + +This module provides abstract aggregator functionality for the PyAML accelerator middle layer. +""" + from abc import ABCMeta, abstractmethod import numpy as np @@ -7,6 +13,19 @@ class ScalarAggregator(metaclass=ABCMeta): """ Abstract class providing access to a list of scalar variables + + Methods + ------- + set(value) + Write a list of variable + set_and_wait(value) + Write a list of variable and wait that setpoint are reached + get() + Return a list variables + readback() + Return a list variables (measurements) + unit() + Return the variables unit """ @abstractmethod diff --git a/pyaml/common/constants.py b/pyaml/common/constants.py index 78c7abd26..e63fa3c25 100644 --- a/pyaml/common/constants.py +++ b/pyaml/common/constants.py @@ -1,10 +1,11 @@ """ -PyAML global constants +Shared constants and callback action identifiers. .. data:: HORIZONTAL_KICK_SIGN - Horizontal kick sign convention for both kick an kick angle (default: -1). - + Sign convention applied to horizontal kicks and kick angles. A value of + ``-1.0`` follows the convention used by the PyAML orbit and response-matrix + tools. """ from enum import Enum @@ -14,12 +15,21 @@ class Action(Enum): """ - Action identifier for callback in measurement tools + Identify callback points in measurement-tool workflows. + + Attributes + ---------- + APPLY : int + Callback triggered immediately after an actuator excitation. + RESTORE : int + Callback triggered immediately after restoring the actuator. + MEASURE : int + Callback triggered immediately after taking a measurement. """ APPLY = 0 - "Triggered imediatly after actuator exitation" + "Triggered immediately after actuator excitation." RESTORE = 1 - "Triggered imediatly after actuator has been restored to initial value" + "Triggered immediately after restoring the actuator to its initial value." MEASURE = 2 - "Triggered imediatly after measurement" + "Triggered immediately after taking a measurement." diff --git a/pyaml/common/element.py b/pyaml/common/element.py index f323f25a4..e18da8d69 100644 --- a/pyaml/common/element.py +++ b/pyaml/common/element.py @@ -1,32 +1,217 @@ -from typing import TYPE_CHECKING +"""Base classes for configured accelerator and lattice elements.""" + +from collections.abc import Mapping, Sequence +from dataclasses import dataclass +from typing import TYPE_CHECKING, Any from pydantic import BaseModel, ConfigDict +from . import abstract from .exception import PyAMLException if TYPE_CHECKING: - from ..common.element_holder import ElementHolder + from .holders.element_holder import ElementHolder + + +@dataclass(frozen=True) +class ReprOptions: + """Limits applied to PyAML object representations.""" + + max_items: int = 3 + max_depth: int = 2 + max_length: int = 800 + + +_repr_options = ReprOptions() + + +def set_repr_options( + max_items: int | None = None, + max_depth: int | None = None, + max_length: int | None = None, +) -> ReprOptions: + """ + Configure the limits used by PyAML object representations. + + Passing no arguments returns the current options. Every supplied value must + be a positive integer. + """ + global _repr_options + + values = { + "max_items": _repr_options.max_items if max_items is None else max_items, + "max_depth": _repr_options.max_depth if max_depth is None else max_depth, + "max_length": _repr_options.max_length if max_length is None else max_length, + } + for name, value in values.items(): + if not isinstance(value, int) or value < 1: + raise ValueError(f"{name} must be a positive integer") + + _repr_options = ReprOptions(**values) + return _repr_options + + +def _unavailable(error: Exception) -> str: + return f"" + + +def _class_exclusions(obj) -> set[str]: + exclusions: set[str] = set() + for cls in type(obj).__mro__: + exclusions.update(getattr(cls, "__pyaml_repr_exclude__", ())) + return exclusions + + +def _properties(obj) -> dict[str, Any]: + values: dict[str, Any] = {} + for cls in reversed(type(obj).__mro__): + for name, descriptor in vars(cls).items(): + if name.startswith("_") or not isinstance(descriptor, property): + continue + try: + values[name] = getattr(obj, name) + except Exception as error: + values[name] = _unavailable(error) + return values + + +def _fields(obj) -> dict[str, Any]: + custom_fields = getattr(obj, "_pyaml_repr_fields", None) + if custom_fields is not None: + try: + return custom_fields() + except Exception as error: + return {"value": _unavailable(error)} + + values = _properties(obj) + for name, value in vars(obj).items(): + if not name.startswith("_"): + values.setdefault(name, value) + return values + + +def _identity(obj) -> str: + name = getattr(obj, "name", None) + try: + name = name() if callable(name) else name + except Exception: + name = None + if isinstance(name, str): + return f"{obj.__class__.__name__}:{name}" + return obj.__class__.__name__ + + +def _short_object_repr(obj) -> str: + name = getattr(obj, "name", None) + try: + name = name() if callable(name) else name + except Exception: + name = None + if isinstance(name, str): + return f"{obj.__class__.__name__}(name={_format_value(name, 0, set())})" + return obj.__class__.__name__ + + +def _selected_items(values: Sequence | set) -> tuple[list[Any], int]: + items = list(values) + omitted = len(items) - _repr_options.max_items + if omitted <= 0: + return items, 0 + + head_count = (_repr_options.max_items + 1) // 2 + tail_count = _repr_options.max_items - head_count + selected = items[:head_count] + if tail_count: + selected.extend(items[-tail_count:]) + return selected, omitted + + +def _format_sequence(values: Sequence | set, depth: int, active: set[int]) -> str: + selected, omitted = _selected_items(values) + parts = [_format_value(value, depth, active) for value in selected] + if omitted: + insert_at = (_repr_options.max_items + 1) // 2 + parts.insert(insert_at, f"... +{omitted} more ...") + + if isinstance(values, tuple): + if len(parts) == 1 and not omitted: + return f"({parts[0]},)" + return f"({', '.join(parts)})" + if isinstance(values, set): + return "{" + ", ".join(parts) + "}" + return "[" + ", ".join(parts) + "]" + + +def _format_mapping(values: Mapping, depth: int, active: set[int]) -> str: + selected, omitted = _selected_items(list(values.items())) + parts = [f"{_format_value(key, depth, active)}: {_format_value(value, depth, active)}" for key, value in selected] + if omitted: + parts.insert((_repr_options.max_items + 1) // 2, f"... +{omitted} more ...") + return "{" + ", ".join(parts) + "}" + + +def _format_object(obj, depth: int, active: set[int], extra_exclusions: set[str] | None = None) -> str: + if depth >= _repr_options.max_depth: + return _short_object_repr(obj) + if id(obj) in active: + return f"" + + active.add(id(obj)) + try: + values = _fields(obj) + exclusions = _class_exclusions(obj) + if extra_exclusions: + exclusions.update(extra_exclusions) + parts = [] + for name, value in values.items(): + if name.startswith("_") or name in exclusions or callable(value): + continue + if isinstance(value, (abstract.ReadFloatScalar, abstract.ReadFloatArray, abstract.ReadWriteFloatArray)): + continue + formatted = _identity(value) if name == "peer" and value is not None else _format_value(value, depth + 1, active) + parts.append(f"{name}={formatted}") + return f"{obj.__class__.__name__}({', '.join(parts)})" if parts else obj.__class__.__name__ + except Exception as error: + return f"{obj.__class__.__name__}({_unavailable(error)})" + finally: + active.remove(id(obj)) + +def _format_value(value, depth: int, active: set[int]) -> str: + if isinstance(value, str): + limit = max(1, _repr_options.max_length // 4) + suffix = "..." if len(value) > limit else "" + return repr(value[:limit] + suffix) + if value is None or isinstance(value, (bool, int, float, complex)): + return repr(value) + if isinstance(value, Mapping): + return _format_mapping(value, depth, active) + if isinstance(value, (list, tuple, set, frozenset)): + return _format_sequence(value, depth, active) + if type(value).__module__.startswith("numpy"): + shape = getattr(value, "shape", None) + dtype = getattr(value, "dtype", None) + return f"{value.__class__.__name__}(shape={shape!r}, dtype={dtype!r})" + if type(value).__module__.startswith("pyaml"): + return _format_object(value, depth, active) + try: + result = repr(value) + except Exception as error: + return _unavailable(error) + limit = max(1, _repr_options.max_length // 2) + return result if len(result) <= limit else result[:limit] + "..." -def __pyaml_repr__(obj): + +def __pyaml_repr__(obj, exclude: list[str] | None = None): """ - Returns a string representation of a pyaml object + Return an informative, bounded representation of a PyAML object. + + Public attributes and read-only properties are included unless they are + excluded. Device accessors are omitted so rendering never reads a control + system value. """ - if hasattr(obj, "_cfg"): - if isinstance(obj, Element): - return repr(obj._cfg).replace( - "ConfigModel(", - obj.__class__.__name__ + "(peer='" + obj.get_peer_name() + "', ", - ) - else: - # no peer - return repr(obj._cfg).replace("ConfigModel", obj.__class__.__name__) - else: - # Object is not yet fully constructed - if isinstance(obj, Element): - return f"{obj.__class__.__name__}: {obj.get_name()}" - else: - return f"{obj.__class__.__name__}" + result = _format_object(obj, 0, set(), set(exclude or ())) + return result[: _repr_options.max_length] + ("..." if len(result) > _repr_options.max_length else "") class ElementConfigModel(BaseModel): @@ -38,7 +223,7 @@ class ElementConfigModel(BaseModel): name : str The name of the PyAML element. description : str, optional - Description of the element. + Human-readable description of the element. lattice_names : str or None, optional The name(s) of the associated element(s) in the lattice. By default, the PyAML element name is used. lattice_name accept the following @@ -57,84 +242,199 @@ class ElementConfigModel(BaseModel): lattice_names: str | None = None -class Element(object): +class Element: """ - Class providing access to one element of a physical or simulated lattice + Base class for an element in a physical or simulated lattice. + + Parameters + ---------- + name : str + Unique element name. + lattice_names : str or None, optional + Lattice element selector associated with this element. Defaults to + ``name`` when omitted. + description : str or None, optional + Human-readable element description. - Attributes: - name: str - The unique name identifying the element in the configuration file + Attributes + ---------- + name + Return the element name. + lattice_names + Return the lattice selector associated with the element. + description + Return the element description, if one is configured. + peer + Return the simulator or control system attached to the element. + + Methods + ------- + get_name() + Return the element name. + get_lattice_names() + Return the lattice selector associated with the element. + get_description() + Return the element description, if available. + set_energy(E) + Set the beam energy used by this element, if supported. + set_mcf(alphac) + Set the momentum compaction factor, if supported. + set_harmonic(h) + Set the RF harmonic number, if supported. + check_peer() + Raise an error if the element is not attached to a peer. + attached_to() + Return a human-readable description of the attached peer. + post_init() + Perform post-construction initialization after attachment. """ - def __init__(self, name: str): - self._name: str = name - self._peer: "ElementHolder" = None # Peer: ControlSystem, Simulator + __pyaml_repr_exclude__ = ("description",) - def get_name(self) -> str: + def __init__( + self, + name: str, + lattice_names: str | None = None, + description: str | None = None, + ): """ - Returns the name of the element + Initialize an element and its optional lattice association. """ - return self._name + self._name = name + self._lattice_names = lattice_names + self._description = description + self._peer: ElementHolder | None = None - def get_lattice_names(self) -> str: + def _cfg_value(self, attr: str, fallback: Any) -> Any: """ - Returns the name of associated lattice element(s) - """ - if not hasattr(self, "_cfg"): - return self._name - else: - return self._cfg.lattice_names + Return a configured attribute, falling back to the base value. - def get_description(self) -> str: - """ - Returns the description of the element + Parameters + ---------- + attr : str + Configuration attribute name. + fallback : object + Value returned when no configured value is available. """ - return self._cfg.description + cfg = getattr(self, "_cfg", None) + if cfg is not None: + value = getattr(cfg, attr, None) + if value is not None: + return value + return fallback + + @property + def name(self) -> str: + """Return the element name.""" + return self._cfg_value("name", self._name) + + @property + def lattice_names(self) -> str: + """Return the lattice selector associated with the element.""" + cfg = getattr(self, "_cfg", None) + + if cfg is not None and cfg.lattice_names is not None: + return cfg.lattice_names + + if self._lattice_names is not None: + return self._lattice_names + + return self.name + + @property + def description(self) -> str | None: + """Return the element description, if one is configured.""" + return self._cfg_value("description", self._description) + + def get_name(self) -> str: + """Return the element name.""" + return self.name + + def get_lattice_names(self) -> str | None: + """Return the lattice selector associated with the element.""" + return self.lattice_names + + def get_description(self) -> str | None: + """Return the element description, if available.""" + return self.description def set_energy(self, E: float): """ - Set the instrument energy on this element + Set the beam energy used by this element, if supported. + + Parameters + ---------- + E : float + Beam energy. """ pass def set_mcf(self, alphac: float): """ - Set the instrument moment compaction factor on this element + Set the momentum compaction factor, if supported. + + Parameters + ---------- + alphac : float + Momentum compaction factor. """ pass def set_harmonic(self, h: int): """ - Sets the harmonic number (number of bucket) on this element + Set the RF harmonic number, if supported. + + Parameters + ---------- + h : int + Number of RF buckets per revolution. """ pass def check_peer(self): """ - Throws an exception if the element is not attacched - to a simulator or to a control system + Raise an error if the element is not attached to a peer. + + Raises + ------ + PyAMLException + If the element is not attached to a simulator or control system. """ if self._peer is None: - raise PyAMLException(f"{str(self)} is not attachedto a control system or the a simulator") + raise PyAMLException(f"{str(self.name)} is not attachedto a control system or the a simulator") @property def peer(self) -> "ElementHolder": - """ - Returns the peer simulator or control system - """ + """Return the simulator or control system attached to the element.""" return self._peer - def get_peer_name(self) -> str: + def attached_to(self) -> str: """ - Returns a string representation of peer simulator or control system + Return a human-readable description of the attached peer. + + Returns + ------- + str + Peer type and name, or ``"None"`` when unattached. """ return "None" if self._peer is None else f"{self._peer.__class__.__name__}:{self._peer.name()}" + def _fill_device(self, holder: "ElementHolder"): + """ + Add this element to a holder (Simultor or ControlSystem) + """ + raise PyAMLException(f"__fill_device() is not implemented for {self.__class__.__name__}") + def post_init(self): """ - Method triggered after all initialisations are done + Perform post-construction initialization after attachment. + + Base elements do not require additional initialization. """ pass def __repr__(self): + """ + Implement the ``__repr__`` string. + """ return __pyaml_repr__(self) diff --git a/pyaml/common/element_holder.py b/pyaml/common/element_holder.py deleted file mode 100644 index 0d34d17e6..000000000 --- a/pyaml/common/element_holder.py +++ /dev/null @@ -1,433 +0,0 @@ -""" -Module handling element references for simulators and control system -""" - -import fnmatch -import re -from typing import TYPE_CHECKING - -from ..arrays.bpm_array import BPMArray -from ..arrays.cfm_magnet_array import CombinedFunctionMagnetArray -from ..arrays.element_array import ElementArray -from ..arrays.magnet_array import MagnetArray -from ..arrays.serialized_magnet_array import SerializedMagnetsArray -from ..bpm.bpm import BPM -from ..common.exception import PyAMLException -from ..diagnostics.chromaticity_monitor import ChomaticityMonitor -from ..diagnostics.tune_monitor import BetatronTuneMonitor -from ..magnet.cfm_magnet import CombinedFunctionMagnet -from ..magnet.magnet import Magnet -from ..magnet.serialized_magnet import SerializedMagnets -from ..rf.rf_plant import RFPlant -from ..rf.rf_transmitter import RFTransmitter -from .element import Element - -if TYPE_CHECKING: - from ..accelerator import Accelerator - from ..tuning_tools.chromaticity import Chromaticity - from ..tuning_tools.chromaticity_response_matrix import ChromaticityResponseMatrix - from ..tuning_tools.dispersion import Dispersion - from ..tuning_tools.orbit import Orbit - from ..tuning_tools.orbit_response_matrix import OrbitResponseMatrix - from ..tuning_tools.tune import Tune - from ..tuning_tools.tune_response_matrix import TuneResponseMatrix - - -class ElementHolder(object): - """ - Class that store references of objects used from both - simulators and control system - """ - - def __init__(self): - # Device handle - self.__MAGNETS: dict[str, Magnet] = {} - self.__CFM_MAGNETS: dict[str, CombinedFunctionMagnet] = {} - self.__SERIALIZED_MAGNETS: dict[str, SerializedMagnets] = {} - self.__BPMS: dict[str, BPM] = {} - self.__RFPLANT: dict[str, RFPlant] = {} - self.__RFTRANSMITTER: dict[str, RFTransmitter] = {} - self.__DIAG: dict[str, Element] = {} - self.__TUNING_TOOLS: dict[str, Element] = {} - self.__ALL: dict[str, Element] = {} - - self.__by_class_elements: dict[type, dict] = { - Magnet: self.__MAGNETS, - CombinedFunctionMagnet: self.__CFM_MAGNETS, - SerializedMagnets: self.__SERIALIZED_MAGNETS, - BPM: self.__BPMS, - RFPlant: self.__RFPLANT, - RFTransmitter: self.__RFTRANSMITTER, - } - - # Array handle - self.__MAGNET_ARRAYS: dict = {} - self.__CFM_MAGNET_ARRAYS: dict = {} - self.__SERIALIZED_MAGNETS_ARRAYS: dict = {} - self.__BPM_ARRAYS: dict = {} - self.__ELEMENT_ARRAYS: dict = {} - - @property - def peer(self) -> "Accelerator": - """ - Returns the peer accelerator of this holder - """ - return self._peer - - def post_init(self): - """ - Method triggered after all initialisations are done - """ - for e in self.get_all_elements(): - e.post_init() - - def fill_device(self, elements: list[Element]): - raise PyAMLException("ElementHolder.fill_device() is not subclassed") - - def find_elements(self, filter: str) -> list[str]: - if filter.startswith("re:"): - pattern = re.compile(rf"{filter[3:]}") - elements = [k for k in self.__ALL.keys() if pattern.fullmatch(k)] - elif "*" in filter or "?" in filter: - elements = [k for k in self.__ALL.keys() if fnmatch.fnmatch(k, filter)] - else: - elements = [filter] - - return elements - - def fill_array( - self, - array_name: str, - element_names: list[str], - get_func, - constructor, - ARR: dict, - ): - # Handle wildcard, regexp and exclusion pattern - all_names: list[str] = [] - excluded_names: list[str] = [] - for name in element_names: - if name.startswith("~"): - names = self.find_elements(name[1:]) - excluded_names.extend(names) - else: - names = self.find_elements(name) - all_names.extend(names) - - [all_names.remove(name) for name in excluded_names] - - a = [] - for n in all_names: - try: - m = get_func(n) - except Exception as err: - raise PyAMLException(f"{constructor.__name__} {array_name} : {err} @index {len(a)}") from None - if m in a: - raise PyAMLException(f"{constructor.__name__} {array_name} : duplicate name {name} @index {len(a)}") from None - a.append(m) - ARR[array_name] = constructor(array_name, a) - - def __add(self, array, element: Element): - if element.get_name() in self.__ALL: # Ensure name unicity - raise PyAMLException(f"Duplicate element {element.__class__.__name__} name {{element.get_name()}}") from None - array[element.get_name()] = element - self.__ALL[element.get_name()] = element - - def __get(self, what, name, array) -> Element: - if name not in array: - raise PyAMLException(f"{what} {name} not defined") - return array[name] - - # Generic elements - def fill_element_array(self, arrayName: str, elementNames: list[str]): - self.fill_array( - arrayName, - elementNames, - self.get_element, - ElementArray, - self.__ELEMENT_ARRAYS, - ) - - def add_element(self, element: Element): - self.__ALL[element.get_name()] = element - - def get_element(self, name: str) -> Element: - return self.__get("Element", name, self.__ALL) - - def get_elements(self, name: str) -> ElementArray: - return self.__get("Element array", name, self.__ELEMENT_ARRAYS) - - def get_all_elements(self) -> list[Element]: - return [value for key, value in self.__ALL.items()] - - # Magnets - - def fill_magnet_array(self, arrayName: str, elementNames: list[str]): - self.fill_array(arrayName, elementNames, self.get_magnet, MagnetArray, self.__MAGNET_ARRAYS) - - def get_magnet(self, name: str) -> Magnet: - return self.__get("Magnet", name, self.__MAGNETS) - - def add_magnet(self, m: Magnet): - self.__add(self.__MAGNETS, m) - - def get_magnets(self, name: str) -> MagnetArray: - return self.__get("Magnet array", name, self.__MAGNET_ARRAYS) - - def get_all_magnets(self) -> list[Magnet]: - return [value for key, value in self.__MAGNETS.items()] - - # Combined Function Magnets - - def fill_cfm_magnet_array(self, arrayName: str, elementNames: list[str]): - self.fill_array( - arrayName, - elementNames, - self.get_cfm_magnet, - CombinedFunctionMagnetArray, - self.__CFM_MAGNET_ARRAYS, - ) - - def get_cfm_magnet(self, name: str) -> Magnet: - return self.__get("CombinedFunctionMagnet", name, self.__CFM_MAGNETS) - - def add_cfm_magnet(self, m: Magnet): - self.__add(self.__CFM_MAGNETS, m) - - def get_cfm_magnets(self, name: str) -> CombinedFunctionMagnetArray: - return self.__get("CombinedFunctionMagnet array", name, self.__CFM_MAGNET_ARRAYS) - - def get_all_cfm_magnets(self) -> list[CombinedFunctionMagnet]: - return [value for key, value in self.__CFM_MAGNETS.items()] - - # Serialized magnets - - def fill_serialized_magnet_array(self, arrayName: str, elementNames: list[str]): - self.fill_array( - arrayName, - elementNames, - self.get_serialized_magnet, - SerializedMagnetsArray, - self.__SERIALIZED_MAGNETS_ARRAYS, - ) - - def get_serialized_magnet(self, name: str) -> Magnet: - return self.__get("SerializedMagnets", name, self.__SERIALIZED_MAGNETS) - - def add_serialized_magnet(self, m: Magnet): - self.__add(self.__SERIALIZED_MAGNETS, m) - - def get_serialized_magnets(self, name: str) -> SerializedMagnetsArray: - return self.__get("SerializedMagnets array", name, self.__SERIALIZED_MAGNETS_ARRAYS) - - def get_all_serialized_magnets(self) -> list[SerializedMagnets]: - return [value for key, value in self.__SERIALIZED_MAGNETS.items()] - - # BPMs - - def fill_bpm_array(self, arrayName: str, elementNames: list[str]): - self.fill_array( - arrayName, - elementNames, - self.get_bpm, - BPMArray, - self.__BPM_ARRAYS, - ) - - def get_bpm(self, name: str) -> Element: - return self.__get("BPM", name, self.__BPMS) - - def add_bpm(self, bpm: BPM): - self.__add(self.__BPMS, bpm) - - def get_bpms(self, name: str) -> BPMArray: - return self.__get("BPM array", name, self.__BPM_ARRAYS) - - def get_all_bpms(self) -> list[BPM]: - return [value for key, value in self.__BPMS.items()] - - # RF - - def get_rf_plant(self, name: str) -> RFPlant: - return self.__get("RFPlant", name, self.__RFPLANT) - - def add_rf_plant(self, rf: RFPlant): - self.__add(self.__RFPLANT, rf) - - def add_rf_transnmitter(self, rf: RFTransmitter): - self.__add(self.__RFTRANSMITTER, rf) - - def get_rf_trasnmitter(self, name: str) -> RFTransmitter: - return self.__get("RFTransmitter", name, self.__RFTRANSMITTER) - - # Tune monitor - - def get_betatron_tune_monitor(self, name: str) -> BetatronTuneMonitor: - return self.__get("Diagnostic", name, self.__DIAG) - - def add_betatron_tune_monitor(self, tune_monitor: Element): - self.__add(self.__DIAG, tune_monitor) - - # Tuning/Measurement tools - - def add_tool(self, tool: Element): - self.__add(self.__TUNING_TOOLS, tool) - - # ---- Chromaticity ------------------------------------------------- - - def get_chromaticity_monitor(self, name: str) -> ChomaticityMonitor: - obj = self.__get("Chomaticity monitor", name, self.__TUNING_TOOLS) - return obj - - def get_chromaticity_tuning(self, name: str) -> "Chromaticity": - return self.__get("Chromaticity tool", name, self.__TUNING_TOOLS) - - def get_crm_tuning(self, name: str) -> "ChromaticityResponseMatrix": - return self.__get("ChromaticityResponseMatrix tool", name, self.__TUNING_TOOLS) - - @property - def chromaticity(self) -> "Chromaticity": - return self.get_chromaticity_tuning("DEFAULT_CHROMATICITY_CORRECTION") - - @property - def crm(self) -> "ChromaticityResponseMatrix": - return self.get_crm_tuning("DEFAULT_CHROMATICITY_RESPONSE_MATRIX") - - # ---- Tune --------------------------------------------------------- - - def get_tune_tuning(self, name: str) -> "Tune": - return self.__get("Tune tuning tool", name, self.__TUNING_TOOLS) - - @property - def tune(self) -> "Tune": - return self.get_tune_tuning("DEFAULT_TUNE_CORRECTION") - - def get_trm_tuning(self, name: str) -> "TuneResponseMatrix": - return self.__get("TuneResponseMatrix tool", name, self.__TUNING_TOOLS) - - @property - def trm(self) -> "TuneResponseMatrix": - return self.get_trm_tuning("DEFAULT_TUNE_RESPONSE_MATRIX") - - # ---- Orbit -------------------------------------------------------- - - def get_orbit_tuning(self, name: str) -> "Orbit": - return self.__get("Orbit tuning tool", name, self.__TUNING_TOOLS) - - @property - def orbit(self) -> "Orbit": - return self.get_orbit_tuning("DEFAULT_ORBIT_CORRECTION") - - def get_orm_tuning(self, name: str) -> "OrbitResponseMatrix": - return self.__get("OrbitResponseMatrix tool", name, self.__TUNING_TOOLS) - - @property - def orm(self) -> "OrbitResponseMatrix": - return self.get_orm_tuning("DEFAULT_ORBIT_RESPONSE_MATRIX") - - # ---- Dispersive orbit -------------------------------------------- - - def get_dispersion_tuning(self, name: str) -> "Dispersion": - return self.__get("Dispersion tool", name, self.__TUNING_TOOLS) - - @property - def dispersion(self) -> "Dispersion": - return self.get_dispersion_tuning("DEFAULT_DISPERSION") - - def _get_array(self, name: str): - """ - Generic array resolver used by YellowPages. - - The method returns the array object referenced by 'name', regardless of its - concrete type. - """ - if name in self.__BPM_ARRAYS: - return self.__BPM_ARRAYS[name] - if name in self.__MAGNET_ARRAYS: - return self.__MAGNET_ARRAYS[name] - if name in self.__CFM_MAGNET_ARRAYS: - return self.__CFM_MAGNET_ARRAYS[name] - if name in self.__SERIALIZED_MAGNETS_ARRAYS: - return self.__SERIALIZED_MAGNETS_ARRAYS[name] - if name in self.__ELEMENT_ARRAYS: - return self.__ELEMENT_ARRAYS[name] - - raise PyAMLException(f"Array {name} not defined") - - def _get_tool(self, name: str): - """ - Generic tuning tool resolver used by YellowPages. - """ - if name not in self.__TUNING_TOOLS: - raise PyAMLException(f"Tool {name} not defined") - return self.__TUNING_TOOLS[name] - - def _get_diagnostic(self, name: str): - """ - Generic diagnostic resolver used by YellowPages. - """ - if name not in self.__DIAG: - raise PyAMLException(f"Diagnostic {name} not defined") - return self.__DIAG[name] - - def _list_arrays(self) -> list[str]: - """ - Return all array identifiers available in this holder. - """ - arrays: list[str] = [] - arrays.extend(self.__BPM_ARRAYS.keys()) - arrays.extend(self.__MAGNET_ARRAYS.keys()) - arrays.extend(self.__CFM_MAGNET_ARRAYS.keys()) - arrays.extend(self.__SERIALIZED_MAGNETS_ARRAYS.keys()) - arrays.extend(self.__ELEMENT_ARRAYS.keys()) - return arrays - - def _list_tools(self) -> list[str]: - """ - Return all tuning tool identifiers available in this holder. - """ - return list(self.__TUNING_TOOLS.keys()) - - def _list_diagnostics(self) -> list[str]: - """ - Return all diagnostic identifiers available in this holder. - """ - return list(self.__DIAG.keys()) - - def _set_energy(self, E: float): - """ - Sets the energy on all elements - - Parameters - ---------- - E : float - Energy in eV - """ - # Needed by energy dependant element (i.e. magnet coil current calculation) - for m in self.get_all_elements(): - m.set_energy(E) - - def _set_mcf(self, alphac: float): - """ - Sets the moment compaction factor on all elements - - Parameters - ---------- - alphac : float - Moment compaction factor - """ - # Needed by some off energy dependant element (i.e. chromaticty tools) - for m in self.get_all_elements(): - m.set_mcf(alphac) - - def _set_harmonic(self, h: int): - """ - Sets the harmonic number (number of bucket) on elements - - Parameters - ---------- - h : int - Harmonic number - """ - for m in self.get_all_elements(): - m.set_harmonic(h) diff --git a/pyaml/common/exception.py b/pyaml/common/exception.py index 3bf9cb787..577c3def2 100644 --- a/pyaml/common/exception.py +++ b/pyaml/common/exception.py @@ -1,22 +1,37 @@ +"""Exception types used to report PyAML and configuration failures.""" + + class PyAMLException(Exception): - """Exception raised for PyAML error scenarios. + """ + Base exception for errors raised by PyAML runtime components. - Attributes: - message -- explanation of the error + Parameters + ---------- + message : object + Error description retained on the exception as ``message``. """ def __init__(self, message): + """ + Initialize a PyAML runtime exception. + """ super().__init__(message) self.message = message class PyAMLConfigException(Exception): - """Exception raised for PyAML configuration error scenarios. + """ + Exception raised when configuration cannot be loaded or validated. - Attributes: - message -- explanation of the error + Parameters + ---------- + message : object + Error description retained on the exception as ``message``. """ def __init__(self, message): + """ + Initialize a configuration exception. + """ super().__init__(message) self.message = message diff --git a/pyaml/common/holders/element_holder.py b/pyaml/common/holders/element_holder.py new file mode 100644 index 000000000..aa2b16dc0 --- /dev/null +++ b/pyaml/common/holders/element_holder.py @@ -0,0 +1,905 @@ +"""Store, resolve, and group elements shared by runtime backends.""" + +import fnmatch +import re +from abc import ABCMeta, abstractmethod +from typing import TYPE_CHECKING, overload + +from ...arrays.element_array import ElementArray +from ...bpm.bpm import BPM +from ...diagnostics.tune_monitor import BetatronTuneMonitor +from ...magnet.cfm_magnet import CombinedFunctionMagnet +from ...magnet.magnet import Magnet +from ...magnet.serialized_magnet import SerializedMagnets +from ...rf.rf_plant import RFPlant +from ...rf.rf_transmitter import RFTransmitter +from ...tuning_tools.chromaticity_monitor import ChromaticityMonitor +from ..abstract_aggregator import ScalarAggregator +from ..element import Element +from ..exception import PyAMLException +from .rf_holder import RFHolder +from .sub_holders import ( + BPMHolder, + BPMsHolder, + CombinedFunctionMagnetHolder, + CombinedFunctionMagnetsHolder, + MagnetHolder, + MagnetsHolder, + SerializedMagnetHolder, + SerializedMagnetsHolder, +) + +if TYPE_CHECKING: + from ...accelerator import Accelerator + from ...configuration.unbound_element import UnboundElement + from ...tuning_tools.bba import BBA + from ...tuning_tools.chromaticity import Chromaticity + from ...tuning_tools.chromaticity_response_matrix import ChromaticityResponseMatrix + from ...tuning_tools.dispersion import Dispersion + from ...tuning_tools.measurement_tool import MeasurementTool + from ...tuning_tools.orbit import Orbit + from ...tuning_tools.orbit_response_matrix import OrbitResponseMatrix + from ...tuning_tools.tune import Tune + from ...tuning_tools.tune_response_matrix import TuneResponseMatrix + from ...tuning_tools.tuning_tool import TuningTool + + +class ElementHolder(metaclass=ABCMeta): + """ + Manage named elements, diagnostics, tools, and element arrays. + + An element holder owns every element of one accelerator mode and exposes them + through per-type accessors. :class:`~pyaml.control.controlsystem.ControlSystem` + and :class:`~pyaml.lattice.simulator.Simulator` both derive from it, so the same + API drives a live machine and a simulation. + + Attributes + ---------- + magnet, magnets + Single magnet by name, or a named magnet array. + bpm, bpms + Single BPM by name, or a named BPM array. + combined_function_magnet, combined_function_magnets + Single combined-function magnet by name, or a named array. + serialized_magnet, serialized_magnets + Single serialized magnet group by name, or a named array. + rf + RF plant and transmitters of this mode. + tune, chromaticity, orbit, dispersion + Tuning tools attached to this mode, looked up by name. + trm, crm, orm + Response-matrix measurement tools, looked up by name. + + Methods + ------- + post_init() + Run post-initialization hooks for every stored element. + fill_device(elements) + Bind configured elements to the holder's runtime backend. + create_magnet_strength_aggregator(magnets) + Create an aggregator exposing the selected magnets' strengths. + create_magnet_hardware_aggregator(magnets) + Create an aggregator exposing the selected hardware values. + create_bpm_aggregators(bpms) + Create aggregate BPM position interfaces. + find_elements(filter) + Find element names matching a literal, wildcard, or regular expression. + fill_element_array(arrayName, elementNames) + Create and register a generic element array. + add_element(element) + Add an element to the global element store. + get_element(name) + Return a named element from the global store. + get_elements(name) + Return a named generic element array. + get_all_elements() + Return all registered elements in insertion order. + get_betatron_tune_monitor(name) + Return a named betatron tune monitor. + add_betatron_tune_monitor(tune_monitor) + Add a betatron tune monitor to the diagnostics store. + add_tool(tool) + Add a tuning or measurement tool to the tool store. + get_chromaticity_monitor(name) + Return a named chromaticity monitor. + get_chromaticity_tuning(name) + Return a named chromaticity tuning tool. + get_crm_tuning(name) + Return a named chromaticity response-matrix tool. + get_tune_tuning(name) + Return a named tune correction tool. + get_trm_tuning(name) + Return a named tune response-matrix tool. + get_orbit_tuning(name) + Return a named orbit correction tool. + get_orm_tuning(name) + Return a named orbit response-matrix tool. + get_bba(name) + Return a named beam-based alignment tool. + get_dispersion_tuning(name) + Return a named dispersion tuning tool. + """ + + def __init__(self): + # Device handle + """Initialize empty element stores and typed sub-holders.""" + self._MAGNETS: dict[str, Magnet] = {} + self._CFM_MAGNETS: dict[str, CombinedFunctionMagnet] = {} + self._SERIALIZED_MAGNETS: dict[str, SerializedMagnets] = {} + self._BPMS: dict[str, BPM] = {} + self._RFPLANT: dict[str, RFPlant] = {} + self._RFTRANSMITTER: dict[str, RFTransmitter] = {} + self._DIAG: dict[str, Element] = {} + self._TOOLS: dict[str, Element] = {} + self._ALL: dict[str, Element] = {} + + self.__by_class_elements: dict[type, dict] = { + Magnet: self._MAGNETS, + CombinedFunctionMagnet: self._CFM_MAGNETS, + SerializedMagnets: self._SERIALIZED_MAGNETS, + BPM: self._BPMS, + RFPlant: self._RFPLANT, + RFTransmitter: self._RFTRANSMITTER, + } + + # Array handle + self._MAGNET_ARRAYS: dict = {} + self._CFM_MAGNET_ARRAYS: dict = {} + self._SERIALIZED_MAGNETS_ARRAYS: dict = {} + self._BPM_ARRAYS: dict = {} + self._ELEMENT_ARRAYS: dict = {} + + # Sub holders + self._magnet_holder = MagnetHolder(self) + self._magnets_holder = MagnetsHolder(self) + self._serialized_magnet_holder = SerializedMagnetHolder(self) + self._serialized_magnets_holder = SerializedMagnetsHolder(self) + self._combined_function_magnet_holder = CombinedFunctionMagnetHolder(self) + self._combined_function_magnets_holder = CombinedFunctionMagnetsHolder(self) + self._bpm_holder = BPMHolder(self) + self._bpms_holder = BPMsHolder(self) + self._rf_holder = RFHolder(self) + + @property + def peer(self) -> "Accelerator": + """Return the accelerator associated with this holder.""" + return self._peer + + # Sub holders ---------------------------------------------------------------- + + @property + def magnet(self) -> MagnetHolder: + """Return the magnet.""" + return self._magnet_holder + + @property + def magnets(self) -> MagnetsHolder: + """Return the magnets.""" + return self._magnets_holder + + @property + def serialized_magnet(self) -> SerializedMagnetHolder: + """Return the serialized magnet.""" + return self._serialized_magnet_holder + + @property + def serialized_magnets(self) -> SerializedMagnetsHolder: + """Return the serialized magnets.""" + return self._serialized_magnets_holder + + @property + def combined_function_magnet(self) -> CombinedFunctionMagnetHolder: + """Return the combined function magnet.""" + return self._combined_function_magnet_holder + + @property + def combined_function_magnets(self) -> CombinedFunctionMagnetsHolder: + """Return the combined function magnets.""" + return self._combined_function_magnets_holder + + @property + def bpm(self) -> BPMHolder: + """Return the bpm.""" + return self._bpm_holder + + @property + def bpms(self) -> BPMsHolder: + """Return the bpms.""" + return self._bpms_holder + + @property + def rf(self) -> RFHolder: + """Return the rf.""" + return self._rf_holder + + def post_init(self): + """Run post-initialization hooks for every stored element.""" + for e in self.get_all_elements(): + e.post_init() + + def fill_device(self, elements: list[Element]): + for element in elements: + element._fill_device(self) + + @abstractmethod + def _fill_magnet(self, magnet: Magnet) -> None: + pass + + @abstractmethod + def _fill_combined_function_magnet(self, magnet: CombinedFunctionMagnet) -> None: + pass + + @abstractmethod + def _fill_serialized_magnets(self, magnets: SerializedMagnets) -> None: + pass + + @abstractmethod + def _fill_bpm(self, bpm: BPM) -> None: + pass + + @abstractmethod + def _fill_rf_plant(self, rf_plant: RFPlant) -> None: + pass + + @abstractmethod + def _fill_betatron_tune_monitor(self, monitor: BetatronTuneMonitor) -> None: + pass + + @abstractmethod + def _fill_tool(self, tool: "TuningTool | MeasurementTool") -> None: + pass + + @abstractmethod + def _fill_unbound_element(self, element: "UnboundElement") -> None: + pass + + # Aggregators + + @abstractmethod + def create_magnet_strength_aggregator(self, magnets: list[Magnet]) -> ScalarAggregator | None: + """ + Create an aggregator exposing the selected magnets' strengths. + + Parameters + ---------- + magnets : list[Magnet] + Magnets to include in the strength aggregator. + + Returns + ------- + ScalarAggregator | None + Strength aggregator, or ``None`` when unsupported. + """ + pass + + @abstractmethod + def create_magnet_hardware_aggregator(self, magnets: list[Magnet]) -> ScalarAggregator | None: + """ + Create an aggregator exposing the selected hardware values. + + Parameters + ---------- + magnets : list[Magnet] + Magnets to include in the hardware aggregator. + + Returns + ------- + ScalarAggregator | None + Hardware aggregator, or ``None`` when unsupported. + """ + pass + + @abstractmethod + def create_bpm_aggregators(self, bpms: list[BPM]) -> list[ScalarAggregator | None]: + """ + Create aggregate BPM position interfaces. + + Parameters + ---------- + bpms : list[BPM] + BPMs to include in the aggregators. + + Returns + ------- + list[ScalarAggregator | None] + Aggregators for combined, horizontal, and vertical positions. + """ + pass + + # Elements + + def find_elements(self, filter: str) -> list[str]: + """ + Find element names matching a literal, wildcard, or regular expression. + + Parameters + ---------- + filter : str + Pattern to match. Prefix with ``re:`` for a regular expression. + + Returns + ------- + list[str] + Matching element names. + """ + if filter.startswith("re:"): + pattern = re.compile(rf"{filter[3:]}") + elements = [k for k in self._ALL.keys() if pattern.fullmatch(k)] + elif "*" in filter or "?" in filter: + elements = [k for k in self._ALL.keys() if fnmatch.fnmatch(k, filter)] + else: + elements = [filter] + + return elements + + def _fill_array( + self, + array_name: str, + element_names: list[str], + get_func, + constructor, + ARR: dict, + ): + # Handle wildcard, regexp and exclusion pattern + """ + Resolve selectors and store a constructed element array. + + Parameters + ---------- + array_name : str + Name of the array to create. + element_names : list[str] + Element names or selectors; prefix with ``~`` to exclude matches. + get_func : object + Callback used to resolve element names. + constructor : object + Constructor for the resulting array. + ARR : dict + Destination array store. + """ + all_names: list[str] = [] + excluded_names: list[str] = [] + for name in element_names: + if name.startswith("~"): + names = self.find_elements(name[1:]) + excluded_names.extend(names) + else: + names = self.find_elements(name) + all_names.extend(names) + + [all_names.remove(name) for name in excluded_names] + + a = [] + for n in all_names: + try: + m = get_func(n) + except Exception as err: + raise PyAMLException(f"{constructor.__name__} {array_name} : {err} @index {len(a)}") from None + if m in a: + raise PyAMLException(f"{constructor.__name__} {array_name} : duplicate name {name} @index {len(a)}") from None + a.append(m) + ARR[array_name] = constructor(array_name, a) + + def _add(self, array, element: Element): + """ + Register an element in a typed store and the global index. + + Parameters + ---------- + array : object + Destination typed store. + element : Element + Element to register. + """ + if element.get_name() in self._ALL: # Ensure name unicity + raise PyAMLException(f"Duplicate element {element.__class__.__name__} name {{element.get_name()}}") from None + array[element.get_name()] = element + self._ALL[element.get_name()] = element + + def _get(self, what, name, array) -> Element: + """ + Return a named object from a typed store. + + Parameters + ---------- + what : object + Object type used in lookup errors. + name : object + Name to look up. + array : object + Name-indexed store to search. + + Returns + ------- + Element + Object registered under ``name``. + """ + if name not in array: + raise PyAMLException(f"{what} {name} not defined") + return array[name] + + # Generic elements + def get(self) -> ElementArray: + """Return all registered elements in insertion order. + + Returns + ------- + ElementArray + New unnamed container sharing the registered element references. + + Notes + ----- + Registration order is not necessarily longitudinal lattice order. + Changing the returned container does not change the holder registry. + Each call reflects the current registry. + + Examples + -------- + >>> elements = sr.live.get() + >>> names = elements.names() + """ + return ElementArray("", list(self._ALL.values())) + + @overload + def __getitem__(self, key: int) -> Element: ... + + @overload + def __getitem__(self, key: slice) -> ElementArray: ... + + @overload + def __getitem__(self, key: str) -> Element | ElementArray | None: ... + + def __getitem__(self, key: int | slice | str) -> Element | ElementArray | None: + """Retrieve an element or select a collection. + + Parameters + ---------- + key : int, slice or str + Index in registration order, slice, exact name, or name pattern. + Strings containing ``*``, ``?`` or ``[`` use fnmatch matching. + Other strings are exact registry keys. Colons are literal. + + Returns + ------- + Element or ElementArray or None + An index returns an element. An exact name returns its element + or None. Patterns and slices return the most specific compatible + array, or an empty ElementArray when nothing matches. + The full slice ``[:]`` returns a generic ElementArray, like get(). + + Raises + ------ + IndexError + If the index is out of bounds. + TypeError + If the key is neither an integer, a slice, nor a string. + ValueError + If a slice has a zero step. + + Notes + ----- + Indices follow insertion order, not necessarily lattice order. + Collections share element references but do not modify the registry. + Field filters and regular expressions are not interpreted here. + + Examples + -------- + >>> bpm = sr.live["BPM01"] + >>> missing = sr.live["UNKNOWN"] # None + >>> bpms = sr.live["BPM*"] + >>> bpms = sr.live["BPM0[123]"] # BPM01, BPM02 or BPM03 + >>> bpms = sr.live["BPM0[1-3]"] # Same selection using a range + >>> quads = sr.live["Q[FD]*"] # Names starting with QF or QD + >>> bpms = sr.live["BPM0[!3]"] # One character after BPM0, except 3 + >>> first = sr.live[0] + >>> subset = sr.live[1:10] + >>> all_elements = sr.live[:] + """ + if isinstance(key, str): + if any(marker in key for marker in "*?["): + return self.get()._select_names(key) + return self._ALL.get(key) + if isinstance(key, int): + return list(self._ALL.values())[key] + if isinstance(key, slice): + elements = self.get() + if key == slice(None): + return elements + return elements._typed_array(list(elements)[key]) + raise TypeError("ElementHolder keys must be integers, slices or strings") + + def fill_element_array(self, arrayName: str, elementNames: list[str]): + """ + Create and register a generic element array. + + Parameters + ---------- + arrayName : str + Name under which the new array is registered. + elementNames : list[str] + Names of the elements to gather into the array, in the order they should appear. + """ + self._fill_array( + arrayName, + elementNames, + self.get_element, + ElementArray, + self._ELEMENT_ARRAYS, + ) + + def add_element(self, element: Element): + """ + Add an element to the global element store. + + Parameters + ---------- + element : Element + Element to register, keyed by its own name. + """ + self._ALL[element.get_name()] = element + + def get_element(self, name: str) -> Element: + """ + Return a named element from the global store. + + Parameters + ---------- + name : str + Name of the element to look up, as declared in the configuration. + + Returns + ------- + Element + The element registered under ``name``. + """ + return self._get("Element", name, self._ALL) + + def get_elements(self, name: str) -> ElementArray: + """ + Return a named generic element array. + + Parameters + ---------- + name : str + Name of the element array to look up, as declared in the configuration. + + Returns + ------- + ElementArray + The element array registered under ``name``. + """ + return self._get("Element array", name, self._ELEMENT_ARRAYS) + + def get_all_elements(self) -> list[Element]: + """Return all registered elements in insertion order.""" + return [value for key, value in self._ALL.items()] + + # Tune monitor + + def get_betatron_tune_monitor(self, name: str) -> BetatronTuneMonitor: + """ + Return a named betatron tune monitor. + + Parameters + ---------- + name : str + Name of the betatron tune monitor to look up, as declared in the configuration. + + Returns + ------- + BetatronTuneMonitor + The betatron tune monitor registered under ``name``. + """ + return self._get("Diagnostic", name, self._DIAG) + + def add_betatron_tune_monitor(self, tune_monitor: Element): + """ + Add a betatron tune monitor to the diagnostics store. + + Parameters + ---------- + tune_monitor : Element + Betatron tune monitor to register, keyed by its own name. + """ + self._add(self._DIAG, tune_monitor) + + # Tuning/Measurement tools + + def add_tool(self, tool: Element): + """ + Add a tuning or measurement tool to the tool store. + + Parameters + ---------- + tool : Element + Tuning or measurement tool to register, keyed by its own name. + """ + self._add(self._TOOLS, tool) + + # ---- Chromaticity ------------------------------------------------- + + def get_chromaticity_monitor(self, name: str) -> ChromaticityMonitor: + """ + Return a named chromaticity monitor. + + Parameters + ---------- + name : str + Name of the chromaticity monitor to look up, as declared in the configuration. + + Returns + ------- + ChromaticityMonitor + The chromaticity monitor registered under ``name``. + """ + obj = self._get("Chromaticity monitor", name, self._TOOLS) + return obj + + def get_chromaticity_tuning(self, name: str) -> "Chromaticity": + """ + Return a named chromaticity tuning tool. + + Parameters + ---------- + name : str + Name of the chromaticity tuning tool to look up, as declared in the configuration. + + Returns + ------- + 'Chromaticity' + The chromaticity tuning tool registered under ``name``. + """ + return self._get("Chromaticity tool", name, self._TOOLS) + + def get_crm_tuning(self, name: str) -> "ChromaticityResponseMatrix": + """ + Return a named chromaticity response-matrix tool. + + Parameters + ---------- + name : str + Name of the chromaticity response-matrix tool to look up, as declared in the configuration. + + Returns + ------- + 'ChromaticityResponseMatrix' + The chromaticity response-matrix tool registered under ``name``. + """ + return self._get("ChromaticityResponseMatrix tool", name, self._TOOLS) + + @property + def chromaticity(self) -> "Chromaticity": + """Return the chromaticity.""" + return self.get_chromaticity_tuning("DEFAULT_CHROMATICITY_CORRECTION") + + @property + def crm(self) -> "ChromaticityResponseMatrix": + """Return the crm.""" + return self.get_crm_tuning("DEFAULT_CHROMATICITY_RESPONSE_MATRIX") + + # ---- Tune --------------------------------------------------------- + + def get_tune_tuning(self, name: str) -> "Tune": + """ + Return a named tune correction tool. + + Parameters + ---------- + name : str + Name of the tune correction tool to look up, as declared in the configuration. + + Returns + ------- + 'Tune' + The tune correction tool registered under ``name``. + """ + return self._get("Tune tuning tool", name, self._TOOLS) + + @property + def tune(self) -> "Tune": + """Return the tune.""" + return self.get_tune_tuning("DEFAULT_TUNE_CORRECTION") + + def get_trm_tuning(self, name: str) -> "TuneResponseMatrix": + """ + Return a named tune response-matrix tool. + + Parameters + ---------- + name : str + Name of the tune response-matrix tool to look up, as declared in the configuration. + + Returns + ------- + 'TuneResponseMatrix' + The tune response-matrix tool registered under ``name``. + """ + return self._get("TuneResponseMatrix tool", name, self._TOOLS) + + @property + def trm(self) -> "TuneResponseMatrix": + """Return the default tune response-matrix tool.""" + return self.get_trm_tuning("DEFAULT_TUNE_RESPONSE_MATRIX") + + # ---- Orbit -------------------------------------------------------- + + def get_orbit_tuning(self, name: str) -> "Orbit": + """ + Return a named orbit correction tool. + + Parameters + ---------- + name : str + Name of the orbit correction tool to look up, as declared in the configuration. + + Returns + ------- + 'Orbit' + The orbit correction tool registered under ``name``. + """ + return self._get("Orbit tuning tool", name, self._TOOLS) + + @property + def orbit(self) -> "Orbit": + """Return the orbit.""" + return self.get_orbit_tuning("DEFAULT_ORBIT_CORRECTION") + + def get_orm_tuning(self, name: str) -> "OrbitResponseMatrix": + """ + Return a named orbit response-matrix tool. + + Parameters + ---------- + name : str + Name of the orbit response-matrix tool to look up, as declared in the configuration. + + Returns + ------- + 'OrbitResponseMatrix' + The orbit response-matrix tool registered under ``name``. + """ + return self._get("OrbitResponseMatrix tool", name, self._TOOLS) + + @property + def orm(self) -> "OrbitResponseMatrix": + """Return the default orbit response-matrix tool.""" + return self.get_orm_tuning("DEFAULT_ORBIT_RESPONSE_MATRIX") + + # ---- BBA -------------------------------------------------------- + + def get_bba(self, name: str) -> "BBA": + """ + Return a named beam-based alignment tool. + + Parameters + ---------- + name : str + Name of the beam-based alignment tool to look up, as declared in the configuration. + + Returns + ------- + 'BBA' + The beam-based alignment tool registered under ``name``. + """ + return self._get("BBA tool", name, self._TOOLS) + + # ---- Dispersive orbit -------------------------------------------- + + def get_dispersion_tuning(self, name: str) -> "Dispersion": + """ + Return a named dispersion tuning tool. + + Parameters + ---------- + name : str + Name of the dispersion tuning tool to look up, as declared in the configuration. + + Returns + ------- + 'Dispersion' + The dispersion tuning tool registered under ``name``. + """ + return self._get("Dispersion tool", name, self._TOOLS) + + @property + def dispersion(self) -> "Dispersion": + """Return the dispersion.""" + return self.get_dispersion_tuning("DEFAULT_DISPERSION") + + def _get_array(self, name: str): + """ + Generic array resolver used by YellowPages. + + The method returns the array object referenced by 'name', regardless of its + concrete type. + """ + if name in self._BPM_ARRAYS: + return self._BPM_ARRAYS[name] + if name in self._MAGNET_ARRAYS: + return self._MAGNET_ARRAYS[name] + if name in self._CFM_MAGNET_ARRAYS: + return self._CFM_MAGNET_ARRAYS[name] + if name in self._SERIALIZED_MAGNETS_ARRAYS: + return self._SERIALIZED_MAGNETS_ARRAYS[name] + if name in self._ELEMENT_ARRAYS: + return self._ELEMENT_ARRAYS[name] + + raise PyAMLException(f"Array {name} not defined") + + def _get_tool(self, name: str): + """ + Generic tuning tool resolver used by YellowPages. + """ + if name not in self._TOOLS: + raise PyAMLException(f"Tool {name} not defined") + return self._TOOLS[name] + + def _get_diagnostic(self, name: str): + """ + Generic diagnostic resolver used by YellowPages. + """ + if name not in self._DIAG: + raise PyAMLException(f"Diagnostic {name} not defined") + return self._DIAG[name] + + def _list_arrays(self) -> list[str]: + """ + Return all array identifiers available in this holder. + """ + arrays: list[str] = [] + arrays.extend(self._BPM_ARRAYS.keys()) + arrays.extend(self._MAGNET_ARRAYS.keys()) + arrays.extend(self._CFM_MAGNET_ARRAYS.keys()) + arrays.extend(self._SERIALIZED_MAGNETS_ARRAYS.keys()) + arrays.extend(self._ELEMENT_ARRAYS.keys()) + return arrays + + def _list_tools(self) -> list[str]: + """ + Return all tuning tool identifiers available in this holder. + """ + return list(self._TOOLS.keys()) + + def _list_diagnostics(self) -> list[str]: + """ + Return all diagnostic identifiers available in this holder. + """ + return list(self._DIAG.keys()) + + def _set_energy(self, E: float): + """ + Sets the energy on all elements + + Parameters + ---------- + E : float + Energy in eV + """ + # Needed by energy dependant element (i.e. magnet coil current calculation) + for m in self.get_all_elements(): + m.set_energy(E) + + def _set_mcf(self, alphac: float): + """ + Sets the moment compaction factor on all elements + + Parameters + ---------- + alphac : float + Moment compaction factor + """ + # Needed by some off energy dependant element (i.e. chromaticty tools) + for m in self.get_all_elements(): + m.set_mcf(alphac) + + def _set_harmonic(self, h: int): + """ + Sets the harmonic number (number of bucket) on elements + + Parameters + ---------- + h : int + Harmonic number + """ + for m in self.get_all_elements(): + m.set_harmonic(h) diff --git a/pyaml/common/holders/generic_array_holder.py b/pyaml/common/holders/generic_array_holder.py new file mode 100644 index 000000000..0ce624410 --- /dev/null +++ b/pyaml/common/holders/generic_array_holder.py @@ -0,0 +1,121 @@ +"""Generic typed storage and lookup for arrays of accelerator elements.""" + +from collections.abc import Callable +from typing import TYPE_CHECKING, Generic, TypeVar + +from ..element import Element, __pyaml_repr__ + +if TYPE_CHECKING: + from .element_holder import ElementHolder + +T = TypeVar("T", bound=Element) +A = TypeVar("A") + + +class GenericArrayHolder(Generic[T, A]): + """ + Provide typed access to named arrays of one element type. + + Concrete holders (:class:`.MagnetsHolder`, :class:`.SerializedMagnetsHolder`, + :class:`.CombinedFunctionMagnetsHolder`, ...) subclass this with the + element type ``T`` and the array type ``A`` they handle, so callers keep + full static typing on :meth:`get`, :meth:`add` and :meth:`__getitem__`. + + Parameters + ---------- + peer : 'ElementHolder' + Parent element holder. + array_store : dict[str, A] + Mapping from array names to stored arrays. + all_func : Callable[[], list[T]] + Callback returning all elements. + get_func : Callable[[str], T] + Callback resolving an element by name. + constructor : Callable[[str, list[T]], A] + Callback constructing an array from a name and elements. + what : str + Human-readable array type used for lookup errors. + + Methods + ------- + get(name=None) + Return a named array or a transient array of all elements. + add(arrayName, elementNames) + Create and register a named array from element selectors. + """ + + def __init__( + self, + peer: "ElementHolder", + array_store: dict[str, A], + all_func: Callable[[], list[T]], + get_func: Callable[[str], T], + constructor: Callable[[str, list[T]], A], + what: str, + ): + """ + Initialize an array holder with storage and lookup callbacks. + """ + self._peer = peer + self._array_store = array_store + self._all_func = all_func + self._get_func = get_func + self._constructor = constructor + self._what = what + + def get(self, name: str | None = None) -> A: + """ + Return a named array or a transient array of all elements. + + Parameters + ---------- + name : str or None, optional + Array name. If ``None``, all available elements are returned. + + Returns + ------- + A + Requested named array or an array containing all elements. + """ + if name is None: + return self._constructor("", self._all_func()) + else: + return self._peer._get(self._what, name, self._array_store) + + def add(self, arrayName: str, elementNames: list[str]): + """ + Create and register a named array from element selectors. + + Parameters + ---------- + arrayName : str + Name under which to store the array. + elementNames : list[str] + Names of elements to include, in array order. + + Notes + ----- + Selectors may use the lookup syntax supported by the parent + :class:`~pyaml.common.holders.element_holder.ElementHolder`, including + wildcard and exclusion patterns. + """ + self._peer._fill_array(arrayName, elementNames, self._get_func, self._constructor, self._array_store) + + def __getitem__(self, key): + """ + Return an element from the aggregate array by index. + + Parameters + ---------- + key : int or slice + Index or slice passed to the aggregate array. + + Returns + ------- + object + Element or sub-array selected by ``key``. + """ + return self.get().__getitem__(key) + + def __repr__(self): + return __pyaml_repr__(self) diff --git a/pyaml/common/holders/generic_element_holder.py b/pyaml/common/holders/generic_element_holder.py new file mode 100644 index 000000000..a23dec8b0 --- /dev/null +++ b/pyaml/common/holders/generic_element_holder.py @@ -0,0 +1,93 @@ +"""Generic typed storage and lookup for accelerator elements.""" + +from typing import TYPE_CHECKING, Generic, TypeVar + +from ..element import Element, __pyaml_repr__ + +if TYPE_CHECKING: + from .element_holder import ElementHolder + +T = TypeVar("T", bound=Element) + + +class GenericElementHolder(Generic[T]): + """ + Provide typed name-based access to one category of elements. + + Concrete holders (:class:`.MagnetHolder`, :class:`.SerializedMagnetHolder`, + :class:`.CombinedFunctionMagnetHolder`, ...) subclass this with the + element type they handle, so callers keep full static typing on + :meth:`all`, :meth:`get` and :meth:`add`. + + Parameters + ---------- + peer : 'ElementHolder' + Parent element holder. + store : dict[str, T] + Mapping from element names to elements. + what : str + Human-readable element type used for lookup errors. + + Methods + ------- + all() + Return all stored elements in insertion order. + get(name) + Return the element with the requested name. + add(m) + Add an element to the holder's name-indexed store. + """ + + def __init__(self, peer: "ElementHolder", store: dict[str, T], what: str): + """ + Initialize a holder backed by an element store. + """ + self._peer = peer + self._store = store + self._what = what + + def all(self) -> list[T]: + """ + Return all stored elements in insertion order. + + Returns + ------- + list of T + Elements currently registered in this category. + """ + return [value for key, value in self._store.items()] + + def get(self, name: str) -> T: + """ + Return the element with the requested name. + + Parameters + ---------- + name : str + Element name. + + Returns + ------- + T + Element registered under ``name``. + """ + return self._peer._get(self._what, name, self._store) + + def add(self, m: T): + """ + Add an element to the holder's name-indexed store. + + Parameters + ---------- + m : T + Element to add. + + Returns + ------- + None + This method updates the holder in place. + """ + self._peer._add(self._store, m) + + def __repr__(self): + return __pyaml_repr__(self) diff --git a/pyaml/common/holders/rf_holder.py b/pyaml/common/holders/rf_holder.py new file mode 100644 index 000000000..257c396a4 --- /dev/null +++ b/pyaml/common/holders/rf_holder.py @@ -0,0 +1,154 @@ +"""Holder interfaces for RF plants and their transmitters.""" + +from typing import TYPE_CHECKING + +from ...rf.rf_plant import RFPlant +from ...rf.rf_transmitter import RFTransmitter +from ..abstract import ReadWriteFloatScalar +from ..element import __pyaml_repr__ + +if TYPE_CHECKING: + from .element_holder import ElementHolder + + +class RFTransmitterHolder: + """ + Provide name-based access to RF transmitter elements. + + Parameters + ---------- + peer : 'ElementHolder' + Parent holder containing the transmitter store. + + Methods + ------- + get(name) + Return a transmitter by name. + add(rf) + Add an RF transmitter to the holder. + """ + + def __init__(self, peer: "ElementHolder"): + """ + Initialize a transmitter holder for an element holder. + """ + self._peer = peer + + def get(self, name: str) -> RFTransmitter: + """ + Return a transmitter by name. + + Parameters + ---------- + name : str + Transmitter name. + + Returns + ------- + RFTransmitter + Matching RF transmitter. + """ + return self._peer._get("RFTransmitter", name, self._peer._RFTRANSMITTER) + + def add(self, rf: RFTransmitter): + """ + Add an RF transmitter to the holder. + + Parameters + ---------- + rf : RFTransmitter + Transmitter to add. + + Returns + ------- + None + The transmitter is registered in the parent holder in place. + """ + self._peer._add(self._peer._RFTRANSMITTER, rf) + + def __repr__(self): + return __pyaml_repr__(self) + + +class RFHolder: + """ + Provide access to RF plants and their transmitters. + + Parameters + ---------- + peer : 'ElementHolder' + Parent holder containing the RF plant store. + + Attributes + ---------- + transmitter + Return the holder for RF transmitter elements. + frequency + Return the default RF plant's frequency interface. + voltage + Return the default RF plant's total-voltage interface. + + Methods + ------- + get(name) + Return an RF plant by name. + add(rf) + Add an RF plant to the holder. + """ + + def __init__(self, peer: "ElementHolder"): + """ + Initialize an RF holder for an element holder. + """ + self._peer = peer + self._rftransmitter_holder = RFTransmitterHolder(peer) + + @property + def transmitter(self) -> RFTransmitterHolder: + """Return the holder for RF transmitter elements.""" + return self._rftransmitter_holder + + @property + def frequency(self) -> ReadWriteFloatScalar: + """Return the default RF plant's frequency interface.""" + return self.get("DEFAULT_RF_PLANT").frequency + + @property + def voltage(self) -> ReadWriteFloatScalar: + """Return the default RF plant's total-voltage interface.""" + return self.get("DEFAULT_RF_PLANT").voltage + + def get(self, name: str) -> RFPlant: + """ + Return an RF plant by name. + + Parameters + ---------- + name : str + RF plant name. + + Returns + ------- + RFPlant + RF plant registered under ``name``. + """ + return self._peer._get("RFPlant", name, self._peer._RFPLANT) + + def add(self, rf: RFPlant): + """ + Add an RF plant to the holder. + + Parameters + ---------- + rf : RFPlant + RF plant to add. + + Returns + ------- + None + The plant is registered in the parent holder in place. + """ + self._peer._add(self._peer._RFPLANT, rf) + + def __repr__(self): + return __pyaml_repr__(self) diff --git a/pyaml/common/holders/sub_holders.py b/pyaml/common/holders/sub_holders.py new file mode 100644 index 000000000..399485eb0 --- /dev/null +++ b/pyaml/common/holders/sub_holders.py @@ -0,0 +1,181 @@ +"""Specialized holders for accelerator element categories and arrays.""" + +from typing import TYPE_CHECKING + +from ...arrays.bpm_array import BPMArray +from ...arrays.cfm_magnet_array import CombinedFunctionMagnetArray +from ...arrays.magnet_array import MagnetArray +from ...arrays.serialized_magnet_array import SerializedMagnetsArray +from ...bpm.bpm import BPM +from ...magnet.cfm_magnet import CombinedFunctionMagnet +from ...magnet.magnet import Magnet +from ...magnet.serialized_magnet import SerializedMagnets +from .generic_array_holder import GenericArrayHolder +from .generic_element_holder import GenericElementHolder + +if TYPE_CHECKING: + from .element_holder import ElementHolder + + +class MagnetHolder(GenericElementHolder[Magnet]): + """ + Provide access to individual magnet elements. + + Parameters + ---------- + peer : 'ElementHolder' + Parent element holder that owns this specialized holder. + """ + + def __init__(self, peer: "ElementHolder"): + """ + Initialize the MagnetHolder. + """ + super().__init__(peer, peer._MAGNETS, "Magnet") + + +class MagnetsHolder(GenericArrayHolder[Magnet, MagnetArray]): + """ + Provide access to arrays of individual magnets. + + Parameters + ---------- + peer : 'ElementHolder' + Parent element holder that owns this specialized holder. + """ + + def __init__(self, peer: "ElementHolder"): + """ + Initialize the MagnetsHolder. + """ + super().__init__( + peer, + peer._MAGNET_ARRAYS, + peer.magnet.all, + peer.magnet.get, + MagnetArray, + "Magnet array", + ) + + +class CombinedFunctionMagnetHolder(GenericElementHolder[CombinedFunctionMagnet]): + """ + Provide access to individual combined-function magnets. + + Parameters + ---------- + peer : 'ElementHolder' + Parent element holder that owns this specialized holder. + """ + + def __init__(self, peer: "ElementHolder"): + """ + Initialize the CombinedFunctionMagnetHolder. + """ + super().__init__(peer, peer._CFM_MAGNETS, "Combined function magnet") + + +class CombinedFunctionMagnetsHolder(GenericArrayHolder[CombinedFunctionMagnet, CombinedFunctionMagnetArray]): + """ + Provide access to arrays of combined-function magnets. + + Parameters + ---------- + peer : 'ElementHolder' + Parent element holder that owns this specialized holder. + """ + + def __init__(self, peer: "ElementHolder"): + """ + Initialize the CombinedFunctionMagnetsHolder. + """ + super().__init__( + peer, + peer._CFM_MAGNET_ARRAYS, + peer.combined_function_magnet.all, + peer.combined_function_magnet.get, + CombinedFunctionMagnetArray, + "Combined function magnet array", + ) + + +class SerializedMagnetHolder(GenericElementHolder[SerializedMagnets]): + """ + Provide access to individual serialized magnet groups. + + Parameters + ---------- + peer : 'ElementHolder' + Parent element holder that owns this specialized holder. + """ + + def __init__(self, peer: "ElementHolder"): + """ + Initialize the SerializedMagnetHolder. + """ + super().__init__(peer, peer._SERIALIZED_MAGNETS, "Serialized magnet") + + +class SerializedMagnetsHolder(GenericArrayHolder[SerializedMagnets, SerializedMagnetsArray]): + """ + Provide access to arrays of serialized magnet groups. + + Parameters + ---------- + peer : 'ElementHolder' + Parent element holder that owns this specialized holder. + """ + + def __init__(self, peer: "ElementHolder"): + """ + Initialize the SerializedMagnetsHolder. + """ + super().__init__( + peer, + peer._SERIALIZED_MAGNETS_ARRAYS, + peer.serialized_magnet.all, + peer.serialized_magnet.get, + SerializedMagnetsArray, + "serialized magnet array", + ) + + +class BPMHolder(GenericElementHolder[BPM]): + """ + Provide access to individual beam-position monitors. + + Parameters + ---------- + peer : 'ElementHolder' + Parent element holder that owns this specialized holder. + """ + + def __init__(self, peer: "ElementHolder"): + """ + Initialize the BPMHolder. + """ + super().__init__(peer, peer._BPMS, "BPM") + + +class BPMsHolder(GenericArrayHolder[BPM, BPMArray]): + """ + Provide access to arrays of beam-position monitors. + + Parameters + ---------- + peer : 'ElementHolder' + Parent element holder that owns this specialized holder. + """ + + def __init__(self, peer: "ElementHolder"): + """ + Initialize the BPMsHolder. + """ + super().__init__( + peer, + peer._BPM_ARRAYS, + peer.bpm.all, + peer.bpm.get, + BPMArray, + "BPM array", + ) diff --git a/pyaml/configuration/__init__.py b/pyaml/configuration/__init__.py index a9bf89d7c..12346acf8 100644 --- a/pyaml/configuration/__init__.py +++ b/pyaml/configuration/__init__.py @@ -3,13 +3,12 @@ """ from .factory import Factory -from .fileloader import get_root_folder, set_root_folder +from .fileloader import ROOT from .manager import ConfigurationManager, UnsupportedConfigurationRootError __all__ = [ "ConfigurationManager", "UnsupportedConfigurationRootError", "Factory", - "get_root_folder", - "set_root_folder", + "ROOT", ] diff --git a/pyaml/configuration/csvcurve.py b/pyaml/configuration/csvcurve.py deleted file mode 100644 index ef8352d37..000000000 --- a/pyaml/configuration/csvcurve.py +++ /dev/null @@ -1,60 +0,0 @@ -from pathlib import Path - -import numpy as np -from pydantic import BaseModel, ConfigDict - -from ..common.exception import PyAMLException -from ..configuration.fileloader import get_path -from .curve import Curve - -# Define the main class name for this module -PYAMLCLASS = "CSVCurve" - - -class ConfigModel(BaseModel): - """ - Configuration model for CSV curve - - Parameters - ---------- - file : str - CSV file that contains the curve (n rows, 2 columns) - """ - - model_config = ConfigDict(arbitrary_types_allowed=True, extra="forbid") - - file: str - - -class CSVCurve(Curve): - """ - Class for load CSV (x,y) curve - """ - - def __init__(self, cfg: ConfigModel): - self._cfg = cfg - - # Load CSV curve - path = get_path(cfg.file) - try: - self._curve = np.genfromtxt(path, delimiter=",", dtype=float, loose=False) - except ValueError as e: - raise PyAMLException(f"CSVCurve(file='{cfg.file}',dtype=float): {str(e)}") from None - - _s = np.shape(self._curve) - if len(_s) != 2 or _s[1] != 2: - raise PyAMLException(f"CSVCurve(file='{cfg.file}',dtype=float):wrong shape (2,2) expected but got {str(_s)}") - - def get_curve(self) -> np.array: - """ - Get the curve data. - - Returns - ------- - np.array - Curve data as a 2D numpy array of shape (n, 2) - """ - return self._curve - - def __repr__(self): - return repr(self._cfg).replace("ConfigModel", self.__class__.__name__) diff --git a/pyaml/configuration/csvmatrix.py b/pyaml/configuration/csvmatrix.py deleted file mode 100644 index 993cec99d..000000000 --- a/pyaml/configuration/csvmatrix.py +++ /dev/null @@ -1,55 +0,0 @@ -from pathlib import Path - -import numpy as np -from pydantic import BaseModel, ConfigDict - -from ..common.exception import PyAMLException -from ..configuration.fileloader import get_path -from .matrix import Matrix - -# Define the main class name for this module -PYAMLCLASS = "CSVMatrix" - - -class ConfigModel(BaseModel): - """ - Configuration model for CSV matrix - - Parameters - ---------- - file : str - CSV file that contains the matrix - """ - - model_config = ConfigDict(arbitrary_types_allowed=True, extra="forbid") - - file: str - - -class CSVMatrix(Matrix): - """ - Class for loading CSV matrix - """ - - def __init__(self, cfg: ConfigModel): - self._cfg = cfg - # Load CSV matrix - path = get_path(cfg.file) - try: - self._mat = np.genfromtxt(path, delimiter=",", dtype=float, loose=False) - except ValueError as e: - raise PyAMLException(f"CSVMatrix(file='{cfg.file}',dtype=float): {str(e)}") from None - - def get_matrix(self) -> np.array: - """ - Get the matrix data. - - Returns - ------- - np.array - Matrix data as a numpy array - """ - return self._mat - - def __repr__(self): - return repr(self._cfg).replace("ConfigModel", self.__class__.__name__) diff --git a/pyaml/configuration/curve.py b/pyaml/configuration/curve.py deleted file mode 100644 index df73ec016..000000000 --- a/pyaml/configuration/curve.py +++ /dev/null @@ -1,32 +0,0 @@ -from abc import ABCMeta, abstractmethod - -import numpy as np - - -class Curve(metaclass=ABCMeta): - """ - Abstract class providing access to a curve - """ - - @abstractmethod - def get_curve(self) -> np.array: - """ - Returns the curve (n rows,2 columns). - Curve is expected to be monotonic (non-decreasing or non-increasing). - """ - pass - - @classmethod - def inverse(cls, curve: np.array) -> np.array: - """ - Returns the inverse curve. - Basically swap x and y and sort y in ascending order. - - Parameters - ---------- - curve : np.array - Curve to be inverted - """ - __curve = curve - __sortedCurve = __curve[__curve[:, 1].argsort()] - return __sortedCurve[:, [1, 0]] diff --git a/pyaml/configuration/factory.py b/pyaml/configuration/factory.py index 8078a3109..445ce9665 100644 --- a/pyaml/configuration/factory.py +++ b/pyaml/configuration/factory.py @@ -1,225 +1,479 @@ -# PyAML factory (construct AML objects from config files) +""" +Build PyAML objects from configuration dictionaries and lists. + +The factory resolves class paths, optionally validates configuration with +Pydantic models, recursively builds nested values, and registers constructed +accelerator elements. +""" + import fnmatch -import importlib -from threading import Lock -from typing import TypedDict, get_type_hints +from dataclasses import dataclass +from importlib import import_module +from types import ModuleType +from typing import Any, TypeVar -from pydantic import ValidationError +from pydantic import BaseModel, ValidationError from ..common.element import Element from ..common.exception import PyAMLConfigException +from ..validation.errors import raise_validation_error +from ..validation.schema_builder import generate_class_path from .unbound_element import UnboundElement +# --------------------------------------------------------------------- +# Element registry +# --------------------------------------------------------------------- -class PyAMLFactory: - """Singleton factory to build PyAML elements with future compatibility logic.""" +TElement = TypeVar("TElement", bound=Element) + + +class ElementRegistry: + """ + Singleton registry of all instantiated Elements. + + Elements are registered by name and can later be retrieved + individually, by wildcard pattern, or by type. + + Methods + ------- + register(element) + Register an Element by name. + get(name) + Return an Element by name. + get_by_name(wildcard) + Return all elements whose name matches a wildcard pattern. + get_by_type(element_type) + Return all registered elements of the given type. + clear() + Remove all registered elements. + """ _instance = None - _lock = Lock() def __new__(cls): """ - No matter how many times you call PyAMLFactory(), - it will be created only once. - """ - with cls._lock: - if cls._instance is None: - cls._instance = super().__new__(cls) - cls._instance._elements = {} - cls._instance._strategies = [] - return cls._instance - - def handle_validation_error(self, e, type_str: str, location_str: str, field_locations: dict): - # Handle pydantic errors - globalMessage = "" - for err in e.errors(): - msg = err["msg"] - field = "" - if len(err["loc"]) == 2: - field, fieldIdx = err["loc"] - message = f"'{field}.{fieldIdx}': {msg}" - else: - field = err["loc"][0] - message = f"'{field}': {msg}" - if field_locations and field in field_locations: - file, line, col = field_locations[field] - loc = f"{file} at line {line}, colum {col}" - message += f" {loc}" - globalMessage += message - globalMessage += ", " - # Discard pydantic stack trace - raise PyAMLConfigException(f"{globalMessage} for object: '{type_str}' {location_str}") from None - - def get_field_type(self, config_cls, field_name) -> type: - # Get type of a pydantic ConfigModel field - if config_cls is None: - return None - type_hints = get_type_hints(config_cls) - return type_hints[field_name] if field_name in type_hints else None - - def get_infos(self, d, ignore_external: bool): - # Retrieve informations of object to be constructed - location = d["__location__"] if "__location__" in d else None - field_locations = d["__fieldlocations__"] if "__fieldlocations__" in d else None - location_str = "" - if location: - file, line, col = location - location_str = f"{file} at line {line}, column {col}." - - if not isinstance(d, dict): - raise PyAMLConfigException(f"Unexpected object {str(d)} {location_str}") - if "type" not in d: - raise PyAMLConfigException(f"No type specified for {str(type(d))}:{str(d)} {location_str}") - - module_str = d["type"] - class_str = d["class"] if "class" in d else None - validation_class_str = d["validation_class"] if "validation_class" in d else "ConfigModel" - - # Import the module + Return the singleton registry instance. + """ + + if cls._instance is None: + cls._instance = super().__new__(cls) + cls._instance._elements = {} + return cls._instance + + def register(self, element: Element) -> None: + """ + Register an Element by name. + + Parameters + ---------- + element : Element + Element to register. + + Raises + ------ + PyAMLConfigException + If the object is not an Element or if another element + with the same name is already registered. + """ + + if not isinstance(element, Element): + raise PyAMLConfigException(f"Cannot register object of type '{type(element).__name__}' since expected Element.") + + name = element.get_name() + if name in self._elements: + raise PyAMLConfigException(f"Element {name} already defined.") + self._elements[name] = element + + def get(self, name: str) -> Element: + """ + Return an Element by name. + + Parameters + ---------- + name : str + Element name. + + Returns + ------- + Element + Registered element. + + Raises + ------ + PyAMLConfigException + If the element is not registered. + """ + try: - module = importlib.import_module(module_str) - except ModuleNotFoundError as ex: - if not ignore_external: - # Discard module not found stack trace - raise PyAMLConfigException( - "Module referenced in type cannot be found:" + f"'{module_str}' {location_str}" - ) from None - else: - return None + return self._elements[name] + except KeyError: + raise PyAMLConfigException(f"Element {name} not defined.") from None - # Get the object class name - if class_str is None: - class_str = getattr(module, "PYAMLCLASS", None) - if class_str is None: - raise PyAMLConfigException( - f"PYAMLCLASS definition not found or class not specified in '{module_str}' {location_str}" - ) + def get_by_name(self, wildcard: str) -> list[Element]: + """ + Return all elements whose name matches a wildcard pattern. + + Parameters + ---------- + wildcard : str + Wildcard expression compatible with ``fnmatch``. + + Returns + ------- + list[Element] + Matching elements. + """ + + return [e for n, e in self._elements.items() if fnmatch.fnmatch(n, wildcard)] + + def get_by_type(self, element_type: type[TElement]) -> list[TElement]: + """ + Return all registered elements of the given type. + + Parameters + ---------- + element_type : type[Element] + Element type to match. + + Returns + ------- + list[TElement] + Matching elements. + """ + + return [e for e in self._elements.values() if isinstance(e, element_type)] + + def clear(self) -> None: + """ + Remove all registered elements. + """ + + self._elements.clear() + + def __contains__(self, name: str) -> bool: + """ + Return whether an element with the given name is registered. + """ + + return name in self._elements + + def __len__(self) -> int: + """ + Return the number of registered elements. + """ - # Get the validation class - config_cls = getattr(module, validation_class_str, None) + return len(self._elements) + + +# Global element registry used during configuration loading. +ELEMENT_REGISTRY = ElementRegistry() + +# --------------------------------------------------------------------- +# Handle build information +# --------------------------------------------------------------------- + +NEW_KEYS = ("class", "class_path") +LEGACY_KEY = "type" +BUILD_KEYS = NEW_KEYS + (LEGACY_KEY,) + + +@dataclass(frozen=True) +class BuildInfo: + """ + Store the resolved information required to construct one object. + + Attributes + ---------- + module : types.ModuleType + Module containing the target class. + config_cls : type[pydantic.BaseModel] or None + Optional configuration model used to validate the object data. + class_cls : type + Class to instantiate. + control_modes : list of str or None + Control-system modes for creating an :class:`UnboundElement`. + config : dict of str to object + Remaining constructor configuration. + """ + + module: ModuleType + config_cls: type[BaseModel] | None # Legacy + class_cls: type[Any] + control_modes: list[str] | None + config: dict[str, Any] + + +def _import_module(module_path: str, ignore_external: bool) -> ModuleType | None: + """ + Import a module referenced by a configuration class path. + + Parameters + ---------- + module_path : str + Dotted module path to import. + ignore_external : bool + If ``True``, return ``None`` when the module is unavailable. + + Returns + ------- + ModuleType | None + Imported module, or ``None`` when an external module is ignored. + """ + try: + return import_module(module_path) + except ModuleNotFoundError as exc: + if ignore_external: + return None + raise PyAMLConfigException(f"Module '{module_path}' cannot be found: {exc}") from None + + +def _resolve_class_name(module: ModuleType, module_path: str) -> str: + # Legacy + """ + Resolve the legacy default class name exposed by a module. + + Parameters + ---------- + module : ModuleType + Imported module containing ``PYAMLCLASS``. + module_path : str + Module path used in configuration error messages. + + Returns + ------- + str + Class name stored in the module's ``PYAMLCLASS`` attribute. + """ + class_name = getattr(module, "PYAMLCLASS", None) + if class_name is None: + raise PyAMLConfigException(f"Module '{module_path}' does not define PYAMLCLASS.") + return class_name + + +def _resolve_build_info(data: dict, ignore_external: bool) -> BuildInfo | None: + """ + Resolve a configuration mapping into object-construction metadata. + + Parameters + ---------- + data : dict + Configuration mapping containing a legacy ``type`` or a class path. + ignore_external : bool + If ``True``, ignore unavailable external modules. + + Returns + ------- + BuildInfo | None + Resolved build metadata, or ``None`` for an ignored external module. + """ + if not isinstance(data, dict): + raise PyAMLConfigException(f"Unexpected object {data!r}. It needs to be a dict.") + + config = dict(data) + + if LEGACY_KEY in config: + # Legacy module/class format: + # type: some.module + # class: MyClass (optional; otherwise PYAMLCLASS is used) + + module_path = config.pop(LEGACY_KEY, None) + + module = _import_module(module_path, ignore_external) + if module is None: + return None + + class_name = config.pop("class", None) + if class_name is None: + class_name = _resolve_class_name(module, module_path) + + class_path = f"{module_path}.{class_name}" + + else: + # New class_path/class alias format: + # class_path: some.module.MyClass + # or + # class: some.module.MyClass + + present = [key for key in NEW_KEYS if key in data] + if len(present) != 1: + raise PyAMLConfigException(f"Exactly one of {NEW_KEYS} must be specified when '{LEGACY_KEY}' is not used.") + + class_key = present[0] + class_path = config.pop(class_key, None) + module_path, class_name = class_path.rsplit(".", 1) + + module = _import_module(module_path, ignore_external) + if module is None: + return None + + # Get the class + class_cls = getattr(module, class_name, None) + if class_cls is None: + raise PyAMLConfigException(f"Unknown class '{class_path}'.") + + # Get the config class if it exists + validation_class_name = config.pop("validation_class", None) + + if validation_class_name is not None: + config_cls = getattr(module, validation_class_name, None) if config_cls is None: - raise PyAMLConfigException(f"No validation class for '{module.__name__}.{class_str}' {location_str}") + raise PyAMLConfigException(f"Module '{module_path}' does not define validation class '{validation_class_name}'.") + else: + config_cls = getattr(module, "ConfigModel", None) - return (module, config_cls, class_str, field_locations, location_str) + control_modes = config.pop("control_modes", None) + if control_modes is not None and not isinstance(control_modes, list): + raise PyAMLConfigException(f"'control_modes' must be a list, got '{type(control_modes).__name__}'.") - def build_object(self, d: dict, ignore_external: bool = False): - """Build an object from the dict""" + return BuildInfo(module=module, config_cls=config_cls, class_cls=class_cls, control_modes=control_modes, config=config) - (module, config_cls, class_str, field_locations, location_str) = self.get_infos(d, ignore_external) - # Clean up dict - d.pop("__location__", None) - d.pop("__fieldlocations__", None) - d.pop("type") - d.pop("class", None) - d.pop("validation_class", None) - control_modes = d.pop("control_modes", None) +# --------------------------------------------------------------------- +# Factory +# --------------------------------------------------------------------- - # Validate the model - try: - cfg = config_cls.model_validate(d) - except ValidationError as e: - self.handle_validation_error(e, module.__name__, location_str, field_locations) - elem_cls = getattr(module, class_str, None) - if elem_cls is None: - raise PyAMLConfigException(f"Unknown element class '{module.__name__}.{class_str}' {location_str}") +class PyAMLFactory: + """ + Construct PyAML objects from recursively nested configuration data. + + Methods + ------- + build(data, ignore_external=False) + Build objects from a top-level mapping or sequence. + clear() + Remove all registered elements from the global registry. + """ + + def build(self, data: dict | list, ignore_external: bool = False) -> Any: + """ + Build objects from a top-level mapping or sequence. - if control_modes is None: - # Immediate contruction of the object - try: - obj = elem_cls(cfg) - self.register_element(obj) - except Exception as e: - raise PyAMLConfigException(f"{str(e)} when creating '{module.__name__}.{class_str}' {location_str}") from e + Parameters + ---------- + data : dict | list + Configuration dictionary or list to resolve. + ignore_external : bool + If ``True``, ignore unavailable external modules. + + Returns + ------- + Any + Built object, list, or recursively processed mapping. + """ + if not isinstance(data, (dict, list)): + raise PyAMLConfigException(f"Unexpected element found. Expected 'dict' or 'list' but got '{type(data).__name__}'") - else: - # Delayed construction - # An UnboundElement will be constructuced during the filling of the ElementHolder - try: - obj = UnboundElement(elem_cls, module.__name__, control_modes, cfg) - self.register_element(obj) - except Exception as e: - raise PyAMLConfigException( - f"{str(e)} when creating unbounded '{module.__name__}.{class_str}' {location_str}" - ) from e + return self._build(data, ignore_external) - return obj + def _build(self, value: Any, ignore_external: bool = False): + """ + Recursively build one configuration value. - def build_unbound(self, e: UnboundElement, holder) -> Element: - try: - obj = e._class(holder, e._config) - except Exception as ex: - raise PyAMLConfigException(f"{str(ex)} when creating '{e._module_name}.{e._class.__name__}'") from ex + Parameters + ---------- + value : Any + Value to process; mappings and lists are traversed recursively. + ignore_external : bool + If ``True``, ignore unavailable external modules. + """ + if isinstance(value, list): + return self._build_list(value, ignore_external) - if not isinstance(obj, Element): - raise PyAMLConfigException(f"'{e._module_name}.{e._class.__name__}' is not a sub class of Element") + if isinstance(value, dict): + return self._build_dict(value, ignore_external) - obj._peer = holder + return value - return obj + def _build_list(self, items: list[Any], ignore_external: bool = False): + """ + Recursively build every item in a configuration list. + + Parameters + ---------- + items : list[Any] + Items to process. + ignore_external : bool + If ``True``, ignore unavailable external modules. + """ + return [self._build(item, ignore_external) for item in items] + + def _build_dict(self, data: dict, ignore_external: bool = False): + """ + Recursively build a mapping or instantiate its declared object. - def depth_first_build(self, d, ignore_external: bool): + Parameters + ---------- + data : dict + Configuration mapping to process. + ignore_external : bool + If ``True``, ignore unavailable external modules. """ - Main factory function (Depth-first factory) + if any(key in data for key in BUILD_KEYS): + return self._build_object(data, ignore_external) + + return {key: self._build(value, ignore_external) for key, value in data.items()} + + def _build_object(self, data: dict, ignore_external: bool = False): + """ + Validate and instantiate an object declared by a configuration mapping. Parameters ---------- - ignore_external: bool - Ignore `module not found` and return None when an object cannot be created + data : dict + Mapping containing a class declaration and constructor data. + ignore_external : bool + If ``True``, ignore unavailable external modules. """ + build_info = _resolve_build_info(data, ignore_external) + if build_info is None: + return None + + config = {key: self._build(value, ignore_external) for key, value in build_info.config.items()} - if isinstance(d, list): - # list can be a list of objects or a list of native types - l = [] - for _index, e in enumerate(d): - if isinstance(e, dict) or isinstance(e, list): - obj = self.depth_first_build(e, ignore_external) - l.append(obj) + if build_info.config_cls is not None: + try: + cfg = build_info.config_cls.model_validate(config) + except ValidationError as exc: + raise_validation_error( + exc, + class_path=generate_class_path(build_info.config_cls), + ) + else: + cfg = config + + try: + if build_info.control_modes is None: + if isinstance(cfg, dict): + obj = build_info.class_cls(**cfg) else: - l.append(e) - return l - - elif isinstance(d, dict): - _, config_cls, *_ = self.get_infos(d, ignore_external) - - for key, value in d.items(): - if not key == "__fieldlocations__": - if isinstance(value, dict) or isinstance(value, list): - # Get the type of the field - fieldType = self.get_field_type(config_cls, key) - # Do not recurse dict defined in ConfigModel - # pydantic use TypedDict not usable with isinstance - if str(fieldType) != "": - obj = self.depth_first_build(value, ignore_external) - # Replace the inner dict by the object itself - d[key] = obj - - # We are now on leaf (no nested object), we can construct - return self.build_object(d, ignore_external) - - raise PyAMLConfigException("Unexpected element found. 'dict' or 'list' expected but got '{d.__class__.__name__}'") - - def register_element(self, elt): - if isinstance(elt, Element): - name = elt.get_name() - if name in self._elements: - raise PyAMLConfigException(f"element {name} already defined") - self._elements[name] = elt - - def get_element(self, name: str): - if name not in self._elements: - raise PyAMLConfigException(f"element {name} not defined") - return self._elements[name] - - def get_elements_by_name(self, wildcard: str) -> list[Element]: - return [e for k, e in self._elements.items() if fnmatch.fnmatch(k, wildcard)] - - def get_elements_by_type(self, type) -> list[Element]: - return [e for k, e in self._elements.items() if isinstance(e, type)] + obj = build_info.class_cls(cfg) + + else: + obj = UnboundElement( + build_info.class_cls, + build_info.module.__name__, + build_info.control_modes, + cfg, + ) + except Exception as exc: + mode = " unbounded" if build_info.control_modes is not None else "" + raise PyAMLConfigException( + f"{exc} when creating{mode} '{build_info.module.__name__}.{build_info.class_cls.__name__}'" + ) from exc + + if isinstance(obj, Element): + ELEMENT_REGISTRY.register(obj) + + return obj def clear(self): - self._elements.clear() + """ + Remove all registered elements from the global registry. + """ + ELEMENT_REGISTRY.clear() +# Shared factory instance maintained for compatibility with +# existing code using Factory.build(...) and Factory.clear(...). Factory = PyAMLFactory() diff --git a/pyaml/configuration/fileloader.py b/pyaml/configuration/fileloader.py index 9aa652a7a..ef5f9f0eb 100644 --- a/pyaml/configuration/fileloader.py +++ b/pyaml/configuration/fileloader.py @@ -1,168 +1,630 @@ -# PyAML config file loader -import collections.abc +""" +Load PyAML configuration files and expand nested references. + +The loader supports YAML and JSON files, environment and path resolvers, +recursive file includes, and optional source-location metadata for diagnostics. +""" + import io import json import logging import os +import re +from abc import ABC, abstractmethod +from collections.abc import Callable, Hashable +from contextlib import contextmanager +from dataclasses import dataclass, field from pathlib import Path -from typing import TYPE_CHECKING, Union +from typing import Any, Union import yaml from yaml import CLoader from yaml.constructor import ConstructorError from yaml.loader import SafeLoader -from pyaml.configuration.factory import Factory - from .. import PyAMLException -if TYPE_CHECKING: - from pyaml.accelerator import Accelerator - - logger = logging.getLogger(__name__) -accepted_suffixes = [".yaml", ".yml", ".json"] -FILE_PREFIX = "file:" -ROOT = {"path": Path.cwd().resolve()} +LOCATION_KEY = "__location__" +FIELD_LOCATIONS_KEY = "__fieldlocations__" +ACCEPTED_SUFFIXES = (".yaml", ".yml", ".json") +RESOLVER_PATTERN = re.compile(r"\$\{([^{}]+)\}") -def set_root_folder(path: Union[str, Path]): +class RootFolder: """ - Set the root path for configuration files. + Manage the base directory for relative configuration paths. + + Parameters + ---------- + path : str or pathlib.Path or None, optional + Directory used to resolve relative paths. + + Methods + ------- + set(path) + Set the directory used to resolve relative configuration files. + get() + Return the resolved configuration root directory. + expand_path(path) + Resolve a configuration path against the root directory. """ - ROOT["path"] = Path(path) + def __init__(self, path: str | Path | None = None): + """ + Initialize the configuration path root. -def get_root_folder() -> Path: - """ - Get the root path for configuration files. - """ - return ROOT["path"] + If ``path`` is omitted, the current working directory is used. + """ + if path is None: + self._path = Path.cwd().resolve() + else: + self._path = Path(path).resolve() + def set(self, path: str | Path) -> None: + """ + Set the directory used to resolve relative configuration files. -def get_path(p: Path) -> Path: - """ - Return unchanged input path if it is an absolute path, - path relative to root folder otherwise. - """ - if os.path.isabs(p): - return p - else: - root = get_root_folder() - return root / p + Parameters + ---------- + path : str or pathlib.Path + New configuration root directory. + """ + self._path = Path(path).resolve() + + def get(self) -> Path: + """Return the resolved configuration root directory.""" + return self._path + + def expand_path(self, path: str | Path) -> Path: + """ + Resolve a configuration path against the root directory. + + Relative paths are interpreted relative to the configured root folder. + + Parameters + ---------- + path : str or pathlib.Path + Path to resolve. + + Returns + ------- + pathlib.Path + Absolute, normalized path. + """ + + path = Path(path) + if not path.is_absolute(): + path = self._path / path + return path.resolve() + + +ROOT = RootFolder() class PyAMLConfigCyclingException(PyAMLException): + """ + Raised when a configuration file includes itself through a cycle. + + Parameters + ---------- + error_filename : str + File that triggered the cycle. + path_stack : list[pathlib.Path] + Include chain leading to the cycle. + """ + def __init__(self, error_filename: str, path_stack: list[Path]): + """ + Initialize an exception describing a circular file include. + """ + self.error_filename = error_filename + parent_file_stack = [parent_path.name for parent_path in path_stack] super().__init__(f"Circular file inclusion of {error_filename}. File list before reaching it: {parent_file_stack}") - pass +@dataclass +class LoadContext: + """ + Track include state during one recursive loading session. + + Parameters + ---------- + include_locations : bool, optional + Preserve source locations in loaded mappings. + include_stack : list[pathlib.Path], optional + Active include chain. Usually left empty for a new session. + + Methods + ------- + loading(path) + Temporarily add a file to the active include chain. + """ -def load(filename: str, paths_stack: list = None, use_fast_loader: bool = False) -> Union[dict, list]: - """Load recursively a configuration setup""" - if filename.endswith(".yaml") or filename.endswith(".yml"): - l = YAMLLoader(filename, paths_stack, use_fast_loader) - elif filename.endswith(".json"): - l = JSONLoader(filename, paths_stack, use_fast_loader) - else: - raise PyAMLException(f"{filename} File format not supported (only .yaml .yml or .json)") - return l.load() + include_locations: bool = False + include_stack: list[Path] = field(default_factory=list) + @contextmanager + def loading(self, path: Path): + """ + Temporarily add a file to the active include chain. -# Expand condition -def hasToLoad(value): - return isinstance(value, str) and any(value.endswith(suffix) for suffix in accepted_suffixes) + Parameters + ---------- + path : pathlib.Path + File that is about to be loaded. + Raises + ------ + PyAMLConfigCyclingException + If ``path`` is already on the active include stack. + """ -# Loader base class (nested files expansion) -class Loader: - def __init__(self, filename: str, parent_path_stack: list[Path]): - self.path: Path = get_path(filename) - self.files_stack: list[Path] = [] - if parent_path_stack: - if any(self.path.samefile(parent_path) for parent_path in parent_path_stack): - raise PyAMLConfigCyclingException(filename, parent_path_stack) - self.files_stack.extend(parent_path_stack) - self.files_stack.append(self.path) + # Check if the file is currently in the chain + # Raise a cycling error if that is the case + if path in self.include_stack: + raise PyAMLConfigCyclingException(path.name, self.include_stack) + + # Add the file to the stack to record that it is now being loaded + self.include_stack.append(path) + try: + # Run the code in the with block + yield + finally: + # Remove the file to stack to record that it has finished loading + self.include_stack.pop() + + +Resolver = Callable[[str, LoadContext | None], Any] +RESOLVERS: dict[str, Resolver] = {} + + +def resolver(name: str): + """ + Register a function as a configuration value resolver. + + Args: + name: Prefix used to invoke the resolver (for example ``"env"`` + or ``"file"``). + + Returns: + A decorator that registers the decorated function in the global + resolver registry. + """ + + def decorate(func: Resolver) -> Resolver: + """ + Register ``func`` under the resolver prefix. + + Parameters + ---------- + func : Resolver + Resolver function accepting a payload and loading context. + + Returns + ------- + Resolver + The original resolver function. + """ + RESOLVERS[name] = func + return func + + return decorate + + +@resolver("env") +def resolve_env(value: str, _context: LoadContext | None = None) -> str: + """ + Resolve an environment variable by name. + + Parameters + ---------- + value : str + Name of the environment variable. + _context : LoadContext or None, optional + Unused loading context retained for resolver compatibility. + + Returns + ------- + str + Environment variable value. + + Raises + ------ + PyAMLException + If the environment variable is not set. + """ + try: + return os.environ[value] + except KeyError as exc: + raise PyAMLException(f"Environment variable '{value}' is not set") from exc + + +@resolver("path") +def resolve_path(value: str, _context: LoadContext | None = None) -> str: + """ + Resolve a configuration path without loading the file. + + Relative paths are expanded using the configured root folder. + + Parameters + ---------- + value : str + Path to resolve. + _context : LoadContext or None, optional + Unused loading context retained for resolver compatibility. + + Returns + ------- + str + Absolute, normalized path. + """ + return str(ROOT.expand_path(value)) + + +@resolver("file") +def resolve_file(value: str, context: LoadContext | None = None) -> Any: + """ + Load and return the contents of a configuration file. + + Parameters + ---------- + value : str + Path to the configuration file. + context : LoadContext, optional + Shared loading context used to detect inclusion cycles. + + Returns + ------- + object + Parsed and expanded configuration data. + + Raises + ------ + RuntimeError + If no loading context is provided. + """ + if context is None: + raise RuntimeError("File resolver requires LoadContext") + return _load(value, context) + + +def load(filename: str, include_locations: bool = False) -> Union[dict, list]: + """ + Load a configuration file. + + When include_locations is False, uses the faster C-based YAML loader + and skips including source location metadata. + """ + + # Create a new context + context = LoadContext(include_locations=include_locations) + + return _load(filename, context) + + +def _load(filename: str, context: LoadContext) -> Union[dict, list]: + """Load a single configuration file using the appropriate parser.""" + + path = ROOT.expand_path(filename) + + with context.loading(path): + if filename.endswith((".yaml", ".yml")): + loader = YAMLLoader(path, context) + elif filename.endswith(".json"): + loader = JSONLoader(path, context) + else: + raise PyAMLException(f"{filename} File format not supported (only .yaml .yml or .json)") + + return loader.load() + + +def _is_supported_file(value: Any) -> bool: + """Return True if the value looks like a supported configuration file name.""" + return isinstance(value, str) and value.endswith(ACCEPTED_SUFFIXES) + + +class ConfigLoader(ABC): + """ + Base class for parsers that expand nested configuration references. + + Parameters + ---------- + path : pathlib.Path + Configuration file being loaded. + context : LoadContext + Shared state for recursive includes and cycle detection. + + Methods + ------- + expand(obj) + Recursively expand configuration values. + load() + Load and parse the current configuration file. + """ + + def __init__(self, path: Path, context: LoadContext): + """Store the file path and shared loading context.""" + + self.path = path + self.context = context + + def expand(self, obj: Union[dict, list, Any]) -> Union[dict, list, Any]: + """ + Recursively expand configuration values. + + Dictionaries and lists are traversed recursively, while string values + are resolved using the registered resolvers. All other values are + returned unchanged. + """ - # Recursively expand a dict - def expand_dict(self, d: dict): - for key, value in d.items(): - try: - if hasToLoad(value): - if value.startswith(FILE_PREFIX): - # remove prefix - stripped_value = value[len(FILE_PREFIX) :] - d[key] = str(get_root_folder() / Path(stripped_value)) - else: - d[key] = load(value, self.files_stack, self.use_fast_loader) - else: - self.expand(value) - except PyAMLConfigCyclingException as pyaml_ex: - location = d.pop("__location__", None) - field_locations = d.pop("__fieldlocations__", None) - location_str = "" - if location: - file, line, col = location - if field_locations and key in field_locations: - location = field_locations[key] - file, line, col = location - location_str = f" in {file} at line {line}, column {col}" - raise PyAMLException(f"Circular file inclusion of {pyaml_ex.error_filename}{location_str}") from pyaml_ex - - # Recursively expand a list - def expand_list(self, l: list): - idx = 0 - while idx < len(l): - value = l[idx] - if hasToLoad(value): - obj = load(value, self.files_stack) - if isinstance(obj, list): - l[idx : idx + 1] = obj - idx += len(obj) - else: - l[idx] = obj - idx += 1 - else: - self.expand(value) - idx += 1 - - # Recursively expand an object - def expand(self, obj: Union[dict, list]): if isinstance(obj, dict): - self.expand_dict(obj) - elif isinstance(obj, list): - self.expand_list(obj) + return self._expand_dict(obj) + if isinstance(obj, list): + return self._expand_list(obj) + if isinstance(obj, str): + return self._expand_string(obj) return obj - # Load a file + def _expand_string(self, value: str) -> Any: + """ + Expand resolver expressions and file references in a string. + + If the entire string is a resolver expression (for example + ``"${env:HOME}"`` or ``"${file:config.yaml}"``), the resolved value is + returned directly and may be of any type. + + Resolver expressions embedded inside a larger string are interpolated + into the surrounding text. Only scalar values may be interpolated; + attempting to embed a dictionary or list raises a ``PyAMLException``. + + After resolver expansion, plain strings that refer to supported + configuration files are loaded automatically. + + Args: + value: The string value to expand. + + Returns: + The expanded value, which may be a string or another object if the + input consists solely of a resolver expression. + """ + + full_match = RESOLVER_PATTERN.fullmatch(value) + if full_match: + return self._resolve_resolver_expression(full_match.group(1).strip()) + + # Handle embedded case + def replace(match: re.Match[str]) -> str: + """ + Replace one embedded resolver expression with its value. + + Parameters + ---------- + match : re.Match[str] + Match containing the resolver expression to expand. + + Returns + ------- + str + String representation of the resolved scalar value. + """ + resolved = self._resolve_resolver_expression(match.group(1).strip()) + + if isinstance(resolved, (dict, list)): + raise PyAMLException( + f"Resolver '{match.group(1)}' returned a {type(resolved).__name__}, " + "which cannot be interpolated into a string." + ) + + return str(resolved) + + value = RESOLVER_PATTERN.sub(replace, value) + + if _is_supported_file(value): + return RESOLVERS["file"](value, self.context) + + return value + + def _resolve_resolver_expression(self, expr: str) -> Any: + """ + Resolve a single resolver expression. + + The expression must have the form ``":"``, for + example ``"env:HOME"`` or ``"file:config.yaml"``. The resolver is + looked up in the global resolver registry and invoked with the + supplied payload. + + Args: + expr: Resolver expression without the surrounding ``"${...}"``. + + Returns: + The value returned by the matching resolver. + + Raises: + PyAMLException: If the expression is malformed or references an + unknown resolver. + """ + if ":" not in expr: + raise PyAMLException(f"Invalid resolver expression '{expr}'") + + prefix, payload = expr.split(":", 1) + resolver = RESOLVERS.get(prefix.strip()) + if resolver is None: + raise PyAMLException(f"Unknown resolver '{prefix.strip()}'") + + return resolver(payload.strip(), self.context) + + def _expand_dict(self, data: dict) -> dict: + """Recursively expand dictionary values and enrich cycle errors with location information.""" + + for key, value in list(data.items()): + try: + data[key] = self.expand(value) + except PyAMLConfigCyclingException as exc: + self._raise_cycle_error(exc, data, key) + return data + + def _raise_cycle_error(self, exc: PyAMLConfigCyclingException, obj: dict, key: Any) -> None: + """Re-raise a cycle error with file location information, if available.""" + + location = obj.get(LOCATION_KEY) + field_locations = obj.get(FIELD_LOCATIONS_KEY) + + location_str = "" + if location: + file, line, col = location + if field_locations and key in field_locations: + file, line, col = field_locations[key] + location_str = f" in {file} at line {line}, column {col}" + + raise PyAMLException(f"Circular file inclusion of {exc.error_filename}{location_str}") from exc + + def _expand_list(self, items: list) -> list: + """ + Recursively expand the elements of a list. + + Plain string values that refer to supported configuration files are + treated as list includes. If the referenced file loads to a list, its + elements are spliced into the current list. Otherwise, the loaded + object is appended as a single element. + + All other items are expanded recursively using :meth:`expand`. + + Args: + items: The list to expand. + + Returns: + The expanded list. + """ + expanded: list[Any] = [] + + for item in items: + if isinstance(item, str) and _is_supported_file(item): + loaded = RESOLVERS["file"](item, self.context) + if isinstance(loaded, list): + expanded.extend(loaded) + else: + expanded.append(loaded) + continue + + expanded.append(self.expand(item)) + + return expanded + + @abstractmethod + def load(self) -> Union[dict, list]: + """Load and parse the current configuration file.""" + ... + + +class YAMLLoader(ConfigLoader): + """ + Load and expand YAML configuration files. + + Parameters + ---------- + path : pathlib.Path + Configuration file being loaded. + context : LoadContext + Shared state for recursive includes and cycle detection. + + Methods + ------- + load() + Parse the YAML file and expand nested configuration references. + """ + + def __init__(self, path: Path, context: LoadContext): + """Create a YAML loader for the given file.""" + + super().__init__(path, context) + self._loader = SafeLineLoader if context.include_locations else CLoader + def load(self) -> Union[dict, list]: - raise PyAMLException(str(self.path) + ": load() method not implemented") + """Parse the YAML file and expand nested configuration references.""" + + logger.log(logging.DEBUG, f"Loading YAML file '{self.path}'") + with open(self.path) as file: + try: + return self.expand(yaml.load(file, Loader=self._loader)) + except yaml.YAMLError as exc: + raise PyAMLException(f"{self.path}: {exc}") from exc + + +class JSONLoader(ConfigLoader): + """ + Load and expand JSON configuration files. + + Parameters + ---------- + path : pathlib.Path + Configuration file being loaded. + context : LoadContext + Shared state for recursive includes and cycle detection. + + Methods + ------- + load() + Parse the JSON file and expand nested configuration references. + """ + + def __init__(self, path: Path, context: LoadContext): + """Create a JSON loader for the given file.""" + + super().__init__(path, context) + + def load(self) -> Union[dict, list]: + """Parse the JSON file and expand nested configuration references.""" + + logger.log(logging.DEBUG, f"Loading JSON file '{self.path}'") + with open(self.path) as file: + try: + return self.expand(json.load(file)) + except json.JSONDecodeError as exc: + raise PyAMLException(f"{self.path}: {exc}") from exc class SafeLineLoader(SafeLoader): + """ + YAML loader that preserves line and column information for mappings. + + Parameters + ---------- + stream : io.TextIOBase + Stream to parse. Its ``name`` is recorded so errors can cite the source file. + + Methods + ------- + construct_mapping(node, deep=False) + Build a mapping and attach location metadata to it. + """ + def __init__(self, stream): + """Create the YAML loader and record the source filename.""" + super().__init__(stream) self.filename = stream.name if isinstance(stream, io.TextIOWrapper) else "" def construct_mapping(self, node, deep=False): + """Build a mapping and attach location metadata to it.""" + mapping = {} field_mapping = {} for key_node, value_node in node.value: key = self.construct_object(key_node, deep=deep) - if not isinstance(key, collections.abc.Hashable): + if not isinstance(key, Hashable): raise ConstructorError( "while constructing a mapping", node.start_mark, "found unhashable key", key_node.start_mark, ) + value = self.construct_object(value_node, deep=deep) mapping[key] = value field_mapping[key] = ( @@ -172,41 +634,10 @@ def construct_mapping(self, node, deep=False): ) # Add location information inside the dict - mapping["__location__"] = ( + mapping[LOCATION_KEY] = ( self.filename, node.start_mark.line + 1, node.start_mark.column + 1, ) - mapping["__fieldlocations__"] = field_mapping + mapping[FIELD_LOCATIONS_KEY] = field_mapping return mapping - - -# YAML loader -class YAMLLoader(Loader): - def __init__(self, filename: str, parent_paths_stack: list, use_fast_loader: bool): - super().__init__(filename, parent_paths_stack) - self._loader = SafeLineLoader if not use_fast_loader else CLoader - self.use_fast_loader = use_fast_loader - - def load(self) -> Union[dict, list]: - logger.log(logging.DEBUG, f"Loading YAML file '{self.path}'") - with open(self.path) as file: - try: - return self.expand(yaml.load(file, Loader=self._loader)) - except yaml.YAMLError as e: - raise PyAMLException(str(self.path) + ": " + str(e)) from e - - -# JSON loader -class JSONLoader(Loader): - def __init__(self, filename: str, parent_paths_stack: list, use_fast_loader: bool): - super().__init__(filename, parent_paths_stack) - self.use_fast_loader = False - - def load(self) -> Union[dict, list]: - logger.log(logging.DEBUG, f"Loading JSON file '{self.path}'") - with open(self.path) as file: - try: - return self.expand(json.load(file)) - except json.JSONDecodeError as e: - raise PyAMLException(str(self.path) + ": " + str(e)) from e diff --git a/pyaml/configuration/inline_curve.py b/pyaml/configuration/inline_curve.py deleted file mode 100644 index a9de9f99b..000000000 --- a/pyaml/configuration/inline_curve.py +++ /dev/null @@ -1,55 +0,0 @@ -from pathlib import Path - -import numpy as np -from pydantic import BaseModel, ConfigDict - -from ..common.exception import PyAMLException -from ..configuration import get_root_folder -from .curve import Curve - -# Define the main class name for this module -PYAMLCLASS = "InlineCurve" - - -class ConfigModel(BaseModel): - """ - Configuration model for inline curve - - Parameters - ---------- - mat : list[list[float]] - Curve data (n rows, 2 columns) - """ - - model_config = ConfigDict(arbitrary_types_allowed=True, extra="forbid") - - mat: list[list[float]] - - -class InlineCurve(Curve): - """ - Class for load CSV (x,y) curve - """ - - def __init__(self, cfg: ConfigModel): - self._cfg = cfg - # Load the curve - self._curve = np.array(self._cfg.mat) - - _s = np.shape(self._curve) - if len(_s) != 2 or _s[1] != 2: - raise PyAMLException(f"InlineCurve(mat='{cfg.mat}',dtype=float): wrong shape (2,2) expected but got {str(_s)}") - - def get_curve(self) -> np.array: - """ - Get the curve data. - - Returns - ------- - np.array - Curve data as a 2D numpy array of shape (n, 2) - """ - return self._curve - - def __repr__(self): - return repr(self._cfg).replace("ConfigModel", self.__class__.__name__) diff --git a/pyaml/configuration/inline_matrix.py b/pyaml/configuration/inline_matrix.py deleted file mode 100644 index 25d03c78d..000000000 --- a/pyaml/configuration/inline_matrix.py +++ /dev/null @@ -1,47 +0,0 @@ -import numpy as np -from pydantic import BaseModel, ConfigDict - -from .matrix import Matrix - -# Define the main class name for this module -PYAMLCLASS = "InlineMatrix" - - -class ConfigModel(BaseModel): - """ - Configuration model for inline matrix - - Parameters - ---------- - mat : list[list[float]] - The matrix - """ - - model_config = ConfigDict(arbitrary_types_allowed=True, extra="forbid") - - mat: list[list[float]] - - -class InlineMatrix(Matrix): - """ - Class for loading CSV matrix - """ - - def __init__(self, cfg: ConfigModel): - self._cfg = cfg - # Load the matrix - self._mat = np.array(self._cfg.mat) - - def get_matrix(self) -> np.array: - """ - Get the matrix data. - - Returns - ------- - np.array - Matrix data as a numpy array - """ - return self._mat - - def __repr__(self): - return repr(self._cfg).replace("ConfigModel", self.__class__.__name__) diff --git a/pyaml/configuration/manager.py b/pyaml/configuration/manager.py index 1d4511133..68baf41c3 100644 --- a/pyaml/configuration/manager.py +++ b/pyaml/configuration/manager.py @@ -1,10 +1,9 @@ """ -manager.py +Aggregate accelerator configuration fragments before runtime construction. -Configuration aggregation helpers for :class:`~pyaml.accelerator.Accelerator`. - -This module provides :class:`ConfigurationManager`, a lightweight service used -to collect configuration fragments before runtime objects are built. +The manager loads dictionaries and YAML/JSON files, merges named categories, +tracks source information, and provides the final configuration to the +accelerator factory. Typical usage is: @@ -15,13 +14,15 @@ import copy import fnmatch +import inspect import os import re +from importlib import import_module from pathlib import Path from typing import Any from ..common.exception import PyAMLConfigException -from .fileloader import get_root_folder, load, set_root_folder +from .fileloader import ROOT, load from .restfetcher import REMOTE_BASE_URL_KEY, SourceRoot, fetch_remote_config, is_remote_url, resolve_reference _INTERNAL_METADATA_KEYS = {"__location__", "__fieldlocations__", REMOTE_BASE_URL_KEY} @@ -35,7 +36,7 @@ class UnsupportedConfigurationRootError(PyAMLConfigException): - """Raised when a fragment root is outside ConfigurationManager scope.""" + """Raised when a fragment contains unsupported root-level fields.""" class ConfigurationManager: @@ -46,6 +47,40 @@ class ConfigurationManager: dictionaries and exposes convenience helpers to inspect, query and update them before constructing the final runtime object graph. + Methods + ------- + root_fields() + Return the supported accelerator root fields in order. Return the ordered root fields supported by the + accelerator configuration. + add(payload, **kwargs) + Add a configuration fragment from a dict or a YAML/JSON file. + remove(category, name) + Remove a named entry from an aggregated category. + replace(category, element) + Replace an existing named entry in an aggregated category. + clear(category=None) + Clear the aggregated state, or a single root field/category. + categories() + Return categories that currently contain entries. + keys(category=None) + Return known entry names. + has(category, name) + Check whether a named entry exists. + get(category, name) + Return a named configuration entry. + find(pattern, category=None) + Search entry names using wildcards or regular expressions. + settings() + Return aggregated scalar accelerator settings. + to_dict() + Return the aggregated configuration as a plain dictionary. + build(ignore_external=False, validate=False) + Build an Accelerator from the aggregated configuration snapshot. + strip_internal_metadata(value) + Remove additionnal internal informations info from value + strip_runtime_internal_metadata(value) + Remove additionnal internal informations info from value + Notes ----- The manager only accepts accelerator-root fragments and merges named @@ -74,6 +109,9 @@ class ConfigurationManager: 'design' """ + DEFAULT_CLASS_PATH = "pyaml.accelerator.Accelerator" + # Kept as a public compatibility constant for callers using the legacy + # module-based manager API. DEFAULT_TYPE = "pyaml.accelerator" NAMED_CATEGORIES = ("controls", "simulators", "arrays", "devices") _SUPPORTED_FILE_SUFFIXES = {".yaml", ".yml", ".json"} @@ -81,35 +119,50 @@ class ConfigurationManager: @classmethod def root_fields(cls) -> tuple[str, ...]: r""" - Return the ordered root fields supported by the accelerator model. + Return the supported accelerator root fields in order. + Return the ordered root fields supported by the accelerator configuration. - The field order is derived from - :class:`~pyaml.accelerator.ConfigModel`. + The field order is derived from :meth:`Accelerator.__init__`, excluding + internal or categorized fields such as control and simulator collections. Returns ------- tuple[str, ...] + Root field names in configuration order, prefixed with ``"type"``. Examples - -------- .. code-block:: python - >>> ConfigurationManager.root_fields() + >>> ConfigurationManager.root_fields() """ - from ..accelerator import ConfigModel as AcceleratorConfigModel - - config_fields = tuple( - field_name for field_name in AcceleratorConfigModel.model_fields if field_name not in cls.NAMED_CATEGORIES + params = inspect.signature(cls.__init__).parameters + + fields = tuple( + name + for name, param in params.items() + if name != "self" + and name not in cls.NAMED_CATEGORIES + and param.kind + in ( + inspect.Parameter.POSITIONAL_OR_KEYWORD, + inspect.Parameter.KEYWORD_ONLY, + ) ) - return ("type", *config_fields) + return ("class_path", *fields) def __init__(self): - self._state: dict[str, Any] = {"type": self.DEFAULT_TYPE} + """ + Initialize an empty configuration manager. + + The manager starts with the default accelerator type and empty named + categories. Source tracking is enabled as fragments are added. + """ + self._state: dict[str, Any] = {"class_path": self.DEFAULT_CLASS_PATH} self._items_by_category: dict[str, dict[str, dict[str, Any]]] = {category: {} for category in self.NAMED_CATEGORIES} self._sources_by_category: dict[str, dict[str, str]] = {category: {} for category in self.NAMED_CATEGORIES} self._field_sources: dict[str, str] = {} - self._build_root: SourceRoot = get_root_folder() + self._build_root: SourceRoot = ROOT.get() self._build_root_locked = False def add(self, payload, **kwargs) -> None: @@ -122,7 +175,7 @@ def add(self, payload, **kwargs) -> None: Fragment to merge into the current aggregated state. source_name : str, optional Explicit source label to associate with the fragment. - use_fast_loader : bool, optional + include_locations : bool, optional Forwarded to the configuration loader. Examples @@ -145,7 +198,7 @@ def add(self, payload, **kwargs) -> None: ... ) """ source_name = kwargs.pop("source_name", None) - use_fast_loader = kwargs.pop("use_fast_loader", False) + include_locations = kwargs.pop("include_locations", False) if kwargs: unknown = ", ".join(sorted(kwargs)) raise PyAMLConfigException(f"Unsupported ConfigurationManager.add() arguments: {unknown}") @@ -153,7 +206,7 @@ def add(self, payload, **kwargs) -> None: fragment, inferred_source_name, source_root = self._load_payload( payload, source_name=source_name, - use_fast_loader=use_fast_loader, + include_locations=include_locations, ) prepared = self._prepare_fragment(fragment, source_root, inferred_source_name) self._merge_fragment(prepared, inferred_source_name) @@ -253,12 +306,12 @@ def clear(self, category: str | None = None) -> None: >>> manager.clear() """ if category is None: - self._state = {"type": self.DEFAULT_TYPE} + self._state = {"class_path": self.DEFAULT_CLASS_PATH} self._field_sources.clear() for name in self.NAMED_CATEGORIES: self._items_by_category[name].clear() self._sources_by_category[name].clear() - self._build_root = get_root_folder() + self._build_root = ROOT.get() self._build_root_locked = False return @@ -268,9 +321,9 @@ def clear(self, category: str | None = None) -> None: self._sources_by_category[category].clear() return - if category == "type": - self._state["type"] = self.DEFAULT_TYPE - self._field_sources.pop("type", None) + if category in ("type", "class_path"): + self._state["class_path"] = self.DEFAULT_CLASS_PATH + self._field_sources.pop("class_path", None) return if category in self._state: @@ -468,7 +521,7 @@ def to_dict(self) -> dict[str, Any]: snapshot = self._snapshot(include_internal_metadata=False) return snapshot - def build(self, ignore_external: bool = False): + def build(self, ignore_external: bool = False, validate: bool = False): r""" Build an Accelerator from the aggregated configuration snapshot. @@ -491,9 +544,9 @@ def build(self, ignore_external: bool = False): from ..accelerator import Accelerator if isinstance(self._build_root, Path): - set_root_folder(self._build_root) + ROOT.set(self._build_root) snapshot = ConfigurationManager.strip_runtime_internal_metadata(self._snapshot(include_internal_metadata=True)) - return Accelerator.from_dict(snapshot, ignore_external=ignore_external) + return Accelerator.from_dict(snapshot, ignore_external=ignore_external, validate=validate) def __dir__(self): """ @@ -599,14 +652,31 @@ def _load_payload( payload, *, source_name: str | None, - use_fast_loader: bool, + include_locations: bool, ) -> tuple[dict[str, Any], str, SourceRoot]: + """ + Load a dictionary or file payload and determine its source metadata. + + Parameters + ---------- + payload : object + Configuration dictionary or path to a YAML/JSON file. + source_name : str | None + Optional explicit source label. + include_locations : bool + Whether to preserve source locations while loading. + + Returns + ------- + tuple[dict[str, Any], str, SourceRoot] + Loaded fragment, source label, and source root directory. + """ if isinstance(payload, dict): return copy.deepcopy(payload), source_name or "", None payload_path = self._coerce_path(payload) if is_remote_url(payload_path): - fragment, source_root = fetch_remote_config(payload_path, use_fast_loader=use_fast_loader) + fragment, source_root = fetch_remote_config(payload_path, include_locations=include_locations) if not self._build_root_locked: self._build_root = source_root self._build_root_locked = True @@ -624,13 +694,13 @@ def _load_payload( raise PyAMLConfigException(f"{payload_path} file not found") resolved_path = path.resolve() - previous_root = get_root_folder() + previous_root = ROOT.get() source_root = resolved_path.parent try: - set_root_folder(source_root) - fragment = load(resolved_path.name, None, use_fast_loader) + ROOT.set(source_root) + fragment = load(resolved_path.name, include_locations) finally: - set_root_folder(previous_root) + ROOT.set(previous_root) if not self._build_root_locked: self._build_root = source_root @@ -639,19 +709,38 @@ def _load_payload( return fragment, source_name or str(resolved_path), source_root def _prepare_fragment(self, fragment: dict[str, Any], source_root: SourceRoot, source_name: str) -> dict[str, Any]: + """ + Validate and normalize a loaded configuration fragment. + + Parameters + ---------- + fragment : dict[str, Any] + Fragment to prepare. + source_root : SourceRoot + Root directory used to resolve relative simulator paths. + source_name : str + Label identifying the fragment source. + + Returns + ------- + dict[str, Any] + Normalized fragment ready to merge. + """ if not isinstance(fragment, dict): raise PyAMLConfigException( f"ConfigurationManager.add() expects a mapping at the top level, got '{type(fragment).__name__}'." ) - accelerator_type = fragment.get("type", self.DEFAULT_TYPE) - if accelerator_type != self.DEFAULT_TYPE: + prepared = self._normalize_class_paths(fragment) + + accelerator_class_path = prepared.get("class_path", self.DEFAULT_CLASS_PATH) + if accelerator_class_path != self.DEFAULT_CLASS_PATH: raise UnsupportedConfigurationRootError( - f"ConfigurationManager only supports '{self.DEFAULT_TYPE}' roots, got '{accelerator_type}'." + f"ConfigurationManager only supports '{self.DEFAULT_CLASS_PATH}' roots, got '{accelerator_class_path}'." ) - prepared = copy.deepcopy(fragment) - prepared["type"] = self.DEFAULT_TYPE + prepared = copy.deepcopy(prepared) + prepared["class_path"] = self.DEFAULT_CLASS_PATH for category in self.NAMED_CATEGORIES: if category not in prepared: @@ -672,9 +761,9 @@ def _prepare_fragment(self, fragment: dict[str, Any], source_root: SourceRoot, s f"Configuration category '{category}' expects named objects, " f"but entry at index {index} from source '{source_name}' has no 'name'." ) - if "type" not in entry: + if "class_path" not in entry: raise PyAMLConfigException( - f"Configuration entry '{entry['name']}' in category '{category}' has no 'type'." + f"Configuration entry '{entry['name']}' in category '{category}' has no 'class_path'." ) if category == "simulators": @@ -682,7 +771,64 @@ def _prepare_fragment(self, fragment: dict[str, Any], source_root: SourceRoot, s return prepared + @classmethod + def _normalize_class_paths(cls, value: Any) -> Any: + """Normalize legacy and new configuration references to ``class_path``. + + Legacy ``type`` entries are resolved using the module's ``PYAMLCLASS`` + value. The modern ``class`` alias is accepted as a fully qualified + class path. The manager then uses only ``class_path`` internally. + """ + if isinstance(value, list): + return [cls._normalize_class_paths(item) for item in value] + if not isinstance(value, dict): + return value + + normalized = { + key: item if key in _INTERNAL_METADATA_KEYS else cls._normalize_class_paths(item) for key, item in value.items() + } + class_path = normalized.pop("class_path", None) + legacy_type = normalized.pop("type", None) + class_alias = normalized.pop("class", None) + if class_path is None and legacy_type is None: + if class_alias is not None: + # ``class`` is also supported as an alias for ``class_path``. + class_path = class_alias + class_alias = None + else: + return normalized + if class_path is not None and (legacy_type is not None or class_alias is not None): + raise PyAMLConfigException("Configuration cannot combine class_path with type or class.") + if class_path is None: + if not isinstance(legacy_type, str): + raise PyAMLConfigException(f"Invalid type '{legacy_type}'.") + if class_alias is None: + module = import_module(legacy_type) + class_alias = getattr(module, "PYAMLCLASS", None) + if class_alias is None: + raise PyAMLConfigException(f"Module '{legacy_type}' does not define PYAMLCLASS.") + class_path = f"{legacy_type}.{class_alias}" + if not isinstance(class_path, str) or "." not in class_path: + raise PyAMLConfigException(f"Invalid class_path '{class_path}'. Expected 'module.Class'.") + normalized["class_path"] = class_path + return normalized + def _merge_fragment(self, fragment: dict[str, Any], source_name: str) -> None: + """ + Merge a prepared fragment into the aggregated configuration. + + Parameters + ---------- + fragment : dict[str, Any] + Normalized fragment to merge. + source_name : str + Source label associated with the fragment. + + Returns + ------- + None + This method returns ``None`` and updates manager state in place. + """ duplicate_errors: list[str] = [] pending_by_category: dict[str, list[dict[str, Any]]] = {} @@ -735,12 +881,40 @@ def _merge_fragment(self, fragment: dict[str, Any], source_name: str) -> None: self._sources_by_category[category][copied["name"]] = source_name def _snapshot(self, *, include_internal_metadata: bool) -> dict[str, Any]: + """ + Return a deep copy of the current aggregated configuration. + + Parameters + ---------- + include_internal_metadata : bool + No arguments are required. + + Returns + ------- + dict[str, Any] + Independent configuration dictionary. + """ snapshot = copy.deepcopy(self._state) if include_internal_metadata: return snapshot return ConfigurationManager.strip_internal_metadata(snapshot) def _normalize_simulator_paths(self, entry: dict[str, Any], source_root: SourceRoot) -> None: + """ + Normalize simulator paths relative to their source configuration. + + Parameters + ---------- + entry : dict[str, Any] + Simulator configuration entry to normalize. + source_root : SourceRoot + Source root used for relative paths. + + Returns + ------- + None + Updated simulator entry. + """ if source_root is None: return @@ -749,12 +923,38 @@ def _normalize_simulator_paths(self, entry: dict[str, Any], source_root: SourceR entry["lattice"] = resolve_reference(lattice, source_root) def _require_named_category(self, category: str) -> None: + """ + Validate that a category supports named entries. + + Parameters + ---------- + category : str + Category name to validate. + + Returns + ------- + None + This method returns ``None`` when the category is valid. + """ if category not in self.NAMED_CATEGORIES: raise PyAMLConfigException( f"Unknown configuration category '{category}'. Expected one of: {', '.join(self.NAMED_CATEGORIES)}." ) def _categories_for_name(self, name: str) -> list[str]: + """ + Find categories containing an entry with the given name. + + Parameters + ---------- + name : str + Entry name to search for. + + Returns + ------- + list[str] + Matching category names. + """ categories: list[str] = [] for category in self.NAMED_CATEGORIES: if name in self._items_by_category[category]: @@ -762,9 +962,24 @@ def _categories_for_name(self, name: str) -> list[str]: return categories def _format_entry(self, category: str, entry: dict[str, Any]) -> str: + """ + Format an entry for a user-facing configuration summary. + + Parameters + ---------- + category : str + Category containing the entry. + entry : dict[str, Any] + Entry to format. + + Returns + ------- + str + Formatted entry description. + """ name = entry.get("name", "") - entry_type = entry.get("type") - type_part = f" ({entry_type})" if entry_type else "" + entry_class_path = entry.get("class_path") + type_part = f" ({entry_class_path})" if entry_class_path else "" details: list[str] = [] if category == "arrays": @@ -783,6 +998,19 @@ def _format_entry(self, category: str, entry: dict[str, Any]) -> str: return f" {name}{type_part}{detail_part}" def _format_source(self, source: str) -> str: + """ + Format a source label for display. + + Parameters + ---------- + source : str + Source path or label. + + Returns + ------- + str + Human-readable source description. + """ if source.startswith("<") and source.endswith(">"): return source source_path = Path(source) @@ -792,6 +1020,21 @@ def _format_source(self, source: str) -> str: return source def _describe_entry_source(self, entry: dict[str, Any], fallback_source: str) -> str: + """ + Describe where a named configuration entry originated. + + Parameters + ---------- + entry : dict[str, Any] + Category containing the entry. + fallback_source : str + Entry name to describe. + + Returns + ------- + str + Source description, or ``None`` if unavailable. + """ location = entry.get("__location__") if isinstance(location, tuple) and len(location) == 3: source, line, column = location @@ -799,11 +1042,39 @@ def _describe_entry_source(self, entry: dict[str, Any], fallback_source: str) -> return f"source '{fallback_source}'" def _coerce_path(self, payload) -> str: + """ + Convert a path-like value to an absolute configuration path. + + Parameters + ---------- + payload : object + Path value to convert. + + Returns + ------- + str + Resolved path. + """ if isinstance(payload, (str, os.PathLike)): return os.fspath(payload) raise PyAMLConfigException(f"Cannot infer configuration source from payload of type '{type(payload).__name__}'.") def _extend_unique(self, target: list[str], values) -> None: + """ + Append values that are not already present. + + Parameters + ---------- + target : list[str] + Destination sequence. + values : object + Values to append while preserving order. + + Returns + ------- + None + This method updates the destination sequence in place. + """ for value in values: if value not in target: target.append(value) diff --git a/pyaml/configuration/restfetcher.py b/pyaml/configuration/restfetcher.py index ea80b58e7..96a754502 100644 --- a/pyaml/configuration/restfetcher.py +++ b/pyaml/configuration/restfetcher.py @@ -1,5 +1,8 @@ """ -HTTP configuration fetch helpers. +Fetch and expand configuration documents from HTTP(S) sources. + +The helpers in this module download YAML or JSON documents, resolve relative +remote includes, expand path references, and detect circular inclusions. """ import io @@ -15,30 +18,89 @@ from yaml import CLoader from ..common.exception import PyAMLConfigException -from .fileloader import FILE_PREFIX, SafeLineLoader, accepted_suffixes +from .fileloader import ACCEPTED_SUFFIXES, SafeLineLoader REMOTE_BASE_URL_KEY = "__baseurl__" SourceRoot = Path | str | None _REMOTE_SCHEMES = {"http", "https"} +FILE_PREFIX = "${path:" + class _NamedStringIO(io.StringIO): + """ + In-memory text stream that preserves a source name for YAML errors. + + Parameters + ---------- + value : str + Text content exposed by the stream. + name : str + Source name retained for parser diagnostics. + """ + def __init__(self, value: str, name: str): + """ + Initialize the _NamedStringIO. + """ super().__init__(value) self.name = name def is_remote_url(value: str) -> bool: + """ + Return whether a string uses the HTTP or HTTPS URL scheme. + + Parameters + ---------- + value : str + Value to inspect. + + Returns + ------- + bool + ``True`` for HTTP(S) URLs; otherwise ``False``. + """ return urlparse(value).scheme in _REMOTE_SCHEMES -def fetch_remote_config(url: str, *, use_fast_loader: bool = False) -> tuple[dict[str, Any] | list[Any], str]: +def fetch_remote_config(url: str, *, include_locations: bool = True) -> tuple[dict[str, Any] | list[Any], str]: + """ + Fetch, parse, and expand a remote configuration document. + + Parameters + ---------- + url : str + HTTP(S) URL of the YAML or JSON document. + include_locations : bool + Preserve source locations in YAML mappings when ``True``. + + Returns + ------- + tuple[dict[str, Any] | list[Any], str] + Expanded document and its base URL for resolving relative includes. + """ normalized_url = _normalize_remote_url(url) - expanded = _load_remote_document(normalized_url, use_fast_loader=use_fast_loader, stack=[]) + expanded = _load_remote_document(normalized_url, include_locations=include_locations, stack=[]) return expanded, _remote_base_url(normalized_url) def resolve_reference(reference: str, source_root: SourceRoot) -> str: + """ + Resolve a local or remote configuration reference. + + Parameters + ---------- + reference : str + Path or URL reference to resolve. + source_root : SourceRoot + Local directory or remote base URL used for relative references. + + Returns + ------- + str + Absolute local path, resolved remote URL, or unchanged reference. + """ if is_remote_url(reference) or os.path.isabs(reference): return reference @@ -52,6 +114,19 @@ def resolve_reference(reference: str, source_root: SourceRoot) -> str: def _normalize_remote_url(url: str) -> str: + """ + Validate that a configuration source is an HTTP(S) URL. + + Parameters + ---------- + url : str + URL to validate. + + Returns + ------- + str + The validated URL. + """ parsed = urlparse(url) if parsed.scheme not in _REMOTE_SCHEMES: raise PyAMLConfigException(f"Unsupported remote configuration source '{url}'.") @@ -61,18 +136,48 @@ def _normalize_remote_url(url: str) -> str: def _load_remote_document( url: str, *, - use_fast_loader: bool, + include_locations: bool, stack: list[str], ) -> dict[str, Any] | list[Any]: + """ + Download, parse, and recursively expand one remote document. + + Parameters + ---------- + url : str + URL of the document to load. + include_locations : bool + Preserve YAML source locations when ``True``. + stack : list[str] + URLs currently being loaded, used for cycle detection. + + Returns + ------- + dict[str, Any] | list[Any] + Parsed and recursively expanded document. + """ if url in stack: raise PyAMLConfigException(f"Circular remote configuration inclusion detected for '{url}'.") payload, content_type = _download_text(url) - document = _parse_remote_document(url, payload, content_type, use_fast_loader=use_fast_loader) - return _expand_remote_value(document, _remote_base_url(url), stack + [url], use_fast_loader=use_fast_loader) + document = _parse_remote_document(url, payload, content_type, include_locations=include_locations) + return _expand_remote_value(document, _remote_base_url(url), stack + [url], include_locations=include_locations) def _download_text(url: str) -> tuple[str, str]: + """ + Download a remote document and return its text and media type. + + Parameters + ---------- + url : str + HTTP(S) URL to request. + + Returns + ------- + tuple[str, str] + Document text and response content type. + """ opener = build_opener(ProxyHandler({})) try: with opener.open(url, timeout=10) as response: @@ -93,8 +198,27 @@ def _parse_remote_document( payload: str, content_type: str, *, - use_fast_loader: bool, + include_locations: bool, ) -> dict[str, Any] | list[Any]: + """ + Parse downloaded JSON or YAML text into Python objects. + + Parameters + ---------- + url : str + Source URL, used for format detection and error messages. + payload : str + Downloaded document text. + content_type : str + HTTP response media type. + include_locations : bool + Preserve source locations in YAML mappings when ``True``. + + Returns + ------- + dict[str, Any] | list[Any] + Parsed mapping or sequence. + """ suffix = Path(urlparse(url).path).suffix.lower() if content_type == "application/json" or suffix == ".json": @@ -103,7 +227,7 @@ def _parse_remote_document( except json.JSONDecodeError as ex: raise PyAMLConfigException(f"{url}: {ex}") from ex - loader = CLoader if use_fast_loader else SafeLineLoader + loader = CLoader if not include_locations else SafeLineLoader try: stream = _NamedStringIO(payload, url) return yaml.load(stream, Loader=loader) @@ -111,11 +235,25 @@ def _parse_remote_document( raise PyAMLConfigException(f"{url}: {ex}") from ex -def _expand_remote_value(value, base_url: str, stack: list[str], *, use_fast_loader: bool): +def _expand_remote_value(value, base_url: str, stack: list[str], *, include_locations: bool): + """ + Recursively expand references in a remote configuration value. + + Parameters + ---------- + value : object + Value to expand. + base_url : str + Base URL for relative references. + stack : list[str] + Active remote include chain. + include_locations : bool + Preserve YAML source locations when ``True``. + """ if isinstance(value, dict): - return _expand_remote_dict(value, base_url, stack, use_fast_loader=use_fast_loader) + return _expand_remote_dict(value, base_url, stack, include_locations=include_locations) if isinstance(value, list): - return _expand_remote_list(value, base_url, stack, use_fast_loader=use_fast_loader) + return _expand_remote_list(value, base_url, stack, include_locations=include_locations) return value @@ -124,14 +262,33 @@ def _expand_remote_dict( base_url: str, stack: list[str], *, - use_fast_loader: bool, + include_locations: bool, ) -> dict[str, Any]: + """ + Expand file and document references within a remote mapping. + + Parameters + ---------- + values : dict[str, Any] + Mapping whose values should be expanded in place. + base_url : str + Base URL for relative references. + stack : list[str] + Active remote include chain. + include_locations : bool + Preserve YAML source locations when ``True``. + + Returns + ------- + dict[str, Any] + The expanded mapping. + """ values.setdefault(REMOTE_BASE_URL_KEY, base_url) for key, value in list(values.items()): if _is_config_reference(value): values[key] = _load_remote_document( _resolve_remote_config_reference(value, base_url), - use_fast_loader=use_fast_loader, + include_locations=include_locations, stack=stack, ) continue @@ -140,18 +297,37 @@ def _expand_remote_dict( values[key] = resolve_reference(value[len(FILE_PREFIX) :], base_url) continue - values[key] = _expand_remote_value(value, base_url, stack, use_fast_loader=use_fast_loader) + values[key] = _expand_remote_value(value, base_url, stack, include_locations=include_locations) return values -def _expand_remote_list(values: list[Any], base_url: str, stack: list[str], *, use_fast_loader: bool) -> list[Any]: +def _expand_remote_list(values: list[Any], base_url: str, stack: list[str], *, include_locations: bool) -> list[Any]: + """ + Expand file and document references within a remote list. + + Parameters + ---------- + values : list[Any] + List whose elements should be expanded in place. + base_url : str + Base URL for relative references. + stack : list[str] + Active remote include chain. + include_locations : bool + Preserve YAML source locations when ``True``. + + Returns + ------- + list[Any] + The expanded list. + """ index = 0 while index < len(values): value = values[index] if _is_config_reference(value): expanded = _load_remote_document( _resolve_remote_config_reference(value, base_url), - use_fast_loader=use_fast_loader, + include_locations=include_locations, stack=stack, ) if isinstance(expanded, list): @@ -167,12 +343,25 @@ def _expand_remote_list(values: list[Any], base_url: str, stack: list[str], *, u index += 1 continue - values[index] = _expand_remote_value(value, base_url, stack, use_fast_loader=use_fast_loader) + values[index] = _expand_remote_value(value, base_url, stack, include_locations=include_locations) index += 1 return values def _is_config_reference(value: Any) -> bool: + """ + Return whether a value names a supported configuration document. + + Parameters + ---------- + value : Any + Value to inspect. + + Returns + ------- + bool + ``True`` for a YAML, JSON, or supported remote document reference. + """ if not isinstance(value, str): return False @@ -181,14 +370,42 @@ def _is_config_reference(value: Any) -> bool: parsed = urlparse(value) path = parsed.path if parsed.scheme in _REMOTE_SCHEMES else value - return any(path.endswith(suffix) for suffix in accepted_suffixes) + return any(path.endswith(suffix) for suffix in ACCEPTED_SUFFIXES) def _resolve_remote_config_reference(reference: str, base_url: str) -> str: + """ + Resolve a remote include against its containing document URL. + + Parameters + ---------- + reference : str + Relative or absolute document reference. + base_url : str + Base URL of the containing document. + + Returns + ------- + str + Absolute URL of the referenced document. + """ if is_remote_url(reference): return reference return urljoin(base_url, reference) def _remote_base_url(url: str) -> str: + """ + Return the directory-like base URL for a remote document. + + Parameters + ---------- + url : str + Remote document URL. + + Returns + ------- + str + Base URL used to resolve relative references. + """ return urljoin(url, ".") diff --git a/pyaml/configuration/unbound_element.py b/pyaml/configuration/unbound_element.py index 244d74ae4..1e1c58d9a 100644 --- a/pyaml/configuration/unbound_element.py +++ b/pyaml/configuration/unbound_element.py @@ -1,26 +1,46 @@ +""" +Deferred construction of control-system-specific elements. + +An :class:`UnboundElement` stores a class, validated configuration, and the +control modes in which it is available until an :class:`ElementHolder` is +known and the concrete element can be instantiated. +""" + +from typing import TYPE_CHECKING + from pydantic import BaseModel from ..common.element import Element +from ..common.exception import PyAMLConfigException + +if TYPE_CHECKING: + from ..common.holders.element_holder import ElementHolder class UnboundElement(Element): """ - Class that holds a configuration for an element created on the fly when ElementHolder is filled + Store configuration for an element instantiated when a holder is filled. + + Parameters + ---------- + element_class : type + Concrete element class to instantiate. + module_name : str + Module path used to identify the element in error messages. + modes : list of str + Control-system modes in which the element should be created. + config : pydantic.BaseModel + Validated configuration passed to the element constructor. + + Methods + ------- + instantiate(holder) + Instantiate the element represented by this UnboundElement. """ def __init__(self, element_class, module_name: str, modes: list[str], config: BaseModel): """ - Construct an External element - Parameters - ---------- - element_class : class - Element class - module_name : str - Element module - control_modes: list[str] - List of control modes to add the element to - config: BaseModel - Element configuration + Initialize a deferred element configuration. """ super().__init__(config.name) self._class = element_class @@ -29,9 +49,53 @@ def __init__(self, element_class, module_name: str, modes: list[str], config: Ba self._config = config def __repr__(self): + """ + Implement the ``__repr__`` string. + """ return "%s(name='%s', class_name='%s', module_name=%s)" % ( self.__class__.__name__, self.get_name(), self._class.__name__, self._module_name, ) + + def _fill_device(self, holder: "ElementHolder") -> None: + holder._fill_unbound_element(self) + + def instantiate(self, holder) -> Element: + """ + Instantiate the element represented by this UnboundElement. + + The element is constructed using the stored configuration and + attached to the given ElementHolder. The returned element is + linked back to the holder through its ``_peer`` attribute. + + Parameters + ---------- + holder : ElementHolder + Holder that owns the instantiated element. + + Returns + ------- + Element + Instantiated element attached to the given holder. + + Raises + ------ + PyAMLConfigException + If the element cannot be instantiated or if the resulting + object is not a subclass of Element. + """ + + cls = self._class + + try: + obj = cls(holder, self._config) + except Exception as exc: + raise PyAMLConfigException(f"{exc} when creating '{self._module_name}.{cls.__name__}'") from exc + + if not isinstance(obj, Element): + raise PyAMLConfigException(f"'{self._module_name}.{cls.__name__}' is not a subclass of Element") + + obj._peer = holder + return obj diff --git a/pyaml/control/abstract_impl.py b/pyaml/control/abstract_impl.py index 95a280847..077a819dd 100644 --- a/pyaml/control/abstract_impl.py +++ b/pyaml/control/abstract_impl.py @@ -1,3 +1,11 @@ +""" +Control-system implementations of PyAML read/write interfaces. + +The classes in this module adapt control-system devices to PyAML scalar and +array interfaces, including conversions between hardware values, magnet +strengths, BPM readings, and RF quantities. +""" + from typing import Any import numpy as np @@ -5,7 +13,6 @@ from numpy.typing import NDArray from .. import PyAMLException -from ..bpm.bpm_model import BPMModel from ..common import abstract from ..common.abstract_aggregator import ScalarAggregator from ..control.deviceaccess import DeviceAccess @@ -80,7 +87,19 @@ def check_range(values: Any, dev_range: Any) -> bool: def _as_1d_float_array(values: Any) -> np.ndarray: - """Normalize input values to a 1D float NumPy array.""" + """ + Convert scalar or array-like values to a one-dimensional float array. + + Parameters + ---------- + values : object + Scalar or array-like values to normalize. + + Returns + ------- + numpy.ndarray + One-dimensional array with ``float`` dtype. + """ v = np.asarray(values, dtype=float) if v.ndim == 0: return v.reshape(1) @@ -89,28 +108,38 @@ def _as_1d_float_array(values: Any) -> np.ndarray: def _iter_devices_and_ranges(devs: DeviceAccess | DeviceAccessList): """ - Yield tuples (device, [min, max]) for each underlying device. + Return each device together with its inclusive hardware range. Works for: - DeviceAccess: yields 1 item - DeviceAccessList: yields N items based on get_devices() and get_range() flattening + + Parameters + ---------- + devs : DeviceAccess or DeviceAccessList + Device or device collection whose ranges should be inspected. + + Returns + ------- + list of tuple + Pairs containing a device and its ``[minimum, maximum]`` range. """ # Single device - if hasattr(devs, "get") and hasattr(devs, "get_range") and not hasattr(devs, "get_devices"): + if isinstance(devs, DeviceAccess): r = devs.get_range() if r is None: r = [None, None] return [(devs, [r[0], r[1]])] - # Device list (expects get_devices() + get_range() flat list) - devices = devs.get_devices() - flat = np.asarray(devs.get_range(), dtype=object).ravel() - if (flat.size % 2) != 0: + # get_range() return a flat list + flat = devs.get_range() + if (len(flat) % 2) != 0: raise ValueError(f"dev_range must have an even length, got {flat.size}") + # Reshape pairs = [] - for i, d in enumerate(devices): - pairs.append((d, [flat[2 * i], flat[2 * i + 1]])) + for i, dev in enumerate(devs): + pairs.append((dev, [flat[2 * i], flat[2 * i + 1]])) return pairs @@ -172,32 +201,94 @@ def format_out_of_range_message( class CSScalarAggregator(ScalarAggregator): """ - Basic control system aggregator for a list of scalar values + Aggregate scalar control-system devices into one PyAML interface. + + Parameters + ---------- + devs : DeviceAccessList + Devices managed by the aggregator. + + Methods + ------- + add_devices(devices) + Add one or more devices to the scalar aggregator. + set(value) + Write scalar values to the managed control-system devices. + set_and_wait(value) + Set values and wait for readback confirmation. + get() + Read the current values from all managed devices. + readback() + Read the last available values from all managed devices. + unit() + Return the unit reported by the managed devices. + nb_device() + Return the number of managed devices. """ def __init__(self, devs: DeviceAccessList): + """ + Initialize the CSScalarAggregator. + """ self._devs = devs def add_devices(self, devices: DeviceAccess | list[DeviceAccess]): + """ + Add one or more devices to the scalar aggregator. + + Parameters + ---------- + devices : DeviceAccess | list[DeviceAccess] + Control-system device or devices to manage. + """ self._devs.add_devices(devices) def set(self, value: NDArray[np.float64]): + """ + Write scalar values to the managed control-system devices. + + Parameters + ---------- + value : NDArray[np.float64] + Values to write, in the same order as the managed devices. + """ self._devs.set(value) def set_and_wait(self, value: NDArray[np.float64]): + """ + Set values and wait for readback confirmation. + + This control-system implementation does not currently support + waiting for device readback and raises :class:`NotImplementedError`. + + Parameters + ---------- + value : NDArray[np.float64] + Values that would be written to the managed devices. + + Raises + ------ + NotImplementedError + Always raised because asynchronous setpoint confirmation is not + implemented. + """ self._devs.set_and_wait(value) def get(self) -> NDArray[np.float64]: + """Read the current values from all managed devices.""" return self._devs.get() def readback(self) -> np.array: + """Read the last available values from all managed devices.""" return self._devs.readback() def unit(self) -> str: + """Return the unit reported by the managed devices.""" return self._devs.unit() def nb_device(self) -> int: - return self._devs.__len__() + """Return the number of managed devices.""" + return self._devs.len() # ------------------------------------------------------------------------------ @@ -205,14 +296,37 @@ def nb_device(self) -> int: class CSStrengthScalarAggregator(CSScalarAggregator): """ - Control system aggregator for a list of magnet strengths. - This aggregator is in charge of computing hardware setpoints - and applying them without overlap. - When virtual magnets exported from combined function mangets are present (RWMapper), - the aggregator prevents to apply several times the same power supply setpoint. + Aggregate magnet strengths while avoiding duplicate hardware writes. + + Magnet models convert between exposed strengths and hardware setpoints. + Shared models, such as those used by virtual magnets from combined-function + magnets, are written only once per underlying power supply. + + Parameters + ---------- + peer : CSScalarAggregator + Scalar device aggregator containing the hardware devices. + + Methods + ------- + add_magnet(magnet, devs) + Register a magnet and its hardware devices with the aggregator. + set(value) + Convert strengths to hardware values and write the setpoints. + set_and_wait(value) + Set magnet strengths and wait for hardware readback. + get() + Read the current values from the underlying devices. + readback() + Read back magnet strengths from measured hardware values. + unit() + Return the units associated with the underlying devices. """ def __init__(self, peer: CSScalarAggregator): + """ + Initialize the CSStrengthScalarAggregator. + """ CSScalarAggregator.__init__(self, peer._devs) self.__models: list[MagnetModel] = [] # List of magnet model self.__modelToMagnet: list[list[tuple[int, int]]] = [] # strengths indexing @@ -223,6 +337,16 @@ def add_magnet(self, magnet: Magnet, devs: list[DeviceAccess]): # a CombinedFunctionMagnet or simple magnet. # All magnets exported from a same CombinedFunctionMagnet share the same model # TODO: check that strength is supported (m.strength may be None) + """ + Register a magnet and its hardware devices with the aggregator. + + Parameters + ---------- + magnet : Magnet + Magnet whose strength is being aggregated. + devs : list[DeviceAccess] + Hardware devices associated with the magnet model. + """ strengthIndex = magnet.strength.index() if isinstance(magnet.strength, abstract.RWMapper) else 0 if magnet.model not in self.__models: index = len(self.__models) @@ -235,11 +359,19 @@ def add_magnet(self, magnet: Magnet, devs: list[DeviceAccess]): self.__nbMagnet += 1 def set(self, value: NDArray[np.float64]): + """ + Convert strengths to hardware values and write the setpoints. + + Parameters + ---------- + value : NDArray[np.float64] + Magnet strengths, ordered according to the registered magnets. + """ allHardwareValues = self._devs.get() # Read all hardware setpoints newHardwareValues = np.zeros(self.nb_device()) hardwareIndex = 0 for modelIndex, model in enumerate(self.__models): - nbDev = len(model.get_devices()) + nbDev = len(model.get_device_names()) mStrengths = model.compute_strengths(allHardwareValues[hardwareIndex : hardwareIndex + nbDev]) for valueIdx, strengthIdx in self.__modelToMagnet[modelIndex]: mStrengths[strengthIdx] = value[valueIdx] @@ -251,14 +383,30 @@ def set(self, value: NDArray[np.float64]): self._devs.set(newHardwareValues) def set_and_wait(self, value: NDArray[np.float64]): + """ + Set magnet strengths and wait for hardware readback. + + Waiting for readback is not implemented by this aggregator. + + Parameters + ---------- + value : NDArray[np.float64] + Magnet strengths to convert and write. + + Raises + ------ + NotImplementedError + Always raised because asynchronous confirmation is unsupported. + """ raise NotImplementedError("Not implemented yet.") def get(self) -> NDArray[np.float64]: + """Read the current values from the underlying devices.""" allHardwareValues = self._devs.get() # Read all hardware setpoints allStrength = np.zeros(self.__nbMagnet) hardwareIndex = 0 for modelIndex, model in enumerate(self.__models): - nbDev = len(model.get_devices()) + nbDev = len(model.get_device_names()) mStrengths = model.compute_strengths(allHardwareValues[hardwareIndex : hardwareIndex + nbDev]) for valueIdx, strengthIdx in self.__modelToMagnet[modelIndex]: allStrength[valueIdx] = mStrengths[strengthIdx] @@ -266,11 +414,19 @@ def get(self) -> NDArray[np.float64]: return allStrength def readback(self) -> np.array: + """ + Read back magnet strengths from measured hardware values. + + Returns + ------- + numpy.ndarray + Magnet strengths corresponding to the latest device readbacks. + """ allHardwareValues = self._devs.readback() # Read all hardware readback allStrength = np.zeros(self.__nbMagnet) hardwareIndex = 0 for modelIndex, model in enumerate(self.__models): - nbDev = len(model.get_devices()) + nbDev = len(model.get_device_names()) mStrengths = model.compute_strengths(allHardwareValues[hardwareIndex : hardwareIndex + nbDev]) for valueIdx, strengthIdx in self.__modelToMagnet[modelIndex]: allStrength[valueIdx] = mStrengths[strengthIdx] @@ -278,74 +434,100 @@ def readback(self) -> np.array: return allStrength def unit(self) -> str: + """Return the units associated with the underlying devices.""" return self._devs.unit() # ------------------------------------------------------------------------------ -class CSBPMArrayMapper(CSScalarAggregator): - """ - Wrapper to a native CS aggregator for BPM - """ - - def __init__(self, devs: list[DeviceAccess], indices: list[list[int]]): - self._indices = indices - self._devs = devs - - def set(self, value: NDArray[np.float64]): - raise Exception("BPM are not writable") - - def get(self) -> NDArray[np.float64]: - if len(self._devs) == 1: - v = self._devs[0].get() - return v[self._indices[0]] - else: - # TODO read using DeviceAccessList - v0 = self._devs[0].get()[self._indices[0]] - v1 = self._devs[1].get()[self._indices[1]] - # Interleave - xy = np.zeros(v0.size + v1.size) - xy[0::2] = v0 - xy[1::2] = v1 - return xy - - def readback(self) -> np.array: - return self.get() - - def unit(self) -> str: - return self._dev.unit() - - # ------------------------------------------------------------------------------ class RWHardwareScalar(abstract.ReadWriteFloatScalar): """ - Class providing read write access to a magnet - of a control system (in hardware units) + Expose one magnet hardware setpoint as a readable/writable scalar. + + Parameters + ---------- + model : MagnetModel + Magnet model used to determine the hardware unit. + dev : DeviceAccess + Control-system device holding the hardware setpoint. + + Methods + ------- + get() + Return the current hardware setpoint. + set(value) + Validate and write a magnet hardware setpoint. + set_and_wait(value) + Set the hardware value and wait for readback confirmation. + unit() + Return the hardware unit defined by the magnet model. + set_magnet_rigidity(brho) + Set the beam rigidity used by the magnet model. """ def __init__(self, model: MagnetModel, dev: DeviceAccess): + """ + Initialize the RWHardwareScalar. + """ self.__model = model self.__dev = dev def get(self) -> float: + """Return the current hardware setpoint.""" return self.__dev.get() def set(self, value: float): + """ + Validate and write a magnet hardware setpoint. + + Parameters + ---------- + value : float + Hardware value to write to the control-system device. + + Raises + ------ + PyAMLException + If ``value`` is outside the device's configured range. + """ dev_range = self.__dev.get_range() if not check_range(value, dev_range): raise PyAMLException(format_out_of_range_message(value, self.__dev)) self.__dev.set(value) def set_and_wait(self, value: double): + """ + Set the hardware value and wait for readback confirmation. + + Parameters + ---------- + value : double + Hardware value to write. + + Raises + ------ + NotImplementedError + Always raised because asynchronous confirmation is unsupported. + """ raise NotImplementedError("Not implemented yet.") def unit(self) -> str: + """Return the hardware unit defined by the magnet model.""" return self.__model.get_hardware_units()[0] def set_magnet_rigidity(self, brho: np.double): + """ + Set the beam rigidity used by the magnet model. + + Parameters + ---------- + brho : np.double + Magnetic rigidity in tesla metres. + """ self.__model.set_magnet_rigidity(brho) @@ -354,20 +536,58 @@ def set_magnet_rigidity(self, brho: np.double): class RWStrengthScalar(abstract.ReadWriteFloatScalar): """ - Class providing read write access to a strength of a control system + Expose one magnet strength with hardware-value conversion. + + Parameters + ---------- + model : MagnetModel + Magnet model used for strength conversion and units. + dev : DeviceAccess + Control-system device holding the corresponding hardware value. + + Methods + ------- + get() + Read the hardware value and convert it to magnet strength. + set(value) + Convert and write a magnet strength setpoint. + set_and_wait(value) + Set a magnet strength and wait for readback confirmation. + unit() + Return the strength unit defined by the magnet model. + set_magnet_rigidity(brho) + Set the beam rigidity used by the magnet model. """ def __init__(self, model: MagnetModel, dev: DeviceAccess): + """ + Initialize the RWStrengthScalar. + """ self.__model = model self.__dev = dev # Gets the value def get(self) -> float: + """Read the hardware value and convert it to magnet strength.""" current = self.__dev.get() return self.__model.compute_strengths([current])[0] # Sets the value def set(self, value: float): + """ + Convert and write a magnet strength setpoint. + + Parameters + ---------- + value : float + Magnet strength to convert to hardware units and write. + + Raises + ------ + PyAMLException + If the converted hardware value is outside the device's + configured range. + """ current = self.__model.compute_hardware_values([value])[0] dev_range = self.__dev.get_range() if not check_range(current, dev_range): @@ -376,13 +596,35 @@ def set(self, value: float): # Sets the value and wait that the read value reach the setpoint def set_and_wait(self, value: float): + """ + Set a magnet strength and wait for readback confirmation. + + Parameters + ---------- + value : float + Magnet strength to convert and write. + + Raises + ------ + NotImplementedError + Always raised because asynchronous confirmation is unsupported. + """ raise NotImplementedError("Not implemented yet.") # Gets the unit of the value def unit(self) -> str: + """Return the strength unit defined by the magnet model.""" return self.__model.get_strength_units()[0] def set_magnet_rigidity(self, brho: np.double): + """ + Set the beam rigidity used by the magnet model. + + Parameters + ---------- + brho : np.double + Magnetic rigidity in tesla metres. + """ self.__model.set_magnet_rigidity(brho) @@ -391,20 +633,54 @@ def set_magnet_rigidity(self, brho: np.double): class RWHardwareArray(abstract.ReadWriteFloatArray): """ - Class providing read write access to a magnet array - of a control system (in hardware units) + Expose multiple magnet hardware setpoints as an array interface. + + Parameters + ---------- + model : MagnetModel + Magnet model defining the hardware units. + devs : list[DeviceAccess] + Control-system devices holding the hardware setpoints. + + Methods + ------- + get() + Return the current hardware values in device order. + set(value) + Validate and write hardware values for all devices. + set_and_wait(value) + Set hardware values and wait for readback confirmation. + unit() + Return the hardware units defined by the magnet model. """ def __init__(self, model: MagnetModel, devs: list[DeviceAccess]): + """ + Initialize the RWHardwareArray. + """ self.__model = model self.__devs = devs # Gets the value def get(self) -> np.array: + """Return the current hardware values in device order.""" return np.array([p.get() for p in self.__devs]) # Sets the value def set(self, value: np.array): + """ + Validate and write hardware values for all devices. + + Parameters + ---------- + value : np.array + Hardware values ordered to match ``self.__devs``. + + Raises + ------ + PyAMLException + If any value is outside its device's configured range. + """ for idx, p in enumerate(self.__devs): dev_range = p.get_range() if not check_range(value[idx], dev_range): @@ -413,10 +689,24 @@ def set(self, value: np.array): # Sets the value and waits that the read value reach the setpoint def set_and_wait(self, value: np.array): + """ + Set hardware values and wait for readback confirmation. + + Parameters + ---------- + value : np.array + Hardware values to write in device order. + + Raises + ------ + NotImplementedError + Always raised because asynchronous confirmation is unsupported. + """ raise NotImplementedError("Not implemented yet.") # Gets the unit of the value def unit(self) -> list[str]: + """Return the hardware units defined by the magnet model.""" return self.__model.get_hardware_units() @@ -425,21 +715,51 @@ def unit(self) -> list[str]: class RWStrengthArray(abstract.ReadWriteFloatArray): """ - Class providing read write access to magnet strengths of a control system + Expose multiple magnet strengths with hardware-value conversion. + + Parameters + ---------- + model : MagnetModel + Magnet model used for strength conversion and units. + devs : list[DeviceAccess] + Control-system devices corresponding to the model's hardware values. + + Methods + ------- + get() + Read hardware values and convert them to magnet strengths. + set(value) + Convert strengths to hardware values and write the setpoints. + set_and_wait(value) + Set magnet strengths and wait for readback confirmation. + unit() + Return the strength units defined by the magnet model. """ def __init__(self, model: MagnetModel, devs: list[DeviceAccess]): + """ + Initialize the RWStrengthArray. + """ self.__model = model self.__devs = devs # Gets the value def get(self) -> np.array: + """Read hardware values and convert them to magnet strengths.""" r = np.array([p.get() for p in self.__devs]) str = self.__model.compute_strengths(r) return str # Sets the value def set(self, value: np.array): + """ + Convert strengths to hardware values and write the setpoints. + + Parameters + ---------- + value : np.array + Magnet strengths ordered to match ``self.__devs``. + """ cur = self.__model.compute_hardware_values(value) for idx, p in enumerate(self.__devs): dev_range = p.get_range() @@ -451,10 +771,24 @@ def set(self, value: np.array): # Sets the value and waits that the read value reach the setpoint def set_and_wait(self, value: np.array): + """ + Set magnet strengths and wait for readback confirmation. + + Parameters + ---------- + value : np.array + Magnet strengths to convert and write. + + Raises + ------ + NotImplementedError + Always raised because asynchronous confirmation is unsupported. + """ raise NotImplementedError("Not implemented yet.") # Gets the unit of the value def unit(self) -> list[str]: + """Return the strength units defined by the magnet model.""" return self.__model.get_strength_units() @@ -463,35 +797,39 @@ def unit(self) -> list[str]: class RBpmArray(abstract.ReadFloatArray): """ - Class providing read access to a BPM position [x,y] of a control system + Expose horizontal and vertical BPM positions as an array. + + Parameters + ---------- + hDev : DeviceAccess + Device providing the horizontal BPM position. + vDev : DeviceAccess + Device providing the vertical BPM position. + + Methods + ------- + get() + Return horizontal and vertical BPM positions. + unit() + Return the unit reported by the BPM device. """ - def __init__(self, model: BPMModel, hDev: DeviceAccess, vDev: DeviceAccess): - self._model = model + def __init__(self, hDev: DeviceAccess, vDev: DeviceAccess): + """ + Initialize the RBpmArray. + """ self._hDev = hDev self._vDev = vDev - self._hIdx = self._model.x_pos_index() - self._vIdx = self._model.y_pos_index() - # Gets the values def get(self) -> np.array: - if self._hDev != self._vDev: - allhVal = self._hDev.get() - allvVal = self._vDev.get() - hVal = allhVal if self._hIdx is None else allhVal[self._hIdx] - vVal = allvVal if self._vIdx is None else allvVal[self._vIdx] - else: - # When h and v devices are identical, indexed - # values are expected - allVal = self._hDev.get() - hVal = allVal[self._hIdx] - vVal = allVal[self._vIdx] - return np.array([hVal, vVal]) + """Return horizontal and vertical BPM positions.""" + return np.array([self._hDev.get(), self._vDev.get()]) # Gets the unit of the value Assume that x and y, offsets and positions # have the same unit def unit(self) -> str: - return self._model.get_pos_devices()[0].unit() + """Return the unit reported by the BPM device.""" + return self._hDev.unit() # ------------------------------------------------------------------------------ @@ -500,30 +838,65 @@ def unit(self) -> str: class RWBpmTiltScalar(abstract.ReadFloatScalar): """ Class providing read access to a BPM tilt of a control system + + Parameters + ---------- + dev : DeviceAccess + Device handle giving access to the BPM tilt attribute. + + Methods + ------- + get() + Return horizontal and vertical BPM positions. + set(value) + Write the BPM tilt value to the control-system device. + set_and_wait(value) + Set the BPM tilt and wait for readback confirmation. + unit() + Return the unit shared by the BPM devices. """ - def __init__(self, model: BPMModel, dev: DeviceAccess): - self._model = model + def __init__(self, dev: DeviceAccess): + """ + Initialize the RWBpmTiltScalar. + """ self._dev = dev - self._idx = model.tilt_index() - # Gets the value def get(self) -> float: - allTilt = self._dev.get() - if self._idx is not None: - return allTilt[self._idx] - else: - return allTilt + """Return horizontal and vertical BPM positions.""" + return self._dev.get() def set(self, value: float): + """ + Write the BPM tilt value to the control-system device. + + Parameters + ---------- + value : float + BPM tilt value in the device's configured units. + """ self._dev.set(value) def set_and_wait(self, value: NDArray[np.float64]): + """ + Set the BPM tilt and wait for readback confirmation. + + Parameters + ---------- + value : NDArray[np.float64] + BPM tilt value to write. + + Raises + ------ + NotImplementedError + Always raised because asynchronous confirmation is unsupported. + """ raise NotImplementedError("Not implemented yet.") # Gets the unit of the value def unit(self) -> str: - return self._model.get_tilt_device().unit() + """Return the unit shared by the BPM devices.""" + return self._dev.unit() # ------------------------------------------------------------------------------ @@ -531,51 +904,71 @@ def unit(self) -> str: class RWBpmOffsetArray(abstract.ReadWriteFloatArray): """ - Class providing read write access to a BPM offset [x,y] of a control system + Expose horizontal and vertical BPM offsets as a writable array. + + Parameters + ---------- + hDev : DeviceAccess + Device handle for the horizontal BPM offset. + vDev : DeviceAccess + Device handle for the vertical BPM offset. + + Methods + ------- + get() + Return horizontal and vertical BPM offsets. + set(value) + Write horizontal and vertical BPM offsets. + set_and_wait(value) + Set BPM offsets and wait for readback confirmation. + unit() + Return the unit shared by the BPM offset devices. """ - def __init__(self, model: BPMModel, hDev: DeviceAccess, vDev: DeviceAccess): - self._model = model + def __init__(self, hDev: DeviceAccess, vDev: DeviceAccess): + """ + Initialize the RWBpmOffsetArray. + """ self._hDev = hDev self._vDev = vDev - self._hIdx = self._model.x_pos_index() - self._vIdx = self._model.y_pos_index() - # Gets the values def get(self) -> np.array: - if self._hDev != self._vDev: - allhVal = self._hDev.get() - allvVal = self._vDev.get() - hVal = allhVal if self._hIdx is None else allhVal[self._hIdx] - vVal = allvVal if self._vIdx is None else allvVal[self._vIdx] - else: - # When h and v devices are identical, indexed - # values are expected - allVal = self._hDev.get() - hVal = allVal[self._hIdx] - vVal = allVal[self._vIdx] - return np.array([hVal, vVal]) - - # Sets the values + """Return horizontal and vertical BPM offsets.""" + return np.array([self._hDev.get(), self._vDev.get()]) + def set(self, value: NDArray[np.float64]): - if self._hDev != self._vDev: - self._hDev.set(value[0]) - self._vDev.set(value[1]) - else: - # When h and v devices are identical, indexed - # values are expected - newValue = self._hDev.get() - newValue[self._hIdx] = value[0] - newValue[self._vIdx] = value[1] - self._hDev.set(newValue) + """ + Write horizontal and vertical BPM offsets. + + Parameters + ---------- + value : NDArray[np.float64] + Two-element array containing horizontal and vertical offsets. + """ + self._hDev.set(value[0]) + self._vDev.set(value[1]) def set_and_wait(self, value: NDArray[np.float64]): + """ + Set BPM offsets and wait for readback confirmation. + + Parameters + ---------- + value : NDArray[np.float64] + Two-element array containing horizontal and vertical offsets. + + Raises + ------ + NotImplementedError + Always raised because asynchronous confirmation is unsupported. + """ raise NotImplementedError("Not implemented yet.") # Gets the unit of the value Assume that x and y, offsets and positions # have the same unit def unit(self) -> str: - return self._model.get_pos_devices()[0].unit() + """Return the unit shared by the BPM offset devices.""" + return self._hDev.unit() # ------------------------------------------------------------------------------ @@ -585,22 +978,66 @@ class RWRFVoltageScalar(abstract.ReadWriteFloatScalar): """ Class providing read write access to cavity voltage for a transmitter of a control system. + + Parameters + ---------- + transmitter : RFTransmitter + RF transmitter whose configuration supplies the voltage unit. + dev : DeviceAccess + Control-system device holding the cavity-voltage value. + + Methods + ------- + get() + Return the current cavity voltage. + set(value) + Write a cavity-voltage setpoint to the transmitter device. + set_and_wait(value) + Set the cavity voltage and wait for readback confirmation. + unit() + Return the configured cavity-voltage unit. """ def __init__(self, transmitter: RFTransmitter, dev: DeviceAccess): + """ + Initialize the RWRFVoltageScalar. + """ self.__transmitter = transmitter self.__dev = dev def get(self) -> float: + """Return the current cavity voltage.""" return self.__dev.get() def set(self, value: float): + """ + Write a cavity-voltage setpoint to the transmitter device. + + Parameters + ---------- + value : float + Cavity-voltage setpoint in the configured voltage unit. + """ self.__dev.set(value) def set_and_wait(self, value: float): + """ + Set the cavity voltage and wait for readback confirmation. + + Parameters + ---------- + value : float + Cavity-voltage setpoint. + + Raises + ------ + NotImplementedError + Always raised because asynchronous confirmation is unsupported. + """ raise NotImplementedError("Not implemented yet.") def unit(self) -> str: + """Return the configured cavity-voltage unit.""" return self.__transmitter._cfg.voltage.unit() @@ -611,22 +1048,66 @@ class RWRFPhaseScalar(abstract.ReadWriteFloatScalar): """ Class providing read write access to cavity phase for a transmitter of a control system. + + Parameters + ---------- + transmitter : RFTransmitter + RF transmitter whose configuration supplies the phase unit. + dev : DeviceAccess + Control-system device holding the cavity phase. + + Methods + ------- + get() + Return the current cavity phase. + set(value) + Write a cavity-phase setpoint to the transmitter device. + set_and_wait(value) + Set the cavity phase and wait for readback confirmation. + unit() + Return the configured cavity-phase unit. """ def __init__(self, transmitter: RFTransmitter, dev: DeviceAccess): + """ + Initialize the RWRFPhaseScalar. + """ self.__transmitter = transmitter self.__dev = dev def get(self) -> float: + """Return the current cavity phase.""" return self.__dev.get() def set(self, value: float): + """ + Write a cavity-phase setpoint to the transmitter device. + + Parameters + ---------- + value : float + Cavity-phase setpoint in the configured phase unit. + """ self.__dev.set(value) def set_and_wait(self, value: float): + """ + Set the cavity phase and wait for readback confirmation. + + Parameters + ---------- + value : float + Cavity-phase setpoint. + + Raises + ------ + NotImplementedError + Always raised because asynchronous confirmation is unsupported. + """ raise NotImplementedError("Not implemented yet.") def unit(self) -> str: + """Return the configured cavity-phase unit.""" return self.__transmitter._cfg.phase.unit() @@ -636,23 +1117,67 @@ def unit(self) -> str: class RWRFFrequencyScalar(abstract.ReadWriteFloatScalar): """ Class providing read write access to RF frequency of a control system. + + Parameters + ---------- + rf : RFPlant + RF plant whose configuration supplies the frequency unit. + dev : DeviceAccess + Control-system device holding the RF frequency. + + Methods + ------- + get() + Return the current RF frequency. + set(value) + Write an RF-frequency setpoint to the plant device. + set_and_wait(value) + Set the RF frequency and wait for readback confirmation. + unit() + Return the configured RF-frequency unit. """ def __init__(self, rf: RFPlant, dev: DeviceAccess): + """ + Initialize the RWRFFrequencyScalar. + """ self.__rf = rf self.__dev = dev def get(self) -> float: # Serialized cavity has the same frequency + """Return the current RF frequency.""" return self.__dev.get() def set(self, value: float): + """ + Write an RF-frequency setpoint to the plant device. + + Parameters + ---------- + value : float + RF-frequency setpoint in the configured frequency unit. + """ self.__dev.set(value) def set_and_wait(self, value: float): + """ + Set the RF frequency and wait for readback confirmation. + + Parameters + ---------- + value : float + RF-frequency setpoint. + + Raises + ------ + NotImplementedError + Always raised because asynchronous confirmation is unsupported. + """ raise NotImplementedError("Not implemented yet.") def unit(self) -> str: + """Return the configured RF-frequency unit.""" return self.__rf._cfg.masterclock.unit() @@ -661,15 +1186,33 @@ def unit(self) -> str: class RBetatronTuneArray(abstract.ReadFloatArray): """ - Class providing read write access to betatron tune of a control system. + Expose horizontal and vertical betatron tunes as a read-only array. + + Parameters + ---------- + tune_monitor : object + Tune monitor configuration supplying the tune unit. + devs : list[DeviceAccess] + Devices providing horizontal and vertical tune measurements. + + Methods + ------- + get() + Return horizontal and vertical betatron tunes. + unit() + Return the configured betatron-tune unit. """ def __init__(self, tune_monitor, devs: list[DeviceAccess]): + """ + Initialize the RBetatronTuneArray. + """ self.__tune_monitor = tune_monitor self.__devs = devs def get(self) -> NDArray: # Return horizontal and vertical betatron tunes as a NumPy array + """Return horizontal and vertical betatron tunes.""" return np.array( [ self.__devs[0].get(), @@ -678,6 +1221,7 @@ def get(self) -> NDArray: ) def unit(self) -> str: + """Return the configured betatron-tune unit.""" return self.__tune_monitor._cfg.tune_v.unit() diff --git a/pyaml/control/controlsystem.py b/pyaml/control/controlsystem.py index 33f57f84c..9199f98de 100644 --- a/pyaml/control/controlsystem.py +++ b/pyaml/control/controlsystem.py @@ -1,17 +1,22 @@ +""" +Control-system element binding and runtime device interfaces. + +The classes in this module resolve configured device references, attach +accelerator elements to a control-system backend, and construct the scalar, +array, and aggregator interfaces used to access those elements at runtime. +""" + from abc import ABCMeta, abstractmethod -from typing import Tuple + +from pydantic import BaseModel from ..bpm.bpm import BPM -from ..bpm.bpm_model import BPMModel from ..common.abstract import RWMapper from ..common.abstract_aggregator import ScalarAggregator -from ..common.element import Element -from ..common.element_holder import ElementHolder from ..common.exception import PyAMLException -from ..configuration.factory import Factory +from ..common.holders.element_holder import ElementHolder from ..configuration.unbound_element import UnboundElement from ..control.abstract_impl import ( - CSBPMArrayMapper, CSScalarAggregator, CSStrengthScalarAggregator, RBetatronTuneArray, @@ -36,255 +41,288 @@ from ..tuning_tools.measurement_tool import MeasurementTool from ..tuning_tools.tuning_tool import TuningTool from .deviceaccess import DeviceAccess +from .deviceaccesslist import DeviceAccessList class ControlSystem(ElementHolder, metaclass=ABCMeta): """ - Abstract class providing access to a control system float variable + Define the interface for binding accelerator elements to a backend. + + A control system resolves PyAML element names to control-system devices and + wraps them in read/write accessors, so tools written against + :class:`~pyaml.common.holders.element_holder.ElementHolder` drive a live + machine unchanged. Concrete backends live in separate packages and are + selected from the configuration. + + Methods + ------- + name() + Return the backend control-system name. + get_aggregator() + Return an empty device aggregator, or ``None`` for direct access. + get_device_access(ref) + Return a device reference for this control system. YAML element configuration passes opaque strings. Public + Python APIs may also pass backend ConfigModel instances. Concrete backends own all lookup, parsing and + DeviceAccess construction. + get_devices_access(refs) + Resolve a list of backend references into device access objects. + create_magnet_strength_aggregator(magnets) + Create an aggregator that exposes magnet strengths. + create_magnet_hardware_aggregator(magnets) + Create an aggregator for magnet hardware values. + create_bpm_aggregators(bpms) + Create aggregate BPM position channels. + fill_device(elements) + Fill device of this control system with Element coming from the configuration file """ def __init__(self): + """ + Initialize the ControlSystem. + """ ElementHolder.__init__(self) @abstractmethod - def attach(self, dev: list[DeviceAccess]) -> list[DeviceAccess]: - """Return new instances of DeviceAccess objects - coming from configuration attached to this CS""" + def name(self) -> str: + """Return the backend control-system name.""" pass @abstractmethod - def attach_array(self, dev: list[DeviceAccess]) -> list[DeviceAccess]: - """Return new instances of DeviceAccess objects - coming from configuration attached to this CS""" + def get_aggregator(self) -> DeviceAccessList | None: + """Return an empty device aggregator, or ``None`` for direct access.""" pass @abstractmethod - def name(self) -> str: - """Return control system name (i.e. live)""" + def get_device_access(self, ref: str | BaseModel | None) -> DeviceAccess: + """ + Return a device reference for this control system. + YAML element configuration passes opaque strings. Public Python APIs may + also pass backend ConfigModel instances. Concrete backends own all + lookup, parsing and DeviceAccess construction. + """ pass - @abstractmethod - def scalar_aggregator(self) -> str | None: - """Returns the module name used for handling aggregator of DeviceAccess""" - return None - - @abstractmethod - def vector_aggregator(self) -> str | None: - """Returns the module name used for handling aggregator of DeviceVectorAccess""" - return None - - def attach_indexed(self, dev: DeviceAccess, idx: int | None) -> DeviceAccess: - if idx is not None: - return self.attach_array([dev])[0] - else: - return self.attach([dev])[0] + def get_devices_access(self, refs: list[str | BaseModel | None]) -> list[DeviceAccess]: + """ + Resolve a list of backend references into device access objects. - def create_scalar_aggregator(self) -> ScalarAggregator: - mod = self.scalar_aggregator() - agg = Factory.build_object({"type": mod}) if mod is not None else None + Parameters + ---------- + refs : list of str or BaseModel or None + Backend-specific device references from the configuration. + + Returns + ------- + list of DeviceAccess + Device access objects in the same order as ``refs``. + + Raises + ------ + PyAMLException + If ``refs`` is not a list. + """ + if not isinstance(refs, list): + raise PyAMLException(f"get_devices() expect a list as input arguments but got {str(type(refs))}") + return [self.get_device_access(ref) for ref in refs] + + def _create_scalar_aggregator(self) -> ScalarAggregator | None: + """Create an empty scalar aggregator for this control-system backend.""" + agg = self.get_aggregator() + if agg is None: + return None return CSScalarAggregator(agg) - def create_magnet_strength_aggregator(self, magnets: list[Magnet]) -> ScalarAggregator: - agg = CSStrengthScalarAggregator(self.create_scalar_aggregator()) + def create_magnet_strength_aggregator(self, magnets: list[Magnet]) -> ScalarAggregator | None: + """ + Create an aggregator that exposes magnet strengths. + + Parameters + ---------- + magnets : list[Magnet] + Magnets whose strength channels should be aggregated. + + Returns + ------- + ScalarAggregator | None + Strength aggregator, or ``None`` when the backend does not use + aggregators. + """ + agg = self._create_scalar_aggregator() + if agg is None: + return None + magg = CSStrengthScalarAggregator(agg) for m in magnets: - devs = self.attach(m.model.get_devices()) - agg.add_magnet(m, devs) - return agg + devs = self.get_devices_access(m.model.get_device_names()) + magg.add_magnet(m, devs) + return magg + + def create_magnet_hardware_aggregator(self, magnets: list[Magnet]) -> ScalarAggregator | None: + """ + Create an aggregator for magnet hardware values. + + One power-supply device is selected for each magnet strength exposed + in hardware space. ``None`` is returned if a magnet lacks hardware + support or the backend does not provide aggregators. + + Parameters + ---------- + magnets : list[Magnet] + Magnets whose hardware channels should be grouped. - def create_magnet_hardware_aggregator(self, magnets: list[Magnet]) -> ScalarAggregator: - """When working in hardware space, 1 single power - supply device per multipolar strength is required + Returns + ------- + ScalarAggregator | None + Grouped accessor, or ``None`` when a magnet exposes no hardware device. """ - agg = self.create_scalar_aggregator() + agg = self._create_scalar_aggregator() + if agg is None: + return None for m in magnets: if not m.model.has_hardware(): return None psIndex = m.hardware.index() if isinstance(m.hardware, RWMapper) else 0 - agg.add_devices(self.attach([m.model.get_devices()[psIndex]])[0]) + agg.add_devices(self.get_devices_access([m.model.get_device_names()[psIndex]])[0]) return agg - def create_bpm_aggregators(self, bpms: list[BPM]) -> list[ScalarAggregator]: - # return [None,None,None] - - if any([not b.model.is_pos_indexed() for b in bpms]): - # Aggregator for single BPM (all values are scalar) - agg = self.create_scalar_aggregator() - aggh = self.create_scalar_aggregator() - aggv = self.create_scalar_aggregator() - for b in bpms: - devs = self.attach(b.model.get_pos_devices()) - agg.add_devices(devs) - aggh.add_devices(devs[0]) - aggv.add_devices(devs[1]) - return [agg, aggh, aggv] - - elif any([b.model.is_pos_indexed() for b in bpms]): - # Aggregator for indexed BPMs - allH = [] - hIdx = [] - allV = [] - vIdx = [] - allHV = [] - for b in bpms: - devs = self.attach_array(b.model.get_pos_devices()) - devH = devs[0] - devV = devs[1] - if devH not in allH: - allH.append(devH) - if devH not in allHV: - allHV.append(devH) - if devV not in allV: - allV.append(devV) - if devV not in allHV: - allHV.append(devV) - hIdx.append(b.model.x_pos_index()) - vIdx.append(b.model.y_pos_index()) - - if len(allH) > 1 or len(allV) > 1: - # Does not support aggregator for individual BPM that - # returns an array of [x,y] - print("Warning, Individual BPM that returns [x,y]" + " are not read in parralell") - # Default to serialized readding - return [None, None, None] - - if devH == devV: - # [x0,y0,x1,y0,....] - idx = [] - for b in bpms: - idx.append(b.model.x_pos_index()) - idx.append(b.model.y_pos_index()) - hvIdx = [idx] - else: - hvIdx = [hIdx, vIdx] - - agg = CSBPMArrayMapper(allHV, hvIdx) - aggh = CSBPMArrayMapper(allH, [hIdx]) - aggv = CSBPMArrayMapper(allV, [vIdx]) - return [agg, aggh, aggv] - else: - raise PyAMLException("Indexed BPM and scalar values cannot be mixed in the same array") - - def fill_device(self, elements: list[Element]): + def create_bpm_aggregators(self, bpms: list[BPM]) -> list[ScalarAggregator | None]: """ - Fill device of this control system with Element - coming from the configuration file + Create aggregate BPM position channels. Parameters ---------- - elements : list[Element] - List of elements coming from the configuration - file to attach to this control system + bpms : list[BPM] + BPM elements whose position devices should be aggregated. + + Returns + ------- + list[ScalarAggregator | None] + Aggregators for combined, horizontal, and vertical positions. """ - for e in elements: - if isinstance(e, Magnet): - dev = self.attach(e.model.get_devices())[0] - current = RWHardwareScalar(e.model, dev) if e.model.has_hardware() else None - strength = RWStrengthScalar(e.model, dev) if e.model.has_physics() else None - # Create a unique ref for this control system - m = e.attach(self, strength, current) - self.add_magnet(m) - - elif isinstance(e, CombinedFunctionMagnet): - devs = self.attach(e.model.get_devices()) - currents = RWHardwareArray(e.model, devs) - strengths = RWStrengthArray(e.model, devs) - # Create unique refs the cfm and - # each of its function for this control system - ms = e.attach(self, strengths, currents) - self.add_cfm_magnet(ms[0]) - for m in ms[1:]: - self.add_magnet(m) - - elif isinstance(e, SerializedMagnets): - devs = self.attach(e.model.get_devices()) - currents = [] - strengths = [] - # Create unique refs the series and each of its function for this - # control system - for i in range(e.get_nb_magnets()): - current = RWHardwareScalar(e.model.get_sub_model(i), devs[i]) if e.model.has_hardware() else None - strength = RWStrengthScalar(e.model.get_sub_model(i), devs[i]) if e.model.has_physics() else None - currents.append(current) - strengths.append(strength) - ms = e.attach(self, strengths, currents) - self.add_serialized_magnet(ms[0]) - for m in ms[1:]: - self.add_magnet(m) - - elif isinstance(e, BPM): - hDev = e.model.get_pos_devices()[0] - vDev = e.model.get_pos_devices()[1] - tiltDev = e.model.get_tilt_device() - hOffsetDev = e.model.get_offset_devices()[0] - vOffsetDev = e.model.get_offset_devices()[1] - ahDev = self.attach_indexed(hDev, e.model.x_pos_index()) - avDev = self.attach_indexed(vDev, e.model.y_pos_index()) - atiltDev = self.attach_indexed(tiltDev, e.model.tilt_index()) - ahOffsetDev = self.attach_indexed(hOffsetDev, e.model.x_offset_index()) - avOffsetDev = self.attach_indexed(vOffsetDev, e.model.y_offset_index()) - positions = RBpmArray(e.model, ahDev, avDev) - tilt = RWBpmTiltScalar(e.model, atiltDev) - offsets = RWBpmOffsetArray(e.model, ahOffsetDev, avOffsetDev) - e = e.attach(self, positions, offsets, tilt) - self.add_bpm(e) - - elif isinstance(e, RFPlant): - attachedTrans: list[RFTransmitter] = [] - if e._cfg.transmitters: - for t in e._cfg.transmitters: - vDev = self.attach([t._cfg.voltage])[0] - pDev = self.attach([t._cfg.phase])[0] - voltage = RWRFVoltageScalar(t, vDev) - phase = RWRFPhaseScalar(t, pDev) - nt = t.attach(self, voltage, phase) - self.add_rf_transnmitter(nt) - attachedTrans.append(nt) - - fDev = self.attach([e._cfg.masterclock])[0] - frequency = RWRFFrequencyScalar(e, fDev) - voltage = RWTotalVoltage(attachedTrans) if e._cfg.transmitters else None - ne = e.attach(self, frequency, voltage) - self.add_rf_plant(ne) - - elif isinstance(e, BetatronTuneMonitor): - # Built in tune monitor - tuneDevs = self.attach([e._cfg.tune_h, e._cfg.tune_v]) - betatron_tune = RBetatronTuneArray(e, tuneDevs) - e = e.attach(self, betatron_tune) - self.add_betatron_tune_monitor(e) - - elif isinstance(e, TuningTool) | isinstance(e, MeasurementTool): - self.add_tool(e.attach(self)) - - elif isinstance(e, UnboundElement): - if self.name() in e._control_modes: - ne = Factory.build_unbound(e, self) - if isinstance(ne, ABetatronTuneMonitor): - self.add_betatron_tune_monitor(ne) - else: - # Default to standard Element - self.add_element(ne) + agg = self._create_scalar_aggregator() + aggh = self._create_scalar_aggregator() + aggv = self._create_scalar_aggregator() + if agg is None or aggh is None or aggv is None: + return [None, None, None] + for b in bpms: + devs = self.get_devices_access(b.get_pos_devices()) + agg.add_devices(devs) + aggh.add_devices(devs[0]) + aggv.add_devices(devs[1]) + return [agg, aggh, aggv] + + def _fill_magnet(self, magnet: Magnet) -> None: + device = self.get_device_access(magnet.model.get_device_names()[0]) + current = RWHardwareScalar(magnet.model, device) if magnet.model.has_hardware() else None + strength = RWStrengthScalar(magnet.model, device) if magnet.model.has_physics() else None + self.magnet.add(magnet.attach(self, strength, current)) + + def _fill_combined_function_magnet(self, magnet: CombinedFunctionMagnet) -> None: + devices = self.get_devices_access(magnet.model.get_device_names()) + currents = RWHardwareArray(magnet.model, devices) + strengths = RWStrengthArray(magnet.model, devices) + attached_magnets = magnet.attach(self, strengths, currents) + self.combined_function_magnet.add(attached_magnets[0]) + for virtual_magnet in attached_magnets[1:]: + self.magnet.add(virtual_magnet) + + def _fill_serialized_magnets(self, magnets: SerializedMagnets) -> None: + devices = self.get_devices_access(magnets.model.get_device_names()) + currents = [] + strengths = [] + for index in range(magnets.get_nb_magnets()): + currents.append( + RWHardwareScalar(magnets.model.get_sub_model(index), devices[index]) if magnets.model.has_hardware() else None + ) + strengths.append( + RWStrengthScalar(magnets.model.get_sub_model(index), devices[index]) if magnets.model.has_physics() else None + ) + attached_magnets = magnets.attach(self, strengths, currents) + self.serialized_magnet.add(attached_magnets[0]) + for magnet in attached_magnets[1:]: + self.magnet.add(magnet) + + def _fill_bpm(self, bpm: BPM) -> None: + position_devices = self.get_devices_access(bpm.get_pos_devices()) + tilt_devices = self.get_devices_access([bpm.get_tilt_device()]) + offset_devices = self.get_devices_access(bpm.get_offset_devices()) + positions = RBpmArray(position_devices[0], position_devices[1]) + tilt = RWBpmTiltScalar(tilt_devices[0]) + offsets = RWBpmOffsetArray(offset_devices[0], offset_devices[1]) + self.bpm.add(bpm.attach(self, positions, offsets, tilt)) + + def _fill_rf_plant(self, rf_plant: RFPlant) -> None: + attached_transmitters: list[RFTransmitter] = [] + if rf_plant.transmitters: + for transmitter in rf_plant.transmitters: + voltage_device = self.get_device_access(transmitter.voltage_name) + phase_device = self.get_device_access(transmitter.phase_name) + voltage = RWRFVoltageScalar(transmitter, voltage_device) + phase = RWRFPhaseScalar(transmitter, phase_device) + attached_transmitter = transmitter.attach(self, voltage, phase) + self.rf.transmitter.add(attached_transmitter) + attached_transmitters.append(attached_transmitter) + frequency_device = self.get_device_access(rf_plant.masterclock) + frequency = RWRFFrequencyScalar(rf_plant, frequency_device) + voltage = RWTotalVoltage(attached_transmitters) if rf_plant.transmitters else None + self.rf.add(rf_plant.attach(self, frequency, voltage)) + + def _fill_betatron_tune_monitor(self, monitor: BetatronTuneMonitor) -> None: + devices = self.get_devices_access([monitor.tune_h, monitor.tune_v]) + self.add_betatron_tune_monitor(monitor.attach(self, RBetatronTuneArray(monitor, devices))) + + def _fill_tool(self, tool: TuningTool | MeasurementTool) -> None: + self.add_tool(tool.attach(self)) + + def _fill_unbound_element(self, element: UnboundElement) -> None: + if self.name() not in element._control_modes: + return + attached_element = element.instantiate(self) + if isinstance(attached_element, ABetatronTuneMonitor): + self.add_betatron_tune_monitor(attached_element) + else: + self.add_element(attached_element) class ControlSystemAdapter(ControlSystem): """ - Control system adapter class + Provide a no-op adapter for serialized or backend-independent access. + + Methods + ------- + name() + Return the adapter's control-system name. + get_aggregator() + Return ``None`` because the adapter has no device aggregator. + get_device_access(ref) + Return the device access object for a backend reference. """ def __init__(self): + """ + Initialize the ControlSystemAdapter. + """ ControlSystem.__init__(self) - def attach(self, dev: list[DeviceAccess]) -> list[DeviceAccess]: - pass - - def attach_array(self, dev: list[DeviceAccess]) -> list[DeviceAccess]: - pass - def name(self) -> str: + """Return the adapter's control-system name.""" pass - def scalar_aggregator(self) -> str | None: + def get_aggregator(self) -> DeviceAccessList | None: + """Return ``None`` because the adapter has no device aggregator.""" return None - def vector_aggregator(self) -> str | None: - return None + def get_device_access(self, ref: str | BaseModel | None) -> DeviceAccess | None: + """ + Return the device access object for a backend reference. + + Parameters + ---------- + ref : str | BaseModel | None + Backend-specific device reference. + + Returns + ------- + DeviceAccess | None + Resolved device access object, or ``None`` when unsupported. + """ + pass diff --git a/pyaml/control/deviceaccess.py b/pyaml/control/deviceaccess.py index ec37cd4f2..5ac63897d 100644 --- a/pyaml/control/deviceaccess.py +++ b/pyaml/control/deviceaccess.py @@ -1,3 +1,10 @@ +""" +Abstract interface for control-system device access. + +Backends implement :class:`DeviceAccess` to expose device names, setpoints, +readbacks, units, limits, and availability through a common PyAML interface. +""" + from abc import ABCMeta, abstractmethod # TODO: correctly type value @@ -5,42 +12,110 @@ class DeviceAccess(metaclass=ABCMeta): """ - Abstract class providing access to a control system variable + Define the interface for one control-system device variable. + + Implementations may represent a process variable, power-supply channel, + measurement channel, or another backend-specific device. ``get`` and + ``readback`` distinguish the requested setpoint from the measured value. + + Methods + ------- + name() + Return the backend identifier of the device variable. + measure_name() + Return the identifier of the device's measurement channel. + set(value) + Write a new setpoint to the device variable. + set_and_wait(value) + Write a setpoint and wait until the device reaches it. + get() + Return the current device setpoint. + readback() + Return the latest measured value reported by the device. + unit() + Return the physical unit of the device variable. + get_range() + Get the valid range for the device variable. + check_device_availability() + Check if the device is available and accessible. """ @abstractmethod def name(self) -> str: - """Return the name of the variable""" + """ + Return the backend identifier of the device variable. + + Returns + ------- + str + Device or process-variable name. + """ pass @abstractmethod def measure_name(self) -> str: - """Return the name of the measure""" + """ + Return the identifier of the device's measurement channel. + + Returns + ------- + str + Measurement-channel name. + """ pass @abstractmethod def set(self, value): - """Write a control system device variable (i.e. a power supply current)""" + """ + Write a new setpoint to the device variable. + + Parameters + ---------- + value : object + Backend-compatible value to write. + """ pass @abstractmethod def set_and_wait(self, value): - """Write a control system device variable (i.e. a power supply current)""" + """ + Write a setpoint and wait until the device reaches it. + + Parameters + ---------- + value : object + Backend-compatible value to write. + """ pass @abstractmethod def get(self): - """Return the setpoint(s) of a control system device variable""" + """Return the current device setpoint.""" pass @abstractmethod def readback(self): - """Return the measured variable""" + """ + Return the latest measured value reported by the device. + + Returns + ------- + object + Backend-provided readback value, which may differ from the + commanded setpoint returned by :meth:`get`. + """ pass @abstractmethod def unit(self) -> str: - """Return the variable unit""" + """ + Return the physical unit of the device variable. + + Returns + ------- + str + Unit label, such as ``"A"`` or ``"Hz"``. + """ pass @abstractmethod @@ -51,7 +126,8 @@ def get_range(self) -> list[float]: Returns ------- list[float] - List containing [min, max] values + Two-element list containing the inclusive minimum and maximum + values. ``None`` may be used for an unbounded limit. """ pass @@ -63,6 +139,6 @@ def check_device_availability(self) -> bool: Returns ------- bool - True if device is available, False otherwise + ``True`` if the device can be accessed; otherwise ``False``. """ pass diff --git a/pyaml/control/deviceaccesslist.py b/pyaml/control/deviceaccesslist.py index e913389ec..38513fee8 100644 --- a/pyaml/control/deviceaccesslist.py +++ b/pyaml/control/deviceaccesslist.py @@ -1,51 +1,129 @@ +""" +Abstract collection interface for control-system devices. + +Backends implement :class:`DeviceAccessList` to expose ordered groups of +device variables with bulk read, write, range, unit, and availability support. +""" + from abc import ABCMeta, abstractmethod import numpy as np import numpy.typing as npt from .deviceaccess import DeviceAccess -from .readback_value import Value -class DeviceAccessList(list[DeviceAccess], metaclass=ABCMeta): +class DeviceAccessList(metaclass=ABCMeta): """ - Abstract class providing access to a list of control system float variable + Define ordered bulk access to control-system device variables. + + The internal representation is backend-dependent. Implementations expose + devices in a stable order so array values correspond to the same order for + reads, writes, readbacks, and ranges. + + Methods + ------- + add_devices(devices) + Add one device or a list of devices to the collection. + get_device_at(index) + Return the device at a zero-based index. + len() + Return the number of devices in the collection. + set(value) + Write one setpoint for each device in collection order. + set_and_wait(value) + Write setpoints and wait for all devices to reach them. + get() + Return all current setpoints in collection order. + readback() + Return the latest measured values in collection order. + unit() + Return the unit or units associated with the devices. + get_range() + Get the valid range for the device variables. + check_device_availability() + Check if all devices in the list are available and accessible. """ @abstractmethod def add_devices(self, devices: DeviceAccess | list[DeviceAccess]): - """Add a DeviceAccess to this list""" + """ + Add one device or a list of devices to the collection. + + Parameters + ---------- + devices : DeviceAccess | list[DeviceAccess] + Device or devices to append, in the order they should be read. + """ + pass + + @abstractmethod + def get_device_at(self, index: int) -> DeviceAccess: + """ + Return the device at a zero-based index. + + Parameters + ---------- + index : int + Position of the requested device. + + Returns + ------- + DeviceAccess + Device at ``index``. + """ pass @abstractmethod - def get_devices(self) -> DeviceAccess | list[DeviceAccess]: - """Get the DeviceAccess list""" + def len(self) -> int: + """Return the number of devices in the collection.""" pass @abstractmethod def set(self, value: npt.NDArray[np.float64]): - """Write a list of control system device variable - (i.e. a power supply currents)""" + """ + Write one setpoint for each device in collection order. + + Parameters + ---------- + value : numpy.typing.NDArray[numpy.float64] + Setpoints ordered to match the devices. + """ pass @abstractmethod def set_and_wait(self, value: npt.NDArray[np.float64]): - """Write a list control system device variable (i.e. a power supply currents)""" + """ + Write setpoints and wait for all devices to reach them. + + Parameters + ---------- + value : numpy.typing.NDArray[numpy.float64] + Setpoints ordered to match the devices. + """ pass @abstractmethod def get(self) -> npt.NDArray[np.float64]: - """Return a list of setpoints of control system device variables""" + """Return all current setpoints in collection order.""" pass @abstractmethod def readback(self) -> np.array: - """Return the measured variables""" + """ + Return the latest measured values in collection order. + + Returns + ------- + numpy.ndarray + Readback values corresponding to the devices returned by + :meth:`get_device_at` at each index. + """ pass @abstractmethod def unit(self) -> str: - """Return the variable unit""" + """Return the unit or units associated with the devices.""" pass @abstractmethod @@ -56,7 +134,8 @@ def get_range(self) -> list[float]: Returns ------- list[float] - List containing [min, max] values + Flat list containing ``[min0, max0, min1, max1, ...]``. + ``None`` may represent an unbounded limit. """ pass @@ -68,6 +147,48 @@ def check_device_availability(self) -> bool: Returns ------- bool - True if all devices are available, False otherwise + ``True`` only if every device is available and accessible. """ pass + + # Immutable list implementation + + def __getitem__(self, index): + """ + Return the device at ``index``. + + Parameters + ---------- + index : object + Integer index of the requested device. + + Returns + ------- + DeviceAccess + Device selected by ``index``. + """ + return self.get_device_at(index) + + def __len__(self): + """Return the number of devices in the collection.""" + return self.len() + + def __iter__(self): + """Return an iterator over the devices in collection order.""" + self._iter_pos = 0 + return self + + def __next__(self): + """ + Return the next device during iteration. + + Raises + ------ + StopIteration + When all devices have been visited. + """ + if self._iter_pos < len(self._items): + self._iter_pos += 1 + return self._items[self._iter_pos - 1] + else: + raise StopIteration diff --git a/pyaml/control/readback_value.py b/pyaml/control/readback_value.py index 207641c35..71f3713cf 100644 --- a/pyaml/control/readback_value.py +++ b/pyaml/control/readback_value.py @@ -1,3 +1,10 @@ +""" +Values returned by control-system readback channels. + +The module provides quality indicators and a :class:`Value` wrapper that keeps +the measured value together with its quality state and acquisition timestamp. +""" + from datetime import datetime from enum import Enum, auto from typing import Union @@ -7,20 +14,20 @@ class Quality(Enum): """ - Enumeration for data quality indicators. + Describe the quality state associated with a readback value. Attributes ---------- VALID : int - Data is valid and reliable + Data is valid and reliable. INVALID : int - Data is invalid + Data is invalid. ALARM : int - Data indicates an alarm condition + Data indicates an alarm condition. CHANGING : int - Data is currently changing + Data is currently changing. WARNING : int - Data indicates a warning condition + Data indicates a warning condition. """ VALID = auto() @@ -30,6 +37,9 @@ class Quality(Enum): WARNING = auto() def __str__(self): + """ + Return a human-readable string representation of the object. + """ return self.name @@ -48,6 +58,11 @@ class Value: The quality of the value. Defaults to Quality.VALID. timestamp : datetime, optional Timestamp associated with the value. Defaults to current time. + + Methods + ------- + is_good() + Check if the value quality is good. """ def __init__( @@ -56,6 +71,9 @@ def __init__( quality: Quality = Quality.VALID, timestamp: datetime = None, ): + """ + Initialize a value with quality metadata and an acquisition time. + """ self.value = value self.quality = quality self.timestamp = timestamp or datetime.now() diff --git a/pyaml/diagnostics/__init__.py b/pyaml/diagnostics/__init__.py new file mode 100644 index 000000000..e69de29bb diff --git a/pyaml/diagnostics/atune_monitor.py b/pyaml/diagnostics/atune_monitor.py index 86698538e..9c9afb9a6 100644 --- a/pyaml/diagnostics/atune_monitor.py +++ b/pyaml/diagnostics/atune_monitor.py @@ -1,3 +1,10 @@ +""" +Abstract interfaces for betatron tune monitors. + +The interfaces describe the tune and frequency quantities exposed by concrete +betatron tune monitor implementations. +""" + from abc import ABCMeta, abstractmethod from ..common.abstract import ReadFloatArray @@ -5,14 +12,30 @@ class ABetatronTuneMonitor(metaclass=ABCMeta): """ - Abstract class providing access to a betatron tune monitor + Define the read-only interface for a betatron tune monitor. + + Concrete monitors provide horizontal and vertical tune values and their + corresponding frequencies. + + Attributes + ---------- + tune + Return the fractional horizontal and vertical betatron tunes. + frequency + Return the horizontal and vertical tune frequencies. """ @property @abstractmethod def tune(self) -> ReadFloatArray: """ - Returns the tune fractionnal part + Return the fractional horizontal and vertical betatron tunes. + + Returns + ------- + ReadFloatArray + Readable array containing the horizontal and vertical tune + fractions. """ ... @@ -20,6 +43,12 @@ def tune(self) -> ReadFloatArray: @abstractmethod def frequency(self) -> ReadFloatArray: """ - Returns the tune in frequency + Return the horizontal and vertical tune frequencies. + + Returns + ------- + ReadFloatArray + Readable array containing the frequencies corresponding to the + tune measurements. """ ... diff --git a/pyaml/diagnostics/tune_monitor.py b/pyaml/diagnostics/tune_monitor.py index 1a534c1ce..3b5206d77 100644 --- a/pyaml/diagnostics/tune_monitor.py +++ b/pyaml/diagnostics/tune_monitor.py @@ -1,62 +1,110 @@ +""" +Betatron tune monitor element and runtime data bindings. + +The monitor identifies tune measurements, attaches them to a runtime peer, +and optionally converts tune fractions to frequencies using an RF plant. +""" + +import copy +from typing import TYPE_CHECKING, Self + +from numpy.typing import NDArray + from ..common.abstract import ReadFloatArray -from ..common.element import Element, ElementConfigModel -from ..control.deviceaccess import DeviceAccess +from ..common.element import Element, __pyaml_repr__ +from ..validation import DynamicValidation, register_schema from .atune_monitor import ABetatronTuneMonitor -try: - from typing import Self # Python 3.11+ -except ImportError: - from typing_extensions import Self # Python 3.10 and earlier -import numpy as np -from pydantic import ConfigDict +if TYPE_CHECKING: + from ..common.holders.element_holder import ElementHolder PYAMLCLASS = "BetatronTuneMonitor" -class ConfigModel(ElementConfigModel): +@register_schema +class BetatronTuneMonitor(Element, DynamicValidation, ABetatronTuneMonitor): """ - Configuration model for BetatronTuneMonitor + Betatron tune monitor. + + Represents a betatron tune monitor in the accelerator lattice and + provides access to the measured horizontal and vertical betatron + tunes. Optionally, the monitor can be associated with an RF plant + used to convert tune measurements to frequency values. Parameters ---------- - tune_h : DeviceAccess, optional - Horizontal betatron tune device - tune_v : DeviceAccess, optional - Vertical betatron tune device + name : str + Name of the betatron tune monitor. + description : str | None, optional + Description of the monitor. + tune_h : str | None, optional + Device catalog key for the horizontal betatron tune measurement. + tune_v : str | None, optional + Device catalog key for the vertical betatron tune measurement. + rf_plant_name : str | None, optional + Name of the associated RF plant element used by the monitor. + + Attributes + ---------- + tune_h + Return the horizontal tune device catalog key. + tune_v + Return the vertical tune device catalog key. + tune + Get the betatron tune values. + frequency + Return the betatron tune values converted to frequency. + + Methods + ------- + set_harmonic(h) + Set the harmonic number used for tune-frequency conversion. + attach(peer, betatron_tune) + Attach the tune monitor to a peer with betatron tune data. """ - model_config = ConfigDict(arbitrary_types_allowed=True, extra="forbid") - - tune_h: DeviceAccess | None - tune_v: DeviceAccess | None - rf_plant_name: str | None = None - - -class BetatronTuneMonitor(Element, ABetatronTuneMonitor): - """ - Class providing access to a betatron tune monitor - of a physical or simulated lattice. - The monitor provides horizontal and vertical betatron tune measurements. - """ + def __init__( + self, + name: str, + description: str | None = None, + tune_h: str | None = None, + tune_v: str | None = None, + rf_plant_name: str | None = None, + ): + """ + Initialize a betatron tune monitor. + """ + super().__init__(name, None, description) + self._tune_h = tune_h + self._tune_v = tune_v + self._rf_plant_name = rf_plant_name + self.__tune = None + self._h = None - def __init__(self, cfg: ConfigModel): + def set_harmonic(self, h: int): """ - Construct a BetatronTuneMonitor + Set the harmonic number used for tune-frequency conversion. Parameters ---------- - cfg : ConfigModel - Configuration for the BetatronTuneMonitor, including - device access for horizontal and vertical tunes. + h : int + Harmonic number relating the RF frequency to the measured + betatron tune frequency. """ + self._h = float(h) - super().__init__(cfg.name) - self._cfg = cfg - self.__tune = None - self._h = None + def _fill_device(self, holder: "ElementHolder") -> None: + holder._fill_betatron_tune_monitor(self) - def set_harmonic(self, h: int): - self._h = float(h) + @property + def tune_h(self) -> str | None: + """Return the horizontal tune device catalog key.""" + return self._tune_h + + @property + def tune_v(self) -> str | None: + """Return the vertical tune device catalog key.""" + return self._tune_v @property def tune(self) -> ReadFloatArray: @@ -66,7 +114,7 @@ def tune(self) -> ReadFloatArray: Returns ------- ReadFloatArray - Array of tune values [horizontal, vertical] + Readable array containing the horizontal and vertical tunes. """ self.check_peer() return self.__tune @@ -74,28 +122,49 @@ def tune(self) -> ReadFloatArray: @property def frequency(self) -> ReadFloatArray: """ - Get the betatron tune values in frequency + Return the betatron tune values converted to frequency. Returns ------- ReadFloatArray - Array of tune values in frequency [horizontal, vertical] + Readable array containing horizontal and vertical frequencies. """ class TuneFreq(ReadFloatArray): + """ + Read-only view that converts tune values to frequencies. + + Parameters + ---------- + parent : BetatronTuneMonitor + Monitor providing the source tune and RF data. + + Methods + ------- + get() + Return tune frequencies in hertz. + unit() + Return the frequency unit label. + """ + def __init__(self, parent: BetatronTuneMonitor): + """ + Initialize the tune-frequency view. + """ self.parent = parent - def get(self) -> np.array: + def get(self) -> NDArray: + """Return tune frequencies in hertz.""" h = self.parent._h - rf_name = self.parent._cfg.rf_plant_name + rf_name = self.parent._rf_plant_name if h is not None and rf_name is not None: tune = self.parent.tune.get() - rf = self.parent.peer.get_rf_plant(rf_name) + rf = self.parent.peer.rf.get(rf_name) freq = rf.frequency.get() return tune * freq / h def unit(self) -> str: + """Return the frequency unit label.""" return "Hz" self.check_peer() @@ -108,16 +177,24 @@ def attach(self, peer, betatron_tune: ReadFloatArray) -> Self: Parameters ---------- peer : object - The peer object (simulator or control system) + Simulator or control-system peer providing the RF plant. betatron_tune : ReadFloatArray - The betatron tune array to monitor + Readable array containing the measured horizontal and vertical + tunes. Returns ------- Self - A new attached instance of TuneMonitor + A shallow copy of this monitor bound to ``peer`` and + ``betatron_tune``. """ - obj = self.__class__(self._cfg) + obj = copy.copy(self) obj.__tune = betatron_tune obj._peer = peer return obj + + def __repr__(self): + """ + Implement the ``__repr__`` string. + """ + return __pyaml_repr__(self, exclude=["tune", "frequency"]) diff --git a/pyaml/external/__init__.py b/pyaml/external/__init__.py new file mode 100644 index 000000000..e69de29bb diff --git a/pyaml/external/pySC_interface.py b/pyaml/external/pySC_interface.py index c553fd1e8..3be5196ea 100644 --- a/pyaml/external/pySC_interface.py +++ b/pyaml/external/pySC_interface.py @@ -1,15 +1,49 @@ +""" +Adapter between PyAML elements and pySC measurement applications. + +The :class:`pySCInterface` exposes the orbit, magnet-strength, and RF-frequency +operations expected by pySC while using PyAML element-holder accessors. +""" + import time from typing import TYPE_CHECKING, Optional, Tuple import numpy as np if TYPE_CHECKING: - from ..common.element_holder import ElementHolder + from ..common.holders.element_holder import ElementHolder from ..common.exception import PyAMLException class pySCInterface: + """ + Provide pySC-compatible access to a PyAML accelerator mode. + + Parameters + ---------- + element_holder : 'ElementHolder' + Accelerator mode, control system or simulator, exposed to pySC. + bpm_array_name : str + Name of the BPM array used for orbit readback. + rf_plant_name : Optional[str] + Optional RF plant name, required for RF-related pySC operations. + + Methods + ------- + get_orbit() + Return horizontal and vertical orbit readings from the BPM array. + get(name) + Return the current strength of a named magnet. + set(name, value) + Set the strength of a named magnet and wait for the configured delay. + get_rf_main_frequency() + Return the main RF frequency from the configured RF plant. + set_rf_main_frequency(value) + Set the main RF frequency and wait for the configured delay. + """ + set_wait_time: float = 0 + read_wait_time: float = 0 def __init__( self, @@ -17,37 +51,83 @@ def __init__( bpm_array_name: str, rf_plant_name: Optional[str] = None, ): + """ + Initialize a pySC adapter from a PyAML element holder. + """ self.element_holder = element_holder - self.bpm_array = element_holder.get_bpms(bpm_array_name) + self.bpm_array = element_holder.bpms.get(bpm_array_name) self.rf_plant_name = rf_plant_name if rf_plant_name is not None: - self.rf_plant = element_holder.get_rf_plant(self.rf_plant_name) + self.rf_plant = element_holder.rf.get(self.rf_plant_name) else: self.rf_plant = None def get_orbit(self) -> Tuple[np.array, np.array]: - # we should wait here somehow according to polling rate + """Return horizontal and vertical orbit readings from the BPM array.""" + time.sleep(self.read_wait_time) positions = self.bpm_array.positions.get() return positions[:, 0], positions[:, 1] def get(self, name: str) -> float: - magnet = self.element_holder.get_magnet(name=name) + """ + Return the current strength of a named magnet. + + Parameters + ---------- + name : str + Magnet name in the configured element holder. + + Returns + ------- + float + Current magnet strength. + """ + magnet = self.element_holder.magnet.get(name=name) return magnet.strength.get() def set(self, name: str, value: float) -> None: - magnet = self.element_holder.get_magnet(name=name) + """ + Set the strength of a named magnet and wait for the configured delay. + + Parameters + ---------- + name : str + Magnet name in the configured element holder. + value : float + New magnet strength. + + Returns + ------- + None + This method does not return a value. + """ + magnet = self.element_holder.magnet.get(name=name) magnet.strength.set(value=value) # ideally set_and_wait but not implemented time.sleep(self.set_wait_time) return def get_rf_main_frequency(self) -> float: + """Return the main RF frequency from the configured RF plant.""" if self.rf_plant is None: raise PyAMLException("RF plant name was not provided.") return self.rf_plant.frequency.get() def set_rf_main_frequency(self, value: float) -> None: + """ + Set the main RF frequency and wait for the configured delay. + + Parameters + ---------- + value : float + New main RF frequency in hertz. + + Returns + ------- + None + This method does not return a value. + """ if self.rf_plant is None: raise PyAMLException("RF plant name was not provided.") self.rf_plant.frequency.set(value) diff --git a/pyaml/lattice/abstract_impl.py b/pyaml/lattice/abstract_impl.py index 69354e912..91c07975e 100644 --- a/pyaml/lattice/abstract_impl.py +++ b/pyaml/lattice/abstract_impl.py @@ -1,3 +1,10 @@ +""" +Read/write interfaces for simulated lattice elements. + +This module adapts Accelerator Toolbox lattice elements to PyAML accessors for +magnet strengths, hardware values, BPM readings, RF parameters, and tune data. +""" + import at import numpy as np from numpy.typing import NDArray @@ -5,10 +12,7 @@ from ..common import abstract from ..common.abstract_aggregator import ScalarAggregator -from ..common.exception import PyAMLException from ..magnet.model import MagnetModel -from ..rf.rf_plant import RFPlant -from ..rf.rf_transmitter import RFTransmitter from .polynom_info import PolynomInfo # TODO handle serialized magnets for magnet array @@ -18,42 +22,97 @@ class RWHardwareScalar(abstract.ReadWriteFloatScalar): """ - Class providing read write access to a magnet of a simulator in hardware unit. - Hardware unit is converted from strength using the magnet model + Provide read/write access to a simulated magnet in hardware units. + + Hardware values are converted through the associated magnet model while + the underlying lattice polynomial is updated on writes. + + Parameters + ---------- + elements : list[at.Element] + Accelerator Toolbox elements making up the magnet; their contributions are summed. + poly : PolynomInfo + Polynomial component driven by this accessor: the ``PolynomA``/``PolynomB`` attribute name, its multipole + index and the sign convention. + model : MagnetModel + Magnet model used to convert between physical strength and hardware value. + + Methods + ------- + get_length() + Return the total length of the lattice elements. + get() + Return the current value. + set(value) + Set the current value. + set_and_wait(value) + Set the value and wait for readback convergence. + unit() + Return the value unit. + get_model() + Return the associated magnet model. """ def __init__(self, elements: list[at.Element], poly: PolynomInfo, model: MagnetModel): - self.__model = model - self.__elements = elements - self.__poly = [e.__getattribute__(poly.attName) for e in elements] - self.__sign = poly.sign - self.__polyIdx = poly.index - self.__length: float = 0.0 + """ + Initialize the RWHardwareScalar. + """ + self._model = model + self._elements = elements + self._poly = [e.__getattribute__(poly.attName) for e in elements] + self._sign = poly.sign + self._polyIdx = poly.index + self._length: float = 0.0 for e in elements: - self.__length += e.Length + self._length += e.Length def get_length(self) -> float: - return self.__length + """Return the total length of the lattice elements.""" + return self._length def get(self) -> float: + """Return the current value.""" s = 0 - for idx, e in enumerate(self.__elements): - s += self.__poly[idx][self.__polyIdx] * self.__sign * e.Length - return self.__model.compute_hardware_values([s])[0] + for idx, e in enumerate(self._elements): + s += self._poly[idx][self._polyIdx] * self._sign * e.Length + return self._model.compute_hardware_values([s])[0] def set(self, value: float): - s = self.__model.compute_strengths([value])[0] - for idx, _ in enumerate(self.__elements): - self.__poly[idx][self.__polyIdx] = s / (self.__length * self.__sign) + """ + Set the current value. + + Parameters + ---------- + value : float + Hardware value to apply, in the unit reported by the magnet model. + """ + s = self._model.compute_strengths([value])[0] + for idx, _ in enumerate(self._elements): + self._poly[idx][self._polyIdx] = s / (self._length * self._sign) def set_and_wait(self, value: float): + """ + Set the value and wait for readback convergence. + + Parameters + ---------- + value : float + Hardware value to apply, in the unit reported by the magnet model. + + Raises + ------ + NotImplementedError + Waiting for readback convergence is not implemented for this accessor. + """ raise NotImplementedError("Not implemented yet.") def unit(self) -> str: - return self.__model.get_hardware_units()[0] + """Return the value unit.""" + return self._model.get_hardware_units()[0] def get_model(self) -> MagnetModel: - return self.__model + """Return the associated magnet model.""" + return self._model # ------------------------------------------------------------------------------ @@ -61,52 +120,175 @@ def get_model(self) -> MagnetModel: class RWStrengthScalar(abstract.ReadWriteFloatScalar): """ - Class providing read write access to a strength of a simulator + Provide read/write access to a simulated magnet strength. + + The accessor aggregates the selected lattice polynomial over all mapped + elements and distributes writes across those elements. + + Parameters + ---------- + elements : list[at.Element] + Accelerator Toolbox elements making up the magnet; their contributions are summed. + poly : PolynomInfo + Polynomial component driven by this accessor: the ``PolynomA``/``PolynomB`` attribute name, its multipole + index and the sign convention. + model : MagnetModel + Magnet model used to convert between physical strength and hardware value. + + Methods + ------- + get_element_length() + Return the total length of the represented element. + get(polynom=None, polyidx=None) + Return the current value. + set(value, polynom=None, polyidx=None) + Set the current value. + set_and_wait(value) + Set the value and wait for readback convergence. + unit() + Return the value unit. + get_model() + Return the associated magnet model. """ def __init__(self, elements: list[at.Element], poly: PolynomInfo, model: MagnetModel): - self.__model = model - self.__elements = elements - self.__poly = [e.__getattribute__(poly.attName) for e in elements] - self.__sign = poly.sign - self.__polyIdx = poly.index - self.__length = 0 + """ + Initialize the RWStrengthScalar. + """ + self._model = model + self._elements = elements + self._poly = [e.__getattribute__(poly.attName) for e in elements] + self._sign = poly.sign + self._polyIdx = poly.index + self._length = 0 for e in elements: - self.__length += e.Length + self._length += e.Length def get_element_length(self) -> float: - return self.__length + """Return the total length of the represented element.""" + return self._length # Gets the value - def get(self) -> float: + def get(self, polynom: str = None, polyidx: int = None) -> float: + """ + Return the current value. + + Parameters + ---------- + polynom : str + Lattice polynomial to address, ``"PolynomA"`` or ``"PolynomB"``. Defaults to the component configured for + this accessor. + polyidx : int + Multipole index within ``polynom``. Only used when ``polynom`` is given. + + Returns + ------- + float + Integrated strength summed over the lattice elements. + """ + if polynom is None: + pIdx = self._polyIdx + poly = self._poly + else: + # Override strength access + pIdx = polyidx + poly = [e.__getattribute__(polynom) for e in self._elements] + s = 0 - for idx, e in enumerate(self.__elements): - s += self.__poly[idx][self.__polyIdx] * self.__sign * e.Length + for idx, e in enumerate(self._elements): + s += poly[idx][pIdx] * self._sign * e.Length return s # Sets the value - def set(self, value: float): - for idx, _ in enumerate(self.__elements): - self.__poly[idx][self.__polyIdx] = value / (self.__length * self.__sign) + def set(self, value: float, polynom: str = None, polyidx: int = None): + """ + Set the current value. + + Parameters + ---------- + value : float + Integrated strength to apply, distributed over the lattice elements. + polynom : str + Lattice polynomial to address, ``"PolynomA"`` or ``"PolynomB"``. Defaults to the component configured for + this accessor. + polyidx : int + Multipole index within ``polynom``. Only used when ``polynom`` is given. + """ + if polynom is None: + pIdx = self._polyIdx + poly = self._poly + else: + # Override strength access + pIdx = polyidx + poly = [e.__getattribute__(polynom) for e in self._elements] + + for idx, _ in enumerate(self._elements): + poly[idx][pIdx] = value / (self._length * self._sign) # Sets the value and wait that the read value reach the setpoint def set_and_wait(self, value: float): + """ + Set the value and wait for readback convergence. + + Parameters + ---------- + value : float + Integrated strength to apply, distributed over the lattice elements. + + Raises + ------ + NotImplementedError + Waiting for readback convergence is not implemented for this accessor. + """ raise NotImplementedError("Not implemented yet.") # Gets the unit of the value def unit(self) -> str: - return self.__model.get_strength_units()[0] + """Return the value unit.""" + return self._model.get_strength_units()[0] # ------------------------------------------------------------------------------ def get_model(self) -> MagnetModel: - return self.__model + """Return the associated magnet model.""" + return self._model # ------------------------------------------------------------------------------ class RWSerializedHardware(abstract.ReadWriteFloatScalar): + """ + RWSerializedHardware configuration or runtime object. + + Parameters + ---------- + elements : list[RWHardwareScalar] + Hardware accessors of the magnets sharing the serialized power supply. + element_index : int + Index of the magnet this accessor represents within the serialized group. + + Methods + ------- + get_element_length() + Return the total length of the represented element. + get_total_length() + Return the total length of the represented elements. + get() + Return the current value. + set(value) + Set the current value. + set_and_wait(value) + Set the value and wait for readback convergence. + unit() + Return the value unit. + set_magnet_rigidity(brho) + Set the magnetic rigidity used for conversion. + """ + def __init__(self, elements: list[RWHardwareScalar], element_index: int): + """ + Initialize the RWSerializedHardware. + """ self.__elements = elements self.__element_index = element_index self.__total_length = 0 @@ -114,38 +296,104 @@ def __init__(self, elements: list[RWHardwareScalar], element_index: int): self.__total_length += e.get_length() def get_element_length(self) -> float: + """Return the total length of the represented element.""" return self.__elements[self.__element_index].get_length() def get_total_length(self) -> float: + """Return the total length of the represented elements.""" return self.__total_length # Gets the value def get(self) -> float: + """Return the current value.""" return self.__elements[self.__element_index].get() # Sets the value def set(self, value: float): + """ + Set the current value. + + Parameters + ---------- + value : float + Hardware value to apply to the whole serialized group. + """ [element.set(value) for element in self.__elements] # Sets the value and wait that the read value reach the setpoint def set_and_wait(self, value: float): + """ + Set the value and wait for readback convergence. + + Parameters + ---------- + value : float + Hardware value to apply to the whole serialized group. + + Raises + ------ + NotImplementedError + Waiting for readback convergence is not implemented for this accessor. + """ raise NotImplementedError("Not implemented yet.") # Gets the unit of the value def unit(self) -> str: + """Return the value unit.""" return self.__elements[self.__element_index].unit() def set_magnet_rigidity(self, brho: np.double): + """ + Set the magnetic rigidity used for conversion. + + Parameters + ---------- + brho : np.double + Magnetic rigidity in tesla metres, used to convert strengths to hardware values. + """ [element.get_model().set_magnet_rigidity(brho) for element in self.__elements] class RWSerializedStrength(abstract.ReadWriteFloatScalar): + """ + RWSerializedStrength configuration or runtime object. + + Parameters + ---------- + elements_strength : list[RWStrengthScalar] + Strength accessors of the magnets sharing the serialized power supply. + elements_hardware : list[RWHardwareScalar] + Hardware accessors of the same magnets, used to apply the shared setpoint. + element_index : int + Index of the magnet this accessor represents within the serialized group. + + Methods + ------- + get_element_length() + Return the total length of the represented element. + get_total_length() + Return the total length of the represented elements. + get() + Return the current value. + set(value) + Set the current value. + set_and_wait(value) + Set the value and wait for readback convergence. + unit() + Return the value unit. + set_magnet_rigidity(brho) + Set the magnetic rigidity used for conversion. + """ + def __init__( self, elements_strength: list[RWStrengthScalar], elements_hardware: list[RWHardwareScalar], element_index: int, ): + """ + Initialize the RWSerializedStrength. + """ self.__element = elements_strength[element_index] self.__elements_strength = elements_strength self.__elements_hardware = elements_hardware @@ -155,17 +403,28 @@ def __init__( self.__total_length += e.get_length() def get_element_length(self) -> float: + """Return the total length of the represented element.""" return self.__element.get_element_length() def get_total_length(self) -> float: + """Return the total length of the represented elements.""" return self.__total_length # Gets the value def get(self) -> float: + """Return the current value.""" return self.__elements_strength[self.__element_index].get() # Sets the value def set(self, value: float): + """ + Set the current value. + + Parameters + ---------- + value : float + Strength to apply to the magnet, converted to the shared hardware setpoint. + """ elements_values = [value * e.get_length() / self.get_total_length() for e in self.__elements_hardware] self.__element.set(elements_values[self.__element_index]) @@ -182,13 +441,35 @@ def set(self, value: float): # Sets the value and wait that the read value reach the setpoint def set_and_wait(self, value: float): + """ + Set the value and wait for readback convergence. + + Parameters + ---------- + value : float + Strength to apply to the magnet, converted to the shared hardware setpoint. + + Raises + ------ + NotImplementedError + Waiting for readback convergence is not implemented for this accessor. + """ raise NotImplementedError("Not implemented yet.") # Gets the unit of the value def unit(self) -> str: + """Return the value unit.""" return self.__element.unit() def set_magnet_rigidity(self, brho: np.double): + """ + Set the magnetic rigidity used for conversion. + + Parameters + ---------- + brho : np.double + Magnetic rigidity in tesla metres, used to convert strengths to hardware values. + """ pass @@ -196,9 +477,33 @@ class RWHardwareArray(abstract.ReadWriteFloatArray): """ Class providing read write access to a magnet of a simulator in hardware units. Hardware units are converted from strengths using the magnet model + + Parameters + ---------- + elements : list[at.Element] + Accelerator Toolbox elements of every magnet in the array. + poly : list[PolynomInfo] + Polynomial component for each magnet, giving the ``PolynomA``/``PolynomB`` attribute name, multipole index + and sign convention. + model : MagnetModel + Magnet model used to convert between physical strength and hardware value. + + Methods + ------- + get() + Return the current value. + set(value) + Set the current value. + set_and_wait(value) + Set the value and wait for readback convergence. + unit() + Return the value unit. """ def __init__(self, elements: list[at.Element], poly: list[PolynomInfo], model: MagnetModel): + """ + Initialize the RWHardwareArray. + """ self.__elements = elements self.__poly = [] self.__polyIdx = [] @@ -211,6 +516,7 @@ def __init__(self, elements: list[at.Element], poly: list[PolynomInfo], model: M # Gets the value def get(self) -> np.array: + """Return the current value.""" nbStrength = len(self.__poly) s = np.zeros(nbStrength) for i in range(nbStrength): @@ -219,6 +525,14 @@ def get(self) -> np.array: # Sets the value def set(self, value: np.array): + """ + Set the current value. + + Parameters + ---------- + value : np.array + Hardware values to apply, one per magnet and ordered like the array. + """ nbStrength = len(self.__poly) s = self.__model.compute_strengths(value) for i in range(nbStrength): @@ -226,10 +540,24 @@ def set(self, value: np.array): # Sets the value and wait that the read value reach the setpoint def set_and_wait(self, value: np.array): + """ + Set the value and wait for readback convergence. + + Parameters + ---------- + value : np.array + Hardware values to apply, one per magnet and ordered like the array. + + Raises + ------ + NotImplementedError + Waiting for readback convergence is not implemented for this accessor. + """ raise NotImplementedError("Not implemented yet.") # Gets the unit of the value def unit(self) -> list[str]: + """Return the value unit.""" return self.__model.get_hardware_units() @@ -239,9 +567,33 @@ def unit(self) -> list[str]: class RWStrengthArray(abstract.ReadWriteFloatArray): """ Class providing read write access to a strength (array) of a simulator + + Parameters + ---------- + elements : list[at.Element] + Accelerator Toolbox elements of every magnet in the array. + poly : list[PolynomInfo] + Polynomial component for each magnet, giving the ``PolynomA``/``PolynomB`` attribute name, multipole index + and sign convention. + model : MagnetModel + Magnet model used to convert between physical strength and hardware value. + + Methods + ------- + get() + Return the current value. + set(value) + Set the current value. + set_and_wait(value) + Set the value and wait for readback convergence. + unit() + Return the value unit. """ def __init__(self, elements: list[at.Element], poly: list[PolynomInfo], model: MagnetModel): + """ + Initialize the RWStrengthArray. + """ self.__elements = elements self.__poly = [] self.__polyIdx = [] @@ -254,6 +606,7 @@ def __init__(self, elements: list[at.Element], poly: list[PolynomInfo], model: M # Gets the value def get(self) -> np.array: + """Return the current value.""" nbStrength = len(self.__poly) s = np.zeros(nbStrength) for i in range(nbStrength): @@ -262,6 +615,14 @@ def get(self) -> np.array: # Sets the value def set(self, value: np.array): + """ + Set the current value. + + Parameters + ---------- + value : np.array + Integrated strengths to apply, one per magnet and ordered like the array. + """ nbStrength = len(self.__poly) s = np.zeros(nbStrength) for i in range(nbStrength): @@ -269,10 +630,24 @@ def set(self, value: np.array): # Sets the value and wait that the read value reach the setpoint def set_and_wait(self, value: np.array): + """ + Set the value and wait for readback convergence. + + Parameters + ---------- + value : np.array + Integrated strengths to apply, one per magnet and ordered like the array. + + Raises + ------ + NotImplementedError + Waiting for readback convergence is not implemented for this accessor. + """ raise NotImplementedError("Not implemented yet.") # Gets the unit of the value def unit(self) -> list[str]: + """Return the value unit.""" return self.__model.get_strength_units() @@ -282,43 +657,107 @@ def unit(self) -> list[str]: class BPMScalarAggregator(ScalarAggregator): """ BPM simulator aggregator + + Parameters + ---------- + ring : at.Lattice + Lattice used to resolve element positions into reference points. + + Methods + ------- + add_elem(elem) + Add a lattice element to the aggregate. + set(value) + Set the current value. + set_and_wait(value) + Set the value and wait for readback convergence. + get() + Return the current value. + readback() + Return the current readback value. + unit() + Return the value unit. """ def __init__(self, ring: at.Lattice): - self.lattice = ring - self.refpts = [] + """ + Initialize the BPMScalarAggregator. + """ + self._lattice = ring + self._refpts = [] + self._matrices = [] def add_elem(self, elem: at.Element): - self.refpts.append(self.lattice.index(elem)) + """ + Add a lattice element to the aggregate. + + Parameters + ---------- + elem : at.Element + BPM lattice element to append to the aggregate. + """ + self._refpts.append(self._lattice.index(elem)) + self._matrices.append(elem._transform) def set(self, value: NDArray[np.float64]): + """ + Set the current value. + + Parameters + ---------- + value : NDArray[np.float64] + Ignored. BPM readings derive from the closed orbit and cannot be written. + """ pass def set_and_wait(self, value: NDArray[np.float64]): + """ + Set the value and wait for readback convergence. + + Parameters + ---------- + value : NDArray[np.float64] + Ignored. BPM readings derive from the closed orbit and cannot be written. + """ pass def get(self) -> np.array: - _, orbit = at.find_orbit(self.lattice, refpts=self.refpts) - return orbit[:, [0, 2]].flatten() + """Return the current value.""" + return self._transform().flatten() def readback(self) -> np.array: + """Return the current readback value.""" return self.get() def unit(self) -> str: + """Return the value unit.""" return "m" + def _transform(self) -> np.array: + """Transform the configured value for the lattice interface.""" + _, orbit = at.find_orbit(self._lattice, refpts=self._refpts) + ones = np.ones(len(self._refpts)) + pts = orbit[:, [0, 2]] # Extract x,y + # Batch matrices multiplication (homogeneous coordinates) + return np.matmul(self._matrices, np.column_stack([pts, ones])[:, :, None]).squeeze(-1) + # ------------------------------------------------------------------------------ class BPMHScalarAggregator(BPMScalarAggregator): """ - Vertical BPM simulator aggregator + Horizontal BPM simulator aggregator + + Methods + ------- + get() + Return the current value. """ def get(self) -> np.array: - _, orbit = at.find_orbit(self.lattice, refpts=self.refpts) - return orbit[:, 0] + """Return the current value.""" + return self._transform()[:, 0] # ------------------------------------------------------------------------------ @@ -326,37 +765,86 @@ def get(self) -> np.array: class BPMVScalarAggregator(BPMScalarAggregator): """ - Horizontal BPM simulator aggregator + Vertical BPM simulator aggregator + + Methods + ------- + get() + Return the current value. """ def get(self) -> np.array: - _, orbit = at.find_orbit(self.lattice, refpts=self.refpts) - return orbit[:, 2] + """Return the current value.""" + return self._transform()[:, 1] # ------------------------------------------------------------------------------ +def update_bpm_transform_matrix(element: at.Element): + # BPM transformation matrix (homogeneous coordinates) + """ + Update the coordinate transform for a beam-position monitor. + + The transform combines the BPM element's horizontal and vertical offsets + with its tilt, allowing measured positions to be expressed in the BPM + coordinate system. + + Parameters + ---------- + element : at.Element + BPM lattice element with ``Offset`` and ``Tilt`` attributes. The + resulting matrix is stored on the element as ``_transform``. + """ + tx = element.Offset[0] + ty = element.Offset[1] + cos_theta = np.cos(element.Tilt) + sin_theta = np.sin(element.Tilt) + if not hasattr(element, "_transform"): + element._transform = np.empty((2, 3)) + element._transform[:, :] = [[cos_theta, -sin_theta, tx], [sin_theta, cos_theta, ty]] + + class RBpmArray(abstract.ReadFloatArray): """ Class providing read access to a BPM position (array) of a simulator. Position in pyAT is calculated using find_orbit function, which returns the orbit at a specified index. The position is then extracted from the orbit array as the first two elements (x, y). + + Parameters + ---------- + element : at.Element + BPM lattice element whose position is read. + lattice : at.Lattice + Lattice on which the closed orbit is computed. + + Methods + ------- + get() + Return the current value. + unit() + Return the value unit. """ def __init__(self, element: at.Element, lattice: at.Lattice): - self.__element = element - self.__lattice = lattice + """ + Initialize the RBpmArray. + """ + self._element = element + self._lattice = lattice # Gets the value def get(self) -> np.array: - index = self.__lattice.index(self.__element) - _, orbit = at.find_orbit(self.__lattice, refpts=index) - return orbit[0, [0, 2]] + """Return the current value.""" + index = self._lattice.index(self._element) + _, orbit = at.find_orbit(self._lattice, refpts=index) + pts = orbit[0, [0, 2]] + return np.dot(self._element._transform, np.hstack([pts, 1])) # Use homogeneous coordinates # Gets the unit of the value def unit(self) -> str: + """Return the value unit.""" return "m" @@ -367,35 +855,68 @@ class RWBpmOffsetArray(abstract.ReadWriteFloatArray): """ Class providing read write access to a BPM offset (array) of a simulator. Offset in pyAT is defined in Offset attribute as a 2-element array. + + Parameters + ---------- + element : at.Element + BPM lattice element whose ``Offset`` attribute is accessed. + + Methods + ------- + get() + Return the current value. + set(value) + Set the current value. + set_and_wait(value) + Set the value and wait for readback convergence. + unit() + Return the value unit. """ def __init__(self, element: at.Element): - self.__element = element - try: - self.__offset = element.__getattribute__("Offset") - except AttributeError: - self.__offset = None + """ + Initialize the RWBpmOffsetArray. + """ + self._element = element # Gets the value def get(self) -> np.array: - if self.__offset is None: - raise PyAMLException("Element does not have an Offset attribute.") - return self.__offset + """Return the current value.""" + return self._element.Offset # Sets the value def set(self, value: np.array): - if self.__offset is None: - raise PyAMLException("Element does not have an Offset attribute.") - if len(value) != 2: - raise PyAMLException("BPM offset must be a 2-element array.") - self.__offset = value + """ + Set the current value. + + Parameters + ---------- + value : np.array + Two-element array with the horizontal and vertical offsets, in metres. + """ + self._element.Offset = value + update_bpm_transform_matrix(self._element) # Sets the value and wait that the read value reach the setpoint def set_and_wait(self, value: np.array): + """ + Set the value and wait for readback convergence. + + Parameters + ---------- + value : np.array + Two-element array with the horizontal and vertical offsets, in metres. + + Raises + ------ + NotImplementedError + Waiting for readback convergence is not implemented for this accessor. + """ raise NotImplementedError("Not implemented yet.") # Gets the unit of the value def unit(self) -> str: + """Return the value unit.""" return "m" # Assuming all offsets are in m @@ -404,37 +925,75 @@ def unit(self) -> str: class RWBpmTiltScalar(abstract.ReadWriteFloatScalar): """ - Class providing read write access to a BPM tilt of a simulator. Tilt in - pyAT is defined in Rotation attribute as a first element. + Provide read/write access to a simulated BPM tilt. + + The value is read from and written to the Accelerator Toolbox ``Tilt`` + attribute. Writing the tilt also refreshes the BPM coordinate transform. + + Parameters + ---------- + element : at.Element + BPM lattice element whose ``Tilt`` attribute is accessed. + + Methods + ------- + get() + Return the current value. + set(value) + Set the current value. + set_and_wait(value) + Set the value and wait for readback convergence. + unit() + Return the value unit. """ def __init__(self, element: at.Element): - self.__element = element - try: - self.__tilt = element.__getattribute__("Rotation")[0] - except AttributeError: - self.__tilt = None + """ + Initialize a BPM-tilt accessor. + """ + self._element = element # Gets the value def get(self) -> float: - if self.__tilt is None: - raise ValueError("Element does not have a Tilt attribute.") - return self.__tilt + """Return the current value.""" + return self._element.Tilt # Sets the value def set( self, value: float, ): - self.__tilt = value - self.__element.__setattr__("Rotation", [value, None, None]) + """ + Set the current value. + + Parameters + ---------- + value : float + Tilt angle to apply, in radians. + """ + self._element.Tilt = value + update_bpm_transform_matrix(self._element) # Sets the value and wait that the read value reach the setpoint def set_and_wait(self, value: float): + """ + Set the value and wait for readback convergence. + + Parameters + ---------- + value : float + Tilt angle to apply, in radians. + + Raises + ------ + NotImplementedError + Waiting for readback convergence is not implemented for this accessor. + """ raise NotImplementedError("Not implemented yet.") # Gets the unit of the value def unit(self) -> str: + """Return the value unit.""" return "rad" # Assuming BPM tilts are in rad @@ -445,26 +1004,68 @@ class RWRFVoltageScalar(abstract.ReadWriteFloatScalar): """ Class providing read write access to a cavity voltage of a simulator for a given RF trasnmitter. + + Parameters + ---------- + elements : list[at.Element] + RF cavity elements sharing this voltage setpoint. + + Methods + ------- + get() + Return the current value. + set(value) + Set the current value. + set_and_wait(value) + Set the value and wait for readback convergence. + unit() + Return the value unit. """ def __init__(self, elements: list[at.Element]): + """ + Initialize the RWRFVoltageScalar. + """ self.__elements = elements def get(self) -> float: + """Return the current value.""" sum = 0 for _idx, e in enumerate(self.__elements): sum += e.Voltage return sum def set(self, value: float): + """ + Set the current value. + + Parameters + ---------- + value : float + Cavity voltage to apply, in volts. + """ v = value / len(self.__elements) for e in self.__elements: e.Voltage = v def set_and_wait(self, value: float): + """ + Set the value and wait for readback convergence. + + Parameters + ---------- + value : float + Cavity voltage to apply, in volts. + + Raises + ------ + NotImplementedError + Waiting for readback convergence is not implemented for this accessor. + """ raise NotImplementedError("Not implemented yet.") def unit(self) -> str: + """Return the value unit.""" return "V" @@ -473,28 +1074,73 @@ def unit(self) -> str: class RWRFPhaseScalar(abstract.ReadWriteFloatScalar): """ - Class providing read write access to a cavity phase of - a simulator for a given RF trasnmitter. + Provide read/write access to the phase of simulated RF cavities. + + Accelerator Toolbox represents the phase through each cavity's + ``TimeLag`` attribute. This accessor uses the first cavity's frequency and + keeps the phase synchronized across all cavities in the transmitter. + + Parameters + ---------- + elements : list[at.Element] + RF cavity elements sharing the transmitter phase. + + Methods + ------- + get() + Return the current value. + set(value) + Set the current value. + set_and_wait(value) + Set the value and wait for readback convergence. + unit() + Return the value unit. """ def __init__(self, elements: list[at.Element]): + """ + Initialize an RF-cavity phase accessor. + """ self.__elements = elements def get(self) -> float: # Assume that all cavities of this transmitter # have the same Time Lag and Frequency + """Return the current value.""" wavelength = speed_of_light / self.__elements[0].Frequency return (wavelength / self.__elements[0].TimeLag) * 2.0 * np.pi def set(self, value: float): + """ + Set the current value. + + Parameters + ---------- + value : float + Cavity phase to apply, in radians. + """ wavelength = speed_of_light / self.__elements[0].Frequency for e in self.__elements: e.TimeLag = wavelength * value / (2.0 * np.pi) def set_and_wait(self, value: float): + """ + Set the value and wait for readback convergence. + + Parameters + ---------- + value : float + Cavity phase to apply, in radians. + + Raises + ------ + NotImplementedError + Waiting for readback convergence is not implemented for this accessor. + """ raise NotImplementedError("Not implemented yet.") def unit(self) -> str: + """Return the value unit.""" return "rad" @@ -504,24 +1150,68 @@ def unit(self) -> str: class RWRFFrequencyScalar(abstract.ReadWriteFloatScalar): """ Class providing read write access to RF frequency of a simulator. + + Parameters + ---------- + elements : list[at.Element] + RF cavity elements driven by this frequency setpoint. + harmonics : list[float] + Multiplier applied to the requested frequency for each cavity. + + Methods + ------- + get() + Return the current value. + set(value) + Set the current value. + set_and_wait(value) + Set the value and wait for readback convergence. + unit() + Return the value unit. """ def __init__(self, elements: list[at.Element], harmonics: list[float]): + """ + Initialize the RWRFFrequencyScalar. + """ self.__elements = elements self.__harm = harmonics def get(self) -> float: # Serialized cavity has the same frequency + """Return the current value.""" return self.__elements[0].Frequency def set(self, value: float): + """ + Set the current value. + + Parameters + ---------- + value : float + Fundamental RF frequency to apply, in hertz. + """ for idx, e in enumerate(self.__elements): e.Frequency = value * self.__harm[idx] def set_and_wait(self, value: float): + """ + Set the value and wait for readback convergence. + + Parameters + ---------- + value : float + Frequency setpoint. Not implemented by the simulator. + + Raises + ------ + NotImplementedError + Waiting for readback convergence is not implemented for this accessor. + """ raise NotImplementedError("Not implemented yet.") def unit(self) -> str: + """Return the value unit.""" return "Hz" @@ -530,23 +1220,67 @@ def unit(self) -> str: class RWRFATFrequencyScalar(abstract.ReadWriteFloatScalar): """ - Class providing read write access to RF frequency of a simulator using - AT methods. + Provide read/write access to simulated RF frequency through AT methods. + + The accessor delegates frequency reads and writes to + ``Lattice.get_rf_frequency`` and ``Lattice.set_rf_frequency``. + + Parameters + ---------- + ring : at.Lattice + Accelerator Toolbox lattice whose RF frequency is accessed. + + Methods + ------- + get() + Return the current value. + set(value) + Set the current value. + set_and_wait(value) + Set the value and wait for readback convergence. + unit() + Return the value unit. """ def __init__(self, ring: at.Lattice): + """ + Initialize an Accelerator Toolbox RF-frequency accessor. + """ self.__ring = ring def get(self) -> float: + """Return the current value.""" return self.__ring.get_rf_frequency() def set(self, value: float): + """ + Set the current value. + + Parameters + ---------- + value : float + RF frequency to apply, in hertz. + """ self.__ring.set_rf_frequency(value) def set_and_wait(self, value: float): + """ + Set the value and wait for readback convergence. + + Parameters + ---------- + value : float + RF frequency to apply, in hertz. + + Raises + ------ + NotImplementedError + Waiting for readback convergence is not implemented for this accessor. + """ raise NotImplementedError("Not implemented yet.") def unit(self) -> str: + """Return the value unit.""" return "Hz" @@ -555,22 +1289,67 @@ def unit(self) -> str: class RWRFATotalVoltageScalar(abstract.ReadWriteFloatScalar): """ - Class providing read write access to a RF voltage of a simulator using AT methods. + Provide read/write access to total simulated RF voltage. + + The accessor delegates to the Accelerator Toolbox lattice methods + ``get_rf_voltage`` and ``set_rf_voltage``. + + Parameters + ---------- + ring : at.Lattice + Accelerator Toolbox lattice whose total RF voltage is accessed. + + Methods + ------- + get() + Return the current value. + set(value) + Set the current value. + set_and_wait(value) + Set the value and wait for readback convergence. + unit() + Return the value unit. """ def __init__(self, ring: at.Lattice): + """ + Initialize an Accelerator Toolbox RF-voltage accessor. + """ self.__ring = ring def get(self) -> float: + """Return the current value.""" return self.__ring.get_rf_voltage() def set(self, value: float): + """ + Set the current value. + + Parameters + ---------- + value : float + Total RF voltage to apply over the whole ring, in volts. + """ self.__ring.set_rf_voltage(value) def set_and_wait(self, value: float): + """ + Set the value and wait for readback convergence. + + Parameters + ---------- + value : float + Total RF voltage to apply over the whole ring, in volts. + + Raises + ------ + NotImplementedError + Waiting for readback convergence is not implemented for this accessor. + """ raise NotImplementedError("Not implemented yet.") def unit(self) -> str: + """Return the value unit.""" return "V" @@ -580,15 +1359,32 @@ def unit(self) -> str: class RBetatronTuneArray(abstract.ReadFloatArray): """ Class providing read-only access to the betatron tune of a ring. + + Parameters + ---------- + ring : at.Lattice + Accelerator Toolbox lattice whose betatron tunes are computed. + + Methods + ------- + get() + Return the current value. + unit() + Return the value unit. """ def __init__(self, ring: at.Lattice): + """ + Initialize the RBetatronTuneArray. + """ self.__ring = ring def get(self) -> float: + """Return the current value.""" return self.__ring.get_tune()[:2] def unit(self) -> str: + """Return the value unit.""" return "1" diff --git a/pyaml/lattice/attribute_linker.py b/pyaml/lattice/attribute_linker.py index 793726f1b..affa5bcf3 100644 --- a/pyaml/lattice/attribute_linker.py +++ b/pyaml/lattice/attribute_linker.py @@ -1,5 +1,13 @@ +""" +Link PyAML elements to Accelerator Toolbox elements by attributes. + +This module compares a configured PyAT attribute with a PyAML element name to +identify the corresponding lattice element during simulator initialization. +""" + +from dataclasses import dataclass + import at -from pydantic import ConfigDict from pyaml.common.element import Element from pyaml.lattice.lattice_elements_linker import ( @@ -8,61 +16,83 @@ LinkerIdentifier, ) -PYAMLCLASS = "PyAtAttributeElementsLinker" +from ..validation import DynamicValidation, register_schema +PYAMLCLASS = "PyAtAttributeElementsLinker" -class ConfigModel(LinkerConfigModel): - """Base configuration model for linker definitions. - This class defines the configuration structure used to instantiate - a specific linking strategy. Each concrete implementation of a - `LatticeElementsLinker` may define its own subclass extending this model - to include additional configuration parameters. +@dataclass +class PyAtAttributeConfigModel(LinkerConfigModel): + """ + Configuration model for ``PyAtAttributeElementsLinker``. - Attributes + Parameters ---------- - model_config : ConfigDict - Pydantic configuration allowing arbitrary field types and forbidding - unexpected extra keys. + attribute_name : str + Name of the PyAT element attribute used to identify matching + lattice elements. """ - model_config = ConfigDict(arbitrary_types_allowed=True, extra="forbid") attribute_name: str class PyAtAttributeIdentifier(LinkerIdentifier): - """Abstract base class for identifiers used to match PyAML and PyAT elements. - - The identifier acts as an intermediate representation between the PyAML - configuration and the PyAT lattice. Its exact structure depends on the - linking strategy (e.g., family name, element index, or user-defined tag). + """ + Identifier based on a PyAT element attribute. - Subclasses should define the fields and logic necessary to represent - a unique reference to one or more PyAT elements. + Parameters + ---------- + attribute_name : str + Name of the PyAT attribute used for matching. + identifier : object + Expected value of the attribute, compared with ``attribute_name`` on each element. """ def __init__(self, attribute_name: str, identifier): + """ + Create an attribute-based lattice-element identifier. + + The identifier is later compared with the value of ``attribute_name`` + on each PyAT element considered by the linker. + """ self.attribute_name = attribute_name self.identifier = identifier def __repr__(self): + """ + Implement the ``__repr__`` string. + """ return f"{self.attribute_name}={self.identifier}" -class PyAtAttributeElementsLinker(LatticeElementsLinker): - """Abstract base class defining the interface for PyAT–PyAML element linking. +@register_schema +class PyAtAttributeElementsLinker(LatticeElementsLinker, DynamicValidation): + """ + Link lattice elements using a specified PyAT element attribute. - Implementations of this class define how PyAML elements are matched - to PyAT elements based on a given linking strategy (e.g., by family name, - by index, or by a custom attribute). + This linker associates PyAML elements with PyAT elements by comparing + the value of a configurable PyAT attribute against the identifier + extracted from the PyAML element. Parameters ---------- - config_model : ConfigModel - The configuration model for the linking strategy. + attribute_name : str + Name of the PyAT attribute used to identify matching elements. + + Methods + ------- + get_element_identifier(element) + Get the element identifier for the given element. """ - def __init__(self, config_model: ConfigModel): + def __init__(self, attribute_name: str): + """ + Configure an attribute-based PyAT element linker. + + During simulator initialization, the linker compares this attribute's + value on each PyAT element with the corresponding PyAML element name. + """ + config_model = PyAtAttributeConfigModel(attribute_name) super().__init__(config_model) def get_element_identifier(self, element: Element) -> LinkerIdentifier: @@ -82,5 +112,20 @@ def get_element_identifier(self, element: Element) -> LinkerIdentifier: return PyAtAttributeIdentifier(self.linker_config_model.attribute_name, element.get_name()) def _test_at_element(self, identifier: PyAtAttributeIdentifier, element: at.Element) -> bool: + """ + Check whether a PyAT element matches a linker identifier. + + Parameters + ---------- + identifier : PyAtAttributeIdentifier + Attribute name and expected identifier to compare. + element : at.Element + PyAT lattice element being tested. + + Returns + ------- + bool + ``True`` if the attribute value matches; otherwise ``False``. + """ attr_value = getattr(element, identifier.attribute_name, None) return attr_value == identifier.identifier diff --git a/pyaml/lattice/lattice_elements_linker.py b/pyaml/lattice/lattice_elements_linker.py index de83cf33c..ef11e559b 100644 --- a/pyaml/lattice/lattice_elements_linker.py +++ b/pyaml/lattice/lattice_elements_linker.py @@ -1,34 +1,36 @@ -from abc import ABCMeta, abstractmethod +""" +Interfaces for linking PyAML elements to PyAT lattice elements. + +Linkers translate PyAML element references into matching Accelerator Toolbox +elements and provide the runtime objects used by simulator accessors. +""" + +from abc import ABC, abstractmethod from typing import Iterable import at from at import Lattice -from pydantic import BaseModel, ConfigDict from pyaml import PyAMLException from pyaml.common.element import Element -class LinkerConfigModel(BaseModel): - """Base configuration model for linker definitions. +class LinkerConfigModel(ABC): + """ + Base configuration model for linker definitions. This class defines the configuration structure used to instantiate a specific linking strategy. Each concrete implementation of a `LatticeElementsLinker` may define its own subclass extending this model to include additional configuration parameters. - - Attributes - ---------- - model_config : ConfigDict - Pydantic configuration allowing arbitrary field types and forbidding - unexpected extra keys. """ - model_config = ConfigDict(arbitrary_types_allowed=True, extra="forbid") + pass -class LinkerIdentifier(metaclass=ABCMeta): - """Abstract base class for identifiers used to match PyAML and PyAT elements. +class LinkerIdentifier(ABC): + """ + Abstract base class for identifiers used to match PyAML and PyAT elements. The identifier acts as an intermediate representation between the PyAML configuration and the PyAT lattice. Its exact structure depends on the @@ -41,27 +43,45 @@ class LinkerIdentifier(metaclass=ABCMeta): pass -class LatticeElementsLinker(metaclass=ABCMeta): - """Abstract base class defining the interface for PyAT–PyAML element linking. +class LatticeElementsLinker(ABC): + """ + Abstract base class defining the interface for PyAT–PyAML element linking. Implementations of this class define how PyAML elements are matched to PyAT elements based on a given linking strategy (e.g., by family name, by index, or by a custom attribute). + linker_config_model : LinkerConfigModel + The configuration model for the linking strategy. + Parameters ---------- linker_config_model : LinkerConfigModel - The configuration model for the linking strategy. + Strategy-specific configuration used to identify lattice elements. Attributes ---------- lattice : at.Lattice Reference to the PyAT lattice handled by this linker. + + Methods + ------- + set_lattice(lattice) + Set the lattice for element linking. + get_element_identifier(element) + Get the identifier for linking an element. + get_at_elements(element_id) + Return a list of PyAT elements matching the given identifiers. + get_at_element(element_id) + Return a single PyAT element matching the given identifier. """ def __init__(self, linker_config_model: LinkerConfigModel): + """ + Initialize a lattice-element linker. + """ self.linker_config_model = linker_config_model - self.lattice: Lattice = None + self.lattice: Lattice | None = None def set_lattice(self, lattice: Lattice): """ @@ -76,6 +96,21 @@ def set_lattice(self, lattice: Lattice): @abstractmethod def _test_at_element(self, identifier: LinkerIdentifier, element: at.Element) -> bool: + """ + Test whether a PyAT element matches a linker identifier. + + Parameters + ---------- + identifier : LinkerIdentifier + Identifier describing the desired lattice element. + element : at.Element + PyAT lattice element to test. + + Returns + ------- + bool + ``True`` if the element matches; otherwise ``False``. + """ pass @abstractmethod @@ -96,13 +131,22 @@ def get_element_identifier(self, element: Element) -> LinkerIdentifier: pass def _iter_matches(self, identifier: LinkerIdentifier) -> Iterable[at.Element]: - """Yield all elements in the lattice whose matches the identifier.""" - for elem in self.lattice: - if self._test_at_element(identifier, elem): - yield elem + """ + Yield all lattice elements matching ``identifier``. + + Parameters + ---------- + identifier : LinkerIdentifier + Criterion used to select the PyAT elements. + """ + if self.lattice: + for elem in self.lattice: + if self._test_at_element(identifier, elem): + yield elem def get_at_elements(self, element_id: LinkerIdentifier | list[LinkerIdentifier]) -> list[at.Element]: - """Return a list of PyAT elements matching the given identifiers. + """ + Return a list of PyAT elements matching the given identifiers. This method should resolve one or multiple PyAML identifiers into their corresponding PyAT elements according to the specific @@ -138,7 +182,8 @@ def get_at_elements(self, element_id: LinkerIdentifier | list[LinkerIdentifier]) return results def get_at_element(self, element_id: LinkerIdentifier) -> at.Element: - """Return a single PyAT element matching the given identifier. + """ + Return a single PyAT element matching the given identifier. Parameters ---------- diff --git a/pyaml/lattice/polynom_info.py b/pyaml/lattice/polynom_info.py index 6e03a49d7..8ac515e46 100644 --- a/pyaml/lattice/polynom_info.py +++ b/pyaml/lattice/polynom_info.py @@ -6,18 +6,18 @@ class PolynomInfo: """ Polynom information + + Parameters + ---------- + attName : str + Name of the AT element attribute ('PolynomA' or 'PolynomB') + index : int + Polynomial coefficients index (sarting from 0) """ def __init__(self, attName: str, index: int, sign: float = 1.0): """ Construct a polynom information object - - Parameters - ---------- - attName : str - Name of the AT element attribute ('PolynomA' or 'PolynomB') - index : int - Polynomial coefficients index (sarting from 0) """ self.attName = attName self.index = index diff --git a/pyaml/lattice/simulator.py b/pyaml/lattice/simulator.py index a877588aa..810928250 100644 --- a/pyaml/lattice/simulator.py +++ b/pyaml/lattice/simulator.py @@ -1,14 +1,21 @@ +""" +PyAT-backed accelerator simulator interfaces. + +This module loads Accelerator Toolbox lattices and binds PyAML elements to +their simulated lattice counterparts. +""" + from pathlib import Path +from typing import TYPE_CHECKING import at -from pydantic import BaseModel, ConfigDict from ..bpm.bpm import BPM from ..common.abstract_aggregator import ScalarAggregator -from ..common.element import Element -from ..common.element_holder import ElementHolder +from ..common.element import Element, __pyaml_repr__ from ..common.exception import PyAMLException -from ..configuration import get_root_folder +from ..common.holders.element_holder import ElementHolder +from ..configuration import ROOT from ..diagnostics.tune_monitor import BetatronTuneMonitor from ..lattice.abstract_impl import ( BPMHScalarAggregator, @@ -29,6 +36,7 @@ RWSerializedStrength, RWStrengthArray, RWStrengthScalar, + update_bpm_transform_matrix, ) from ..magnet.cfm_magnet import CombinedFunctionMagnet from ..magnet.magnet import Magnet @@ -37,61 +45,104 @@ from ..rf.rf_transmitter import RFTransmitter from ..tuning_tools.measurement_tool import MeasurementTool from ..tuning_tools.tuning_tool import TuningTool -from .attribute_linker import ( - ConfigModel as PyAtAttrLinkerConfigModel, -) -from .attribute_linker import ( - PyAtAttributeElementsLinker, -) +from ..validation import DynamicValidation, register_schema from .lattice_elements_linker import LatticeElementsLinker +if TYPE_CHECKING: + from ..configuration.unbound_element import UnboundElement + # Define the main class name for this module PYAMLCLASS = "Simulator" -class ConfigModel(BaseModel): +@register_schema +class Simulator(ElementHolder, DynamicValidation): """ - Configuration model for Simulator + Simulator interface backed by a PyAT lattice. + + The simulator loads a PyAT lattice from disk and attaches PyAML + elements to their corresponding PyAT elements. Once attached, the + resulting device objects expose read/write interfaces operating + directly on the simulation model. + + Elements may be matched either using the default name-based lookup + or a custom :class:`LatticeElementsLinker`. Parameters ---------- name : str - Simulator name + Name of the simulator. lattice : str - AT lattice file + Path to the PyAT lattice file, relative to the configured + PyAML root directory. mat_key : str, optional - AT lattice ring name + Variable name of the lattice when loading a MATLAB ``.mat`` + lattice file. linker : LatticeElementsLinker, optional - The linker configuration model - description : str , optional - Simulator description - """ - - model_config = ConfigDict(arbitrary_types_allowed=True, extra="forbid") + Custom linker used to associate PyAML elements with PyAT + lattice elements. If omitted, elements are matched by name. + description : str, optional + Human-readable description of the simulator. - name: str - lattice: str - mat_key: str = None - linker: LatticeElementsLinker = None - description: str | None = None + Attributes + ---------- + lattice + Underlying PyAT lattice. + mat_key + Key used to read the lattice out of a MATLAB file. + + Methods + ------- + name() + Return the simulator name. + get_lattice() + Return the loaded Accelerator Toolbox lattice. + get_description() + Returns the description of the accelerator + create_magnet_strength_aggregator(magnets) + Return the magnet-strength aggregator for this simulator. + create_magnet_hardware_aggregator(magnets) + Return the magnet-hardware aggregator for this simulator. + create_bpm_aggregators(bpms) + Create BPM position aggregators for the loaded lattice. + fill_device(elements) + Attach PyAML elements to their matching PyAT lattice elements. + get_names(element) + Parse element lattice_name syntax. see Element.ConfigModel.lattice_name. + get_indices(element) + Parse element lattice_name syntax. see Element.ConfigModel.lattice_name. + get_at_elems(element) + Resolve a PyAML element to matching PyAT lattice elements. + """ + __pyaml_repr_exclude__ = ("description", "ring") -class Simulator(ElementHolder): - """ - Class that implements access to AT simulator - """ + def __init__( + self, + name: str, + lattice: str, + mat_key: str | None = None, + linker: LatticeElementsLinker | None = None, + description: str | None = None, + ): + """ + Create a simulator from a PyAT lattice. + """ - def __init__(self, cfg: ConfigModel): super().__init__() - self._cfg = cfg - path: Path = get_root_folder() / cfg.lattice + self._name = name + self._lattice = lattice + self._mat_key = mat_key + self.description = description + + path: Path = ROOT.get() / self._lattice - if self._cfg.mat_key is None: + if self._mat_key is None: self.ring = at.load_lattice(path) else: - self.ring = at.load_lattice(path, mat_key=f"{self._cfg.mat_key}") + self.ring = at.load_lattice(path, mat_key=f"{self._mat_key}") - self._linker = cfg.linker + self._linker = linker if self._linker: self._linker.set_lattice(self.ring) else: @@ -103,26 +154,77 @@ def __init__(self, cfg: ConfigModel): self._elements_indexing[e.FamName] = [e] def name(self) -> str: - return self._cfg.name + """Return the simulator name.""" + return self._name + + @property + def lattice(self) -> str: + """Return the configured lattice file path.""" + return self._lattice def get_lattice(self) -> at.Lattice: + """Return the loaded Accelerator Toolbox lattice.""" return self.ring - def get_description(self) -> str: + @property + def mat_key(self) -> str | None: + """Return the MATLAB variable name used to load the lattice.""" + return self._mat_key + + def get_description(self) -> str | None: """ Returns the description of the accelerator """ - return self._cfg.description + return self.description def create_magnet_strength_aggregator(self, magnets: list[Magnet]) -> ScalarAggregator: # No magnet aggregator for simulator + """ + Return the magnet-strength aggregator for this simulator. + + Parameters + ---------- + magnets : list[Magnet] + Magnets for which aggregation was requested. + + Returns + ------- + ScalarAggregator + ``None`` because simulated magnet values are accessed directly. + """ return None def create_magnet_hardware_aggregator(self, magnets: list[Magnet]) -> ScalarAggregator: # No magnet aggregator for simulator + """ + Return the magnet-hardware aggregator for this simulator. + + Parameters + ---------- + magnets : list[Magnet] + Magnets for which aggregation was requested. + + Returns + ------- + ScalarAggregator + ``None`` because simulated hardware values are accessed directly. + """ return None def create_bpm_aggregators(self, bpms: list[BPM]) -> list[ScalarAggregator]: + """ + Create BPM position aggregators for the loaded lattice. + + Parameters + ---------- + bpms : list[BPM] + BPM elements whose positions should be read. + + Returns + ------- + list[ScalarAggregator] + Aggregators for combined, horizontal, and vertical BPM positions. + """ agg = BPMScalarAggregator(self.get_lattice()) aggh = BPMHScalarAggregator(self.get_lattice()) aggv = BPMVScalarAggregator(self.get_lattice()) @@ -133,113 +235,97 @@ def create_bpm_aggregators(self, bpms: list[BPM]) -> list[ScalarAggregator]: aggv.add_elem(e) return [agg, aggh, aggv] - def fill_device(self, elements: list[Element]): - for e in elements: - # Need conversion to physics unit to work with simulator - if isinstance(e, Magnet): - current = RWHardwareScalar(self.get_at_elems(e), e.polynom, e.model) if e.model.has_physics() else None - strength = RWStrengthScalar(self.get_at_elems(e), e.polynom, e.model) if e.model.has_physics() else None - # Create a unique ref for this simulator - m = e.attach(self, strength, current) - self.add_magnet(m) - - elif isinstance(e, CombinedFunctionMagnet): - currents = RWHardwareArray(self.get_at_elems(e), e.polynoms, e.model) if e.model.has_physics() else None - strengths = RWStrengthArray(self.get_at_elems(e), e.polynoms, e.model) if e.model.has_physics() else None - # Create unique refs of each function for this simulator - ms = e.attach(self, strengths, currents) - self.add_cfm_magnet(ms[0]) - for m in ms[1:]: - self.add_magnet(m) - - elif isinstance(e, SerializedMagnets): - currents = [] - strengths = [] - # Create unique refs the series and each of its function for this - # control system - # Link hardware to strengths and bind strength together - for index, magnet in enumerate(e.get_magnets()): - current = ( - RWHardwareScalar( - self.get_at_elems(magnet), - e.polynom, - e.model.get_sub_model(index), - ) - if e.model.has_hardware() - else None - ) - strength = ( - RWStrengthScalar( - self.get_at_elems(magnet), - e.polynom, - e.model.get_sub_model(index), - ) - if e.model.has_physics() - else None - ) - currents.append(current) - strengths.append(strength) - linked_currents = [] - linked_strengths = [] - for i in range(e.get_nb_magnets()): - current = RWSerializedHardware(currents, i) if e.model.has_hardware() else None - strength = RWSerializedStrength(strengths, currents, i) if e.model.has_physics() else None - linked_currents.append(current) - linked_strengths.append(strength) - ms = e.attach(self, linked_strengths, linked_currents) - self.add_serialized_magnet(ms[0]) - for m in ms[1:]: - self.add_magnet(m) - - elif isinstance(e, BPM): - # This assumes unique BPM names in the pyAT lattice - tilt = RWBpmTiltScalar(self.get_at_elems(e)[0]) - offsets = RWBpmOffsetArray(self.get_at_elems(e)[0]) - positions = RBpmArray(self.get_at_elems(e)[0], self.ring) - e = e.attach(self, positions, offsets, tilt) - self.add_bpm(e) - - elif isinstance(e, RFPlant): - if e._cfg.transmitters: - cavs: list[at.Element] = [] - harmonics: list[float] = [] - attachedTrans: list[RFTransmitter] = [] - for t in e._cfg.transmitters: - cavsPerTrans: list[at.Element] = [] - for c in t._cfg.cavities: - # Expect unique name for cavities - cav = self.get_at_elems(Element(c)) - if len(cav) > 1: - raise PyAMLException(f"RF transmitter {t.get_name()},multiple cavity definition:{{cav[0]}}") - if len(cav) == 0: - raise PyAMLException(f"RF transmitter {t.get_name()}, No cavity found") - cavsPerTrans.append(cav[0]) - harmonics.append(t._cfg.harmonic) - voltage = RWRFVoltageScalar(cavsPerTrans) - phase = RWRFPhaseScalar(cavsPerTrans) - nt = t.attach(self, voltage, phase) - self.add_rf_transnmitter(nt) - cavs.extend(cavsPerTrans) - attachedTrans.append(nt) - - frequency = RWRFFrequencyScalar(cavs, harmonics) - voltage = RWTotalVoltage(attachedTrans) - ne = e.attach(self, frequency, voltage) - self.add_rf_plant(ne) - else: - # No transmitter defined switch to AT methods - frequency = RWRFATFrequencyScalar(self.ring) - voltage = RWRFATotalVoltageScalar(self.ring) - ne = e.attach(self, frequency, voltage) - self.add_rf_plant(ne) + def _fill_magnet(self, magnet: Magnet) -> None: + current = ( + RWHardwareScalar(self.get_at_elems(magnet), magnet.polynom, magnet.model) if magnet.model.has_physics() else None + ) + strength = ( + RWStrengthScalar(self.get_at_elems(magnet), magnet.polynom, magnet.model) if magnet.model.has_physics() else None + ) + self.magnet.add(magnet.attach(self, strength, current)) + + def _fill_combined_function_magnet(self, magnet: CombinedFunctionMagnet) -> None: + currents = ( + RWHardwareArray(self.get_at_elems(magnet), magnet.polynoms, magnet.model) if magnet.model.has_physics() else None + ) + strengths = ( + RWStrengthArray(self.get_at_elems(magnet), magnet.polynoms, magnet.model) if magnet.model.has_physics() else None + ) + magnets = magnet.attach(self, strengths, currents) + self.combined_function_magnet.add(magnets[0]) + for virtual_magnet in magnets[1:]: + self.magnet.add(virtual_magnet) + + def _fill_serialized_magnets(self, magnets: SerializedMagnets) -> None: + currents = [] + strengths = [] + for index, magnet in enumerate(magnets.get_magnets()): + current = ( + RWHardwareScalar(self.get_at_elems(magnet), magnets.polynom, magnets.model.get_sub_model(index)) + if magnets.model.has_hardware() + else None + ) + strength = ( + RWStrengthScalar(self.get_at_elems(magnet), magnets.polynom, magnets.model.get_sub_model(index)) + if magnets.model.has_physics() + else None + ) + currents.append(current) + strengths.append(strength) + linked_currents = [] + linked_strengths = [] + for index in range(magnets.get_nb_magnets()): + linked_currents.append(RWSerializedHardware(currents, index) if magnets.model.has_hardware() else None) + linked_strengths.append(RWSerializedStrength(strengths, currents, index) if magnets.model.has_physics() else None) + attached_magnets = magnets.attach(self, linked_strengths, linked_currents) + self.serialized_magnet.add(attached_magnets[0]) + for magnet in attached_magnets[1:]: + self.magnet.add(magnet) + + def _fill_bpm(self, bpm: BPM) -> None: + bpm_elt = self.get_at_elems(bpm)[0] + if not hasattr(bpm_elt, "Tilt"): + bpm_elt.Tilt = 0.0 + if not hasattr(bpm_elt, "Offset"): + bpm_elt.Offset = [0.0, 0.0] + if len(bpm_elt.Offset) != 2: + raise PyAMLException(f"BPM {bpm.get_name()} offset must be a 2-element array.") + update_bpm_transform_matrix(bpm_elt) + self.bpm.add(bpm.attach(self, RBpmArray(bpm_elt, self.ring), RWBpmOffsetArray(bpm_elt), RWBpmTiltScalar(bpm_elt))) + + def _fill_rf_plant(self, rf_plant: RFPlant) -> None: + if rf_plant.transmitters: + cavities: list[at.Element] = [] + harmonics: list[float] = [] + attached_transmitters: list[RFTransmitter] = [] + for transmitter in rf_plant.transmitters: + transmitter_cavities: list[at.Element] = [] + for cavity_name in transmitter.cavities: + cavity = self.get_at_elems(Element(cavity_name)) + if len(cavity) > 1: + raise PyAMLException(f"RF transmitter {transmitter.get_name()},multiple cavity definition:{{cav[0]}}") + if len(cavity) == 0: + raise PyAMLException(f"RF transmitter {transmitter.get_name()}, No cavity found") + transmitter_cavities.append(cavity[0]) + harmonics.append(transmitter.harmonic) + voltage = RWRFVoltageScalar(transmitter_cavities) + phase = RWRFPhaseScalar(transmitter_cavities) + attached_transmitter = transmitter.attach(self, voltage, phase) + self.rf.transmitter.add(attached_transmitter) + cavities.extend(transmitter_cavities) + attached_transmitters.append(attached_transmitter) + self.rf.add(rf_plant.attach(self, RWRFFrequencyScalar(cavities, harmonics), RWTotalVoltage(attached_transmitters))) + else: + self.rf.add(rf_plant.attach(self, RWRFATFrequencyScalar(self.ring), RWRFATotalVoltageScalar(self.ring))) + + def _fill_betatron_tune_monitor(self, monitor: BetatronTuneMonitor) -> None: + self.add_betatron_tune_monitor(monitor.attach(self, RBetatronTuneArray(self.ring))) - elif isinstance(e, BetatronTuneMonitor): - betatron_tune = RBetatronTuneArray(self.ring) - e = e.attach(self, betatron_tune) - self.add_betatron_tune_monitor(e) + def _fill_tool(self, tool: TuningTool | MeasurementTool) -> None: + self.add_tool(tool.attach(self)) - elif isinstance(e, MeasurementTool) | isinstance(e, TuningTool): - self.add_tool(e.attach(self)) + def _fill_unbound_element(self, element: "UnboundElement") -> None: + pass def get_names(self, element: Element) -> list[str] | None: """ @@ -298,6 +384,19 @@ def get_indices(self, element: Element) -> (str | None, list[int] | None): return (element.get_name(), None) def get_at_elems(self, element: Element) -> list[at.Element]: + """ + Resolve a PyAML element to matching PyAT lattice elements. + + Parameters + ---------- + element : Element + PyAML element whose lattice mapping should be resolved. + + Returns + ------- + list[at.Element] + Matching Accelerator Toolbox lattice elements. + """ if self._linker: identifier = self._linker.get_element_identifier(element) element_list = self._linker.get_at_elements(identifier) @@ -332,5 +431,16 @@ def get_at_elems(self, element: Element) -> list[at.Element]: else: return [elts[idx] for idx in indices] + def _pyaml_repr_fields(self) -> dict[str, object]: + return { + "name": self.name(), + "lattice": self.lattice, + "mat_key": self.mat_key, + "n_elements": len(self.ring), + } + def __repr__(self): - return repr(self._cfg).replace("ConfigModel", self.__class__.__name__) + """ + Implement the ``__repr__`` string. + """ + return __pyaml_repr__(self) diff --git a/pyaml/magnet/cfm_magnet.py b/pyaml/magnet/cfm_magnet.py index 957c0e19c..eb7db64e8 100644 --- a/pyaml/magnet/cfm_magnet.py +++ b/pyaml/magnet/cfm_magnet.py @@ -1,12 +1,22 @@ +""" +Combined-function magnet elements. + +This module defines magnets that combine multiple multipole components and +provide separate strength and hardware access for those components. +""" + +from typing import TYPE_CHECKING + from scipy.constants import speed_of_light from ..common import abstract from ..common.abstract import RWMapper -from ..common.element import Element, ElementConfigModel, __pyaml_repr__ +from ..common.element import Element, __pyaml_repr__ from ..common.exception import PyAMLException -from ..configuration import Factory +from ..configuration.factory import ELEMENT_REGISTRY +from ..validation import DynamicValidation, register_schema from .hcorrector import HCorrector -from .magnet import Magnet, MagnetConfigModel +from .magnet import Magnet from .model import MagnetModel from .octupole import Octupole from .quadrupole import Quadrupole @@ -16,6 +26,9 @@ from .skewsext import SkewSext from .vcorrector import VCorrector +if TYPE_CHECKING: + from ..common.holders.element_holder import ElementHolder + _fmap: dict = { "B0": HCorrector, "A0": VCorrector, @@ -31,39 +44,85 @@ PYAMLCLASS = "CombinedFunctionMagnet" -class ConfigModel(ElementConfigModel): - mapping: list[list[str]] - """Name mapping for multipoles - (i.e. [[B0,C01A-H],[A0,C01A-H],[B2,C01A-S]])""" - model: MagnetModel | None = None - """Object in charge of converting magnet strenghts to currents""" +@register_schema +class CombinedFunctionMagnet(Element, DynamicValidation): + """ + Combined function magnet made up of several virtual single-function magnets. + + This class represents a magnet whose effect is described by multiple multipole + components, such as a corrector, quadrupole, sextupole, or octupole family. + Each entry in ``mapping`` creates a virtual magnet backed by the same + underlying magnet model, and the virtual magnets are exposed as individual + elements while still belonging to the same combined-function object. + + Parameters + ---------- + name : str + Name of the combined-function magnet. + mapping : list[list[str]] + List of ``[multipole, magnet_name]`` pairs. The first entry selects the + virtual magnet type, and the second entry gives the name of the virtual + magnet. + model : MagnetModel | None, optional + Magnet model used to convert strengths to hardware values and vice versa. + description : str | None, optional + Human-readable description of the magnet. + peer : object, optional + Control-system or simulator peer used when attaching the magnet. + + Attributes + ---------- + strengths + Gives access to the strengths of this combined function magnet in physics unit + hardwares + Gives access to the strengths of this combined function magnet in hardware unit when possible + Methods + ------- + get_model_name() + Returns the model name of this magnet + nb_multipole() + Return the number of configured multipole components. + attach(peer, strengths, hardwares) + Attach the combined-function magnet and its virtual components. + set_energy(E) + Set beam energy for magnetic-strength conversion. + + Raises + ------ + PyAMLException + If the mapping is invalid, if an unsupported multipole is requested, or + if the model does not provide the required multipole information. + """ -class CombinedFunctionMagnet(Element): - """CombinedFunctionMagnet class""" + def __init__( + self, name: str, mapping: list[list[str]], model: MagnetModel | None = None, description: str | None = None, peer=None + ): + """ + Initialize the CombinedFunctionMagnet. + """ + super().__init__(name, None, description) - def __init__(self, cfg: ConfigModel, peer=None): - super().__init__(cfg.name) - self._cfg = cfg - self.model = cfg.model + self._mapping = mapping + self.model = model self.__virtuals: list[Magnet] = [] - self.__strengths: abstract.ReadWriteFloatArray = None - self.__hardwares: abstract.ReadWriteFloatArray = None + self.__strengths: abstract.ReadWriteFloatArray | None = None + self.__hardwares: abstract.ReadWriteFloatArray | None = None if peer is None: # Configuration part - if self.model is not None and not hasattr(self.model._cfg, "multipoles"): - raise PyAMLException(f"{cfg.name} model: mutipolesfield required for combined function magnet") + if self.model is not None and not hasattr(self.model, "multipoles"): + raise PyAMLException(f"{name} model: mutipoles field required for combined function magnet") idx = 0 self.polynoms = [] - for _idx, m in enumerate(cfg.mapping): + for _idx, m in enumerate(self._mapping): # Check mapping validity if len(m) != 2: raise PyAMLException("Invalid CombinedFunctionMagnet mapping for {m}") if m[0] not in _fmap: raise PyAMLException(m[0] + " not implemented for combined function magnet") - if m[0] not in self.model._cfg.multipoles: + if m[0] not in self.model.multipoles: raise PyAMLException(m[0] + " not found in underlying magnet model") self.polynoms.append(_fmap[m[0]].polynom) # Create the virtual magnet for the correspoding multipole @@ -71,26 +130,48 @@ def __init__(self, cfg: ConfigModel, peer=None): self.__virtuals.append(vm) # Register the virtual element in the factory to have # a coherent factory and improve error reporting - Factory.register_element(vm) + ELEMENT_REGISTRY.register(vm) else: # Attach self._peer = peer + def _fill_device(self, holder: "ElementHolder") -> None: + holder._fill_combined_function_magnet(self) + def get_model_name(self) -> str: """ Returns the model name of this magnet """ - return self._cfg.name + return self._name def __create_virutal_manget(self, name: str, idx: int) -> Magnet: + """ + Create a virtual magnet for one multipole component. + + The virtual magnet provides the standard single-function magnet + interface for a component of this combined-function magnet. + + Parameters + ---------- + name : str + Name assigned to the virtual magnet. + idx : int + Multipole key used to select the virtual-magnet class. + + Returns + ------- + Magnet + Newly created virtual magnet linked to this magnet's model. + """ args = {"name": name, "model": self.model} - mVirtual: Magnet = _fmap[idx](MagnetConfigModel(**args)) + mVirtual: Magnet = _fmap[idx](**args) mVirtual.set_model_name(self.get_name()) return mVirtual def nb_multipole(self) -> int: - return len(self._cfg.mapping) + """Return the number of configured multipole components.""" + return len(self._mapping) def attach( self, @@ -98,15 +179,38 @@ def attach( strengths: abstract.ReadWriteFloatArray, hardwares: abstract.ReadWriteFloatArray, ) -> list[Magnet]: + """ + Attach the combined-function magnet and its virtual components. + + The returned list contains the attached combined-function magnet + followed by one attached single-function virtual magnet per configured + multipole. Each virtual magnet receives a mapped view of the shared + strength and hardware arrays. + + Parameters + ---------- + peer : object + Simulator or control-system element holder. + strengths : abstract.ReadWriteFloatArray + Array accessor for the physical multipole strengths. + hardwares : abstract.ReadWriteFloatArray + Array accessor for the hardware values. + + Returns + ------- + list[Magnet] + Attached combined-function magnet and its virtual component + magnets. + """ l = [] # Attached the CombinedFunctionMagnet itself - nCFM = CombinedFunctionMagnet(self._cfg, peer) + nCFM = CombinedFunctionMagnet(self._name, self._mapping, self.model, self._description, peer) nCFM.__strengths = strengths nCFM.__hardwares = hardwares l.append(nCFM) # Construct a single function magnet for each multipole # of this combined function magnet - for idx, _m in enumerate(self._cfg.mapping): + for idx, _m in enumerate(self._mapping): strength = RWMapper(strengths, idx) hardware = RWMapper(hardwares, idx) if self.model.has_hardware() else None l.append(self.__virtuals[idx].attach(peer, strength, hardware)) @@ -135,8 +239,22 @@ def hardwares(self) -> abstract.ReadWriteFloatScalar: return self.__hardwares def set_energy(self, E: float): + """ + Set beam energy for magnetic-strength conversion. + + The energy is converted from electronvolts to magnetic rigidity and + supplied to the underlying combined-function magnet model. + + Parameters + ---------- + E : float + Beam energy in electronvolts. + """ if self.model is not None: self.model.set_magnet_rigidity(E / speed_of_light) def __repr__(self): + """ + Implement the ``__repr__`` string. + """ return __pyaml_repr__(self) diff --git a/pyaml/magnet/corrector.py b/pyaml/magnet/corrector.py index fc9de1294..1f828450a 100644 --- a/pyaml/magnet/corrector.py +++ b/pyaml/magnet/corrector.py @@ -1,3 +1,9 @@ +""" +Corrector magnet elements. + +This module defines horizontal and vertical orbit-corrector elements. +""" + import numpy as np from ..common import abstract @@ -7,14 +13,35 @@ class RWCorrectorAngle(abstract.ReadWriteFloatScalar): """ Set the angle of a horizontal or vertical corrector. - KickAngle sign convention is defined the a global PyAML constant - (see pyaml.common.constant.HORIZONATL_KICK_SIGN). - To change the convention, you have execute the code below prior to everything: - import pyaml.common.constants - pyaml.common.constants.HORIZONTAL_KICK_SIGN = -1.0 + + The kick-angle sign convention is defined by the global PyAML constant + :data:`pyaml.common.constants.HORIZONTAL_KICK_SIGN`. To change the convention, + run the following before building the accelerator:: + + import pyaml.common.constants + pyaml.common.constants.HORIZONTAL_KICK_SIGN = -1.0 + + Parameters + ---------- + corr : Magnet + Corrector magnet whose strength represents the kick angle. + + Methods + ------- + get() + Get the corrector kick angle. + set(value) + Set the corrector kick angle. + set_and_wait(value) + Set the kick angle and wait for it to reach the setpoint. + unit() + Get the unit for the kick angle. """ def __init__(self, corr: Magnet): + """ + Initialize a corrector-angle access wrapper. + """ self._mag = corr def get(self) -> float: @@ -24,7 +51,7 @@ def get(self) -> float: Returns ------- float - Kick angle in radians + Kick angle in radians. """ return np.arctan(self._mag.strength.get()) @@ -35,7 +62,7 @@ def set(self, value: float): Parameters ---------- value : float - Kick angle to set in radians + Target kick angle in radians. """ self._mag.strength.set(np.tan(value)) diff --git a/pyaml/magnet/csvcurve.py b/pyaml/magnet/csvcurve.py new file mode 100644 index 000000000..c9cb55285 --- /dev/null +++ b/pyaml/magnet/csvcurve.py @@ -0,0 +1,103 @@ +""" +CSV-backed magnet excitation curves. + +This module loads two-column excitation data from CSV files for magnet-model +calibration and interpolation. +""" + +import numpy as np +from numpy.typing import NDArray + +from ..common.element import __pyaml_repr__ +from ..common.exception import PyAMLException +from ..configuration.fileloader import ROOT +from ..validation import DynamicValidation, register_schema +from .curve import Curve + +# Define the main class name for this module +PYAMLCLASS = "CSVCurve" + + +@register_schema +class CSVCurve(Curve, DynamicValidation): + """ + Curve loaded from a CSV file. + + This class reads a CSV file containing a two-column numeric dataset + representing ``(x, y)`` coordinate pairs. The file is loaded during + initialization and stored internally as a NumPy array. + + The CSV file must: + + - contain exactly two columns, + - use commas as the delimiter, + - contain values that can be converted to ``float``. + + Parameters + ---------- + file : str + Path to the CSV file. Relative paths are resolved using the + project's configured root directory. + + Attributes + ---------- + file : str + Path to the CSV file provided during initialization. + + Methods + ------- + get_curve() + Get the curve data. + + Raises + ------ + PyAMLException + If the file cannot be parsed as a numeric CSV or if the loaded + data does not have shape ``(n, 2)``. + + Notes + ----- + The loaded curve is stored internally as a NumPy array with shape + ``(n, 2)``, where the first column contains x-values and the second + column contains y-values. The data can be accessed using + :meth:`get_curve`. + """ + + def __init__(self, file: str): + """ + Initialize the CSVCurve. + """ + self._file = file + + # Load CSV curve + path = ROOT.expand_path(self._file) + try: + self._curve = np.genfromtxt(path, delimiter=",", dtype=float, loose=False) + except ValueError as e: + raise PyAMLException(f"CSVCurve(file='{self._file}',dtype=float): {str(e)}") from None + + _s = np.shape(self._curve) + if len(_s) != 2 or _s[1] != 2: + raise PyAMLException(f"CSVCurve(file='{self._file}',dtype=float):wrong shape (2,2) expected but got {str(_s)}") + + @property + def file(self): + """Return the configured CSV file path.""" + return self._file + + def get_curve(self) -> NDArray[np.float64]: + """ + Get the curve data. + + Returns + ------- + np.array + Curve data as a 2D numpy array of shape (n, 2) + """ + return self._curve + + def __repr__(self): + """ + Implement the ``__repr__`` string. + """ + return __pyaml_repr__(self) diff --git a/pyaml/magnet/csvmatrix.py b/pyaml/magnet/csvmatrix.py new file mode 100644 index 000000000..a7babee17 --- /dev/null +++ b/pyaml/magnet/csvmatrix.py @@ -0,0 +1,83 @@ +""" +Magnet response matrices. + +This module defines matrix representations used by magnet models. +""" + +import numpy as np +from numpy.typing import NDArray + +from ..common.element import __pyaml_repr__ +from ..common.exception import PyAMLException +from ..configuration.fileloader import ROOT +from ..validation import DynamicValidation, register_schema +from .matrix import Matrix + +# Define the main class name for this module +PYAMLCLASS = "CSVMatrix" + + +@register_schema +class CSVMatrix(Matrix, DynamicValidation): + """ + Matrix loaded from a CSV file. + + This class reads a CSV file containing numeric values and stores the + resulting matrix as a NumPy array. + + Parameters + ---------- + file : str + Path to the CSV file. Relative paths are resolved using the + project's configured root directory. + + Attributes + ---------- + file + Return the configured CSV file path. + + Methods + ------- + get_matrix() + Get the matrix data. + + Raises + ------ + PyAMLException + If the CSV file cannot be parsed as a numeric array. + """ + + def __init__(self, file: str): + """ + Initialize the CSVMatrix. + """ + self._file = file + + # Load CSV matrix + path = ROOT.expand_path(self._file) + try: + self._mat = np.genfromtxt(path, delimiter=",", dtype=float, loose=False) + except ValueError as e: + raise PyAMLException(f"CSVMatrix(file='{self._file}',dtype=float): {str(e)}") from None + + @property + def file(self): + """Return the configured CSV file path.""" + return self._file + + def get_matrix(self) -> NDArray[np.float64]: + """ + Get the matrix data. + + Returns + ------- + np.array + Matrix data as a numpy array + """ + return self._mat + + def __repr__(self): + """ + Implement the ``__repr__`` string. + """ + return __pyaml_repr__(self) diff --git a/pyaml/magnet/curve.py b/pyaml/magnet/curve.py new file mode 100644 index 000000000..d541ec676 --- /dev/null +++ b/pyaml/magnet/curve.py @@ -0,0 +1,51 @@ +""" +Excitation-curve interfaces for magnet calibration. + +An excitation curve represents paired magnet-strength and hardware values as +an ``(n, 2)`` array. Concrete implementations provide those points from a +file or in-memory data, while :class:`Curve` supplies the inverse-curve +operation used for reverse conversion. +""" + +from abc import ABCMeta, abstractmethod + +import numpy as np + + +class Curve(metaclass=ABCMeta): + """ + Define the interface for a monotonic magnet excitation curve. + + Curves are represented by two columns of paired values and are used to + interpolate between physical magnet strengths and hardware setpoints. + + Methods + ------- + get_curve() + Returns the curve (n rows,2 columns). Curve is expected to be monotonic (non-decreasing or non-increasing). + inverse(curve) + Returns the inverse curve. Basically swap x and y and sort y in ascending order. + """ + + @abstractmethod + def get_curve(self) -> np.array: + """ + Returns the curve (n rows,2 columns). + Curve is expected to be monotonic (non-decreasing or non-increasing). + """ + pass + + @classmethod + def inverse(cls, curve: np.array) -> np.array: + """ + Returns the inverse curve. + Basically swap x and y and sort y in ascending order. + + Parameters + ---------- + curve : np.array + Curve to be inverted + """ + __curve = curve + __sortedCurve = __curve[__curve[:, 1].argsort()] + return __sortedCurve[:, [1, 0]] diff --git a/pyaml/magnet/function_mapping.py b/pyaml/magnet/function_mapping.py index 343f5d5d6..c1977e2b7 100644 --- a/pyaml/magnet/function_mapping.py +++ b/pyaml/magnet/function_mapping.py @@ -1,3 +1,10 @@ +""" +Function mappings used by magnet models. + +This module provides mappings between configured magnet functions and the +corresponding model or hardware channels. +""" + from pyaml.magnet.hcorrector import HCorrector from pyaml.magnet.octupole import Octupole from pyaml.magnet.quadrupole import Quadrupole diff --git a/pyaml/magnet/hcorrector.py b/pyaml/magnet/hcorrector.py index 964c4e292..84bfbfb2e 100644 --- a/pyaml/magnet/hcorrector.py +++ b/pyaml/magnet/hcorrector.py @@ -1,35 +1,92 @@ +""" +Horizontal orbit-corrector elements. + +This module defines the horizontal corrector configuration and runtime +interface, including its horizontal kick-angle access. +""" + +from typing import Self + from ..common import abstract from ..common.constants import HORIZONTAL_KICK_SIGN from ..lattice.polynom_info import PolynomInfo +from ..validation import DynamicValidation, register_schema from .corrector import RWCorrectorAngle -from .magnet import Magnet, MagnetConfigModel +from .magnet import Magnet +from .model import MagnetModel # Define the main class name for this module PYAMLCLASS = "HCorrector" -class ConfigModel(MagnetConfigModel): - """Configuration model for Horizontal Corrector magnet.""" +@register_schema +class HCorrector(Magnet, DynamicValidation): + """ + Represent a horizontal orbit corrector. - ... + Parameters + ---------- + name : str + Corrector name. + model : MagnetModel | None + Optional magnet model. + lattice_names : str | None + Optional lattice-element mapping. + description : str | None + Optional human-readable description. + Attributes + ---------- + angle + Return read/write access to the horizontal kick angle in radians. -class HCorrector(Magnet): - """Horizontal Corrector class""" + Methods + ------- + attach(peer, strength, hardware) + Return an attached copy with a bound horizontal-angle handle. + """ polynom = PolynomInfo("PolynomB", 0, HORIZONTAL_KICK_SIGN) - def __init__(self, cfg: ConfigModel): - super().__init__( - cfg.name, - cfg.model if hasattr(cfg, "model") else None, - ) - self._cfg = cfg + def __init__( + self, name: str, model: MagnetModel | None = None, lattice_names: str | None = None, description: str | None = None + ): + """ + Initialize the HCorrector. + """ + super().__init__(name, model, lattice_names, description) self.__angle = RWCorrectorAngle(self) @property def angle(self) -> abstract.ReadWriteFloatScalar: """ - Set the kick angle. + Return read/write access to the horizontal kick angle in radians. """ return self.__angle + + def attach( + self, + peer, + strength: abstract.ReadWriteFloatScalar, + hardware: abstract.ReadWriteFloatScalar, + ) -> Self: + """ + Return an attached copy with a bound horizontal-angle handle. + + Parameters + ---------- + peer : ElementHolder + Control system or simulator the copy is bound to. + strength : abstract.ReadWriteFloatScalar + Accessor for the physical strength on that peer. + hardware : abstract.ReadWriteFloatScalar + Accessor for the hardware value on that peer. + + Returns + ------- + Self + Copy of this magnet bound to ``peer``. + """ + obj = super().attach(peer, strength, hardware) + obj.__angle = RWCorrectorAngle(obj) + return obj diff --git a/pyaml/magnet/identity_cfm_model.py b/pyaml/magnet/identity_cfm_model.py index 8333b3b18..0f578f2cc 100644 --- a/pyaml/magnet/identity_cfm_model.py +++ b/pyaml/magnet/identity_cfm_model.py @@ -1,66 +1,129 @@ +""" +Identity conversion model for combined-function magnets. + +This model provides direct per-multipole conversion without excitation-curve interpolation. +""" + import numpy as np -from pydantic import BaseModel, ConfigDict from .. import PyAMLException from ..common.element import __pyaml_repr__ -from ..control.deviceaccess import DeviceAccess +from ..validation import DynamicValidation, register_schema from .model import MagnetModel # Define the main class name for this module PYAMLCLASS = "IdentityCFMagnetModel" -class ConfigModel(BaseModel): +@register_schema +class IdentityCFMagnetModel(MagnetModel, DynamicValidation): """ - Configuration model for identity combined function magnet model + Identity combined-function magnet model. + + This magnet model maps strengths and hardware values directly to the + underlying devices without applying any conversion. It is intended for cases + where the physics values and hardware values are identical, so the model acts + as an identity transform for all supported multipoles. Parameters - ---------- - multipoles : list[str] - List of supported functions: A0, B0, A1, B1, etc (i.e. [B0, A1, B2]) - powerconverters : list[DeviceAccess], optional - Power converter devices to apply current - physics : list[DeviceAccess], optional - Magnet devices to apply strength - units : list[str] - List of strength units (i.e. ['rad', 'm-1', 'm-2']) - """ - model_config = ConfigDict(arbitrary_types_allowed=True, extra="forbid") + multipoles : list[str] + List of supported multipoles, for example ["B0", "A1", "B2"]. + powerconverters : list[str | None] | None, optional + Names of the power converter devices used for hardware access. + physics : list[str | None] | None, optional + Names of the physics devices used for strength access. + units : list[str] | None, optional + List of units for the supported multipoles. - multipoles: list[str] - powerconverters: list[DeviceAccess | None] | None = None - physics: list[DeviceAccess | None] | None = None - units: list[str] + Raises + PyAMLException + If both physics and powerconverters are missing, if both are + provided at the same time, or if the configuration lengths do not match. -class IdentityCFMagnetModel(MagnetModel): - """ - Class that map values to underlying devices without conversion + Parameters + ---------- + multipoles : list[str] + List of supported multipoles, for example ["B0", "A1", "B2"]. + powerconverters : list[str | None] | None + Names of the power converter devices used for hardware access. + physics : list[str | None] | None + Names of the physics devices used for strength access. + units : list[str] | None + List of units for the supported multipoles. + + Methods + ------- + compute_hardware_values(strengths) + Convert magnet strengths to hardware values. + compute_strengths(currents) + Convert hardware values to magnet strengths. + get_strength_units() + Return the units of magnet strengths. + get_hardware_units() + Return the units of hardware values. + get_device_names() + Return the associated device names. + set_magnet_rigidity(brho) + Set the magnetic rigidity used for conversion. + has_physics() + Return whether the model provides physics strengths. + has_hardware() + Return whether the model provides hardware values. """ - def __init__(self, cfg: ConfigModel): - self._cfg = cfg + def __init__( + self, + multipoles: list[str], + powerconverters: list[str | None] | None = None, + physics: list[str | None] | None = None, + units: list[str] | None = None, + ): + """ + Initialize the IdentityCFMagnetModel. + """ + self.multipoles = multipoles + self._powerconverters = powerconverters + self._physics = physics + self.units = units # Check config - self.__nbFunction: int = len(cfg.multipoles) + self.__nbFunction: int = len(multipoles) - if cfg.physics is None and cfg.powerconverters is None: + if self._physics is None and self._powerconverters is None: raise PyAMLException("Invalid IdentityCFMagnetModel configuration,physics or powerconverters device required") - if cfg.physics is not None and cfg.powerconverters is not None: + if self._physics is not None and self._powerconverters is not None: raise PyAMLException( "Invalid IdentityCFMagnetModel configuration,physics or powerconverters device required but not both" ) - if cfg.physics: - self.__devices = cfg.physics + if self._physics: + self.__devices = self._physics else: - self.__devices = cfg.powerconverters + self.__devices = self._powerconverters self.__nbDev: int = len(self.__devices) - self.__check_len(cfg.units, "units", self.__nbFunction) + self.__check_len(self.units, "units", self.__nbFunction) def __check_len(self, obj, name, expected_len): + """ + Validate the length of a model configuration sequence. + + Parameters + ---------- + obj : object + Sequence whose length should be checked. + name : object + Configuration-field name used in an error message. + expected_len : object + Required number of entries. + + Raises + ------ + PyAMLException + If ``obj`` does not contain ``expected_len`` entries. + """ lgth = len(obj) if lgth != expected_len: raise PyAMLException( @@ -68,28 +131,70 @@ def __check_len(self, obj, name, expected_len): ) def compute_hardware_values(self, strengths: np.array) -> np.array: + """ + Convert magnet strengths to hardware values. + + Parameters + ---------- + strengths : np.array + Strength of each magnet function, ordered as declared by the model. + + Returns + ------- + np.array + Hardware value of each power converter, ordered as declared by the model. + """ return strengths def compute_strengths(self, currents: np.array) -> np.array: + """ + Convert hardware values to magnet strengths. + + Parameters + ---------- + currents : np.array + Hardware value of each power converter, ordered as declared by the model. + + Returns + ------- + np.array + Strength of each magnet function, ordered as declared by the model. + """ return currents def get_strength_units(self) -> list[str]: - return self._cfg.units + """Return the units of magnet strengths.""" + return self.units def get_hardware_units(self) -> list[str]: - return self._cfg.units + """Return the units of hardware values.""" + return self.units - def get_devices(self) -> list[DeviceAccess | None]: + def get_device_names(self) -> list[str | None]: + """Return the associated device names.""" return self.__devices def set_magnet_rigidity(self, brho: np.double): + """ + Set the magnetic rigidity used for conversion. + + Parameters + ---------- + brho : np.double + Magnetic rigidity in tesla metres. Ignored: an identity model applies no rigidity scaling. + """ pass def has_physics(self) -> bool: - return self._cfg.physics is not None + """Return whether the model provides physics strengths.""" + return self._physics is not None def has_hardware(self) -> bool: - return self._cfg.powerconverters is not None + """Return whether the model provides hardware values.""" + return self._powerconverters is not None def __repr__(self): + """ + Implement the ``__repr__`` string. + """ return __pyaml_repr__(self) diff --git a/pyaml/magnet/identity_model.py b/pyaml/magnet/identity_model.py index 9692de6dc..9d5f94f6a 100644 --- a/pyaml/magnet/identity_model.py +++ b/pyaml/magnet/identity_model.py @@ -1,78 +1,160 @@ +""" +Identity conversion model for magnets without calibration curves. + +This model passes physical values through to hardware values, subject to the configured units and magnetic-rigidity scaling. +""" + import numpy as np -from pydantic import BaseModel, ConfigDict + +from pyaml.validation import DynamicValidation, register_schema from .. import PyAMLException from ..common.element import __pyaml_repr__ -from ..control.deviceaccess import DeviceAccess from .model import MagnetModel # Define the main class name for this module PYAMLCLASS = "IdentityMagnetModel" -class ConfigModel(BaseModel): +@register_schema +class IdentityMagnetModel(MagnetModel, DynamicValidation): """ - Configuration model for identity magnet model + Identity magnet model. + + This model maps magnet strengths directly to hardware values without applying + any conversion. It is intended for cases where the physics value and the + hardware value are identical, so the model behaves as an identity transform. Parameters ---------- - powerconverter : DeviceAccess, optional - Power converter device to apply current - physics : DeviceAccess, optional - Magnet device to apply strength - unit : str - Unit of the strength (i.e. 1/m or m-1) - """ - - model_config = ConfigDict(arbitrary_types_allowed=True, extra="forbid") - - powerconverter: DeviceAccess | None = None - physics: DeviceAccess | None = None - unit: str - - -class IdentityMagnetModel(MagnetModel): - """ - Class that map value to underlying device without conversion + powerconverter : str | None, optional + Name of the power converter device used to apply current. + physics : str | None, optional + Name of the physics device used to apply strength. + unit : str | None, optional + Unit of the magnet strength and hardware value, for example ``"1/m"`` or + ``"m-1"``. + + Methods + ------- + compute_hardware_values(strengths) + Convert magnet strengths to hardware values. + compute_strengths(currents) + Convert hardware values to magnet strengths. + get_strength_units() + Return the units of magnet strengths. + get_hardware_units() + Return the units of hardware values. + get_device_names() + Return the associated device names. + set_magnet_rigidity(brho) + Set the magnetic rigidity used for conversion. + has_physics() + Return whether the model provides physics strengths. + has_hardware() + Return whether the model provides hardware values. + + Raises + ------ + PyAMLException + If both ``physics`` and ``powerconverter`` are missing, or if both are + provided at the same time. + + Notes + ----- + The model does not perform any numerical conversion: strengths are returned + as hardware values and hardware values are returned as strengths. """ - def __init__(self, cfg: ConfigModel): - self._cfg = cfg - self.__unit = cfg.unit - if cfg.physics is None and cfg.powerconverter is None: + def __init__( + self, + powerconverter: str | None = None, + physics: str | None = None, + unit: str | None = None, + ): + """ + Initialize the IdentityMagnetModel. + """ + self.physics = physics + self.powerconverter = powerconverter + self.unit = unit + + if self.physics is None and self.powerconverter is None: raise PyAMLException("Invalid IdentityMagnetModel configuration,physics or powerconverter device required") - if cfg.physics is not None and cfg.powerconverter is not None: + if self.physics is not None and self.powerconverter is not None: raise PyAMLException( "Invalid IdentityMagnetModel configuration,physics or powerconverter device required but not both" ) - if cfg.physics: - self.__device = cfg.physics + if self.physics: + self.__device = self.physics else: - self.__device = cfg.powerconverter + self.__device = self.powerconverter def compute_hardware_values(self, strengths: np.array) -> np.array: + """ + Convert magnet strengths to hardware values. + + Parameters + ---------- + strengths : np.array + Magnet strengths to convert, in the unit reported by :meth:`get_strength_unit`. + + Returns + ------- + np.array + Hardware values corresponding to ``strengths``. + """ return strengths def compute_strengths(self, currents: np.array) -> np.array: + """ + Convert hardware values to magnet strengths. + + Parameters + ---------- + currents : np.array + Hardware values to convert, in the unit reported by :meth:`get_hardware_unit`. + + Returns + ------- + np.array + Strengths corresponding to ``currents``. + """ return currents def get_strength_units(self) -> list[str]: - return [self.__unit] + """Return the units of magnet strengths.""" + return [self.unit] def get_hardware_units(self) -> list[str]: - return [self.__unit] + """Return the units of hardware values.""" + return [self.unit] - def get_devices(self) -> list[DeviceAccess]: + def get_device_names(self) -> list[str | None]: + """Return the associated device names.""" return [self.__device] def set_magnet_rigidity(self, brho: np.double): + """ + Set the magnetic rigidity used for conversion. + + Parameters + ---------- + brho : np.double + Magnetic rigidity in tesla metres. Ignored: an identity model applies no rigidity scaling. + """ pass def has_physics(self) -> bool: - return self._cfg.physics is not None + """Return whether the model provides physics strengths.""" + return self.physics is not None def has_hardware(self) -> bool: - return self._cfg.powerconverter is not None + """Return whether the model provides hardware values.""" + return self.powerconverter is not None def __repr__(self): + """ + Implement the ``__repr__`` string. + """ return __pyaml_repr__(self) diff --git a/pyaml/magnet/inline_curve.py b/pyaml/magnet/inline_curve.py new file mode 100644 index 000000000..1bc3a1c05 --- /dev/null +++ b/pyaml/magnet/inline_curve.py @@ -0,0 +1,85 @@ +""" +In-memory magnet excitation curves. + +This module validates and exposes two-column excitation data supplied directly +as Python sequences. +""" + +import numpy as np +from numpy.typing import NDArray + +from ..common.element import __pyaml_repr__ +from ..common.exception import PyAMLException +from ..validation import DynamicValidation, register_schema +from .curve import Curve + +# Define the main class name for this module +PYAMLCLASS = "InlineCurve" + + +@register_schema +class InlineCurve(Curve, DynamicValidation): + """ + Curve defined directly from an in-memory matrix of (x, y) points. + + This class stores curve data provided as a list of rows, where each row must + contain exactly two values: the x-coordinate and the y-coordinate. The data is + converted to a NumPy array and validated to ensure it has shape ``(n, 2)``. + + Parameters + ---------- + mat : list[list[float]] + Curve data as a two-column matrix. Each row represents one point in the + curve, with ``mat[i][0]`` being the x-value and ``mat[i][1]`` being the + y-value. + + Attributes + ---------- + mat + Return the original in-memory curve point matrix. + + Methods + ------- + get_curve() + Get the curve data. + + Raises + ------ + PyAMLException + If the provided matrix does not have two columns. + """ + + def __init__(self, mat: list[list[float]]): + """ + Initialize the InlineCurve. + """ + self._mat = mat + + # Load the curve + self._curve = np.array(self._mat) + + _s = np.shape(self._curve) + if len(_s) != 2 or _s[1] != 2: + raise PyAMLException(f"InlineCurve(mat='{self._mat}',dtype=float): wrong shape (2,2) expected but got {str(_s)}") + + @property + def mat(self): + """Return the original in-memory curve point matrix.""" + return self._mat + + def get_curve(self) -> NDArray[np.float64]: + """ + Get the curve data. + + Returns + ------- + np.array + Curve data as a 2D numpy array of shape (n, 2) + """ + return self._curve + + def __repr__(self): + """ + Implement the ``__repr__`` string. + """ + return __pyaml_repr__(self) diff --git a/pyaml/magnet/inline_matrix.py b/pyaml/magnet/inline_matrix.py new file mode 100644 index 000000000..d26b082a1 --- /dev/null +++ b/pyaml/magnet/inline_matrix.py @@ -0,0 +1,66 @@ +""" +Magnet response matrices. + +This module defines matrix representations used by magnet models. +""" + +import numpy as np +from numpy.typing import NDArray + +from ..common.element import __pyaml_repr__ +from ..validation import DynamicValidation, register_schema +from .matrix import Matrix + +# Define the main class name for this module +PYAMLCLASS = "InlineMatrix" + + +@register_schema +class InlineMatrix(Matrix, DynamicValidation): + """ + Matrix defined directly from in-memory data. + + Parameters + ---------- + mat : list[list[float]] + Matrix data given as a nested list of numbers. + + Attributes + ---------- + _mat : np.ndarray + Internal NumPy representation of the matrix. + + Methods + ------- + get_matrix() + Get the matrix data. + """ + + def __init__(self, mat: list[list[float]]): + # Load the matrix + """ + Initialize the InlineMatrix. + """ + self._mat = np.array(mat) + + @property + def mat(self): + """Return the original in-memory magnet matrix.""" + return self._mat + + def get_matrix(self) -> NDArray[np.float64]: + """ + Get the matrix data. + + Returns + ------- + np.array + Matrix data as a numpy array + """ + return self._mat + + def __repr__(self): + """ + Implement the ``__repr__`` string. + """ + return __pyaml_repr__(self) diff --git a/pyaml/magnet/linear_cfm_model.py b/pyaml/magnet/linear_cfm_model.py index c1795c124..75489526b 100644 --- a/pyaml/magnet/linear_cfm_model.py +++ b/pyaml/magnet/linear_cfm_model.py @@ -1,108 +1,172 @@ +""" +Linear conversion model for combined-function magnets. + +This model converts multiple multipole strengths to hardware values using per-function linear calibration parameters. +""" + import numpy as np -from pydantic import BaseModel, ConfigDict from ..common.element import __pyaml_repr__ from ..common.exception import PyAMLException -from ..configuration.curve import Curve -from ..configuration.matrix import Matrix -from ..control.deviceaccess import DeviceAccess +from ..validation import DynamicValidation, register_schema +from .curve import Curve +from .matrix import Matrix from .model import MagnetModel # Define the main class name for this module PYAMLCLASS = "LinearCFMagnetModel" -class ConfigModel(BaseModel): +@register_schema +class LinearCFMagnetModel(MagnetModel, DynamicValidation): """ - Configuration model for linear combined function magnet model + Linear combined-function magnet model. + + This model converts between magnet strengths and hardware currents using + precomputed excitation curves, optional calibration and pseudo-current + corrections, and an optional coupling matrix to separate or combine multipole + responses. It is intended for combined-function magnets where several + multipoles share a common hardware representation. Parameters - ---------- + multipoles : list[str] - List of supported functions: A0, B0, A1, B1, etc (i.e. [B0, A1, B2]) + Names of the supported multipoles, for example ["B0", "A1", "B2"]. curves : list[Curve] - Excitation curves, 1 curve per function - calibration_factors : list[float], optional - Correction factor applied to curves, 1 factor per function. - Default: ones - calibration_offsets : list[float], optional - Correction offset applied to curves, 1 offset per function. - Default: zeros - pseudo_factors : list[float], optional - Factors applied to 'pseudo currents', 1 factor per function. - Default: ones - pseudo_offsets : list[float], optional - Offsets applied to 'pseudo currents', 1 offset per function. - Default: zeros - powerconverters : list[DeviceAccess] - List of power converter devices to apply currents (can be different - from number of functions) - matrix : Matrix, optional - n x m matrix (n rows for n functions, m columns for m currents) - to handle multipoles separation. Default: Identity - units : list[str] - List of strength units (i.e. ['rad', 'm-1', 'm-2']) - """ + Excitation curves, one per multipole. + powerconverters : list[str | None] + Names of the power converter devices associated with the hardware currents. + hardware_units : list[str] + Units of the hardware variables, one per power converter. + calibration_factors : list[float] | None, optional + Multiplicative correction factors applied to the excitation curves. + Defaults to ones. + calibration_offsets : list[float] | None, optional + Additive correction offsets applied to the excitation curves. + Defaults to zeros. + pseudo_factors : list[float] | None, optional + Multiplicative factors applied to pseudo currents. + Defaults to ones. + pseudo_offsets : list[float] | None, optional + Additive offsets applied to pseudo currents. + Defaults to zeros. + matrix : Matrix | None, optional + Coupling matrix mapping power-supply currents to pseudo currents. + Defaults to the identity matrix. + units : list[str] | None, optional + Strength units, one per multipole. - model_config = ConfigDict(arbitrary_types_allowed=True, extra="forbid") + Raises - multipoles: list[str] - curves: list[Curve] - calibration_factors: list[float] = None - calibration_offsets: list[float] = None - pseudo_factors: list[float] = None - pseudo_offsets: list[float] = None - powerconverters: list[DeviceAccess | None] - matrix: Matrix = None - units: list[str] + PyAMLException + If the list lengths do not match, if the matrix has the wrong shape, or + if the configuration is otherwise inconsistent. + Parameters + ---------- + multipoles : list[str] + Names of the supported multipoles, for example ["B0", "A1", "B2"]. + curves : list[Curve] + Excitation curves, one per multipole. + powerconverters : list[str | None] + Names of the power converter devices associated with the hardware currents. + hardware_units : list[str] + Units of the hardware variables, one per power converter. + calibration_factors : list[float] | None + Multiplicative correction factors applied to the excitation curves. Defaults to ones. + calibration_offsets : list[float] | None + Additive correction offsets applied to the excitation curves. Defaults to zeros. + pseudo_factors : list[float] | None + Multiplicative factors applied to pseudo currents. Defaults to ones. + pseudo_offsets : list[float] | None + Additive offsets applied to pseudo currents. Defaults to zeros. + matrix : Matrix | None + Coupling matrix mapping power-supply currents to pseudo currents. Defaults to the identity matrix. + units : list[str] | None + Strength units, one per multipole. -class LinearCFMagnetModel(MagnetModel): - """ - Class providing a simple linear model for combined function magnets. A matrix - can handle separation of multipoles. A pseudo current is a linear combination - of power supply currents associated to a single function. + Methods + ------- + compute_hardware_values(strengths) + Convert magnet strengths to hardware values. + compute_strengths(currents) + Convert hardware values to magnet strengths. + get_strength_units() + Return the units of magnet strengths. + get_hardware_units() + Return the units of hardware values. + get_device_names() + Return the associated device names. + set_magnet_rigidity(brho) + Set the magnetic rigidity used for conversion. + has_hardware() + Return whether the model provides hardware values. """ - def __init__(self, cfg: ConfigModel): - self._cfg = cfg + def __init__( + self, + multipoles: list[str], + curves: list[Curve], + powerconverters: list[str | None], + hardware_units: list[str], + calibration_factors: list[float] | None = None, + calibration_offsets: list[float] | None = None, + pseudo_factors: list[float] | None = None, + pseudo_offsets: list[float] | None = None, + matrix: Matrix | None = None, + units: list[str] | None = None, + ): + """ + Initialize the LinearCFMagnetModel. + """ + self.multipoles = multipoles + self._curves = curves + self._powerconverters = powerconverters + self.hardware_units = hardware_units + self._calibration_factors = calibration_factors + self._calibration_offsets = calibration_offsets + self._pseudo_factors = pseudo_factors + self._pseudo_offsets = pseudo_offsets + self._matrix = matrix + self.units = units self._brho = np.nan # Check config - self.__nbFunction: int = len(cfg.multipoles) - self.__nbPS: int = len(cfg.powerconverters) + self.__nbFunction: int = len(self.multipoles) + self.__nbPS: int = len(self._powerconverters) - if cfg.calibration_factors is None: + if self._calibration_factors is None: self.__calibration_factors = np.ones(self.__nbFunction) else: - self.__calibration_factors = cfg.calibration_factors + self.__calibration_factors = self._calibration_factors - if cfg.calibration_offsets is None: + if self._calibration_offsets is None: self.__calibration_offsets = np.zeros(self.__nbFunction) else: - self.__calibration_offsets = cfg.calibration_offsets + self.__calibration_offsets = self._calibration_offsets - if cfg.pseudo_factors is None: + if self._pseudo_factors is None: self.__pf = np.ones(self.__nbFunction) else: - self.__pf = cfg.pseudo_factors + self.__pf = self._pseudo_factors - if cfg.pseudo_offsets is None: + if self._pseudo_offsets is None: self.__po = np.zeros(self.__nbFunction) else: - self.__po = cfg.pseudo_factors + self.__po = self._pseudo_factors self.__check_len(self.__calibration_factors, "calibration_factors", self.__nbFunction) self.__check_len(self.__calibration_offsets, "calibration_offsets", self.__nbFunction) self.__check_len(self.__pf, "pseudo_factors", self.__nbFunction) self.__check_len(self.__po, "pseudo_offsets", self.__nbFunction) - self.__check_len(cfg.units, "units", self.__nbFunction) - self.__check_len(cfg.curves, "curves", self.__nbFunction) + self.__check_len(self.units, "units", self.__nbFunction) + self.__check_len(self.hardware_units, "hardware_units", self.__nbPS) + self.__check_len(self._curves, "curves", self.__nbFunction) - if cfg.matrix is None: + if self._matrix is None: self.__matrix = np.identity(self.__nbFunction) else: - self.__matrix = cfg.matrix.get_matrix() + self.__matrix = self._matrix.get_matrix() _s = np.shape(self.__matrix) @@ -115,7 +179,7 @@ def __init__(self, cfg: ConfigModel): self.__rcurves = [] # Apply factor and offset - for idx, c in enumerate(cfg.curves): + for idx, c in enumerate(self._curves): self.__curves.append(c.get_curve()) self.__curves[idx][:, 1] *= self.__calibration_factors[idx] self.__curves[idx][:, 1] += self.__calibration_offsets[idx] @@ -125,6 +189,23 @@ def __init__(self, cfg: ConfigModel): self.__inv = np.linalg.pinv(self.__matrix) def __check_len(self, obj, name, expected_len): + """ + Validate the length of a model configuration sequence. + + Parameters + ---------- + obj : object + Sequence whose length should be checked. + name : object + Configuration-field name used in an error message. + expected_len : object + Required number of entries. + + Raises + ------ + PyAMLException + If ``obj`` does not contain ``expected_len`` entries. + """ lgth = len(obj) if lgth != expected_len: raise PyAMLException( @@ -132,6 +213,19 @@ def __check_len(self, obj, name, expected_len): ) def compute_hardware_values(self, strengths: np.array) -> np.array: + """ + Convert magnet strengths to hardware values. + + Parameters + ---------- + strengths : np.array + Strength of each magnet function, ordered as declared by the model. + + Returns + ------- + np.array + Hardware value of each power converter, ordered as declared by the model. + """ _pI = np.zeros(self.__nbFunction) for idx, c in enumerate(self.__rcurves): _pI[idx] = self.__pf[idx] * np.interp(strengths[idx] * self._brho, c[:, 0], c[:, 1]) + self.__po[idx] @@ -139,6 +233,19 @@ def compute_hardware_values(self, strengths: np.array) -> np.array: return _currents def compute_strengths(self, currents: np.array) -> np.array: + """ + Convert hardware values to magnet strengths. + + Parameters + ---------- + currents : np.array + Hardware value of each power converter, ordered as declared by the model. + + Returns + ------- + np.array + Strength of each magnet function, ordered as declared by the model. + """ _strength = np.zeros(self.__nbFunction) _pI = np.matmul(self.__matrix, currents) for idx, c in enumerate(self.__curves): @@ -146,19 +253,34 @@ def compute_strengths(self, currents: np.array) -> np.array: return _strength def get_strength_units(self) -> list[str]: - return self._cfg.units + """Return the units of magnet strengths.""" + return self.units def get_hardware_units(self) -> list[str]: - return np.array([p.unit() for p in self._cfg.powerconverters]) + """Return the units of hardware values.""" + return self.hardware_units - def get_devices(self) -> list[DeviceAccess]: - return self._cfg.powerconverters + def get_device_names(self) -> list[str | None]: + """Return the associated device names.""" + return self._powerconverters def set_magnet_rigidity(self, brho: np.double): + """ + Set the magnetic rigidity used for conversion. + + Parameters + ---------- + brho : np.double + Magnetic rigidity in tesla metres, used to scale strengths into hardware values. + """ self._brho = brho def has_hardware(self) -> bool: + """Return whether the model provides hardware values.""" return (self.__nbPS == self.__nbFunction) and np.allclose(self.__matrix, np.eye(self.__nbFunction)) def __repr__(self): + """ + Implement the ``__repr__`` string. + """ return __pyaml_repr__(self) diff --git a/pyaml/magnet/linear_model.py b/pyaml/magnet/linear_model.py index ac9b57e0f..148629bf5 100644 --- a/pyaml/magnet/linear_model.py +++ b/pyaml/magnet/linear_model.py @@ -1,70 +1,114 @@ +""" +Linear conversion model for single-function magnets. + +This model maps one magnet strength to one hardware value using linear calibration parameters and an optional excitation curve. +""" + import numpy as np -from pydantic import BaseModel, ConfigDict from ..common.element import __pyaml_repr__ -from ..configuration.curve import Curve -from ..control.deviceaccess import DeviceAccess +from ..validation import DynamicValidation, register_schema +from .curve import Curve from .model import MagnetModel # Define the main class name for this module PYAMLCLASS = "LinearMagnetModel" -class ConfigModel(BaseModel): +@register_schema +class LinearMagnetModel(MagnetModel, DynamicValidation): """ - Linear magnet model. + Linear magnet model for a single magnet function. + + This model converts between magnet strengths and hardware currents using a + single excitation curve or, if no curve is provided, a linear scaling with an + optional offset. It is intended for single-function magnets such as correctors + or other elements that use one current channel. Parameters ---------- - curve : Curve or None, optional - Curve object used for interpolation. By default, - identity curve is used. - powerconverter : DeviceAccess or None, optional - Power converter device to apply currrent + unit : str + Unit of the magnet strength, for example ``"1/m"`` or ``"m-1"``. + hardware_unit : str + Unit of the hardware value, for example ``"A"`` or ``"V"``. + curve : Curve | None, optional + Excitation curve used for interpolation. If omitted, a linear conversion + is used instead. + powerconverter : str | None, optional + Name of the power converter device used to apply current. calibration_factor : float, optional - Correction factor applied to the curve. Default: 1.0 + Multiplicative correction applied to the curve or linear scaling. + Default is ``1.0``. calibration_offset : float, optional - Correction offset applied to the curve. Default: 0.0 + Additive correction applied to the curve or linear scaling. + Default is ``0.0``. crosstalk : float, optional - Crosstalk factor. Default: 1.0 - unit : str - Unit of the strength (i.e. 1/m or m-1) - - """ - - model_config = ConfigDict(arbitrary_types_allowed=True, extra="forbid") - - curve: Curve | None = None - powerconverter: DeviceAccess | None - calibration_factor: float = 1.0 - calibration_offset: float = 0.0 - crosstalk: float = 1.0 - unit: str - - -class LinearMagnetModel(MagnetModel): - """ - Class that handle manget current/strength conversion using - linear interpolation for a single function magnet + Crosstalk factor applied together with the calibration factor. + Default is ``1.0``. + + Methods + ------- + compute_hardware_values(strengths) + Convert magnet strengths to hardware values. + compute_strengths(currents) + Convert hardware values to magnet strengths. + get_strength_units() + Return the units of magnet strengths. + get_hardware_units() + Return the units of hardware values. + get_device_names() + Return the associated device names. + set_magnet_rigidity(brho) + Set the magnetic rigidity used for conversion. + + Notes + ----- + If a curve is provided, the model interpolates between strength and current + values using the curve and its inverse. If no curve is provided, the model + uses a simple linear relation with the stored scaling factor and offset. """ - def __init__(self, cfg: ConfigModel): - self._cfg = cfg - if self._cfg.curve: - self.__curve = cfg.curve.get_curve() - self.__curve[:, 1] = self.__curve[:, 1] * cfg.calibration_factor * cfg.crosstalk + cfg.calibration_offset + def __init__( + self, + unit: str, + hardware_unit: str, + curve: Curve | None = None, + powerconverter: str | None = None, + calibration_factor: float = 1.0, + calibration_offset: float = 0.0, + crosstalk: float = 1.0, + ): + """ + Initialize the LinearMagnetModel. + """ + if curve: + self.__curve = curve.get_curve() + self.__curve[:, 1] = self.__curve[:, 1] * calibration_factor * crosstalk + calibration_offset self.__rcurve = Curve.inverse(self.__curve) else: self.__curve = None self.__rcurve = None - self.__g = cfg.calibration_factor * cfg.crosstalk - self.__o = cfg.calibration_offset - self.__strength_unit = cfg.unit - self.__hardware_unit = cfg.powerconverter.unit() + self.__g = calibration_factor * crosstalk + self.__o = calibration_offset + self.__strength_unit = unit + self.__hardware_unit = hardware_unit + self.__ps = powerconverter self.__brho = np.nan - self.__ps = cfg.powerconverter def compute_hardware_values(self, strengths: np.array) -> np.array: + """ + Convert magnet strengths to hardware values. + + Parameters + ---------- + strengths : np.array + Magnet strengths to convert, in the unit reported by :meth:`get_strength_unit`. + + Returns + ------- + np.array + Hardware values corresponding to ``strengths``. + """ if self.__rcurve is not None: _current = np.interp(strengths[0] * self.__brho, self.__rcurve[:, 0], self.__rcurve[:, 1]) else: @@ -72,6 +116,19 @@ def compute_hardware_values(self, strengths: np.array) -> np.array: return np.array([_current]) def compute_strengths(self, currents: np.array) -> np.array: + """ + Convert hardware values to magnet strengths. + + Parameters + ---------- + currents : np.array + Hardware values to convert, in the unit reported by :meth:`get_hardware_unit`. + + Returns + ------- + np.array + Strengths corresponding to ``currents``. + """ if self.__curve is not None: _strength = np.interp(currents[0], self.__curve[:, 0], self.__curve[:, 1]) / self.__brho else: @@ -79,16 +136,30 @@ def compute_strengths(self, currents: np.array) -> np.array: return np.array([_strength]) def get_strength_units(self) -> list[str]: + """Return the units of magnet strengths.""" return [self.__strength_unit] if self.__strength_unit is not None else [""] def get_hardware_units(self) -> list[str]: + """Return the units of hardware values.""" return [self.__hardware_unit] if self.__hardware_unit is not None else [""] - def get_devices(self) -> list[DeviceAccess]: + def get_device_names(self) -> list[str | None]: + """Return the associated device names.""" return [self.__ps] def set_magnet_rigidity(self, brho: np.double): + """ + Set the magnetic rigidity used for conversion. + + Parameters + ---------- + brho : np.double + Magnetic rigidity in tesla metres, used to scale strengths into hardware values. + """ self.__brho = brho def __repr__(self): + """ + Implement the ``__repr__`` string. + """ return __pyaml_repr__(self) diff --git a/pyaml/magnet/linear_serialized_model.py b/pyaml/magnet/linear_serialized_model.py index 6e6be33e3..7b30c2ea5 100644 --- a/pyaml/magnet/linear_serialized_model.py +++ b/pyaml/magnet/linear_serialized_model.py @@ -1,14 +1,16 @@ +""" +Linear conversion model for serialized magnets. + +This model applies linear calibration to a configurable sequence of serialized magnet elements and hardware channels. +""" + import numpy as np -from pydantic import BaseModel, ConfigDict from ..common.element import __pyaml_repr__ from ..common.exception import PyAMLException -from ..configuration.curve import Curve -from ..configuration.inline_curve import ConfigModel as InlineCurveModel -from ..configuration.inline_curve import InlineCurve -from ..configuration.matrix import Matrix -from ..control.deviceaccess import DeviceAccess -from .linear_model import ConfigModel as LinearConfigModel +from ..validation import DynamicValidation, register_schema +from .curve import Curve +from .inline_curve import InlineCurve from .linear_model import LinearMagnetModel from .model import MagnetModel @@ -16,40 +18,23 @@ PYAMLCLASS = "LinearSerializedMagnetModel" -class ConfigModel(BaseModel): +def _get_length(elem) -> int: """ - Configuration model for linear serialized magnet model + Return the number of serialized entries represented by a value. + + ``None`` represents no entries, a list represents one entry per item, and + any other value represents a single entry. Parameters ---------- - curves : Curve or list[Curve] - Excitation curves, 1 curve for all or 1 curve per magnet - calibration_factors : float or list[float], optional - Correction factor applied to curves, 1 factor for all or 1 factor per magnet. - Default: ones - calibration_offsets : float or list[float], optional - Correction offset applied to curves, 1 offset for all or 1 offset per magnet. - Default: zeros - crosstalk : float or list[float], optional - Crosstalk factors. Default: 1.0 - powerconverter : DeviceAccess - The hardware can be a single power supply or a list of power supplies. - If a list is provided, the same value will be affected to all of them - unit : str - Strength unit: rad, m-1, m-2 - """ - - model_config = ConfigDict(arbitrary_types_allowed=True, extra="forbid") + elem : object + Configuration value to inspect. - curves: Curve | list[Curve] - calibration_factors: float | list[float] = None - calibration_offsets: float | list[float] = None - crosstalk: float | list[float] = 1.0 - powerconverter: DeviceAccess - unit: str - - -def _get_length(elem) -> int: + Returns + ------- + int + Number of serialized entries represented by ``elem``. + """ if elem is None: return 0 if isinstance(elem, list): @@ -59,12 +44,46 @@ def _get_length(elem) -> int: def _get_max_length(*args, **kwargs) -> int: + """ + Return the largest serialized-entry count among the inputs. + + Each positional and keyword value is measured with :func:`_get_length`. + This is used to determine the sequence length needed when scalar and list + configuration values are supplied together. + + Parameters + ---------- + *args : object + Positional configuration values. + **kwargs : object + Keyword configuration values. + + Returns + ------- + int + Largest represented entry count, or ``0`` when no values are given. + """ max_args = max([_get_length(elem) for elem in args]) if args else 0 max_kwargs = max([_get_length(elem) for elem in kwargs.values()]) if kwargs else 0 return max(max_args, max_kwargs) def _to_list_of_length(elem, length: int) -> list: + """ + Expand a scalar configuration value to a list of the requested length. + + Parameters + ---------- + elem : object + Scalar or list configuration value. + length : int + Required list length when ``elem`` is scalar. + + Returns + ------- + list + The original list, or a list repeating ``elem`` ``length`` times. + """ if isinstance(elem, list): return elem else: @@ -72,6 +91,23 @@ def _to_list_of_length(elem, length: int) -> list: def _check_len(obj, name, expected_length): + """ + Validate the length of a serialized-magnet configuration sequence. + + Parameters + ---------- + obj : object + Sequence whose length should be checked. + name : object + Configuration-field name used in an error message. + expected_length : object + Required number of entries. + + Raises + ------ + PyAMLException + If ``obj`` does not contain ``expected_length`` entries. + """ length = len(obj) if length != expected_length: raise PyAMLException( @@ -79,47 +115,129 @@ def _check_len(obj, name, expected_length): ) -class LinearSerializedMagnetModel(MagnetModel): +@register_schema +class LinearSerializedMagnetModel(MagnetModel, DynamicValidation): """ - Class providing a simple linear model for combined function magnets. A matrix - can handle separation of multipoles. A pseudo current is a linear combination - of power supply currents associated to a single function. + Linear model for a serialized combined-function magnet. + + This model wraps one or more :class:`LinearMagnetModel` instances and + represents a combined-function magnet as a set of sub-models that share a + common hardware readout. The excitation curve may be provided either as a + single :class:`Curve` instance, which is replicated for all magnets, or as a + list of curves with one entry per magnet. + + The model supports per-magnet calibration factors, calibration offsets, and + crosstalk values. Strengths are converted to a single hardware current by + evaluating the individual sub-models and averaging their corresponding + hardware values. Conversely, a hardware current is mapped back to a + strength value for each sub-model. + + Parameters + ---------- + curves : Curve or list[Curve] + Excitation curve(s) used by the magnet model. A single curve is reused + for all magnets, while a list must contain one curve per magnet. + calibration_factors : float or list[float], optional + Multiplicative correction factor applied to each curve. + If omitted, defaults to 1.0 for all magnets. + calibration_offsets : float or list[float], optional + Additive correction offset applied to each curve. + If omitted, defaults to 0.0 for all magnets. + crosstalk : float or list[float], optional + Crosstalk factor for each magnet. If omitted, defaults to 1.0. + powerconverter : str, optional + Name of the associated power converter or power converter group. + unit : str, optional + Strength unit, such as ``rad``, ``m-1`` or ``m-2``. + hardware_unit : str, optional + Hardware unit, typically ``A`` or ``V``. + + Methods + ------- + set_number_of_magnets(nb_magnets) + Set the number of serialized magnets and rebuild submodels. + get_sub_model(index) + Return the linear submodel for one serialized magnet. + compute_hardware_values(strengths) + Convert magnet strengths to hardware values. + compute_strengths(currents) + Convert hardware values to magnet strengths. + get_strength_units() + Return the units of magnet strengths. + get_hardware_units() + Return the units of hardware values. + get_device_names() + Return the associated device names. + set_magnet_rigidity(brho) + Set the magnetic rigidity used for conversion. + get_magnet_rigidity() + Return the configured magnetic rigidity. + + Notes + ----- + The number of magnets is inferred from the longest list among the supplied + configuration values. Scalars are expanded to match that length. """ - def __init__(self, cfg: ConfigModel): - self._cfg = cfg + def __init__( + self, + curves: Curve | list[Curve], + calibration_factors: float | list[float] | None = None, + calibration_offsets: float | list[float] | None = None, + crosstalk: float | list[float] = 1.0, + powerconverter: str | None = None, + unit: str | None = None, + hardware_unit: str | None = None, + ): + """ + Initialize a linear model for serialized magnets. + """ self.__brho = np.nan + self._curves = curves + self._calibration_factors = calibration_factors + self._calibration_offsets = calibration_offsets + self._crosstalk = crosstalk + self._powerconverter = powerconverter + self._unit = unit + self._hardware_unit = hardware_unit # Check config - self.__nbMagnets: int = _get_max_length(cfg.curves, cfg.calibration_factors, cfg.calibration_offsets, cfg.crosstalk) + self.__nbMagnets: int = _get_max_length(curves, calibration_factors, calibration_offsets, crosstalk) self.__calibration_factors = np.ones(self.__nbMagnets) self.__calibration_offsets = np.ones(self.__nbMagnets) self.__crosstalk = np.ones(self.__nbMagnets) - self.__curves = _to_list_of_length(self._cfg.curves, self.__nbMagnets) + self.__curves = _to_list_of_length(curves, self.__nbMagnets) self.__sub_models: list[LinearMagnetModel] = [] def __initialize(self): - if self._cfg.calibration_factors is None: + """ + Normalize serialized-magnet calibration and build submodels. + + Scalar calibration values are expanded to the configured number of + magnets, sequence lengths are validated, and one + :class:`LinearMagnetModel` is created for each serialized element. + """ + if self._calibration_factors is None: self.__calibration_factors = np.ones(self.__nbMagnets) else: - self.__calibration_factors = _to_list_of_length(self._cfg.calibration_factors, self.__nbMagnets) + self.__calibration_factors = _to_list_of_length(self._calibration_factors, self.__nbMagnets) - if self._cfg.calibration_offsets is None: + if self._calibration_offsets is None: self.__calibration_offsets = np.zeros(self.__nbMagnets) else: - self.__calibration_offsets = _to_list_of_length(self._cfg.calibration_offsets, self.__nbMagnets) + self.__calibration_offsets = _to_list_of_length(self._calibration_offsets, self.__nbMagnets) - if self._cfg.crosstalk is None: + if self._crosstalk is None: self.__crosstalk = np.zeros(self.__nbMagnets) else: - self.__crosstalk = _to_list_of_length(self._cfg.crosstalk, self.__nbMagnets) - self.__curves = _to_list_of_length(self._cfg.curves, self.__nbMagnets) - if isinstance(self._cfg.curves, list): - self.__curves = self._cfg.curves + self.__crosstalk = _to_list_of_length(self._crosstalk, self.__nbMagnets) + self.__curves = _to_list_of_length(self._curves, self.__nbMagnets) + if isinstance(self._curves, list): + self.__curves = self._curves else: self.__curves: list[Curve] = [] for _ in range(self.__nbMagnets): - curve = InlineCurve(InlineCurveModel(mat=self._cfg.curves.get_curve())) + curve = InlineCurve(mat=self._curves.get_curve()) self.__curves.append(curve) _check_len(self.__calibration_factors, "calibration_factors", self.__nbMagnets) @@ -129,46 +247,109 @@ def __initialize(self): self.__sub_models: list[LinearMagnetModel] = [] for magnet_idx in range(self.__nbMagnets): - sub_model = LinearConfigModel( + sub_model = dict( curve=self.__curves[magnet_idx], calibration_factor=self.__calibration_factors[magnet_idx], calibration_offset=self.__calibration_offsets[magnet_idx], crosstalk=self.__crosstalk[magnet_idx], - powerconverter=self._cfg.powerconverter, - unit=self._cfg.unit, + powerconverter=self._powerconverter, + unit=self._unit, + hardware_unit=self._hardware_unit, ) - self.__sub_models.append(LinearMagnetModel(sub_model)) + self.__sub_models.append(LinearMagnetModel(**sub_model)) def set_number_of_magnets(self, nb_magnets: int): + """ + Set the number of serialized magnets and rebuild submodels. + + Parameters + ---------- + nb_magnets : int + Number of serialized magnets represented by the model. + """ self.__nbMagnets = nb_magnets self.__initialize() def get_sub_model(self, index: int) -> LinearMagnetModel: + """ + Return the linear submodel for one serialized magnet. + + Parameters + ---------- + index : int + Zero-based serialized-magnet index. + + Returns + ------- + LinearMagnetModel + Linear conversion model for the selected magnet. + """ return self.__sub_models[index] def compute_hardware_values(self, strengths: np.array) -> np.array: + """ + Convert magnet strengths to hardware values. + + Parameters + ---------- + strengths : np.array + Physical strengths, one per serialized magnet. + + Returns + ------- + np.array + Hardware value obtained from the submodels. + """ currents = [model.compute_hardware_values([s])[0] for s, model in zip(strengths, self.__sub_models, strict=True)] return np.array([np.mean(currents)]) def compute_strengths(self, currents: np.array) -> np.array: + """ + Convert hardware values to magnet strengths. + + Parameters + ---------- + currents : np.array + Hardware value shared by the serialized magnets. + + Returns + ------- + np.array + Physical strength calculated for each serialized magnet. + """ current = currents[0] return np.array([model.compute_strengths([current])[0] for model in self.__sub_models]) def get_strength_units(self) -> list[str]: - return [self._cfg.unit] * self.__nbMagnets + """Return the units of magnet strengths.""" + return [self._unit] * self.__nbMagnets def get_hardware_units(self) -> list[str]: - return [self.__sub_models[0].get_hardware_units()[0]] + """Return the units of hardware values.""" + return [self._hardware_unit] - def get_devices(self) -> list[DeviceAccess]: - return [self._cfg.powerconverter] + def get_device_names(self) -> list[str | None]: + """Return the associated device names.""" + return [self._powerconverter] def set_magnet_rigidity(self, brho: np.double): + """ + Set the magnetic rigidity used for conversion. + + Parameters + ---------- + brho : np.double + Magnetic rigidity in tesla-metres used by the submodels. + """ self.__brho = brho [model.set_magnet_rigidity(brho) for model in self.__sub_models] def get_magnet_rigidity(self) -> np.double: + """Return the configured magnetic rigidity.""" return self.__brho def __repr__(self): + """ + Implement the ``__repr__`` string. + """ return __pyaml_repr__(self) diff --git a/pyaml/magnet/magnet.py b/pyaml/magnet/magnet.py index d98b5ca72..b01491d73 100644 --- a/pyaml/magnet/magnet.py +++ b/pyaml/magnet/magnet.py @@ -1,47 +1,76 @@ +""" +Base interfaces for physical and simulated magnets. + +This module defines the common magnet element interface and its access to +strength, hardware, and magnet-model information. +""" + +import copy +from typing import TYPE_CHECKING, Self + +import numpy as np from scipy.constants import speed_of_light from .. import PyAMLException from ..common import abstract -from ..common.element import Element, ElementConfigModel +from ..common.element import Element, __pyaml_repr__ from .model import MagnetModel -try: - from typing import Self # Python 3.11+ -except ImportError: - from typing_extensions import Self # Python 3.10 and earlier -import numpy as np - +if TYPE_CHECKING: + from ..common.holders.element_holder import ElementHolder -class MagnetConfigModel(ElementConfigModel): - """ - Configuration model for magnet elements. - Attributes - ---------- - model : MagnetModel or None, optional - Object in charge of converting magnet strengths to power supply values +class Magnet(Element): """ + Access one magnet of a physical or simulated lattice. - model: MagnetModel | None = None + A magnet couples a device to its calibration: the attached + :class:`~pyaml.magnet.model.MagnetModel` owns the strength to hardware-current + conversion and the underlying control-system device names. The same magnet is + therefore readable and writable both as a physical strength and as a raw + hardware value. + Parameters + ---------- + name : str + Element name. + model : MagnetModel | None, optional + Magnet model used to convert between strength and hardware value, and to + resolve the underlying control-system device names. + lattice_names : str | None, optional + Name or names of the matching element(s) in the simulated lattice. Defaults + to ``name``. + description : str | None, optional + Human-readable description of the magnet. -class Magnet(Element): - """ - Class providing access to one magnet of a physical or simulated lattice + Attributes + ---------- + strength + Read/write accessor for the physical strength, in the model's strength unit. + hardware + Read/write accessor for the hardware value, in the model's hardware unit. + model + Magnet model performing the strength to hardware conversion. + + Methods + ------- + attach(peer, strength, hardware) + Return a copy of this magnet bound to a control system or simulator. + set_energy(energy) + Set the energy in eV to compute and set the magnet rigidity on the underlying magnet model. + set_model_name(name) + Sets the name of this magnet in the model (Used for combined function magnet) + get_model_name() + Returns the model name of this magnet """ - def __init__(self, name: str, model: MagnetModel = None): + def __init__( + self, name: str, model: MagnetModel | None = None, lattice_names: str | None = None, description: str | None = None + ): """ Construct a magnet - - Parameters - ---------- - name : str - Element name - model : MagnetModel - Magnet model in charge of computing coil(s) current """ - super().__init__(name) + super().__init__(name, lattice_names, description) self.__model = model self.__strength: abstract.ReadWriteFloatScalar = None self.__hardware: abstract.ReadWriteFloatScalar = None @@ -82,16 +111,32 @@ def attach( hardware: abstract.ReadWriteFloatScalar, ) -> Self: """ - Create a new reference to attach this magnet to a simulator - or a control systemand. - """ - obj = self.__class__(self._cfg) + Return a copy of this magnet bound to a control system or simulator. + + Parameters + ---------- + peer : ElementHolder + Control system or simulator the copy is bound to. + strength : abstract.ReadWriteFloatScalar + Accessor for the physical strength on that peer. + hardware : abstract.ReadWriteFloatScalar + Accessor for the hardware value on that peer. + + Returns + ------- + Self + Copy of this magnet bound to ``peer``. + """ + obj = copy.copy(self) obj.__modelName = self.__modelName obj.__strength = strength obj.__hardware = hardware obj._peer = peer return obj + def _fill_device(self, holder: "ElementHolder") -> None: + holder._fill_magnet(self) + def set_energy(self, energy: float): """ Set the energy in eV to compute and set the magnet rigidity @@ -103,7 +148,7 @@ def set_energy(self, energy: float): def set_model_name(self, name: str): """ Sets the name of this magnet in the model - (Used for combined function manget) + (Used for combined function magnet) """ self.__modelName = name @@ -113,11 +158,13 @@ def get_model_name(self) -> str: """ return self.__modelName + @property + def model_name(self) -> str: + """Name used to identify this magnet in its model.""" + return self.__modelName + def __repr__(self): - return "%s(peer='%s', name='%s', model_name='%s', magnet_model=%s)" % ( - self.__class__.__name__, - self.get_peer_name(), - self.get_name(), - self.__modelName, - repr(self.__model), - ) + """ + Implement the ``__repr__`` string. + """ + return __pyaml_repr__(self, exclude=["strength", "hardware"]) diff --git a/pyaml/configuration/matrix.py b/pyaml/magnet/matrix.py similarity index 60% rename from pyaml/configuration/matrix.py rename to pyaml/magnet/matrix.py index dc5b9ac71..580a9b94e 100644 --- a/pyaml/configuration/matrix.py +++ b/pyaml/magnet/matrix.py @@ -1,3 +1,9 @@ +""" +Magnet response matrices. + +This module defines matrix representations used by magnet models. +""" + from abc import ABCMeta, abstractmethod from numpy import array @@ -6,6 +12,11 @@ class Matrix(metaclass=ABCMeta): """ Abstract class providing access to a matrix + + Methods + ------- + get_matrix() + Returns the matrix """ @abstractmethod diff --git a/pyaml/magnet/model.py b/pyaml/magnet/model.py index 4b48c546d..47ffe3661 100644 --- a/pyaml/magnet/model.py +++ b/pyaml/magnet/model.py @@ -1,15 +1,39 @@ +""" +Abstract interfaces for magnet conversion models. + +The :class:`MagnetModel` contract covers conversion between physical strengths +and hardware setpoints, unit metadata, device names, and magnetic rigidity. +""" + from abc import ABCMeta, abstractmethod import numpy as np import numpy.typing as npt -from ..control.deviceaccess import DeviceAccess - class MagnetModel(metaclass=ABCMeta): """ - Abstract class providing strength to coil current conversion - and access to underlying power supplies + Define the interface for magnet strength and hardware conversion. + + Concrete models implement the relationship between accelerator physics + strengths and power-supply values for one or more magnet functions. + + Methods + ------- + compute_hardware_values(strengths) + Compute hardware value(s) from magnet strength(s) + compute_strengths(hardware_values) + Compute magnet strength(s) from hardware value(s) + get_strength_units() + Get strength units + get_device_names() + Return the control-system device names used by this model. + set_magnet_rigidity(brho) + Set the magnet rigidity. + has_hardware() + Tells if the model allows to work in hardware unit. + has_physics() + Tells if the model allows to work in physics unit. """ @abstractmethod @@ -62,38 +86,25 @@ def get_strength_units(self) -> list[str]: pass @abstractmethod - def get_hardware_units(self) -> list[str]: - """ - Get hardware units - - Returns - ------- - list[str] - Array of hardware units. For a single multipole, - returns a list of 1 item - """ - pass - - @abstractmethod - def get_devices(self) -> list[DeviceAccess | None]: + def get_device_names(self) -> list[str | None]: """ - Get device handles + Return the control-system device names used by this model. Returns ------- - list[DeviceAccess] - Array of DeviceAcess + list[str | None] + Array of associated device names. """ pass @abstractmethod def set_magnet_rigidity(self, brho: np.double): """ - Set magnet rigidity + Set the magnet rigidity. Parameters ---------- - brho: np.double + brho : np.double Magnet rigidity used to calculate power supply setpoints """ pass diff --git a/pyaml/magnet/octupole.py b/pyaml/magnet/octupole.py index d9710a093..2247c1afd 100644 --- a/pyaml/magnet/octupole.py +++ b/pyaml/magnet/octupole.py @@ -1,24 +1,51 @@ +""" +Octupole magnet elements. + +This module defines normal octupole configuration and runtime interfaces. +""" + from ..lattice.polynom_info import PolynomInfo -from .magnet import Magnet, MagnetConfigModel +from ..validation import DynamicValidation, register_schema +from .magnet import Magnet +from .model import MagnetModel # Define the main class name for this module PYAMLCLASS = "Octupole" -class ConfigModel(MagnetConfigModel): - """Configuration model for Octupole magnet.""" - - ... - - -class Octupole(Magnet): - """Octupole class""" +@register_schema +class Octupole(Magnet, DynamicValidation): + """ + Normal octupole magnet element. + + The strength is applied to the ``PolynomB[3]`` component of the underlying lattice element, the + field component used for controlling amplitude-dependent tune shift. Strengths are expressed in + ``m-3`` and converted to power-converter values by the attached magnet model. + + Parameters + ---------- + name : str + Element name. + model : MagnetModel | None, optional + Magnet model used to convert between strength and hardware value, and to + resolve the underlying control-system device names. + lattice_names : str | None, optional + Name or names of the matching element(s) in the simulated lattice. Defaults + to ``name``. + description : str | None, optional + Human-readable description of the magnet. + + See Also + -------- + Magnet : Base class listing the strength and hardware accessors. + """ polynom = PolynomInfo("PolynomB", 3) - def __init__(self, cfg: ConfigModel): - super().__init__( - cfg.name, - cfg.model if hasattr(cfg, "model") else None, - ) - self._cfg = cfg + def __init__( + self, name: str, model: MagnetModel | None = None, lattice_names: str | None = None, description: str | None = None + ): + """ + Initialize the Octupole. + """ + super().__init__(name, model, lattice_names, description) diff --git a/pyaml/magnet/quadrupole.py b/pyaml/magnet/quadrupole.py index 3c720ab6d..c3b749a12 100644 --- a/pyaml/magnet/quadrupole.py +++ b/pyaml/magnet/quadrupole.py @@ -1,24 +1,51 @@ +""" +Quadrupole magnet elements. + +This module defines normal quadrupole configuration and runtime interfaces. +""" + from ..lattice.polynom_info import PolynomInfo -from .magnet import Magnet, MagnetConfigModel +from ..validation import DynamicValidation, register_schema +from .magnet import Magnet +from .model import MagnetModel # Define the main class name for this module PYAMLCLASS = "Quadrupole" -class ConfigModel(MagnetConfigModel): - """Configuration model for Quadrupole magnet.""" - - ... - - -class Quadrupole(Magnet): - """Quadrupole class""" +@register_schema +class Quadrupole(Magnet, DynamicValidation): + """ + Normal quadrupole magnet element. + + The strength is applied to the ``PolynomB[1]`` component of the underlying lattice element, the + field component used for focusing or defocusing the beam. Strengths are expressed in ``m-1`` and + converted to power-converter values by the attached magnet model. + + Parameters + ---------- + name : str + Element name. + model : MagnetModel | None, optional + Magnet model used to convert between strength and hardware value, and to + resolve the underlying control-system device names. + lattice_names : str | None, optional + Name or names of the matching element(s) in the simulated lattice. Defaults + to ``name``. + description : str | None, optional + Human-readable description of the magnet. + + See Also + -------- + Magnet : Base class listing the strength and hardware accessors. + """ polynom = PolynomInfo("PolynomB", 1) - def __init__(self, cfg: ConfigModel): - super().__init__( - cfg.name, - cfg.model if hasattr(cfg, "model") else None, - ) - self._cfg = cfg + def __init__( + self, name: str, model: MagnetModel | None = None, lattice_names: str | None = None, description: str | None = None + ): + """ + Initialize the Quadrupole. + """ + super().__init__(name, model, lattice_names, description) diff --git a/pyaml/magnet/serialized_magnet.py b/pyaml/magnet/serialized_magnet.py index a5d1fdf7f..58ef44222 100644 --- a/pyaml/magnet/serialized_magnet.py +++ b/pyaml/magnet/serialized_magnet.py @@ -1,120 +1,298 @@ +""" +Serialized magnet elements. + +This module defines magnet elements composed of multiple serialized magnets. +""" + +from typing import TYPE_CHECKING + import numpy as np from scipy.constants import speed_of_light from .. import PyAMLException from ..common import abstract -from ..common.element import Element, ElementConfigModel, __pyaml_repr__ -from ..configuration import Factory -from ..control.deviceaccess import DeviceAccess +from ..common.element import Element, __pyaml_repr__ +from ..configuration.factory import ELEMENT_REGISTRY +from ..validation import DynamicValidation, register_schema from .function_mapping import function_map -from .magnet import Magnet, MagnetConfigModel +from .magnet import Magnet from .model import MagnetModel +if TYPE_CHECKING: + from ..common.holders.element_holder import ElementHolder + # Define the main class name for this module PYAMLCLASS = "SerializedMagnets" -class ConfigModel(ElementConfigModel): - function: str - """List of magnets""" - elements: list[str] | str - """List of magnets""" - model: MagnetModel | None = None - """Object in charge of converting magnet strengths to currents""" +class ReadWriteSerializedStrengths(abstract.ReadWriteFloatScalar): + """ + Read/write aggregate for serialized-magnet strengths. + Parameters + ---------- + elements : list[abstract.ReadWriteFloatScalar] + Per-magnet accessors sharing the group setpoint. + model : MagnetModel | None + Magnet model used to convert between strength and hardware value. Optional for a hardware-only group. + + Methods + ------- + get() + Return the sum of the serialized element strengths. + set(value) + Set the shared serialized-magnet strength. + set_and_wait(value) + Set the shared strength and wait for convergence. + unit() + Return the physical strength unit. + get_model() + Return the magnet conversion model. + get_elements() + Return the underlying scalar element accessors. + set_magnet_rigidity(brho) + Set the magnetic rigidity used for conversion. + """ -class ReadWriteSerializedStrengths(abstract.ReadWriteFloatScalar): - def __init__(self, cfg: ConfigModel, elements: list[abstract.ReadWriteFloatScalar]): + def __init__( + self, + elements: list[abstract.ReadWriteFloatScalar], + model: MagnetModel | None = None, + ): + """ + Initialize a shared strength accessor for serialized elements. + """ self.elements = elements - self._cfg = cfg + self.model = model def get(self) -> float: + """Return the sum of the serialized element strengths.""" return sum([elem.get() for elem in self.elements]) def set(self, value: float): + """ + Set the shared serialized-magnet strength. + + Parameters + ---------- + value : float + Strength applied to every magnet of the group. + """ self.elements[0].set(value) def set_and_wait(self, value: float): + """ + Set the shared strength and wait for convergence. + + Parameters + ---------- + value : float + Strength applied to every magnet of the group. + + Raises + ------ + NotImplementedError + Waiting for readback convergence is not implemented for this accessor. + """ raise NotImplementedError("Not implemented yet.") def unit(self) -> str: - return self._cfg.model.get_strength_units()[0] + """Return the physical strength unit.""" + return self.model.get_strength_units()[0] def get_model(self) -> MagnetModel: - return self._cfg.model + """Return the magnet conversion model.""" + return self.model def get_elements(self): + """Return the underlying scalar element accessors.""" return self.elements def set_magnet_rigidity(self, brho: np.double): + """ + Set the magnetic rigidity used for conversion. + + Parameters + ---------- + brho : np.double + Magnetic rigidity in tesla metres, forwarded to the magnet model. + """ [element.set_magnet_rigidity(brho) for element in self.elements] class ReadWriteSerializedHardwares(ReadWriteSerializedStrengths): - def __init__(self, cfg: ConfigModel, elements: list[abstract.ReadWriteFloatScalar]): - super().__init__(cfg, elements) + """ + Read/write aggregate for serialized-magnet hardware values. + + Parameters + ---------- + elements : list[abstract.ReadWriteFloatScalar] + Per-magnet accessors sharing the group setpoint. + model : MagnetModel | None + Magnet model used to convert between strength and hardware value. Optional for a hardware-only group. + + Methods + ------- + unit() + Return the hardware-value unit. + set_magnet_rigidity(brho) + Set the magnetic rigidity used for conversion. + """ + + def __init__( + self, + elements: list[abstract.ReadWriteFloatScalar], + model: MagnetModel | None = None, + ): + """ + Initialize a shared hardware accessor for serialized elements. + """ + super().__init__(elements, model) def unit(self) -> str: - return self._cfg.model.get_hardware_units()[0] + """Return the hardware-value unit.""" + return self.model.get_hardware_units()[0] def set_magnet_rigidity(self, brho: np.double): + """ + Set the magnetic rigidity used for conversion. + + Parameters + ---------- + brho : np.double + Magnetic rigidity in tesla metres, forwarded to the magnet model. + """ [element.set_magnet_rigidity(brho) for element in self.elements] -class SerializedMagnets(Element): +@register_schema +class SerializedMagnets(Element, DynamicValidation): """ - Class managing serialized magnets: a set of magnet with the same set point. - The set point is usually managed by only one power supply but it can be covered by several ones. - If several power supplies + Serialized group of magnets that share the same set point. + This class represents a set of magnets that are controlled together as a + single logical device. The serialized magnets may be driven by one power + supply or by several power supplies, but they share a common physics or + hardware set point through a combined read/write interface. Parameters ---------- - cfg : ConfigModel - Configuration object TODO: to describe + name : str + Name of the serialized magnet group. + function : str + Magnet function identifier used to select the concrete virtual magnet type. + elements : list[str] | str + Names of the individual magnets in the group. + model : MagnetModel | None, optional + Magnet model used to convert between strengths and hardware values. + description : str | None, optional + Human-readable description of the serialized magnet group. + peer : object, optional + Control-system or simulator peer used when attaching the magnet group. + + Attributes + ---------- + strength + Gives access to the strengths of those magnets in physics unit + hardware + Gives access to the strengths of this those magnets in hardware unit when possible + + Methods + ------- + get_nb_magnets() + Return the number of magnets in the serialized group. + get_magnets() + Return the group's virtual single-function magnets. + attach(peer, strengths, hardwares) + Attach the group and its virtual magnets to a runtime peer. + set_energy(energy) + Set beam energy for serialized-magnet strength conversion. + get_device_names() + Return the associated device names. Raises ------ - pyaml.PyAMLException - In case of wrong initialization + PyAMLException + If the requested function is not implemented or if the configuration is + invalid. + + Notes + ----- + The serialized group stores a virtual magnet for each underlying element. When + attached, each virtual magnet is bound to the same peer and the group exposes + aggregate strength and hardware accessors. """ - def __init__(self, cfg: ConfigModel, peer=None): - super().__init__(cfg.name) - self._cfg = cfg - self.model = cfg.model + def __init__( + self, + name: str, + function: str, + elements: list[str] | str, + model: MagnetModel | None = None, + description: str | None = None, + peer=None, + ): + """ + Initialize a group of magnets sharing one setpoint. + """ + super().__init__(name, None, description) + + self.function = function + self.model = model + self.polynom = None self.__strengths = None self.__hardwares = None self.__virtuals: list[Magnet] = [] - self.__elements = cfg.elements if isinstance(cfg.elements, list) else [cfg.elements] + self.__elements = elements if isinstance(elements, list) else [elements] self.model.set_number_of_magnets(len(self.__elements)) if peer is None: # Configuration part - self.polynom = function_map[self._cfg.function].polynom - if self._cfg.function not in function_map: - raise PyAMLException(self._cfg.function + " not implemented for serialized magnet") + self.polynom = function_map[self.function].polynom + if self.function not in function_map: + raise PyAMLException(self.function + " not implemented for serialized magnet") for element in self.__elements: # Check mapping validity # Create the virtual magnet for the corresponding magnet vm = self.__create_virtual_magnet(element) self.__virtuals.append(vm) # Register the virtual element in the factory to have a coherent factory and improve error reporting - Factory.register_element(vm) + ELEMENT_REGISTRY.register(vm) else: # Attach self._peer = peer + def _fill_device(self, holder: "ElementHolder") -> None: + holder._fill_serialized_magnets(self) + def __create_virtual_magnet(self, name: str) -> Magnet: + """ + Create a virtual magnet for one serialized element. + + The configured function mapping selects the concrete magnet class, and + the serialized group's model is shared with the new virtual magnet. + + Parameters + ---------- + name : str + Name assigned to the virtual magnet. + + Returns + ------- + Magnet + Newly created virtual magnet linked to the serialized group. + """ args = {"name": name, "model": self.model} - virtual: Magnet = function_map[self._cfg.function](MagnetConfigModel(**args)) + virtual: Magnet = function_map[self.function](**args) virtual.set_model_name(self.get_name()) return virtual def get_nb_magnets(self) -> int: + """Return the number of magnets in the serialized group.""" return len(self.__elements) def get_magnets(self) -> list[Magnet]: + """Return the group's virtual single-function magnets.""" return self.__virtuals def attach( @@ -123,10 +301,27 @@ def attach( strengths: list[abstract.ReadWriteFloatScalar], hardwares: list[abstract.ReadWriteFloatScalar], ) -> list[Magnet]: + """ + Attach the group and its virtual magnets to a runtime peer. + + Parameters + ---------- + peer : object + Control system or simulator the group is bound to. + strengths : list[abstract.ReadWriteFloatScalar] + Strength accessor of each magnet in the group, in declaration order. + hardwares : list[abstract.ReadWriteFloatScalar] + Hardware accessor of each magnet in the group, in declaration order. + + Returns + ------- + list[Magnet] + Virtual magnets of the group, each bound to ``peer``. + """ l = [] - n_ser_mag = SerializedMagnets(self._cfg, peer) - n_ser_mag.__strengths = ReadWriteSerializedStrengths(self._cfg, strengths) - n_ser_mag.__hardwares = ReadWriteSerializedHardwares(self._cfg, hardwares) + n_ser_mag = SerializedMagnets(self._name, self.function, self.__elements, self.model, self.description, peer) + n_ser_mag.__strengths = ReadWriteSerializedStrengths(strengths, self.model) + n_ser_mag.__hardwares = ReadWriteSerializedHardwares(hardwares, self.model) l.append(n_ser_mag) # Construct a single magnet for each magnet. sub_magnets: list[Magnet] = [] @@ -159,6 +354,17 @@ def hardware(self) -> abstract.ReadWriteFloatScalar: return self.__hardwares def set_energy(self, energy: float): + """ + Set beam energy for serialized-magnet strength conversion. + + The energy is converted to magnetic rigidity and propagated to the + serialized magnet model. + + Parameters + ---------- + energy : float + Beam energy in electronvolts. + """ brho = energy / speed_of_light if self.model is not None: self.model.set_magnet_rigidity(brho) @@ -168,7 +374,11 @@ def set_energy(self, energy: float): self.__strengths.set_magnet_rigidity(brho) def __repr__(self): + """ + Implement the ``__repr__`` string. + """ return __pyaml_repr__(self) - def get_devices(self) -> list[DeviceAccess]: - return self.model.get_devices() + def get_device_names(self) -> list[str | None]: + """Return the associated device names.""" + return self.model.get_device_names() diff --git a/pyaml/magnet/sextupole.py b/pyaml/magnet/sextupole.py index e8218ca38..7928c6395 100644 --- a/pyaml/magnet/sextupole.py +++ b/pyaml/magnet/sextupole.py @@ -1,24 +1,51 @@ +""" +Sextupole magnet elements. + +This module defines normal sextupole configuration and runtime interfaces. +""" + from ..lattice.polynom_info import PolynomInfo -from .magnet import Magnet, MagnetConfigModel +from ..validation import DynamicValidation, register_schema +from .magnet import Magnet +from .model import MagnetModel # Define the main class name for this module PYAMLCLASS = "Sextupole" -class ConfigModel(MagnetConfigModel): - """Configuration model for Sextupole magnet.""" - - ... - - -class Sextupole(Magnet): - """Sextupole class""" +@register_schema +class Sextupole(Magnet, DynamicValidation): + """ + Normal sextupole magnet element. + + The strength is applied to the ``PolynomB[2]`` component of the underlying lattice element, the + field component used for correcting chromaticity. Strengths are expressed in ``m-2`` and + converted to power-converter values by the attached magnet model. + + Parameters + ---------- + name : str + Element name. + model : MagnetModel | None, optional + Magnet model used to convert between strength and hardware value, and to + resolve the underlying control-system device names. + lattice_names : str | None, optional + Name or names of the matching element(s) in the simulated lattice. Defaults + to ``name``. + description : str | None, optional + Human-readable description of the magnet. + + See Also + -------- + Magnet : Base class listing the strength and hardware accessors. + """ polynom = PolynomInfo("PolynomB", 2) - def __init__(self, cfg: ConfigModel): - super().__init__( - cfg.name, - cfg.model if hasattr(cfg, "model") else None, - ) - self._cfg = cfg + def __init__( + self, name: str, model: MagnetModel | None = None, lattice_names: str | None = None, description: str | None = None + ): + """ + Initialize the Sextupole. + """ + super().__init__(name, model, lattice_names, description) diff --git a/pyaml/magnet/skewoctu.py b/pyaml/magnet/skewoctu.py index 109edd786..b76bf3ccc 100644 --- a/pyaml/magnet/skewoctu.py +++ b/pyaml/magnet/skewoctu.py @@ -1,24 +1,51 @@ +""" +Skew-octupole magnet elements. + +This module defines skew-octupole configuration and runtime interfaces. +""" + from ..lattice.polynom_info import PolynomInfo -from .magnet import Magnet, MagnetConfigModel +from ..validation import DynamicValidation, register_schema +from .magnet import Magnet +from .model import MagnetModel # Define the main class name for this module PYAMLCLASS = "SkewOctu" -class ConfigModel(MagnetConfigModel): - """Configuration model for SkewOctu magnet.""" - - ... - - -class SkewOctu(Magnet): - """SkewOctu class""" +@register_schema +class SkewOctu(Magnet, DynamicValidation): + """ + Skew octupole magnet element. + + The strength is applied to the ``PolynomA[3]`` component of the underlying lattice element, the + field component used for correcting high-order coupled resonances. Strengths are expressed in + ``m-3`` and converted to power-converter values by the attached magnet model. + + Parameters + ---------- + name : str + Element name. + model : MagnetModel | None, optional + Magnet model used to convert between strength and hardware value, and to + resolve the underlying control-system device names. + lattice_names : str | None, optional + Name or names of the matching element(s) in the simulated lattice. Defaults + to ``name``. + description : str | None, optional + Human-readable description of the magnet. + + See Also + -------- + Magnet : Base class listing the strength and hardware accessors. + """ polynom = PolynomInfo("PolynomA", 3) - def __init__(self, cfg: ConfigModel): - super().__init__( - cfg.name, - cfg.model if hasattr(cfg, "model") else None, - ) - self._cfg = cfg + def __init__( + self, name: str, model: MagnetModel | None = None, lattice_names: str | None = None, description: str | None = None + ): + """ + Initialize the SkewOctu. + """ + super().__init__(name, model, lattice_names, description) diff --git a/pyaml/magnet/skewquad.py b/pyaml/magnet/skewquad.py index f79e2c309..abf6bab9b 100644 --- a/pyaml/magnet/skewquad.py +++ b/pyaml/magnet/skewquad.py @@ -1,24 +1,51 @@ +""" +Skew-quadrupole magnet elements. + +This module defines skew-quadrupole configuration and runtime interfaces. +""" + from ..lattice.polynom_info import PolynomInfo -from .magnet import Magnet, MagnetConfigModel +from ..validation import DynamicValidation, register_schema +from .magnet import Magnet +from .model import MagnetModel # Define the main class name for this module PYAMLCLASS = "SkewQuad" -class ConfigModel(MagnetConfigModel): - """Configuration model for SkewQuad magnet.""" - - ... - - -class SkewQuad(Magnet): - """SkewQuad class""" +@register_schema +class SkewQuad(Magnet, DynamicValidation): + """ + Skew quadrupole magnet element. + + The strength is applied to the ``PolynomA[1]`` component of the underlying lattice element, the + field component used for correcting betatron coupling. Strengths are expressed in ``m-1`` and + converted to power-converter values by the attached magnet model. + + Parameters + ---------- + name : str + Element name. + model : MagnetModel | None, optional + Magnet model used to convert between strength and hardware value, and to + resolve the underlying control-system device names. + lattice_names : str | None, optional + Name or names of the matching element(s) in the simulated lattice. Defaults + to ``name``. + description : str | None, optional + Human-readable description of the magnet. + + See Also + -------- + Magnet : Base class listing the strength and hardware accessors. + """ polynom = PolynomInfo("PolynomA", 1) - def __init__(self, cfg: ConfigModel): - super().__init__( - cfg.name, - cfg.model if hasattr(cfg, "model") else None, - ) - self._cfg = cfg + def __init__( + self, name: str, model: MagnetModel | None = None, lattice_names: str | None = None, description: str | None = None + ): + """ + Initialize the SkewQuad. + """ + super().__init__(name, model, lattice_names, description) diff --git a/pyaml/magnet/skewsext.py b/pyaml/magnet/skewsext.py index 640d996e1..5d82c1d16 100644 --- a/pyaml/magnet/skewsext.py +++ b/pyaml/magnet/skewsext.py @@ -1,24 +1,51 @@ +""" +Skew-sextupole magnet elements. + +This module defines skew-sextupole configuration and runtime interfaces. +""" + from ..lattice.polynom_info import PolynomInfo -from .magnet import Magnet, MagnetConfigModel +from ..validation import DynamicValidation, register_schema +from .magnet import Magnet +from .model import MagnetModel # Define the main class name for this module PYAMLCLASS = "SkewSext" -class ConfigModel(MagnetConfigModel): - """Configuration model for SkewSext magnet.""" - - ... - - -class SkewSext(Magnet): - """SkewSext class""" +@register_schema +class SkewSext(Magnet, DynamicValidation): + """ + Skew sextupole magnet element. + + The strength is applied to the ``PolynomA[2]`` component of the underlying lattice element, the + field component used for correcting coupled chromatic effects. Strengths are expressed in + ``m-2`` and converted to power-converter values by the attached magnet model. + + Parameters + ---------- + name : str + Element name. + model : MagnetModel | None, optional + Magnet model used to convert between strength and hardware value, and to + resolve the underlying control-system device names. + lattice_names : str | None, optional + Name or names of the matching element(s) in the simulated lattice. Defaults + to ``name``. + description : str | None, optional + Human-readable description of the magnet. + + See Also + -------- + Magnet : Base class listing the strength and hardware accessors. + """ polynom = PolynomInfo("PolynomA", 2) - def __init__(self, cfg: ConfigModel): - super().__init__( - cfg.name, - cfg.model if hasattr(cfg, "model") else None, - ) - self._cfg = cfg + def __init__( + self, name: str, model: MagnetModel | None = None, lattice_names: str | None = None, description: str | None = None + ): + """ + Initialize the SkewSext. + """ + super().__init__(name, model, lattice_names, description) diff --git a/pyaml/magnet/spline_model.py b/pyaml/magnet/spline_model.py index bc6d20d37..e38734451 100644 --- a/pyaml/magnet/spline_model.py +++ b/pyaml/magnet/spline_model.py @@ -1,87 +1,160 @@ +""" +Spline-based conversion model for calibrated magnets. + +This model uses excitation-curve interpolation to convert between physical magnet strengths and hardware values. +""" + import numpy as np -from pydantic import BaseModel, ConfigDict from scipy.interpolate import make_smoothing_spline from ..common.element import __pyaml_repr__ -from ..configuration.curve import Curve -from ..control.deviceaccess import DeviceAccess +from ..validation import DynamicValidation, register_schema +from .curve import Curve from .model import MagnetModel # Define the main class name for this module PYAMLCLASS = "SplineMagnetModel" -class ConfigModel(BaseModel): +@register_schema +class SplineMagnetModel(MagnetModel, DynamicValidation): """ - Configuration model for spline magnet model + Magnet model that converts between strength and hardware current using + spline interpolation. + + The model represents a single-function magnet and builds two smoothing + splines from the supplied excitation curve: + + - a forward spline for converting hardware current to magnet strength + - an inverse spline for converting magnet strength to hardware current + + The input curve is first scaled by ``calibration_factor`` and ``crosstalk`` + and shifted by ``calibration_offset`` before the splines are created. Parameters ---------- curve : Curve - Curve object used for interpolation - powerconverter : DeviceAccess, optional - Power converter device to apply current + Excitation curve used for interpolation. + powerconverter : str | None, optional + Name of the associated power converter device. calibration_factor : float, optional - Correction factor applied to the curve. Default: 1.0 + Multiplicative correction applied to the curve. Default is ``1.0``. calibration_offset : float, optional - Correction offset applied to the curve. Default: 0.0 + Additive correction applied to the curve. Default is ``0.0``. crosstalk : float, optional - Crosstalk factor. Default: 1.0 - unit : str - Unit of the strength (i.e. 1/m or m-1) + Crosstalk factor applied to the curve. Default is ``1.0``. + unit : str | None, optional + Strength unit, such as ``m-1`` or ``m-2``. + hardware_unit : str | None, optional + Hardware unit, such as ``A`` or ``V``. alpha : float, optional - Regularization parameter (alpha >= 0). alpha = 0 means the interpolation - passes through all the points of the curve. Default: 0.0 - """ - - model_config = ConfigDict(arbitrary_types_allowed=True, extra="forbid") - - curve: Curve - powerconverter: DeviceAccess | None - calibration_factor: float = 1.0 - calibration_offset: float = 0.0 - crosstalk: float = 1.0 - unit: str - alpha: float = 0.0 - - -class SplineMagnetModel(MagnetModel): - """ - Class that handle manget current/strength conversion using - spline interpolation for a single function magnet + Smoothing parameter passed to :func:`scipy.interpolate.make_smoothing_spline`. + ``alpha = 0`` gives exact interpolation through the data points. + + Methods + ------- + compute_hardware_values(strengths) + Convert magnet strengths to hardware values. + compute_strengths(currents) + Convert hardware values to magnet strengths. + get_strength_units() + Return the units of magnet strengths. + get_hardware_units() + Return the units of hardware values. + get_device_names() + Return the associated device names. + set_magnet_rigidity(brho) + Set the magnetic rigidity used for conversion. + + Notes + ----- + The magnet rigidity ``brho`` must be set with :meth:`set_magnet_rigidity` + before using the conversion methods. """ - def __init__(self, cfg: ConfigModel): - self._cfg = cfg - self.__curve = cfg.curve.get_curve() - self.__curve[:, 1] = self.__curve[:, 1] * cfg.calibration_factor * cfg.crosstalk + cfg.calibration_offset + def __init__( + self, + curve: Curve, + powerconverter: str | None = None, + calibration_factor: float = 1.0, + calibration_offset: float = 0.0, + crosstalk: float = 1.0, + unit: str | None = None, + hardware_unit: str | None = None, + alpha: float = 0.0, + ): + """ + Initialize the SplineMagnetModel. + """ + self.__curve = curve.get_curve() + self.__curve[:, 1] = self.__curve[:, 1] * calibration_factor * crosstalk + calibration_offset rcurve = Curve.inverse(self.__curve) - self.__strength_unit = cfg.unit - self.__hardware_unit = cfg.powerconverter.unit() + self.__strength_unit = unit + self.__hardware_unit = hardware_unit self.__brho = np.nan - self.__ps = cfg.powerconverter - self.__spl = make_smoothing_spline(self.__curve[:, 0], self.__curve[:, 1], lam=cfg.alpha) - self.__rspl = make_smoothing_spline(rcurve[:, 0], rcurve[:, 1], lam=cfg.alpha) + self.__ps = powerconverter + self.__spl = make_smoothing_spline(self.__curve[:, 0], self.__curve[:, 1], lam=alpha) + self.__rspl = make_smoothing_spline(rcurve[:, 0], rcurve[:, 1], lam=alpha) def compute_hardware_values(self, strengths: np.array) -> np.array: + """ + Convert magnet strengths to hardware values. + + Parameters + ---------- + strengths : np.array + Magnet strengths to convert, in the unit reported by :meth:`get_strength_unit`. + + Returns + ------- + np.array + Hardware values corresponding to ``strengths``. + """ _current = self.__rspl(strengths[0] * self.__brho) return np.array([_current]) def compute_strengths(self, currents: np.array) -> np.array: + """ + Convert hardware values to magnet strengths. + + Parameters + ---------- + currents : np.array + Hardware values to convert, in the unit reported by :meth:`get_hardware_unit`. + + Returns + ------- + np.array + Strengths corresponding to ``currents``. + """ _strength = self.__spl(currents[0]) / self.__brho return np.array([_strength]) def get_strength_units(self) -> list[str]: + """Return the units of magnet strengths.""" return [self.__strength_unit] if self.__strength_unit is not None else [""] def get_hardware_units(self) -> list[str]: + """Return the units of hardware values.""" return [self.__hardware_unit] if self.__hardware_unit is not None else [""] - def get_devices(self) -> list[DeviceAccess]: + def get_device_names(self) -> list[str | None]: + """Return the associated device names.""" return [self.__ps] def set_magnet_rigidity(self, brho: np.double): + """ + Set the magnetic rigidity used for conversion. + + Parameters + ---------- + brho : np.double + Magnetic rigidity in tesla metres, used to scale strengths into hardware values. + """ self.__brho = brho def __repr__(self): + """ + Implement the ``__repr__`` string. + """ return __pyaml_repr__(self) diff --git a/pyaml/magnet/vcorrector.py b/pyaml/magnet/vcorrector.py index cf3a0d08e..f9614754f 100644 --- a/pyaml/magnet/vcorrector.py +++ b/pyaml/magnet/vcorrector.py @@ -1,34 +1,91 @@ +""" +Vertical orbit-corrector elements. + +This module defines the vertical corrector configuration and runtime +interface, including its vertical kick-angle access. +""" + +from typing import Self + from ..common import abstract from ..lattice.polynom_info import PolynomInfo +from ..validation import DynamicValidation, register_schema from .corrector import RWCorrectorAngle -from .magnet import Magnet, MagnetConfigModel +from .magnet import Magnet +from .model import MagnetModel # Define the main class name for this module PYAMLCLASS = "VCorrector" -class ConfigModel(MagnetConfigModel): - """Configuration model for Vertical Corrector magnet.""" +@register_schema +class VCorrector(Magnet, DynamicValidation): + """ + Represent a vertical orbit corrector. - ... + Parameters + ---------- + name : str + Corrector name. + model : MagnetModel | None + Optional magnet model. + lattice_names : str | None + Optional lattice-element mapping. + description : str | None + Optional human-readable description. + Attributes + ---------- + angle + Return read/write access to the vertical kick angle in radians. -class VCorrector(Magnet): - """Vertical Corrector class""" + Methods + ------- + attach(peer, strength, hardware) + Return an attached copy with a bound vertical-angle handle. + """ polynom = PolynomInfo("PolynomA", 0) - def __init__(self, cfg: ConfigModel): - super().__init__( - cfg.name, - cfg.model if hasattr(cfg, "model") else None, - ) - self._cfg = cfg + def __init__( + self, name: str, model: MagnetModel | None = None, lattice_names: str | None = None, description: str | None = None + ): + """ + Initialize the VCorrector. + """ + super().__init__(name, model, lattice_names, description) self.__angle = RWCorrectorAngle(self) @property def angle(self) -> abstract.ReadWriteFloatScalar: """ - Set the kick angle. + Return read/write access to the vertical kick angle in radians. """ return self.__angle + + def attach( + self, + peer, + strength: abstract.ReadWriteFloatScalar, + hardware: abstract.ReadWriteFloatScalar, + ) -> Self: + """ + Return an attached copy with a bound vertical-angle handle. + + Parameters + ---------- + peer : ElementHolder + Control system or simulator the copy is bound to. + strength : abstract.ReadWriteFloatScalar + Accessor for the physical strength on that peer. + hardware : abstract.ReadWriteFloatScalar + Accessor for the hardware value on that peer. + + Returns + ------- + Self + Copy of this magnet bound to ``peer``. + """ + obj = super().attach(peer, strength, hardware) + obj.__angle = RWCorrectorAngle(obj) + return obj diff --git a/pyaml/rf/rf_plant.py b/pyaml/rf/rf_plant.py index 5c5bfe53e..4a0055370 100644 --- a/pyaml/rf/rf_plant.py +++ b/pyaml/rf/rf_plant.py @@ -1,49 +1,91 @@ -import numpy as np -from pydantic import BaseModel, ConfigDict +""" +RF-plant interfaces for accelerator frequency and voltage control. -try: - from typing import Self # Python 3.11+ -except ImportError: - from typing_extensions import Self # Python 3.10 and earlier +This module models the master clock and RF transmitters and exposes combined +read/write handles for the plant frequency and total fundamental-harmonic +voltage. +""" + +import copy +from typing import TYPE_CHECKING, Self from .. import PyAMLException from ..common import abstract -from ..common.element import Element, ElementConfigModel -from ..control.deviceaccess import DeviceAccess +from ..common.element import Element, __pyaml_repr__ +from ..validation import DynamicValidation, register_schema from .rf_transmitter import RFTransmitter +if TYPE_CHECKING: + from ..common.holders.element_holder import ElementHolder + # Define the main class name for this module PYAMLCLASS = "RFPlant" -class ConfigModel(ElementConfigModel): - masterclock: DeviceAccess | None = None - """Device to apply main RF frequency""" - transmitters: list[RFTransmitter] | None = None - """List of RF trasnmitters""" - - -class RFPlant(Element): +@register_schema +class RFPlant(Element, DynamicValidation): """ - Main RF object + Represent an accelerator RF plant and its transmitters. + + The plant exposes frequency and voltage handles after it is attached to a + simulator or control-system element holder. + + Parameters + ---------- + name : str + Name of the RF plant. + masterclock : str | None + Name of the master-clock device, if configured. + transmitters : list[RFTransmitter] | None + RF transmitters belonging to the plant. + lattice_names : str | None + Optional lattice-element mapping. + description : str | None + Optional human-readable description. + + Attributes + ---------- + frequency + Read/write accessor for the RF frequency, in hertz. + voltage + Read/write accessor for the total accelerating voltage, in volts. + + Methods + ------- + attach(peer, frequency, voltage) + Return a copy attached to RF read/write handles. """ - def __init__(self, cfg: ConfigModel): - super().__init__(cfg.name) - self._cfg = cfg + def __init__( + self, + name: str, + masterclock: str | None = None, + transmitters: list[RFTransmitter] | None = None, + lattice_names: str | None = None, + description: str | None = None, + ): + """ + Initialize an RF plant configuration. + """ + super().__init__(name, lattice_names, description) + + self.masterclock = masterclock + self.transmitters = transmitters self.__frequency = None self.__voltage = None @property def frequency(self) -> abstract.ReadWriteFloatScalar: + """Return the read/write master-clock frequency handle.""" if self.__frequency is None: - raise PyAMLException(f"{str(self)} has no masterclock device defined") + raise PyAMLException(f"{str(self.name)} has no masterclock device defined") return self.__frequency @property def voltage(self) -> abstract.ReadWriteFloatScalar: + """Return the read/write total fundamental-harmonic voltage handle.""" if self.__voltage is None: - raise PyAMLException(f"{str(self)} has no trasmitter device defined") + raise PyAMLException(f"{str(self.name)} has no transmitter device defined") return self.__voltage def attach( @@ -53,42 +95,107 @@ def attach( voltage: abstract.ReadWriteFloatScalar, ) -> Self: # Attach frequency attribute and returns a new reference - obj = self.__class__(self._cfg) + """ + Return a copy attached to RF read/write handles. + + Parameters + ---------- + peer : object + Simulator or control-system element holder. + frequency : abstract.ReadWriteFloatScalar + Read/write master-clock frequency handle. + voltage : abstract.ReadWriteFloatScalar + Read/write total-voltage handle. + + Returns + ------- + Self + Attached RF-plant instance. + """ + obj = copy.copy(self) obj.__frequency = frequency obj.__voltage = voltage obj._peer = peer return obj + def _fill_device(self, holder: "ElementHolder") -> None: + holder._fill_rf_plant(self) + class RWTotalVoltage(abstract.ReadWriteFloatScalar): + """ + Read/write aggregate for fundamental-harmonic transmitter voltage. + + Parameters + ---------- + transmitters : list[RFTransmitter] + Transmitters whose fundamental-harmonic voltages are summed. + + Methods + ------- + get() + Return the sum of the fundamental-harmonic transmitter voltages. + set(value) + Set the total fundamental-harmonic voltage. + set_and_wait(value) + Set the total voltage and wait for readback convergence. + unit() + Return the voltage unit reported by the first transmitter. + """ + def __init__(self, transmitters: list[RFTransmitter]): """ - Construct a RWTotalVoltage setter - - Parameters - ---------- - transmitters : list[RFTransmitter] - List of attached transmitters + Construct an aggregate transmitter-voltage handle. """ self.__trans = transmitters def get(self) -> float: + """Return the sum of the fundamental-harmonic transmitter voltages.""" sum = 0 # Count only fundamental harmonic for t in self.__trans: - if t._cfg.harmonic == 1.0: + if t.harmonic == 1.0: sum += t.voltage.get() return sum def set(self, value: float): # Assume that sum of transmitter (fundamental harmonic) distribution is 1 + """ + Set the total fundamental-harmonic voltage. + + Parameters + ---------- + value : float + Total voltage to distribute among fundamental-harmonic + transmitters. + """ for t in self.__trans: - if t._cfg.harmonic == 1.0: - v = value * t._cfg.distribution + if t.harmonic == 1.0: + v = value * t.distribution t.voltage.set(v) def set_and_wait(self, value: float): + """ + Set the total voltage and wait for readback convergence. + + Parameters + ---------- + value : float + Requested total voltage. + + Raises + ------ + NotImplementedError + This operation is not implemented for aggregate voltage access. + """ raise NotImplementedError("Not implemented yet.") def unit(self) -> str: - return self.__trans[0]._cfg.phase.unit() + """Return the voltage unit reported by the first transmitter.""" + return self.__trans[0].phase_device_access.unit() + + def __repr__(self): + """ + Implement the ``__repr__`` string. + """ + return __pyaml_repr__(self, exclude=["frequency", "voltage"]) diff --git a/pyaml/rf/rf_transmitter.py b/pyaml/rf/rf_transmitter.py index 9014d72b6..69abe2296 100644 --- a/pyaml/rf/rf_transmitter.py +++ b/pyaml/rf/rf_transmitter.py @@ -1,95 +1,122 @@ -import numpy as np -from pydantic import BaseModel, ConfigDict +""" +RF-transmitter configuration and read/write interfaces. -try: - from typing import Self # Python 3.11+ -except ImportError: - from typing_extensions import Self # Python 3.10 and earlier +This module models RF transmitters, their cavity assignments, harmonic and +voltage distribution, and the voltage and phase handles bound on attachment. +""" + +import copy +from typing import Self from .. import PyAMLException from ..common import abstract -from ..common.element import Element, ElementConfigModel -from ..control.deviceaccess import DeviceAccess +from ..common.element import Element, __pyaml_repr__ +from ..validation import DynamicValidation, register_schema # Define the main class name for this module PYAMLCLASS = "RFTransmitter" -class ConfigModel(ElementConfigModel): +@register_schema +class RFTransmitter(Element, DynamicValidation): """ - Configuration model for RF Transmitter. + Represent an RF transmitter and its cavity controls. - Attributes + A transmitter may expose read/write voltage and phase handles after it is + attached to a simulator or control-system element holder. + + Parameters ---------- - voltage : DeviceAccess or None, optional - Device to apply cavity voltage - phase : DeviceAccess or None, optional - Device to apply cavity phase + name : str + Name of the transmitter. cavities : list[str] - List of cavity names connected to this transmitter - harmonic : float, optional - Harmonic frequency ratio, 1.0 for main frequency, by default 1.0 - distribution : float, optional - RF distribution (Part of the total RF voltage powered by this transmitter), - by default 1.0 - """ - - model_config = ConfigDict(arbitrary_types_allowed=True, extra="forbid") + Names of cavities driven by the transmitter. + voltage : str | None + Name of the voltage device, if configured. + phase : str | None + Name of the phase device, if configured. + harmonic : float + Harmonic number associated with the transmitter. + distribution : float + Fraction of aggregate voltage assigned to this transmitter. + lattice_names : str | None + Optional lattice-element mapping. + description : str | None + Optional human-readable description. - voltage: DeviceAccess | None = None - phase: DeviceAccess | None = None - cavities: list[str] - harmonic: float = 1.0 - distribution: float = 1.0 - - -class RFTransmitter(Element): - """ - Class that handle a RF transmitter + Attributes + ---------- + voltage + Return the read/write RF-voltage handle in volts. + phase + Return the read/write RF-phase handle in radians. + + Methods + ------- + attach(peer, voltage, phase) + Return a copy with voltage and phase handles attached. """ - def __init__(self, cfg: ConfigModel): - super().__init__(cfg.name) - self._cfg = cfg + def __init__( + self, + name: str, + cavities: list[str], + voltage: str | None = None, + phase: str | None = None, + harmonic: float = 1.0, + distribution: float = 1.0, + lattice_names: str | None = None, + description: str | None = None, + ): + """ + Initialize an RF-transmitter configuration. + """ + super().__init__(name, lattice_names, description) + self.voltage_name = voltage + self.phase_name = phase + self.cavities = cavities + self.harmonic = harmonic + self.distribution = distribution + self.__voltage = None self.__phase = None @property def voltage(self) -> abstract.ReadWriteFloatScalar: """ - Get the RF voltage in [V]. + Return the read/write RF-voltage handle in volts. Returns ------- abstract.ReadWriteFloatScalar - Read/write access to RF voltage + Read/write access to the transmitter voltage. Raises ------ PyAMLException - If transmitter is unattached or has no voltage device defined + If the transmitter is unattached or has no voltage device. """ if self.__voltage is None: - raise PyAMLException(f"{str(self)} is unattached or has no voltage device defined") + raise PyAMLException(f"{str(self.name)} is unattached or has no voltage device defined") return self.__voltage @property def phase(self) -> abstract.ReadWriteFloatScalar: """ - Get the RF phase in [rad]. + Return the read/write RF-phase handle in radians. Returns ------- abstract.ReadWriteFloatScalar - Read/write access to RF phase + Read/write access to the transmitter phase. Raises ------ PyAMLException - If transmitter is unattached or has no phase device defined + If the transmitter is unattached or has no phase device. """ if self.__phase is None: - raise PyAMLException(f"{str(self)} is unattached or has no phase device defined") + raise PyAMLException(f"{str(self.name)} is unattached or has no phase device defined") return self.__phase def attach( @@ -99,25 +126,31 @@ def attach( phase: abstract.ReadWriteFloatScalar, ) -> Self: """ - Attach voltage and phase attributes to a peer. + Return a copy with voltage and phase handles attached. Parameters ---------- peer : object - The peer object (simulator or control system) + Simulator or control-system element holder. voltage : abstract.ReadWriteFloatScalar - Voltage accessor to attach + Read/write voltage accessor. phase : abstract.ReadWriteFloatScalar - Phase accessor to attach + Read/write phase accessor. Returns ------- Self - A new attached instance of RFTransmitter + Attached copy of the transmitter. """ # Attach voltage and phase attribute and returns a new reference - obj = self.__class__(self._cfg) + obj = copy.copy(self) obj.__voltage = voltage obj.__phase = phase obj._peer = peer return obj + + def __repr__(self): + """ + Implement the ``__repr__`` string. + """ + return __pyaml_repr__(self, exclude=["voltage", "phase"]) diff --git a/pyaml/tuning_tools/LOCO/__init__.py b/pyaml/tuning_tools/LOCO/__init__.py index 8cfe36909..d25534cde 100644 --- a/pyaml/tuning_tools/LOCO/__init__.py +++ b/pyaml/tuning_tools/LOCO/__init__.py @@ -3,7 +3,6 @@ ~~~~~~~~~~~~~~~~ pyAML - """ __title__ = "pyAML" diff --git a/pyaml/tuning_tools/LOCO/loco.py b/pyaml/tuning_tools/LOCO/loco.py index 3e0515dc9..feda3a0be 100644 --- a/pyaml/tuning_tools/LOCO/loco.py +++ b/pyaml/tuning_tools/LOCO/loco.py @@ -1,8 +1,25 @@ +""" +Linear optics from closed orbit (LOCO) analysis tools. + +This module contains the interface for measuring an orbit response matrix and +running linear-optics analysis with the accelerator commissioning tools. +""" + + class loco: - """loco help""" + """ + Coordinate LOCO measurements and linear-optics analysis. + + Methods + ------- + run() + Run the configured LOCO analysis. + measure_orm() + Measure the orbit response matrix required by LOCO. + """ def run(): - """loco run help""" + """Run the configured LOCO analysis.""" def measure_orm(): - """loco measure help""" + """Measure the orbit response matrix required by LOCO.""" diff --git a/pyaml/tuning_tools/SOFB/__init__.py b/pyaml/tuning_tools/SOFB/__init__.py index 2f86fabeb..8cec004e4 100644 --- a/pyaml/tuning_tools/SOFB/__init__.py +++ b/pyaml/tuning_tools/SOFB/__init__.py @@ -3,7 +3,6 @@ ~~~~~~~~~~~~~~~~ pyAML - """ __title__ = "pyAML" diff --git a/pyaml/tuning_tools/SOFB/sofb.py b/pyaml/tuning_tools/SOFB/sofb.py index 1530e58c1..69114732c 100644 --- a/pyaml/tuning_tools/SOFB/sofb.py +++ b/pyaml/tuning_tools/SOFB/sofb.py @@ -1,8 +1,25 @@ +""" +Slow-orbit feedback control tools. + +This module provides the interface for applying slow orbit corrections and +analyzing the singular-value decomposition used to select orbit steerers. +""" + + class slow_orbit_feeback: - """slow orbit feedback help""" + """ + Coordinate slow orbit feedback corrections. + + Methods + ------- + run() + Run the configured slow-orbit feedback correction. + get_svd_decomposition() + Return the SVD decomposition used for orbit steering. + """ def run(): - """run slow orbit feedback""" + """Run the configured slow-orbit feedback correction.""" def get_svd_decomposition(): - """get steerers svd decomposition""" + """Return the SVD decomposition used for orbit steering.""" diff --git a/pyaml/tuning_tools/__init__.py b/pyaml/tuning_tools/__init__.py index 851e406c4..2008ae441 100644 --- a/pyaml/tuning_tools/__init__.py +++ b/pyaml/tuning_tools/__init__.py @@ -3,7 +3,6 @@ ~~~~~~~~~~~~~~~~~~~~ pyAML - """ __title__ = "pyAML" diff --git a/pyaml/tuning_tools/bba.py b/pyaml/tuning_tools/bba.py new file mode 100644 index 000000000..05293bc3f --- /dev/null +++ b/pyaml/tuning_tools/bba.py @@ -0,0 +1,354 @@ +""" +Beam-based alignment measurement tools. + +The :class:`BBA` tool determines the magnetic center of a quadrupole by +combining controlled quadrupole-strength changes with orbit measurements from +nearby beam-position monitors. +""" + +import logging +from typing import Callable, Optional + +import matplotlib.pyplot as plt +import numpy as np +import pySC +from pySC.apps import measure_bba +from pySC.apps.bba import BBAAnalysis +from pySC.apps.codes import BBACode + +from ..common.constants import Action +from ..common.exception import PyAMLException +from ..external.pySC_interface import pySCInterface +from ..validation import DynamicValidation, register_schema +from .measurement_tool import MeasurementTool + +logger = logging.getLogger(__name__) + +PYAMLCLASS = "BBA" + + +@register_schema +class BBA(MeasurementTool, DynamicValidation): + """ + Beam-based alignment measurement tool. + + This tool determines the magnetic center of a quadrupole by varying its + strength while applying controlled horizontal and vertical orbit offsets. + The quadrupole center is identified from the corresponding zero crossings + in the BPM response. + + Parameters + ---------- + name : str + Name of the measurement tool. + bpm_array_name : str + Name of the BPM array used to measure the orbit. + bpm_name : str + Name of the BPM located near the quadrupole whose center is measured. + hcorr_name : str + Name of the horizontal corrector used to create horizontal orbit + offsets at the quadrupole. + vcorr_name : str + Name of the vertical corrector used to create vertical orbit offsets + at the quadrupole. + quad_name : str + Name of the quadrupole to align. + hcorr_delta : float + Change in horizontal corrector strength used for each horizontal + orbit-offset step. + vcorr_delta : float + Change in vertical corrector strength used for each vertical + orbit-offset step. + hquad_delta : float + Change in quadrupole strength used during the horizontal alignment + measurement. + vquad_delta : float + Change in quadrupole strength used during the vertical alignment + measurement. + n_step : int, default=1 + Number of orbit-offset steps to perform in each plane. + sleep_between_step : float, default=0 + Time in seconds to wait after changing an orbit offset. + n_avg_meas : int, default=1 + Number of BPM measurements to average at each step. + sleep_between_meas : float, default=0 + Time in seconds to wait between individual BPM measurements. + + Methods + ------- + measure(...) + Measure BBA. + h_offset() + Return the measured horizontal magnetic-center offset. + h_offset_error() + Return the uncertainty of the horizontal center offset. + v_offset() + Return the measured vertical magnetic-center offset. + v_offset_error() + Return the uncertainty of the vertical center offset. + plot_data(plane) + Plot BBA data. + """ + + def __init__( + self, + name: str, + bpm_array_name: str, + bpm_name: str, + hcorr_name: str, + vcorr_name: str, + quad_name: str, + hcorr_delta: float, + vcorr_delta: float, + hquad_delta: float, + vquad_delta: float, + n_step: int = 1, + sleep_between_step: float = 0, + n_avg_meas: int = 1, + sleep_between_meas: float = 0, + ): + """ + Initialize the BBA. + """ + super().__init__(name) + self.bpm_array_name = bpm_array_name + self.bpm_name = bpm_name + self.hcorr_name = hcorr_name + self.vcorr_name = vcorr_name + self.quad_name = quad_name + self.hcorr_delta = hcorr_delta + self.vcorr_delta = vcorr_delta + self.hquad_delta = hquad_delta + self.vquad_delta = vquad_delta + self.n_step = n_step + self.sleep_between_step = sleep_between_step + self.n_avg_meas = n_avg_meas + self.sleep_between_meas = sleep_between_meas + + def measure( + self, + sleep_between_step: Optional[float] = None, + n_avg_meas: Optional[int] = None, + sleep_between_meas: Optional[float] = None, + callback: Optional[Callable] = None, + plane: Optional[str] = None, + ): + """ + Measure BBA. + + **Example** + + .. code-block:: python + + sr = Accelerator.load("tests/config/EBSOrbit.yaml") + SR = sr.design + bba = SR.get_bba("BBA-BPM_C04-04") + + # Add a misalignement + SR.get_bpm("BPM_C04-04").offset.set([20e-6,-15e-6]) + + bba.measure(plane="H") + print(f"HOffset: {bba.h_offset()}") + + bba.plot_data("H") + + Parameters + ---------- + sleep_between_step : float + Default time sleep after steerer or quad excitation + Default: from config + n_avg_meas : int, optional + Default number of orbit measurement per step used for averaging + Default from config + sleep_between_meas : float + Default time sleep between two orbit measurment + Default: from config + callback : Callable, optional + example: callback(action:int, callback_data: 'Complicated struct') + callback is executed after each strength setting and after each orbit + reading. + If the callback returns false, then the process is aborted. + plane : str, optional + Plane to perform ("H" or "V", None => both plane) + """ + nb_meas = n_avg_meas if n_avg_meas is not None else self.n_avg_meas + sleep_step = sleep_between_step if sleep_between_step is not None else self.sleep_between_step + sleep_meas = sleep_between_meas if sleep_between_meas is not None else self.sleep_between_meas + + element_holder = self._peer + interface = pySCInterface( + element_holder=element_holder, + bpm_array_name=self.bpm_array_name, + ) + interface.set_wait_time = sleep_step + interface.read_wait_time = sleep_meas + + bpms_names = element_holder.bpms.get(self.bpm_array_name).names() + + bba_pySC_config = { + "number": bpms_names.index(self.bpm_name), + "QUAD": self.quad_name, + "HCORR": self.hcorr_name, + "VCORR": self.vcorr_name, + "HCORR_delta": self.hcorr_delta, + "QUAD_dk_H": self.hquad_delta, + "VCORR_delta": self.vcorr_delta, + "QUAD_dk_V": self.vquad_delta, + "magnet_type": "normal_quadrupole", + } + + # logging.getLogger("pySC.apps.measurements").setLevel(logging.DEBUG) + # logging.getLogger("pySC.apps.bba").setLevel(logging.DEBUG) + + generator = measure_bba( + interface=interface, + bpm_name=self.bpm_name, + config=bba_pySC_config, + shots_per_orbit=nb_meas, + n_corr_steps=self.n_step, + bipolar=False, + skip_save=True, + plane=plane, + live_ios=True, + ) + + pySC.disable_pySC_rich() + aborted = False + err = None + hstep = 0 + vstep = 0 + + try: + self._register_callback(callback) + self._init_measure() + self.latest_measurement["HData"] = None + self.latest_measurement["VData"] = None + for code, measurement_object in generator: + if code == BBACode.HORIZONTAL_IOS_READY: + self.send_callback( + Action.MEASURE, + { + "step": hstep, + "plane": "H", + "bpm_pos": measurement_object.last_bpm_pos, + "ios": measurement_object.last_ios, + "bba_data": measurement_object.H_data, + }, + ) + hstep += 1 + if code == BBACode.VERTICAL_IOS_READY: + self.send_callback( + Action.MEASURE, + { + "step": vstep, + "plane": "V", + "bpm_pos": measurement_object.last_bpm_pos, + "ios": measurement_object.last_ios, + "bba_data": measurement_object.V_data, + }, + ) + vstep += 1 + if code == BBACode.HORIZONTAL_DONE: + result = BBAAnalysis.analyze(measurement_object.H_data) + self.latest_measurement["HData"] = result + if code == BBACode.VERTICAL_DONE: + result = BBAAnalysis.analyze(measurement_object.V_data) + self.latest_measurement["VData"] = result + + except Exception as ex: + err = ex + except KeyboardInterrupt as ex: + aborted = True + finally: + # Restore steerer/quad strength + # TODO + self.send_callback( + Action.RESTORE, + {}, + raiseException=False, + ) + + if err is not None: + raise (err) + + if aborted: + logger.warning(f"{self.get_name()} : measurement aborted (settings not restored)") + return False + + return True + + def h_offset(self) -> float: + """Return the measured horizontal magnetic-center offset.""" + return self.latest_measurement["HData"].offset if self.latest_measurement["HData"] is not None else np.nan + + def h_offset_error(self) -> float: + """Return the uncertainty of the horizontal center offset.""" + return self.latest_measurement["HData"].offset_error if self.latest_measurement["HData"] is not None else np.nan + + def v_offset(self) -> float: + """Return the measured vertical magnetic-center offset.""" + return self.latest_measurement["VData"].offset if self.latest_measurement["VData"] is not None else np.nan + + def v_offset_error(self) -> float: + """Return the uncertainty of the vertical center offset.""" + return self.latest_measurement["VData"].offset_error if self.latest_measurement["VData"] is not None else np.nan + + def plot_data(self, plane: str): + """ + Plot BBA data. + + Parameters + ---------- + plane : str + Plane to plot ("H" or "V") + """ + + planeData = plane + "Data" + if planeData not in self.latest_measurement or self.latest_measurement[planeData] is None: + raise PyAMLException("No BBA data to plot, please call measure() first") + + fig, axes = plt.subplot_mosaic(mosaic=[["A", "A", "S", "S"], ["A", "A", "C", "C"]]) + + bpm_pos = self.latest_measurement[planeData].bpm_position + ios = self.latest_measurement[planeData].induced_orbit_shift + slopes = self.latest_measurement[planeData].slopes + centers = self.latest_measurement[planeData].centers + final_mask = self.latest_measurement[planeData].mask_accepted + offset = self.latest_measurement[planeData].offset + + xp_min = np.min(bpm_pos) * 1e6 + xp_max = np.max(bpm_pos) * 1e6 + for kk in range(len(ios[0, :])): + p0 = np.polyfit(bpm_pos[:] * 1e6, ios[:, kk] * 1e6, 1) + xp = np.linspace(xp_min, xp_max, 10) + yp = p0[0] * xp + p0[1] + axes["A"].plot(xp, yp, "-", c="C0" if final_mask[kk] else "C1", alpha=0.3) + + for kk in range(len(bpm_pos[:])): + yy = ios[kk] * 1e6 + xx = np.ones_like(yy) * bpm_pos[kk] * 1e6 + axes["A"].plot(xx[final_mask], yy[final_mask], ".", c="C0") + axes["A"].plot(xx[~final_mask], yy[~final_mask], ".", c="C1") + + axes["A"].set_xlabel(f"BPM position [μm]\n{self.bpm_name} offset = {offset * 1e6:.3f} [μm]") + axes["A"].set_ylabel("Modulation [μm]") + axes["A"].grid() + + bpm_numbers = np.arange(len(final_mask)) + axes["S"].plot(bpm_numbers[final_mask], slopes[final_mask], ".", c="C0", label="") + axes["S"].plot(bpm_numbers[~final_mask], slopes[~final_mask], ".", c="C1") + axes["S"].set_xlabel("BPM number") + axes["S"].set_ylabel("Slope") + axes["S"].grid() + + axes["C"].plot(bpm_numbers[final_mask], centers[final_mask] * 1e6, ".", c="C0") + axes["C"].plot(bpm_numbers[~final_mask], centers[~final_mask] * 1e6, ".", c="C1", label="rejected") + axes["C"].set_xlabel("BPM number") + axes["C"].set_ylabel("Center [μm]") + axes["C"].legend() + axes["C"].grid() + + fig.tight_layout() + fig.canvas.manager.set_window_title(f"{plane} BBA {self.bpm_name}") + + plt.show() diff --git a/pyaml/tuning_tools/bba2.py b/pyaml/tuning_tools/bba2.py new file mode 100644 index 000000000..cbee35105 --- /dev/null +++ b/pyaml/tuning_tools/bba2.py @@ -0,0 +1,771 @@ +""" +Beam-based alignment analysis tools. + +This module contains data structures and analysis helpers for estimating +quadrupole magnetic-center offsets from beam-position-monitor responses. +""" + +import logging +import time +from typing import Callable, Optional + +import matplotlib.pyplot as plt +import numpy as np + +from ..common.constants import Action +from ..common.exception import PyAMLException +from ..validation import DynamicValidation, register_schema +from .measurement_tool import MeasurementTool + +logger = logging.getLogger(__name__) + +PYAMLCLASS = "BBA2" + + +class BBAData: + """ + Store intermediate data from one beam-based alignment plane. + + The container keeps fitted kicks, steerer steps, BPM responses, and the + latest magnetic-center estimate for either the horizontal or vertical + measurement. + + Methods + ------- + append(st, dk, bpm, allbpm) + Append one steerer-step measurement to the alignment data. + update_offset(x, error, fit) + Store the fitted magnetic-center offset and its uncertainty. + """ + + def __init__(self): + """ + Initialize the BBAData. + """ + self.k = [] # Fitted kick + self.bpm_pos = [] # BPM#i position + self.allbpm_pos = [] # IOS (Induced Orbit Shift) + self.s2 = [] # sum of square + self.steps = [] # steerer step + self.lastfit = [] # Last linear fit + + self.offset = np.nan + self.error = np.nan + + def append(self, st, dk, bpm, allbpm): + # Append new dataset + """ + Append one steerer-step measurement to the alignment data. + + Parameters + ---------- + st : object + Steerer kick applied for the measurement. + dk : object + Fitted kick response. + bpm : object + Orbit position at the reference BPM. + allbpm : object + Induced orbit shift measured at all BPMs. + """ + self.steps.append(st) + self.k.append(dk) + self.bpm_pos.append(bpm) + self.allbpm_pos.append(allbpm) + + def update_offset(self, x, error, fit): + # Update offset value + """ + Store the fitted magnetic-center offset and its uncertainty. + + Parameters + ---------- + x : object + Estimated magnetic-center offset. + error : object + Estimated standard error of the offset. + fit : object + Coefficients of the final linear fit. + """ + self.offset = x + self.error = error + self.lastfit = fit + + +@register_schema +class BBA2(MeasurementTool, DynamicValidation): + """ + Beam-based alignment tool with tune correction. + + This tool determines the magnetic center of a quadrupole from the BPM + response to controlled horizontal and vertical orbit offsets. During the + measurement, the quadrupole strength is varied and tune correction is used + to compensate for the resulting tune change. + + Parameters + ---------- + name : str + Name of the measurement tool. + bpm_array_name : str + Name of the BPM array used to measure the orbit. + bpm_name : str + Name of the BPM located near the quadrupole whose center is measured. + hcorr_name : str + Name of the horizontal corrector used to create horizontal orbit + offsets at the quadrupole. + vcorr_name : str + Name of the vertical corrector used to create vertical orbit offsets + at the quadrupole. + quad_name : str + Name of the quadrupole to align. + tune_correction_name : str + Name of the tune-correction tool used to compensate for tune changes + caused by varying the quadrupole strength. + hcorr_delta : float + Change in horizontal corrector strength used for each horizontal + orbit-offset step. + vcorr_delta : float + Change in vertical corrector strength used for each vertical + orbit-offset step. + quad_delta : float + Change in quadrupole strength used for the alignment measurement. + bipolar_delta : bool, default=False + If `True`, vary the quadrupole strength both above and below its + initial value by `quad_delta`. If `False`, apply the change in one + direction only. + minicycle_sleep_time : float, default=5 + Time in seconds to wait for the quadrupole minicycle to complete after + changing its strength. + n_step : int, default=1 + Number of orbit-offset steps to perform in each plane. + sleep_between_step : float, default=0 + Time in seconds to wait after changing an orbit offset. + n_avg_meas : int, default=1 + Number of BPM measurements to average at each step. + sleep_between_meas : float, default=0 + Time in seconds to wait between individual BPM measurements. + + Methods + ------- + measure(...) + Measure BBA. + h_offset() + Return the measured horizontal magnetic-center offset. + h_offset_error() + Return the uncertainty of the horizontal center offset. + v_offset() + Return the measured vertical magnetic-center offset. + v_offset_error() + Return the uncertainty of the vertical center offset. + plot_plane_data(ax, plane) + Plot measured kicks and the fitted alignment response for one plane. + plot_data() + Plot BBA data. + """ + + def __init__( + self, + name: str, + bpm_array_name: str, + bpm_name: str, + hcorr_name: str, + vcorr_name: str, + quad_name: str, + tune_correction_name: str, + hcorr_delta: float, + vcorr_delta: float, + quad_delta: float, + bipolar_delta: bool = False, + minicycle_sleep_time: float = 5, + n_step: int = 1, + sleep_between_step: float = 0, + n_avg_meas: int = 1, + sleep_between_meas: float = 0, + ): + """ + Initialize a beam-based alignment tool with tune compensation. + """ + super().__init__(name) + self.bpm_array_name = bpm_array_name + self.bpm_name = bpm_name + self.hcorr_name = hcorr_name + self.vcorr_name = vcorr_name + self.quad_name = quad_name + self.tune_correction_name = tune_correction_name + self.hcorr_delta = hcorr_delta + self.vcorr_delta = vcorr_delta + self.quad_delta = quad_delta + self.bipolar_delta = bipolar_delta + self.minicycle_sleep_time = minicycle_sleep_time + self.n_step = n_step + self.sleep_between_step = sleep_between_step + self.n_avg_meas = n_avg_meas + self.sleep_between_meas = sleep_between_meas + + @staticmethod + def _x_intercept(x, k, n): + # Linear fit on last n points + # x is not necessary ordered + """ + Estimate the zero crossing of a linear fit. + + A first-degree polynomial is fitted to the final ``n`` samples of + ``(x, k)``. The zero crossing of that fit and, when enough samples are + available, its propagated standard error are returned. + + Parameters + ---------- + x : array_like + Independent-variable samples used for the fit. + k : array_like + Dependent-variable samples to fit as a function of ``x``. + n : int + Number of trailing samples to include in the fit. + + Returns + ------- + intercept : float + Estimated value of ``x`` for which the fitted ``k`` is zero. + coefficients : numpy.ndarray + Polynomial coefficients in increasing order, ``[intercept, + slope]`` for the fitted ``k`` values. + error : float + Propagated standard error of ``intercept``. This is zero when + fewer than three samples are used. + """ + xx = np.polynomial.polynomial.polyfit(x[-n:], k[-n:], 1) + err = 0 + if n > 2: + # Compute error of the ratio r = -xx[0] / xx[1] + X = np.polynomial.polynomial.polyvander(x[-n:], 1) + R = k[-n:] - X @ xx + S2 = np.sum(R**2) / float(n - 2) + COV = S2 * np.linalg.inv(X.T @ X) + J = [-1 / xx[1], xx[0] / xx[1] ** 2] # Jacobian [dr/d(xx[0]) , dr/d(xx[1])] + err = np.sqrt(J @ COV @ J) + + # return x @y=0 + return (-xx[0] / xx[1], xx, err) + + def _init_responses( + self, tunename: str, bpmname: str, quadname: str, steererhname: str, steerervname: str, bpmi: int, dk0=1e-5 + ): + # Return: + # normalized response of a dipolar kick in a quad from the model (all bpms) + # normalized response of horizontal steerer from the model at bpm #i + # normalized response of vertical steerer from the model at bpm #i + + # Retrieve model handle + """ + Calculate normalized model responses for the alignment scan. + + The responses describe the effect of a dipole kick at the quadrupole + and the horizontal and vertical steerers at the reference BPM. + + Parameters + ---------- + tunename : str + Name of the tune-correction tool. + bpmname : str + Name of the BPM array. + quadname : str + Name of the quadrupole. + steererhname : str + Name of the horizontal steerer. + steerervname : str + Name of the vertical steerer. + bpmi : int + Index of the reference BPM. + dk0 : object + Small calibration kick used to calculate model responses. + """ + design = self.peer.peer.design + + # handles + quad = design.magnet.get(quadname) + sth = design.magnet.get(steererhname) + stv = design.magnet.get(steerervname) + orbit = design.bpms.get(bpmname).positions + tune_design = design.get_tune_tuning(tunename) + tune_live = self._peer.get_tune_tuning(tunename) + + # Get tune from live and adjust the model to improve quad response phase + tune0 = tune_design.readback() + tune = tune_live.readback() + logger.debug(f"Live tune: {tune}") + logger.debug(f"Model tune: {tune0}") + tune_design.set(tune) + logger.debug(f"Model tune: {tune_design.readback()}") + + # quadrupole + a0 = quad.strength.get("PolynomA", 0) + b0 = quad.strength.get("PolynomB", 0) + step = [-dk0, 0, dk0] + + orb0 = orbit.get() + quad.strength.set(b0 - dk0, "PolynomB", 0) + orbm = orbit.get() + quad.strength.set(b0 + dk0, "PolynomB", 0) + orbp = orbit.get() + quad.strength.set(b0, "PolynomB", 0) + + orbx = [orbm[:, 0], orb0[:, 0], orbp[:, 0]] + fit = np.polynomial.polynomial.polyfit(step, orbx, 1) + ref_ios_x = fit[1] + + quad.strength.set(a0 - dk0, "PolynomA", 0) + orbm = orbit.get() + quad.strength.set(a0 + dk0, "PolynomA", 0) + orbp = orbit.get() + quad.strength.set(a0, "PolynomA", 0) + + orby = [orbm[:, 1], orb0[:, 1], orbp[:, 1]] + fit = np.polynomial.polynomial.polyfit(step, orby, 1) + ref_ios_y = fit[1] + + # steerers + a0 = sth.strength.get() + b0 = stv.strength.get() + step = [-dk0, 0, dk0] + + orb0 = orbit.get() + sth.strength.set(b0 - dk0) + orbm = orbit.get() + sth.strength.set(b0 + dk0) + orbp = orbit.get() + sth.strength.set(b0) + + orbx = [orbm[bpmi, 0], orb0[bpmi, 0], orbp[bpmi, 0]] + fit = np.polynomial.polynomial.polyfit(step, orbx, 1) + bpm_fact_x = fit[1] + + stv.strength.set(a0 - dk0) + orbm = orbit.get() + stv.strength.set(a0 + dk0) + orbp = orbit.get() + stv.strength.set(a0) + + orby = [orbm[bpmi, 1], orb0[bpmi, 1], orbp[bpmi, 1]] + fit = np.polynomial.polynomial.polyfit(step, orby, 1) + bpm_fact_y = fit[1] + + # Restore tune + tune_design.set(tune0) + + ref = np.array([ref_ios_x, ref_ios_y]).T + return ref, bpm_fact_x, bpm_fact_y + + def _fit_kick(self, meas, ref, mask): + # Correlate measured ios and theoretical one + + """ + Fit a scale factor between measured and reference orbit shifts. + + The fit is performed through the origin using the selected samples. + This estimates the kick amplitude that best matches ``ref`` to + ``meas`` in a least-squares sense. + + Parameters + ---------- + meas : array_like + Measured induced orbit shifts. + ref : array_like + Reference or theoretical orbit shifts. + mask : array_like + Boolean mask selecting samples included in the fit. + + Returns + ------- + float + Fitted scale factor. Returns ``0`` when the selected reference + shifts contain no signal. + """ + xy = np.multiply(meas[mask], ref[mask]) + xx = np.multiply(ref[mask], ref[mask]) + if sum(xx) == 0: + return 0 + else: + return sum(xy) / sum(xx) + + def _get_averaged_orbit(self): + # Get averaged orbit + + """Return the orbit averaged over the configured measurements.""" + avgorb = np.zeros((len(self._bpms), 2)) + for avg in range(self._nb_meas): + o = self._bpms.positions.get() + avgorb += o + if avg < self._nb_meas - 1: + time.sleep(self._sleep_meas) + + avgorb /= float(self._nb_meas) + return avgorb + + def _one_step_dk(self, dk0: list[float], dk1: float, bipolar_delta: bool): + # Measrue IOS + + """ + Measure the induced orbit shift for one quadrupole-strength step. + + The configured steerers and quadrupole are changed temporarily. The + orbit is measured before and after the quadrupole step, then the + quadrupole is restored to its initial strength. For bipolar steps, the + response is calculated from both positive and negative perturbations. + + Parameters + ---------- + dk0 : list[float] + Horizontal and vertical steerer kicks to apply. + dk1 : float + Quadrupole-strength step. + bipolar_delta : bool + If ``True``, measure both positive and negative quadrupole steps. + + Returns + ------- + tuple + ``(x, dkx, y, dky, ios_x, ios_y)`` containing the orbit at the + reference BPM, fitted horizontal and vertical kick factors, and + the horizontal and vertical induced orbit shifts. + + Raises + ------ + PyAMLException + If either requested steerer kick exceeds 200 microradians. + """ + if any(abs(dk) > 200e-6 for dk in dk0): + raise PyAMLException("Requested dk too high (>200urad), consider using bump") + + # Set steerer + if np.fabs(dk0[0]) > 0: + _str = dk0[0] + self._initial_k0[0] + self._h_steer.strength.set(_str) + self.send_callback(Action.APPLY, {"step": self._step, "magnet": self._h_steer.name, "strength": _str}) + if np.fabs(dk0[1]) > 0: + _str = dk0[1] + self._initial_k0[1] + self._v_steer.strength.set(_str) + self.send_callback(Action.APPLY, {"step": self._step, "magnet": self._v_steer.name, "strength": _str}) + + time.sleep(self._sleep_step) + orb0 = self._get_averaged_orbit() + + # Set quad + _str = self._initial_k1 + dk1 * self._quad_polarity + self._quad.strength.set(_str) + self.send_callback(Action.APPLY, {"step": self._step, "magnet": self._quad.name, "strength": _str}) + time.sleep(self._sleep_step) + orbp = self._get_averaged_orbit() + + ios_x = [] + ios_y = [] + + if bipolar_delta: + # one more point at k1 - dk1 + _str = self._initial_k1 - dk1 * self._quad_polarity + self._quad.strength.set(_str) + self.send_callback(Action.APPLY, {"step": self._step, "magnet": self._quad.name, "strength": _str}) + time.sleep(self._sleep_step) + orbm = self._get_averaged_orbit() + # take slopes and compute corresponding delta orbit + stepx = [-dk1 * self._quad_polarity, 0, dk1 * self._quad_polarity] + orbx = [orbm[:, 0], orb0[:, 0], orbp[:, 0]] + fit = np.polynomial.polynomial.polyfit(stepx, orbx, 1) + ios_x = fit[1] * dk1 + + orby = [orbm[:, 1], orb0[:, 1], orbp[:, 1]] + fit = np.polynomial.polynomial.polyfit(stepx, orby, 1) + ios_y = fit[1] * dk1 + else: + ios_x = orbp[:, 0] - orb0[:, 0] + ios_y = orbp[:, 1] - orb0[:, 1] + + # resotre quad + _str = self._initial_k1 + self._quad.strength.set(_str) + self.send_callback(Action.APPLY, {"step": self._step, "magnet": self._quad.name, "strength": _str}) + + nanx = ~np.isnan(ios_x) + x = orb0[self._bpmi, 0] + dkx = self._fit_kick(ios_x, self._ref_ios[:, 0], nanx) + + nany = ~np.isnan(ios_y) + y = orb0[self._bpmi, 1] + dky = self._fit_kick(ios_y, self._ref_ios[:, 1], nany) + + return x, dkx, y, dky, ios_x, ios_y + + def measure( + self, + sleep_between_step: Optional[float] = None, + n_avg_meas: Optional[int] = None, + sleep_between_meas: Optional[float] = None, + callback: Optional[Callable] = None, + plane: Optional[str] = None, + ): + """ + Measure BBA. + + **Example** + + .. code-block:: python + + sr = Accelerator.load("tests/config/EBSOrbit.yaml") + SR = sr.live + bba = SR.get_bba("BBA2-BPM_C04-04") + + # Add a misalignement + SR.get_bpm("BPM_C04-04").offset.set([200e-6,-150e-6]) + + bba.measure(sleep_between_step=6,plane='V',callback=bba_callback) + + print(f"HOffset: {bba.h_offset()*1e6:.3f} um {bba.h_offset_error()}") + print(f"VOffset: {bba.v_offset()*1e6:.3f} um {bba.v_offset_error()}") + + bba.plot_data() + + Parameters + ---------- + sleep_between_step : float + Default time sleep after steerer or quad excitation + Default: from config + n_avg_meas : int, optional + Default number of orbit measurement per step used for averaging + Default from config + sleep_between_meas : float + Default time sleep between two orbit measurment + Default: from config + callback : Callable, optional + example: callback(action:int, callback_data: 'Complicated struct') + callback is executed after each strength setting and after each orbit + reading. + If the callback returns false, then the process is aborted. + plane : str, optional + Plane to perform ("H" or "V", None => both plane) + """ + self._nb_meas = n_avg_meas if n_avg_meas is not None else self.n_avg_meas + self._sleep_step = sleep_between_step if sleep_between_step is not None else self.sleep_between_step + self._sleep_meas = sleep_between_meas if sleep_between_meas is not None else self.sleep_between_meas + + # Device handles + self.check_peer() + self._h_steer = self.peer.magnet.get(self.hcorr_name) + self._v_steer = self.peer.magnet.get(self.vcorr_name) + self._quad = self.peer.magnet.get(self.quad_name) + self._bpms = self.peer.bpms.get(self.bpm_array_name) + self._bpmi = self._bpms.names().index(self.bpm_name) + + # Initial values + self._initial_k0 = [self._h_steer.strength.get(), self._v_steer.strength.get()] + self._initial_k1 = self._quad.strength.get() + self._quad_polarity = np.sign(self._initial_k1) if self._initial_k1 != 0 else 1 + + self._ref_ios, fx, fy = self._init_responses( + self.tune_correction_name, + self.bpm_array_name, + self.quad_name, + self.hcorr_name, + self.vcorr_name, + self._bpmi, + ) + + dk0h = self.hcorr_delta if plane is None or plane == "H" else 0 + dk0v = self.vcorr_delta if plane is None or plane == "V" else 0 + dk1 = self.quad_delta + bidelta = self.bipolar_delta + doH = dk0h != 0 + doV = dk0v != 0 + aborted = False + err = None + + logger.debug(f"Initial H corrector {self.hcorr_name} value: {self._initial_k0[0]} rad") + logger.debug(f"Initial V corrector {self.vcorr_name} value: {self._initial_k0[1]} rad") + logger.debug(f"Initial quad {self.quad_name} value: {self._initial_k1} m-1") + + try: + self._register_callback(callback) + self._init_measure() + self.latest_measurement["HData"] = None + self.latest_measurement["VData"] = None + X = BBAData() + Y = BBAData() + + # Mini cycle + if self.minicycle_sleep_time > 0: + logger.debug(f"Quad mini cycling {self.quad_name}") + _str = self._initial_k1 + dk1 * self._quad_polarity + self._quad.strength.set(_str) + self.send_callback(Action.APPLY, {"step": -1, "magnet": self._quad.name, "strength": _str}) + time.sleep(self.minicycle_sleep_time) + _str = self._initial_k1 + self._quad.strength.set(_str) + self.send_callback(Action.APPLY, {"step": -1, "magnet": self._quad.name, "strength": _str}) + time.sleep(self.minicycle_sleep_time) + + opt_found = False + self._step = 0 + stx = 0 + sty = 0 + while not opt_found and self._step < 9: + ist = self._step % 3 + _from = f"{stx},{sty}" + + if ist == 0: + stx -= dk0h + sty -= dk0v + _to = f"{stx},{sty}" + logger.debug(f"Moving in the negative direction: {_from} -> {_to}") + + if ist == 1: + stx += 2 * dk0h + sty += 2 * dk0v + _to = f"{stx},{sty}" + logger.debug(f"Moving in the positive direction: {_from} -> {_to}") + + if ist == 2: + H_found = False + V_found = False + + if doH: + stx, _, _ = BBA2._x_intercept(X.steps, X.k, 2) + H_found = X.steps[-2] <= stx <= X.steps[-1] # don't rely on extrapolation + if doV: + sty, _, _ = BBA2._x_intercept(Y.steps, Y.k, 2) + V_found = Y.steps[-2] <= sty <= Y.steps[-1] # don't rely on extrapolation + + opt_found = ( + doH and not doV and H_found or not doH and doV and V_found or doH and doV and H_found and V_found + ) + + _to = f"{stx},{sty}" + logger.debug(f"Moving to the best guess: {_from} -> {_to}") + + x, dkx, y, dky, dataxbpm, dataybpm = self._one_step_dk([stx, sty], dk1, bidelta) + X.append(stx, dkx, x, dataxbpm) + Y.append(sty, dky, y, dataybpm) + + if doH: + self.send_callback(Action.MEASURE, {"step": self._step, "plane": "H", "bpm_pos": x, "ios": dataxbpm}) + + if doV: + self.send_callback(Action.MEASURE, {"step": self._step, "plane": "V", "bpm_pos": y, "ios": dataybpm}) + + self._step += 1 + + # Final step + + if doH: + stx, lxfit, errx = BBA2._x_intercept(X.steps, X.k, 3) + + if doV: + sty, lyfit, erry = BBA2._x_intercept(Y.steps, Y.k, 3) + + _to = f"{stx},{sty}" + logger.debug(f"Moving to the optimum: {_to}") + + x, dkx, y, dky, dataxbpm, dataybpm = self._one_step_dk([stx, sty], dk1, bidelta) + X.append(stx, dkx, x, dataxbpm) + Y.append(sty, dky, y, dataybpm) + + if doH: + X.update_offset(x, errx * np.fabs(fx), lxfit) + self.latest_measurement["HData"] = X + + if doV: + Y.update_offset(y, erry * np.fabs(fy), lyfit) + self.latest_measurement["VData"] = Y + + except Exception as ex: + err = ex + except KeyboardInterrupt as ex: + aborted = True + finally: + # Restore steerer/quad strength + if doH: + self._h_steer.strength.set(self._initial_k0[0]) + if doV: + self._v_steer.strength.set(self._initial_k0[1]) + self._quad.strength.set(self._initial_k1) + self.send_callback( + Action.RESTORE, + {}, + raiseException=False, + ) + + if err is not None: + raise (err) + + if aborted: + logger.warning(f"{self.get_name()} : measurement aborted (settings not restored)") + return False + + return True + + def h_offset(self) -> float: + """Return the measured horizontal magnetic-center offset.""" + return self.latest_measurement["HData"].offset if self.latest_measurement["HData"] is not None else np.nan + + def h_offset_error(self) -> float: + """Return the uncertainty of the horizontal center offset.""" + return self.latest_measurement["HData"].error if self.latest_measurement["HData"] is not None else np.nan + + def v_offset(self) -> float: + """Return the measured vertical magnetic-center offset.""" + return self.latest_measurement["VData"].offset if self.latest_measurement["VData"] is not None else np.nan + + def v_offset_error(self) -> float: + """Return the uncertainty of the vertical center offset.""" + return self.latest_measurement["VData"].error if self.latest_measurement["VData"] is not None else np.nan + + def plot_plane_data(self, ax, plane: str): + """ + Plot measured kicks and the fitted alignment response for one plane. + + Parameters + ---------- + ax : object + Matplotlib axes on which to draw the data. + plane : str + Plane data key, typically ``"HData"`` or ``"VData"``. + """ + yp = self.latest_measurement[plane].k + xp = self.latest_measurement[plane].steps + + b = self.latest_measurement[plane].lastfit[0] + a = self.latest_measurement[plane].lastfit[1] + + ax.plot(xp, yp, marker="o", linewidth=0) + ax.axline((0, b), slope=a, linestyle="--", color="lightblue", label="last fit") + ax.plot(xp[-4:-1], yp[-4:-1], color="salmon", marker="o", linewidth=0, label="last fit") + ax.plot(xp[-1:], yp[-1:], color="green", marker="o", linewidth=0, label="optimum") + ax.set_xlabel(f"Steerer (rad)\nOptimun kick @ bpm={self.latest_measurement[plane].offset * 1e6:.3f} um") + ax.set_ylabel("Fitted kick") + ax.grid() + ax.legend() + + def plot_data(self): + """ + Plot BBA data. + """ + + noH = "HData" not in self.latest_measurement or self.latest_measurement["HData"] is None + noV = "VData" not in self.latest_measurement or self.latest_measurement["VData"] is None + nrow = 0 if noH else 1 + nrow += 0 if noV else 1 + + if nrow == 0: + raise PyAMLException("No BBA data to plot, please call measure() first") + + fig = plt.figure() + irow = 1 + if not noH: + ax = fig.add_subplot(nrow, 1, irow) + self.plot_plane_data(ax, "HData") + irow += 1 + if not noV: + ax = fig.add_subplot(nrow, 1, irow) + self.plot_plane_data(ax, "VData") + + fig.tight_layout() + fig.canvas.manager.set_window_title(f"BBA {self.bpm_name}") + + plt.show() diff --git a/pyaml/tuning_tools/chromaticity.py b/pyaml/tuning_tools/chromaticity.py index a57457cd2..280c9690a 100644 --- a/pyaml/tuning_tools/chromaticity.py +++ b/pyaml/tuning_tools/chromaticity.py @@ -1,19 +1,23 @@ +""" +Chromaticity correction and response-matrix tools. + +The :class:`Chromaticity` tool reads measured chromaticity, computes sextupole +strength corrections from a response matrix, and applies those corrections to +an accelerator model or control-system interface. +""" + from pathlib import Path from typing import TYPE_CHECKING from .. import PyAMLException -from ..common.element import ElementConfigModel -from ..diagnostics.chromaticity_monitor import ChomaticityMonitor +from ..validation import DynamicValidation, register_schema +from .chromaticity_monitor import ChromaticityMonitor from .response_matrix_data import ResponseMatrixData from .tuning_tool import TuningTool if TYPE_CHECKING: from ..arrays.magnet_array import MagnetArray -try: - from typing import Self # Python 3.11+ -except ImportError: - from typing_extensions import Self # Python 3.10 and earlier import logging import time @@ -25,55 +29,71 @@ PYAMLCLASS = "Chromaticity" -class ConfigModel(ElementConfigModel): +@register_schema +class Chromaticity(TuningTool, DynamicValidation): """ - Configuration model for Tune + Adjust horizontal and vertical chromaticity with sextupole strengths. + + A response matrix maps sextupole-strength changes to chromaticity changes. + Its pseudoinverse is used to calculate the strength correction required for + a requested chromaticity change. Parameters ---------- + name : str + Name of the tuning tool. sextu_array_name : str - Array name of sextu used to adjust the chromaticity - chromaticty_monitor_name : str - Name of the diagnostic pyaml device for measuring the chromaticity + Name of the sextupole array used to adjust the chromaticity. + chromaticity_monitor_name : str + Name of the chromaticity monitor used for readback. response_matrix : str | ResponseMatrixData - filename or data of the chromaticity response matrix - """ - - sextu_array_name: str - chromaticty_monitor_name: str - response_matrix: str | ResponseMatrixData + Chromaticity response matrix or path to a saved response matrix file. - -class Chromaticity(TuningTool): - """ - Class providing chromaticity adjustment tool + Attributes + ---------- + response_matrix + Return the loaded chromaticity response matrix, if available. + + Methods + ------- + load(load_path) + Load a chromaticity response matrix and prepare its pseudoinverse. + get() + Return the requested horizontal and vertical chromaticity. + readback() + Measure and return the current horizontal and vertical chromaticity. + set(chroma, iter=1, wait_time=0.0) + Iteratively correct chromaticity to a requested setpoint. + correct(dchroma) + Calculate sextupole-strength changes for a chromaticity change. + add(dchroma, wait_time=0.0) + Apply a chromaticity correction relative to the current setpoint. """ - def __init__(self, cfg: ConfigModel): + def __init__( + self, name: str, sextu_array_name: str, chromaticity_monitor_name: str, response_matrix: str | ResponseMatrixData + ): """ - Construct a chromaticity adjustment object. - - Parameters - ---------- - cfg : ConfigModel - Configuration for the tune adjustment. + Initialize a chromaticity adjustment tool. """ - super().__init__(cfg.name) - self._cfg = cfg + super().__init__(name) + self.sextu_array_name = sextu_array_name + self._chromaticity_monitor_name = chromaticity_monitor_name + self.response_matrix_file = response_matrix self._response_matrix = None self._correctionmat = None # If the configuration response matrix is a filename, load it - if type(cfg.response_matrix) is str: + if type(self.response_matrix_file) is str: try: - cfg.response_matrix = ResponseMatrixData.load(cfg.response_matrix) + self._response_matrix = ResponseMatrixData.load(self.response_matrix_file) except Exception as e: logger.warning(f"{str(e)}") - cfg.response_matrix = None + self._response_matrix = None # Invert matrix - if cfg.response_matrix: - self._response_matrix = np.array(cfg.response_matrix._cfg.matrix) + if self._response_matrix: + self._response_matrix = np.array(self._response_matrix.matrix) self._correctionmat = np.linalg.pinv(self._response_matrix) # TODO: Initialise first setpoint @@ -81,59 +101,55 @@ def __init__(self, cfg: ConfigModel): @property def response_matrix(self) -> ResponseMatrixData | None: - """ - Return the response matrix if it has been loaded None otherwise - """ - return self._cfg.response_matrix + """Return the loaded chromaticity response matrix, if available.""" + return self._response_matrix def load(self, load_path: Path): """ - Dynamically loads a response matrix. + Load a chromaticity response matrix and prepare its pseudoinverse. Parameters ---------- load_path : Path - Filename of the :class:`~.ResponseMatrixData` to load + Path to the serialized :class:`~.ResponseMatrixData` file. """ - self._cfg.response_matrix = ResponseMatrixData.load(load_path) - self._response_matrix = np.array(self._cfg.response_matrix._cfg.matrix) + self._response_matrix = ResponseMatrixData.load(load_path) + self._response_matrix = np.array(self._response_matrix.matrix) self._correctionmat = np.linalg.pinv(self._response_matrix) @property - def _cm(self) -> "ChomaticityMonitor": + def _cm(self) -> "ChromaticityMonitor": + """Return the chromaticity monitor.""" self.check_peer() - return self.peer.get_chromaticity_monitor(self._cfg.chromaticty_monitor_name) + return self.peer.get_chromaticity_monitor(self._chromaticity_monitor_name) @property def _sextu(self) -> "MagnetArray": + """Return the sextupole array.""" self.check_peer() - return self.peer.get_magnets(self._cfg.sextu_array_name) + return self.peer.magnets.get(self.sextu_array_name) def get(self): - """ - Return the chromaticity setpoint - """ + """Return the requested horizontal and vertical chromaticity.""" return self._setpoint def readback(self): - """ - Launch a chromaticty scan and returns the measured chromaticity. - """ + """Measure and return the current horizontal and vertical chromaticity.""" self._cm.measure() return self._cm.chromaticity.get() def set(self, chroma: np.array, iter: int = 1, wait_time: float = 0.0): """ - Sets the chromaticity + Iteratively correct chromaticity to a requested setpoint. Parameters ---------- - chromaticity : np.array - Chromaticity setpoint - iter_nb : int - Number of iteration + chroma : numpy.ndarray + Target horizontal and vertical chromaticity values. + iter : int + Number of correction iterations. wait_time : float - Time to wait in second between 2 iterations + Delay in seconds between correction iterations. """ for i in range(iter): diff_chroma = chroma - self.readback() @@ -144,12 +160,23 @@ def set(self, chroma: np.array, iter: int = 1, wait_time: float = 0.0): def correct(self, dchroma: np.array) -> np.array: """ - Return delta strengths for chromaticity correction + Calculate sextupole-strength changes for a chromaticity change. Parameters ---------- - dchroma : np.array - Delta chroma + dchroma : numpy.ndarray + Desired horizontal and vertical chromaticity change. + + Returns + ------- + numpy.ndarray + Sextupole-strength changes obtained from the response-matrix + pseudoinverse. + + Raises + ------ + PyAMLException + If no response matrix has been loaded or measured. """ if self._correctionmat is None: raise PyAMLException("Chromaticity.correct(): no matrix loaded or measured") @@ -157,14 +184,14 @@ def correct(self, dchroma: np.array) -> np.array: def add(self, dchroma: np.array, wait_time: float = 0.0): """ - Add delta chromaticity to the actual chromaticity + Apply a chromaticity correction relative to the current setpoint. Parameters ---------- - dchroma : np.array - Delta tune - iter_nb: int - wait_time: float + dchroma : numpy.ndarray + Horizontal and vertical chromaticity change to apply. + wait_time : float + Delay in seconds after changing sextupole strengths. """ strengths = self._sextu.strengths.get() strengths += self.correct(dchroma) diff --git a/pyaml/diagnostics/chromaticity_monitor.py b/pyaml/tuning_tools/chromaticity_monitor.py similarity index 59% rename from pyaml/diagnostics/chromaticity_monitor.py rename to pyaml/tuning_tools/chromaticity_monitor.py index 4c4ea1ccc..cd9aa3026 100644 --- a/pyaml/diagnostics/chromaticity_monitor.py +++ b/pyaml/tuning_tools/chromaticity_monitor.py @@ -1,76 +1,62 @@ -from ..common.abstract import ReadFloatArray -from ..common.constants import Action -from ..common.element import ElementConfigModel -from ..common.exception import PyAMLException -from ..tuning_tools.measurement_tool import MeasurementTool, MeasurementToolConfigModel +""" +Chromaticity and dispersion measurement tools. + +The :class:`ChromaticityMonitor` acquires and exposes fitted chromaticity or +dispersion data from sextupole-based measurements, including read access to +the resulting values and their associated units. +""" -try: - from typing import Self # Python 3.11+ -except ImportError: - from typing_extensions import Self # Python 3.10 and earlier import logging +from collections.abc import Callable from time import sleep import matplotlib.pyplot as plt import numpy as np -from pydantic import ConfigDict - -logger = logging.getLogger(__name__) - -PYAMLCLASS = "ChomaticityMonitor" - - -class ConfigModel(MeasurementToolConfigModel): - """ - Configuration model for Chromaticity Monitor. - Parameters - ---------- - betatron_tune_name : str - Name of the diagnostic pyaml device for measuring the tune - rf_plant_name : str - Name of main RF frequency plant - bpm_array_name : str,optional - Name of main BPM array used for dispersion fit - e_delta : float, optional - Default variation of relative energy during chromaticity measurement: - f0 - f0 * E_delta * alphac < f_RF < f0 + f0 * E_delta * alphac, - by default 0.001 - max_e_delta : float, optional - Maximum authorized variation of relative energy during chromaticity - measurement, by default 0.004 - fit_order : int, optional - Chomaticity fitting order, by default 1 - fit_disp_order : int, optional - Dispersion fitting order, by default 1 - fit_dispersion : bool, optional - Dispersion fitting, by default False - """ +from ..common.abstract import ReadFloatArray +from ..common.constants import Action +from ..common.element import __pyaml_repr__ +from ..common.exception import PyAMLException +from ..tuning_tools.measurement_tool import MeasurementTool +from ..validation import DynamicValidation, register_schema - model_config = ConfigDict(arbitrary_types_allowed=True, extra="forbid") +logger = logging.getLogger(__name__) - betatron_tune_name: str - rf_plant_name: str - bpm_array_name: str | None = None - e_delta: float = 0.001 - max_e_delta: float = 0.004 - fit_order: int = 1 - fit_disp_order: int = 1 - fit_dispersion: bool = False +PYAMLCLASS = "ChromaticityMonitor" class RChromaDispArray(ReadFloatArray): """ Class providing read access to chromaticity or dispersion. Returns arrays of shape (fit_order,2) or None + + Parameters + ---------- + parent : 'ChromaticityMonitor' + Monitor owning the measured values. + name : str + Attribute of the parent monitor to read, such as chromaticity or dispersion. + unit : str + Unit reported for the values, such as ``m``. + + Methods + ------- + get() + Return the latest chromaticity or dispersion values. + unit() + Return the unit of the reported values. """ - def __init__(self, parent: "ChomaticityMonitor", name: str, unit: str): + def __init__(self, parent: "ChromaticityMonitor", name: str, unit: str): + """ + Initialize the RChromaDispArray. + """ self._parent = parent self._name = name self._unit = unit def get(self) -> np.array: + """Return the latest chromaticity or dispersion values.""" last = self._parent.latest_measurement if last is not None and self._name in last: return np.array(last[self._name]) @@ -78,30 +64,112 @@ def get(self) -> np.array: return None def unit(self) -> str: + """Return the unit of the reported values.""" return self.unit -class ChomaticityMonitor(MeasurementTool): +@register_schema +class ChromaticityMonitor(MeasurementTool, DynamicValidation): """ Class providing access to a chromaticity monitor of a physical or simulated lattice. The monitor provides horizontal and vertical chromaticity measurements. + + Parameters + ---------- + name : str + Name of the chromaticity monitor. + betatron_tune_name : str + Name of the betatron tune monitor used to measure the horizontal + and vertical tunes. + rf_plant_name : str + Name of the RF plant used to vary the RF frequency. + bpm_array_name : str, optional + Name of the BPM array used for dispersion measurements. Required + only when dispersion fitting is enabled. + e_delta : float, optional + Default relative momentum deviation used during the measurement. + max_e_delta : float, optional + Maximum permitted relative momentum deviation. + fit_order : int, optional + Polynomial order used to fit the chromaticity. + fit_disp_order : int, optional + Polynomial order used to fit the dispersion. + fit_dispersion : bool, optional + Whether to fit the machine dispersion in addition to the + chromaticity. + n_step : int, optional + Number of RF frequency steps. + sleep_between_step : float, optional + Delay in seconds after changing the RF frequency. + n_avg_meas : int, optional + Number of tune (and orbit) measurements to average at each RF + frequency. + sleep_between_meas : float, optional + Delay in seconds between consecutive measurements during + averaging. + + Attributes + ---------- + chromaticity + Get the chromaticity values. + dispersion + Get the dispersion values. + + Methods + ------- + set_mcf(alphac) + Set the momentum-compaction factor for frequency-step measurements. + measure(...) + Main function for chromaticity measurement. + + :py:attr:`~pyaml.tuning_tools.measurement_tool.MeasurementTool.latest_measurement` contains: + fit(deltas, Q, order, orbit=None, fit_disp_order=None, do_plot=False) + Compute chromaticity (and dispersion) from input data and update + :py:attr:`~pyaml.tuning_tools.measurement_tool.MeasurementTool.latest_measurement`. """ - def __init__(self, cfg: ConfigModel): + def __init__( + self, + name: str, + betatron_tune_name: str, + rf_plant_name: str, + bpm_array_name: str | None = None, + e_delta: float = 0.001, + max_e_delta: float = 0.004, + fit_order: int = 1, + fit_disp_order: int = 1, + fit_dispersion: bool = False, + n_step: int = 1, + sleep_between_step: float = 0, + n_avg_meas: int = 1, + sleep_between_meas: float = 0, + ): """ - Construct a ChomaticityMonitor. + Initialize a chromaticity monitor. - Parameters - ---------- - cfg : ConfigModel - Configuration for the ChromaticityMonitor, including betatron - tune monitor, RF plant, and defaults parameters. + The monitor performs chromaticity measurements by varying the RF + frequency, acquiring tune measurements from a betatron tune monitor, + and optionally fitting the machine dispersion using BPM orbit data. """ - super().__init__(cfg.name) - self._cfg = cfg + + super().__init__(name) + + self.betatron_tune_name = betatron_tune_name + self.rf_plant_name = rf_plant_name + self.bpm_array_name = bpm_array_name + self.e_delta = e_delta + self.max_e_delta = max_e_delta + self.fit_order = fit_order + self.fit_disp_order = fit_disp_order + self.fit_dispersion = fit_dispersion + self.n_step = n_step + self.sleep_between_step = sleep_between_step + self.n_avg_meas = n_avg_meas + self.sleep_between_meas = sleep_between_meas + self._chromaticity = RChromaDispArray(self, "chromaticity", "1") - self._dipsersion = RChromaDispArray(self, "dispersion", "m") + self._dispersion = RChromaDispArray(self, "dispersion", "m") self._alphac = None @property @@ -117,6 +185,17 @@ def chromaticity(self) -> ReadFloatArray: return self._chromaticity def set_mcf(self, alphac: float): + """ + Set the momentum-compaction factor for frequency-step measurements. + + The factor is used to convert an RF-frequency variation into the + corresponding relative energy deviation when measuring chromaticity. + + Parameters + ---------- + alphac : float + Momentum-compaction factor, usually dimensionless. + """ self._alphac = alphac @property @@ -129,25 +208,26 @@ def dispersion(self) -> ReadFloatArray: ReadFloatArray Array of dispersion values [[dx, dy],[d'x, d'y],...] """ - return self._dipsersion + return self._dispersion def measure( self, - n_step: int = None, - alphac: float = None, - e_delta: float = None, - max_e_delta: float = None, - n_avg_meas: int = None, - sleep_between_meas: float = None, - sleep_between_step: float = None, - fit_order: int = None, - fit_disp_order: int = None, + n_step: int | None = None, + alphac: float | None = None, + e_delta: float | None = None, + max_e_delta: float | None = None, + n_avg_meas: int | None = None, + sleep_between_meas: float | None = None, + sleep_between_step: float | None = None, + fit_order: int | None = None, + fit_disp_order: int | None = None, fit_dispersion: bool | None = None, - do_plot: bool = None, - callback: callable = None, + do_plot: bool | None = None, + callback: Callable | None = None, ): """ Main function for chromaticity measurment. + :py:attr:`~pyaml.tuning_tools.measurement_tool.MeasurementTool.latest_measurement` contains: .. code-block:: python @@ -160,33 +240,33 @@ def measure( Parameters ---------- - n_step: int + n_step : int Default number of RF step during chromaticity measurment [default: from config] - alphac: float | None + alphac : float | None Moment compaction factor [default: from config] - w_delta: float + e_delta : float Default variation of relative energy during chromaticity measurment: f0 - f0 * E_delta * alphac < f_RF < f0 + f0 * E_delta * alphac [default: from config] - max_e_delta: float + max_e_delta : float Maximum autorized variation of relative energy during chromaticity measurment [default: from config] - n_avg_meas: int + n_avg_meas : int Default number of tune/orbit measurment per RF frequency [default: from config] - sleep_between_meas: float + sleep_between_meas : float Default time sleep between two tune measurment [default: from config] - sleep_between_step: float + sleep_between_step : float Default time sleep after RF frequency variation [default: from config] - fit_order: int + fit_order : int Fitting order [default: from config] fit_disp_order : int, optional Dispersion fitting order [default: from config] - fit_dispersion : bool, optionnal + fit_dispersion : bool, optional Fit dispersion, [default: from config] do_plot : bool Do you want to plot the fitting results ? - callback: Callable, optional + callback : Callable, optional Callback is executed after each measurement or setting. If the callback return false, then the process is aborted. callback_data dict contains: @@ -200,18 +280,17 @@ def measure( tune:np.array # The measured tune (on Action.MEASURE) orbit:np_array # The measured orbit, if fit_dispersion is True, (on Action.MEASURE) dtune:np.array # The tune variation (on Action.RESTORE) - """ - n_step = n_step if n_step is not None else self._cfg.n_step + n_step = n_step if n_step is not None else self.n_step alphac = alphac if alphac is not None else self._alphac - e_delta = e_delta if e_delta is not None else self._cfg.e_delta - max_e_delta = max_e_delta if max_e_delta is not None else self._cfg.max_e_delta - n_avg_meas = n_avg_meas if n_avg_meas is not None else self._cfg.n_avg_meas - sleep_between_meas = sleep_between_meas if sleep_between_meas is not None else self._cfg.sleep_between_meas - sleep_between_step = sleep_between_step if sleep_between_step is not None else self._cfg.sleep_between_step - fit_order = fit_order if fit_order is not None else self._cfg.fit_order - fit_disp_order = fit_disp_order if fit_disp_order is not None else self._cfg.fit_disp_order - fit_dispersion = fit_dispersion if fit_dispersion is not None else self._cfg.fit_dispersion + e_delta = e_delta if e_delta is not None else self.e_delta + max_e_delta = max_e_delta if max_e_delta is not None else self.max_e_delta + n_avg_meas = n_avg_meas if n_avg_meas is not None else self.n_avg_meas + sleep_between_meas = sleep_between_meas if sleep_between_meas is not None else self.sleep_between_meas + sleep_between_step = sleep_between_step if sleep_between_step is not None else self.sleep_between_step + fit_order = fit_order if fit_order is not None else self.fit_order + fit_disp_order = fit_disp_order if fit_disp_order is not None else self.fit_disp_order + fit_dispersion = fit_dispersion if fit_dispersion is not None else self.fit_dispersion if abs(e_delta) > abs(max_e_delta): logger.warning(f"e_delta={e_delta} is greater than max_e_delta={max_e_delta}") @@ -224,14 +303,14 @@ def measure( # Get devices self.check_peer() - tm = self.peer.get_betatron_tune_monitor(self._cfg.betatron_tune_name) - rf = self.peer.get_rf_plant(self._cfg.rf_plant_name) + tm = self.peer.get_betatron_tune_monitor(self.betatron_tune_name) + rf = self.peer.rf.get(self.rf_plant_name) bpms = None n_bpm = 0 orbit = None - if fit_dispersion and fit_disp_order is not None and self._cfg.bpm_array_name is not None: + if fit_dispersion and fit_disp_order is not None and self.bpm_array_name is not None: # For dispersion fit - bpms = self.peer.get_bpms(self._cfg.bpm_array_name) + bpms = self.peer.bpms.get(self.bpm_array_name) n_bpm = len(bpms) f0 = rf.frequency.get() @@ -307,14 +386,14 @@ def fit(self, deltas, Q, order, orbit=None, fit_disp_order=None, do_plot=False): Relative energy (delta) variation steps done. Q : array of [Qx,Qy] Horizontal,Vertical tune measured. - orbit: array of [[x0,y0],[x1,y1],...] - fit_order: int - Chromaticity fitting order + order : int + Chromaticity fitting order. + orbit : array of [[x0,y0],[x1,y1],...], optional + Horizontal and vertical orbit at each energy step, used to fit the dispersion. fit_disp_order : int, optional - Dispersion fitting order - plot : bool, optional - If True, plot the fit. - + Dispersion fitting order. + do_plot : bool, optional + If ``True``, plot the fit. """ chroma = np.polynomial.polynomial.polyfit(deltas, Q, order).T self.latest_measurement["chromaticity_fit"] = chroma @@ -365,3 +444,20 @@ def fit(self, deltas, Q, order, orbit=None, fit_disp_order=None, do_plot=False): fig.tight_layout() plt.show() + + def _after_attach(self): + """ + Recreate readback handles after attaching the monitor. + + The handles are bound to the attached monitor instance and therefore + must be refreshed after the monitor is copied and attached to an + element holder. + """ + self._chromaticity = RChromaDispArray(self, "chromaticity", "1") + self._dispersion = RChromaDispArray(self, "dispersion", "m") + + def __repr__(self): + """ + Implement the ``__repr__`` string. + """ + return __pyaml_repr__(self, exclude=["chromaticity", "dispersion"]) diff --git a/pyaml/tuning_tools/chromaticity_response_matrix.py b/pyaml/tuning_tools/chromaticity_response_matrix.py index 8b995fbf4..1c919fa9d 100644 --- a/pyaml/tuning_tools/chromaticity_response_matrix.py +++ b/pyaml/tuning_tools/chromaticity_response_matrix.py @@ -1,45 +1,86 @@ +""" +Chromaticity response-matrix measurement tools. + +The :class:`ChromaticityResponseMatrix` measures how sextupole-strength +changes affect horizontal and vertical chromaticity and stores the fitted +slopes as a response matrix. +""" + import logging import time +from dataclasses import asdict from typing import Callable, Optional import numpy as np -from pydantic import ConfigDict from ..common.constants import Action -from ..common.element import ElementConfigModel -from .measurement_tool import MeasurementTool, MeasurementToolConfigModel -from .response_matrix_data import ConfigModel as ResponseMatrixDataConfigModel +from ..validation import DynamicValidation, register_schema +from .measurement_tool import MeasurementTool +from .response_matrix_data import ResponseMatrixData logger = logging.getLogger(__name__) PYAMLCLASS = "ChromaticityResponseMatrix" -class ConfigModel(MeasurementToolConfigModel): +@register_schema +class ChromaticityResponseMatrix(MeasurementTool, DynamicValidation): """ - Configuration model for Tune response matrix + Measure the chromaticity response matrix of a lattice. + + This tool perturbs each sextupole in a sextupole array and measures the + resulting chromaticity variation using a chromaticity monitor. The measured + slopes are assembled into a response matrix with chromaticity components as + the observables and sextupoles as the variables. Parameters ---------- + name : str + Name of the response matrix measurement tool. sextu_array_name : str - Array name of sextupole used to adjust the chromaticity + Name of the sextupole array to excite. chromaticity_name : str - Name of the diagnostic chromaticy monitor + Name of the chromaticity monitor used to measure the response. sextu_delta : float - Delta strength used to get the response matrix + Default sextupole excitation applied during the measurement. + n_step : int, optional + Default number of excitation steps used to fit the response. + sleep_between_step : float, optional + Default delay in seconds after changing the sextupole strength. + n_avg_meas : int, optional + Default number of chromaticity measurements to average at each step. + sleep_between_meas : float, optional + Default delay in seconds between averaged measurements. + + Methods + ------- + measure(...) + Measure the chromaticity response matrix. """ - model_config = ConfigDict(arbitrary_types_allowed=True, extra="forbid") - - sextu_array_name: str - chromaticity_name: str - sextu_delta: float - + def __init__( + self, + name: str, + sextu_array_name: str, + chromaticity_name: str, + sextu_delta: float, + n_step: int = 1, + sleep_between_step: float = 0, + n_avg_meas: int = 1, + sleep_between_meas: float = 0, + ): + """ + Initialize the chromaticity response matrix measurement tool. + """ -class ChromaticityResponseMatrix(MeasurementTool): - def __init__(self, cfg: ConfigModel): - super().__init__(cfg.name) - self._cfg = cfg + super().__init__(name) + self.sextu_array_name = sextu_array_name + self.chromaticity_name = chromaticity_name + self.sextu_delta = sextu_delta + self.n_step = n_step + self.sleep_between_step = sleep_between_step + self.n_avg_meas = n_avg_meas + self.sleep_between_meas = sleep_between_meas self.aborted = False def measure( @@ -52,7 +93,8 @@ def measure( callback: Optional[Callable] = None, ): """ - Measure chromaticity response matrix. + Measure the chromaticity response matrix. + :py:attr:`~pyaml.tuning_tools.measurement_tool.MeasurementTool.latest_measurement` contains: .. code-block:: python @@ -80,21 +122,20 @@ def callback(action: Action, data:dict): acc.crm.save("ideal_crm.yaml", with_type="yaml") acc.crm.save("ideal_crm.npz", with_type="npz") - Parameters ---------- sextu_delta : float Delta strength used to get the response matrix - n_step: int, optional + n_step : int, optional Number of step for fitting the chomaticity slope [-sextu_delta/n_step..sextu_delta/n_step] Default from config - sleep_between_step: float - Default time sleep after sextu exitation + sleep_between_step : float + Default time sleep after sextu excitation Default: from config n_avg_meas : int, optional Default number of chromaticity measurement per step used for averaging Default from config - sleep_between_meas: float + sleep_between_meas : float Default time sleep between two chomaticity measurment Default: from config callback : Callable, optional @@ -114,11 +155,16 @@ def callback(action: Action, data:dict): chroma:np.array # The measured chroma (on Action.MEASURE) dchroma:np.array # The chroma variation (on Action.RESTORE) + Returns + ------- + bool + ``True`` when the response matrix is measured successfully; + ``False`` when the measurement is aborted by the callback. """ # Get devices self.check_peer() - sextus = self._peer.get_magnets(self._cfg.sextu_array_name) - cm = self._peer.get_chromaticity_monitor(self._cfg.chromaticity_name) + sextus = self._peer.magnets.get(self.sextu_array_name) + cm = self._peer.get_chromaticity_monitor(self.chromaticity_name) self._register_callback(callback) self._init_measure("pyaml.tuning_tools.response_matrix_data") @@ -131,11 +177,11 @@ def callback(action: Action, data:dict): return False initial_chroma = cm.chromaticity.get() - delta = sextu_delta if sextu_delta is not None else self._cfg.sextu_delta - nb_step = n_step if n_step is not None else self._cfg.n_step - nb_meas = n_avg_meas if n_avg_meas is not None else self._cfg.n_avg_meas - sleep_step = sleep_between_step if sleep_between_step is not None else self._cfg.sleep_between_step - sleep_meas = sleep_between_meas if sleep_between_meas is not None else self._cfg.sleep_between_meas + delta = sextu_delta if sextu_delta is not None else self.sextu_delta + nb_step = n_step if n_step is not None else self.n_step + nb_meas = n_avg_meas if n_avg_meas is not None else self.n_avg_meas + sleep_step = sleep_between_step if sleep_between_step is not None else self.sleep_between_step + sleep_meas = sleep_between_meas if sleep_between_meas is not None else self.sleep_between_meas err = None aborted = False @@ -206,12 +252,12 @@ def callback(action: Action, data:dict): logger.warning(f"{self.get_name()} : measurement aborted") return False - mat = ResponseMatrixDataConfigModel( + mat = ResponseMatrixData( matrix=chromamat.T.tolist(), variable_names=sextus.names(), observable_names=[cm.get_name() + ".x", cm.get_name() + ".y"], ) - self.latest_measurement.update(mat.model_dump()) + self.latest_measurement.update(asdict(mat)) self.latest_measurement["type"] = "pyaml.tuning_tools.response_matrix_data" return True diff --git a/pyaml/tuning_tools/dispersion.py b/pyaml/tuning_tools/dispersion.py index d62dbefe5..3efd54f3a 100644 --- a/pyaml/tuning_tools/dispersion.py +++ b/pyaml/tuning_tools/dispersion.py @@ -1,14 +1,20 @@ +""" +Beam-dispersion measurement tools. + +The :class:`Dispersion` tool varies an RF-plant frequency, measures the orbit +response with a BPM array, and stores the resulting horizontal and vertical +dispersion data. +""" + import logging -from typing import Callable, Optional, Self +from typing import Callable, Optional -from pydantic import ConfigDict from pySC.apps import measure_dispersion from pySC.apps.codes import DispersionCode from ..common.constants import Action -from ..common.element import ElementConfigModel -from ..common.element_holder import ElementHolder from ..external.pySC_interface import pySCInterface +from ..validation import DynamicValidation, register_schema from .measurement_tool import MeasurementTool logger = logging.getLogger(__name__) @@ -16,41 +22,79 @@ PYAMLCLASS = "Dispersion" -class ConfigModel(ElementConfigModel): +@register_schema +class Dispersion(MeasurementTool, DynamicValidation): """ - Configuration model for dispersion measurement + Measure beam dispersion by changing the RF frequency. + + The measurement uses a :class:`pySCInterface` to change the frequency of + an RF plant and acquire orbit data from a BPM array. Progress is reported + through the callback mechanism provided by :class:`MeasurementTool`. Parameters ---------- + name : str + Name of the dispersion measurement tool. bpm_array_name : str - BPM array name + Name of the BPM array used to measure the orbit. rf_plant_name : str - RF plant name + Name of the RF plant whose frequency is varied. frequency_delta : float - Frequency delta for measurement - """ - - model_config = ConfigDict(arbitrary_types_allowed=True, extra="forbid") - - bpm_array_name: str - rf_plant_name: str - frequency_delta: float + RF-frequency change applied during the measurement. + Attributes + ---------- + bpm_array_name : str + Name of the BPM array used for the measurement. + rf_plant_name : str + Name of the RF plant used for the measurement. + frequency_delta : float + RF-frequency change applied during the measurement. + + Methods + ------- + measure(set_waiting_time=0, callback=None) + Measure beam dispersion by varying the RF frequency. + get() + Return the most recently measured dispersion data. + """ -class Dispersion(MeasurementTool): - def __init__(self, cfg: ConfigModel): - super().__init__(cfg.name) - self._cfg = cfg + def __init__(self, name: str, bpm_array_name: str, rf_plant_name: str, frequency_delta: float): + """ + Initialize a beam-dispersion measurement tool. + """ + super().__init__(name) - self.bpm_array_name = cfg.bpm_array_name - self.rf_plant_name = cfg.rf_plant_name - self.frequency_delta = cfg.frequency_delta + self.bpm_array_name = bpm_array_name + self.rf_plant_name = rf_plant_name + self.frequency_delta = frequency_delta def measure( self, set_waiting_time: float = 0, callback: Optional[Callable] = None, ): + """ + Measure beam dispersion by varying the RF frequency. + + Measurements are reported through ``callback``. If the callback + requests an abort, the measurement returns ``False``; otherwise the + dispersion data are stored in ``latest_measurement``. + + Parameters + ---------- + set_waiting_time : float + Delay in seconds after changing the RF frequency. + callback : Optional[Callable] + Optional callback invoked after applying, measuring, and restoring + settings. + + Returns + ------- + bool + ``True`` when the measurement completes successfully, or ``False`` + when it is aborted by the callback. + """ element_holder = self._peer interface = pySCInterface( element_holder=element_holder, @@ -117,4 +161,5 @@ def measure( return True def get(self): + """Return the most recently measured dispersion data.""" return self.latest_measurement diff --git a/pyaml/tuning_tools/measurement_tool.py b/pyaml/tuning_tools/measurement_tool.py index e2e409554..7411c4a28 100644 --- a/pyaml/tuning_tools/measurement_tool.py +++ b/pyaml/tuning_tools/measurement_tool.py @@ -1,63 +1,81 @@ +""" +Base classes for accelerator measurement tools. + +Measurement tools perform scans or response measurements, report progress +through callbacks, and retain their latest results for inspection or export. +""" + +import copy import logging from abc import ABCMeta, abstractmethod from pathlib import Path -from typing import TYPE_CHECKING, Callable, Optional, Self - -from pydantic import ConfigDict +from typing import TYPE_CHECKING, Callable, Self from ..common.constants import Action -from ..common.element import Element, ElementConfigModel +from ..common.element import Element from ..common.exception import PyAMLException if TYPE_CHECKING: - from ..common.element_holder import ElementHolder + from ..common.holders.element_holder import ElementHolder logger = logging.getLogger(__name__) -class MeasurementToolConfigModel(ElementConfigModel): +class MeasurementTool(Element, metaclass=ABCMeta): """ - Measurement tool configuration model + Base class for response-matrix measurements and accelerator scans. + + Subclasses implement :meth:`measure` and may use the shared callback, + result-storage, attachment, and persistence helpers provided here. Parameters ---------- - n_step: int, optional - Number of measurement step [-delta/n_step..delta/n_step] - Default 1 - sleep_between_step: float, optional - Default sleep time after an actuator excitation - Default: 0 - n_avg_meas : int, optional - Default number of measurement per step used for averaging - Default 1 - sleep_between_meas: float, optional - Default sleep time between two measurments - Default: 0 - """ + name : object + Name of the measurement tool. - model_config = ConfigDict(arbitrary_types_allowed=True, extra="forbid") - - n_step: Optional[int] = 1 - sleep_between_step: Optional[float] = 0 - n_avg_meas: Optional[int] = 1 - sleep_between_meas: Optional[float] = 0 - - -class MeasurementTool(Element, metaclass=ABCMeta): - """ - Base class for measurement tool such as reponse matrix measurement or other scans. + Attributes + ---------- + latest_measurement + Data produced by the last measurement, or ``None`` before the first one. + + Methods + ------- + measure() + Run the measurement implemented by a subclass. + get() + Return the most recently stored measurement data. + save(save_path, with_type='json') + Save the latest measurement data to disk. + send_callback(action, cb_data, raiseException=True) + Notify the caller about measurement progress. + attach(peer) + Return a copy attached to an element holder. """ def __init__(self, name): - super().__init__(name) - self._latest_measurement: dict = None """ + Initialize a measurement tool. """ + super().__init__(name) + self._latest_measurement: dict = None self._peer: "ElementHolder" = None # Peer: ControlSystem or Simulator self._callback: Callable = None + def _fill_device(self, holder: "ElementHolder") -> None: + holder._fill_tool(self) + def _init_measure(self, measurement_type: str | None = None): # Initialize measurement data + # type is used there to be able to reload a measurement, typically a reponse matrix, using the PyAML factory. + """ + Reset the latest measurement before starting a new scan. + + Parameters + ---------- + measurement_type : str | None + Optional fully qualified configuration type to store with the + measurement data. + """ self._latest_measurement = {} if measurement_type is not None: self._latest_measurement["type"] = measurement_type @@ -65,49 +83,54 @@ def _init_measure(self, measurement_type: str | None = None): @abstractmethod def measure(self) -> bool: """ - Launch measurement + Run the measurement implemented by a subclass. + Returns ------- bool - True if the process has been aborted + ``True`` when the measurement completes; ``False`` when it is + aborted according to the subclass contract. """ raise NotImplementedError() @property def latest_measurement(self) -> dict: """ - Return last measurement data, a dictionary containing last measurement data. - See sub class of MeasurementTool to get description. + Return the most recently stored measurement data. Returns ------- dict - Return latest measurement or None + Measurement data, or ``None`` before the first measurement. """ return self._latest_measurement def get(self) -> dict: """ - Return last measurement data, a dictionary containing last measurement data. - See sub class of MeasurementTool to get description. + Return the most recently stored measurement data. Returns ------- dict - Return latest measurement or None + Measurement data, or ``None`` before the first measurement. """ return self._latest_measurement def save(self, save_path: Path, with_type: str = "json"): """ - Save measurement data + Save the latest measurement data to disk. Parameters ---------- - save_path: Path - Matrix filename - with_type: str - File type (json,yaml,npz) + save_path : Path + Destination filename. + with_type : str + Serialization format: ``"json"``, ``"yaml"``, or ``"npz"``. + + Raises + ------ + PyAMLException + If ``with_type`` is not a supported serialization format. """ if with_type == "json": import json @@ -129,8 +152,12 @@ def save(self, save_path: Path, with_type: str = "json"): def send_callback(self, action: Action, cb_data: dict, raiseException: bool = True): """ - Send callback from this Measurement tool to the caller. - If the callback returns False, the scan is aborted and actuators are restored to their orignal values. + Notify the caller about measurement progress. + + If the registered callback returns ``False``, the scan is aborted by + raising ``KeyboardInterrupt`` when ``raiseException`` is ``True``. + The measurement tool adds its mode and source to ``cb_data`` before + invoking the callback. Callback example: .. code-block:: python @@ -144,16 +171,23 @@ def callback(action: Action, data: dict): Parameters ---------- - action: Action - See :py:class:`pyaml.common.constants.Action` + action : Action + Measurement lifecycle event. - cb_data: dict - Callback data + cb_data : dict + Mutable event data passed to the callback. + raiseException : bool, optional + Whether a callback rejection should raise ``KeyboardInterrupt``. + + Returns + ------- + bool + Callback result, or ``True`` when no callback is registered. """ ok = True if self._callback is not None: # Add source and peer - cb_data["mode"] = f"{self.get_peer_name()}" + cb_data["mode"] = f"{self.attached_to()}" cb_data["source"] = self ok = self._callback(action, cb_data) if not ok and raiseException: @@ -162,13 +196,38 @@ def callback(action: Action, data: dict): return ok def _register_callback(self, callback: Callable): + """ + Register a progress callback for the next measurement. + + Parameters + ---------- + callback : Callable + Callable receiving an :class:`Action` and event-data dictionary. + """ self._callback = callback def attach(self, peer: "ElementHolder") -> Self: """ - Create a new reference to attach this measurement tool object to a simulator - or a control system. + Return a copy attached to an element holder. + + A shallow copy is created so the configured measurement tool remains + reusable. Subclasses can rebind internal handles in :meth:`_after_attach`. + + Parameters + ---------- + peer : 'ElementHolder' + Accelerator, simulator, or control-system element holder. + + Returns + ------- + Self + Attached copy of this measurement tool. """ - obj = self.__class__(self._cfg) + obj = copy.copy(self) + obj._after_attach() obj._peer = peer return obj + + def _after_attach(self) -> None: + """Hook for subclasses to rebind internal references after attach.""" + pass diff --git a/pyaml/tuning_tools/orbit.py b/pyaml/tuning_tools/orbit.py index 6baa1f884..2212c3f81 100644 --- a/pyaml/tuning_tools/orbit.py +++ b/pyaml/tuning_tools/orbit.py @@ -1,25 +1,24 @@ +""" +Orbit measurement and correction tools. + +The :class:`Orbit` tool reads orbit response data, computes corrector changes, +and applies horizontal, vertical, and optional RF corrections. +""" + import logging +from dataclasses import asdict from pathlib import Path -from typing import TYPE_CHECKING, Literal, Optional, Union - -try: - from typing import Self # Python 3.11+ -except ImportError: - from typing_extensions import Self # Python 3.10 and earlier +from typing import Literal, Optional, Union import numpy as np -from pydantic import ConfigDict - -if TYPE_CHECKING: - from ..common.element_holder import ElementHolder from pySC import ResponseMatrix as pySC_ResponseMatrix from pySC.apps import orbit_correction from ..arrays.magnet_array import MagnetArray -from ..common.element import Element, ElementConfigModel from ..common.exception import PyAMLException from ..external.pySC_interface import pySCInterface from ..rf.rf_plant import RFPlant +from ..validation import DynamicValidation, register_schema from .orbit_response_matrix_data import OrbitResponseMatrixData from .tuning_tool import TuningTool @@ -29,57 +28,112 @@ PYAMLCLASS = "Orbit" -class ConfigModel(ElementConfigModel): - model_config = ConfigDict(arbitrary_types_allowed=True, extra="forbid") - - bpm_array_name: str - hcorr_array_name: str - vcorr_array_name: str - rf_plant_name: Optional[str] = None - singular_values: Optional[int] = None - singular_values_H: Optional[int] = None - singular_values_V: Optional[int] = None - virtual_target: float = 0 - response_matrix: Union[str, OrbitResponseMatrixData] +@register_schema +class Orbit(TuningTool, DynamicValidation): + """ + Correct the measured orbit using a configured response matrix. + + Parameters + ---------- + name : str + Name of the orbit tool. + bpm_array_name : str + Name of the BPM array used for orbit readback. + hcorr_array_name : str + Name of the horizontal corrector array. + vcorr_array_name : str + Name of the vertical corrector array. + response_matrix : Union[str, OrbitResponseMatrixData] + Orbit response matrix or path to a serialized matrix. + rf_plant_name : Optional[str] + Optional RF plant used for RF orbit correction. + singular_values : Optional[int] + Common number of singular values retained for both planes. + singular_values_H : Optional[int] + Number of horizontal singular values retained. + singular_values_V : Optional[int] + Number of vertical singular values retained. + virtual_target : float + Target value for virtual orbit correction. + + Attributes + ---------- + response_matrix + Return the response matrix if it has been loaded None otherwise + Methods + ------- + load(load_path) + Dynamically loads a response matrix. + correct(...) + Perform orbit correction using the configured response matrix and corrector arrays. + set_weight(name, weight, plane=None) + Set the weight of a response-matrix input or output. + set_virtual_weight(weight) + Set the weight of the virtual orbit target. + set_rf_weight(weight) + Set the weight of the RF-frequency correction variable. + get_weight(name, plane=None) + Return the response-matrix weight for a named input or output. + get_virtual_weight() + Return the configured virtual-orbit target weight. + get_rf_weight() + Return the configured RF-frequency correction weight. + post_init() + Bind orbit corrector and RF handles after attachment. + """ + + def __init__( + self, + name: str, + bpm_array_name: str, + hcorr_array_name: str, + vcorr_array_name: str, + response_matrix: Union[str, OrbitResponseMatrixData], + rf_plant_name: Optional[str] = None, + singular_values: Optional[int] = None, + singular_values_H: Optional[int] = None, + singular_values_V: Optional[int] = None, + virtual_target: float = 0, + ): + """ + Initialize the Orbit. + """ + super().__init__(name) -class Orbit(TuningTool): - def __init__(self, cfg: ConfigModel): - super().__init__(cfg.name) - self._cfg = cfg - self.bpm_array_name = cfg.bpm_array_name - self.hcorr_array_name = cfg.hcorr_array_name - self.vcorr_array_name = cfg.vcorr_array_name + self.bpm_array_name = bpm_array_name + self.hcorr_array_name = hcorr_array_name + self.vcorr_array_name = vcorr_array_name self._pySC_response_matrix = None + self.rf_plant_name = rf_plant_name + self.virtual_target = virtual_target - self.virtual_target = cfg.virtual_target - - if cfg.singular_values is None: - if cfg.singular_values_H is None or cfg.singular_values_V is None: + if singular_values is None: + if singular_values_H is None or singular_values_V is None: raise PyAMLException( "Either `singular_values` or `singular_values_H` and `singular_values_V` must be provided." ) - self.singular_values_H = cfg.singular_values_H - self.singular_values_V = cfg.singular_values_V + self.singular_values_H = singular_values_H + self.singular_values_V = singular_values_V else: - if cfg.singular_values_H is not None or cfg.singular_values_V is not None: + if singular_values_H is not None or singular_values_V is not None: raise PyAMLException( "Either `singular_values` or `singular_values_H` and `singular_values_V` must be provided, not both." ) - self.singular_values_H = cfg.singular_values - self.singular_values_V = cfg.singular_values + self.singular_values_H = singular_values + self.singular_values_V = singular_values # If the configuration response matrix is a filename, load it - if type(cfg.response_matrix) is str: + if type(response_matrix) is str: try: - cfg.response_matrix = OrbitResponseMatrixData.load(cfg.response_matrix) + self._response_matrix = OrbitResponseMatrixData.load(response_matrix) except Exception as e: - logger.warning(f"Loading {cfg.response_matrix} failed {str(e)}") - cfg.response_matrix = None + logger.warning(f"Loading {response_matrix} failed {str(e)}") + self._response_matrix = None # Converts to self._pySC_response_matrix - if cfg.response_matrix: - self._set_response_matrix(cfg.response_matrix) + if self._response_matrix: + self._set_response_matrix(self._response_matrix) self._hcorr: MagnetArray = None self._vcorr: MagnetArray = None @@ -95,16 +149,30 @@ def load(self, load_path: Path): load_path : Path Filename of the :class:`~.OrbitResponseMatrixData` to load """ - self._cfg.response_matrix = OrbitResponseMatrixData.load(load_path) - self._set_response_matrix(self._cfg.response_matrix) + self._response_matrix = OrbitResponseMatrixData.load(load_path) + self._set_response_matrix(self.response_matrix) def _set_response_matrix(self, mat): - m = mat._cfg.model_dump() + """ + Configure the pySC response matrix from PyAML response data. + + The PyAML variable and observable fields are renamed to the names + expected by pySC, including their horizontal and vertical plane + metadata. The original PyAML model is retained for later access. + + Parameters + ---------- + mat : OrbitResponseMatrixData + Orbit response-matrix data containing the matrix, names, and + plane metadata. + """ + m = asdict(mat) m["input_names"] = m.pop("variable_names") m["output_names"] = m.pop("observable_names") m["input_planes"] = m.pop("variable_planes") m["output_planes"] = m.pop("observable_planes") - self._cfg.response_matrix = mat + m.pop("type", None) + self._response_matrix = mat self._pySC_response_matrix = pySC_ResponseMatrix.model_validate(m) @property @@ -112,7 +180,7 @@ def response_matrix(self) -> OrbitResponseMatrixData | None: """ Return the response matrix if it has been loaded None otherwise """ - return self._cfg.response_matrix + return self._response_matrix def correct( self, @@ -264,18 +332,83 @@ def correct( return def set_weight(self, name: str, weight: float, plane: Optional[Literal["H", "V"]] = None) -> None: + """ + Set the weight of a response-matrix input or output. + + Weights affect the relative importance of variables and observables + during orbit correction. A plane is required when ``name`` occurs in + more than one plane. + + Parameters + ---------- + name : str + Variable or observable name whose weight should be changed. + weight : float + New weight applied during orbit correction. + plane : Optional[Literal['H', 'V']] + Optional plane selector, either ``"H"`` or ``"V"``. + + Returns + ------- + None + This method does not return a value. + """ self._pySC_response_matrix.set_weight(name, weight, plane=plane) return def set_virtual_weight(self, weight: float) -> None: + """ + Set the weight of the virtual orbit target. + + Parameters + ---------- + weight : float + New virtual-target weight used during correction. + + Returns + ------- + None + This method does not return a value. + """ self._pySC_response_matrix.virtual_weight = weight return def set_rf_weight(self, weight: float) -> None: + """ + Set the weight of the RF-frequency correction variable. + + Parameters + ---------- + weight : float + New RF-variable weight used during correction. + + Returns + ------- + None + This method does not return a value. + """ self._pySC_response_matrix.rf_weight = weight return def get_weight(self, name: str, plane: Optional[Literal["H", "V"]] = None) -> float: + """ + Return the response-matrix weight for a named input or output. + + If the name is present in multiple planes, pass ``plane`` to select + the desired weight. + + Parameters + ---------- + name : str + Variable or observable name whose weight should be returned. + plane : Optional[Literal['H', 'V']] + Optional plane selector, either ``"H"`` or ``"V"``. + + Returns + ------- + float + Configured response-matrix weight. + """ names = [] planes = [] weights = [] @@ -306,17 +439,20 @@ def get_weight(self, name: str, plane: Optional[Literal["H", "V"]] = None) -> fl raise PyAMLException(f"More than one weight found, please select plane. {names=}, {planes=}, {weights=}") def get_virtual_weight(self) -> float: + """Return the configured virtual-orbit target weight.""" return self._pySC_response_matrix.virtual_weight def get_rf_weight(self) -> float: + """Return the configured RF-frequency correction weight.""" return self._pySC_response_matrix.rf_weight def post_init(self): - self._hcorr = self.peer.get_magnets(self._cfg.hcorr_array_name) - self._vcorr = self.peer.get_magnets(self._cfg.vcorr_array_name) + """Bind orbit corrector and RF handles after attachment.""" + self._hcorr = self.peer.magnets.get(self.hcorr_array_name) + self._vcorr = self.peer.magnets.get(self.vcorr_array_name) hvElts = [] hvElts.extend(self._hcorr) hvElts.extend(self._vcorr) self._hvcorr = MagnetArray("", hvElts) - if self._cfg.rf_plant_name is not None: - self._rf_plant = self.peer.get_rf_plant(self._cfg.rf_plant_name) + if self.rf_plant_name is not None: + self._rf_plant = self.peer.rf.get(self.rf_plant_name) diff --git a/pyaml/tuning_tools/orbit_response_matrix.py b/pyaml/tuning_tools/orbit_response_matrix.py index 064399d74..62fb755ba 100644 --- a/pyaml/tuning_tools/orbit_response_matrix.py +++ b/pyaml/tuning_tools/orbit_response_matrix.py @@ -1,55 +1,119 @@ +""" +Orbit response-matrix measurement tools. + +This module measures BPM orbit changes caused by horizontal and vertical +corrector perturbations and stores the fitted response in a structured data +model. +""" + import logging -from pathlib import Path -from typing import Callable, List, Optional, Self +from dataclasses import asdict +from typing import Callable, List, Optional import pySC -from pydantic import ConfigDict from pySC.apps import measure_ORM from pySC.apps.codes import ResponseCode from ..common.constants import Action from ..external.pySC_interface import pySCInterface -from .measurement_tool import MeasurementTool, MeasurementToolConfigModel -from .orbit_response_matrix_data import ConfigModel as OrbitResponseMatrixDataConfigModel +from ..validation import DynamicValidation, register_schema +from .measurement_tool import MeasurementTool +from .orbit_response_matrix_data import OrbitResponseMatrixData logger = logging.getLogger(__name__) PYAMLCLASS = "OrbitResponseMatrix" -class ConfigModel(MeasurementToolConfigModel): +@register_schema +class OrbitResponseMatrix(MeasurementTool, DynamicValidation): """ - Configuration model for orbit response matrix measurement + Measure an orbit response matrix using BPMs and orbit correctors. + + The orbit response matrix describes the change in measured beam position + produced by a change in corrector strength. This measurement tool uses + horizontal and vertical corrector arrays together with a BPM array to + perform the measurement through the pySC interface. + + After a successful measurement, the result is converted to + :class:`OrbitResponseMatrixData` and stored in ``latest_measurement``. + The stored data includes the response matrix, corrector and BPM names, + and the plane associated with each variable and observable. Parameters ---------- + name : str + Name of the measurement tool. bpm_array_name : str - BPM array name + Name of the BPM array used to measure the orbit. hcorr_array_name : str - Horizontal corrector array name + Name of the horizontal corrector array. vcorr_array_name : str - Vertical corrector array name + Name of the vertical corrector array. corrector_delta : float - Corrector delta for measurement - """ - - model_config = ConfigDict(arbitrary_types_allowed=True, extra="forbid") + Change in corrector strength applied during the measurement. + n_step : int, optional + Number of strength steps used for each corrector. The default is 1. + sleep_between_step : float, optional + Time in seconds to wait after changing a corrector strength. The + default is 0. + n_avg_meas : int, optional + Number of orbit measurements averaged at each corrector setting. The + default is 1. + sleep_between_meas : float, optional + Time in seconds to wait between orbit measurements used for averaging. + The default is 0. - bpm_array_name: str - hcorr_array_name: str - vcorr_array_name: str - corrector_delta: float + Attributes + ---------- + bpm_array_name : str + Name of the configured BPM array. + hcorr_array_name : str + Name of the configured horizontal corrector array. + vcorr_array_name : str + Name of the configured vertical corrector array. + corrector_delta : float + Corrector-strength change used for the measurement. + n_step : int + Configured number of corrector-strength steps. + sleep_between_step : float + Configured delay between corrector-strength changes. + n_avg_meas : int + Configured number of orbit measurements to average. + sleep_between_meas : float + Configured delay between averaged orbit measurements. + Methods + ------- + measure(...) + Measure orbit response matrix. + """ -class OrbitResponseMatrix(MeasurementTool): - def __init__(self, cfg: ConfigModel): - super().__init__(cfg.name) - self._cfg = cfg + def __init__( + self, + name: str, + bpm_array_name: str, + hcorr_array_name: str, + vcorr_array_name: str, + corrector_delta: float, + n_step: Optional[int] = 1, + sleep_between_step: Optional[float] = 0, + n_avg_meas: Optional[int] = 1, + sleep_between_meas: Optional[float] = 0, + ): + """ + Initialize an orbit response-matrix measurement tool. + """ + super().__init__(name) - self.bpm_array_name = cfg.bpm_array_name - self.hcorr_array_name = cfg.hcorr_array_name - self.vcorr_array_name = cfg.vcorr_array_name - self.corrector_delta = cfg.corrector_delta + self.bpm_array_name = bpm_array_name + self.hcorr_array_name = hcorr_array_name + self.vcorr_array_name = vcorr_array_name + self.corrector_delta = corrector_delta + self.n_step = n_step + self.sleep_between_step = sleep_between_step + self.n_avg_meas = n_avg_meas + self.sleep_between_meas = sleep_between_meas def measure( self, @@ -76,13 +140,16 @@ def measure( Parameters ---------- - sleep_between_step: float - Default time sleep after steerer exitation + corrector_names : list[str], optional + Correctors to excite. Defaults to every corrector of the horizontal and + vertical arrays. + sleep_between_step : float + Default time sleep after steerer excitation Default: from config n_avg_meas : int, optional Default number of orbit measurement per step used for averaging Default from config - sleep_between_meas: float + sleep_between_meas : float Default time sleep between two orbit measurment Default: from config callback : Callable, optional @@ -91,9 +158,9 @@ def measure( reading. If the callback returns false, then the process is aborted. """ - nb_meas = n_avg_meas if n_avg_meas is not None else self._cfg.n_avg_meas - sleep_step = sleep_between_step if sleep_between_step is not None else self._cfg.sleep_between_step - sleep_meas = sleep_between_meas if sleep_between_meas is not None else self._cfg.sleep_between_meas + nb_meas = n_avg_meas if n_avg_meas is not None else self.n_avg_meas + sleep_step = sleep_between_step if sleep_between_step is not None else self.sleep_between_step + sleep_meas = sleep_between_meas if sleep_between_meas is not None else self.sleep_between_meas element_holder = self._peer interface = pySCInterface( @@ -105,8 +172,8 @@ def measure( if corrector_names is None: logger.info(f"Measuring correctors from the default arrays: {self.hcorr_array_name} and {self.vcorr_array_name}.") - hcorrector_names = element_holder.get_magnets(self.hcorr_array_name).names() - vcorrector_names = element_holder.get_magnets(self.vcorr_array_name).names() + hcorrector_names = element_holder.magnets.get(self.hcorr_array_name).names() + vcorrector_names = element_holder.magnets.get(self.vcorr_array_name).names() corrector_names = hcorrector_names + vcorrector_names generator = measure_ORM( @@ -123,7 +190,7 @@ def measure( idx = 0 try: self._register_callback(callback) - self._init_measure() + self._init_measure("pyaml.tuning_tools.orbit_response_matrix_data") for code, measurement in generator: callback_data = {"idx": idx, "response_data": measurement.response_data} if code is ResponseCode.AFTER_SET: @@ -155,17 +222,36 @@ def measure( return False orm_data = self._pySC_response_data_to_ORMData(measurement.response_data.model_dump()) - self.latest_measurement.update(orm_data.model_dump()) - self.latest_measurement["type"] = "pyaml.tuning_tools.orbit_response_matrix_data" + self.latest_measurement.update(asdict(orm_data)) return True - def _pySC_response_data_to_ORMData(self, data: dict) -> OrbitResponseMatrixDataConfigModel: + def _pySC_response_data_to_ORMData(self, data: dict) -> OrbitResponseMatrixData: # all metadata is discarded here. Should we keep something? + """ + Convert pySC response data to an orbit response-matrix model. + + pySC uses ``input_names`` and ``output_names`` fields, whereas PyAML + stores actuator and observable names separately. This method performs + that conversion, infers the horizontal or vertical plane for each + actuator, and represents every BPM as one horizontal and one vertical + observable. + + Parameters + ---------- + data : dict + pySC response data containing ``matrix`` and ``input_names``. + + Returns + ------- + OrbitResponseMatrixData + PyAML response-matrix data with actuator names, BPM names, and + their associated planes. + """ element_holder = self._peer - all_hcorrector_names = element_holder.get_magnets(self.hcorr_array_name).names() - all_vcorrector_names = element_holder.get_magnets(self.vcorr_array_name).names() + all_hcorrector_names = element_holder.magnets.get(self.hcorr_array_name).names() + all_vcorrector_names = element_holder.magnets.get(self.vcorr_array_name).names() variable_planes = [] for corr in data["input_names"]: if corr in all_hcorrector_names: @@ -173,7 +259,7 @@ def _pySC_response_data_to_ORMData(self, data: dict) -> OrbitResponseMatrixDataC elif corr in all_vcorrector_names: variable_planes.append("V") - bpm_names = element_holder.get_bpms(self.bpm_array_name).names() + bpm_names = element_holder.bpms.get(self.bpm_array_name).names() # This is because we assume always dual-plane bpms now. len_b = len(bpm_names) observable_names = bpm_names * 2 @@ -188,5 +274,5 @@ def _pySC_response_data_to_ORMData(self, data: dict) -> OrbitResponseMatrixDataC "observable_planes": observable_planes, } - orm_data = OrbitResponseMatrixDataConfigModel(**orm_data_model) + orm_data = OrbitResponseMatrixData(**orm_data_model) return orm_data diff --git a/pyaml/tuning_tools/orbit_response_matrix_data.py b/pyaml/tuning_tools/orbit_response_matrix_data.py index 6baa9d10d..fad6fb76f 100644 --- a/pyaml/tuning_tools/orbit_response_matrix_data.py +++ b/pyaml/tuning_tools/orbit_response_matrix_data.py @@ -1,34 +1,49 @@ +""" +Data model for measured orbit response matrices. + +The data model stores the response matrix together with actuator and BPM names, +plane information, and optional RF response data. +""" + +from dataclasses import dataclass from typing import Optional -from .response_matrix_data import ConfigModel as ReponseMatrixDataConfigModel +from ..validation import DynamicValidation, register_schema from .response_matrix_data import ResponseMatrixData PYAMLCLASS = "OrbitResponseMatrixData" -class ConfigModel(ReponseMatrixDataConfigModel): +@register_schema +@dataclass +class OrbitResponseMatrixData(ResponseMatrixData, DynamicValidation): """ - Configuration model for orbit response matrix + Store orbit response matrix data and related metadata. + + In addition to the response matrix, variable names, and observable names + provided by :class:`ResponseMatrixData`, this class stores the RF response + and the plane associated with each variable and observable. Parameters ---------- - rf_response : list[float], optional - RF response data - variable_names : list[str], optional - Vaiable plane names, basically the plane of the actuators - observable_names : list[str], optional - Observable plane names, basically the plane of measurements + matrix : list[list[float]] + Orbit response matrix. Each row corresponds to an observable and each + column corresponds to a variable. + variable_names : list[str] or None + Names of the response-matrix variables, typically orbit correctors. + observable_names : list[str] + Names of the response-matrix observables, typically beam position + monitors. + rf_response : list[float] or None, optional + Orbit response to an RF-frequency change. + variable_planes : list[str] or None, optional + Plane associated with each response-matrix variable, typically the + plane of the corresponding actuator. + observable_planes : list[str] or None, optional + Plane associated with each response-matrix observable, typically the + plane of the corresponding measurement. """ rf_response: Optional[list[float]] = None variable_planes: Optional[list[str]] = None observable_planes: Optional[list[str]] = None - - -class OrbitResponseMatrixData(ResponseMatrixData): - """ - Orbit response matrix loader - """ - - def __init__(self, cfg: ConfigModel): - self._cfg = cfg diff --git a/pyaml/tuning_tools/response_matrix_data.py b/pyaml/tuning_tools/response_matrix_data.py index 4cfd4800e..d3310d7b8 100644 --- a/pyaml/tuning_tools/response_matrix_data.py +++ b/pyaml/tuning_tools/response_matrix_data.py @@ -1,55 +1,77 @@ -from pathlib import Path -from typing import Optional +""" +Serializable response-matrix data models. + +The :class:`ResponseMatrixData` model stores a numerical response matrix and +the names of the variables and observables represented by its columns and +rows. It is used to persist and exchange measured or calculated accelerator +response data. +""" -from pydantic import BaseModel, ConfigDict +from dataclasses import dataclass +from pathlib import Path -from pyaml.common.element import __pyaml_repr__ from pyaml.configuration.factory import Factory +from pyaml.validation import SchemaValidator from .. import PyAMLException from ..configuration.fileloader import load +from ..validation import DynamicValidation, register_schema PYAMLCLASS = "ResponseMatrixData" -class ConfigModel(BaseModel): +@register_schema +@dataclass +class ResponseMatrixData(DynamicValidation): """ - Base configuration model for response matrix + Response matrix data and its associated variable and observable names. Parameters ---------- matrix : list[list[float]] - Response matrix data (rows for observable, cols for variables) - variable_names : list[str], optional - Variable names, basically the actuators - observables_names : list[str] - Observable names, basically the measurements + Response matrix values. Each row corresponds to an observable and each + column corresponds to a variable. + variable_names : list[str] or None + Names of the variables represented by the matrix columns, typically + actuators. May be ``None`` if the names are unavailable. + observable_names : list[str] + Names of the observables represented by the matrix rows, typically + measured quantities. + + Methods + ------- + load(filename) + Load response matrix data from a configuration file. """ matrix: list[list[float]] - variable_names: Optional[list[str]] observable_names: list[str] - - -class ResponseMatrixData(object): - """ - Generic response matrix loader - """ - - def __init__(self, cfg: ConfigModel): - self._cfg = cfg + variable_names: list[str] | None = None @staticmethod def load(filename: str) -> "ResponseMatrixData": """ - Load a reponse matrix from a configuration file + Load response matrix data from a configuration file. + + Parameters + ---------- + filename : str + Path to the response matrix configuration file. + + Returns + ------- + ResponseMatrixData + Response matrix data constructed from the configuration file. + + Raises + ------ + PyAMLException + If the specified file does not exist. """ path = Path(filename) if path.exists(): config_dict = load(str(path.resolve())) - return Factory.depth_first_build(config_dict, ignore_external=False) + SchemaValidator.validate(config_dict) + return Factory.build(config_dict, ignore_external=False) else: raise PyAMLException(f"{filename}: file not found") - - def __repr__(self): - return __pyaml_repr__(self) diff --git a/pyaml/tuning_tools/tune.py b/pyaml/tuning_tools/tune.py index 382092bf5..1013f91ca 100644 --- a/pyaml/tuning_tools/tune.py +++ b/pyaml/tuning_tools/tune.py @@ -1,3 +1,11 @@ +""" +Betatron-tune measurement and correction tools. + +The :class:`Tune` tool reads horizontal and vertical betatron tune, computes +quadrupole-strength corrections from a response matrix, and applies those +corrections to the configured quadrupole array. +""" + import logging from pathlib import Path from time import sleep @@ -5,13 +13,7 @@ import numpy as np -try: - from typing import Self # Python 3.11+ -except ImportError: - from typing_extensions import Self # Python 3.10 and earlier - from .. import PyAMLException -from ..common.element import ElementConfigModel from .response_matrix_data import ResponseMatrixData from .tuning_tool import TuningTool @@ -19,62 +21,96 @@ from ..arrays.magnet_array import MagnetArray from ..diagnostics.tune_monitor import BetatronTuneMonitor +from ..validation import DynamicValidation, register_schema + logger = logging.getLogger(__name__) # Define the main class name for this module PYAMLCLASS = "Tune" -class ConfigModel(ElementConfigModel): +@register_schema +class Tune(TuningTool, DynamicValidation): """ - Configuration model for Tune + Adjust the horizontal and vertical betatron tunes. + + The tune correction is calculated from a response matrix describing the + change in horizontal and vertical tune produced by changes in quadrupole + strength. The pseudo-inverse of this matrix is used to convert a requested + tune change into the corresponding quadrupole-strength changes. + + The response matrix may be supplied directly as a + :class:`ResponseMatrixData` instance or loaded from a file. The tune is + measured using the configured betatron tune monitor, while corrections are + applied through the configured quadrupole array. Parameters ---------- + name : str + Name of the tuning tool. quad_array_name : str - Array name of quad used to adjust the tune + Name of the quadrupole array used to adjust the tune. betatron_tune_name : str - Name of the diagnostic pyaml device for measuring the tune - quad_delta : float - Delta strength used to get the response matrix - - """ - - quad_array_name: str - betatron_tune_name: str - response_matrix: str | ResponseMatrixData - - -class Tune(TuningTool): - """ - Class providing tune adjustment tool + Name of the betatron tune monitor used to measure the horizontal and + vertical tunes. + response_matrix : str or ResponseMatrixData + Tune response matrix or path to a file containing the response matrix. + The matrix is expected to have one row for each tune plane and one + column for each quadrupole. + + Attributes + ---------- + quad_array_name : str + Name of the configured quadrupole array. + betatron_tune_name : str + Name of the configured betatron tune monitor. + response_matrix : ResponseMatrixData or None + Loaded tune response matrix. + + Methods + ------- + load(load_path) + Load a tune response matrix and prepare its pseudoinverse. + get() + Return the requested horizontal and vertical tune setpoint. + readback() + Return the current horizontal and vertical betatron tune. + set(tune, iter=1, wait_time=0.0) + Iteratively correct the betatron tune to a requested setpoint. + correct(dtune) + Calculate quadrupole-strength changes for a tune change. + add(dtune, wait_time=0.0) + Apply a tune correction relative to the current setpoint. """ - def __init__(self, cfg: ConfigModel): + def __init__( + self, + name: str, + quad_array_name: str, + betatron_tune_name: str, + response_matrix: str | ResponseMatrixData, + ): """ - Construct a Tune adjustment object. - - Parameters - ---------- - cfg : ConfigModel - Configuration for the tune adjustment. + Initialize a betatron-tune correction tool. """ - super().__init__(cfg.name) - self._cfg = cfg - self._response_matrix = None + super().__init__(name) + + self.quad_array_name = quad_array_name + self.betatron_tune_name = betatron_tune_name + self._response_matrix = response_matrix self._correctionmat = None # If the configuration response matrix is a filename, load it - if type(cfg.response_matrix) is str: + if type(self._response_matrix) is str: try: - cfg.response_matrix = ResponseMatrixData.load(cfg.response_matrix) + self._response_matrix = ResponseMatrixData.load(self._response_matrix) except Exception as e: logger.warning(f"{str(e)}") - cfg.response_matrix = None + self._response_matrix = None # Invert matrix - if cfg.response_matrix: - self._response_matrix = np.array(cfg.response_matrix._cfg.matrix) + if self._response_matrix: + self._response_matrix = np.array(self._response_matrix.matrix) self._correctionmat = np.linalg.pinv(self._response_matrix) # TODO: Initialise first setpoint @@ -82,61 +118,58 @@ def __init__(self, cfg: ConfigModel): def load(self, load_path: Path): """ - Dynamically loads a response matrix. + Load a tune response matrix and prepare its pseudoinverse. Parameters ---------- load_path : Path - Filename of the :class:`~.ResponseMatrixData` to load - + Path to the serialized :class:`~.ResponseMatrixData` file. """ - self._cfg.response_matrix = ResponseMatrixData.load(load_path) - self._response_matrix = np.array(self._cfg.response_matrix._cfg.matrix) + self._response_matrix = ResponseMatrixData.load(load_path) + self._response_matrix = np.array(self._response_matrix.matrix) self._correctionmat = np.linalg.pinv(self._response_matrix) @property def response_matrix(self) -> ResponseMatrixData | None: - """ - Return the response matrix if it has been loaded None otherwise - """ - return self._cfg.response_matrix + """Return the loaded tune response matrix, if available.""" + return self._response_matrix @property def _tm(self) -> "BetatronTuneMonitor": + """Return the betatron tune monitor.""" self.check_peer() - return self.peer.get_betatron_tune_monitor(self._cfg.betatron_tune_name) + return self.peer.get_betatron_tune_monitor(self.betatron_tune_name) @property def _quads(self) -> "MagnetArray": + """Return the quadrupole array.""" self.check_peer() - return self.peer.get_magnets(self._cfg.quad_array_name) + return self.peer.magnets.get(self.quad_array_name) def get(self): - """ - Return the betatron tune setpoint - """ + """Return the requested horizontal and vertical tune setpoint.""" return self._setpoint def readback(self): - """ - Return the betatron tune measurement - """ + """Return the current horizontal and vertical betatron tune.""" self.check_peer() return self._tm.tune.get() def set(self, tune: np.array, iter: int = 1, wait_time: float = 0.0): """ - Sets the tune + Iteratively correct the betatron tune to a requested setpoint. Parameters ---------- tune : np.array - Tune setpoint - iter_nb : int - Number of iteration + Target horizontal and vertical tune values. + iter : int + Number of correction iterations. wait_time : float - Time to wait in second between 2 iterations + Delay in seconds between correction iterations. """ + if np.shape(tune) != (2,): + raise PyAMLException("Tune.add(): invalid input tune dimension, (2,) expected") for i in range(iter): diff_tune = tune - self.readback() if i == iter: @@ -146,12 +179,23 @@ def set(self, tune: np.array, iter: int = 1, wait_time: float = 0.0): def correct(self, dtune: np.array) -> np.array: """ - Return delta strengths for tune correction + Calculate quadrupole-strength changes for a tune change. Parameters ---------- dtune : np.array - Delta tune + Desired horizontal and vertical tune change. + + Returns + ------- + numpy.ndarray + Quadrupole-strength changes calculated from the response-matrix + pseudoinverse. + + Raises + ------ + PyAMLException + If no response matrix has been loaded. """ if self._correctionmat is None: raise PyAMLException("Tune.correct(): no matrix loaded or measured") @@ -159,15 +203,17 @@ def correct(self, dtune: np.array) -> np.array: def add(self, dtune: np.array, wait_time: float = 0.0): """ - Add delta tune to the tune + Apply a tune correction relative to the current setpoint. Parameters ---------- dtune : np.array - Delta tune - iter_nb: int - wait_time: float + Horizontal and vertical tune change to apply. + wait_time : float + Delay in seconds after changing quadrupole strengths. """ + if np.shape(dtune) != (2,): + raise PyAMLException("Tune.add(): invalid input dtune dimension, (2,) expected") strengths = self._quads.strengths.get() strengths += self.correct(dtune) self._quads.strengths.set(strengths) diff --git a/pyaml/tuning_tools/tune_response_matrix.py b/pyaml/tuning_tools/tune_response_matrix.py index 15f432dc0..12908e73c 100644 --- a/pyaml/tuning_tools/tune_response_matrix.py +++ b/pyaml/tuning_tools/tune_response_matrix.py @@ -1,44 +1,128 @@ +""" +Betatron-tune response-matrix measurement tools. + +The :class:`TuneResponseMatrix` measures the sensitivity of horizontal and +vertical betatron tune to quadrupole-strength changes and stores the fitted +responses in a serializable response-matrix data model. +""" + import logging +from dataclasses import asdict from time import sleep from typing import Callable, Optional import numpy as np -from pydantic import ConfigDict from ..common.constants import Action -from .measurement_tool import MeasurementTool, MeasurementToolConfigModel -from .response_matrix_data import ConfigModel as ResponseMatrixDataConfigModel +from ..validation import DynamicValidation, register_schema +from .measurement_tool import MeasurementTool +from .response_matrix_data import ResponseMatrixData logger = logging.getLogger(__name__) PYAMLCLASS = "TuneResponseMatrix" -class ConfigModel(MeasurementToolConfigModel): +@register_schema +class TuneResponseMatrix(MeasurementTool, DynamicValidation): """ - Configuration model for Tune response matrix + Measure the response of the betatron tune to quadrupole-strength changes. + + The tune response matrix describes the change in horizontal and vertical + betatron tune produced by changes in quadrupole strength. Each quadrupole + in the configured magnet array is varied over a range of strengths, and + the resulting tune values are measured and averaged. + + For measurements using more than one strength step, a linear fit is used + to determine the tune response to each quadrupole. The resulting matrix + has one row for each tune plane and one column for each quadrupole. + + After a successful measurement, the result is stored in + :attr:`MeasurementTool.latest_measurement` as a + :class:`ResponseMatrixData` representation. Parameters ---------- + name : str + Name of the measurement tool. quad_array_name : str - Array name of quad used to adjust the tune + Name of the quadrupole array used for the measurement. betatron_tune_name : str - Name of the diagnostic pyaml device for measuring the tune + Name of the betatron tune monitor used to measure the horizontal and + vertical tunes. quad_delta : float - Delta strength used to get the response matrix - """ + Maximum positive and negative quadrupole-strength change applied during + the measurement. + n_step : int, optional + Number of quadrupole-strength settings used for each quadrupole. The + settings are distributed linearly from ``-quad_delta`` to + ``quad_delta``. The default is 1. + sleep_between_step : float, optional + Time in seconds to wait after changing a quadrupole strength and before + measuring the tune. The default is 0. + n_avg_meas : int, optional + Number of tune measurements averaged at each strength setting. The + default is 1. + sleep_between_meas : float, optional + Time in seconds to wait between tune measurements used for averaging. + The default is 0. + + Attributes + ---------- + quad_array_name : str + Name of the configured quadrupole array. + betatron_tune_name : str + Name of the configured betatron tune monitor. + quad_delta : float + Configured quadrupole-strength change. + n_step : int + Configured number of strength settings. + sleep_between_step : float + Configured delay after each strength change. + n_avg_meas : int + Configured number of tune measurements to average. + sleep_between_meas : float + Configured delay between averaged tune measurements. + + Methods + ------- + measure(...) + Measure tune response matrix. - model_config = ConfigDict(arbitrary_types_allowed=True, extra="forbid") + :py:attr:`~pyaml.tuning_tools.measurement_tool.MeasurementTool.latest_measurement` contains: - quad_array_name: str - betatron_tune_name: str - quad_delta: float + Notes + ----- + The generated response matrix has shape ``(2, n_quadrupoles)``. The first + row contains the horizontal tune response and the second row contains the + vertical tune response. + Quadrupole strengths are restored after each individual scan and again when + the measurement exits because of an error or interruption. + """ -class TuneResponseMatrix(MeasurementTool): - def __init__(self, cfg: ConfigModel): - super().__init__(cfg.name) - self._cfg = cfg + def __init__( + self, + name: str, + quad_array_name: str, + betatron_tune_name: str, + quad_delta: float, + n_step: Optional[int] = 1, + sleep_between_step: Optional[float] = 0, + n_avg_meas: Optional[int] = 1, + sleep_between_meas: Optional[float] = 0, + ): + """ + Initialize a betatron-tune response-matrix measurement tool. + """ + super().__init__(name) + self.quad_array_name = quad_array_name + self.betatron_tune_name = betatron_tune_name + self.quad_delta = quad_delta + self.n_step = n_step + self.sleep_between_step = sleep_between_step + self.n_avg_meas = n_avg_meas + self.sleep_between_meas = sleep_between_meas def measure( self, @@ -51,6 +135,7 @@ def measure( ): """ Measure tune response matrix. + :py:attr:`~pyaml.tuning_tools.measurement_tool.MeasurementTool.latest_measurement` contains: .. code-block:: python @@ -82,16 +167,16 @@ def callback(action: Action, data:dict): ---------- quad_delta : float Delta strength used to get the response matrix - n_step: int, optional + n_step : int, optional Number of step for fitting the tune slope [-quad_delta/n_step..quad_delta/n_step] Default from config - sleep_between_step: float - Default time sleep after quad exitation + sleep_between_step : float + Default time sleep after quad excitation Default: from config n_avg_meas : int, optional Default number of tune measurement per step used for averaging Default from config - sleep_between_meas: float + sleep_between_meas : float Default time sleep between two tune measurment Default: from config callback : Callable, optional @@ -110,20 +195,19 @@ def callback(action: Action, data:dict): strength:float # Magnet strength tune:np.array # The measured tune (on Action.MEASURE) dtune:np.array # The tune variation (on Action.RESTORE) - """ # Get devices self.check_peer() - quads = self._peer.get_magnets(self._cfg.quad_array_name) - tm = self._peer.get_betatron_tune_monitor(self._cfg.betatron_tune_name) + quads = self._peer.magnets.get(self.quad_array_name) + tm = self._peer.get_betatron_tune_monitor(self.betatron_tune_name) tunemat = np.zeros((len(quads), 2)) initial_tune = tm.tune.get() - delta = quad_delta if quad_delta is not None else self._cfg.quad_delta - nb_step = n_step if n_step is not None else self._cfg.n_step - nb_meas = n_avg_meas if n_avg_meas is not None else self._cfg.n_avg_meas - sleep_step = sleep_between_step if sleep_between_step is not None else self._cfg.sleep_between_step - sleep_meas = sleep_between_meas if sleep_between_meas is not None else self._cfg.sleep_between_meas + delta = quad_delta if quad_delta is not None else self.quad_delta + nb_step = n_step if n_step is not None else self.n_step + nb_meas = n_avg_meas if n_avg_meas is not None else self.n_avg_meas + sleep_step = sleep_between_step if sleep_between_step is not None else self.sleep_between_step + sleep_meas = sleep_between_meas if sleep_between_meas is not None else self.sleep_between_meas self._register_callback(callback) self._init_measure("pyaml.tuning_tools.response_matrix_data") @@ -193,12 +277,12 @@ def callback(action: Action, data:dict): logger.warning(f"{self.get_name()} : measurement aborted") return False - mat = ResponseMatrixDataConfigModel( + mat = ResponseMatrixData( matrix=tunemat.T.tolist(), variable_names=quads.names(), observable_names=[tm.get_name() + ".x", tm.get_name() + ".y"], ) - self.latest_measurement.update(mat.model_dump()) + self.latest_measurement.update(asdict(mat)) self.latest_measurement["type"] = "pyaml.tuning_tools.response_matrix_data" return True diff --git a/pyaml/tuning_tools/tuning_tool.py b/pyaml/tuning_tools/tuning_tool.py index 8f043bc4a..4ad02fe5f 100644 --- a/pyaml/tuning_tools/tuning_tool.py +++ b/pyaml/tuning_tools/tuning_tool.py @@ -1,22 +1,70 @@ +""" +Base class for accelerator tuning tools. + +The classes in this module provide the common lifecycle for tools that adjust +accelerator parameters, including attachment to a simulator or control system. +""" + +import copy from typing import Self from ..common.element import Element -from ..common.element_holder import ElementHolder +from ..common.holders.element_holder import ElementHolder class TuningTool(Element): """ - Base class for tuning tool such as tune adjustment or other tuning tools. + Base class for tools that measure or adjust accelerator parameters. + + Tuning tools are configured independently and attached to an element holder + before they access accelerator devices. + + Parameters + ---------- + name : object + Name of the tuning tool. + + Methods + ------- + attach(peer) + Return a copy attached to a simulator or control system. """ def __init__(self, name): + """ + Initialize a tuning tool. + """ super().__init__(name) def attach(self, peer: "ElementHolder") -> Self: """ - Create a new reference to attach this tuning tool object to a simulator - or a control system. + Return a copy attached to a simulator or control system. + + The configured tool remains reusable. Subclasses may override + :meth:`_after_attach` to recreate handles that depend on the attached + element holder. + + Parameters + ---------- + peer : ElementHolder + Element holder providing access to accelerator devices. + + Returns + ------- + Self + Attached copy of the tuning tool. """ - obj = self.__class__(self._cfg) + if hasattr(self, "_cfg"): + obj = self.__class__(self._cfg) + else: + obj = copy.copy(self) + obj._after_attach() obj._peer = peer return obj + + def _fill_device(self, holder: "ElementHolder") -> None: + holder._fill_tool(self) + + def _after_attach(self) -> None: + """Hook for subclasses to rebind internal references after attach.""" + pass diff --git a/pyaml/validation/__init__.py b/pyaml/validation/__init__.py new file mode 100644 index 000000000..be0ca3a05 --- /dev/null +++ b/pyaml/validation/__init__.py @@ -0,0 +1,19 @@ +""" +PyAML validation subpackage. +""" + +from .configuration_models import ConfigurationSchema +from .generator import SchemaGenerator +from .registry import SchemaRegistry, register_schema +from .validation_models import DynamicValidation, StaticValidation +from .validator import SchemaValidator + +__all__ = [ + "ConfigurationSchema", + "DynamicValidation", + "SchemaRegistry", + "SchemaValidator", + "SchemaGenerator", + "StaticValidation", + "register_schema", +] diff --git a/pyaml/validation/configuration_models.py b/pyaml/validation/configuration_models.py new file mode 100644 index 000000000..d544b147b --- /dev/null +++ b/pyaml/validation/configuration_models.py @@ -0,0 +1,310 @@ +"""Datamodels for configuration.""" + +import importlib +import logging +from typing import Any, ClassVar + +from pydantic import AliasChoices, BaseModel, ConfigDict, Field, GetCoreSchemaHandler +from pydantic_core import CoreSchema, core_schema + +logger = logging.getLogger(__name__) + + +class PyAMLBaseModel(BaseModel): + """ + Base model for pyAML schemas. + + Overrides ``model_dump()`` and ``model_dump_json()`` to enable + ``serialize_as_any=True`` by default. This ensures that fields are + serialized according to their runtime type rather than their declared + annotation type. + + Methods + ------- + model_dump(**kwargs) + Serialize the model to a dictionary, using each field's runtime type. + model_dump_json(**kwargs) + Serialize the model to a JSON string, using each field's runtime type. + describe() + Return a readable description of the model fields. + """ + + def model_dump(self, **kwargs): + """Serialize the model to a dictionary, using each field's runtime type.""" + kwargs.setdefault("serialize_as_any", True) + return super().model_dump(**kwargs) + + def model_dump_json(self, **kwargs): + """Serialize the model to a JSON string, using each field's runtime type.""" + kwargs.setdefault("serialize_as_any", True) + return super().model_dump_json(**kwargs) + + @classmethod + def describe(cls) -> str: + """Return a readable description of the model fields.""" + lines = [f"{cls.__name__}("] + + for name, field in cls.model_fields.items(): + line = f" {name}: {getattr(field.annotation, '__name__', field.annotation)}" + if field.description: + line += f" — {field.description}" + lines.append(line) + + lines.append(")") + return "\n".join(lines) + + +class ConfigurationSchema(PyAMLBaseModel): + """ + Base model for configuration schemas. + + Each configuration schema defines the expected input for constructing a + specific object. The required ``class`` field specifies the fully + qualified class path of the object to construct. + + Methods + ------- + virtual_subclasses() + Return the registered virtual subclasses. + register_virtual_subclass(subclass) + Register a virtual subclass. + is_virtual_subclass_of(superclass) + Check whether this class is a subclass of another schema. + + Notes + ----- + Virtual subclasses may be registered to allow compatible schema types to + be accepted during validation. + """ + + model_config = ConfigDict(validate_by_name=True, validate_by_alias=True, arbitrary_types_allowed=False, extra="forbid") + + class_path: str = Field( + description="Fully qualified class path.", + alias="class", + ) + + # Add implementation which mimics required behaviour of virtual subclasses + # Real virtual subclasses are not compatible with Pydantic + + _virtual_subclasses: ClassVar[set[type["ConfigurationSchema"]]] + + def __init_subclass__(cls, **kwargs): + """ + Implement the __init_subclass__ protocol operation. + """ + super().__init_subclass__(**kwargs) + cls._virtual_subclasses = set() + + @classmethod + def virtual_subclasses(cls) -> set[type["ConfigurationSchema"]]: + """ + Return the registered virtual subclasses. + + Returns + ------- + set[type[ConfigurationSchema]] + A copy of the set containing all virtual subclasses registered + for this schema class. + """ + return set(cls._virtual_subclasses) + + @classmethod + def register_virtual_subclass(cls, subclass: type["ConfigurationSchema"]) -> None: + """ + Register a virtual subclass. + + Parameters + ---------- + subclass : type[ConfigurationSchema] + Subclass to register as a virtual subclass of this schema. + + Raises + ------ + TypeError + If ``subclass`` is not a ``ConfigurationSchema`` subclass. + """ + + if not isinstance(subclass, type) or not issubclass(subclass, ConfigurationSchema): + raise TypeError( + f"Cannot register {subclass!r} as a virtual subclass of {cls.__name__}: " + "it is not a ConfigurationSchema subclass." + ) + + cls._virtual_subclasses.add(subclass) + + @classmethod + def is_virtual_subclass_of(cls, superclass: type["ConfigurationSchema"]) -> bool: + """ + Check whether this class is a subclass of another schema. + + Parameters + ---------- + superclass : type[ConfigurationSchema] + Schema class to compare against. + + Returns + ------- + bool + ``True`` if ``cls`` is ``superclass`` or a registered virtual + subclass of it, otherwise ``False``. + + Raises + ------ + TypeError + If ``superclass`` is not a ``ConfigurationSchema`` subclass. + """ + + if not isinstance(superclass, type) or not issubclass(superclass, ConfigurationSchema): + raise TypeError(f"{superclass!r} is not a ConfigurationSchema.") + + checked: set[type["ConfigurationSchema"]] = set() + + def subclass_exists(current_cls: type["ConfigurationSchema"]) -> bool: + """ + Recursively check whether a registered subclass exists. + + The ``checked`` set prevents cycles while traversing the virtual + subclass hierarchy. + + Parameters + ---------- + current_cls : type[ConfigurationSchema] + Schema class whose registered subclasses are inspected. + + Returns + ------- + bool + ``True`` if ``current_cls`` has a registered subclass; + otherwise, ``False``. + """ + if current_cls in checked: + return False + checked.add(current_cls) + + if current_cls is cls: + return True + + for child in current_cls._virtual_subclasses: + if subclass_exists(child): + return True + + return False + + return subclass_exists(superclass) + + @classmethod + def __get_pydantic_core_schema__(cls, source: Any, handler: GetCoreSchemaHandler) -> CoreSchema: + """ + Customize Pydantic core schema generation. + + Parameters + ---------- + source : Any + Source type passed by Pydantic during schema generation. + handler : GetCoreSchemaHandler + Pydantic schema handler used to generate the default schema. + + Returns + ------- + CoreSchema + Wrapped core schema that accepts registered virtual subclasses. + """ + + # Get the normal schema + schema = handler(source) + + def validate(value, nxt): + # Already the expected schema type + """ + Accept schema instances and delegate other values to Pydantic. + + Instances of ``cls`` and its registered virtual subclasses are + returned unchanged. All other values are passed to the wrapped + Pydantic validator. + + Parameters + ---------- + value : object + Value being validated. + nxt : object + Wrapped Pydantic validator used for ordinary input values. + + Returns + ------- + object + The original schema instance or the value returned by + ``nxt``. + """ + if isinstance(value, cls): + return value + + # A registered virtual subclass instance should also be accepted + if isinstance(value, ConfigurationSchema) and type(value).is_virtual_subclass_of(cls): + return value + + # Otherwise let Pydantic validate normally + return nxt(value) + + return core_schema.no_info_wrap_validator_function(validate, schema) + + +class ModuleConfigurationSchema(PyAMLBaseModel): + """ + Base model for validating externally supplied configuration data. + + This schema exists to support legacy module-based configurations. It + defines the expected input for configuring a specific object, with the + target class resolved from the module's ``PYAMLCLASS`` attribute. + + Methods + ------- + to_configuration() + Convert the module-based configuration to a ``ConfigurationSchema``. + """ + + model_config = ConfigDict(validate_by_name=True, validate_by_alias=True, extra="forbid") + + MODULE_PATH_ALIASES: ClassVar[tuple[str, ...]] = ("module", "type") + + module_path: str = Field( + description="Fully qualified module path.", + validation_alias=AliasChoices(*MODULE_PATH_ALIASES), + ) + + def to_configuration(self) -> ConfigurationSchema: + """ + Convert the module-based configuration to a ``ConfigurationSchema``. + + Imports the referenced module, resolves the target class from its + ``PYAMLCLASS`` attribute, and returns an equivalent + :class:`ConfigurationSchema`. Any additional configuration fields are + preserved. + + Returns + ------- + ConfigurationSchema + Configuration schema with the resolved fully qualified class path. + + Raises + ------ + ImportError + If the referenced module cannot be imported. + ValueError + If the module does not define ``PYAMLCLASS``. + """ + + module = importlib.import_module(self.module_path) + + try: + class_name = module.PYAMLCLASS + except AttributeError as e: + raise ValueError(f"Module '{self.module_path}' does not define PYAMLCLASS.") from e + + return ConfigurationSchema.model_validate( + { + "class_path": f"{self.module_path}.{class_name}", + **(self.model_extra or {}), + }, + extra="allow", + ) diff --git a/pyaml/validation/errors.py b/pyaml/validation/errors.py new file mode 100644 index 000000000..a3ebe0124 --- /dev/null +++ b/pyaml/validation/errors.py @@ -0,0 +1,205 @@ +"""Functionality for attaching location information to validation errors.""" + +from dataclasses import dataclass +from typing import Any, NoReturn + +from pydantic import ValidationError + +from ..common.exception import PyAMLConfigException + + +@dataclass(frozen=True) +class Location: + """ + Source location within a configuration file. + + Parameters + ---------- + file : str + Name of the configuration file. + line : int + Line number where the object or field was defined. + column : int + Column number where the object or field was defined. + """ + + file: str + line: int + column: int + + def __str__(self) -> str: + """ + Return a human-readable string representation of the object. + + Returns + ------- + str + Location rendered as ``file:line:column``. + """ + return f"{self.file}: line {self.line}, column {self.column}" + + +@dataclass(frozen=True) +class LocationMetadata: + """ + Location metadata extracted from configuration data. + + Parameters + ---------- + location : Location | None + Source location of the configuration object itself. + field_locations : dict[str, Location] | None, optional + Source locations for individual configuration fields. + """ + + location: Location | None + field_locations: dict[str, Location] | None = None + + +def extract_location_metadata(data: dict[str, Any]) -> tuple[dict[str, Any], LocationMetadata]: + """ + Extract loader-added location metadata from configuration data. + + Parameters + ---------- + data : dict[str, Any] + Configuration data potentially containing loader-added metadata. + + Returns + ------- + tuple[dict[str, Any], LocationMetadata] + A copy of the configuration dictionary with the metadata removed, + together with the extracted location information. + """ + + cleaned = dict(data) + + # Get the location + raw_location = cleaned.pop("__location__", None) + location = Location(*raw_location) if raw_location is not None else None + + # Get the field locations + raw_field_locations = cleaned.pop("__fieldlocations__", None) + field_locations = ( + {field: Location(*raw_loc) for field, raw_loc in raw_field_locations.items()} + if raw_field_locations is not None + else None + ) + + return cleaned, LocationMetadata( + location=location, + field_locations=field_locations, + ) + + +def _format_value(value: Any, max_len: int = 120) -> str: + """ + Format a value for inclusion in an error message. + + Parameters + ---------- + value : Any + Value to format. + max_len : int, optional + Maximum length of the formatted representation, by default 120. + + Returns + ------- + str + Formatted value string. + """ + + text = repr(value) + return text if len(text) <= max_len else text[: max_len - 3] + "..." + + +def _format_location_path(loc: tuple[Any, ...]) -> str: + """ + Format a Pydantic error location as a human-readable path. + + Parameters + ---------- + loc : tuple[Any, ...] + Location tuple from a Pydantic validation error. + + Returns + ------- + str + Human-readable location path such as ``items[0].name``. + Returns ```` for an empty location. + """ + + parts: list[str] = [] + + for item in loc: + if isinstance(item, int): + if parts: + parts[-1] = f"{parts[-1]}[{item}]" + else: + parts.append(f"[{item}]") + else: + parts.append(str(item)) + + return ".".join(parts) if parts else "" + + +def raise_validation_error( + exc: ValidationError, + class_path: str, + location_metadata: LocationMetadata | None = None, +) -> NoReturn: + """ + Raise a configuration exception from a Pydantic validation error. + + Parameters + ---------- + exc : ValidationError + Validation error raised by Pydantic. + class_path : str + Fully qualified class path of the configuration object being validated. + location_metadata : LocationMetadata | None, optional + Source location metadata extracted from the configuration data, by + default None. + + Raises + ------ + PyAMLConfigException + Always raised with a formatted human-readable error message. + """ + + header = [f"Validation failed for class: '{class_path}'"] + + if location_metadata is not None and location_metadata.location is not None: + header.append(f"at {location_metadata.location}.") + + else: + header[-1] += "." + + error_lines: list[str] = [] + + for err in exc.errors(): + loc = tuple(err.get("loc", ())) + msg = err["msg"] + bad_value = err.get("input", None) + + path = _format_location_path(loc) + error_lines.append(f"Field '{path}' is invalid:") + error_lines.append(f" error: {msg}") + + if bad_value is not None: + error_lines.append(f" got: {_format_value(bad_value)}") + + field_name = loc[0] if loc else None + if ( + location_metadata is not None + and location_metadata.field_locations is not None + and field_name in location_metadata.field_locations + ): + error_lines.append(f" location: {location_metadata.field_locations[field_name]}") + + if header[-1].endswith("."): + message = "\n".join(header + error_lines) + else: + message = f"{header[0]} {' '.join(header[1:])} {error_lines[0]}\n" + "\n".join(error_lines[1:]) + + raise PyAMLConfigException(message) from None diff --git a/pyaml/validation/generator.py b/pyaml/validation/generator.py new file mode 100644 index 000000000..8767b65ad --- /dev/null +++ b/pyaml/validation/generator.py @@ -0,0 +1,281 @@ +"""Module for generating JSON Schema from registered configuration schemas.""" + +import json +import logging +from copy import deepcopy +from pathlib import Path +from typing import Any + +from pydantic.json_schema import GenerateJsonSchema +from pydantic_core import core_schema + +from .configuration_models import ConfigurationSchema +from .registry import SchemaRegistry + +logger = logging.getLogger(__name__) + + +METADATA_KEYS = ( + "title", + "description", + "examples", + "deprecated", + "readOnly", + "writeOnly", +) + +CLASS_ALIAS = "class" + + +class SchemaGenerator: + """ + Generate JSON Schemas for registered configuration models. + + This class provides convenience methods for generating and exporting + JSON Schemas from models registered in the ``SchemaRegistry``. Schema + generation is delegated to a custom Pydantic JSON Schema generator + that adds support for registry-aware polymorphism. + + Configuration base classes with registered subclasses are represented + as ``oneOf`` unions over their concrete implementations, allowing + generated schemas to describe all valid registered configuration types. + + Primitive unions such as ``str | None`` are emitted using compact + ``type: [...]`` representations when supported by Pydantic. + + Methods + ------- + generate(class_path) + Generate a JSON Schema for a registered configuration schema. + save(class_path, filename, *, indent=2) + Generate JSON Schema and save it to a file. + """ + + _registry = SchemaRegistry() + + @classmethod + def generate(cls, class_path: str) -> dict[str, Any]: + """ + Generate a JSON Schema for a registered configuration schema. + + The schema is generated using a custom Pydantic JSON Schema generator + that expands registered configuration subclasses into ``oneOf`` unions + and preserves compact representations for primitive unions such as + ``str | None``. + + Parameters + ---------- + class_path : str + Registry key identifying the configuration schema class. + + Returns + ------- + dict[str, Any] + Generated JSON Schema for the requested configuration schema. + + Raises + ------ + KeyError + If no schema is registered for the given class path. + """ + + schema_cls = cls._registry.get(class_path) + + logger.debug("Generating schema for %s.", schema_cls) + + if schema_cls is None: + raise KeyError(f"No schema registered for '{class_path}'") + + return schema_cls.model_json_schema( + by_alias=True, + union_format="primitive_type_array", + schema_generator=RegistryJsonSchema, + ) + + @classmethod + def save( + cls, + class_path: str, + filename: str | Path, + *, + indent: int = 2, + ) -> Path: + """ + Generate JSON Schema and save it to a file. + + Parameters + ---------- + class_path : str + Registered class path to generate schema for. + filename : str or Path + Output filename. + indent : int, optional + JSON indentation level. Default: 2. + + Returns + ------- + Path + Path to the written file. + """ + schema = cls.generate(class_path) + + path = Path(filename) + + with path.open("w", encoding="utf-8") as file: + json.dump(schema, file, indent=indent) + + return path + + +class RegistryJsonSchema(GenerateJsonSchema): + """ + Custom Pydantic JSON Schema generator for configuration schemas. + + This generator extends the default Pydantic schema generation to support + registry-aware polymorphism for ``ConfigurationSchema`` subclasses. + + For configuration base classes with registered subclasses, the generated + schema is replaced by a ``oneOf`` union over all registered concrete + subclasses. Human-facing schema metadata such as titles and descriptions + are preserved from the original schema. + + In addition, all generated schema unions are normalized to use ``oneOf`` + instead of ``anyOf`` for improved compatibility with downstream tooling. + Primitive unions such as ``str | None`` continue to use compact + ``type: [...]`` representations when supported by Pydantic. + + Methods + ------- + model_schema(schema) + Generate a JSON Schema for a Pydantic model. + """ + + _registry = SchemaRegistry() + + def model_schema(self, schema: core_schema.ModelSchema) -> dict[str, Any]: + """ + Generate a JSON Schema for a Pydantic model. + + For ``ConfigurationSchema`` subclasses, the generated schema may be + transformed into a polymorphic schema based on the registered schema + registry: + + - If the model defines a ``class`` field, all registered aliases + corresponding to the model are added as allowed literal values. + + - If registered subclasses exist, the schema is replaced by an + ``anyOf`` union containing the schemas of all registered subclasses. + + Metadata fields from the original schema, such as titles and + descriptions, are preserved in the merged schema. + + Parameters + ---------- + schema : core_schema.ModelSchema + Pydantic core schema describing the model. + + Returns + ------- + dict[str, Any] + Generated JSON Schema for the model or polymorphic union schema. + + Notes + ----- + The generated polymorphic schema uses ``anyOf`` instead of ``oneOf`` + because nested ``oneOf`` unions may lead to ambiguous validation in + downstream JSON Schema tooling when subclass schemas contain nullable + or overlapping branches. + """ + + base_schema = super().model_schema(schema) + + model_cls = schema.get("cls") + logging.debug(f"Base schema is extracted from {model_cls}.") + + if not isinstance(model_cls, type) or not issubclass(model_cls, ConfigurationSchema): + return base_schema + + # If the baseschema has a class field, add literal for all keys. + properties = base_schema.get("properties") + if isinstance(properties, dict) and CLASS_ALIAS in properties and isinstance(properties[CLASS_ALIAS], dict): + logging.debug(f"Adding list of classes to: {model_cls}.") + + # Find keys that correspond to the same schema + base_keys = sorted(key for key, schema_cls in self._registry.items() if schema_cls is model_cls) + + base_schema = deepcopy(base_schema) + properties = base_schema["properties"] + self._add_literals_to_class_path(properties[CLASS_ALIAS], base_keys) + + # Get subclasses in registry sorted by module name + subclasses = sorted( + { + schema_cls + for _, schema_cls in self._registry.items() + if ( + isinstance(schema_cls, type) + and issubclass(schema_cls, ConfigurationSchema) + and schema_cls is not model_cls + and (issubclass(schema_cls, model_cls) or schema_cls.is_virtual_subclass_of(model_cls)) + ) + }, + key=lambda cls: f"{cls.__module__}.{cls.__name__}", + ) + logging.debug(f"Subclasses found in registry: {subclasses}.") + + if not subclasses: + return base_schema + + # Generate schemas of subclasses + subschemas = [self.generate_inner(item.__pydantic_core_schema__) for item in subclasses] + + # TODO: get the schemas to work when using oneOf instead + merged: dict[str, Any] = {"oneOf": subschemas} + + for key in METADATA_KEYS: + if key in base_schema and key not in merged: + merged[key] = deepcopy(base_schema[key]) + + return merged + + @staticmethod + def _add_literals_to_class_path(schema: dict[str, Any], literals: list[str]) -> None: + """ + Add allowed literal values to a JSON Schema string field. + + The provided literals are merged with any existing ``enum`` values in + the schema while preserving insertion order and removing duplicates. + + If the resulting set contains only a single value, the schema is + simplified by replacing ``enum`` with ``const``. + + The schema is modified in place. + + Parameters + ---------- + schema : dict[str, Any] + JSON Schema fragment representing a string-like field. + literals : list[str] + Literal values to add to the schema. + + Notes + ----- + Only schemas representing string values or existing enumerations are + modified. Empty literal lists are ignored. + """ + + if not literals: + return + + # Add registry keys as literals + if schema.get("type") == "string" or "enum" in schema: + existing = schema.get("enum", []) + merged = list(dict.fromkeys([*existing, *literals])) + schema["enum"] = merged + + # If only one value exists use const + if len(merged) == 1: + schema["const"] = merged[0] + schema.pop("enum", None) + + return diff --git a/pyaml/validation/registry.py b/pyaml/validation/registry.py new file mode 100644 index 000000000..276d73e3d --- /dev/null +++ b/pyaml/validation/registry.py @@ -0,0 +1,465 @@ +"""Registry for schemas.""" + +import importlib +import logging +import pkgutil +from collections.abc import ItemsView, Iterator, KeysView, ValuesView +from importlib import metadata +from typing import Callable, Type, TypeVar, overload + +from .configuration_models import ConfigurationSchema + +logger = logging.getLogger(__name__) + +_SCHEMA_ENTRY_POINT_GROUP = "pyaml.schemas" + + +def _import_module(module_name: str) -> None: + """Import a module and recursively import its submodules. + + Parameters + ---------- + module_name : str + Fully qualified name of the module or package to import. + """ + + module = importlib.import_module(module_name) + + # Check if module is a package and then recursively import + if hasattr(module, "__path__"): + for _, submodule_name, _ in pkgutil.walk_packages( + module.__path__, + module.__name__ + ".", + ): + importlib.import_module(submodule_name) + + +class SchemaRegistry: + """ + Singleton registry for dynamically registered schemas. + + The registry is used to validate data and produce + jsonschemas for dynamic nested models. + + Methods + ------- + register(class_path, schema) + Register a schema for a class path. + discover() + Discover and register schemas. + unregister(class_path) + Unregister a schema. + clear() + Remove all registered schemas. + get(class_path) + Return the registered schema for a class path. + items() + Return a view of registered schema items. + keys() + Return a view of registered class paths. + values() + Return a view of registered schemas. + update(class_path, schema) + Replace the schema registered for a class path. + """ + + _instance: "SchemaRegistry | None" = None + _schemas: dict[str, Type[ConfigurationSchema]] + + def __new__(cls) -> "SchemaRegistry": + """ + Return the shared schema registry instance. + + The registry is a singleton: the first call creates the instance and + initializes its schema store; subsequent calls return the same object. + + Returns + ------- + SchemaRegistry + The shared schema registry. + """ + if cls._instance is None: + cls._instance = super().__new__(cls) + cls._instance._schemas = {} + return cls._instance + + # ========================================================== + # Registration + # ========================================================== + + def register( + self, + class_path: str, + schema: type[ConfigurationSchema], + ) -> None: + """ + Register a schema for a class path. + + Parameters + ---------- + class_path : str + Fully qualified class path. + schema : type[ConfigurationSchema] + Schema class used for validation. Must inherit from + :class:`ConfigurationSchema`. + + Raises + ------ + TypeError + If ``schema`` is not a subclass of + :class:`ConfigurationSchema`. + ValueError + If a different schema has already been registered for + ``class_path``. + """ + existing = self._schemas.get(class_path) + if existing is not None and existing is not schema: + raise ValueError(f"{class_path} already registered with a different schema.") + + if not isinstance(schema, type) or not issubclass(schema, ConfigurationSchema): + raise TypeError(f"{schema!r} must inherit from ConfigurationSchema.") + + self._schemas[class_path] = schema + + def discover(self) -> None: + """ + Discover and register schemas. + + This recursively imports modules in the :mod:`pyaml` package so + classes decorated with :func:`register_schema` are registered. It + also imports modules and packages advertised through the + ``pyaml.schemas`` entry-point group, allowing external packages to + register schemas. + """ + + # Discover schemas inside the pyaml core + # Import package modules so schema registration runs + + root_package = __package__.split(".")[0] + + _import_module(root_package) + + # Discover schemas from external packages + # This uses entry points + + for entry_point in metadata.entry_points(group=_SCHEMA_ENTRY_POINT_GROUP): + logger.debug("Loading schema entry point %s", entry_point) + + if entry_point.attr is not None: + raise ValueError( + f"Schema entry point {entry_point.name!r} must reference a package or module, not an attribute." + ) + + _import_module(entry_point.value) + + def unregister( + self, + class_path: str, + ) -> None: + """ + Unregister a schema. + + Parameters + ---------- + class_path : str + Fully qualified class path. + + Raises + ------ + KeyError + If no schema has been registered for ``class_path``. + """ + try: + del self._schemas[class_path] + + except KeyError: + raise KeyError(f"No schema registered for '{class_path}'") from None + + def clear(self) -> None: + """ + Remove all registered schemas. + + This clears the registry in place. + """ + self._schemas.clear() + + def __repr__( + self, + ) -> str: + """Return a string representation of the registry.""" + if not self._schemas: + return f"{self.__class__.__name__}({{}})" + + lines = [f"{self.__class__.__name__}("] + + for class_path, schema in sorted(self._schemas.items()): + lines.append(f" {class_path!r}: {schema.__module__}.{schema.__name__},") + + lines.append(")") + + return "\n".join(lines) + + # ========================================================== + # Lookup + # ========================================================== + + def __getitem__( + self, + class_path: str, + ) -> Type[ConfigurationSchema]: + """ + Return the registered schema for a class path. + + Parameters + ---------- + class_path : str + Fully qualified class path. + + Returns + ------- + Type[ConfigurationSchema] + Registered schema class. + + Raises + ------ + KeyError + If no schema has been registered for ``class_path``. + """ + + try: + return self._schemas[class_path] + + except KeyError: + raise KeyError(f"No schema registered for '{class_path}.'") from None + + def get( + self, + class_path: str, + ) -> type[ConfigurationSchema] | None: + """ + Return the registered schema for a class path. + + Parameters + ---------- + class_path : str + Fully qualified class path. + + Returns + ------- + type[ConfigurationSchema] | None + Registered schema class, or ``None`` if no schema is + registered for ``class_path``. + """ + return self._schemas.get(class_path) + + # ========================================================== + # Contents + # ========================================================== + + def __contains__( + self, + class_path: str, + ) -> bool: + """ + Return whether a schema is registered for a class path. + + Parameters + ---------- + class_path : str + Fully qualified class path. + + Returns + ------- + bool + ``True`` if a schema is registered for ``class_path``, + otherwise ``False``. + """ + return class_path in self._schemas + + def items( + self, + ) -> ItemsView[str, Type[ConfigurationSchema]]: + """ + Return a view of registered schema items. + + Returns + ------- + ItemsView[str, Type[ConfigurationSchema]] + View of registered ``(class_path, schema)`` pairs. + """ + return self._schemas.items() + + def keys( + self, + ) -> KeysView[str]: + """ + Return a view of registered class paths. + + Returns + ------- + KeysView[str] + View of registered class paths. + """ + return self._schemas.keys() + + def values( + self, + ) -> ValuesView[Type[ConfigurationSchema]]: + """ + Return a view of registered schemas. + + Returns + ------- + ValuesView[Type[ConfigurationSchema]] + View of registered schema classes. + """ + return self._schemas.values() + + def __len__( + self, + ) -> int: + """ + Return the number of registered schemas. + + Returns + ------- + int + Number of registered schemas. + """ + return len(self._schemas) + + def __iter__( + self, + ) -> Iterator[str]: + """ + Iterate over registered class paths. + + Returns + ------- + Iterator[str] + Iterator over registered class paths. + """ + return iter(self._schemas) + + # ========================================================== + # Updating + # ========================================================== + + def update( + self, + class_path: str, + schema: type[ConfigurationSchema], + ) -> None: + """ + Replace the schema registered for a class path. + + Parameters + ---------- + class_path : str + Fully qualified class path. + schema : type[ConfigurationSchema] + Schema class used for validation. Must inherit from + :class:`ConfigurationSchema`. + + Raises + ------ + TypeError + If ``schema`` is not a subclass of + :class:`ConfigurationSchema`. + KeyError + If no schema has been registered for ``class_path``. + """ + if not isinstance(schema, type) or not issubclass(schema, ConfigurationSchema): + raise TypeError(f"{schema!r} must inherit from ConfigurationSchema.") + + if class_path not in self._schemas: + raise KeyError(f"{class_path} is not registered.") + + self._schemas[class_path] = schema + + +# ========================================================== +# Decorator to register schemas +# ========================================================== + +ClassT = TypeVar("ClassT") + + +@overload +def register_schema(cls: type[ClassT]) -> type[ClassT]: ... + + +@overload +def register_schema(schema: type[ConfigurationSchema]) -> Callable[[type[ClassT]], type[ClassT]]: ... + + +@overload +def register_schema() -> Callable[[type[ClassT]], type[ClassT]]: ... + + +def register_schema(arg: type | None = None): + """ + Register a configuration schema for a class. + + This decorator supports three forms: + + - ``@register_schema``: generate and register a configuration schema + from the decorated class. + - ``@register_schema()``: equivalent to ``@register_schema``. + - ``@register_schema(MyConfigurationSchema)``: register an explicit + :class:`ConfigurationSchema` subclass for the decorated class. + + Automatically generated schemas are created using + :func:`generate_configuration_schema` and registered in the + :class:`SchemaRegistry`. + """ + + from .schema_builder import generate_configuration_schema + + registry = SchemaRegistry() + + def _generate_and_register_schema(cls: type[ClassT]) -> type[ClassT]: + """ + Generate and register a schema for a decorated class. + + Parameters + ---------- + cls : type[ClassT] + Configuration class for which a schema should be generated. + + Returns + ------- + type[ClassT] + The original class, unchanged, for use as a decorator result. + """ + generate_configuration_schema(cls) + return cls + + # Used as: @register_schema(schema) + # Explicit registration of schema + if isinstance(arg, type) and issubclass(arg, ConfigurationSchema): + schema = arg + + def decorator(cls: type[ClassT]) -> type[ClassT]: + class_path = f"{cls.__module__}.{cls.__name__}" + logger.debug("Register schema for %s.", class_path) + registry.register(class_path=class_path, schema=schema) + return cls + + return decorator + + # Used as: @register_schema() + # Registration is done when generating the schema + if arg is None: + + def decorator(cls: type[ClassT]) -> type[ClassT]: + return _generate_and_register_schema(cls) + + return decorator + + # Used as: @register_schema + # Registration is done when generating the schema + if isinstance(arg, type): + return _generate_and_register_schema(arg) + + raise TypeError("register_schema must be used as a decorator or decorator factory.") diff --git a/pyaml/validation/schema_builder.py b/pyaml/validation/schema_builder.py new file mode 100644 index 000000000..4912b2098 --- /dev/null +++ b/pyaml/validation/schema_builder.py @@ -0,0 +1,396 @@ +"""Functionality for dynamically generating configuration schemas.""" + +import inspect +import logging +import types +from abc import ABC +from datetime import date, datetime, time, timedelta +from decimal import Decimal +from enum import Enum +from functools import reduce +from pathlib import Path +from typing import Annotated, Any, Literal, Union, get_args, get_origin, get_type_hints +from uuid import UUID + +from pydantic import BaseModel, Field, create_model +from pydantic.fields import FieldInfo +from pydantic_core import PydanticUndefined + +from .configuration_models import ConfigurationSchema +from .registry import SchemaRegistry + +logger = logging.getLogger(__name__) + +RESERVED_CONFIGURATION_FIELDS = {"class_path"} + +# Types that should not be included in the registry when +# registing classes by walking a class's MRO. +EXCLUDED_TYPES: set[object] = { + object, + BaseModel, + ConfigurationSchema, + ABC, +} + +SUPPORTED_TYPES = ( + int, + str, + float, + bool, + bytes, + dict, + list, + tuple, + set, + frozenset, + type(None), + datetime, + date, + time, + timedelta, + Decimal, + Path, + UUID, +) + + +def generate_class_path(source: type) -> str: + """ + Generate the fully qualified class path for a type. + + Parameters + ---------- + source : type + Class or type object to convert into a fully qualified path. + + Returns + ------- + str + Fully qualified class path in the form ``module.name``. + """ + return f"{source.__module__}.{source.__name__}" + + +def _extract_source_bases(source: type) -> list[type]: + """ + Extract relevant base classes from a type's method resolution order. + + Parameters + ---------- + source : type + Class whose non-framework base classes should be collected. + + Returns + ------- + list[type] + List of base classes from the class hierarchy, excluding + ``object``, :class:`pydantic.BaseModel`, and + :class:`ConfigurationSchema`. + """ + bases: list[type] = [] + + for base in source.__mro__[1:]: + if base in EXCLUDED_TYPES: + continue + bases.append(base) + + return bases + + +def generate_configuration_schema(source: type) -> type[ConfigurationSchema]: + """ + Generate a configuration schema for a class or Pydantic model. + + If the source defines a ``validation_model`` attribute containing a + Pydantic model, the configuration schema is generated from that model. + Otherwise, the schema is generated from the source class constructor + signature. + + Generated schemas are registered in the :class:`SchemaRegistry` and + reused on subsequent requests. + """ + + if not isinstance(source, type): + raise TypeError("Source must be a class.") + + registry = SchemaRegistry() + class_path = generate_class_path(source) + + existing = registry.get(class_path) + if existing is not None: + return existing + + # Check if the class has a validation model + validation_model = getattr(source, "validation_model", None) + + if isinstance(validation_model, type) and issubclass(validation_model, BaseModel): + schema = _configuration_schema_from_basemodel( + validation_model, + _generate_schema_name(source), + source.__module__, + ) + else: + schema = _configuration_schema_from_constructor(source) + + logger.debug("Register schema for %s.", class_path) + registry.register(class_path, schema) + + # Keep information about the inheritance relations + bases = _extract_source_bases(source) + base_schemas: list[type[ConfigurationSchema]] = [] + + for base in bases: + base_class_path = generate_class_path(base) + base_schema = registry.get(base_class_path) + + if base_schema is None: + base_schema = generate_configuration_schema(base) + logger.debug("Generate and register schema for base class %s.", base) + + base_schemas.append(base_schema) + + # Register virtual subclass links + for base_schema in base_schemas: + logger.debug("Register virtual subclass %s under %s.", schema, base_schema) + base_schema.register_virtual_subclass(schema) + + return schema + + +def _generate_schema_name(source: type) -> str: + """ + Generate the default configuration schema name for a source class. + """ + return f"{source.__name__}ConfigurationSchema" + + +def _configuration_schema_from_basemodel( + validation_model: type[BaseModel], + schema_name: str, + module_name: str, +) -> type[ConfigurationSchema]: + """ + Generate a configuration schema from a Pydantic model. + + The resulting schema contains one field for each field defined on the + validation model, with field metadata and defaults preserved. + """ + + if not isinstance(validation_model, type) or not issubclass(validation_model, BaseModel): + raise TypeError("validation_model must be a subclass of pydantic.BaseModel.") + + fields: dict[str, Any] = {} + + for field_name, field_info in validation_model.model_fields.items(): + if field_name in RESERVED_CONFIGURATION_FIELDS: + raise ValueError( + f"{validation_model.__name__} defines reserved field {field_name!r}, which is owned by ConfigurationSchema." + ) + + fields[field_name] = _field_definition_from_field_info(field_name, field_info) + + return create_model( + schema_name, + __base__=ConfigurationSchema, + __module__=module_name, + **fields, + ) + + +def _field_definition_from_field_info(field_name: str, field_info: FieldInfo) -> tuple[Any, Any]: + """ + Convert a Pydantic field definition into a ``create_model`` field tuple. + """ + + # Get the annotation + annotation = _resolve_annotation(field_info.annotation) + + # Handle default + default = field_info.default + if default is PydanticUndefined: + default = ... + + # Handle default factory + default_factory = field_info.default_factory + + # Collect metadata + field_kwargs = _field_kwargs(field_name, field_info) + + if default_factory is not None: + return annotation, Field(default_factory=default_factory, **field_kwargs) + elif field_kwargs: + return annotation, Field(default, **field_kwargs) + else: + return annotation, default + + +def _resolve_annotation(annotation: Any) -> Any: + """ + Resolve an annotation into a schema-friendly type. + + Supported annotations are passed through directly, while supported + generic types are resolved recursively into equivalent type hints. + """ + + if annotation is inspect._empty or annotation is Any: + return Any + + if annotation is None: + return type(None) + + if isinstance(annotation, str): + raise TypeError(f"Unable to resolve annotation {annotation!r}. Forward references are not currently supported.") + + # Check if is a generic type + origin = get_origin(annotation) + + # If not a generic type + if origin is None: + if isinstance(annotation, type): + if annotation in SUPPORTED_TYPES: + return annotation + + if issubclass(annotation, Enum): + return annotation + + if issubclass(annotation, ConfigurationSchema): + return annotation + + return generate_configuration_schema(annotation) + + raise TypeError(f"Unsupported annotation: {annotation!r}") + + # If is generic type + args = get_args(annotation) + + if origin is Annotated: + return Annotated[_resolve_annotation(args[0]), *args[1:]] # type: ignore[index] + + elif origin is Literal: + return annotation + + elif origin is list: + return list[_resolve_annotation(args[0])] + + elif origin is dict: + return dict[_resolve_annotation(args[0]), _resolve_annotation(args[1])] + + elif origin is tuple: + # Handle variable length tuple + if len(args) == 2 and args[1] is Ellipsis: + return tuple[_resolve_annotation(args[0]), ...] + + resolved_args = tuple(_resolve_annotation(arg) for arg in args) + return tuple[resolved_args] + + elif origin is set: + return set[_resolve_annotation(args[0])] + + elif origin is frozenset: + return frozenset[_resolve_annotation(args[0])] + + elif origin is Union or origin is types.UnionType: + resolved_args = tuple(_resolve_annotation(arg) for arg in args) + return reduce(lambda a, b: a | b, resolved_args[1:], resolved_args[0]) + + else: + raise TypeError(f"Unsupported generic annotation: {annotation!r}") + + +def _field_kwargs(field_name: str, field_info: Any) -> dict[str, Any]: + """ + Collect supported field metadata for ``pydantic.create_model``. + """ + + kwargs: dict[str, Any] = {} + + description = getattr(field_info, "description", None) + if description is not None: + kwargs["description"] = description + + title = getattr(field_info, "title", None) + if title is not None: + kwargs["title"] = title + + examples = getattr(field_info, "examples", None) + if examples: + kwargs["examples"] = examples + + deprecated = getattr(field_info, "deprecated", None) + if deprecated is not None: + kwargs["deprecated"] = deprecated + + alias = getattr(field_info, "alias", None) + if alias and alias != field_name: + kwargs["alias"] = alias + + return kwargs + + +def _configuration_schema_from_constructor(cls: type) -> type[ConfigurationSchema]: + """ + Generate a configuration schema from a class constructor signature. + + The resulting schema contains one field for each constructor parameter, + with annotations and default values preserved. + """ + + if not isinstance(cls, type): + raise TypeError("cls must be a class.") + + fields: dict[str, Any] = _fields_from_constructor_signature( + cls, + expand_arbitrary_types=True, + ) + + return create_model( + _generate_schema_name(cls), + __base__=ConfigurationSchema, + __module__=cls.__module__, + **fields, + ) + + +def _fields_from_constructor_signature(cls: type, expand_arbitrary_types: bool = False) -> dict[str, tuple[Any, Any]]: + """ + Extract field definitions from a class constructor signature. + + Parameters + ---------- + cls + Class whose ``__init__`` method should be inspected. + expand_arbitrary_types + If true, unsupported annotations are expanded recursively into + schema-friendly types. + """ + + signature = inspect.signature(cls.__init__) + type_hints = get_type_hints(cls.__init__, include_extras=True) + + fields: dict[str, tuple[Any, Any]] = {} + + # Skip *args and **kwargs + for name, param in signature.parameters.items(): + if name == "self": + continue + + if param.kind in ( + inspect.Parameter.VAR_POSITIONAL, + inspect.Parameter.VAR_KEYWORD, + ): + continue + + if name in RESERVED_CONFIGURATION_FIELDS: + raise ValueError( + f"{cls.__name__}.__init__ defines reserved parameter {name!r}, which is owned by ConfigurationSchema." + ) + + annotation = type_hints.get(name, Any) + + if expand_arbitrary_types: + annotation = _resolve_annotation(annotation) + + default = param.default if param.default is not inspect._empty else ... + fields[name] = (annotation, default) + + return fields diff --git a/pyaml/validation/validation_models.py b/pyaml/validation/validation_models.py new file mode 100644 index 000000000..8c5d77037 --- /dev/null +++ b/pyaml/validation/validation_models.py @@ -0,0 +1,281 @@ +"""Classes for validation during object creation.""" + +import inspect +import logging +from abc import ABCMeta +from typing import Any, ClassVar, cast + +from pydantic import BaseModel, ConfigDict, ValidationError, create_model + +from .configuration_models import PyAMLBaseModel +from .errors import raise_validation_error +from .schema_builder import _fields_from_constructor_signature, generate_class_path + +logger = logging.getLogger(__name__) + + +class ValidationModel(PyAMLBaseModel): + """ + Base model for validating object constructor arguments. + + Each validation model defines the expected input for constructing a + specific object. + """ + + model_config = ConfigDict(arbitrary_types_allowed=True, extra="forbid") + + +class ValidationMeta(ABCMeta): + """ + Metaclass that validates constructor arguments before object creation. + + Classes using this metaclass must define a ``validation_model`` + attribute containing a subclass of :class:`pydantic.BaseModel`. + Whenever an instance is created, the supplied constructor arguments + are validated against the model before the class constructor is + invoked. + + Pass `validate=False` to skip validation for a single construction. + + The signature reported by :func:`inspect.signature` for classes using this + metaclass is that of their ``__init__``, not of :meth:`__call__`. The + ``validate`` keyword is therefore not part of the reported signature. + """ + + @property + def __signature__(cls) -> inspect.Signature | None: + """ + Report the constructor signature of the class. + + Without this, :func:`inspect.signature` resolves to :meth:`__call__` and + reports ``(*args, **kwargs)`` for every class using this metaclass, which + hides the real parameters from ``help()``, Sphinx and other tooling. + + Returns + ------- + inspect.Signature | None + Signature of ``cls.__init__`` without ``self``, or ``None`` if it + cannot be determined, in which case the default introspection applies. + """ + # Classes relying on ``object.__init__`` take no argument, as reported by + # ``inspect.signature`` for a class without a metaclass + if cls.__init__ is object.__init__ and cls.__new__ is object.__new__: + return inspect.Signature() + + try: + signature = inspect.signature(cls.__init__) + except (TypeError, ValueError): # pragma: no cover - defensive + return None + + # Drop ``self`` and the constructor return annotation + parameters = list(signature.parameters.values())[1:] + + return signature.replace(parameters=parameters, return_annotation=inspect.Signature.empty) + + def __call__(cls, *args: Any, **kwargs: Any): + """ + Create an instance after optionally validating constructor arguments. + + Parameters + ---------- + *args : Any + Positional constructor arguments. + **kwargs : Any + Keyword constructor arguments. + validate : bool, optional + If ``True`` (default), validate constructor arguments before + instantiation. If ``False``, skip validation and pass the + supplied arguments directly to the constructor. + + Returns + ------- + object + Instance of the class after validation and construction. + + Raises + ------ + TypeError + If the class does not define ``validation_model``. + PyAMLConfigException + If the supplied arguments do not conform to the validation + model. + """ + validate = kwargs.pop("validate", True) + + if not validate: + return super().__call__(*args, **kwargs) + + validation_model = getattr(cls, "validation_model", None) + + if validation_model is None: + raise TypeError(f"{cls.__name__} must define validation_model.") + + # Inspect the signature of the class + signature = inspect.signature(cls.__init__) + + # Map arguments to parameters + bound = signature.bind(None, *args, **kwargs) + + # Include default arguments + bound.apply_defaults() + + # Remove self from list + bound.arguments.pop("self", None) + arguments = dict(bound.arguments) + + # Validate the model + logger.debug("Validating input against schema: %s", validation_model.model_fields) + + try: + validated = validation_model.model_validate(arguments) + except ValidationError as exc: + raise_validation_error( + exc, + class_path=generate_class_path(cls), + ) + + # Return the object + return super().__call__(**validated.model_dump()) + + +class ValidationModelDescriptor: + """Provide a lazily generated validation model on the class.""" + + def __get__( + self, + instance: object | None, + owner: type["DynamicValidation"], + ) -> type[ValidationModel]: + """ + Return the validation model associated with ``owner``. + + The model is generated on first access and cached on the owning class. + Because this descriptor exposes class-level metadata, ``instance`` is + not used. + + Parameters + ---------- + instance : object | None + Instance through which the descriptor was accessed, or ``None`` + when accessed on the class. + owner : type[DynamicValidation] + Class whose validation model is requested. + + Returns + ------- + type[ValidationModel] + The cached or newly generated validation model. + """ + model = owner.__dict__.get("_validation_model") + + if model is None: + model = owner._build_validation_model() + owner._validation_model = model + + return model + + +class DynamicValidation(metaclass=ValidationMeta): + """ + Base class for automatic constructor argument validation. + + When a subclass is defined, a validation model is generated from either + its explicitly declared constructor or its directly declared class + annotations. + + Class annotations are used when no constructor has yet been defined. This + supports classes decorated with ``@dataclass``, because their generated + constructor is not available while ``__init_subclass__`` is running. + + Subclasses must not define ``validation_model`` manually. + """ + + _validation_model: ClassVar[type[ValidationModel] | None] = None + + # Lazy construction of the validation class + validation_model: ClassVar[ValidationModelDescriptor] = ValidationModelDescriptor() + + def __init_subclass__(cls, **kwargs): + """ + Generate and attach a validation model for the subclass. + + Parameters + ---------- + **kwargs : Any + Additional keyword arguments passed to ``super().__init_subclass__``. + + Raises + ------ + TypeError + If ``validation_model`` is defined manually on the subclass. + """ + + super().__init_subclass__(**kwargs) + + # Check if validation model already exists + # This only checks for the current class and not parent classes + if "validation_model" in cls.__dict__: + raise TypeError(f"{cls.__name__} may not define validation_model manually.") + + # Set the _validation_model to None since should be built using lazy construction + cls._validation_model = None + + @classmethod + def _build_validation_model(cls) -> type[ValidationModel]: + """ + Generate a validation model from the class definition. + + For classes with an explicitly defined ``__init__``, fields are + extracted from the constructor signature. Otherwise, fields are + extracted from annotations declared directly on the class. The latter + supports dataclasses before their generated constructor is available. + + Returns + ------- + type[ValidationModel] + Dynamically generated validation model representing the arguments + accepted by the class. + """ + + logger.debug("Building validation model for %s.", f"{cls.__module__}.{cls.__name__}") + + fields: dict[str, Any] = _fields_from_constructor_signature(cls, expand_arbitrary_types=False) + + model = create_model(f"{cls.__name__}ValidationModel", **cast(Any, fields), __base__=ValidationModel) + + logger.debug("Created model: %s", model.model_fields) + + return model + + +class StaticValidation(metaclass=ValidationMeta): + """ + Base class for explicit constructor argument validation. + + Subclasses must define a ``validation_model`` attribute containing a + subclass of :class:`pydantic.BaseModel`. The model is used to validate + constructor arguments before object creation. + """ + + validation_model: type[BaseModel] + + def __init_subclass__(cls, **kwargs): + """ + Verify that the subclass defines a validation model. + + Parameters + ---------- + **kwargs : Any + Additional keyword arguments passed to ``super().__init_subclass__``. + + Raises + ------ + TypeError + If the subclass does not define a ``validation_model`` + attribute. + """ + + super().__init_subclass__(**kwargs) + + if getattr(cls, "validation_model", None) is None: + raise TypeError(f"{cls.__name__} must define validation_model.") diff --git a/pyaml/validation/validator.py b/pyaml/validation/validator.py new file mode 100644 index 000000000..3de8b4a92 --- /dev/null +++ b/pyaml/validation/validator.py @@ -0,0 +1,232 @@ +"""Module for schema validation.""" + +import logging +import warnings +from collections.abc import Mapping +from typing import Any + +from pydantic import BaseModel, ValidationError + +from .configuration_models import ConfigurationSchema, ModuleConfigurationSchema +from .errors import extract_location_metadata, raise_validation_error +from .registry import SchemaRegistry + +logger = logging.getLogger(__name__) + + +def dump_nested(value: Any) -> Any: + """ + Recursively convert nested Pydantic models to plain Python objects. + + Traverses mappings, lists, and tuples, replacing any + :class:`pydantic.BaseModel` instances with the result of + :meth:`BaseModel.model_dump`. All other values are returned unchanged. + + Parameters + ---------- + value : Any + The object to convert. + + Returns + ------- + Any + The converted object with all nested Pydantic models represented as + dictionaries. + """ + + if isinstance(value, BaseModel): + return value.model_dump() + if isinstance(value, Mapping): + return {k: dump_nested(v) for k, v in value.items()} + if isinstance(value, list): + return [dump_nested(v) for v in value] + if isinstance(value, tuple): + return tuple(dump_nested(v) for v in value) + return value + + +class SchemaValidator: + """ + Recursive validator for configuration dictionaries. + + The validator traverses nested configuration data structures and + converts dictionaries representing configuration objects into + validated Pydantic schema models. + + Validation is performed recursively: + + - Lists are traversed element-by-element + - Dictionaries are recursively validated + - Dictionaries matching configuration schemas are converted into + validated schema models + - Dictionaries with unknown schemas are left unchanged + + Schema lookup is performed through the :class:`SchemaRegistry`. + + Methods + ------- + validate(data) + Validate configuration data recursively. + validate_to_dict(data) + Validate configuration data recursively and return it as a dictionary. + """ + + _registry = SchemaRegistry() + + @classmethod + def validate( + cls, + data: dict[str, Any], + ) -> ConfigurationSchema: + """ + Validate configuration data recursively. + + Parameters + ---------- + data : dict[str, Any] + Configuration dictionary to validate. + + Returns + ------- + ConfigurationSchema + Fully validated top-level configuration model. + + Raises + ------ + TypeError + If the validated top-level object is not a + :class:`ConfigurationSchema`. + """ + validated = cls._recursive_validate(data) + + # if not isinstance(validated, ConfigurationSchema): + # raise TypeError("Top-level configuration did not validate to a ConfigurationSchema.") + + return validated + + @classmethod + def validate_to_dict( + cls, + data: dict[str, Any], + ) -> dict: + """ + Validate configuration data recursively and return it as a dictionary. + """ + + validated = cls.validate(data) + return dump_nested(validated) + + @classmethod + def _recursive_validate(cls, obj: Any) -> Any: + """ + Recursively validate nested configuration objects. + + Lists are traversed recursively element-by-element. Dictionaries + are recursively traversed and then interpreted as configuration + objects when possible. + + If a dictionary corresponds to a registered configuration schema, + it is converted into a validated schema model. Otherwise, the + dictionary is returned unchanged. + + Parameters + ---------- + obj : Any + Object to validate recursively. + + Returns + ------- + Any + Validated object. This may be: + + - A validated configuration model + - A recursively validated list + - A recursively validated dictionary + - The original object if no validation applies + """ + if isinstance(obj, list): + return [cls._recursive_validate(item) for item in obj] + + if not isinstance(obj, dict): + return obj + + # Remove loader metadata and keep it for error reporting. + cleaned_dict, location_metadata = extract_location_metadata(obj) + + logger.debug("Validating dict with keys: %s", list(obj)) + validated_dict = {key: cls._recursive_validate(value) for key, value in cleaned_dict.items()} + + # Check if the dict is a configuration object + # If it follows the old convention for configuration + # translate the data to the new one + parsed = cls._parse_configuration(validated_dict) + + if parsed is None: + return validated_dict + else: + validated_dict = parsed + + class_path = validated_dict["class_path"] + schema = cls._registry.get(class_path) + + if schema is None: + warnings.warn( + f"Unknown schema for '{class_path}' so cannot validate. Leaving data as raw dict.", + stacklevel=2, + ) + return validated_dict + + try: + return schema.model_validate(validated_dict) + except ValidationError as exc: + raise_validation_error( + exc, + class_path=class_path, + location_metadata=location_metadata, + ) + + @classmethod + def _parse_configuration( + cls, + validated_dict: dict[str, Any], + ) -> dict[str, Any] | None: + """ + Interpret a dictionary as configuration metadata. + + Returns the dictionary unchanged if it already matches + :class:`ConfigurationSchema`. If it matches + :class:`ModuleConfigurationSchema`, the legacy module-based format is + rewritten into the modern ``class_path`` form. Otherwise returns + ``None``. + """ + + try: + ConfigurationSchema.model_validate(validated_dict, extra="allow") + # ``class`` is accepted as a validation alias for ``class_path`` + # by ConfigurationSchema, but schema lookup below requires the + # canonical key to be present in the dictionary itself. + if "class_path" not in validated_dict and "class" in validated_dict: + validated_dict = dict(validated_dict) + validated_dict["class_path"] = validated_dict.pop("class") + return validated_dict + except ValidationError: + logger.debug("Could not validate against ConfigurationSchema.") + + try: + module_config = ModuleConfigurationSchema.model_validate( + validated_dict, + extra="allow", + ) + except ValidationError: + logger.debug("Could not validate against ModuleConfigurationSchema; returning raw dict.") + return None + + class_config = module_config.to_configuration() + + rewritten = dict(validated_dict) + rewritten["class_path"] = class_config.class_path + rewritten.pop("type", None) + rewritten.pop("module", None) + + logger.debug("Configuration transformed from legacy configuration format.") + return rewritten diff --git a/pyaml/yellow_pages.py b/pyaml/yellow_pages.py index cc8793aaa..1a03c666a 100644 --- a/pyaml/yellow_pages.py +++ b/pyaml/yellow_pages.py @@ -1,5 +1,5 @@ """ -yellow_pages.py +Dynamic discovery service for accelerator objects. Fully dynamic YellowPages service attached to :class:`~pyaml.accelerator.Accelerator`. @@ -14,7 +14,7 @@ yp["re:^SH1A-C0[12]-H$"] :class:`~pyaml.accelerator.Accelerator` interface ------------------------------- +-------------------------------------------------- - controls() -> dict[str, ElementHolder] - simulators() -> dict[str, ElementHolder] - modes() -> dict[str, ElementHolder] @@ -32,6 +32,19 @@ class YellowPagesCategory(str, Enum): + """ + Kind of object a YellowPages entry refers to. + + Attributes + ---------- + ARRAYS : str + Named element families declared in the ``arrays`` configuration section. + TOOLS : str + Tuning and measurement tools attached to a mode. + DIAGNOSTICS : str + Monitors such as betatron tune and chromaticity monitors. + """ + ARRAYS = "Arrays" TOOLS = "Tools" DIAGNOSTICS = "Diagnostics" @@ -60,6 +73,24 @@ class YellowPages: :class:`~pyaml.element_holder.ElementHolder` instances associated with the :class:`~pyaml.accelerator.Accelerator` control and simulation modes. + Parameters + ---------- + accelerator : 'Accelerator' + Accelerator whose modes are scanned on every query. + + Methods + ------- + has(key) + Check whether a YellowPages key exists. + categories() + Return the list of available categories. + keys(category=None) + Return available YellowPages keys. + availability(key) + Return the set of modes where a key is available. + get(query, mode=None) + Search identifiers using a wildcard or regular expression. + Notes ----- The :class:`~pyaml.accelerator.Accelerator` must provide: @@ -103,6 +134,9 @@ class YellowPages: """ def __init__(self, accelerator: "Accelerator"): + """ + Initialize the YellowPages. + """ self._acc = accelerator def has(self, key: str) -> bool: @@ -131,7 +165,6 @@ def has(self, key: str) -> bool: >>> sr.yellow_pages.has("UNKNOWN") False - """ return key in self._all_keys() @@ -152,7 +185,6 @@ def categories(self) -> list[str]: >>> sr.yellow_pages.categories() ['Arrays', 'Tools', 'Diagnostics'] - """ discovered = self._discover() present = {cat for cat, keys in discovered.items() if keys} @@ -191,7 +223,6 @@ def keys(self, category: str | YellowPagesCategory | None = None) -> list[str]: .. code-block:: python >>> sr.yellow_pages.keys(YellowPagesCategory.ARRAYS) - """ discovered = self._discover() @@ -299,7 +330,6 @@ def _get_object(self, key: str, *, mode: str | None = None): .. code-block:: python >>> sr.yellow_pages.BPM - """ self._require_key(key) @@ -350,7 +380,6 @@ def get(self, query: str, mode: str | None = None) -> list[str]: >>> sr.yellow_pages.get("OH4*", mode="live") >>> sr.yellow_pages.get("re:^SH1A-C0[12]-H$") - """ if not query or not query.strip(): raise YellowPagesQueryError("Empty YellowPages query.") @@ -471,9 +500,18 @@ def __repr__(self) -> str: return "\n".join(lines).rstrip() def __str__(self) -> str: + """ + Return a human-readable string representation of the object. + + Returns + ------- + str + Table of the discovered categories and their keys. + """ return self.__repr__() def _discover(self) -> dict[YellowPagesCategory, list[str]]: + """Scan every mode and group the objects it exposes by category.""" arrays: list[str] = [] tools: list[str] = [] diags: list[str] = [] @@ -507,6 +545,7 @@ def _extend_unique(self, target: list[str], values: list[str]) -> None: target.append(value) def _all_keys(self) -> list[str]: + """Return every discovered key, across all categories.""" discovered = self._discover() out: list[str] = [] for keys in discovered.values(): @@ -514,10 +553,36 @@ def _all_keys(self) -> list[str]: return out def _require_key(self, key: str) -> None: + """ + Raise if a key is not present in any discovered category. + + Parameters + ---------- + key : str + Key to check. + + Returns + ------- + None + Nothing; raises ``KeyError`` if the key is unknown. + """ if key not in self._all_keys(): raise KeyError(self._unknown_key_message(key)) def _unknown_key_message(self, key: str) -> str: + """ + Build the error message listing the available keys. + + Parameters + ---------- + key : str + Key that could not be resolved. + + Returns + ------- + str + Error message naming the available keys. + """ available = ", ".join(self._all_keys()) return f"Unknown YellowPages key '{key}'. Available keys: {available if available else ''}" @@ -641,6 +706,19 @@ def _object_to_ids(self, obj: Any) -> list[str]: return [str(obj)] def _ids_for_key_union_all_modes(self, key: str) -> list[str]: + """ + Collect the identifiers behind a key across every mode, without duplicates. + + Parameters + ---------- + key : str + Key to resolve in every mode. + + Returns + ------- + list[str] + Element identifiers, in discovery order and without duplicates. + """ out: list[str] = [] resolved = self._get_object(key) for obj in resolved.values(): @@ -660,6 +738,19 @@ def _all_known_ids(self) -> list[str]: return all_ids def _ids_from_holder(self, holder) -> list[str]: + """ + Collect the identifiers of every array exposed by a holder. + + Parameters + ---------- + holder : object + Control system or simulator to scan. + + Returns + ------- + list[str] + Element identifiers of every array the holder exposes. + """ ids: list[str] = [] try: diff --git a/pyproject.toml b/pyproject.toml index 470b48047..7f3e2f6a9 100644 --- a/pyproject.toml +++ b/pyproject.toml @@ -28,7 +28,7 @@ dependencies = [ "accelerator-toolbox>=0.6.1", "PyYAML>=6.0.2", "pydantic>=2.11.7", - "accelerator-commissioning==1.1.0", #pySC + "accelerator-commissioning==1.5.3", #pySC "h5py", "matplotlib" ] @@ -50,6 +50,7 @@ cs-oa-tango = [ test = [ "pytest>=7.4", "pytest-cov>=3.0", + "pyaml-test-lattice @ git+https://github.com/python-accelerator-middle-layer/pyaml-test-lattice.git@main", ] doc = [ "sphinx ~= 8.1", @@ -126,3 +127,8 @@ skip-magic-trailing-comma = false python_version = "3.11" strict = false ignore_missing_imports = true + +[tool.pytest.ini_options] +markers = [ + "integration: tests requiring an external integration runtime", +] diff --git a/tests/arrays/test_array_selection_types.py b/tests/arrays/test_array_selection_types.py new file mode 100644 index 000000000..d5cc782bf --- /dev/null +++ b/tests/arrays/test_array_selection_types.py @@ -0,0 +1,62 @@ +import pytest + +from pyaml.arrays.element_array import ElementArray +from pyaml.arrays.magnet_array import MagnetArray + + +@pytest.fixture +def design(accelerator_from_fragments, sr_configuration_fragments): + sr = accelerator_from_fragments(*sr_configuration_fragments) + return sr.design + + +def test_slices_keep_the_common_magnet_type(design): + magnets = design.magnets.get() + assert len({type(magnet) for magnet in magnets}) > 1 + + assert type(magnets[:]) is MagnetArray + assert type(magnets[::-1]) is MagnetArray + assert magnets[:].names() == magnets.names() + assert magnets[::-1].names() == list(reversed(magnets.names())) + assert magnets[:][0] is magnets[0] + assert magnets[:].get_peer() is design + + +def test_filters_keep_the_common_magnet_type(design): + magnets = design.magnets.get() + expected = ["SH1A-C01-H", "SH1A-C01-V", "SH1A-C01-SQ"] + + selected = magnets["SH1A-C01*"] + by_model = magnets["model_name:SH1A-C01"] + + assert len({type(magnet) for magnet in selected}) > 1 + assert type(selected) is MagnetArray + assert type(by_model) is MagnetArray + assert selected.names() == expected + assert by_model.names() == expected + + +def test_magnet_holder_selection_uses_the_same_typing(design): + assert type(design.magnets[:]) is MagnetArray + assert type(design.magnets["SH*"]) is MagnetArray + assert design.magnets[:].names() == design.magnets.get().names() + + +def test_mixed_array_stays_generic_until_only_magnets_are_selected(design): + mixed = design.get_elements("ElArray") + + assert type(mixed[:]) is ElementArray + assert mixed[:].names() == mixed.names() + assert type(mixed["SH*"]) is MagnetArray + assert mixed["SH*"].names() == ["SH1A-C01-V", "SH1A-C02-H"] + + +def test_empty_selections_and_integer_indexing_keep_their_behavior(design): + magnets = design.magnets.get() + + assert type(magnets[0:0]) is ElementArray + assert magnets[0:0] == [] + assert type(magnets["UNKNOWN*"]) is ElementArray + assert magnets["UNKNOWN*"] == [] + assert magnets[0] is design.magnet.get(magnets.names()[0]) + assert type(magnets - magnets) is list diff --git a/tests/test_arrays.py b/tests/arrays/test_arrays.py similarity index 70% rename from tests/test_arrays.py rename to tests/arrays/test_arrays.py index 526d4ab5b..7ae9b8710 100644 --- a/tests/test_arrays.py +++ b/tests/arrays/test_arrays.py @@ -5,12 +5,9 @@ from pyaml.accelerator import Accelerator from pyaml.arrays.bpm import BPM -from pyaml.arrays.bpm import ConfigModel as BPMArrayConfigModel from pyaml.arrays.bpm_array import BPMArray from pyaml.arrays.cfm_magnet import CombinedFunctionMagnet -from pyaml.arrays.cfm_magnet import ConfigModel as CombinedFunctionMagnetConfigModel from pyaml.arrays.element_array import ElementArray -from pyaml.arrays.magnet import ConfigModel as MagnetArrayConfigModel from pyaml.arrays.magnet import Magnet from pyaml.arrays.magnet_array import MagnetArray @@ -26,8 +23,8 @@ def test_arrays(install_test_package): # Test on model - sr.design.get_magnet("SH1A-C01-H").strength.set(0.000010) - sr.design.get_magnet("SH1A-C01-V").strength.set(0.000015) + sr.design.magnet.get("SH1A-C01-H").strength.set(0.000010) + sr.design.magnet.get("SH1A-C01-V").strength.set(0.000015) o, _ = sr.design.get_lattice().find_orbit() assert np.abs(o[0] - 9.90267693e-05) < 1e-10 @@ -35,8 +32,8 @@ def test_arrays(install_test_package): assert np.abs(o[2] + 1.59928207e-06) < 1e-10 assert np.abs(o[3] + 1.74771216e-05) < 1e-10 - sr.design.get_magnet("SH1A-C02-H").strength.set(-0.000008) - sr.design.get_magnet("SH1A-C02-V").strength.set(-0.000017) + sr.design.magnet.get("SH1A-C02-H").strength.set(-0.000008) + sr.design.magnet.get("SH1A-C02-V").strength.set(-0.000017) o, _ = sr.design.get_lattice().find_orbit() assert np.abs(o[0] - 1.60555804e-04) < 1e-10 @@ -44,8 +41,8 @@ def test_arrays(install_test_package): assert np.abs(o[2] - 3.62695844e-05) < 1e-10 assert np.abs(o[3] + 5.97692290e-06) < 1e-10 - sr.design.get_magnets("HCORR").strengths.set([0.000010, -0.000008]) - sr.design.get_magnets("VCORR").strengths.set([0.000015, -0.000017]) + sr.design.magnets.get("HCORR").strengths.set([0.000010, -0.000008]) + sr.design.magnets.get("VCORR").strengths.set([0.000015, -0.000017]) o, _ = sr.design.get_lattice().find_orbit() assert np.abs(o[0] - 1.60555804e-04) < 1e-10 @@ -56,7 +53,7 @@ def test_arrays(install_test_package): p0 = o[0] # Test kick angle (small angle, no change from above) - sr.design.get_magnet("SH1A-C02-H").angle.set(-0.000008) + sr.design.magnet.get("SH1A-C02-H").angle.set(-0.000008) o, _ = sr.design.get_lattice().find_orbit() assert np.abs(o[0] - 1.60555804e-04) < 1e-10 assert np.abs(o[1] + 2.37234366e-06) < 1e-10 @@ -70,22 +67,22 @@ def test_arrays(install_test_package): # Test on control system # Assert that the virtual magnet share the same model - assert sr.live.get_magnet("SH1A-C01-H").model == sr.live.get_magnet("SH1A-C01-V").model - assert sr.live.get_magnet("SH1A-C02-H").model == sr.live.get_magnet("SH1A-C02-V").model + assert sr.live.magnet.get("SH1A-C01-H").model == sr.live.magnet.get("SH1A-C01-V").model + assert sr.live.magnet.get("SH1A-C02-H").model == sr.live.magnet.get("SH1A-C02-V").model # Using aggregators - sr.live.get_magnets("HCORR").strengths.set([0.000010, -0.000008]) - ps1 = sr.live.get_cfm_magnet("SH1A-C01").hardwares.get() - ps2 = sr.live.get_cfm_magnet("SH1A-C02").hardwares.get() + sr.live.magnets.get("HCORR").strengths.set([0.000010, -0.000008]) + ps1 = sr.live.combined_function_magnet.get("SH1A-C01").hardwares.get() + ps2 = sr.live.combined_function_magnet.get("SH1A-C02").hardwares.get() assert np.abs(ps1[0] - 0.02956737880874648) < 1e-10 assert np.abs(ps1[1] - 0) < 1e-10 assert np.abs(ps1[2] - 0) < 1e-10 assert np.abs(ps2[0] + 0.02365390304699716) < 1e-10 assert np.abs(ps2[1] - 0) < 1e-10 assert np.abs(ps2[2] - 0) < 1e-10 - sr.live.get_magnets("VCORR").strengths.set([0.000015, -0.000017]) - ps1 = sr.live.get_cfm_magnet("SH1A-C01").hardwares.get() - ps2 = sr.live.get_cfm_magnet("SH1A-C02").hardwares.get() + sr.live.magnets.get("VCORR").strengths.set([0.000015, -0.000017]) + ps1 = sr.live.combined_function_magnet.get("SH1A-C01").hardwares.get() + ps2 = sr.live.combined_function_magnet.get("SH1A-C02").hardwares.get() assert np.abs(ps1[0] - 0.02956737880874648) < 1e-10 assert np.abs(ps1[1] + 0.058240333933172066) < 1e-10 assert np.abs(ps1[2] - 0.05601656539392866) < 1e-10 @@ -93,7 +90,7 @@ def test_arrays(install_test_package): assert np.abs(ps2[1] - 0.06600571179092833) < 1e-10 assert np.abs(ps2[2] + 0.0634854407797858) < 1e-10 - strHV = sr.live.get_magnets("HVCORR").strengths.get() + strHV = sr.live.magnets.get("HVCORR").strengths.get() assert np.abs(strHV[0] - 0.000010) < 1e-10 assert np.abs(strHV[1] + 0.000008) < 1e-10 assert np.abs(strHV[2] - 0.000015) < 1e-10 @@ -102,10 +99,10 @@ def test_arrays(install_test_package): # Reset to 0 ma = importlib.import_module("tango.pyaml.multi_attribute") ma.LAST_NB_WRITTEN = 0 # Total number of setpoints done by multi_attribute - sr.live.get_magnets("HVCORR").strengths.set(0.0) + sr.live.magnets.get("HVCORR").strengths.set(0.0) assert ma.LAST_NB_WRITTEN == 6 # 6 power supply setpoints are needed - ps1 = sr.live.get_cfm_magnet("SH1A-C01").hardwares.get() - ps2 = sr.live.get_cfm_magnet("SH1A-C02").hardwares.get() + ps1 = sr.live.combined_function_magnet.get("SH1A-C01").hardwares.get() + ps2 = sr.live.combined_function_magnet.get("SH1A-C02").hardwares.get() assert np.abs(ps1[0]) < 1e-10 assert np.abs(ps1[1]) < 1e-10 assert np.abs(ps1[2]) < 1e-10 @@ -115,12 +112,12 @@ def test_arrays(install_test_package): # Check that the behavior is the same without aggregator mags = [] - for m in sr.live.get_magnets("HVCORR"): + for m in sr.live.magnets.get("HVCORR"): mags.append(m) array = MagnetArray("HVCOOR_noagg", mags, use_aggregator=False) array.strengths.set([0.000010, -0.000008, 0.000015, -0.000017]) - ps1 = sr.live.get_cfm_magnet("SH1A-C01").hardwares.get() - ps2 = sr.live.get_cfm_magnet("SH1A-C02").hardwares.get() + ps1 = sr.live.combined_function_magnet.get("SH1A-C01").hardwares.get() + ps2 = sr.live.combined_function_magnet.get("SH1A-C02").hardwares.get() assert np.abs(ps1[0] - 0.02956737880874648) < 1e-10 assert np.abs(ps1[1] + 0.058240333933172066) < 1e-10 assert np.abs(ps1[2] - 0.05601656539392866) < 1e-10 @@ -131,21 +128,32 @@ def test_arrays(install_test_package): # Test BPMs array # Using aggregator - pos = sr.design.get_bpms("BPMS").positions.get() + pos = sr.design.bpms.get("BPMS").positions.get() assert np.abs(pos[0][0] - 7.22262850488348e-05) < 1e-10 assert np.abs(pos[0][1] - 3.4291613955705856e-05) < 1e-10 assert np.abs(pos[1][0] + 1.1696152238807462e-04) < 1e-10 assert np.abs(pos[1][1] - 7.4265634524358045e-06) < 1e-10 # Using aggregator (h and v) - pos_h = sr.design.get_bpms("BPMS").h.get() - pos_v = sr.design.get_bpms("BPMS").v.get() + pos_h = sr.design.bpms.get("BPMS").h.get() + pos_v = sr.design.bpms.get("BPMS").v.get() assert np.all(np.isclose(pos[:, 0], pos_h, rtol=1e-15, atol=1e-15)) assert np.all(np.isclose(pos[:, 1], pos_v, rtol=1e-15, atol=1e-15)) + # Test BPM transformation matrices + sr.design.bpm.get("BPM_C04-01").offset.set([0.1, 0.2]) + sr.design.bpm.get("BPM_C04-02").offset.set([0.3, 0.4]) + pos = sr.design.bpms.get("BPMS").positions.get() + assert np.abs(pos[0][0] - 7.22262850488348e-05 - 0.1) < 1e-10 + assert np.abs(pos[0][1] - 3.4291613955705856e-05 - 0.2) < 1e-10 + assert np.abs(pos[1][0] + 1.1696152238807462e-04 - 0.3) < 1e-10 + assert np.abs(pos[1][1] - 7.4265634524358045e-06 - 0.4) < 1e-10 + sr.design.bpm.get("BPM_C04-01").offset.set([0.0, 0.0]) + sr.design.bpm.get("BPM_C04-02").offset.set([0.0, 0.0]) + # No aggregator bpms = [] - for b in sr.design.get_bpms("BPMS"): + for b in sr.design.bpms.get("BPMS"): bpms.append(b) bpms = BPMArray("BPM_noagg", bpms, use_aggregator=False) @@ -163,14 +171,14 @@ def test_arrays(install_test_package): assert len(allElts) == 11 # Create an array that contains all elements - allMags = MagnetArray("AllMagnets", sr.design.get_all_magnets()) + allMags = MagnetArray("AllMagnets", sr.design.magnets.get()) assert len(allMags) == 7 # Create an array that contains all BPM - allBpms = BPMArray("AllBPMs", sr.design.get_all_bpms()) + allBpms = BPMArray("AllBPMs", sr.design.bpm.all()) assert len(allBpms) == 2 - cfm = sr.design.get_cfm_magnets("CFM") + cfm = sr.design.combined_function_magnets.get("CFM") strHVSQ = cfm.strengths.get() assert np.abs(strHVSQ[0] - 0.000010) < 1e-10 # H assert np.abs(strHVSQ[1] - 0.000015) < 1e-10 # V @@ -196,14 +204,14 @@ def test_arrays(install_test_package): assert np.abs(strHVSQ[4] + 0.000017) < 1e-10 # V assert np.abs(strHVSQ[5] - 1e-6) < 1e-10 # SQ - bpmsLive = BPMArray("", sr.live.get_all_bpms()) + bpmsLive = BPMArray("", sr.live.bpm.all()) bpmsLive.positions.get() # Test dynamic arrays - sr: Accelerator = Accelerator.load("tests/config/EBSOrbit.yaml", use_fast_loader=True) + sr: Accelerator = Accelerator.load("tests/config/EBSOrbit.yaml", include_locations=False) ae = ElementArray("All", sr.design.get_all_elements()) - acfm = ElementArray("AllCFM", sr.design.get_all_cfm_magnets(), use_aggregator=False) + acfm = ElementArray("AllCFM", sr.design.combined_function_magnet.all(), use_aggregator=False) bpmC5 = ae["BPM*"][10:20] # All BPM C5 assert isinstance(bpmC5, BPMArray) and len(bpmC5) == 10 @@ -217,19 +225,19 @@ def test_arrays(install_test_package): assert isinstance(magSH1AC, ElementArray) and len(magSH1AC) == 32 # Empty arrays - emptyMag = Magnet(MagnetArrayConfigModel(name="EmptyMag", elements=[])) + emptyMag = Magnet(name="EmptyMag", elements=[]) emptyMag.fill_array(sr.design) # Attach the array - v = sr.design.get_magnets("EmptyMag").strengths.get() # Ensure good attach + v = sr.design.magnets.get("EmptyMag").strengths.get() # Ensure good attach assert np.shape(v) == (0,) - emptyBPM = BPM(BPMArrayConfigModel(name="emptyBPM", elements=[])) + emptyBPM = BPM(name="emptyBPM", elements=[]) emptyBPM.fill_array(sr.design) # Attach the array - v = sr.design.get_bpms("emptyBPM").positions.get() # Ensure good attach + v = sr.design.bpms.get("emptyBPM").positions.get() # Ensure good attach assert np.shape(v) == (0,) - emptyCFM = CombinedFunctionMagnet(CombinedFunctionMagnetConfigModel(name="emptyCFM", elements=[])) + emptyCFM = CombinedFunctionMagnet(name="emptyCFM", elements=[]) emptyCFM.fill_array(sr.design) # Attach the array - v = sr.design.get_cfm_magnets("emptyCFM").strengths.get() # Ensure good attach + v = sr.design.combined_function_magnets.get("emptyCFM").strengths.get() # Ensure good attach assert np.shape(v) == (0,) @@ -240,8 +248,8 @@ def test_arrays(install_test_package): ], ) def test_serialized_magnets_arrays(sr_file): - sr: Accelerator = Accelerator.load(sr_file, use_fast_loader=True, ignore_external=True) - the_serie = sr.design.get_serialized_magnets("series") + sr: Accelerator = Accelerator.load(sr_file, include_locations=False, ignore_external=True) + the_serie = sr.design.serialized_magnets.get("series") strength = the_serie.strengths.get() assert len(strength) == 1 print(strength) diff --git a/tests/test_arrays_ops.py b/tests/arrays/test_arrays_ops.py similarity index 96% rename from tests/test_arrays_ops.py rename to tests/arrays/test_arrays_ops.py index 7027c761a..5fd706e2c 100644 --- a/tests/test_arrays_ops.py +++ b/tests/arrays/test_arrays_ops.py @@ -18,8 +18,8 @@ def test_element_array_and_array_intersection_is_autotyped( sr = accelerator_from_fragments(*sr_configuration_fragments) sr.design.get_lattice().disable_6d() - hcorr = sr.live.get_magnets("HCORR") - hvcorr = sr.live.get_magnets("HVCORR") + hcorr = sr.live.magnets.get("HCORR") + hvcorr = sr.live.magnets.get("HVCORR") inter = hvcorr & hcorr @@ -203,8 +203,8 @@ def test_element_array_or_union_is_unique_stable_and_autotyped( sr = accelerator_from_fragments(*sr_configuration_fragments) sr.design.get_lattice().disable_6d() - hcorr = sr.live.get_magnets("HCORR") - vcorr = sr.live.get_magnets("VCORR") + hcorr = sr.live.magnets.get("HCORR") + vcorr = sr.live.magnets.get("VCORR") u = hcorr | vcorr @@ -230,8 +230,8 @@ def test_element_array_add_is_alias_of_union(install_test_package, accelerator_f sr = accelerator_from_fragments(*sr_configuration_fragments) sr.design.get_lattice().disable_6d() - hcorr = sr.live.get_magnets("HCORR") - vcorr = sr.live.get_magnets("VCORR") + hcorr = sr.live.magnets.get("HCORR") + vcorr = sr.live.magnets.get("VCORR") u1 = hcorr | vcorr u2 = hcorr + vcorr diff --git a/tests/test_patterns.py b/tests/arrays/test_patterns.py similarity index 66% rename from tests/test_patterns.py rename to tests/arrays/test_patterns.py index 79dbe8359..9b7ba7329 100644 --- a/tests/test_patterns.py +++ b/tests/arrays/test_patterns.py @@ -8,11 +8,11 @@ def test_tune(): sr: Accelerator = Accelerator.load("tests/config/EBSTune-patterns.yaml", ignore_external=True) sr.design.get_lattice().disable_6d() - quadForTune = sr.design.get_magnets("QForTune") + quadForTune = sr.design.magnets.get("QForTune") assert len(quadForTune.names()) == 124 - quadForTest = sr.design.get_magnets("QForTest") - assert sr.design.get_magnet("QF1E-C06") is not None - assert sr.design.get_magnet("QF1E-C05") is not None + quadForTest = sr.design.magnets.get("QForTest") + assert sr.design.magnet.get("QF1E-C06") is not None + assert sr.design.magnet.get("QF1E-C05") is not None assert "QF1E-C05" not in quadForTest.names() assert all([not (name.startswith("Q") and name.endswith("-C06")) for name in quadForTest.names()]) diff --git a/tests/test_ranges_array.py b/tests/arrays/test_ranges_array.py similarity index 69% rename from tests/test_ranges_array.py rename to tests/arrays/test_ranges_array.py index c4d577449..77c8c6d9c 100644 --- a/tests/test_ranges_array.py +++ b/tests/arrays/test_ranges_array.py @@ -10,11 +10,11 @@ indirect=True, ) def test_ranges_array(install_test_package): - sr: Accelerator = Accelerator.load("tests/config/EBSTune-range.yaml") - mag_cur = sr.live.get_magnets("QForTune").hardwares + sr: Accelerator = Accelerator.load("tests/config/EBSTune.yaml") + mag_cur = sr.live.magnets.get("QForTune").hardwares mag_cur.set(mag_cur.get() + 50) - mag = sr.live.get_magnets("QForTune").strengths + mag = sr.live.magnets.get("QForTune").strengths with pytest.raises(pyaml.PyAMLException, match="out of range") as excinfo: mag.set(mag.get() * 1000.0) diff --git a/tests/test_bpm.py b/tests/bpm/test_bpm.py similarity index 52% rename from tests/test_bpm.py rename to tests/bpm/test_bpm.py index 914d179ff..93ac68ec5 100644 --- a/tests/test_bpm.py +++ b/tests/bpm/test_bpm.py @@ -7,23 +7,37 @@ def test_simulator_bpm_tilt(): sr: Accelerator = Accelerator.load("tests/config/bpms.yaml", ignore_external=True) sr.design.get_lattice().disable_6d() - bpm = sr.design.get_bpm("BPM_C01-01") + sr.design.magnet.get("SH1A-C01-H").strength.set(10e-6) # Add orbit + sr.design.magnet.get("SH1A-C01-V").strength.set(10e-6) # Add orbit + bpm = sr.design.bpm.get("BPM_C01-01") + assert np.allclose(bpm.positions.get(), np.array([5.90809968e-05, 2.24832853e-05])) assert bpm.tilt.get() == 0 - bpm.tilt.set(0.01) - assert bpm.tilt.get() == 0.01 + alpha = np.pi / 3 + bpm.tilt.set(alpha) + assert bpm.tilt.get() == alpha + + new_x = 5.908792e-05 * np.cos(alpha) - 2.24832853e-05 * np.sin(alpha) + new_y = 5.908792e-05 * np.sin(alpha) + 2.24832853e-05 * np.cos(alpha) + assert np.allclose(bpm.positions.get(), np.array([new_x, new_y])) + + alpha = np.pi / 2 + bpm.tilt.set(alpha) + new_x = 5.908792e-05 * np.cos(alpha) - 2.24832853e-05 * np.sin(alpha) + new_y = 5.908792e-05 * np.sin(alpha) + 2.24832853e-05 * np.cos(alpha) + assert np.allclose(bpm.positions.get(), np.array([new_x, new_y])) def test_simulator_bpm_offset(): sr: Accelerator = Accelerator.load("tests/config/bpms.yaml", ignore_external=True) sr.design.get_lattice().disable_6d() - bpm = sr.design.get_bpm("BPM_C01-01") + bpm = sr.design.bpm.get("BPM_C01-01") assert bpm.offset.get()[0] == 0 assert bpm.offset.get()[1] == 0 bpm.offset.set(np.array([0.1, 0.2])) assert bpm.offset.get()[0] == 0.1 assert bpm.offset.get()[1] == 0.2 - assert np.allclose(bpm.positions.get(), np.array([0.0, 0.0])) + assert np.allclose(bpm.positions.get(), np.array([0.1, 0.2])) @pytest.mark.parametrize( @@ -34,8 +48,8 @@ def test_simulator_bpm_offset(): def test_simulator_bpm_position(install_test_package): sr: Accelerator = Accelerator.load("tests/config/bpms.yaml") sr.design.get_lattice().disable_6d() - bpm = sr.design.get_bpm("BPM_C01-01") - bpm_simple = sr.live.get_bpm("BPM_C01-02") + bpm = sr.design.bpm.get("BPM_C01-01") + bpm_simple = sr.live.bpm.get("BPM_C01-02") assert np.allclose(bpm.positions.get(), np.array([0.0, 0.0])) assert np.allclose(bpm_simple.positions.get(), np.array([0.0, 0.0])) @@ -44,12 +58,12 @@ def test_simulator_bpm_position(install_test_package): def test_simulator_bpm_position_with_bad_corrector_strength(): sr: Accelerator = Accelerator.load("tests/config/bpms.yaml", ignore_external=True) sr.design.get_lattice().disable_6d() - bpm1 = sr.design.get_bpm("BPM_C01-01") - bpm_simple = sr.design.get_bpm("BPM_C01-02") - bpm3 = sr.design.get_bpm("BPM_C01-03") + bpm1 = sr.design.bpm.get("BPM_C01-01") + bpm_simple = sr.design.bpm.get("BPM_C01-02") + bpm3 = sr.design.bpm.get("BPM_C01-03") - sr.design.get_magnet("SH1A-C01-H").strength.set(-1e-6) - sr.design.get_magnet("SH1A-C01-V").strength.set(-1e-6) + sr.design.magnet.get("SH1A-C01-H").strength.set(-1e-6) + sr.design.magnet.get("SH1A-C01-V").strength.set(-1e-6) for bpm in [bpm1, bpm_simple, bpm3]: assert bpm.positions.get()[0] != 0.0 assert bpm.positions.get()[1] != 0.0 diff --git a/tests/test_bpm_controlsystem.py b/tests/bpm/test_bpm_controlsystem.py similarity index 57% rename from tests/test_bpm_controlsystem.py rename to tests/bpm/test_bpm_controlsystem.py index c6aa51875..13321ca12 100644 --- a/tests/test_bpm_controlsystem.py +++ b/tests/bpm/test_bpm_controlsystem.py @@ -11,7 +11,7 @@ ) def test_controlsystem_bpm_tilt(install_test_package): sr: Accelerator = Accelerator.load("tests/config/bpms.yaml") - bpm = sr.live.get_bpm("BPM_C01-01") + bpm = sr.live.bpm.get("BPM_C01-01") print(bpm.tilt.get()) assert bpm.tilt.get() == 0 @@ -26,7 +26,7 @@ def test_controlsystem_bpm_tilt(install_test_package): ) def test_controlsystem_bpm_offset(install_test_package): sr: Accelerator = Accelerator.load("tests/config/bpms.yaml") - bpm = sr.live.get_bpm("BPM_C01-01") + bpm = sr.live.bpm.get("BPM_C01-01") assert bpm.offset.get()[0] == 0 assert bpm.offset.get()[1] == 0 @@ -43,13 +43,43 @@ def test_controlsystem_bpm_offset(install_test_package): ) def test_controlsystem_bpm_position(install_test_package): sr: Accelerator = Accelerator.load("tests/config/bpms.yaml") - bpm = sr.live.get_bpm("BPM_C01-01") - bpm_simple = sr.live.get_bpm("BPM_C01-02") + bpm = sr.live.bpm.get("BPM_C01-01") + bpm_simple = sr.live.bpm.get("BPM_C01-02") assert np.allclose(bpm.positions.get(), np.array([0.0, 0.0])) assert np.allclose(bpm_simple.positions.get(), np.array([0.0, 0.0])) +@pytest.mark.parametrize( + "install_test_package", + [{"name": "tango-pyaml", "path": "tests/dummy_cs/tango-pyaml"}], + indirect=True, +) +def test_controlsystem_get_devices_returns_attached_devices(install_test_package): + sr: Accelerator = Accelerator.load("tests/config/bpms.yaml") + + devs = sr.live.get_devices_access(["srdiag/bpm/c01-01/SA_HPosition", "srdiag/bpm/c01-01/SA_VPosition"]) + + assert devs[0].name() == "//ebs-simu-3:10000/srdiag/bpm/c01-01/SA_HPosition" + assert devs[1].name() == "//ebs-simu-3:10000/srdiag/bpm/c01-01/SA_VPosition" + + +@pytest.mark.parametrize( + "install_test_package", + [{"name": "tango-pyaml", "path": "tests/dummy_cs/tango-pyaml"}], + indirect=True, +) +def test_controlsystem_get_device_accepts_backend_config_model(install_test_package): + from tango.pyaml.attribute import ConfigModel as AttributeConfigModel + + sr: Accelerator = Accelerator.load("tests/config/bpms.yaml") + + dev = sr.live.get_device_access(AttributeConfigModel(attribute="srdiag/bpm/c01-05/SA_HPosition", unit="mm")) + + assert dev.name() == "//ebs-simu-3:10000/srdiag/bpm/c01-05/SA_HPosition" + assert dev.unit() == "mm" + + @pytest.mark.parametrize( "install_test_package", [{"name": "tango-pyaml", "path": "tests/dummy_cs/tango-pyaml"}], @@ -61,6 +91,6 @@ def test_controlsystem_bpm_position_indexed(install_test_package): set_attribute("srdiag/bpm/c01-04/Position", [0.0, 1.0], unit="mm") sr: Accelerator = Accelerator.load("tests/config/bpms.yaml") - bpm = sr.live.get_bpm("BPM_C01-04") + bpm = sr.live.bpm.get("BPM_C01-04") assert np.allclose(bpm.positions.get(), np.array([0.0, 1.0])) diff --git a/tests/common/test_element_holder.py b/tests/common/test_element_holder.py new file mode 100644 index 000000000..d7f66540f --- /dev/null +++ b/tests/common/test_element_holder.py @@ -0,0 +1,55 @@ +from pyaml.common.element import Element +from pyaml.common.holders.element_holder import ElementHolder + + +class DispatchElement(Element): + def _fill_device(self, holder: ElementHolder) -> None: + holder.filled_elements.append(self) + + +class DispatchHolder(ElementHolder): + def __init__(self): + super().__init__() + self.filled_elements = [] + + def create_magnet_strength_aggregator(self, magnets): + return None + + def create_magnet_hardware_aggregator(self, magnets): + return None + + def create_bpm_aggregators(self, bpms): + return [None, None, None] + + def _fill_magnet(self, magnet) -> None: + raise AssertionError("Unexpected magnet dispatch") + + def _fill_combined_function_magnet(self, magnet) -> None: + raise AssertionError("Unexpected combined-function magnet dispatch") + + def _fill_serialized_magnets(self, magnets) -> None: + raise AssertionError("Unexpected serialized magnet dispatch") + + def _fill_bpm(self, bpm) -> None: + raise AssertionError("Unexpected BPM dispatch") + + def _fill_rf_plant(self, rf_plant) -> None: + raise AssertionError("Unexpected RF plant dispatch") + + def _fill_betatron_tune_monitor(self, monitor) -> None: + raise AssertionError("Unexpected betatron tune monitor dispatch") + + def _fill_tool(self, tool) -> None: + raise AssertionError("Unexpected tool dispatch") + + def _fill_unbound_element(self, element) -> None: + raise AssertionError("Unexpected unbound element dispatch") + + +def test_fill_device_delegates_to_elements(): + holder = DispatchHolder() + elements = [DispatchElement("FIRST"), DispatchElement("SECOND")] + + holder.fill_device(elements) + + assert holder.filled_elements == elements diff --git a/tests/common/test_element_holder_collection.py b/tests/common/test_element_holder_collection.py new file mode 100644 index 000000000..937d2da79 --- /dev/null +++ b/tests/common/test_element_holder_collection.py @@ -0,0 +1,150 @@ +import pytest + +from pyaml.arrays.bpm_array import BPMArray +from pyaml.arrays.element_array import ElementArray +from pyaml.arrays.magnet_array import MagnetArray +from pyaml.bpm.bpm import BPM +from pyaml.common.exception import PyAMLException +from pyaml.lattice.simulator import Simulator + + +@pytest.fixture +def holder(accelerator_from_fragments, sr_configuration_fragments): + sr = accelerator_from_fragments(*sr_configuration_fragments) + sr.design.get_lattice().disable_6d() + return sr.design + + +def test_exact_name_returns_the_element_or_none(holder): + assert holder["BPM_C04-01"] is holder.bpm.get("BPM_C04-01") + assert holder["UNKNOWN"] is None + + +def test_get_and_full_slice_keep_registration_order(holder): + names = [element.get_name() for element in holder.get_all_elements()] + + assert type(holder.get()) is ElementArray + assert type(holder[:]) is ElementArray + assert holder.get().names() == names + assert holder[:].names() == names + assert names != sorted(names) + + +def test_collections_are_independent_but_share_elements(holder): + collection = holder.get() + first = holder[0] + original_names = collection.names() + + assert collection[0] is first + collection.clear() + assert holder[0] is first + assert holder.get().names() == original_names + + +def test_new_calls_reflect_registry_additions(holder): + previous = holder.get() + holder.fill_device([BPM("EXTRA_BPM", lattice_names="list(BPM_C04-01)")]) + + assert "EXTRA_BPM" not in previous.names() + assert holder.get().names() == previous.names() + ["EXTRA_BPM"] + assert holder["EXTRA_BPM"] is holder.bpm.get("EXTRA_BPM") + + +def test_patterns_always_return_arrays(holder): + assert isinstance(holder["BPM*"], BPMArray) + assert holder["BPM*"].names() == ["BPM_C04-01", "BPM_C04-02"] + assert isinstance(holder["BPM_C04-0[1]"], BPMArray) + assert holder["BPM_C04-0[1]"].names() == ["BPM_C04-01"] + assert holder["BPM_C04-0?"].names() == ["BPM_C04-01", "BPM_C04-02"] + assert type(holder["MISSING*"]) is ElementArray + assert holder["MISSING*"].names() == [] + + +def test_character_classes_in_name_patterns(holder): + assert holder["BPM_C04-0[12]"].names() == ["BPM_C04-01", "BPM_C04-02"] + assert holder["BPM_C04-0[1-2]"].names() == ["BPM_C04-01", "BPM_C04-02"] + assert holder["SH1A-C01-[HV]*"].names() == ["SH1A-C01-H", "SH1A-C01-V"] + assert holder["BPM_C04-0[!2]"].names() == ["BPM_C04-01"] + + +def test_colons_are_part_of_names(holder): + holder.fill_device([BPM("CELL04:BPM01", lattice_names="list(BPM_C04-01)")]) + + assert holder["CELL04:BPM01"] is holder.bpm.get("CELL04:BPM01") + assert holder["CELL04:BPM*"].names() == ["CELL04:BPM01"] + assert holder["model_name:*"].names() == [] + + +def test_magnet_subclasses_share_a_typed_array_in_either_order(holder): + horizontal = holder.magnet.get("SH1A-C01-H") + vertical = holder.magnet.get("SH1A-C01-V") + start = holder.get_all_elements().index(horizontal) + + assert type(horizontal) is not type(vertical) + assert isinstance(holder["SH1A-C01-[HV]"], MagnetArray) + assert isinstance(holder[start : start + 2], MagnetArray) + assert isinstance(holder[start + 1 : start - 1 : -1], MagnetArray) + assert holder[start + 1 : start - 1 : -1].names() == ["SH1A-C01-V", "SH1A-C01-H"] + + +def test_mixed_selection_returns_a_generic_array(holder): + selected = holder["*-C01*"] + + assert type(selected) is ElementArray + assert "QF1A-C01" in selected.names() + assert "SH1A-C01" in selected.names() + + +def test_indices_and_slices_follow_insertion_order(holder): + registered = holder.get_all_elements() + + assert holder[0] is registered[0] + assert holder[-1] is registered[-1] + assert list(holder[1:3]) == registered[1:3] + assert list(holder[::2]) == registered[::2] + assert isinstance(holder[-2:], BPMArray) + assert holder[-2:].names() == ["BPM_C04-01", "BPM_C04-02"] + assert type(holder[len(registered) :]) is ElementArray + + +def test_empty_holder_returns_empty_collections(ebs_lattice_file): + holder = Simulator(name="empty", lattice=str(ebs_lattice_file)) + + assert type(holder.get()) is ElementArray + assert holder[:].names() == [] + assert holder["BPM*"].names() == [] + assert holder["BPM_C04-01"] is None + + +def test_invalid_indices_and_keys_raise_clear_errors(holder): + size = len(holder.get_all_elements()) + + with pytest.raises(IndexError): + holder[size] + with pytest.raises(IndexError): + holder[-size - 1] + with pytest.raises(TypeError): + holder[1.5] + with pytest.raises(ValueError): + holder[::0] + + +def test_selection_intersects_with_a_configured_family(holder): + selected = holder["SH1A-C0?-H"] & holder.get_elements("ElArray") + + assert isinstance(selected, MagnetArray) + assert selected.names() == ["SH1A-C02-H"] + assert holder.get_element("SH1A-C02-H") is holder["SH1A-C02-H"] + assert holder.get_all_elements() == list(holder.get()) + with pytest.raises(PyAMLException): + holder.get_element("UNKNOWN") + + +def test_existing_array_field_filters_still_work(holder): + selected = holder["SH1A-C0?-H"]["model_name:SH1A-C01"] + + assert selected.names() == ["SH1A-C01-H"] + + +def test_existing_empty_intersection_stays_a_list(holder): + assert type(holder["SH1A-C0?-H"] & holder["SH1A-C0?-V"]) is list diff --git a/tests/test_errors.py b/tests/common/test_errors.py similarity index 81% rename from tests/test_errors.py rename to tests/common/test_errors.py index e58cc7cbf..38ce79f56 100644 --- a/tests/test_errors.py +++ b/tests/common/test_errors.py @@ -13,48 +13,49 @@ ) def test_tune(install_test_package): with pytest.raises(PyAMLConfigException) as exc: - ml: Accelerator = Accelerator.load("tests/config/bad_conf_duplicate_1.yaml") - assert "MagnetArray HCORR : duplicate name SH1A-C02-H @index 2" in str(exc) + ml: Accelerator = Accelerator.load("tests/config/bad_conf_duplicate_1.yaml", include_locations=True, validate=False) + print(exc.value) + assert "MagnetArray HCORR : duplicate name SH1A-C02-H @index 2" in str(exc.value) with pytest.raises(PyAMLConfigException) as exc: - ml: Accelerator = Accelerator.load("tests/config/bad_conf_duplicate_2.yaml") - assert "BPMArray BPM : duplicate name BPM_C04-06 @index 3" in str(exc) + ml: Accelerator = Accelerator.load("tests/config/bad_conf_duplicate_2.yaml", include_locations=True, validate=False) + assert "BPMArray BPM : duplicate name BPM_C04-06 @index 3" in str(exc.value) with pytest.raises(PyAMLConfigException) as exc: - ml: Accelerator = Accelerator.load("tests/config/bad_conf_duplicate_3.yaml") - assert "Configuration entry 'BPM_C04-06' is duplicated inside category 'devices'" in str(exc) - assert "bad_conf_duplicate_3.yaml" in str(exc) - assert "line 58, column 3" in str(exc) + ml: Accelerator = Accelerator.load("tests/config/bad_conf_duplicate_3.yaml", include_locations=True, validate=True) + assert "Configuration entry 'BPM_C04-06' is duplicated inside category 'devices'" in str(exc.value) + assert "bad_conf_duplicate_3.yaml" in str(exc.value) + assert "line 37, column 3" in str(exc.value) with pytest.raises(PyAMLConfigException) as exc: - ml: Accelerator = Accelerator.load("tests/config/bad_conf_duplicate_4.yaml") - assert "MagnetArray HCORR : duplicate name SH1A-C02-H @index 2" in str(exc) + ml: Accelerator = Accelerator.load("tests/config/bad_conf_duplicate_4.yaml", include_locations=True, validate=False) + assert "MagnetArray HCORR : duplicate name SH1A-C02-H @index 2" in str(exc.value) - sr: Accelerator = Accelerator.load("tests/config/EBSTune.yaml") - m1 = sr.live.get_magnet("QF1E-C04") - m2 = sr.design.get_magnet("QF1A-C05") + sr: Accelerator = Accelerator.load("tests/config/EBSTune.yaml", include_locations=True, validate=False) + m1 = sr.live.magnet.get("QF1E-C04") + m2 = sr.design.magnet.get("QF1A-C05") with pytest.raises(PyAMLException) as exc: ma = MagnetArray("Test", [m1, m2]) - assert "MagnetArray Test: All elements must be attached to the same instance" in str(exc) + assert "MagnetArray Test: All elements must be attached to the same instance" in str(exc.value) with pytest.raises(PyAMLException) as exc: - m2 = sr.design.get_magnet("QF1A-C05XX") - assert "Magnet QF1A-C05XX not defined" in str(exc) + m2 = sr.design.magnet.get("QF1A-C05XX") + assert "Magnet QF1A-C05XX not defined" in str(exc.value) with pytest.raises(PyAMLException) as exc: - m2 = sr.design.get_bpm("QF1A-C05XX") - assert "BPM QF1A-C05XX not defined" in str(exc) + m2 = sr.design.bpm.get("QF1A-C05XX") + assert "BPM QF1A-C05XX not defined" in str(exc.value) def test_duplicate_error_reports_source_line_and_column_across_files(tmp_path): devices_a = tmp_path / "devices_a.yaml" devices_a.write_text( - "- type: test.device\n name: BPM_DUPLICATE\n", + "- type: pyaml.bpm.bpm\n name: BPM_DUPLICATE\n", encoding="utf-8", ) devices_b = tmp_path / "devices_b.yaml" devices_b.write_text( - "- type: test.device\n name: BPM_UNIQUE\n- type: test.device\n name: BPM_DUPLICATE\n", + "- type: pyaml.bpm.bpm\n name: BPM_UNIQUE\n- type: pyaml.bpm.bpm\n name: BPM_DUPLICATE\n", encoding="utf-8", ) root = tmp_path / "root.yaml" @@ -64,7 +65,7 @@ def test_duplicate_error_reports_source_line_and_column_across_files(tmp_path): ) with pytest.raises(PyAMLConfigException) as exc: - Accelerator.load(str(root)) + Accelerator.load(str(root), include_locations=True, validate=True) message = str(exc.value) assert "Configuration entry 'BPM_DUPLICATE' is duplicated inside category 'devices'" in message @@ -90,7 +91,7 @@ def test_malformed_local_included_yaml_reports_source_line_and_column(tmp_path): ) with pytest.raises(PyAMLException) as exc: - Accelerator.load(str(root)) + Accelerator.load(str(root), include_locations=True, validate=False) message = str(exc.value) assert str(broken_devices) in message @@ -115,7 +116,7 @@ def test_truncated_local_included_json_reports_source_and_position(tmp_path): ) with pytest.raises(PyAMLException) as exc: - Accelerator.load(str(root)) + Accelerator.load(str(root), include_locations=True, validate=False) message = str(exc.value) assert str(broken_devices) in message diff --git a/tests/config/EBSNames.yaml b/tests/config/EBSNames.yaml index c359cecbd..b0eee6afc 100644 --- a/tests/config/EBSNames.yaml +++ b/tests/config/EBSNames.yaml @@ -10,6 +10,7 @@ controls: - type: tango.pyaml.controlsystem tango_host: ebs-simu-3:10000 name: live + catalog: catalogs/ebs_catalogs.yaml data_folder: /data/store devices: - type: pyaml.magnet.quadrupole @@ -19,13 +20,11 @@ devices: calibration_factor: 1.00054 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c04-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c04-e/current - type: pyaml.magnet.quadrupole name: QF1E-ALL lattice_names: list(QF1E,QF1I) @@ -34,13 +33,11 @@ devices: calibration_factor: 1.00054 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c04-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c04-e/current - type: pyaml.magnet.quadrupole name: QF1E-C05 lattice_names: QF1E@1 @@ -49,13 +46,11 @@ devices: calibration_factor: 0.996841 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c05-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c05-a/current - type: pyaml.magnet.quadrupole name: QF1E-C04-C05-C06 lattice_names: QF1E@0,1,2 @@ -64,13 +59,11 @@ devices: calibration_factor: 1.00191 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c05-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c05-e/current - type: pyaml.magnet.quadrupole name: QF1E-C04-C05-C06-2 lattice_names: "@140,290,424" @@ -79,13 +72,11 @@ devices: calibration_factor: 1.00191 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c05-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c05-e/current - type: pyaml.magnet.quadrupole name: QF1E-C04-C05-C06-3 lattice_names: QF1E#0..3 @@ -94,10 +85,8 @@ devices: calibration_factor: 1.00191 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c05-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c05-e/current diff --git a/tests/config/EBSOrbit.yaml b/tests/config/EBSOrbit.yaml index 39df579a0..5d6ea2570 100644 --- a/tests/config/EBSOrbit.yaml +++ b/tests/config/EBSOrbit.yaml @@ -1,6 +1,6 @@ type: pyaml.accelerator -facility: ESRF machine: sr +facility: ESRF energy: 6e9 alphac: 8.623614679299252e-05 simulators: @@ -11,6 +11,7 @@ controls: - type: tango.pyaml.controlsystem tango_host: ebs-simu-3:10000 name: live + catalog: catalogs/ebs_catalogs.yaml data_folder: /data/store arrays: - type: pyaml.arrays.magnet @@ -34,23 +35,55 @@ arrays: name: BPM elements: - BPM* + - type: pyaml.arrays.magnet + name: QForTune + elements: + - QD2* + - QF1* devices: +- type: pyaml.tuning_tools.bba + name: BBA-BPM_C04-04 + bpm_array_name: BPM + bpm_name : BPM_C04-04 + hcorr_name : SF2E-C02-H + vcorr_name : SD1A-C26-V + quad_name : QF6B-C04 + n_step: 7 + hcorr_delta : 1e-05 + vcorr_delta : 1e-05 + hquad_delta : 0.005 + vquad_delta : 0.005 +- type: pyaml.tuning_tools.bba2 + name: BBA2-BPM_C04-04 + bpm_array_name: BPM + bpm_name : BPM_C04-04 + hcorr_name : SF2E-C02-H + vcorr_name : SD1A-C26-V + quad_name : QF6B-C04 + tune_correction_name: DEFAULT_TUNE_CORRECTION + hcorr_delta : 1e-05 + vcorr_delta : 1e-05 + quad_delta : 0.005 - type: pyaml.diagnostics.tune_monitor name: BETATRON_TUNE - tune_h: - type: tango.pyaml.attribute_read_only - attribute: sys/ringsimulator/ebs/Tune_h - unit: "" - tune_v: - type: tango.pyaml.attribute_read_only - attribute: sys/ringsimulator/ebs/Tune_v - unit: "" -- type: pyaml.diagnostics.chromaticity_monitor + tune_h: srdiag/beam-tune/main/Qh + tune_v: srdiag/beam-tune/main/Qv +- type: pyaml.tuning_tools.chromaticity_monitor name: CHROMATICITY_MONITOR betatron_tune_name: BETATRON_TUNE - rf_plant_name: RF + rf_plant_name: DEFAULT_RF_PLANT bpm_array_name: BPM n_step: 5 +- type: pyaml.tuning_tools.tune + name: DEFAULT_TUNE_CORRECTION + quad_array_name: QForTune + betatron_tune_name: BETATRON_TUNE + response_matrix: ${path:tune_response.json} +- type: pyaml.tuning_tools.tune_response_matrix + name: DEFAULT_TUNE_RESPONSE_MATRIX + quad_array_name: QForTune + betatron_tune_name: BETATRON_TUNE + quad_delta: 1e-4 - type: pyaml.tuning_tools.chromaticity_response_matrix name: DEFAULT_CHROMATICITY_RESPONSE_MATRIX sextu_array_name: Sext @@ -58,17 +91,17 @@ devices: sextu_delta: 1e-6 - type: pyaml.tuning_tools.chromaticity name: DEFAULT_CHROMATICITY_CORRECTION - chromaticty_monitor_name: CHROMATICITY_MONITOR + chromaticity_monitor_name: CHROMATICITY_MONITOR sextu_array_name: Sext - response_matrix: file:ideal_chroma_resp.json + response_matrix: ${path:ideal_chroma_resp.json} - type: pyaml.tuning_tools.orbit bpm_array_name: BPM hcorr_array_name: HCorr vcorr_array_name: VCorr - rf_plant_name: RF + rf_plant_name: DEFAULT_RF_PLANT name: DEFAULT_ORBIT_CORRECTION singular_values: 162 - response_matrix: file:ideal_orm_disp.json + response_matrix: ${path:ideal_orm_disp.json} - type: pyaml.tuning_tools.orbit_response_matrix bpm_array_name: BPM hcorr_array_name: HCorr @@ -77,25 +110,31 @@ devices: name: DEFAULT_ORBIT_RESPONSE_MATRIX - type: pyaml.tuning_tools.dispersion bpm_array_name: BPM - rf_plant_name: RF + rf_plant_name: DEFAULT_RF_PLANT frequency_delta: 10 name: DEFAULT_DISPERSION - type: pyaml.rf.rf_plant - name: RF - masterclock: - type: tango.pyaml.attribute - attribute: sy/ms/1/Frequency - unit: Hz + name: DEFAULT_RF_PLANT + masterclock: sy/ms/1/Frequency transmitters: - type: pyaml.rf.rf_transmitter name: RFTRA cavities: [CAV_C05_01,CAV_C05_02,CAV_C05_03,CAV_C05_04,CAV_C05_05,CAV_C07_01,CAV_C07_02,CAV_C07_03,CAV_C07_04,CAV_C07_05,CAV_C25_01,CAV_C25_02,CAV_C25_03] harmonic: 1 distribution: 1 - voltage: - type: tango.pyaml.attribute - attribute: sys/ringsimulator/ebs/RfVoltage - unit: V + voltage: sys/ringsimulator/ebs/RfVoltage +- type: pyaml.magnet.quadrupole + name: QF6B-C04 + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.998960997 + crosstalk: 0.99918 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF6_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf6/c04-b/current - type: pyaml.magnet.cfm_magnet name: SH1A-C04 mapping: @@ -108,34 +147,25 @@ devices: multipoles: [B0,A0,A1,B2] pseudo_factors: [1.0,-1.0,-1.0,-1.0] units: [rad,rad,m-1,m-2] + hardware_units: ["A","A","A","A","A"] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SHI_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SHI_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SHI_sq_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SHI_sext_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SHI_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c04-a-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c04-a-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c04-a-ch3/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c04-a-ch5/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c04-a-ch6/current - unit: A + - srmag/ps-corr-sh1/c04-a-ch1/current + - srmag/ps-corr-sh1/c04-a-ch2/current + - srmag/ps-corr-sh1/c04-a-ch3/current + - srmag/ps-corr-sh1/c04-a-ch5/current + - srmag/ps-corr-sh1/c04-a-ch6/current - type: pyaml.magnet.cfm_magnet name: SJ1A-C04 mapping: @@ -148,18 +178,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c04-a/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c04-a/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c04-a/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c04-a/Strength - unit: m-2 + - srmag/m-sd1/c04-a/Strength_H + - srmag/m-sd1/c04-a/Strength_V + - srmag/m-sd1/c04-a/Strength_SQ + - srmag/m-sd1/c04-a/Strength - type: pyaml.magnet.cfm_magnet name: SJ2A-C04 mapping: @@ -172,18 +194,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c04-a/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c04-a/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c04-a/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c04-a/Strength - unit: m-2 + - srmag/m-sf2/c04-a/Strength_H + - srmag/m-sf2/c04-a/Strength_V + - srmag/m-sf2/c04-a/Strength_SQ + - srmag/m-sf2/c04-a/Strength - type: pyaml.magnet.cfm_magnet name: SJ1B-C04 mapping: @@ -196,18 +210,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c04-b/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c04-b/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c04-b/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c04-b/Strength - unit: m-2 + - srmag/m-sd1/c04-b/Strength_H + - srmag/m-sd1/c04-b/Strength_V + - srmag/m-sd1/c04-b/Strength_SQ + - srmag/m-sd1/c04-b/Strength - type: pyaml.magnet.cfm_magnet name: SH2B-C04 mapping: @@ -218,27 +224,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c04-b-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c04-b-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c04-b-ch3/current - unit: A + - srmag/ps-corr-sh2/c04-b-ch1/current + - srmag/ps-corr-sh2/c04-b-ch2/current + - srmag/ps-corr-sh2/c04-b-ch3/current - type: pyaml.magnet.cfm_magnet name: SJ1D-C04 mapping: @@ -251,18 +252,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c04-d/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c04-d/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c04-d/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c04-d/Strength - unit: m-2 + - srmag/m-sd1/c04-d/Strength_H + - srmag/m-sd1/c04-d/Strength_V + - srmag/m-sd1/c04-d/Strength_SQ + - srmag/m-sd1/c04-d/Strength - type: pyaml.magnet.cfm_magnet name: SJ2E-C04 mapping: @@ -275,18 +268,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c04-e/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c04-e/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c04-e/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c04-e/Strength - unit: m-2 + - srmag/m-sf2/c04-e/Strength_H + - srmag/m-sf2/c04-e/Strength_V + - srmag/m-sf2/c04-e/Strength_SQ + - srmag/m-sf2/c04-e/Strength - type: pyaml.magnet.cfm_magnet name: SJ1E-C04 mapping: @@ -299,18 +284,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c04-e/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c04-e/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c04-e/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c04-e/Strength - unit: m-2 + - srmag/m-sd1/c04-e/Strength_H + - srmag/m-sd1/c04-e/Strength_V + - srmag/m-sd1/c04-e/Strength_SQ + - srmag/m-sd1/c04-e/Strength - type: pyaml.magnet.cfm_magnet name: SH3E-C04 mapping: @@ -321,27 +298,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c04-e-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c04-e-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c04-e-ch3/current - unit: A + - srmag/ps-corr-sh3/c04-e-ch1/current + - srmag/ps-corr-sh3/c04-e-ch2/current + - srmag/ps-corr-sh3/c04-e-ch3/current - type: pyaml.magnet.cfm_magnet name: SH1A-C05 mapping: @@ -352,27 +324,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c05-a-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c05-a-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c05-a-ch3/current - unit: A + - srmag/ps-corr-sh1/c05-a-ch1/current + - srmag/ps-corr-sh1/c05-a-ch2/current + - srmag/ps-corr-sh1/c05-a-ch3/current - type: pyaml.magnet.cfm_magnet name: SD1A-C05 mapping: @@ -385,18 +352,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c05-a/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c05-a/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c05-a/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c05-a/Strength - unit: m-2 + - srmag/m-sd1/c05-a/Strength_H + - srmag/m-sd1/c05-a/Strength_V + - srmag/m-sd1/c05-a/Strength_SQ + - srmag/m-sd1/c05-a/Strength - type: pyaml.magnet.cfm_magnet name: SF2A-C05 mapping: @@ -409,18 +368,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c05-a/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c05-a/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c05-a/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c05-a/Strength - unit: m-2 + - srmag/m-sf2/c05-a/Strength_H + - srmag/m-sf2/c05-a/Strength_V + - srmag/m-sf2/c05-a/Strength_SQ + - srmag/m-sf2/c05-a/Strength - type: pyaml.magnet.cfm_magnet name: SD1B-C05 mapping: @@ -433,18 +384,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c05-b/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c05-b/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c05-b/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c05-b/Strength - unit: m-2 + - srmag/m-sd1/c05-b/Strength_H + - srmag/m-sd1/c05-b/Strength_V + - srmag/m-sd1/c05-b/Strength_SQ + - srmag/m-sd1/c05-b/Strength - type: pyaml.magnet.cfm_magnet name: SH2B-C05 mapping: @@ -455,27 +398,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c05-b-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c05-b-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c05-b-ch3/current - unit: A + - srmag/ps-corr-sh2/c05-b-ch1/current + - srmag/ps-corr-sh2/c05-b-ch2/current + - srmag/ps-corr-sh2/c05-b-ch3/current - type: pyaml.magnet.cfm_magnet name: SD1D-C05 mapping: @@ -488,18 +426,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c05-d/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c05-d/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c05-d/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c05-d/Strength - unit: m-2 + - srmag/m-sd1/c05-d/Strength_H + - srmag/m-sd1/c05-d/Strength_V + - srmag/m-sd1/c05-d/Strength_SQ + - srmag/m-sd1/c05-d/Strength - type: pyaml.magnet.cfm_magnet name: SF2E-C05 mapping: @@ -512,18 +442,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c05-e/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c05-e/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c05-e/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c05-e/Strength - unit: m-2 + - srmag/m-sf2/c05-e/Strength_H + - srmag/m-sf2/c05-e/Strength_V + - srmag/m-sf2/c05-e/Strength_SQ + - srmag/m-sf2/c05-e/Strength - type: pyaml.magnet.cfm_magnet name: SD1E-C05 mapping: @@ -536,18 +458,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c05-e/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c05-e/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c05-e/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c05-e/Strength - unit: m-2 + - srmag/m-sd1/c05-e/Strength_H + - srmag/m-sd1/c05-e/Strength_V + - srmag/m-sd1/c05-e/Strength_SQ + - srmag/m-sd1/c05-e/Strength - type: pyaml.magnet.cfm_magnet name: SH3E-C05 mapping: @@ -558,27 +472,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c05-e-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c05-e-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c05-e-ch3/current - unit: A + - srmag/ps-corr-sh3/c05-e-ch1/current + - srmag/ps-corr-sh3/c05-e-ch2/current + - srmag/ps-corr-sh3/c05-e-ch3/current - type: pyaml.magnet.cfm_magnet name: SH1A-C06 mapping: @@ -589,27 +498,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c06-a-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c06-a-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c06-a-ch3/current - unit: A + - srmag/ps-corr-sh1/c06-a-ch1/current + - srmag/ps-corr-sh1/c06-a-ch2/current + - srmag/ps-corr-sh1/c06-a-ch3/current - type: pyaml.magnet.cfm_magnet name: SD1A-C06 mapping: @@ -622,18 +526,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c06-a/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c06-a/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c06-a/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c06-a/Strength - unit: m-2 + - srmag/m-sd1/c06-a/Strength_H + - srmag/m-sd1/c06-a/Strength_V + - srmag/m-sd1/c06-a/Strength_SQ + - srmag/m-sd1/c06-a/Strength - type: pyaml.magnet.cfm_magnet name: SF2A-C06 mapping: @@ -646,18 +542,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c06-a/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c06-a/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c06-a/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c06-a/Strength - unit: m-2 + - srmag/m-sf2/c06-a/Strength_H + - srmag/m-sf2/c06-a/Strength_V + - srmag/m-sf2/c06-a/Strength_SQ + - srmag/m-sf2/c06-a/Strength - type: pyaml.magnet.cfm_magnet name: SD1B-C06 mapping: @@ -670,18 +558,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c06-b/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c06-b/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c06-b/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c06-b/Strength - unit: m-2 + - srmag/m-sd1/c06-b/Strength_H + - srmag/m-sd1/c06-b/Strength_V + - srmag/m-sd1/c06-b/Strength_SQ + - srmag/m-sd1/c06-b/Strength - type: pyaml.magnet.cfm_magnet name: SH2B-C06 mapping: @@ -692,27 +572,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c06-b-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c06-b-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c06-b-ch3/current - unit: A + - srmag/ps-corr-sh2/c06-b-ch1/current + - srmag/ps-corr-sh2/c06-b-ch2/current + - srmag/ps-corr-sh2/c06-b-ch3/current - type: pyaml.magnet.cfm_magnet name: SD1D-C06 mapping: @@ -725,18 +600,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c06-d/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c06-d/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c06-d/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c06-d/Strength - unit: m-2 + - srmag/m-sd1/c06-d/Strength_H + - srmag/m-sd1/c06-d/Strength_V + - srmag/m-sd1/c06-d/Strength_SQ + - srmag/m-sd1/c06-d/Strength - type: pyaml.magnet.cfm_magnet name: SF2E-C06 mapping: @@ -749,18 +616,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c06-e/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c06-e/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c06-e/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c06-e/Strength - unit: m-2 + - srmag/m-sf2/c06-e/Strength_H + - srmag/m-sf2/c06-e/Strength_V + - srmag/m-sf2/c06-e/Strength_SQ + - srmag/m-sf2/c06-e/Strength - type: pyaml.magnet.cfm_magnet name: SD1E-C06 mapping: @@ -773,18 +632,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c06-e/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c06-e/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c06-e/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c06-e/Strength - unit: m-2 + - srmag/m-sd1/c06-e/Strength_H + - srmag/m-sd1/c06-e/Strength_V + - srmag/m-sd1/c06-e/Strength_SQ + - srmag/m-sd1/c06-e/Strength - type: pyaml.magnet.cfm_magnet name: SH3E-C06 mapping: @@ -795,27 +646,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c06-e-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c06-e-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c06-e-ch3/current - unit: A + - srmag/ps-corr-sh3/c06-e-ch1/current + - srmag/ps-corr-sh3/c06-e-ch2/current + - srmag/ps-corr-sh3/c06-e-ch3/current - type: pyaml.magnet.cfm_magnet name: SH1A-C07 mapping: @@ -826,27 +672,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c07-a-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c07-a-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c07-a-ch3/current - unit: A + - srmag/ps-corr-sh1/c07-a-ch1/current + - srmag/ps-corr-sh1/c07-a-ch2/current + - srmag/ps-corr-sh1/c07-a-ch3/current - type: pyaml.magnet.cfm_magnet name: SD1A-C07 mapping: @@ -859,18 +700,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c07-a/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c07-a/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c07-a/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c07-a/Strength - unit: m-2 + - srmag/m-sd1/c07-a/Strength_H + - srmag/m-sd1/c07-a/Strength_V + - srmag/m-sd1/c07-a/Strength_SQ + - srmag/m-sd1/c07-a/Strength - type: pyaml.magnet.cfm_magnet name: SF2A-C07 mapping: @@ -883,18 +716,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c07-a/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c07-a/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c07-a/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c07-a/Strength - unit: m-2 + - srmag/m-sf2/c07-a/Strength_H + - srmag/m-sf2/c07-a/Strength_V + - srmag/m-sf2/c07-a/Strength_SQ + - srmag/m-sf2/c07-a/Strength - type: pyaml.magnet.cfm_magnet name: SD1B-C07 mapping: @@ -907,18 +732,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c07-b/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c07-b/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c07-b/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c07-b/Strength - unit: m-2 + - srmag/m-sd1/c07-b/Strength_H + - srmag/m-sd1/c07-b/Strength_V + - srmag/m-sd1/c07-b/Strength_SQ + - srmag/m-sd1/c07-b/Strength - type: pyaml.magnet.cfm_magnet name: SH2B-C07 mapping: @@ -929,27 +746,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c07-b-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c07-b-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c07-b-ch3/current - unit: A + - srmag/ps-corr-sh2/c07-b-ch1/current + - srmag/ps-corr-sh2/c07-b-ch2/current + - srmag/ps-corr-sh2/c07-b-ch3/current - type: pyaml.magnet.cfm_magnet name: SD1D-C07 mapping: @@ -962,18 +774,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c07-d/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c07-d/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c07-d/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c07-d/Strength - unit: m-2 + - srmag/m-sd1/c07-d/Strength_H + - srmag/m-sd1/c07-d/Strength_V + - srmag/m-sd1/c07-d/Strength_SQ + - srmag/m-sd1/c07-d/Strength - type: pyaml.magnet.cfm_magnet name: SF2E-C07 mapping: @@ -986,18 +790,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c07-e/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c07-e/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c07-e/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c07-e/Strength - unit: m-2 + - srmag/m-sf2/c07-e/Strength_H + - srmag/m-sf2/c07-e/Strength_V + - srmag/m-sf2/c07-e/Strength_SQ + - srmag/m-sf2/c07-e/Strength - type: pyaml.magnet.cfm_magnet name: SD1E-C07 mapping: @@ -1010,18 +806,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c07-e/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c07-e/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c07-e/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c07-e/Strength - unit: m-2 + - srmag/m-sd1/c07-e/Strength_H + - srmag/m-sd1/c07-e/Strength_V + - srmag/m-sd1/c07-e/Strength_SQ + - srmag/m-sd1/c07-e/Strength - type: pyaml.magnet.cfm_magnet name: SH3E-C07 mapping: @@ -1032,27 +820,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c07-e-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c07-e-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c07-e-ch3/current - unit: A + - srmag/ps-corr-sh3/c07-e-ch1/current + - srmag/ps-corr-sh3/c07-e-ch2/current + - srmag/ps-corr-sh3/c07-e-ch3/current - type: pyaml.magnet.cfm_magnet name: SH1A-C08 mapping: @@ -1063,27 +846,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c08-a-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c08-a-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c08-a-ch3/current - unit: A + - srmag/ps-corr-sh1/c08-a-ch1/current + - srmag/ps-corr-sh1/c08-a-ch2/current + - srmag/ps-corr-sh1/c08-a-ch3/current - type: pyaml.magnet.cfm_magnet name: SD1A-C08 mapping: @@ -1096,18 +874,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c08-a/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c08-a/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c08-a/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c08-a/Strength - unit: m-2 + - srmag/m-sd1/c08-a/Strength_H + - srmag/m-sd1/c08-a/Strength_V + - srmag/m-sd1/c08-a/Strength_SQ + - srmag/m-sd1/c08-a/Strength - type: pyaml.magnet.cfm_magnet name: SF2A-C08 mapping: @@ -1120,18 +890,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c08-a/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c08-a/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c08-a/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c08-a/Strength - unit: m-2 + - srmag/m-sf2/c08-a/Strength_H + - srmag/m-sf2/c08-a/Strength_V + - srmag/m-sf2/c08-a/Strength_SQ + - srmag/m-sf2/c08-a/Strength - type: pyaml.magnet.cfm_magnet name: SD1B-C08 mapping: @@ -1144,18 +906,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c08-b/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c08-b/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c08-b/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c08-b/Strength - unit: m-2 + - srmag/m-sd1/c08-b/Strength_H + - srmag/m-sd1/c08-b/Strength_V + - srmag/m-sd1/c08-b/Strength_SQ + - srmag/m-sd1/c08-b/Strength - type: pyaml.magnet.cfm_magnet name: SH2B-C08 mapping: @@ -1166,27 +920,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c08-b-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c08-b-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c08-b-ch3/current - unit: A + - srmag/ps-corr-sh2/c08-b-ch1/current + - srmag/ps-corr-sh2/c08-b-ch2/current + - srmag/ps-corr-sh2/c08-b-ch3/current - type: pyaml.magnet.cfm_magnet name: SD1D-C08 mapping: @@ -1199,18 +948,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c08-d/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c08-d/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c08-d/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c08-d/Strength - unit: m-2 + - srmag/m-sd1/c08-d/Strength_H + - srmag/m-sd1/c08-d/Strength_V + - srmag/m-sd1/c08-d/Strength_SQ + - srmag/m-sd1/c08-d/Strength - type: pyaml.magnet.cfm_magnet name: SF2E-C08 mapping: @@ -1223,18 +964,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c08-e/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c08-e/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c08-e/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c08-e/Strength - unit: m-2 + - srmag/m-sf2/c08-e/Strength_H + - srmag/m-sf2/c08-e/Strength_V + - srmag/m-sf2/c08-e/Strength_SQ + - srmag/m-sf2/c08-e/Strength - type: pyaml.magnet.cfm_magnet name: SD1E-C08 mapping: @@ -1247,18 +980,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c08-e/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c08-e/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c08-e/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c08-e/Strength - unit: m-2 + - srmag/m-sd1/c08-e/Strength_H + - srmag/m-sd1/c08-e/Strength_V + - srmag/m-sd1/c08-e/Strength_SQ + - srmag/m-sd1/c08-e/Strength - type: pyaml.magnet.cfm_magnet name: SH3E-C08 mapping: @@ -1269,27 +994,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c08-e-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c08-e-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c08-e-ch3/current - unit: A + - srmag/ps-corr-sh3/c08-e-ch1/current + - srmag/ps-corr-sh3/c08-e-ch2/current + - srmag/ps-corr-sh3/c08-e-ch3/current - type: pyaml.magnet.cfm_magnet name: SH1A-C09 mapping: @@ -1300,27 +1020,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c09-a-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c09-a-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c09-a-ch3/current - unit: A + - srmag/ps-corr-sh1/c09-a-ch1/current + - srmag/ps-corr-sh1/c09-a-ch2/current + - srmag/ps-corr-sh1/c09-a-ch3/current - type: pyaml.magnet.cfm_magnet name: SD1A-C09 mapping: @@ -1333,18 +1048,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c09-a/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c09-a/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c09-a/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c09-a/Strength - unit: m-2 + - srmag/m-sd1/c09-a/Strength_H + - srmag/m-sd1/c09-a/Strength_V + - srmag/m-sd1/c09-a/Strength_SQ + - srmag/m-sd1/c09-a/Strength - type: pyaml.magnet.cfm_magnet name: SF2A-C09 mapping: @@ -1357,18 +1064,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c09-a/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c09-a/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c09-a/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c09-a/Strength - unit: m-2 + - srmag/m-sf2/c09-a/Strength_H + - srmag/m-sf2/c09-a/Strength_V + - srmag/m-sf2/c09-a/Strength_SQ + - srmag/m-sf2/c09-a/Strength - type: pyaml.magnet.cfm_magnet name: SD1B-C09 mapping: @@ -1381,18 +1080,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c09-b/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c09-b/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c09-b/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c09-b/Strength - unit: m-2 + - srmag/m-sd1/c09-b/Strength_H + - srmag/m-sd1/c09-b/Strength_V + - srmag/m-sd1/c09-b/Strength_SQ + - srmag/m-sd1/c09-b/Strength - type: pyaml.magnet.cfm_magnet name: SH2B-C09 mapping: @@ -1403,27 +1094,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c09-b-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c09-b-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c09-b-ch3/current - unit: A + - srmag/ps-corr-sh2/c09-b-ch1/current + - srmag/ps-corr-sh2/c09-b-ch2/current + - srmag/ps-corr-sh2/c09-b-ch3/current - type: pyaml.magnet.cfm_magnet name: SD1D-C09 mapping: @@ -1436,18 +1122,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c09-d/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c09-d/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c09-d/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c09-d/Strength - unit: m-2 + - srmag/m-sd1/c09-d/Strength_H + - srmag/m-sd1/c09-d/Strength_V + - srmag/m-sd1/c09-d/Strength_SQ + - srmag/m-sd1/c09-d/Strength - type: pyaml.magnet.cfm_magnet name: SF2E-C09 mapping: @@ -1460,18 +1138,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c09-e/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c09-e/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c09-e/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c09-e/Strength - unit: m-2 + - srmag/m-sf2/c09-e/Strength_H + - srmag/m-sf2/c09-e/Strength_V + - srmag/m-sf2/c09-e/Strength_SQ + - srmag/m-sf2/c09-e/Strength - type: pyaml.magnet.cfm_magnet name: SD1E-C09 mapping: @@ -1484,18 +1154,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c09-e/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c09-e/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c09-e/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c09-e/Strength - unit: m-2 + - srmag/m-sd1/c09-e/Strength_H + - srmag/m-sd1/c09-e/Strength_V + - srmag/m-sd1/c09-e/Strength_SQ + - srmag/m-sd1/c09-e/Strength - type: pyaml.magnet.cfm_magnet name: SH3E-C09 mapping: @@ -1506,27 +1168,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c09-e-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c09-e-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c09-e-ch3/current - unit: A + - srmag/ps-corr-sh3/c09-e-ch1/current + - srmag/ps-corr-sh3/c09-e-ch2/current + - srmag/ps-corr-sh3/c09-e-ch3/current - type: pyaml.magnet.cfm_magnet name: SH1A-C10 mapping: @@ -1537,27 +1194,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c10-a-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c10-a-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c10-a-ch3/current - unit: A + - srmag/ps-corr-sh1/c10-a-ch1/current + - srmag/ps-corr-sh1/c10-a-ch2/current + - srmag/ps-corr-sh1/c10-a-ch3/current - type: pyaml.magnet.cfm_magnet name: SD1A-C10 mapping: @@ -1570,18 +1222,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c10-a/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c10-a/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c10-a/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c10-a/Strength - unit: m-2 + - srmag/m-sd1/c10-a/Strength_H + - srmag/m-sd1/c10-a/Strength_V + - srmag/m-sd1/c10-a/Strength_SQ + - srmag/m-sd1/c10-a/Strength - type: pyaml.magnet.cfm_magnet name: SF2A-C10 mapping: @@ -1594,18 +1238,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c10-a/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c10-a/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c10-a/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c10-a/Strength - unit: m-2 + - srmag/m-sf2/c10-a/Strength_H + - srmag/m-sf2/c10-a/Strength_V + - srmag/m-sf2/c10-a/Strength_SQ + - srmag/m-sf2/c10-a/Strength - type: pyaml.magnet.cfm_magnet name: SD1B-C10 mapping: @@ -1618,18 +1254,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c10-b/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c10-b/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c10-b/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c10-b/Strength - unit: m-2 + - srmag/m-sd1/c10-b/Strength_H + - srmag/m-sd1/c10-b/Strength_V + - srmag/m-sd1/c10-b/Strength_SQ + - srmag/m-sd1/c10-b/Strength - type: pyaml.magnet.cfm_magnet name: SH2B-C10 mapping: @@ -1640,27 +1268,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c10-b-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c10-b-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c10-b-ch3/current - unit: A + - srmag/ps-corr-sh2/c10-b-ch1/current + - srmag/ps-corr-sh2/c10-b-ch2/current + - srmag/ps-corr-sh2/c10-b-ch3/current - type: pyaml.magnet.cfm_magnet name: SD1D-C10 mapping: @@ -1673,18 +1296,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c10-d/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c10-d/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c10-d/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c10-d/Strength - unit: m-2 + - srmag/m-sd1/c10-d/Strength_H + - srmag/m-sd1/c10-d/Strength_V + - srmag/m-sd1/c10-d/Strength_SQ + - srmag/m-sd1/c10-d/Strength - type: pyaml.magnet.cfm_magnet name: SF2E-C10 mapping: @@ -1697,18 +1312,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c10-e/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c10-e/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c10-e/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c10-e/Strength - unit: m-2 + - srmag/m-sf2/c10-e/Strength_H + - srmag/m-sf2/c10-e/Strength_V + - srmag/m-sf2/c10-e/Strength_SQ + - srmag/m-sf2/c10-e/Strength - type: pyaml.magnet.cfm_magnet name: SD1E-C10 mapping: @@ -1721,18 +1328,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c10-e/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c10-e/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c10-e/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c10-e/Strength - unit: m-2 + - srmag/m-sd1/c10-e/Strength_H + - srmag/m-sd1/c10-e/Strength_V + - srmag/m-sd1/c10-e/Strength_SQ + - srmag/m-sd1/c10-e/Strength - type: pyaml.magnet.cfm_magnet name: SH3E-C10 mapping: @@ -1743,27 +1342,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c10-e-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c10-e-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c10-e-ch3/current - unit: A + - srmag/ps-corr-sh3/c10-e-ch1/current + - srmag/ps-corr-sh3/c10-e-ch2/current + - srmag/ps-corr-sh3/c10-e-ch3/current - type: pyaml.magnet.cfm_magnet name: SH1A-C11 mapping: @@ -1774,27 +1368,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c11-a-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c11-a-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c11-a-ch3/current - unit: A + - srmag/ps-corr-sh1/c11-a-ch1/current + - srmag/ps-corr-sh1/c11-a-ch2/current + - srmag/ps-corr-sh1/c11-a-ch3/current - type: pyaml.magnet.cfm_magnet name: SD1A-C11 mapping: @@ -1807,18 +1396,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c11-a/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c11-a/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c11-a/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c11-a/Strength - unit: m-2 + - srmag/m-sd1/c11-a/Strength_H + - srmag/m-sd1/c11-a/Strength_V + - srmag/m-sd1/c11-a/Strength_SQ + - srmag/m-sd1/c11-a/Strength - type: pyaml.magnet.cfm_magnet name: SF2A-C11 mapping: @@ -1831,18 +1412,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c11-a/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c11-a/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c11-a/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c11-a/Strength - unit: m-2 + - srmag/m-sf2/c11-a/Strength_H + - srmag/m-sf2/c11-a/Strength_V + - srmag/m-sf2/c11-a/Strength_SQ + - srmag/m-sf2/c11-a/Strength - type: pyaml.magnet.cfm_magnet name: SD1B-C11 mapping: @@ -1855,18 +1428,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c11-b/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c11-b/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c11-b/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c11-b/Strength - unit: m-2 + - srmag/m-sd1/c11-b/Strength_H + - srmag/m-sd1/c11-b/Strength_V + - srmag/m-sd1/c11-b/Strength_SQ + - srmag/m-sd1/c11-b/Strength - type: pyaml.magnet.cfm_magnet name: SH2B-C11 mapping: @@ -1877,27 +1442,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c11-b-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c11-b-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c11-b-ch3/current - unit: A + - srmag/ps-corr-sh2/c11-b-ch1/current + - srmag/ps-corr-sh2/c11-b-ch2/current + - srmag/ps-corr-sh2/c11-b-ch3/current - type: pyaml.magnet.cfm_magnet name: SD1D-C11 mapping: @@ -1910,18 +1470,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c11-d/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c11-d/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c11-d/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c11-d/Strength - unit: m-2 + - srmag/m-sd1/c11-d/Strength_H + - srmag/m-sd1/c11-d/Strength_V + - srmag/m-sd1/c11-d/Strength_SQ + - srmag/m-sd1/c11-d/Strength - type: pyaml.magnet.cfm_magnet name: SF2E-C11 mapping: @@ -1934,18 +1486,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c11-e/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c11-e/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c11-e/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c11-e/Strength - unit: m-2 + - srmag/m-sf2/c11-e/Strength_H + - srmag/m-sf2/c11-e/Strength_V + - srmag/m-sf2/c11-e/Strength_SQ + - srmag/m-sf2/c11-e/Strength - type: pyaml.magnet.cfm_magnet name: SD1E-C11 mapping: @@ -1958,18 +1502,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c11-e/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c11-e/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c11-e/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c11-e/Strength - unit: m-2 + - srmag/m-sd1/c11-e/Strength_H + - srmag/m-sd1/c11-e/Strength_V + - srmag/m-sd1/c11-e/Strength_SQ + - srmag/m-sd1/c11-e/Strength - type: pyaml.magnet.cfm_magnet name: SH3E-C11 mapping: @@ -1980,27 +1516,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c11-e-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c11-e-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c11-e-ch3/current - unit: A + - srmag/ps-corr-sh3/c11-e-ch1/current + - srmag/ps-corr-sh3/c11-e-ch2/current + - srmag/ps-corr-sh3/c11-e-ch3/current - type: pyaml.magnet.cfm_magnet name: SH1A-C12 mapping: @@ -2011,27 +1542,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c12-a-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c12-a-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c12-a-ch3/current - unit: A + - srmag/ps-corr-sh1/c12-a-ch1/current + - srmag/ps-corr-sh1/c12-a-ch2/current + - srmag/ps-corr-sh1/c12-a-ch3/current - type: pyaml.magnet.cfm_magnet name: SD1A-C12 mapping: @@ -2044,18 +1570,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c12-a/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c12-a/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c12-a/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c12-a/Strength - unit: m-2 + - srmag/m-sd1/c12-a/Strength_H + - srmag/m-sd1/c12-a/Strength_V + - srmag/m-sd1/c12-a/Strength_SQ + - srmag/m-sd1/c12-a/Strength - type: pyaml.magnet.cfm_magnet name: SF2A-C12 mapping: @@ -2068,18 +1586,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c12-a/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c12-a/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c12-a/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c12-a/Strength - unit: m-2 + - srmag/m-sf2/c12-a/Strength_H + - srmag/m-sf2/c12-a/Strength_V + - srmag/m-sf2/c12-a/Strength_SQ + - srmag/m-sf2/c12-a/Strength - type: pyaml.magnet.cfm_magnet name: SD1B-C12 mapping: @@ -2092,18 +1602,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c12-b/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c12-b/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c12-b/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c12-b/Strength - unit: m-2 + - srmag/m-sd1/c12-b/Strength_H + - srmag/m-sd1/c12-b/Strength_V + - srmag/m-sd1/c12-b/Strength_SQ + - srmag/m-sd1/c12-b/Strength - type: pyaml.magnet.cfm_magnet name: SH2B-C12 mapping: @@ -2114,27 +1616,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c12-b-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c12-b-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c12-b-ch3/current - unit: A + - srmag/ps-corr-sh2/c12-b-ch1/current + - srmag/ps-corr-sh2/c12-b-ch2/current + - srmag/ps-corr-sh2/c12-b-ch3/current - type: pyaml.magnet.cfm_magnet name: SD1D-C12 mapping: @@ -2147,18 +1644,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c12-d/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c12-d/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c12-d/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c12-d/Strength - unit: m-2 + - srmag/m-sd1/c12-d/Strength_H + - srmag/m-sd1/c12-d/Strength_V + - srmag/m-sd1/c12-d/Strength_SQ + - srmag/m-sd1/c12-d/Strength - type: pyaml.magnet.cfm_magnet name: SF2E-C12 mapping: @@ -2171,18 +1660,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c12-e/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c12-e/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c12-e/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c12-e/Strength - unit: m-2 + - srmag/m-sf2/c12-e/Strength_H + - srmag/m-sf2/c12-e/Strength_V + - srmag/m-sf2/c12-e/Strength_SQ + - srmag/m-sf2/c12-e/Strength - type: pyaml.magnet.cfm_magnet name: SD1E-C12 mapping: @@ -2195,18 +1676,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c12-e/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c12-e/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c12-e/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c12-e/Strength - unit: m-2 + - srmag/m-sd1/c12-e/Strength_H + - srmag/m-sd1/c12-e/Strength_V + - srmag/m-sd1/c12-e/Strength_SQ + - srmag/m-sd1/c12-e/Strength - type: pyaml.magnet.cfm_magnet name: SH3E-C12 mapping: @@ -2217,27 +1690,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c12-e-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c12-e-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c12-e-ch3/current - unit: A + - srmag/ps-corr-sh3/c12-e-ch1/current + - srmag/ps-corr-sh3/c12-e-ch2/current + - srmag/ps-corr-sh3/c12-e-ch3/current - type: pyaml.magnet.cfm_magnet name: SH1A-C13 mapping: @@ -2248,27 +1716,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c13-a-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c13-a-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c13-a-ch3/current - unit: A + - srmag/ps-corr-sh1/c13-a-ch1/current + - srmag/ps-corr-sh1/c13-a-ch2/current + - srmag/ps-corr-sh1/c13-a-ch3/current - type: pyaml.magnet.cfm_magnet name: SD1A-C13 mapping: @@ -2281,18 +1744,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c13-a/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c13-a/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c13-a/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c13-a/Strength - unit: m-2 + - srmag/m-sd1/c13-a/Strength_H + - srmag/m-sd1/c13-a/Strength_V + - srmag/m-sd1/c13-a/Strength_SQ + - srmag/m-sd1/c13-a/Strength - type: pyaml.magnet.cfm_magnet name: SF2A-C13 mapping: @@ -2305,18 +1760,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c13-a/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c13-a/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c13-a/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c13-a/Strength - unit: m-2 + - srmag/m-sf2/c13-a/Strength_H + - srmag/m-sf2/c13-a/Strength_V + - srmag/m-sf2/c13-a/Strength_SQ + - srmag/m-sf2/c13-a/Strength - type: pyaml.magnet.cfm_magnet name: SD1B-C13 mapping: @@ -2329,18 +1776,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c13-b/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c13-b/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c13-b/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c13-b/Strength - unit: m-2 + - srmag/m-sd1/c13-b/Strength_H + - srmag/m-sd1/c13-b/Strength_V + - srmag/m-sd1/c13-b/Strength_SQ + - srmag/m-sd1/c13-b/Strength - type: pyaml.magnet.cfm_magnet name: SH2B-C13 mapping: @@ -2351,27 +1790,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c13-b-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c13-b-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c13-b-ch3/current - unit: A + - srmag/ps-corr-sh2/c13-b-ch1/current + - srmag/ps-corr-sh2/c13-b-ch2/current + - srmag/ps-corr-sh2/c13-b-ch3/current - type: pyaml.magnet.cfm_magnet name: SD1D-C13 mapping: @@ -2384,18 +1818,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c13-d/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c13-d/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c13-d/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c13-d/Strength - unit: m-2 + - srmag/m-sd1/c13-d/Strength_H + - srmag/m-sd1/c13-d/Strength_V + - srmag/m-sd1/c13-d/Strength_SQ + - srmag/m-sd1/c13-d/Strength - type: pyaml.magnet.cfm_magnet name: SF2E-C13 mapping: @@ -2408,18 +1834,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c13-e/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c13-e/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c13-e/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c13-e/Strength - unit: m-2 + - srmag/m-sf2/c13-e/Strength_H + - srmag/m-sf2/c13-e/Strength_V + - srmag/m-sf2/c13-e/Strength_SQ + - srmag/m-sf2/c13-e/Strength - type: pyaml.magnet.cfm_magnet name: SD1E-C13 mapping: @@ -2432,18 +1850,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c13-e/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c13-e/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c13-e/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c13-e/Strength - unit: m-2 + - srmag/m-sd1/c13-e/Strength_H + - srmag/m-sd1/c13-e/Strength_V + - srmag/m-sd1/c13-e/Strength_SQ + - srmag/m-sd1/c13-e/Strength - type: pyaml.magnet.cfm_magnet name: SH3E-C13 mapping: @@ -2454,27 +1864,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c13-e-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c13-e-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c13-e-ch3/current - unit: A + - srmag/ps-corr-sh3/c13-e-ch1/current + - srmag/ps-corr-sh3/c13-e-ch2/current + - srmag/ps-corr-sh3/c13-e-ch3/current - type: pyaml.magnet.cfm_magnet name: SH1A-C14 mapping: @@ -2485,27 +1890,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c14-a-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c14-a-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c14-a-ch3/current - unit: A + - srmag/ps-corr-sh1/c14-a-ch1/current + - srmag/ps-corr-sh1/c14-a-ch2/current + - srmag/ps-corr-sh1/c14-a-ch3/current - type: pyaml.magnet.cfm_magnet name: SD1A-C14 mapping: @@ -2518,18 +1918,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c14-a/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c14-a/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c14-a/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c14-a/Strength - unit: m-2 + - srmag/m-sd1/c14-a/Strength_H + - srmag/m-sd1/c14-a/Strength_V + - srmag/m-sd1/c14-a/Strength_SQ + - srmag/m-sd1/c14-a/Strength - type: pyaml.magnet.cfm_magnet name: SF2A-C14 mapping: @@ -2542,18 +1934,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c14-a/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c14-a/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c14-a/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c14-a/Strength - unit: m-2 + - srmag/m-sf2/c14-a/Strength_H + - srmag/m-sf2/c14-a/Strength_V + - srmag/m-sf2/c14-a/Strength_SQ + - srmag/m-sf2/c14-a/Strength - type: pyaml.magnet.cfm_magnet name: SD1B-C14 mapping: @@ -2566,18 +1950,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c14-b/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c14-b/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c14-b/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c14-b/Strength - unit: m-2 + - srmag/m-sd1/c14-b/Strength_H + - srmag/m-sd1/c14-b/Strength_V + - srmag/m-sd1/c14-b/Strength_SQ + - srmag/m-sd1/c14-b/Strength - type: pyaml.magnet.cfm_magnet name: SH2B-C14 mapping: @@ -2588,27 +1964,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c14-b-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c14-b-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c14-b-ch3/current - unit: A + - srmag/ps-corr-sh2/c14-b-ch1/current + - srmag/ps-corr-sh2/c14-b-ch2/current + - srmag/ps-corr-sh2/c14-b-ch3/current - type: pyaml.magnet.cfm_magnet name: SD1D-C14 mapping: @@ -2621,18 +1992,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c14-d/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c14-d/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c14-d/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c14-d/Strength - unit: m-2 + - srmag/m-sd1/c14-d/Strength_H + - srmag/m-sd1/c14-d/Strength_V + - srmag/m-sd1/c14-d/Strength_SQ + - srmag/m-sd1/c14-d/Strength - type: pyaml.magnet.cfm_magnet name: SF2E-C14 mapping: @@ -2645,18 +2008,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c14-e/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c14-e/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c14-e/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c14-e/Strength - unit: m-2 + - srmag/m-sf2/c14-e/Strength_H + - srmag/m-sf2/c14-e/Strength_V + - srmag/m-sf2/c14-e/Strength_SQ + - srmag/m-sf2/c14-e/Strength - type: pyaml.magnet.cfm_magnet name: SD1E-C14 mapping: @@ -2669,18 +2024,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c14-e/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c14-e/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c14-e/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c14-e/Strength - unit: m-2 + - srmag/m-sd1/c14-e/Strength_H + - srmag/m-sd1/c14-e/Strength_V + - srmag/m-sd1/c14-e/Strength_SQ + - srmag/m-sd1/c14-e/Strength - type: pyaml.magnet.cfm_magnet name: SH3E-C14 mapping: @@ -2691,27 +2038,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c14-e-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c14-e-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c14-e-ch3/current - unit: A + - srmag/ps-corr-sh3/c14-e-ch1/current + - srmag/ps-corr-sh3/c14-e-ch2/current + - srmag/ps-corr-sh3/c14-e-ch3/current - type: pyaml.magnet.cfm_magnet name: SH1A-C15 mapping: @@ -2722,27 +2064,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c15-a-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c15-a-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c15-a-ch3/current - unit: A + - srmag/ps-corr-sh1/c15-a-ch1/current + - srmag/ps-corr-sh1/c15-a-ch2/current + - srmag/ps-corr-sh1/c15-a-ch3/current - type: pyaml.magnet.cfm_magnet name: SD1A-C15 mapping: @@ -2755,18 +2092,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c15-a/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c15-a/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c15-a/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c15-a/Strength - unit: m-2 + - srmag/m-sd1/c15-a/Strength_H + - srmag/m-sd1/c15-a/Strength_V + - srmag/m-sd1/c15-a/Strength_SQ + - srmag/m-sd1/c15-a/Strength - type: pyaml.magnet.cfm_magnet name: SF2A-C15 mapping: @@ -2779,18 +2108,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c15-a/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c15-a/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c15-a/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c15-a/Strength - unit: m-2 + - srmag/m-sf2/c15-a/Strength_H + - srmag/m-sf2/c15-a/Strength_V + - srmag/m-sf2/c15-a/Strength_SQ + - srmag/m-sf2/c15-a/Strength - type: pyaml.magnet.cfm_magnet name: SD1B-C15 mapping: @@ -2803,18 +2124,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c15-b/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c15-b/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c15-b/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c15-b/Strength - unit: m-2 + - srmag/m-sd1/c15-b/Strength_H + - srmag/m-sd1/c15-b/Strength_V + - srmag/m-sd1/c15-b/Strength_SQ + - srmag/m-sd1/c15-b/Strength - type: pyaml.magnet.cfm_magnet name: SH2B-C15 mapping: @@ -2825,27 +2138,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c15-b-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c15-b-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c15-b-ch3/current - unit: A + - srmag/ps-corr-sh2/c15-b-ch1/current + - srmag/ps-corr-sh2/c15-b-ch2/current + - srmag/ps-corr-sh2/c15-b-ch3/current - type: pyaml.magnet.cfm_magnet name: SD1D-C15 mapping: @@ -2858,18 +2166,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c15-d/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c15-d/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c15-d/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c15-d/Strength - unit: m-2 + - srmag/m-sd1/c15-d/Strength_H + - srmag/m-sd1/c15-d/Strength_V + - srmag/m-sd1/c15-d/Strength_SQ + - srmag/m-sd1/c15-d/Strength - type: pyaml.magnet.cfm_magnet name: SF2E-C15 mapping: @@ -2882,18 +2182,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c15-e/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c15-e/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c15-e/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c15-e/Strength - unit: m-2 + - srmag/m-sf2/c15-e/Strength_H + - srmag/m-sf2/c15-e/Strength_V + - srmag/m-sf2/c15-e/Strength_SQ + - srmag/m-sf2/c15-e/Strength - type: pyaml.magnet.cfm_magnet name: SD1E-C15 mapping: @@ -2906,18 +2198,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c15-e/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c15-e/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c15-e/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c15-e/Strength - unit: m-2 + - srmag/m-sd1/c15-e/Strength_H + - srmag/m-sd1/c15-e/Strength_V + - srmag/m-sd1/c15-e/Strength_SQ + - srmag/m-sd1/c15-e/Strength - type: pyaml.magnet.cfm_magnet name: SH3E-C15 mapping: @@ -2928,27 +2212,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c15-e-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c15-e-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c15-e-ch3/current - unit: A + - srmag/ps-corr-sh3/c15-e-ch1/current + - srmag/ps-corr-sh3/c15-e-ch2/current + - srmag/ps-corr-sh3/c15-e-ch3/current - type: pyaml.magnet.cfm_magnet name: SH1A-C16 mapping: @@ -2959,27 +2238,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c16-a-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c16-a-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c16-a-ch3/current - unit: A + - srmag/ps-corr-sh1/c16-a-ch1/current + - srmag/ps-corr-sh1/c16-a-ch2/current + - srmag/ps-corr-sh1/c16-a-ch3/current - type: pyaml.magnet.cfm_magnet name: SD1A-C16 mapping: @@ -2992,18 +2266,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c16-a/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c16-a/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c16-a/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c16-a/Strength - unit: m-2 + - srmag/m-sd1/c16-a/Strength_H + - srmag/m-sd1/c16-a/Strength_V + - srmag/m-sd1/c16-a/Strength_SQ + - srmag/m-sd1/c16-a/Strength - type: pyaml.magnet.cfm_magnet name: SF2A-C16 mapping: @@ -3016,18 +2282,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c16-a/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c16-a/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c16-a/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c16-a/Strength - unit: m-2 + - srmag/m-sf2/c16-a/Strength_H + - srmag/m-sf2/c16-a/Strength_V + - srmag/m-sf2/c16-a/Strength_SQ + - srmag/m-sf2/c16-a/Strength - type: pyaml.magnet.cfm_magnet name: SD1B-C16 mapping: @@ -3040,18 +2298,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c16-b/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c16-b/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c16-b/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c16-b/Strength - unit: m-2 + - srmag/m-sd1/c16-b/Strength_H + - srmag/m-sd1/c16-b/Strength_V + - srmag/m-sd1/c16-b/Strength_SQ + - srmag/m-sd1/c16-b/Strength - type: pyaml.magnet.cfm_magnet name: SH2B-C16 mapping: @@ -3062,27 +2312,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c16-b-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c16-b-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c16-b-ch3/current - unit: A + - srmag/ps-corr-sh2/c16-b-ch1/current + - srmag/ps-corr-sh2/c16-b-ch2/current + - srmag/ps-corr-sh2/c16-b-ch3/current - type: pyaml.magnet.cfm_magnet name: SD1D-C16 mapping: @@ -3095,18 +2340,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c16-d/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c16-d/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c16-d/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c16-d/Strength - unit: m-2 + - srmag/m-sd1/c16-d/Strength_H + - srmag/m-sd1/c16-d/Strength_V + - srmag/m-sd1/c16-d/Strength_SQ + - srmag/m-sd1/c16-d/Strength - type: pyaml.magnet.cfm_magnet name: SF2E-C16 mapping: @@ -3119,18 +2356,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c16-e/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c16-e/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c16-e/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c16-e/Strength - unit: m-2 + - srmag/m-sf2/c16-e/Strength_H + - srmag/m-sf2/c16-e/Strength_V + - srmag/m-sf2/c16-e/Strength_SQ + - srmag/m-sf2/c16-e/Strength - type: pyaml.magnet.cfm_magnet name: SD1E-C16 mapping: @@ -3143,18 +2372,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c16-e/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c16-e/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c16-e/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c16-e/Strength - unit: m-2 + - srmag/m-sd1/c16-e/Strength_H + - srmag/m-sd1/c16-e/Strength_V + - srmag/m-sd1/c16-e/Strength_SQ + - srmag/m-sd1/c16-e/Strength - type: pyaml.magnet.cfm_magnet name: SH3E-C16 mapping: @@ -3165,27 +2386,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c16-e-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c16-e-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c16-e-ch3/current - unit: A + - srmag/ps-corr-sh3/c16-e-ch1/current + - srmag/ps-corr-sh3/c16-e-ch2/current + - srmag/ps-corr-sh3/c16-e-ch3/current - type: pyaml.magnet.cfm_magnet name: SH1A-C17 mapping: @@ -3196,27 +2412,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c17-a-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c17-a-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c17-a-ch3/current - unit: A + - srmag/ps-corr-sh1/c17-a-ch1/current + - srmag/ps-corr-sh1/c17-a-ch2/current + - srmag/ps-corr-sh1/c17-a-ch3/current - type: pyaml.magnet.cfm_magnet name: SD1A-C17 mapping: @@ -3229,18 +2440,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c17-a/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c17-a/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c17-a/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c17-a/Strength - unit: m-2 + - srmag/m-sd1/c17-a/Strength_H + - srmag/m-sd1/c17-a/Strength_V + - srmag/m-sd1/c17-a/Strength_SQ + - srmag/m-sd1/c17-a/Strength - type: pyaml.magnet.cfm_magnet name: SF2A-C17 mapping: @@ -3253,18 +2456,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c17-a/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c17-a/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c17-a/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c17-a/Strength - unit: m-2 + - srmag/m-sf2/c17-a/Strength_H + - srmag/m-sf2/c17-a/Strength_V + - srmag/m-sf2/c17-a/Strength_SQ + - srmag/m-sf2/c17-a/Strength - type: pyaml.magnet.cfm_magnet name: SD1B-C17 mapping: @@ -3277,18 +2472,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c17-b/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c17-b/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c17-b/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c17-b/Strength - unit: m-2 + - srmag/m-sd1/c17-b/Strength_H + - srmag/m-sd1/c17-b/Strength_V + - srmag/m-sd1/c17-b/Strength_SQ + - srmag/m-sd1/c17-b/Strength - type: pyaml.magnet.cfm_magnet name: SH2B-C17 mapping: @@ -3299,27 +2486,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c17-b-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c17-b-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c17-b-ch3/current - unit: A + - srmag/ps-corr-sh2/c17-b-ch1/current + - srmag/ps-corr-sh2/c17-b-ch2/current + - srmag/ps-corr-sh2/c17-b-ch3/current - type: pyaml.magnet.cfm_magnet name: SD1D-C17 mapping: @@ -3332,18 +2514,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c17-d/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c17-d/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c17-d/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c17-d/Strength - unit: m-2 + - srmag/m-sd1/c17-d/Strength_H + - srmag/m-sd1/c17-d/Strength_V + - srmag/m-sd1/c17-d/Strength_SQ + - srmag/m-sd1/c17-d/Strength - type: pyaml.magnet.cfm_magnet name: SF2E-C17 mapping: @@ -3356,18 +2530,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c17-e/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c17-e/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c17-e/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c17-e/Strength - unit: m-2 + - srmag/m-sf2/c17-e/Strength_H + - srmag/m-sf2/c17-e/Strength_V + - srmag/m-sf2/c17-e/Strength_SQ + - srmag/m-sf2/c17-e/Strength - type: pyaml.magnet.cfm_magnet name: SD1E-C17 mapping: @@ -3380,18 +2546,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c17-e/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c17-e/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c17-e/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c17-e/Strength - unit: m-2 + - srmag/m-sd1/c17-e/Strength_H + - srmag/m-sd1/c17-e/Strength_V + - srmag/m-sd1/c17-e/Strength_SQ + - srmag/m-sd1/c17-e/Strength - type: pyaml.magnet.cfm_magnet name: SH3E-C17 mapping: @@ -3402,27 +2560,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c17-e-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c17-e-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c17-e-ch3/current - unit: A + - srmag/ps-corr-sh3/c17-e-ch1/current + - srmag/ps-corr-sh3/c17-e-ch2/current + - srmag/ps-corr-sh3/c17-e-ch3/current - type: pyaml.magnet.cfm_magnet name: SH1A-C18 mapping: @@ -3433,27 +2586,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c18-a-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c18-a-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c18-a-ch3/current - unit: A + - srmag/ps-corr-sh1/c18-a-ch1/current + - srmag/ps-corr-sh1/c18-a-ch2/current + - srmag/ps-corr-sh1/c18-a-ch3/current - type: pyaml.magnet.cfm_magnet name: SD1A-C18 mapping: @@ -3466,18 +2614,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c18-a/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c18-a/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c18-a/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c18-a/Strength - unit: m-2 + - srmag/m-sd1/c18-a/Strength_H + - srmag/m-sd1/c18-a/Strength_V + - srmag/m-sd1/c18-a/Strength_SQ + - srmag/m-sd1/c18-a/Strength - type: pyaml.magnet.cfm_magnet name: SF2A-C18 mapping: @@ -3490,18 +2630,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c18-a/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c18-a/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c18-a/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c18-a/Strength - unit: m-2 + - srmag/m-sf2/c18-a/Strength_H + - srmag/m-sf2/c18-a/Strength_V + - srmag/m-sf2/c18-a/Strength_SQ + - srmag/m-sf2/c18-a/Strength - type: pyaml.magnet.cfm_magnet name: SD1B-C18 mapping: @@ -3514,18 +2646,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c18-b/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c18-b/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c18-b/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c18-b/Strength - unit: m-2 + - srmag/m-sd1/c18-b/Strength_H + - srmag/m-sd1/c18-b/Strength_V + - srmag/m-sd1/c18-b/Strength_SQ + - srmag/m-sd1/c18-b/Strength - type: pyaml.magnet.cfm_magnet name: SH2B-C18 mapping: @@ -3536,27 +2660,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c18-b-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c18-b-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c18-b-ch3/current - unit: A + - srmag/ps-corr-sh2/c18-b-ch1/current + - srmag/ps-corr-sh2/c18-b-ch2/current + - srmag/ps-corr-sh2/c18-b-ch3/current - type: pyaml.magnet.cfm_magnet name: SD1D-C18 mapping: @@ -3569,18 +2688,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c18-d/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c18-d/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c18-d/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c18-d/Strength - unit: m-2 + - srmag/m-sd1/c18-d/Strength_H + - srmag/m-sd1/c18-d/Strength_V + - srmag/m-sd1/c18-d/Strength_SQ + - srmag/m-sd1/c18-d/Strength - type: pyaml.magnet.cfm_magnet name: SF2E-C18 mapping: @@ -3593,18 +2704,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c18-e/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c18-e/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c18-e/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c18-e/Strength - unit: m-2 + - srmag/m-sf2/c18-e/Strength_H + - srmag/m-sf2/c18-e/Strength_V + - srmag/m-sf2/c18-e/Strength_SQ + - srmag/m-sf2/c18-e/Strength - type: pyaml.magnet.cfm_magnet name: SD1E-C18 mapping: @@ -3617,18 +2720,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c18-e/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c18-e/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c18-e/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c18-e/Strength - unit: m-2 + - srmag/m-sd1/c18-e/Strength_H + - srmag/m-sd1/c18-e/Strength_V + - srmag/m-sd1/c18-e/Strength_SQ + - srmag/m-sd1/c18-e/Strength - type: pyaml.magnet.cfm_magnet name: SH3E-C18 mapping: @@ -3639,27 +2734,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c18-e-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c18-e-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c18-e-ch3/current - unit: A + - srmag/ps-corr-sh3/c18-e-ch1/current + - srmag/ps-corr-sh3/c18-e-ch2/current + - srmag/ps-corr-sh3/c18-e-ch3/current - type: pyaml.magnet.cfm_magnet name: SH1A-C19 mapping: @@ -3670,27 +2760,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c19-a-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c19-a-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c19-a-ch3/current - unit: A + - srmag/ps-corr-sh1/c19-a-ch1/current + - srmag/ps-corr-sh1/c19-a-ch2/current + - srmag/ps-corr-sh1/c19-a-ch3/current - type: pyaml.magnet.cfm_magnet name: SD1A-C19 mapping: @@ -3703,18 +2788,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c19-a/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c19-a/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c19-a/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c19-a/Strength - unit: m-2 + - srmag/m-sd1/c19-a/Strength_H + - srmag/m-sd1/c19-a/Strength_V + - srmag/m-sd1/c19-a/Strength_SQ + - srmag/m-sd1/c19-a/Strength - type: pyaml.magnet.cfm_magnet name: SF2A-C19 mapping: @@ -3727,18 +2804,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c19-a/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c19-a/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c19-a/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c19-a/Strength - unit: m-2 + - srmag/m-sf2/c19-a/Strength_H + - srmag/m-sf2/c19-a/Strength_V + - srmag/m-sf2/c19-a/Strength_SQ + - srmag/m-sf2/c19-a/Strength - type: pyaml.magnet.cfm_magnet name: SD1B-C19 mapping: @@ -3751,18 +2820,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c19-b/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c19-b/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c19-b/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c19-b/Strength - unit: m-2 + - srmag/m-sd1/c19-b/Strength_H + - srmag/m-sd1/c19-b/Strength_V + - srmag/m-sd1/c19-b/Strength_SQ + - srmag/m-sd1/c19-b/Strength - type: pyaml.magnet.cfm_magnet name: SH2B-C19 mapping: @@ -3773,27 +2834,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c19-b-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c19-b-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c19-b-ch3/current - unit: A + - srmag/ps-corr-sh2/c19-b-ch1/current + - srmag/ps-corr-sh2/c19-b-ch2/current + - srmag/ps-corr-sh2/c19-b-ch3/current - type: pyaml.magnet.cfm_magnet name: SD1D-C19 mapping: @@ -3806,18 +2862,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c19-d/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c19-d/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c19-d/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c19-d/Strength - unit: m-2 + - srmag/m-sd1/c19-d/Strength_H + - srmag/m-sd1/c19-d/Strength_V + - srmag/m-sd1/c19-d/Strength_SQ + - srmag/m-sd1/c19-d/Strength - type: pyaml.magnet.cfm_magnet name: SF2E-C19 mapping: @@ -3830,18 +2878,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c19-e/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c19-e/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c19-e/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c19-e/Strength - unit: m-2 + - srmag/m-sf2/c19-e/Strength_H + - srmag/m-sf2/c19-e/Strength_V + - srmag/m-sf2/c19-e/Strength_SQ + - srmag/m-sf2/c19-e/Strength - type: pyaml.magnet.cfm_magnet name: SD1E-C19 mapping: @@ -3854,18 +2894,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c19-e/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c19-e/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c19-e/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c19-e/Strength - unit: m-2 + - srmag/m-sd1/c19-e/Strength_H + - srmag/m-sd1/c19-e/Strength_V + - srmag/m-sd1/c19-e/Strength_SQ + - srmag/m-sd1/c19-e/Strength - type: pyaml.magnet.cfm_magnet name: SH3E-C19 mapping: @@ -3876,27 +2908,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c19-e-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c19-e-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c19-e-ch3/current - unit: A + - srmag/ps-corr-sh3/c19-e-ch1/current + - srmag/ps-corr-sh3/c19-e-ch2/current + - srmag/ps-corr-sh3/c19-e-ch3/current - type: pyaml.magnet.cfm_magnet name: SH1A-C20 mapping: @@ -3907,27 +2934,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c20-a-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c20-a-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c20-a-ch3/current - unit: A + - srmag/ps-corr-sh1/c20-a-ch1/current + - srmag/ps-corr-sh1/c20-a-ch2/current + - srmag/ps-corr-sh1/c20-a-ch3/current - type: pyaml.magnet.cfm_magnet name: SD1A-C20 mapping: @@ -3940,18 +2962,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c20-a/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c20-a/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c20-a/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c20-a/Strength - unit: m-2 + - srmag/m-sd1/c20-a/Strength_H + - srmag/m-sd1/c20-a/Strength_V + - srmag/m-sd1/c20-a/Strength_SQ + - srmag/m-sd1/c20-a/Strength - type: pyaml.magnet.cfm_magnet name: SF2A-C20 mapping: @@ -3964,18 +2978,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c20-a/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c20-a/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c20-a/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c20-a/Strength - unit: m-2 + - srmag/m-sf2/c20-a/Strength_H + - srmag/m-sf2/c20-a/Strength_V + - srmag/m-sf2/c20-a/Strength_SQ + - srmag/m-sf2/c20-a/Strength - type: pyaml.magnet.cfm_magnet name: SD1B-C20 mapping: @@ -3988,18 +2994,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c20-b/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c20-b/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c20-b/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c20-b/Strength - unit: m-2 + - srmag/m-sd1/c20-b/Strength_H + - srmag/m-sd1/c20-b/Strength_V + - srmag/m-sd1/c20-b/Strength_SQ + - srmag/m-sd1/c20-b/Strength - type: pyaml.magnet.cfm_magnet name: SH2B-C20 mapping: @@ -4010,27 +3008,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c20-b-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c20-b-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c20-b-ch3/current - unit: A + - srmag/ps-corr-sh2/c20-b-ch1/current + - srmag/ps-corr-sh2/c20-b-ch2/current + - srmag/ps-corr-sh2/c20-b-ch3/current - type: pyaml.magnet.cfm_magnet name: SD1D-C20 mapping: @@ -4043,18 +3036,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c20-d/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c20-d/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c20-d/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c20-d/Strength - unit: m-2 + - srmag/m-sd1/c20-d/Strength_H + - srmag/m-sd1/c20-d/Strength_V + - srmag/m-sd1/c20-d/Strength_SQ + - srmag/m-sd1/c20-d/Strength - type: pyaml.magnet.cfm_magnet name: SF2E-C20 mapping: @@ -4067,18 +3052,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c20-e/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c20-e/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c20-e/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c20-e/Strength - unit: m-2 + - srmag/m-sf2/c20-e/Strength_H + - srmag/m-sf2/c20-e/Strength_V + - srmag/m-sf2/c20-e/Strength_SQ + - srmag/m-sf2/c20-e/Strength - type: pyaml.magnet.cfm_magnet name: SD1E-C20 mapping: @@ -4091,18 +3068,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c20-e/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c20-e/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c20-e/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c20-e/Strength - unit: m-2 + - srmag/m-sd1/c20-e/Strength_H + - srmag/m-sd1/c20-e/Strength_V + - srmag/m-sd1/c20-e/Strength_SQ + - srmag/m-sd1/c20-e/Strength - type: pyaml.magnet.cfm_magnet name: SH3E-C20 mapping: @@ -4113,27 +3082,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c20-e-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c20-e-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c20-e-ch3/current - unit: A + - srmag/ps-corr-sh3/c20-e-ch1/current + - srmag/ps-corr-sh3/c20-e-ch2/current + - srmag/ps-corr-sh3/c20-e-ch3/current - type: pyaml.magnet.cfm_magnet name: SH1A-C21 mapping: @@ -4144,27 +3108,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c21-a-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c21-a-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c21-a-ch3/current - unit: A + - srmag/ps-corr-sh1/c21-a-ch1/current + - srmag/ps-corr-sh1/c21-a-ch2/current + - srmag/ps-corr-sh1/c21-a-ch3/current - type: pyaml.magnet.cfm_magnet name: SD1A-C21 mapping: @@ -4177,18 +3136,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c21-a/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c21-a/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c21-a/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c21-a/Strength - unit: m-2 + - srmag/m-sd1/c21-a/Strength_H + - srmag/m-sd1/c21-a/Strength_V + - srmag/m-sd1/c21-a/Strength_SQ + - srmag/m-sd1/c21-a/Strength - type: pyaml.magnet.cfm_magnet name: SF2A-C21 mapping: @@ -4201,18 +3152,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c21-a/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c21-a/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c21-a/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c21-a/Strength - unit: m-2 + - srmag/m-sf2/c21-a/Strength_H + - srmag/m-sf2/c21-a/Strength_V + - srmag/m-sf2/c21-a/Strength_SQ + - srmag/m-sf2/c21-a/Strength - type: pyaml.magnet.cfm_magnet name: SD1B-C21 mapping: @@ -4225,18 +3168,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c21-b/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c21-b/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c21-b/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c21-b/Strength - unit: m-2 + - srmag/m-sd1/c21-b/Strength_H + - srmag/m-sd1/c21-b/Strength_V + - srmag/m-sd1/c21-b/Strength_SQ + - srmag/m-sd1/c21-b/Strength - type: pyaml.magnet.cfm_magnet name: SH2B-C21 mapping: @@ -4247,27 +3182,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c21-b-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c21-b-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c21-b-ch3/current - unit: A + - srmag/ps-corr-sh2/c21-b-ch1/current + - srmag/ps-corr-sh2/c21-b-ch2/current + - srmag/ps-corr-sh2/c21-b-ch3/current - type: pyaml.magnet.cfm_magnet name: SD1D-C21 mapping: @@ -4280,18 +3210,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c21-d/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c21-d/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c21-d/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c21-d/Strength - unit: m-2 + - srmag/m-sd1/c21-d/Strength_H + - srmag/m-sd1/c21-d/Strength_V + - srmag/m-sd1/c21-d/Strength_SQ + - srmag/m-sd1/c21-d/Strength - type: pyaml.magnet.cfm_magnet name: SF2E-C21 mapping: @@ -4304,18 +3226,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c21-e/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c21-e/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c21-e/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c21-e/Strength - unit: m-2 + - srmag/m-sf2/c21-e/Strength_H + - srmag/m-sf2/c21-e/Strength_V + - srmag/m-sf2/c21-e/Strength_SQ + - srmag/m-sf2/c21-e/Strength - type: pyaml.magnet.cfm_magnet name: SD1E-C21 mapping: @@ -4328,18 +3242,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c21-e/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c21-e/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c21-e/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c21-e/Strength - unit: m-2 + - srmag/m-sd1/c21-e/Strength_H + - srmag/m-sd1/c21-e/Strength_V + - srmag/m-sd1/c21-e/Strength_SQ + - srmag/m-sd1/c21-e/Strength - type: pyaml.magnet.cfm_magnet name: SH3E-C21 mapping: @@ -4350,27 +3256,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c21-e-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c21-e-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c21-e-ch3/current - unit: A + - srmag/ps-corr-sh3/c21-e-ch1/current + - srmag/ps-corr-sh3/c21-e-ch2/current + - srmag/ps-corr-sh3/c21-e-ch3/current - type: pyaml.magnet.cfm_magnet name: SH1A-C22 mapping: @@ -4381,27 +3282,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c22-a-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c22-a-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c22-a-ch3/current - unit: A + - srmag/ps-corr-sh1/c22-a-ch1/current + - srmag/ps-corr-sh1/c22-a-ch2/current + - srmag/ps-corr-sh1/c22-a-ch3/current - type: pyaml.magnet.cfm_magnet name: SD1A-C22 mapping: @@ -4414,18 +3310,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c22-a/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c22-a/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c22-a/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c22-a/Strength - unit: m-2 + - srmag/m-sd1/c22-a/Strength_H + - srmag/m-sd1/c22-a/Strength_V + - srmag/m-sd1/c22-a/Strength_SQ + - srmag/m-sd1/c22-a/Strength - type: pyaml.magnet.cfm_magnet name: SF2A-C22 mapping: @@ -4438,18 +3326,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c22-a/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c22-a/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c22-a/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c22-a/Strength - unit: m-2 + - srmag/m-sf2/c22-a/Strength_H + - srmag/m-sf2/c22-a/Strength_V + - srmag/m-sf2/c22-a/Strength_SQ + - srmag/m-sf2/c22-a/Strength - type: pyaml.magnet.cfm_magnet name: SD1B-C22 mapping: @@ -4462,18 +3342,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c22-b/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c22-b/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c22-b/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c22-b/Strength - unit: m-2 + - srmag/m-sd1/c22-b/Strength_H + - srmag/m-sd1/c22-b/Strength_V + - srmag/m-sd1/c22-b/Strength_SQ + - srmag/m-sd1/c22-b/Strength - type: pyaml.magnet.cfm_magnet name: SH2B-C22 mapping: @@ -4484,27 +3356,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c22-b-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c22-b-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c22-b-ch3/current - unit: A + - srmag/ps-corr-sh2/c22-b-ch1/current + - srmag/ps-corr-sh2/c22-b-ch2/current + - srmag/ps-corr-sh2/c22-b-ch3/current - type: pyaml.magnet.cfm_magnet name: SD1D-C22 mapping: @@ -4517,18 +3384,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c22-d/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c22-d/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c22-d/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c22-d/Strength - unit: m-2 + - srmag/m-sd1/c22-d/Strength_H + - srmag/m-sd1/c22-d/Strength_V + - srmag/m-sd1/c22-d/Strength_SQ + - srmag/m-sd1/c22-d/Strength - type: pyaml.magnet.cfm_magnet name: SF2E-C22 mapping: @@ -4541,18 +3400,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c22-e/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c22-e/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c22-e/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c22-e/Strength - unit: m-2 + - srmag/m-sf2/c22-e/Strength_H + - srmag/m-sf2/c22-e/Strength_V + - srmag/m-sf2/c22-e/Strength_SQ + - srmag/m-sf2/c22-e/Strength - type: pyaml.magnet.cfm_magnet name: SD1E-C22 mapping: @@ -4565,18 +3416,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c22-e/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c22-e/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c22-e/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c22-e/Strength - unit: m-2 + - srmag/m-sd1/c22-e/Strength_H + - srmag/m-sd1/c22-e/Strength_V + - srmag/m-sd1/c22-e/Strength_SQ + - srmag/m-sd1/c22-e/Strength - type: pyaml.magnet.cfm_magnet name: SH3E-C22 mapping: @@ -4587,27 +3430,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c22-e-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c22-e-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c22-e-ch3/current - unit: A + - srmag/ps-corr-sh3/c22-e-ch1/current + - srmag/ps-corr-sh3/c22-e-ch2/current + - srmag/ps-corr-sh3/c22-e-ch3/current - type: pyaml.magnet.cfm_magnet name: SH1A-C23 mapping: @@ -4618,27 +3456,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c23-a-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c23-a-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c23-a-ch3/current - unit: A + - srmag/ps-corr-sh1/c23-a-ch1/current + - srmag/ps-corr-sh1/c23-a-ch2/current + - srmag/ps-corr-sh1/c23-a-ch3/current - type: pyaml.magnet.cfm_magnet name: SD1A-C23 mapping: @@ -4651,18 +3484,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c23-a/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c23-a/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c23-a/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c23-a/Strength - unit: m-2 + - srmag/m-sd1/c23-a/Strength_H + - srmag/m-sd1/c23-a/Strength_V + - srmag/m-sd1/c23-a/Strength_SQ + - srmag/m-sd1/c23-a/Strength - type: pyaml.magnet.cfm_magnet name: SF2A-C23 mapping: @@ -4675,18 +3500,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c23-a/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c23-a/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c23-a/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c23-a/Strength - unit: m-2 + - srmag/m-sf2/c23-a/Strength_H + - srmag/m-sf2/c23-a/Strength_V + - srmag/m-sf2/c23-a/Strength_SQ + - srmag/m-sf2/c23-a/Strength - type: pyaml.magnet.cfm_magnet name: SD1B-C23 mapping: @@ -4699,18 +3516,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c23-b/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c23-b/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c23-b/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c23-b/Strength - unit: m-2 + - srmag/m-sd1/c23-b/Strength_H + - srmag/m-sd1/c23-b/Strength_V + - srmag/m-sd1/c23-b/Strength_SQ + - srmag/m-sd1/c23-b/Strength - type: pyaml.magnet.cfm_magnet name: SH2B-C23 mapping: @@ -4721,27 +3530,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c23-b-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c23-b-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c23-b-ch3/current - unit: A + - srmag/ps-corr-sh2/c23-b-ch1/current + - srmag/ps-corr-sh2/c23-b-ch2/current + - srmag/ps-corr-sh2/c23-b-ch3/current - type: pyaml.magnet.cfm_magnet name: SD1D-C23 mapping: @@ -4754,18 +3558,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c23-d/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c23-d/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c23-d/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c23-d/Strength - unit: m-2 + - srmag/m-sd1/c23-d/Strength_H + - srmag/m-sd1/c23-d/Strength_V + - srmag/m-sd1/c23-d/Strength_SQ + - srmag/m-sd1/c23-d/Strength - type: pyaml.magnet.cfm_magnet name: SF2E-C23 mapping: @@ -4778,18 +3574,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c23-e/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c23-e/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c23-e/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c23-e/Strength - unit: m-2 + - srmag/m-sf2/c23-e/Strength_H + - srmag/m-sf2/c23-e/Strength_V + - srmag/m-sf2/c23-e/Strength_SQ + - srmag/m-sf2/c23-e/Strength - type: pyaml.magnet.cfm_magnet name: SD1E-C23 mapping: @@ -4802,18 +3590,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c23-e/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c23-e/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c23-e/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c23-e/Strength - unit: m-2 + - srmag/m-sd1/c23-e/Strength_H + - srmag/m-sd1/c23-e/Strength_V + - srmag/m-sd1/c23-e/Strength_SQ + - srmag/m-sd1/c23-e/Strength - type: pyaml.magnet.cfm_magnet name: SH3E-C23 mapping: @@ -4824,27 +3604,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c23-e-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c23-e-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c23-e-ch3/current - unit: A + - srmag/ps-corr-sh3/c23-e-ch1/current + - srmag/ps-corr-sh3/c23-e-ch2/current + - srmag/ps-corr-sh3/c23-e-ch3/current - type: pyaml.magnet.cfm_magnet name: SH1A-C24 mapping: @@ -4855,27 +3630,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c24-a-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c24-a-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c24-a-ch3/current - unit: A + - srmag/ps-corr-sh1/c24-a-ch1/current + - srmag/ps-corr-sh1/c24-a-ch2/current + - srmag/ps-corr-sh1/c24-a-ch3/current - type: pyaml.magnet.cfm_magnet name: SD1A-C24 mapping: @@ -4888,18 +3658,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c24-a/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c24-a/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c24-a/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c24-a/Strength - unit: m-2 + - srmag/m-sd1/c24-a/Strength_H + - srmag/m-sd1/c24-a/Strength_V + - srmag/m-sd1/c24-a/Strength_SQ + - srmag/m-sd1/c24-a/Strength - type: pyaml.magnet.cfm_magnet name: SF2A-C24 mapping: @@ -4912,18 +3674,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c24-a/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c24-a/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c24-a/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c24-a/Strength - unit: m-2 + - srmag/m-sf2/c24-a/Strength_H + - srmag/m-sf2/c24-a/Strength_V + - srmag/m-sf2/c24-a/Strength_SQ + - srmag/m-sf2/c24-a/Strength - type: pyaml.magnet.cfm_magnet name: SD1B-C24 mapping: @@ -4936,18 +3690,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c24-b/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c24-b/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c24-b/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c24-b/Strength - unit: m-2 + - srmag/m-sd1/c24-b/Strength_H + - srmag/m-sd1/c24-b/Strength_V + - srmag/m-sd1/c24-b/Strength_SQ + - srmag/m-sd1/c24-b/Strength - type: pyaml.magnet.cfm_magnet name: SH2B-C24 mapping: @@ -4958,27 +3704,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c24-b-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c24-b-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c24-b-ch3/current - unit: A + - srmag/ps-corr-sh2/c24-b-ch1/current + - srmag/ps-corr-sh2/c24-b-ch2/current + - srmag/ps-corr-sh2/c24-b-ch3/current - type: pyaml.magnet.cfm_magnet name: SD1D-C24 mapping: @@ -4991,18 +3732,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c24-d/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c24-d/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c24-d/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c24-d/Strength - unit: m-2 + - srmag/m-sd1/c24-d/Strength_H + - srmag/m-sd1/c24-d/Strength_V + - srmag/m-sd1/c24-d/Strength_SQ + - srmag/m-sd1/c24-d/Strength - type: pyaml.magnet.cfm_magnet name: SF2E-C24 mapping: @@ -5015,18 +3748,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c24-e/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c24-e/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c24-e/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c24-e/Strength - unit: m-2 + - srmag/m-sf2/c24-e/Strength_H + - srmag/m-sf2/c24-e/Strength_V + - srmag/m-sf2/c24-e/Strength_SQ + - srmag/m-sf2/c24-e/Strength - type: pyaml.magnet.cfm_magnet name: SD1E-C24 mapping: @@ -5039,18 +3764,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c24-e/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c24-e/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c24-e/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c24-e/Strength - unit: m-2 + - srmag/m-sd1/c24-e/Strength_H + - srmag/m-sd1/c24-e/Strength_V + - srmag/m-sd1/c24-e/Strength_SQ + - srmag/m-sd1/c24-e/Strength - type: pyaml.magnet.cfm_magnet name: SH3E-C24 mapping: @@ -5061,27 +3778,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c24-e-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c24-e-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c24-e-ch3/current - unit: A + - srmag/ps-corr-sh3/c24-e-ch1/current + - srmag/ps-corr-sh3/c24-e-ch2/current + - srmag/ps-corr-sh3/c24-e-ch3/current - type: pyaml.magnet.cfm_magnet name: SH1A-C25 mapping: @@ -5092,27 +3804,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c25-a-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c25-a-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c25-a-ch3/current - unit: A + - srmag/ps-corr-sh1/c25-a-ch1/current + - srmag/ps-corr-sh1/c25-a-ch2/current + - srmag/ps-corr-sh1/c25-a-ch3/current - type: pyaml.magnet.cfm_magnet name: SD1A-C25 mapping: @@ -5125,18 +3832,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c25-a/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c25-a/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c25-a/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c25-a/Strength - unit: m-2 + - srmag/m-sd1/c25-a/Strength_H + - srmag/m-sd1/c25-a/Strength_V + - srmag/m-sd1/c25-a/Strength_SQ + - srmag/m-sd1/c25-a/Strength - type: pyaml.magnet.cfm_magnet name: SF2A-C25 mapping: @@ -5149,18 +3848,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c25-a/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c25-a/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c25-a/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c25-a/Strength - unit: m-2 + - srmag/m-sf2/c25-a/Strength_H + - srmag/m-sf2/c25-a/Strength_V + - srmag/m-sf2/c25-a/Strength_SQ + - srmag/m-sf2/c25-a/Strength - type: pyaml.magnet.cfm_magnet name: SD1B-C25 mapping: @@ -5173,18 +3864,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c25-b/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c25-b/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c25-b/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c25-b/Strength - unit: m-2 + - srmag/m-sd1/c25-b/Strength_H + - srmag/m-sd1/c25-b/Strength_V + - srmag/m-sd1/c25-b/Strength_SQ + - srmag/m-sd1/c25-b/Strength - type: pyaml.magnet.cfm_magnet name: SH2B-C25 mapping: @@ -5195,27 +3878,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c25-b-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c25-b-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c25-b-ch3/current - unit: A + - srmag/ps-corr-sh2/c25-b-ch1/current + - srmag/ps-corr-sh2/c25-b-ch2/current + - srmag/ps-corr-sh2/c25-b-ch3/current - type: pyaml.magnet.cfm_magnet name: SD1D-C25 mapping: @@ -5228,18 +3906,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c25-d/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c25-d/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c25-d/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c25-d/Strength - unit: m-2 + - srmag/m-sd1/c25-d/Strength_H + - srmag/m-sd1/c25-d/Strength_V + - srmag/m-sd1/c25-d/Strength_SQ + - srmag/m-sd1/c25-d/Strength - type: pyaml.magnet.cfm_magnet name: SF2E-C25 mapping: @@ -5252,18 +3922,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c25-e/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c25-e/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c25-e/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c25-e/Strength - unit: m-2 + - srmag/m-sf2/c25-e/Strength_H + - srmag/m-sf2/c25-e/Strength_V + - srmag/m-sf2/c25-e/Strength_SQ + - srmag/m-sf2/c25-e/Strength - type: pyaml.magnet.cfm_magnet name: SD1E-C25 mapping: @@ -5276,18 +3938,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c25-e/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c25-e/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c25-e/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c25-e/Strength - unit: m-2 + - srmag/m-sd1/c25-e/Strength_H + - srmag/m-sd1/c25-e/Strength_V + - srmag/m-sd1/c25-e/Strength_SQ + - srmag/m-sd1/c25-e/Strength - type: pyaml.magnet.cfm_magnet name: SH3E-C25 mapping: @@ -5298,27 +3952,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c25-e-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c25-e-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c25-e-ch3/current - unit: A + - srmag/ps-corr-sh3/c25-e-ch1/current + - srmag/ps-corr-sh3/c25-e-ch2/current + - srmag/ps-corr-sh3/c25-e-ch3/current - type: pyaml.magnet.cfm_magnet name: SH1A-C26 mapping: @@ -5329,27 +3978,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c26-a-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c26-a-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c26-a-ch3/current - unit: A + - srmag/ps-corr-sh1/c26-a-ch1/current + - srmag/ps-corr-sh1/c26-a-ch2/current + - srmag/ps-corr-sh1/c26-a-ch3/current - type: pyaml.magnet.cfm_magnet name: SD1A-C26 mapping: @@ -5362,18 +4006,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c26-a/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c26-a/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c26-a/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c26-a/Strength - unit: m-2 + - srmag/m-sd1/c26-a/Strength_H + - srmag/m-sd1/c26-a/Strength_V + - srmag/m-sd1/c26-a/Strength_SQ + - srmag/m-sd1/c26-a/Strength - type: pyaml.magnet.cfm_magnet name: SF2A-C26 mapping: @@ -5386,18 +4022,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c26-a/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c26-a/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c26-a/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c26-a/Strength - unit: m-2 + - srmag/m-sf2/c26-a/Strength_H + - srmag/m-sf2/c26-a/Strength_V + - srmag/m-sf2/c26-a/Strength_SQ + - srmag/m-sf2/c26-a/Strength - type: pyaml.magnet.cfm_magnet name: SD1B-C26 mapping: @@ -5410,18 +4038,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c26-b/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c26-b/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c26-b/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c26-b/Strength - unit: m-2 + - srmag/m-sd1/c26-b/Strength_H + - srmag/m-sd1/c26-b/Strength_V + - srmag/m-sd1/c26-b/Strength_SQ + - srmag/m-sd1/c26-b/Strength - type: pyaml.magnet.cfm_magnet name: SH2B-C26 mapping: @@ -5432,27 +4052,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c26-b-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c26-b-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c26-b-ch3/current - unit: A + - srmag/ps-corr-sh2/c26-b-ch1/current + - srmag/ps-corr-sh2/c26-b-ch2/current + - srmag/ps-corr-sh2/c26-b-ch3/current - type: pyaml.magnet.cfm_magnet name: SD1D-C26 mapping: @@ -5465,18 +4080,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c26-d/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c26-d/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c26-d/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c26-d/Strength - unit: m-2 + - srmag/m-sd1/c26-d/Strength_H + - srmag/m-sd1/c26-d/Strength_V + - srmag/m-sd1/c26-d/Strength_SQ + - srmag/m-sd1/c26-d/Strength - type: pyaml.magnet.cfm_magnet name: SF2E-C26 mapping: @@ -5489,18 +4096,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c26-e/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c26-e/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c26-e/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c26-e/Strength - unit: m-2 + - srmag/m-sf2/c26-e/Strength_H + - srmag/m-sf2/c26-e/Strength_V + - srmag/m-sf2/c26-e/Strength_SQ + - srmag/m-sf2/c26-e/Strength - type: pyaml.magnet.cfm_magnet name: SD1E-C26 mapping: @@ -5513,18 +4112,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c26-e/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c26-e/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c26-e/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c26-e/Strength - unit: m-2 + - srmag/m-sd1/c26-e/Strength_H + - srmag/m-sd1/c26-e/Strength_V + - srmag/m-sd1/c26-e/Strength_SQ + - srmag/m-sd1/c26-e/Strength - type: pyaml.magnet.cfm_magnet name: SH3E-C26 mapping: @@ -5535,27 +4126,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c26-e-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c26-e-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c26-e-ch3/current - unit: A + - srmag/ps-corr-sh3/c26-e-ch1/current + - srmag/ps-corr-sh3/c26-e-ch2/current + - srmag/ps-corr-sh3/c26-e-ch3/current - type: pyaml.magnet.cfm_magnet name: SH1A-C27 mapping: @@ -5566,27 +4152,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c27-a-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c27-a-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c27-a-ch3/current - unit: A + - srmag/ps-corr-sh1/c27-a-ch1/current + - srmag/ps-corr-sh1/c27-a-ch2/current + - srmag/ps-corr-sh1/c27-a-ch3/current - type: pyaml.magnet.cfm_magnet name: SD1A-C27 mapping: @@ -5599,18 +4180,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c27-a/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c27-a/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c27-a/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c27-a/Strength - unit: m-2 + - srmag/m-sd1/c27-a/Strength_H + - srmag/m-sd1/c27-a/Strength_V + - srmag/m-sd1/c27-a/Strength_SQ + - srmag/m-sd1/c27-a/Strength - type: pyaml.magnet.cfm_magnet name: SF2A-C27 mapping: @@ -5623,18 +4196,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c27-a/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c27-a/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c27-a/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c27-a/Strength - unit: m-2 + - srmag/m-sf2/c27-a/Strength_H + - srmag/m-sf2/c27-a/Strength_V + - srmag/m-sf2/c27-a/Strength_SQ + - srmag/m-sf2/c27-a/Strength - type: pyaml.magnet.cfm_magnet name: SD1B-C27 mapping: @@ -5647,18 +4212,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c27-b/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c27-b/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c27-b/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c27-b/Strength - unit: m-2 + - srmag/m-sd1/c27-b/Strength_H + - srmag/m-sd1/c27-b/Strength_V + - srmag/m-sd1/c27-b/Strength_SQ + - srmag/m-sd1/c27-b/Strength - type: pyaml.magnet.cfm_magnet name: SH2B-C27 mapping: @@ -5669,27 +4226,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c27-b-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c27-b-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c27-b-ch3/current - unit: A + - srmag/ps-corr-sh2/c27-b-ch1/current + - srmag/ps-corr-sh2/c27-b-ch2/current + - srmag/ps-corr-sh2/c27-b-ch3/current - type: pyaml.magnet.cfm_magnet name: SD1D-C27 mapping: @@ -5702,18 +4254,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c27-d/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c27-d/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c27-d/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c27-d/Strength - unit: m-2 + - srmag/m-sd1/c27-d/Strength_H + - srmag/m-sd1/c27-d/Strength_V + - srmag/m-sd1/c27-d/Strength_SQ + - srmag/m-sd1/c27-d/Strength - type: pyaml.magnet.cfm_magnet name: SF2E-C27 mapping: @@ -5726,18 +4270,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c27-e/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c27-e/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c27-e/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c27-e/Strength - unit: m-2 + - srmag/m-sf2/c27-e/Strength_H + - srmag/m-sf2/c27-e/Strength_V + - srmag/m-sf2/c27-e/Strength_SQ + - srmag/m-sf2/c27-e/Strength - type: pyaml.magnet.cfm_magnet name: SD1E-C27 mapping: @@ -5750,18 +4286,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c27-e/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c27-e/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c27-e/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c27-e/Strength - unit: m-2 + - srmag/m-sd1/c27-e/Strength_H + - srmag/m-sd1/c27-e/Strength_V + - srmag/m-sd1/c27-e/Strength_SQ + - srmag/m-sd1/c27-e/Strength - type: pyaml.magnet.cfm_magnet name: SH3E-C27 mapping: @@ -5772,27 +4300,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c27-e-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c27-e-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c27-e-ch3/current - unit: A + - srmag/ps-corr-sh3/c27-e-ch1/current + - srmag/ps-corr-sh3/c27-e-ch2/current + - srmag/ps-corr-sh3/c27-e-ch3/current - type: pyaml.magnet.cfm_magnet name: SH1A-C28 mapping: @@ -5803,27 +4326,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c28-a-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c28-a-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c28-a-ch3/current - unit: A + - srmag/ps-corr-sh1/c28-a-ch1/current + - srmag/ps-corr-sh1/c28-a-ch2/current + - srmag/ps-corr-sh1/c28-a-ch3/current - type: pyaml.magnet.cfm_magnet name: SD1A-C28 mapping: @@ -5836,18 +4354,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c28-a/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c28-a/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c28-a/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c28-a/Strength - unit: m-2 + - srmag/m-sd1/c28-a/Strength_H + - srmag/m-sd1/c28-a/Strength_V + - srmag/m-sd1/c28-a/Strength_SQ + - srmag/m-sd1/c28-a/Strength - type: pyaml.magnet.cfm_magnet name: SF2A-C28 mapping: @@ -5860,18 +4370,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c28-a/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c28-a/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c28-a/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c28-a/Strength - unit: m-2 + - srmag/m-sf2/c28-a/Strength_H + - srmag/m-sf2/c28-a/Strength_V + - srmag/m-sf2/c28-a/Strength_SQ + - srmag/m-sf2/c28-a/Strength - type: pyaml.magnet.cfm_magnet name: SD1B-C28 mapping: @@ -5884,18 +4386,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c28-b/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c28-b/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c28-b/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c28-b/Strength - unit: m-2 + - srmag/m-sd1/c28-b/Strength_H + - srmag/m-sd1/c28-b/Strength_V + - srmag/m-sd1/c28-b/Strength_SQ + - srmag/m-sd1/c28-b/Strength - type: pyaml.magnet.cfm_magnet name: SH2B-C28 mapping: @@ -5906,27 +4400,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c28-b-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c28-b-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c28-b-ch3/current - unit: A + - srmag/ps-corr-sh2/c28-b-ch1/current + - srmag/ps-corr-sh2/c28-b-ch2/current + - srmag/ps-corr-sh2/c28-b-ch3/current - type: pyaml.magnet.cfm_magnet name: SD1D-C28 mapping: @@ -5939,18 +4428,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c28-d/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c28-d/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c28-d/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c28-d/Strength - unit: m-2 + - srmag/m-sd1/c28-d/Strength_H + - srmag/m-sd1/c28-d/Strength_V + - srmag/m-sd1/c28-d/Strength_SQ + - srmag/m-sd1/c28-d/Strength - type: pyaml.magnet.cfm_magnet name: SF2E-C28 mapping: @@ -5963,18 +4444,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c28-e/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c28-e/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c28-e/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c28-e/Strength - unit: m-2 + - srmag/m-sf2/c28-e/Strength_H + - srmag/m-sf2/c28-e/Strength_V + - srmag/m-sf2/c28-e/Strength_SQ + - srmag/m-sf2/c28-e/Strength - type: pyaml.magnet.cfm_magnet name: SD1E-C28 mapping: @@ -5987,18 +4460,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c28-e/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c28-e/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c28-e/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c28-e/Strength - unit: m-2 + - srmag/m-sd1/c28-e/Strength_H + - srmag/m-sd1/c28-e/Strength_V + - srmag/m-sd1/c28-e/Strength_SQ + - srmag/m-sd1/c28-e/Strength - type: pyaml.magnet.cfm_magnet name: SH3E-C28 mapping: @@ -6009,27 +4474,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c28-e-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c28-e-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c28-e-ch3/current - unit: A + - srmag/ps-corr-sh3/c28-e-ch1/current + - srmag/ps-corr-sh3/c28-e-ch2/current + - srmag/ps-corr-sh3/c28-e-ch3/current - type: pyaml.magnet.cfm_magnet name: SH1A-C29 mapping: @@ -6040,27 +4500,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c29-a-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c29-a-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c29-a-ch3/current - unit: A + - srmag/ps-corr-sh1/c29-a-ch1/current + - srmag/ps-corr-sh1/c29-a-ch2/current + - srmag/ps-corr-sh1/c29-a-ch3/current - type: pyaml.magnet.cfm_magnet name: SD1A-C29 mapping: @@ -6073,18 +4528,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c29-a/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c29-a/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c29-a/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c29-a/Strength - unit: m-2 + - srmag/m-sd1/c29-a/Strength_H + - srmag/m-sd1/c29-a/Strength_V + - srmag/m-sd1/c29-a/Strength_SQ + - srmag/m-sd1/c29-a/Strength - type: pyaml.magnet.cfm_magnet name: SF2A-C29 mapping: @@ -6097,18 +4544,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c29-a/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c29-a/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c29-a/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c29-a/Strength - unit: m-2 + - srmag/m-sf2/c29-a/Strength_H + - srmag/m-sf2/c29-a/Strength_V + - srmag/m-sf2/c29-a/Strength_SQ + - srmag/m-sf2/c29-a/Strength - type: pyaml.magnet.cfm_magnet name: SD1B-C29 mapping: @@ -6121,18 +4560,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c29-b/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c29-b/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c29-b/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c29-b/Strength - unit: m-2 + - srmag/m-sd1/c29-b/Strength_H + - srmag/m-sd1/c29-b/Strength_V + - srmag/m-sd1/c29-b/Strength_SQ + - srmag/m-sd1/c29-b/Strength - type: pyaml.magnet.cfm_magnet name: SH2B-C29 mapping: @@ -6143,27 +4574,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c29-b-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c29-b-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c29-b-ch3/current - unit: A + - srmag/ps-corr-sh2/c29-b-ch1/current + - srmag/ps-corr-sh2/c29-b-ch2/current + - srmag/ps-corr-sh2/c29-b-ch3/current - type: pyaml.magnet.cfm_magnet name: SD1D-C29 mapping: @@ -6176,18 +4602,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c29-d/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c29-d/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c29-d/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c29-d/Strength - unit: m-2 + - srmag/m-sd1/c29-d/Strength_H + - srmag/m-sd1/c29-d/Strength_V + - srmag/m-sd1/c29-d/Strength_SQ + - srmag/m-sd1/c29-d/Strength - type: pyaml.magnet.cfm_magnet name: SF2E-C29 mapping: @@ -6200,18 +4618,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c29-e/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c29-e/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c29-e/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c29-e/Strength - unit: m-2 + - srmag/m-sf2/c29-e/Strength_H + - srmag/m-sf2/c29-e/Strength_V + - srmag/m-sf2/c29-e/Strength_SQ + - srmag/m-sf2/c29-e/Strength - type: pyaml.magnet.cfm_magnet name: SD1E-C29 mapping: @@ -6224,18 +4634,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c29-e/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c29-e/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c29-e/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c29-e/Strength - unit: m-2 + - srmag/m-sd1/c29-e/Strength_H + - srmag/m-sd1/c29-e/Strength_V + - srmag/m-sd1/c29-e/Strength_SQ + - srmag/m-sd1/c29-e/Strength - type: pyaml.magnet.cfm_magnet name: SH3E-C29 mapping: @@ -6246,27 +4648,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c29-e-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c29-e-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c29-e-ch3/current - unit: A + - srmag/ps-corr-sh3/c29-e-ch1/current + - srmag/ps-corr-sh3/c29-e-ch2/current + - srmag/ps-corr-sh3/c29-e-ch3/current - type: pyaml.magnet.cfm_magnet name: SH1A-C30 mapping: @@ -6277,27 +4674,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c30-a-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c30-a-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c30-a-ch3/current - unit: A + - srmag/ps-corr-sh1/c30-a-ch1/current + - srmag/ps-corr-sh1/c30-a-ch2/current + - srmag/ps-corr-sh1/c30-a-ch3/current - type: pyaml.magnet.cfm_magnet name: SD1A-C30 mapping: @@ -6310,18 +4702,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c30-a/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c30-a/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c30-a/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c30-a/Strength - unit: m-2 + - srmag/m-sd1/c30-a/Strength_H + - srmag/m-sd1/c30-a/Strength_V + - srmag/m-sd1/c30-a/Strength_SQ + - srmag/m-sd1/c30-a/Strength - type: pyaml.magnet.cfm_magnet name: SF2A-C30 mapping: @@ -6334,18 +4718,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c30-a/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c30-a/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c30-a/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c30-a/Strength - unit: m-2 + - srmag/m-sf2/c30-a/Strength_H + - srmag/m-sf2/c30-a/Strength_V + - srmag/m-sf2/c30-a/Strength_SQ + - srmag/m-sf2/c30-a/Strength - type: pyaml.magnet.cfm_magnet name: SD1B-C30 mapping: @@ -6358,18 +4734,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c30-b/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c30-b/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c30-b/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c30-b/Strength - unit: m-2 + - srmag/m-sd1/c30-b/Strength_H + - srmag/m-sd1/c30-b/Strength_V + - srmag/m-sd1/c30-b/Strength_SQ + - srmag/m-sd1/c30-b/Strength - type: pyaml.magnet.cfm_magnet name: SH2B-C30 mapping: @@ -6380,27 +4748,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c30-b-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c30-b-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c30-b-ch3/current - unit: A + - srmag/ps-corr-sh2/c30-b-ch1/current + - srmag/ps-corr-sh2/c30-b-ch2/current + - srmag/ps-corr-sh2/c30-b-ch3/current - type: pyaml.magnet.cfm_magnet name: SD1D-C30 mapping: @@ -6413,18 +4776,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c30-d/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c30-d/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c30-d/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c30-d/Strength - unit: m-2 + - srmag/m-sd1/c30-d/Strength_H + - srmag/m-sd1/c30-d/Strength_V + - srmag/m-sd1/c30-d/Strength_SQ + - srmag/m-sd1/c30-d/Strength - type: pyaml.magnet.cfm_magnet name: SF2E-C30 mapping: @@ -6437,18 +4792,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c30-e/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c30-e/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c30-e/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c30-e/Strength - unit: m-2 + - srmag/m-sf2/c30-e/Strength_H + - srmag/m-sf2/c30-e/Strength_V + - srmag/m-sf2/c30-e/Strength_SQ + - srmag/m-sf2/c30-e/Strength - type: pyaml.magnet.cfm_magnet name: SD1E-C30 mapping: @@ -6461,18 +4808,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c30-e/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c30-e/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c30-e/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c30-e/Strength - unit: m-2 + - srmag/m-sd1/c30-e/Strength_H + - srmag/m-sd1/c30-e/Strength_V + - srmag/m-sd1/c30-e/Strength_SQ + - srmag/m-sd1/c30-e/Strength - type: pyaml.magnet.cfm_magnet name: SH3E-C30 mapping: @@ -6483,27 +4822,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c30-e-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c30-e-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c30-e-ch3/current - unit: A + - srmag/ps-corr-sh3/c30-e-ch1/current + - srmag/ps-corr-sh3/c30-e-ch2/current + - srmag/ps-corr-sh3/c30-e-ch3/current - type: pyaml.magnet.cfm_magnet name: SH1A-C31 mapping: @@ -6514,27 +4848,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c31-a-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c31-a-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c31-a-ch3/current - unit: A + - srmag/ps-corr-sh1/c31-a-ch1/current + - srmag/ps-corr-sh1/c31-a-ch2/current + - srmag/ps-corr-sh1/c31-a-ch3/current - type: pyaml.magnet.cfm_magnet name: SD1A-C31 mapping: @@ -6547,18 +4876,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c31-a/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c31-a/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c31-a/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c31-a/Strength - unit: m-2 + - srmag/m-sd1/c31-a/Strength_H + - srmag/m-sd1/c31-a/Strength_V + - srmag/m-sd1/c31-a/Strength_SQ + - srmag/m-sd1/c31-a/Strength - type: pyaml.magnet.cfm_magnet name: SF2A-C31 mapping: @@ -6571,18 +4892,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c31-a/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c31-a/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c31-a/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c31-a/Strength - unit: m-2 + - srmag/m-sf2/c31-a/Strength_H + - srmag/m-sf2/c31-a/Strength_V + - srmag/m-sf2/c31-a/Strength_SQ + - srmag/m-sf2/c31-a/Strength - type: pyaml.magnet.cfm_magnet name: SD1B-C31 mapping: @@ -6595,18 +4908,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c31-b/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c31-b/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c31-b/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c31-b/Strength - unit: m-2 + - srmag/m-sd1/c31-b/Strength_H + - srmag/m-sd1/c31-b/Strength_V + - srmag/m-sd1/c31-b/Strength_SQ + - srmag/m-sd1/c31-b/Strength - type: pyaml.magnet.cfm_magnet name: SH2B-C31 mapping: @@ -6617,27 +4922,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c31-b-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c31-b-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c31-b-ch3/current - unit: A + - srmag/ps-corr-sh2/c31-b-ch1/current + - srmag/ps-corr-sh2/c31-b-ch2/current + - srmag/ps-corr-sh2/c31-b-ch3/current - type: pyaml.magnet.cfm_magnet name: SD1D-C31 mapping: @@ -6650,18 +4950,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c31-d/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c31-d/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c31-d/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c31-d/Strength - unit: m-2 + - srmag/m-sd1/c31-d/Strength_H + - srmag/m-sd1/c31-d/Strength_V + - srmag/m-sd1/c31-d/Strength_SQ + - srmag/m-sd1/c31-d/Strength - type: pyaml.magnet.cfm_magnet name: SF2E-C31 mapping: @@ -6674,18 +4966,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c31-e/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c31-e/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c31-e/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c31-e/Strength - unit: m-2 + - srmag/m-sf2/c31-e/Strength_H + - srmag/m-sf2/c31-e/Strength_V + - srmag/m-sf2/c31-e/Strength_SQ + - srmag/m-sf2/c31-e/Strength - type: pyaml.magnet.cfm_magnet name: SD1E-C31 mapping: @@ -6698,18 +4982,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c31-e/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c31-e/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c31-e/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c31-e/Strength - unit: m-2 + - srmag/m-sd1/c31-e/Strength_H + - srmag/m-sd1/c31-e/Strength_V + - srmag/m-sd1/c31-e/Strength_SQ + - srmag/m-sd1/c31-e/Strength - type: pyaml.magnet.cfm_magnet name: SH3E-C31 mapping: @@ -6720,27 +4996,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c31-e-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c31-e-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c31-e-ch3/current - unit: A + - srmag/ps-corr-sh3/c31-e-ch1/current + - srmag/ps-corr-sh3/c31-e-ch2/current + - srmag/ps-corr-sh3/c31-e-ch3/current - type: pyaml.magnet.cfm_magnet name: SH1A-C32 mapping: @@ -6751,27 +5022,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c32-a-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c32-a-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c32-a-ch3/current - unit: A + - srmag/ps-corr-sh1/c32-a-ch1/current + - srmag/ps-corr-sh1/c32-a-ch2/current + - srmag/ps-corr-sh1/c32-a-ch3/current - type: pyaml.magnet.cfm_magnet name: SD1A-C32 mapping: @@ -6784,18 +5050,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c32-a/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c32-a/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c32-a/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c32-a/Strength - unit: m-2 + - srmag/m-sd1/c32-a/Strength_H + - srmag/m-sd1/c32-a/Strength_V + - srmag/m-sd1/c32-a/Strength_SQ + - srmag/m-sd1/c32-a/Strength - type: pyaml.magnet.cfm_magnet name: SF2A-C32 mapping: @@ -6808,18 +5066,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c32-a/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c32-a/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c32-a/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c32-a/Strength - unit: m-2 + - srmag/m-sf2/c32-a/Strength_H + - srmag/m-sf2/c32-a/Strength_V + - srmag/m-sf2/c32-a/Strength_SQ + - srmag/m-sf2/c32-a/Strength - type: pyaml.magnet.cfm_magnet name: SD1B-C32 mapping: @@ -6832,18 +5082,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c32-b/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c32-b/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c32-b/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c32-b/Strength - unit: m-2 + - srmag/m-sd1/c32-b/Strength_H + - srmag/m-sd1/c32-b/Strength_V + - srmag/m-sd1/c32-b/Strength_SQ + - srmag/m-sd1/c32-b/Strength - type: pyaml.magnet.cfm_magnet name: SH2B-C32 mapping: @@ -6854,27 +5096,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c32-b-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c32-b-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c32-b-ch3/current - unit: A + - srmag/ps-corr-sh2/c32-b-ch1/current + - srmag/ps-corr-sh2/c32-b-ch2/current + - srmag/ps-corr-sh2/c32-b-ch3/current - type: pyaml.magnet.cfm_magnet name: SD1D-C32 mapping: @@ -6887,18 +5124,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c32-d/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c32-d/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c32-d/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c32-d/Strength - unit: m-2 + - srmag/m-sd1/c32-d/Strength_H + - srmag/m-sd1/c32-d/Strength_V + - srmag/m-sd1/c32-d/Strength_SQ + - srmag/m-sd1/c32-d/Strength - type: pyaml.magnet.cfm_magnet name: SF2E-C32 mapping: @@ -6911,18 +5140,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c32-e/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c32-e/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c32-e/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c32-e/Strength - unit: m-2 + - srmag/m-sf2/c32-e/Strength_H + - srmag/m-sf2/c32-e/Strength_V + - srmag/m-sf2/c32-e/Strength_SQ + - srmag/m-sf2/c32-e/Strength - type: pyaml.magnet.cfm_magnet name: SD1E-C32 mapping: @@ -6935,18 +5156,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c32-e/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c32-e/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c32-e/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c32-e/Strength - unit: m-2 + - srmag/m-sd1/c32-e/Strength_H + - srmag/m-sd1/c32-e/Strength_V + - srmag/m-sd1/c32-e/Strength_SQ + - srmag/m-sd1/c32-e/Strength - type: pyaml.magnet.cfm_magnet name: SH3E-C32 mapping: @@ -6957,27 +5170,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c32-e-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c32-e-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c32-e-ch3/current - unit: A + - srmag/ps-corr-sh3/c32-e-ch1/current + - srmag/ps-corr-sh3/c32-e-ch2/current + - srmag/ps-corr-sh3/c32-e-ch3/current - type: pyaml.magnet.cfm_magnet name: SH1A-C01 mapping: @@ -6988,27 +5196,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c01-a-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c01-a-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c01-a-ch3/current - unit: A + - srmag/ps-corr-sh1/c01-a-ch1/current + - srmag/ps-corr-sh1/c01-a-ch2/current + - srmag/ps-corr-sh1/c01-a-ch3/current - type: pyaml.magnet.cfm_magnet name: SD1A-C01 mapping: @@ -7021,18 +5224,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c01-a/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c01-a/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c01-a/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c01-a/Strength - unit: m-2 + - srmag/m-sd1/c01-a/Strength_H + - srmag/m-sd1/c01-a/Strength_V + - srmag/m-sd1/c01-a/Strength_SQ + - srmag/m-sd1/c01-a/Strength - type: pyaml.magnet.cfm_magnet name: SF2A-C01 mapping: @@ -7045,18 +5240,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c01-a/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c01-a/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c01-a/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c01-a/Strength - unit: m-2 + - srmag/m-sf2/c01-a/Strength_H + - srmag/m-sf2/c01-a/Strength_V + - srmag/m-sf2/c01-a/Strength_SQ + - srmag/m-sf2/c01-a/Strength - type: pyaml.magnet.cfm_magnet name: SD1B-C01 mapping: @@ -7069,18 +5256,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c01-b/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c01-b/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c01-b/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c01-b/Strength - unit: m-2 + - srmag/m-sd1/c01-b/Strength_H + - srmag/m-sd1/c01-b/Strength_V + - srmag/m-sd1/c01-b/Strength_SQ + - srmag/m-sd1/c01-b/Strength - type: pyaml.magnet.cfm_magnet name: SH2B-C01 mapping: @@ -7091,27 +5270,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c01-b-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c01-b-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c01-b-ch3/current - unit: A + - srmag/ps-corr-sh2/c01-b-ch1/current + - srmag/ps-corr-sh2/c01-b-ch2/current + - srmag/ps-corr-sh2/c01-b-ch3/current - type: pyaml.magnet.cfm_magnet name: SD1D-C01 mapping: @@ -7124,18 +5298,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c01-d/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c01-d/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c01-d/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c01-d/Strength - unit: m-2 + - srmag/m-sd1/c01-d/Strength_H + - srmag/m-sd1/c01-d/Strength_V + - srmag/m-sd1/c01-d/Strength_SQ + - srmag/m-sd1/c01-d/Strength - type: pyaml.magnet.cfm_magnet name: SF2E-C01 mapping: @@ -7148,18 +5314,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c01-e/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c01-e/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c01-e/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c01-e/Strength - unit: m-2 + - srmag/m-sf2/c01-e/Strength_H + - srmag/m-sf2/c01-e/Strength_V + - srmag/m-sf2/c01-e/Strength_SQ + - srmag/m-sf2/c01-e/Strength - type: pyaml.magnet.cfm_magnet name: SD1E-C01 mapping: @@ -7172,18 +5330,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c01-e/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c01-e/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c01-e/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c01-e/Strength - unit: m-2 + - srmag/m-sd1/c01-e/Strength_H + - srmag/m-sd1/c01-e/Strength_V + - srmag/m-sd1/c01-e/Strength_SQ + - srmag/m-sd1/c01-e/Strength - type: pyaml.magnet.cfm_magnet name: SH3E-C01 mapping: @@ -7194,27 +5344,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c01-e-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c01-e-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c01-e-ch3/current - unit: A + - srmag/ps-corr-sh3/c01-e-ch1/current + - srmag/ps-corr-sh3/c01-e-ch2/current + - srmag/ps-corr-sh3/c01-e-ch3/current - type: pyaml.magnet.cfm_magnet name: SH1A-C02 mapping: @@ -7225,27 +5370,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c02-a-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c02-a-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c02-a-ch3/current - unit: A + - srmag/ps-corr-sh1/c02-a-ch1/current + - srmag/ps-corr-sh1/c02-a-ch2/current + - srmag/ps-corr-sh1/c02-a-ch3/current - type: pyaml.magnet.cfm_magnet name: SD1A-C02 mapping: @@ -7258,18 +5398,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c02-a/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c02-a/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c02-a/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c02-a/Strength - unit: m-2 + - srmag/m-sd1/c02-a/Strength_H + - srmag/m-sd1/c02-a/Strength_V + - srmag/m-sd1/c02-a/Strength_SQ + - srmag/m-sd1/c02-a/Strength - type: pyaml.magnet.cfm_magnet name: SF2A-C02 mapping: @@ -7282,18 +5414,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c02-a/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c02-a/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c02-a/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c02-a/Strength - unit: m-2 + - srmag/m-sf2/c02-a/Strength_H + - srmag/m-sf2/c02-a/Strength_V + - srmag/m-sf2/c02-a/Strength_SQ + - srmag/m-sf2/c02-a/Strength - type: pyaml.magnet.cfm_magnet name: SD1B-C02 mapping: @@ -7306,18 +5430,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c02-b/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c02-b/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c02-b/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c02-b/Strength - unit: m-2 + - srmag/m-sd1/c02-b/Strength_H + - srmag/m-sd1/c02-b/Strength_V + - srmag/m-sd1/c02-b/Strength_SQ + - srmag/m-sd1/c02-b/Strength - type: pyaml.magnet.cfm_magnet name: SH2B-C02 mapping: @@ -7328,27 +5444,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c02-b-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c02-b-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c02-b-ch3/current - unit: A + - srmag/ps-corr-sh2/c02-b-ch1/current + - srmag/ps-corr-sh2/c02-b-ch2/current + - srmag/ps-corr-sh2/c02-b-ch3/current - type: pyaml.magnet.cfm_magnet name: SD1D-C02 mapping: @@ -7361,18 +5472,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c02-d/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c02-d/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c02-d/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c02-d/Strength - unit: m-2 + - srmag/m-sd1/c02-d/Strength_H + - srmag/m-sd1/c02-d/Strength_V + - srmag/m-sd1/c02-d/Strength_SQ + - srmag/m-sd1/c02-d/Strength - type: pyaml.magnet.cfm_magnet name: SF2E-C02 mapping: @@ -7385,18 +5488,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c02-e/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c02-e/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c02-e/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c02-e/Strength - unit: m-2 + - srmag/m-sf2/c02-e/Strength_H + - srmag/m-sf2/c02-e/Strength_V + - srmag/m-sf2/c02-e/Strength_SQ + - srmag/m-sf2/c02-e/Strength - type: pyaml.magnet.cfm_magnet name: SD1E-C02 mapping: @@ -7409,18 +5504,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c02-e/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c02-e/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c02-e/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c02-e/Strength - unit: m-2 + - srmag/m-sd1/c02-e/Strength_H + - srmag/m-sd1/c02-e/Strength_V + - srmag/m-sd1/c02-e/Strength_SQ + - srmag/m-sd1/c02-e/Strength - type: pyaml.magnet.cfm_magnet name: SH3E-C02 mapping: @@ -7431,27 +5518,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c02-e-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c02-e-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c02-e-ch3/current - unit: A + - srmag/ps-corr-sh3/c02-e-ch1/current + - srmag/ps-corr-sh3/c02-e-ch2/current + - srmag/ps-corr-sh3/c02-e-ch3/current - type: pyaml.magnet.cfm_magnet name: SH1A-C03 mapping: @@ -7462,27 +5544,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c03-a-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c03-a-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c03-a-ch3/current - unit: A + - srmag/ps-corr-sh1/c03-a-ch1/current + - srmag/ps-corr-sh1/c03-a-ch2/current + - srmag/ps-corr-sh1/c03-a-ch3/current - type: pyaml.magnet.cfm_magnet name: SI1A-C03 mapping: @@ -7495,18 +5572,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c03-a/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c03-a/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c03-a/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c03-a/Strength - unit: m-2 + - srmag/m-sd1/c03-a/Strength_H + - srmag/m-sd1/c03-a/Strength_V + - srmag/m-sd1/c03-a/Strength_SQ + - srmag/m-sd1/c03-a/Strength - type: pyaml.magnet.cfm_magnet name: SI2A-C03 mapping: @@ -7519,18 +5588,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c03-a/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c03-a/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c03-a/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c03-a/Strength - unit: m-2 + - srmag/m-sf2/c03-a/Strength_H + - srmag/m-sf2/c03-a/Strength_V + - srmag/m-sf2/c03-a/Strength_SQ + - srmag/m-sf2/c03-a/Strength - type: pyaml.magnet.cfm_magnet name: SI1B-C03 mapping: @@ -7543,18 +5604,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c03-b/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c03-b/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c03-b/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c03-b/Strength - unit: m-2 + - srmag/m-sd1/c03-b/Strength_H + - srmag/m-sd1/c03-b/Strength_V + - srmag/m-sd1/c03-b/Strength_SQ + - srmag/m-sd1/c03-b/Strength - type: pyaml.magnet.cfm_magnet name: SH2B-C03 mapping: @@ -7565,27 +5618,22 @@ devices: type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: ["A","A","A"] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH2_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c03-b-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c03-b-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh2/c03-b-ch3/current - unit: A + - srmag/ps-corr-sh2/c03-b-ch1/current + - srmag/ps-corr-sh2/c03-b-ch2/current + - srmag/ps-corr-sh2/c03-b-ch3/current - type: pyaml.magnet.cfm_magnet name: SI1D-C03 mapping: @@ -7598,18 +5646,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c03-d/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c03-d/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c03-d/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c03-d/Strength - unit: m-2 + - srmag/m-sd1/c03-d/Strength_H + - srmag/m-sd1/c03-d/Strength_V + - srmag/m-sd1/c03-d/Strength_SQ + - srmag/m-sd1/c03-d/Strength - type: pyaml.magnet.cfm_magnet name: SI2E-C03 mapping: @@ -7622,18 +5662,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c03-e/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c03-e/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c03-e/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sf2/c03-e/Strength - unit: m-2 + - srmag/m-sf2/c03-e/Strength_H + - srmag/m-sf2/c03-e/Strength_V + - srmag/m-sf2/c03-e/Strength_SQ + - srmag/m-sf2/c03-e/Strength - type: pyaml.magnet.cfm_magnet name: SI1E-C03 mapping: @@ -7646,18 +5678,10 @@ devices: multipoles: [B0,A0,A1,B2] units: [rad,rad,m-1,m-2] physics: - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c03-e/Strength_H - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c03-e/Strength_V - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c03-e/Strength_SQ - unit: m-1 - - type: tango.pyaml.attribute - attribute: srmag/m-sd1/c03-e/Strength - unit: m-2 + - srmag/m-sd1/c03-e/Strength_H + - srmag/m-sd1/c03-e/Strength_V + - srmag/m-sd1/c03-e/Strength_SQ + - srmag/m-sd1/c03-e/Strength - type: pyaml.magnet.cfm_magnet name: SH3E-C03 mapping: @@ -7670,3871 +5694,2916 @@ devices: multipoles: [B0,A0,A1,B2] pseudo_factors: [1.0,-1.0,-1.0,-1.0] units: [rad,rad,m-1,m-2] + hardware_units: ["A","A","A","A","A"] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SHI_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SHI_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SHI_sq_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SHI_sext_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SHI_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c03-e-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c03-e-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c03-e-ch3/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c03-e-ch5/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh3/c03-e-ch6/current - unit: A + - srmag/ps-corr-sh3/c03-e-ch1/current + - srmag/ps-corr-sh3/c03-e-ch2/current + - srmag/ps-corr-sh3/c03-e-ch3/current + - srmag/ps-corr-sh3/c03-e-ch5/current + - srmag/ps-corr-sh3/c03-e-ch6/current - type: pyaml.bpm.bpm name: BPM_C04-01 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c04-01/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c04-01/SA_VPosition - unit: m + x_pos: srdiag/bpm/c04-01/SA_HPosition + y_pos: srdiag/bpm/c04-01/SA_VPosition - type: pyaml.bpm.bpm name: BPM_C04-02 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c04-02/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c04-02/SA_VPosition - unit: m + x_pos: srdiag/bpm/c04-02/SA_HPosition + y_pos: srdiag/bpm/c04-02/SA_VPosition - type: pyaml.bpm.bpm name: BPM_C04-03 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c04-03/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c04-03/SA_VPosition - unit: m + x_pos: srdiag/bpm/c04-03/SA_HPosition + y_pos: srdiag/bpm/c04-03/SA_VPosition - type: pyaml.bpm.bpm name: BPM_C04-04 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c04-04/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c04-04/SA_VPosition - unit: m + x_pos: srdiag/bpm/c04-04/SA_HPosition + y_pos: srdiag/bpm/c04-04/SA_VPosition + x_offset: srdiag/bpm/c04-04/HOffset + y_offset: srdiag/bpm/c04-04/VOffset - type: pyaml.bpm.bpm name: BPM_C04-05 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: 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srdiag/bpm/c04-07/SA_VPosition - type: pyaml.bpm.bpm name: BPM_C04-08 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c04-08/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c04-08/SA_VPosition - unit: m + x_pos: srdiag/bpm/c04-08/SA_HPosition + y_pos: srdiag/bpm/c04-08/SA_VPosition - type: pyaml.bpm.bpm name: BPM_C04-09 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c04-09/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c04-09/SA_VPosition - unit: m + x_pos: srdiag/bpm/c04-09/SA_HPosition + y_pos: srdiag/bpm/c04-09/SA_VPosition - type: pyaml.bpm.bpm name: BPM_C04-10 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c04-10/SA_HPosition - unit: m - y_pos: - type: 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unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c05-a/current +- type: pyaml.magnet.quadrupole + name: QF1E-C05 + description: "QF1E-C05 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.00191 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c05-e/current +- type: pyaml.magnet.quadrupole + name: QF1A-C06 + description: "QF1A-C06 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.0003 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c06-a/current +- type: pyaml.magnet.quadrupole + name: QF1E-C06 + description: "QF1E-C06 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.997615 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c06-e/current +- type: pyaml.magnet.quadrupole + name: QF1A-C07 + description: "QF1A-C07 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.998152 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c07-a/current +- type: pyaml.magnet.quadrupole + name: QF1E-C07 + description: "QF1E-C07 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.00262 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c07-e/current +- type: pyaml.magnet.quadrupole + name: QF1A-C08 + description: "QF1A-C08 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.00319 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c08-a/current +- type: pyaml.magnet.quadrupole + name: QF1E-C08 + description: "QF1E-C08 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.996180929 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c08-e/current +- type: pyaml.magnet.quadrupole + name: QF1A-C09 + description: "QF1A-C09 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.00206 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c09-a/current +- type: pyaml.magnet.quadrupole + name: QF1E-C09 + description: "QF1E-C09 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.999285 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c09-e/current +- type: pyaml.magnet.quadrupole + name: QF1A-C10 + description: "QF1A-C10 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.00232 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c10-a/current +- type: pyaml.magnet.quadrupole + name: QF1E-C10 + description: "QF1E-C10 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.998212 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c10-e/current +- type: pyaml.magnet.quadrupole + name: QF1A-C11 + description: "QF1A-C11 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.999225 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c11-a/current +- type: pyaml.magnet.quadrupole + name: QF1E-C11 + description: "QF1E-C11 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.998033 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c11-e/current +- type: pyaml.magnet.quadrupole + name: QF1A-C12 + description: "QF1A-C12 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.998748 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c12-a/current +- type: pyaml.magnet.quadrupole + name: QF1E-C12 + description: "QF1E-C12 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.0023 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c12-e/current +- type: pyaml.magnet.quadrupole + name: QF1A-C13 + description: "QF1A-C13 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.00337 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c13-a/current +- type: pyaml.magnet.quadrupole + name: QF1E-C13 + description: "QF1E-C13 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.00403 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c13-e/current +- type: pyaml.magnet.quadrupole + name: QF1A-C14 + description: "QF1A-C14 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.00182 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c14-a/current +- type: pyaml.magnet.quadrupole + name: QF1E-C14 + description: "QF1E-C14 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.998303 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c14-e/current +- type: pyaml.magnet.quadrupole + name: QF1A-C15 + description: "QF1A-C15 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.998748 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c15-a/current +- type: pyaml.magnet.quadrupole + name: QF1E-C15 + description: "QF1E-C15 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.994098 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c15-e/current +- type: pyaml.magnet.quadrupole + name: QF1A-C16 + description: "QF1A-C16 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.00232 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c16-a/current +- type: pyaml.magnet.quadrupole + name: QF1E-C16 + description: "QF1E-C16 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.99884 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c16-e/current +- type: pyaml.magnet.quadrupole + name: QF1A-C17 + description: "QF1A-C17 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.0079 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c17-a/current +- type: pyaml.magnet.quadrupole + name: QF1E-C17 + description: "QF1E-C17 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.999523 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c17-e/current +- type: pyaml.magnet.quadrupole + name: QF1A-C18 + description: "QF1A-C18 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c18-a/current +- type: pyaml.magnet.quadrupole + name: QF1E-C18 + description: "QF1E-C18 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.999854 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c18-e/current +- type: pyaml.magnet.quadrupole + name: QF1A-C19 + description: "QF1A-C19 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.99845 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c19-a/current +- type: pyaml.magnet.quadrupole + name: QF1E-C19 + description: "QF1E-C19 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c19-e/current +- type: pyaml.magnet.quadrupole + name: QF1A-C20 + description: "QF1A-C20 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.00095 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c20-a/current +- type: pyaml.magnet.quadrupole + name: QF1E-C20 + description: "QF1E-C20 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.996753 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c20-e/current +- type: pyaml.magnet.quadrupole + name: QF1A-C21 + description: "QF1A-C21 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.00334 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c21-a/current +- type: pyaml.magnet.quadrupole + name: QF1E-C21 + description: "QF1E-C21 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.997707 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c21-e/current +- type: pyaml.magnet.quadrupole + name: QF1A-C22 + description: "QF1A-C22 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.00152 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c22-a/current +- type: pyaml.magnet.quadrupole + name: QF1E-C22 + description: "QF1E-C22 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.998124 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c22-e/current +- type: pyaml.magnet.quadrupole + name: QF1A-C23 + description: "QF1A-C23 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.996662 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c23-a/current +- type: pyaml.magnet.quadrupole + name: QF1E-C23 + description: "QF1E-C23 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.0017 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c23-e/current +- type: pyaml.magnet.quadrupole + name: QF1A-C24 + description: "QF1A-C24 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.999642 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c24-a/current +- type: pyaml.magnet.quadrupole + name: QF1E-C24 + description: "QF1E-C24 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.00042 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c24-e/current +- type: pyaml.magnet.quadrupole + name: QF1A-C25 + description: "QF1A-C25 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.00471 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c25-a/current +- type: pyaml.magnet.quadrupole + name: QF1E-C25 + description: "QF1E-C25 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.00393 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c25-e/current +- type: pyaml.magnet.quadrupole + name: QF1A-C26 + description: "QF1A-C26 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.992906 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c26-a/current +- type: pyaml.magnet.quadrupole + name: QF1E-C26 + description: "QF1E-C26 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.00268 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c26-e/current +- type: pyaml.magnet.quadrupole + name: QF1A-C27 + description: "QF1A-C27 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.00248 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c27-a/current +- type: pyaml.magnet.quadrupole + name: QF1E-C27 + description: "QF1E-C27 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.00203 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c27-e/current +- type: pyaml.magnet.quadrupole + name: QF1A-C28 + description: "QF1A-C28 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.998030791 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c28-a/current +- type: pyaml.magnet.quadrupole + name: QF1E-C28 + description: "QF1E-C28 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.00232 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c28-e/current +- type: pyaml.magnet.quadrupole + name: QF1A-C29 + description: "QF1A-C29 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.995052 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c29-a/current +- type: pyaml.magnet.quadrupole + name: QF1E-C29 + description: "QF1E-C29 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.00155 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c29-e/current +- type: pyaml.magnet.quadrupole + name: QF1A-C30 + description: "QF1A-C30 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.998271 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c30-a/current +- type: pyaml.magnet.quadrupole + name: QF1E-C30 + description: "QF1E-C30 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.999702 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c30-e/current +- type: pyaml.magnet.quadrupole + name: QF1A-C31 + description: "QF1A-C31 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.998005 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c31-a/current +- type: pyaml.magnet.quadrupole + name: QF1E-C31 + description: "QF1E-C31 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.999463 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c31-e/current +- type: pyaml.magnet.quadrupole + name: QF1A-C32 + description: "QF1A-C32 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.997794 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c32-a/current +- type: pyaml.magnet.quadrupole + name: QF1E-C32 + description: "QF1E-C32 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.00203 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c32-e/current +- type: pyaml.magnet.quadrupole + name: QF1A-C01 + description: "QF1A-C01 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.00504 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c01-a/current +- type: pyaml.magnet.quadrupole + name: QF1E-C01 + description: "QF1E-C01 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.998212 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c01-e/current +- type: pyaml.magnet.quadrupole + name: QF1A-C02 + description: "QF1A-C02 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.0037 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c02-a/current +- type: pyaml.magnet.quadrupole + name: QF1E-C02 + description: "QF1E-C02 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.00093 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c02-e/current +- type: pyaml.magnet.quadrupole + name: QF1A-C03 + description: "QF1A-C03 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.0025 + crosstalk: 1.0 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QF1_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qf1/c03-a/current +- type: pyaml.magnet.quadrupole + name: QD2E-C04 + description: "QD2E-C04 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.999305341 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c04-e/current +- type: pyaml.magnet.quadrupole + name: QD2A-C05 + description: "QD2A-C05 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.997452918 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c05-a/current +- type: pyaml.magnet.quadrupole + name: QD2E-C05 + description: "QD2E-C05 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.997993208 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c05-e/current +- type: pyaml.magnet.quadrupole + name: QD2A-C06 + description: "QD2A-C06 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.006031322 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c06-a/current +- type: pyaml.magnet.quadrupole + name: QD2E-C06 + description: "QD2E-C06 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.998547233 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c06-e/current +- type: pyaml.magnet.quadrupole + name: QD2A-C07 + description: "QD2A-C07 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.002327856 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c07-a/current +- type: pyaml.magnet.quadrupole + name: QD2E-C07 + description: "QD2E-C07 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.000154369 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c07-e/current +- type: pyaml.magnet.quadrupole + name: QD2A-C08 + description: "QD2A-C08 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.009580478 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c08-a/current +- type: pyaml.magnet.quadrupole + name: QD2E-C08 + description: "QD2E-C08 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.00447669 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c08-e/current +- type: pyaml.magnet.quadrupole + name: QD2A-C09 + description: "QD2A-C09 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.0015563 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c09-a/current +- type: pyaml.magnet.quadrupole + name: QD2E-C09 + description: "QD2E-C09 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.997221365 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c09-e/current +- type: pyaml.magnet.quadrupole + name: QD2A-C10 + description: "QD2A-C10 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.005954167 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c10-a/current +- type: pyaml.magnet.quadrupole + name: QD2E-C10 + description: "QD2E-C10 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.006725723 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c10-e/current +- type: pyaml.magnet.quadrupole + name: QD2A-C11 + description: "QD2A-C11 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.994535144 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c11-a/current +- type: pyaml.magnet.quadrupole + name: QD2E-C11 + description: "QD2E-C11 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.999550256 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c11-e/current +- type: pyaml.magnet.quadrupole + name: QD2A-C12 + description: "QD2A-C12 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.001479145 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c12-a/current +- type: pyaml.magnet.quadrupole + name: QD2E-C12 + description: "QD2E-C12 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.000321811 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c12-e/current +- type: pyaml.magnet.quadrupole + name: QD2A-C13 + description: "QD2A-C13 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.006715036 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c13-a/current +- type: pyaml.magnet.quadrupole + name: QD2E-C13 + description: "QD2E-C13 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.0036395 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c13-e/current +- type: pyaml.magnet.quadrupole + name: QD2A-C14 + description: "QD2A-C14 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.997684471 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c14-a/current +- type: pyaml.magnet.quadrupole + name: QD2E-C14 + description: "QD2E-C14 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.000385922 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c14-e/current +- type: pyaml.magnet.quadrupole + name: QD2A-C15 + description: "QD2A-C15 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.999010167 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c15-a/current +- type: pyaml.magnet.quadrupole + name: QD2E-C15 + description: "QD2E-C15 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.998392922 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c15-e/current +- type: pyaml.magnet.quadrupole + name: QD2A-C16 + description: "QD2A-C16 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.999318789 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c16-a/current +- type: pyaml.magnet.quadrupole + name: QD2E-C16 + description: "QD2E-C16 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.996926967 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c16-e/current +- type: pyaml.magnet.quadrupole + name: QD2A-C17 + description: "QD2A-C17 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.000849027 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c17-a/current +- type: pyaml.magnet.quadrupole + name: QD2E-C17 + description: "QD2E-C17 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.003392444 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c17-e/current +- type: pyaml.magnet.quadrupole + name: QD2A-C18 + description: "QD2A-C18 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.001312133 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c18-a/current +- type: pyaml.magnet.quadrupole + name: QD2E-C18 + description: "QD2E-C18 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.005402902 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c18-e/current +- type: pyaml.magnet.quadrupole + name: QD2A-C19 + description: "QD2A-C19 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.995846789 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c19-a/current +- type: pyaml.magnet.quadrupole + name: QD2E-C19 + description: "QD2E-C19 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.005877011 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c19-e/current +- type: pyaml.magnet.quadrupole + name: QD2A-C20 + description: "QD2A-C20 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.001016211 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c20-a/current +- type: pyaml.magnet.quadrupole + name: QD2E-C20 + description: "QD2E-C20 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.999010167 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c20-e/current +- type: pyaml.magnet.quadrupole + name: QD2A-C21 + description: "QD2A-C21 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.007265811 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c21-a/current +- type: pyaml.magnet.quadrupole + name: QD2E-C21 + description: "QD2E-C21 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.998238611 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c21-e/current +- type: pyaml.magnet.quadrupole + name: QD2A-C22 + description: "QD2A-C22 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.998161456 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c22-a/current +- type: pyaml.magnet.quadrupole + name: QD2E-C22 + description: "QD2E-C22 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.004642522 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c22-e/current +- type: pyaml.magnet.quadrupole + name: QD2A-C23 + description: "QD2A-C23 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.001479145 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c23-a/current +- type: pyaml.magnet.quadrupole + name: QD2E-C23 + description: "QD2E-C23 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.001942078 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c23-e/current +- type: pyaml.magnet.quadrupole + name: QD2A-C24 + description: "QD2A-C24 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.999087322 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c24-a/current +- type: pyaml.magnet.quadrupole + name: QD2E-C24 + description: "QD2E-C24 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.998547233 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c24-e/current +- type: pyaml.magnet.quadrupole + name: QD2A-C25 + description: "QD2A-C25 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.001698055 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c25-a/current +- type: pyaml.magnet.quadrupole + name: QD2E-C25 + description: "QD2E-C25 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.999704567 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c25-e/current +- type: pyaml.magnet.quadrupole + name: QD2A-C26 + description: "QD2A-C26 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.999164478 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c26-a/current +- type: pyaml.magnet.quadrupole + name: QD2E-C26 + description: "QD2E-C26 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.000694659 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c26-e/current +- type: pyaml.magnet.quadrupole + name: QD2A-C27 + description: "QD2A-C27 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.99945971 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c27-a/current +- type: pyaml.magnet.quadrupole + name: QD2E-C27 + description: "QD2E-C27 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.999922816 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c27-e/current +- type: pyaml.magnet.quadrupole + name: QD2A-C28 + description: "QD2A-C28 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.999922816 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c28-a/current +- type: pyaml.magnet.quadrupole + name: QD2E-C28 + description: "QD2E-C28 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.997838839 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c28-e/current +- type: pyaml.magnet.quadrupole + name: QD2A-C29 + description: "QD2A-C29 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.003318926 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c29-a/current +- type: pyaml.magnet.quadrupole + name: QD2E-C29 + description: "QD2E-C29 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.004179589 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c29-e/current +- type: pyaml.magnet.quadrupole + name: QD2A-C30 + description: "QD2A-C30 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.999010167 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c30-a/current +- type: pyaml.magnet.quadrupole + name: QD2E-C30 + description: "QD2E-C30 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.9987787 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c30-e/current +- type: pyaml.magnet.quadrupole + name: QD2A-C31 + description: "QD2A-C31 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.004411056 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c31-a/current +- type: pyaml.magnet.quadrupole + name: QD2E-C31 + description: "QD2E-C31 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.0029451 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c31-e/current +- type: pyaml.magnet.quadrupole + name: QD2A-C32 + description: "QD2A-C32 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.009426167 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c32-a/current +- type: pyaml.magnet.quadrupole + name: QD2E-C32 + description: "QD2E-C32 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.0050283 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c32-e/current +- type: pyaml.magnet.quadrupole + name: QD2A-C01 + description: "QD2A-C01 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 0.998533498 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c01-a/current +- type: pyaml.magnet.quadrupole + name: QD2E-C01 + description: "QD2E-C01 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.003485189 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c01-e/current +- type: pyaml.magnet.quadrupole + name: QD2A-C02 + description: "QD2A-C02 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.001389318 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c02-a/current +- type: pyaml.magnet.quadrupole + name: QD2E-C02 + description: "QD2E-C02 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.006108478 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c02-e/current +- type: pyaml.magnet.quadrupole + name: QD2A-C03 + description: "QD2A-C03 quadrupole" + model: + type: pyaml.magnet.linear_model + calibration_factor: 1.002096389 + crosstalk: 0.99912 + curve: + type: pyaml.magnet.csvcurve + file: sr/magnet_models/QD2_strength.csv + unit: 1/m + hardware_unit: A + powerconverter: srmag/vps-qd2/c03-a/current diff --git a/tests/config/EBSTune-patterns.yaml b/tests/config/EBSTune-patterns.yaml index cc8fde6a4..0c258bdea 100644 --- a/tests/config/EBSTune-patterns.yaml +++ b/tests/config/EBSTune-patterns.yaml @@ -12,6 +12,7 @@ controls: - type: tango.pyaml.controlsystem tango_host: ebs-simu-3:10000 name: live + catalog: catalogs/ebs_catalogs.yaml data_folder: /data/store arrays: - type: pyaml.arrays.magnet @@ -27,1760 +28,1629 @@ arrays: - ~QF1E-C05 - ~Q???-C06 devices: +- type: pyaml.diagnostics.tune_monitor + name: BETATRON_TUNE + tune_h: srdiag/beam-tune/main/Qh + tune_v: srdiag/beam-tune/main/Qv +- type: pyaml.tuning_tools.tune + name: DEFAULT_TUNE_CORRECTION + quad_array_name: QForTune + betatron_tune_name: BETATRON_TUNE + response_matrix: ${path:tune_response.json} +- type: pyaml.tuning_tools.tune_response_matrix + name: DEFAULT_TUNE_RESPONSE_MATRIX + quad_array_name: QForTune + betatron_tune_name: BETATRON_TUNE + quad_delta: 1e-4 - type: pyaml.magnet.quadrupole - description: "QF1E-C04 quadrupole" name: QF1E-C04 + description: "QF1E-C04 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.00054 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c04-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c04-e/current - type: pyaml.magnet.quadrupole name: QF1A-C05 + description: "QF1A-C05 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.996841 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c05-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c05-a/current - type: pyaml.magnet.quadrupole name: QF1E-C05 + description: "QF1E-C05 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.00191 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c05-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c05-e/current - type: pyaml.magnet.quadrupole name: QF1A-C06 + description: "QF1A-C06 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.0003 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c06-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c06-a/current - type: pyaml.magnet.quadrupole name: QF1E-C06 + description: "QF1E-C06 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.997615 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c06-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c06-e/current - type: pyaml.magnet.quadrupole name: QF1A-C07 + description: "QF1A-C07 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.998152 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c07-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c07-a/current - type: pyaml.magnet.quadrupole name: QF1E-C07 + description: "QF1E-C07 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.00262 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c07-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c07-e/current - type: pyaml.magnet.quadrupole name: QF1A-C08 + description: "QF1A-C08 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.00319 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c08-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c08-a/current - type: pyaml.magnet.quadrupole name: QF1E-C08 + description: "QF1E-C08 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.996180929 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c08-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c08-e/current - type: pyaml.magnet.quadrupole name: QF1A-C09 + description: "QF1A-C09 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.00206 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c09-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c09-a/current - type: pyaml.magnet.quadrupole name: QF1E-C09 + description: "QF1E-C09 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.999285 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c09-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c09-e/current - type: pyaml.magnet.quadrupole name: QF1A-C10 + description: "QF1A-C10 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.00232 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c10-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c10-a/current - type: pyaml.magnet.quadrupole name: QF1E-C10 + description: "QF1E-C10 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.998212 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c10-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c10-e/current - type: pyaml.magnet.quadrupole name: QF1A-C11 + description: "QF1A-C11 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.999225 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c11-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c11-a/current - type: pyaml.magnet.quadrupole name: QF1E-C11 + description: "QF1E-C11 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.998033 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c11-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c11-e/current - type: pyaml.magnet.quadrupole name: QF1A-C12 + description: "QF1A-C12 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.998748 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c12-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c12-a/current - type: pyaml.magnet.quadrupole name: QF1E-C12 + description: "QF1E-C12 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.0023 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c12-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c12-e/current - type: pyaml.magnet.quadrupole name: QF1A-C13 + description: "QF1A-C13 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.00337 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c13-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c13-a/current - type: pyaml.magnet.quadrupole name: QF1E-C13 + description: "QF1E-C13 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.00403 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c13-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c13-e/current - type: pyaml.magnet.quadrupole name: QF1A-C14 + description: "QF1A-C14 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.00182 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c14-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c14-a/current - type: pyaml.magnet.quadrupole name: QF1E-C14 + description: "QF1E-C14 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.998303 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c14-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c14-e/current - type: pyaml.magnet.quadrupole name: QF1A-C15 + description: "QF1A-C15 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.998748 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c15-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c15-a/current - type: pyaml.magnet.quadrupole name: QF1E-C15 + description: "QF1E-C15 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.994098 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c15-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c15-e/current - type: pyaml.magnet.quadrupole name: QF1A-C16 + description: "QF1A-C16 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.00232 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c16-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c16-a/current - type: pyaml.magnet.quadrupole name: QF1E-C16 + description: "QF1E-C16 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.99884 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c16-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c16-e/current - type: pyaml.magnet.quadrupole name: QF1A-C17 + description: "QF1A-C17 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.0079 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c17-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c17-a/current - type: pyaml.magnet.quadrupole name: QF1E-C17 + description: "QF1E-C17 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.999523 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c17-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c17-e/current - type: pyaml.magnet.quadrupole name: QF1A-C18 + description: "QF1A-C18 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c18-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c18-a/current - type: pyaml.magnet.quadrupole name: QF1E-C18 + description: "QF1E-C18 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.999854 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c18-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c18-e/current - type: pyaml.magnet.quadrupole name: QF1A-C19 + description: "QF1A-C19 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.99845 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c19-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c19-a/current - type: pyaml.magnet.quadrupole name: QF1E-C19 + description: "QF1E-C19 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c19-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c19-e/current - type: pyaml.magnet.quadrupole name: QF1A-C20 + description: "QF1A-C20 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.00095 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c20-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c20-a/current - type: pyaml.magnet.quadrupole name: QF1E-C20 + description: "QF1E-C20 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.996753 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c20-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c20-e/current - type: pyaml.magnet.quadrupole name: QF1A-C21 + description: "QF1A-C21 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.00334 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c21-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c21-a/current - type: pyaml.magnet.quadrupole name: QF1E-C21 + description: "QF1E-C21 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.997707 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c21-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c21-e/current - type: pyaml.magnet.quadrupole name: QF1A-C22 + description: "QF1A-C22 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.00152 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c22-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c22-a/current - type: pyaml.magnet.quadrupole name: QF1E-C22 + description: "QF1E-C22 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.998124 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c22-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c22-e/current - type: pyaml.magnet.quadrupole name: QF1A-C23 + description: "QF1A-C23 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.996662 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c23-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c23-a/current - type: pyaml.magnet.quadrupole name: QF1E-C23 + description: "QF1E-C23 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.0017 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c23-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c23-e/current - type: pyaml.magnet.quadrupole name: QF1A-C24 + description: "QF1A-C24 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.999642 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c24-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c24-a/current - type: pyaml.magnet.quadrupole name: QF1E-C24 + description: "QF1E-C24 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.00042 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c24-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c24-e/current - type: pyaml.magnet.quadrupole name: QF1A-C25 + description: "QF1A-C25 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.00471 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c25-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c25-a/current - type: pyaml.magnet.quadrupole name: QF1E-C25 + description: "QF1E-C25 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.00393 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c25-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c25-e/current - type: pyaml.magnet.quadrupole name: QF1A-C26 + description: "QF1A-C26 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.992906 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c26-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c26-a/current - type: pyaml.magnet.quadrupole name: QF1E-C26 + description: "QF1E-C26 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.00268 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c26-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c26-e/current - type: pyaml.magnet.quadrupole name: QF1A-C27 + description: "QF1A-C27 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.00248 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c27-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c27-a/current - type: pyaml.magnet.quadrupole name: QF1E-C27 + description: "QF1E-C27 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.00203 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c27-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c27-e/current - type: pyaml.magnet.quadrupole name: QF1A-C28 + description: "QF1A-C28 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.998030791 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c28-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c28-a/current - type: pyaml.magnet.quadrupole name: QF1E-C28 + description: "QF1E-C28 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.00232 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c28-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c28-e/current - type: pyaml.magnet.quadrupole name: QF1A-C29 + description: "QF1A-C29 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.995052 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c29-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c29-a/current - type: pyaml.magnet.quadrupole name: QF1E-C29 + description: "QF1E-C29 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.00155 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c29-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c29-e/current - type: pyaml.magnet.quadrupole name: QF1A-C30 + description: "QF1A-C30 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.998271 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c30-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c30-a/current - type: pyaml.magnet.quadrupole name: QF1E-C30 + description: "QF1E-C30 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.999702 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c30-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c30-e/current - type: pyaml.magnet.quadrupole name: QF1A-C31 + description: "QF1A-C31 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.998005 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c31-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c31-a/current - type: pyaml.magnet.quadrupole name: QF1E-C31 + description: "QF1E-C31 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.999463 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c31-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c31-e/current - type: pyaml.magnet.quadrupole name: QF1A-C32 + description: "QF1A-C32 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.997794 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c32-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c32-a/current - type: pyaml.magnet.quadrupole name: QF1E-C32 + description: "QF1E-C32 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.00203 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c32-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c32-e/current - type: pyaml.magnet.quadrupole name: QF1A-C01 + description: "QF1A-C01 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.00504 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c01-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c01-a/current - type: pyaml.magnet.quadrupole name: QF1E-C01 + description: "QF1E-C01 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.998212 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c01-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c01-e/current - type: pyaml.magnet.quadrupole name: QF1A-C02 + description: "QF1A-C02 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.0037 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c02-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c02-a/current - type: pyaml.magnet.quadrupole name: QF1E-C02 + description: "QF1E-C02 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.00093 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c02-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c02-e/current - type: pyaml.magnet.quadrupole name: QF1A-C03 + description: "QF1A-C03 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.0025 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c03-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c03-a/current - type: pyaml.magnet.quadrupole name: QD2E-C04 + description: "QD2E-C04 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.999305341 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c04-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c04-e/current - type: pyaml.magnet.quadrupole name: QD2A-C05 + description: "QD2A-C05 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.997452918 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c05-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c05-a/current - type: pyaml.magnet.quadrupole name: QD2E-C05 + description: "QD2E-C05 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.997993208 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c05-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c05-e/current - type: pyaml.magnet.quadrupole name: QD2A-C06 + description: "QD2A-C06 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.006031322 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c06-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c06-a/current - type: pyaml.magnet.quadrupole name: QD2E-C06 + description: "QD2E-C06 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.998547233 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c06-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c06-e/current - type: pyaml.magnet.quadrupole name: QD2A-C07 + description: "QD2A-C07 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.002327856 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c07-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c07-a/current - type: pyaml.magnet.quadrupole name: QD2E-C07 + description: "QD2E-C07 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.000154369 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c07-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c07-e/current - type: pyaml.magnet.quadrupole name: QD2A-C08 + description: "QD2A-C08 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.009580478 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c08-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c08-a/current - type: pyaml.magnet.quadrupole name: QD2E-C08 + description: "QD2E-C08 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.00447669 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c08-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c08-e/current - type: pyaml.magnet.quadrupole name: QD2A-C09 + description: "QD2A-C09 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.0015563 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c09-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c09-a/current - type: pyaml.magnet.quadrupole name: QD2E-C09 + description: "QD2E-C09 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.997221365 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c09-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c09-e/current - type: pyaml.magnet.quadrupole name: QD2A-C10 + description: "QD2A-C10 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.005954167 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c10-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c10-a/current - type: pyaml.magnet.quadrupole name: QD2E-C10 + description: "QD2E-C10 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.006725723 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c10-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c10-e/current - type: pyaml.magnet.quadrupole name: QD2A-C11 + description: "QD2A-C11 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.994535144 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c11-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c11-a/current - type: pyaml.magnet.quadrupole name: QD2E-C11 + description: "QD2E-C11 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.999550256 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c11-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c11-e/current - type: pyaml.magnet.quadrupole name: QD2A-C12 + description: "QD2A-C12 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.001479145 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c12-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c12-a/current - type: pyaml.magnet.quadrupole name: QD2E-C12 + description: "QD2E-C12 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.000321811 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c12-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c12-e/current - type: pyaml.magnet.quadrupole name: QD2A-C13 + description: "QD2A-C13 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.006715036 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c13-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c13-a/current - type: pyaml.magnet.quadrupole name: QD2E-C13 + description: "QD2E-C13 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.0036395 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c13-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c13-e/current - type: pyaml.magnet.quadrupole name: QD2A-C14 + description: "QD2A-C14 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.997684471 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c14-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c14-a/current - type: pyaml.magnet.quadrupole name: QD2E-C14 + description: "QD2E-C14 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.000385922 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c14-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c14-e/current - type: pyaml.magnet.quadrupole name: QD2A-C15 + description: "QD2A-C15 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.999010167 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c15-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c15-a/current - type: pyaml.magnet.quadrupole name: QD2E-C15 + description: "QD2E-C15 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.998392922 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c15-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c15-e/current - type: pyaml.magnet.quadrupole name: QD2A-C16 + description: "QD2A-C16 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.999318789 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c16-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c16-a/current - type: pyaml.magnet.quadrupole name: QD2E-C16 + description: "QD2E-C16 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.996926967 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c16-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c16-e/current - type: pyaml.magnet.quadrupole name: QD2A-C17 + description: "QD2A-C17 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.000849027 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c17-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c17-a/current - type: pyaml.magnet.quadrupole name: QD2E-C17 + description: "QD2E-C17 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.003392444 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c17-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c17-e/current - type: pyaml.magnet.quadrupole name: QD2A-C18 + description: "QD2A-C18 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.001312133 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c18-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c18-a/current - type: pyaml.magnet.quadrupole name: QD2E-C18 + description: "QD2E-C18 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.005402902 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c18-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c18-e/current - type: pyaml.magnet.quadrupole name: QD2A-C19 + description: "QD2A-C19 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.995846789 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c19-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c19-a/current - type: pyaml.magnet.quadrupole name: QD2E-C19 + description: "QD2E-C19 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.005877011 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c19-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c19-e/current - type: pyaml.magnet.quadrupole name: QD2A-C20 + description: "QD2A-C20 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.001016211 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c20-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c20-a/current - type: pyaml.magnet.quadrupole name: QD2E-C20 + description: "QD2E-C20 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.999010167 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c20-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c20-e/current - type: pyaml.magnet.quadrupole name: QD2A-C21 + description: "QD2A-C21 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.007265811 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c21-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c21-a/current - type: pyaml.magnet.quadrupole name: QD2E-C21 + description: "QD2E-C21 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.998238611 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c21-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c21-e/current - type: pyaml.magnet.quadrupole name: QD2A-C22 + description: "QD2A-C22 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.998161456 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c22-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c22-a/current - type: pyaml.magnet.quadrupole name: QD2E-C22 + description: "QD2E-C22 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.004642522 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c22-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c22-e/current - type: pyaml.magnet.quadrupole name: QD2A-C23 + description: "QD2A-C23 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.001479145 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c23-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c23-a/current - type: pyaml.magnet.quadrupole name: QD2E-C23 + description: "QD2E-C23 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.001942078 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c23-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c23-e/current - type: pyaml.magnet.quadrupole name: QD2A-C24 + description: "QD2A-C24 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.999087322 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c24-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c24-a/current - type: pyaml.magnet.quadrupole name: QD2E-C24 + description: "QD2E-C24 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.998547233 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c24-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c24-e/current - type: pyaml.magnet.quadrupole name: QD2A-C25 + description: "QD2A-C25 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.001698055 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c25-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c25-a/current - type: pyaml.magnet.quadrupole name: QD2E-C25 + description: "QD2E-C25 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.999704567 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c25-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c25-e/current - type: pyaml.magnet.quadrupole name: QD2A-C26 + description: "QD2A-C26 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.999164478 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c26-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c26-a/current - type: pyaml.magnet.quadrupole name: QD2E-C26 + description: "QD2E-C26 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.000694659 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c26-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c26-e/current - type: pyaml.magnet.quadrupole name: QD2A-C27 + description: "QD2A-C27 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.99945971 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c27-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c27-a/current - type: pyaml.magnet.quadrupole name: QD2E-C27 + description: "QD2E-C27 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.999922816 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c27-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c27-e/current - type: pyaml.magnet.quadrupole name: QD2A-C28 + description: "QD2A-C28 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.999922816 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c28-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c28-a/current - type: pyaml.magnet.quadrupole name: QD2E-C28 + description: "QD2E-C28 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.997838839 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c28-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c28-e/current - type: pyaml.magnet.quadrupole name: QD2A-C29 + description: "QD2A-C29 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.003318926 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c29-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c29-a/current - type: pyaml.magnet.quadrupole name: QD2E-C29 + description: "QD2E-C29 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.004179589 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c29-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c29-e/current - type: pyaml.magnet.quadrupole name: QD2A-C30 + description: "QD2A-C30 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.999010167 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c30-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c30-a/current - type: pyaml.magnet.quadrupole name: QD2E-C30 + description: "QD2E-C30 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.9987787 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c30-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c30-e/current - type: pyaml.magnet.quadrupole name: QD2A-C31 + description: "QD2A-C31 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.004411056 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c31-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c31-a/current - type: pyaml.magnet.quadrupole name: QD2E-C31 + description: "QD2E-C31 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.0029451 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c31-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c31-e/current - type: pyaml.magnet.quadrupole name: QD2A-C32 + description: "QD2A-C32 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.009426167 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c32-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c32-a/current - type: pyaml.magnet.quadrupole name: QD2E-C32 + description: "QD2E-C32 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.0050283 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c32-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c32-e/current - type: pyaml.magnet.quadrupole name: QD2A-C01 + description: "QD2A-C01 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.998533498 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c01-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c01-a/current - type: pyaml.magnet.quadrupole name: QD2E-C01 + description: "QD2E-C01 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.003485189 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c01-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c01-e/current - type: pyaml.magnet.quadrupole name: QD2A-C02 + description: "QD2A-C02 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.001389318 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c02-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c02-a/current - type: pyaml.magnet.quadrupole name: QD2E-C02 + description: "QD2E-C02 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.006108478 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c02-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c02-e/current - type: pyaml.magnet.quadrupole name: QD2A-C03 + description: "QD2A-C03 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.002096389 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c03-a/current - unit: A -- type: pyaml.diagnostics.tune_monitor - name: BETATRON_TUNE - tune_h: - type: tango.pyaml.attribute_read_only - attribute: srdiag/beam-tune/main/Qh - unit: mm - tune_v: - type: tango.pyaml.attribute_read_only - attribute: srdiag/beam-tune/main/Qv - unit: mm -- type: pyaml.tuning_tools.tune - name: DEFAULT_TUNE_CORRECTION - quad_array_name: QForTune - betatron_tune_name: BETATRON_TUNE - response_matrix: file:tune_response.json -- type: pyaml.tuning_tools.tune_response_matrix - name: DEFAULT_TUNE_RESPONSE_MATRIX - quad_array_name: QForTune - betatron_tune_name: BETATRON_TUNE - quad_delta: 1e-4 + hardware_unit: A + powerconverter: srmag/vps-qd2/c03-a/current diff --git a/tests/config/EBSTune-range.yaml b/tests/config/EBSTune-range.yaml deleted file mode 100644 index 3f22f1328..000000000 --- a/tests/config/EBSTune-range.yaml +++ /dev/null @@ -1,1777 +0,0 @@ -type: pyaml.accelerator -facility: ESRF -machine: sr -energy: 6e9 -simulators: - - type: pyaml.lattice.simulator - lattice: sr/lattices/ebs.mat - name: design -controls: - - type: tango.pyaml.controlsystem - tango_host: ebs-simu-3:10000 - name: live -data_folder: /data/store -arrays: - - type: pyaml.arrays.magnet - name: QForTune - elements: - - QD2* - - QF1* -devices: -- type: pyaml.magnet.quadrupole - name: QF1E-C04 - model: - type: pyaml.magnet.linear_model - calibration_factor: 1.00054 - crosstalk: 1.0 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QF1_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c04-e/current - unit: A -- type: pyaml.magnet.quadrupole - name: QF1A-C05 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.996841 - crosstalk: 1.0 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QF1_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c05-a/current - unit: A - range: [10,109] -- type: pyaml.magnet.quadrupole - name: QF1E-C05 - model: - type: pyaml.magnet.linear_model - calibration_factor: 1.00191 - crosstalk: 1.0 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QF1_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c05-e/current - unit: A -- type: pyaml.magnet.quadrupole - name: QF1A-C06 - model: - type: pyaml.magnet.linear_model - calibration_factor: 1.0003 - crosstalk: 1.0 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QF1_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c06-a/current - unit: A -- type: pyaml.magnet.quadrupole - name: QF1E-C06 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.997615 - crosstalk: 1.0 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QF1_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c06-e/current - unit: A -- type: pyaml.magnet.quadrupole - name: QF1A-C07 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.998152 - crosstalk: 1.0 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QF1_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c07-a/current - unit: A -- type: pyaml.magnet.quadrupole - name: QF1E-C07 - model: - type: pyaml.magnet.linear_model - calibration_factor: 1.00262 - crosstalk: 1.0 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QF1_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c07-e/current - unit: A -- type: pyaml.magnet.quadrupole - name: QF1A-C08 - model: - type: pyaml.magnet.linear_model - calibration_factor: 1.00319 - crosstalk: 1.0 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QF1_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c08-a/current - unit: A -- type: pyaml.magnet.quadrupole - name: QF1E-C08 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.996180929 - crosstalk: 1.0 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QF1_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c08-e/current - unit: A -- type: pyaml.magnet.quadrupole - name: QF1A-C09 - model: - type: pyaml.magnet.linear_model - calibration_factor: 1.00206 - crosstalk: 1.0 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QF1_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c09-a/current - unit: A -- type: pyaml.magnet.quadrupole - name: QF1E-C09 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.999285 - crosstalk: 1.0 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QF1_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c09-e/current - unit: A -- type: pyaml.magnet.quadrupole - name: QF1A-C10 - model: - type: pyaml.magnet.linear_model - calibration_factor: 1.00232 - crosstalk: 1.0 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QF1_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c10-a/current - unit: A -- type: pyaml.magnet.quadrupole - name: QF1E-C10 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.998212 - crosstalk: 1.0 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QF1_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c10-e/current - unit: A -- type: pyaml.magnet.quadrupole - name: QF1A-C11 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.999225 - crosstalk: 1.0 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QF1_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c11-a/current - unit: A -- type: pyaml.magnet.quadrupole - name: QF1E-C11 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.998033 - crosstalk: 1.0 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QF1_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c11-e/current - unit: A -- type: pyaml.magnet.quadrupole - name: QF1A-C12 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.998748 - crosstalk: 1.0 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QF1_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c12-a/current - unit: A -- type: pyaml.magnet.quadrupole - name: QF1E-C12 - model: - type: pyaml.magnet.linear_model - calibration_factor: 1.0023 - crosstalk: 1.0 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QF1_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c12-e/current - unit: A -- type: pyaml.magnet.quadrupole - name: QF1A-C13 - model: - type: pyaml.magnet.linear_model - calibration_factor: 1.00337 - crosstalk: 1.0 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QF1_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c13-a/current - unit: A -- type: pyaml.magnet.quadrupole - name: QF1E-C13 - model: - type: pyaml.magnet.linear_model - calibration_factor: 1.00403 - crosstalk: 1.0 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QF1_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c13-e/current - unit: A -- type: pyaml.magnet.quadrupole - name: QF1A-C14 - model: - type: pyaml.magnet.linear_model - calibration_factor: 1.00182 - crosstalk: 1.0 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QF1_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c14-a/current - unit: A -- type: pyaml.magnet.quadrupole - name: QF1E-C14 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.998303 - crosstalk: 1.0 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QF1_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c14-e/current - unit: A -- type: pyaml.magnet.quadrupole - name: QF1A-C15 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.998748 - crosstalk: 1.0 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QF1_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c15-a/current - unit: A -- type: pyaml.magnet.quadrupole - name: QF1E-C15 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.994098 - crosstalk: 1.0 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QF1_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c15-e/current - unit: A -- type: pyaml.magnet.quadrupole - name: QF1A-C16 - model: - type: pyaml.magnet.linear_model - calibration_factor: 1.00232 - crosstalk: 1.0 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QF1_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c16-a/current - unit: A -- type: pyaml.magnet.quadrupole - name: QF1E-C16 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.99884 - crosstalk: 1.0 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QF1_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c16-e/current - unit: A -- type: pyaml.magnet.quadrupole - name: QF1A-C17 - model: - type: pyaml.magnet.linear_model - calibration_factor: 1.0079 - crosstalk: 1.0 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QF1_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c17-a/current - unit: A -- type: pyaml.magnet.quadrupole - name: QF1E-C17 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.999523 - crosstalk: 1.0 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QF1_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c17-e/current - unit: A -- type: pyaml.magnet.quadrupole - name: QF1A-C18 - model: - type: pyaml.magnet.linear_model - calibration_factor: 1 - crosstalk: 1.0 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QF1_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c18-a/current - unit: A -- type: pyaml.magnet.quadrupole - name: QF1E-C18 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.999854 - crosstalk: 1.0 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QF1_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c18-e/current - unit: A -- type: pyaml.magnet.quadrupole - name: QF1A-C19 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.99845 - crosstalk: 1.0 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QF1_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c19-a/current - unit: A -- type: pyaml.magnet.quadrupole - name: QF1E-C19 - model: - type: pyaml.magnet.linear_model - calibration_factor: 1 - crosstalk: 1.0 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QF1_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c19-e/current - unit: A -- type: pyaml.magnet.quadrupole - name: QF1A-C20 - model: - type: pyaml.magnet.linear_model - calibration_factor: 1.00095 - crosstalk: 1.0 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QF1_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c20-a/current - unit: A -- type: pyaml.magnet.quadrupole - name: QF1E-C20 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.996753 - crosstalk: 1.0 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QF1_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c20-e/current - unit: A -- type: pyaml.magnet.quadrupole - name: QF1A-C21 - model: - type: pyaml.magnet.linear_model - calibration_factor: 1.00334 - crosstalk: 1.0 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QF1_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c21-a/current - unit: A -- type: pyaml.magnet.quadrupole - name: QF1E-C21 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.997707 - crosstalk: 1.0 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QF1_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c21-e/current - unit: A -- type: pyaml.magnet.quadrupole - name: QF1A-C22 - model: - type: pyaml.magnet.linear_model - calibration_factor: 1.00152 - crosstalk: 1.0 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QF1_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c22-a/current - unit: A -- type: pyaml.magnet.quadrupole - name: QF1E-C22 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.998124 - crosstalk: 1.0 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QF1_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c22-e/current - unit: A -- type: pyaml.magnet.quadrupole - name: QF1A-C23 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.996662 - crosstalk: 1.0 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QF1_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c23-a/current - unit: A -- type: pyaml.magnet.quadrupole - name: QF1E-C23 - model: - type: pyaml.magnet.linear_model - calibration_factor: 1.0017 - crosstalk: 1.0 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QF1_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c23-e/current - unit: A -- type: pyaml.magnet.quadrupole - name: QF1A-C24 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.999642 - crosstalk: 1.0 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QF1_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c24-a/current - unit: A -- type: pyaml.magnet.quadrupole - name: QF1E-C24 - model: - type: pyaml.magnet.linear_model - calibration_factor: 1.00042 - crosstalk: 1.0 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QF1_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c24-e/current - unit: A -- type: pyaml.magnet.quadrupole - name: QF1A-C25 - model: - type: pyaml.magnet.linear_model - calibration_factor: 1.00471 - crosstalk: 1.0 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QF1_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c25-a/current - unit: A -- type: pyaml.magnet.quadrupole - name: QF1E-C25 - model: - type: pyaml.magnet.linear_model - calibration_factor: 1.00393 - crosstalk: 1.0 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QF1_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c25-e/current - unit: A -- type: pyaml.magnet.quadrupole - name: QF1A-C26 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.992906 - crosstalk: 1.0 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QF1_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c26-a/current - unit: A -- type: pyaml.magnet.quadrupole - name: QF1E-C26 - model: - type: pyaml.magnet.linear_model - calibration_factor: 1.00268 - crosstalk: 1.0 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QF1_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c26-e/current - unit: A -- type: pyaml.magnet.quadrupole - name: QF1A-C27 - model: - type: pyaml.magnet.linear_model - calibration_factor: 1.00248 - crosstalk: 1.0 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QF1_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c27-a/current - unit: A -- type: pyaml.magnet.quadrupole - name: QF1E-C27 - model: - type: pyaml.magnet.linear_model - calibration_factor: 1.00203 - crosstalk: 1.0 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QF1_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c27-e/current - unit: A -- type: pyaml.magnet.quadrupole - name: QF1A-C28 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.998030791 - crosstalk: 1.0 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QF1_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c28-a/current - unit: A -- type: pyaml.magnet.quadrupole - name: QF1E-C28 - model: - type: pyaml.magnet.linear_model - calibration_factor: 1.00232 - crosstalk: 1.0 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QF1_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c28-e/current - unit: A -- type: pyaml.magnet.quadrupole - name: QF1A-C29 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.995052 - crosstalk: 1.0 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QF1_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c29-a/current - unit: A -- type: pyaml.magnet.quadrupole - name: QF1E-C29 - model: - type: pyaml.magnet.linear_model - calibration_factor: 1.00155 - crosstalk: 1.0 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QF1_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c29-e/current - unit: A -- type: pyaml.magnet.quadrupole - name: QF1A-C30 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.998271 - crosstalk: 1.0 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QF1_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c30-a/current - unit: A -- type: pyaml.magnet.quadrupole - name: QF1E-C30 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.999702 - crosstalk: 1.0 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QF1_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c30-e/current - unit: A -- type: pyaml.magnet.quadrupole - name: QF1A-C31 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.998005 - crosstalk: 1.0 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QF1_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c31-a/current - unit: A -- type: pyaml.magnet.quadrupole - name: QF1E-C31 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.999463 - crosstalk: 1.0 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QF1_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c31-e/current - unit: A -- type: pyaml.magnet.quadrupole - name: QF1A-C32 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.997794 - crosstalk: 1.0 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QF1_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c32-a/current - unit: A -- type: pyaml.magnet.quadrupole - name: QF1E-C32 - model: - type: pyaml.magnet.linear_model - calibration_factor: 1.00203 - crosstalk: 1.0 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QF1_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c32-e/current - unit: A -- type: pyaml.magnet.quadrupole - name: QF1A-C01 - model: - type: pyaml.magnet.linear_model - calibration_factor: 1.00504 - crosstalk: 1.0 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QF1_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c01-a/current - unit: A -- type: pyaml.magnet.quadrupole - name: QF1E-C01 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.998212 - crosstalk: 1.0 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QF1_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c01-e/current - unit: A -- type: pyaml.magnet.quadrupole - name: QF1A-C02 - model: - type: pyaml.magnet.linear_model - calibration_factor: 1.0037 - crosstalk: 1.0 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QF1_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c02-a/current - unit: A -- type: pyaml.magnet.quadrupole - name: QF1E-C02 - model: - type: pyaml.magnet.linear_model - calibration_factor: 1.00093 - crosstalk: 1.0 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QF1_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c02-e/current - unit: A -- type: pyaml.magnet.quadrupole - name: QF1A-C03 - model: - type: pyaml.magnet.linear_model - calibration_factor: 1.0025 - crosstalk: 1.0 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QF1_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c03-a/current - unit: A -- type: pyaml.magnet.quadrupole - name: QD2E-C04 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.999305341 - crosstalk: 0.99912 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QD2_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c04-e/current - unit: A -- type: pyaml.magnet.quadrupole - name: QD2A-C05 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.997452918 - crosstalk: 0.99912 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QD2_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c05-a/current - unit: A -- type: pyaml.magnet.quadrupole - name: QD2E-C05 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.997993208 - crosstalk: 0.99912 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QD2_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c05-e/current - unit: A -- type: pyaml.magnet.quadrupole - name: QD2A-C06 - model: - type: pyaml.magnet.linear_model - calibration_factor: 1.006031322 - crosstalk: 0.99912 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QD2_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c06-a/current - unit: A -- type: pyaml.magnet.quadrupole - name: QD2E-C06 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.998547233 - crosstalk: 0.99912 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QD2_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c06-e/current - unit: A -- type: pyaml.magnet.quadrupole - name: QD2A-C07 - model: - type: pyaml.magnet.linear_model - calibration_factor: 1.002327856 - crosstalk: 0.99912 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QD2_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c07-a/current - unit: A -- type: pyaml.magnet.quadrupole - name: QD2E-C07 - model: - type: pyaml.magnet.linear_model - calibration_factor: 1.000154369 - crosstalk: 0.99912 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QD2_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c07-e/current - unit: A -- type: pyaml.magnet.quadrupole - name: QD2A-C08 - model: - type: pyaml.magnet.linear_model - calibration_factor: 1.009580478 - crosstalk: 0.99912 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QD2_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c08-a/current - unit: A -- type: pyaml.magnet.quadrupole - name: QD2E-C08 - model: - type: pyaml.magnet.linear_model - calibration_factor: 1.00447669 - crosstalk: 0.99912 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QD2_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c08-e/current - unit: A -- type: pyaml.magnet.quadrupole - name: QD2A-C09 - model: - type: pyaml.magnet.linear_model - calibration_factor: 1.0015563 - crosstalk: 0.99912 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QD2_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c09-a/current - unit: A -- type: pyaml.magnet.quadrupole - name: QD2E-C09 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.997221365 - crosstalk: 0.99912 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QD2_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c09-e/current - unit: A -- type: pyaml.magnet.quadrupole - name: QD2A-C10 - model: - type: pyaml.magnet.linear_model - calibration_factor: 1.005954167 - crosstalk: 0.99912 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QD2_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c10-a/current - unit: A -- type: pyaml.magnet.quadrupole - name: QD2E-C10 - model: - type: pyaml.magnet.linear_model - calibration_factor: 1.006725723 - crosstalk: 0.99912 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QD2_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c10-e/current - unit: A -- type: pyaml.magnet.quadrupole - name: QD2A-C11 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.994535144 - crosstalk: 0.99912 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QD2_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c11-a/current - unit: A -- type: pyaml.magnet.quadrupole - name: QD2E-C11 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.999550256 - crosstalk: 0.99912 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QD2_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c11-e/current - unit: A -- type: pyaml.magnet.quadrupole - name: QD2A-C12 - model: - type: pyaml.magnet.linear_model - calibration_factor: 1.001479145 - crosstalk: 0.99912 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QD2_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c12-a/current - unit: A -- type: pyaml.magnet.quadrupole - name: QD2E-C12 - model: - type: pyaml.magnet.linear_model - calibration_factor: 1.000321811 - crosstalk: 0.99912 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QD2_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c12-e/current - unit: A -- type: pyaml.magnet.quadrupole - name: QD2A-C13 - model: - type: pyaml.magnet.linear_model - calibration_factor: 1.006715036 - crosstalk: 0.99912 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QD2_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c13-a/current - unit: A -- type: pyaml.magnet.quadrupole - name: QD2E-C13 - model: - type: pyaml.magnet.linear_model - calibration_factor: 1.0036395 - crosstalk: 0.99912 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QD2_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c13-e/current - unit: A -- type: pyaml.magnet.quadrupole - name: QD2A-C14 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.997684471 - crosstalk: 0.99912 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QD2_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c14-a/current - unit: A -- type: pyaml.magnet.quadrupole - name: QD2E-C14 - model: - type: pyaml.magnet.linear_model - calibration_factor: 1.000385922 - crosstalk: 0.99912 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QD2_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c14-e/current - unit: A -- type: pyaml.magnet.quadrupole - name: QD2A-C15 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.999010167 - crosstalk: 0.99912 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QD2_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c15-a/current - unit: A -- type: pyaml.magnet.quadrupole - name: QD2E-C15 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.998392922 - crosstalk: 0.99912 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QD2_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c15-e/current - unit: A -- type: pyaml.magnet.quadrupole - name: QD2A-C16 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.999318789 - crosstalk: 0.99912 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QD2_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c16-a/current - unit: A -- type: pyaml.magnet.quadrupole - name: QD2E-C16 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.996926967 - crosstalk: 0.99912 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QD2_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c16-e/current - unit: A -- type: pyaml.magnet.quadrupole - name: QD2A-C17 - model: - type: pyaml.magnet.linear_model - calibration_factor: 1.000849027 - crosstalk: 0.99912 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QD2_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c17-a/current - unit: A -- type: pyaml.magnet.quadrupole - name: QD2E-C17 - model: - type: pyaml.magnet.linear_model - calibration_factor: 1.003392444 - crosstalk: 0.99912 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QD2_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c17-e/current - unit: A -- type: pyaml.magnet.quadrupole - name: QD2A-C18 - model: - type: pyaml.magnet.linear_model - calibration_factor: 1.001312133 - crosstalk: 0.99912 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QD2_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c18-a/current - unit: A -- type: pyaml.magnet.quadrupole - name: QD2E-C18 - model: - type: pyaml.magnet.linear_model - calibration_factor: 1.005402902 - crosstalk: 0.99912 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QD2_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c18-e/current - unit: A -- type: pyaml.magnet.quadrupole - name: QD2A-C19 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.995846789 - crosstalk: 0.99912 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QD2_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c19-a/current - unit: A -- type: pyaml.magnet.quadrupole - name: QD2E-C19 - model: - type: pyaml.magnet.linear_model - calibration_factor: 1.005877011 - crosstalk: 0.99912 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QD2_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c19-e/current - unit: A -- type: pyaml.magnet.quadrupole - name: QD2A-C20 - model: - type: pyaml.magnet.linear_model - calibration_factor: 1.001016211 - crosstalk: 0.99912 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QD2_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c20-a/current - unit: A -- type: pyaml.magnet.quadrupole - name: QD2E-C20 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.999010167 - crosstalk: 0.99912 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QD2_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c20-e/current - unit: A -- type: pyaml.magnet.quadrupole - name: QD2A-C21 - model: - type: pyaml.magnet.linear_model - calibration_factor: 1.007265811 - crosstalk: 0.99912 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QD2_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c21-a/current - unit: A -- type: pyaml.magnet.quadrupole - name: QD2E-C21 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.998238611 - crosstalk: 0.99912 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QD2_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c21-e/current - unit: A -- type: pyaml.magnet.quadrupole - name: QD2A-C22 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.998161456 - crosstalk: 0.99912 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QD2_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c22-a/current - unit: A -- type: pyaml.magnet.quadrupole - name: QD2E-C22 - model: - type: pyaml.magnet.linear_model - calibration_factor: 1.004642522 - crosstalk: 0.99912 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QD2_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c22-e/current - unit: A -- type: pyaml.magnet.quadrupole - name: QD2A-C23 - model: - type: pyaml.magnet.linear_model - calibration_factor: 1.001479145 - crosstalk: 0.99912 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QD2_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c23-a/current - unit: A -- type: pyaml.magnet.quadrupole - name: QD2E-C23 - model: - type: pyaml.magnet.linear_model - calibration_factor: 1.001942078 - crosstalk: 0.99912 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QD2_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c23-e/current - unit: A -- type: pyaml.magnet.quadrupole - name: QD2A-C24 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.999087322 - crosstalk: 0.99912 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QD2_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c24-a/current - unit: A -- type: pyaml.magnet.quadrupole - name: QD2E-C24 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.998547233 - crosstalk: 0.99912 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QD2_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c24-e/current - unit: A -- type: pyaml.magnet.quadrupole - name: QD2A-C25 - model: - type: pyaml.magnet.linear_model - calibration_factor: 1.001698055 - crosstalk: 0.99912 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QD2_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c25-a/current - unit: A -- type: pyaml.magnet.quadrupole - name: QD2E-C25 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.999704567 - crosstalk: 0.99912 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QD2_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c25-e/current - unit: A -- type: pyaml.magnet.quadrupole - name: QD2A-C26 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.999164478 - crosstalk: 0.99912 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QD2_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c26-a/current - unit: A -- type: pyaml.magnet.quadrupole - name: QD2E-C26 - model: - type: pyaml.magnet.linear_model - calibration_factor: 1.000694659 - crosstalk: 0.99912 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QD2_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c26-e/current - unit: A -- type: pyaml.magnet.quadrupole - name: QD2A-C27 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.99945971 - crosstalk: 0.99912 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QD2_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c27-a/current - unit: A -- type: pyaml.magnet.quadrupole - name: QD2E-C27 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.999922816 - crosstalk: 0.99912 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QD2_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c27-e/current - unit: A -- type: pyaml.magnet.quadrupole - name: QD2A-C28 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.999922816 - crosstalk: 0.99912 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QD2_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c28-a/current - unit: A -- type: pyaml.magnet.quadrupole - name: QD2E-C28 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.997838839 - crosstalk: 0.99912 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QD2_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c28-e/current - unit: A -- type: pyaml.magnet.quadrupole - name: QD2A-C29 - model: - type: pyaml.magnet.linear_model - calibration_factor: 1.003318926 - crosstalk: 0.99912 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QD2_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c29-a/current - unit: A -- type: pyaml.magnet.quadrupole - name: QD2E-C29 - model: - type: pyaml.magnet.linear_model - calibration_factor: 1.004179589 - crosstalk: 0.99912 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QD2_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c29-e/current - unit: A -- type: pyaml.magnet.quadrupole - name: QD2A-C30 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.999010167 - crosstalk: 0.99912 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QD2_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c30-a/current - unit: A -- type: pyaml.magnet.quadrupole - name: QD2E-C30 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.9987787 - crosstalk: 0.99912 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QD2_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c30-e/current - unit: A -- type: pyaml.magnet.quadrupole - name: QD2A-C31 - model: - type: pyaml.magnet.linear_model - calibration_factor: 1.004411056 - crosstalk: 0.99912 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QD2_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c31-a/current - unit: A -- type: pyaml.magnet.quadrupole - name: QD2E-C31 - model: - type: pyaml.magnet.linear_model - calibration_factor: 1.0029451 - crosstalk: 0.99912 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QD2_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c31-e/current - unit: A -- type: pyaml.magnet.quadrupole - name: QD2A-C32 - model: - type: pyaml.magnet.linear_model - calibration_factor: 1.009426167 - crosstalk: 0.99912 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QD2_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c32-a/current - unit: A -- type: pyaml.magnet.quadrupole - name: QD2E-C32 - model: - type: pyaml.magnet.linear_model - calibration_factor: 1.0050283 - crosstalk: 0.99912 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QD2_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c32-e/current - unit: A -- type: pyaml.magnet.quadrupole - name: QD2A-C01 - model: - type: pyaml.magnet.linear_model - calibration_factor: 0.998533498 - crosstalk: 0.99912 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QD2_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c01-a/current - unit: A -- type: pyaml.magnet.quadrupole - name: QD2E-C01 - model: - type: pyaml.magnet.linear_model - calibration_factor: 1.003485189 - crosstalk: 0.99912 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QD2_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c01-e/current - unit: A -- type: pyaml.magnet.quadrupole - name: QD2A-C02 - model: - type: pyaml.magnet.linear_model - calibration_factor: 1.001389318 - crosstalk: 0.99912 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QD2_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c02-a/current - unit: A -- type: pyaml.magnet.quadrupole - name: QD2E-C02 - model: - type: pyaml.magnet.linear_model - calibration_factor: 1.006108478 - crosstalk: 0.99912 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QD2_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c02-e/current - unit: A -- type: pyaml.magnet.quadrupole - name: QD2A-C03 - model: - type: pyaml.magnet.linear_model - calibration_factor: 1.002096389 - crosstalk: 0.99912 - curve: - type: pyaml.configuration.csvcurve - file: sr/magnet_models/QD2_strength.csv - unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c03-a/current - unit: A -- type: pyaml.diagnostics.tune_monitor - name: BETATRON_TUNE - tune_h: - type: tango.pyaml.attribute_read_only - attribute: srdiag/beam-tune/main/Qh - unit: mm - tune_v: - type: tango.pyaml.attribute_read_only - attribute: srdiag/beam-tune/main/Qv - unit: mm -- type: pyaml.tuning_tools.tune - name: DEFAULT_TUNE_CORRECTION - quad_array_name: QForTune - betatron_tune_name: BETATRON_TUNE - response_matrix: file:tune_response.json -- type: pyaml.tuning_tools.tune_response_matrix - name: DEFAULT_TUNE_RESPONSE_MATRIX - quad_array_name: QForTune - betatron_tune_name: BETATRON_TUNE - quad_delta: 1e-4 diff --git a/tests/config/EBSTune.yaml b/tests/config/EBSTune.yaml index a631c34d4..f5a8d5c08 100644 --- a/tests/config/EBSTune.yaml +++ b/tests/config/EBSTune.yaml @@ -5,13 +5,14 @@ energy: 6e9 description: "Accelerator configuration for EBS storage ring" simulators: - type: pyaml.lattice.simulator - description: "EBS lattice" lattice: sr/lattices/ebs.mat name: design + description: "EBS lattice" controls: - type: tango.pyaml.controlsystem tango_host: ebs-simu-3:10000 name: live + catalog: catalogs/ebs_catalogs.yaml data_folder: /data/store arrays: - type: pyaml.arrays.magnet @@ -20,1760 +21,1629 @@ arrays: - QD2* - QF1* devices: +- type: pyaml.diagnostics.tune_monitor + name: BETATRON_TUNE + tune_h: srdiag/beam-tune/main/Qh + tune_v: srdiag/beam-tune/main/Qv +- type: pyaml.tuning_tools.tune + name: DEFAULT_TUNE_CORRECTION + quad_array_name: QForTune + betatron_tune_name: BETATRON_TUNE + response_matrix: ${path:tune_response.json} +- type: pyaml.tuning_tools.tune_response_matrix + name: DEFAULT_TUNE_RESPONSE_MATRIX + quad_array_name: QForTune + betatron_tune_name: BETATRON_TUNE + quad_delta: 1e-4 - type: pyaml.magnet.quadrupole - description: "QF1E-C04 quadrupole" name: QF1E-C04 + description: "QF1E-C04 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.00054 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c04-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c04-e/current - type: pyaml.magnet.quadrupole name: QF1A-C05 + description: "QF1A-C05 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.996841 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c05-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c05-a/current - type: pyaml.magnet.quadrupole name: QF1E-C05 + description: "QF1E-C05 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.00191 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c05-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c05-e/current - type: pyaml.magnet.quadrupole name: QF1A-C06 + description: "QF1A-C06 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.0003 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c06-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c06-a/current - type: pyaml.magnet.quadrupole name: QF1E-C06 + description: "QF1E-C06 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.997615 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c06-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c06-e/current - type: pyaml.magnet.quadrupole name: QF1A-C07 + description: "QF1A-C07 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.998152 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c07-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c07-a/current - type: pyaml.magnet.quadrupole name: QF1E-C07 + description: "QF1E-C07 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.00262 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c07-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c07-e/current - type: pyaml.magnet.quadrupole name: QF1A-C08 + description: "QF1A-C08 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.00319 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c08-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c08-a/current - type: pyaml.magnet.quadrupole name: QF1E-C08 + description: "QF1E-C08 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.996180929 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c08-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c08-e/current - type: pyaml.magnet.quadrupole name: QF1A-C09 + description: "QF1A-C09 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.00206 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c09-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c09-a/current - type: pyaml.magnet.quadrupole name: QF1E-C09 + description: "QF1E-C09 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.999285 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c09-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c09-e/current - type: pyaml.magnet.quadrupole name: QF1A-C10 + description: "QF1A-C10 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.00232 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c10-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c10-a/current - type: pyaml.magnet.quadrupole name: QF1E-C10 + description: "QF1E-C10 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.998212 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c10-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c10-e/current - type: pyaml.magnet.quadrupole name: QF1A-C11 + description: "QF1A-C11 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.999225 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c11-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c11-a/current - type: pyaml.magnet.quadrupole name: QF1E-C11 + description: "QF1E-C11 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.998033 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c11-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c11-e/current - type: pyaml.magnet.quadrupole name: QF1A-C12 + description: "QF1A-C12 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.998748 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c12-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c12-a/current - type: pyaml.magnet.quadrupole name: QF1E-C12 + description: "QF1E-C12 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.0023 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c12-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c12-e/current - type: pyaml.magnet.quadrupole name: QF1A-C13 + description: "QF1A-C13 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.00337 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c13-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c13-a/current - type: pyaml.magnet.quadrupole name: QF1E-C13 + description: "QF1E-C13 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.00403 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c13-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c13-e/current - type: pyaml.magnet.quadrupole name: QF1A-C14 + description: "QF1A-C14 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.00182 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c14-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c14-a/current - type: pyaml.magnet.quadrupole name: QF1E-C14 + description: "QF1E-C14 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.998303 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c14-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c14-e/current - type: pyaml.magnet.quadrupole name: QF1A-C15 + description: "QF1A-C15 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.998748 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c15-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c15-a/current - type: pyaml.magnet.quadrupole name: QF1E-C15 + description: "QF1E-C15 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.994098 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c15-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c15-e/current - type: pyaml.magnet.quadrupole name: QF1A-C16 + description: "QF1A-C16 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.00232 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c16-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c16-a/current - type: pyaml.magnet.quadrupole name: QF1E-C16 + description: "QF1E-C16 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.99884 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c16-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c16-e/current - type: pyaml.magnet.quadrupole name: QF1A-C17 + description: "QF1A-C17 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.0079 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c17-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c17-a/current - type: pyaml.magnet.quadrupole name: QF1E-C17 + description: "QF1E-C17 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.999523 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c17-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c17-e/current - type: pyaml.magnet.quadrupole name: QF1A-C18 + description: "QF1A-C18 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c18-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c18-a/current - type: pyaml.magnet.quadrupole name: QF1E-C18 + description: "QF1E-C18 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.999854 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c18-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c18-e/current - type: pyaml.magnet.quadrupole name: QF1A-C19 + description: "QF1A-C19 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.99845 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c19-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c19-a/current - type: pyaml.magnet.quadrupole name: QF1E-C19 + description: "QF1E-C19 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c19-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c19-e/current - type: pyaml.magnet.quadrupole name: QF1A-C20 + description: "QF1A-C20 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.00095 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c20-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c20-a/current - type: pyaml.magnet.quadrupole name: QF1E-C20 + description: "QF1E-C20 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.996753 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c20-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c20-e/current - type: pyaml.magnet.quadrupole name: QF1A-C21 + description: "QF1A-C21 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.00334 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c21-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c21-a/current - type: pyaml.magnet.quadrupole name: QF1E-C21 + description: "QF1E-C21 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.997707 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c21-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c21-e/current - type: pyaml.magnet.quadrupole name: QF1A-C22 + description: "QF1A-C22 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.00152 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c22-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c22-a/current - type: pyaml.magnet.quadrupole name: QF1E-C22 + description: "QF1E-C22 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.998124 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c22-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c22-e/current - type: pyaml.magnet.quadrupole name: QF1A-C23 + description: "QF1A-C23 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.996662 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c23-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c23-a/current - type: pyaml.magnet.quadrupole name: QF1E-C23 + description: "QF1E-C23 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.0017 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c23-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c23-e/current - type: pyaml.magnet.quadrupole name: QF1A-C24 + description: "QF1A-C24 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.999642 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c24-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c24-a/current - type: pyaml.magnet.quadrupole name: QF1E-C24 + description: "QF1E-C24 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.00042 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c24-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c24-e/current - type: pyaml.magnet.quadrupole name: QF1A-C25 + description: "QF1A-C25 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.00471 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c25-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c25-a/current - type: pyaml.magnet.quadrupole name: QF1E-C25 + description: "QF1E-C25 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.00393 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c25-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c25-e/current - type: pyaml.magnet.quadrupole name: QF1A-C26 + description: "QF1A-C26 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.992906 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c26-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c26-a/current - type: pyaml.magnet.quadrupole name: QF1E-C26 + description: "QF1E-C26 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.00268 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c26-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c26-e/current - type: pyaml.magnet.quadrupole name: QF1A-C27 + description: "QF1A-C27 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.00248 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c27-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c27-a/current - type: pyaml.magnet.quadrupole name: QF1E-C27 + description: "QF1E-C27 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.00203 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c27-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c27-e/current - type: pyaml.magnet.quadrupole name: QF1A-C28 + description: "QF1A-C28 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.998030791 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c28-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c28-a/current - type: pyaml.magnet.quadrupole name: QF1E-C28 + description: "QF1E-C28 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.00232 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c28-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c28-e/current - type: pyaml.magnet.quadrupole name: QF1A-C29 + description: "QF1A-C29 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.995052 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c29-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c29-a/current - type: pyaml.magnet.quadrupole name: QF1E-C29 + description: "QF1E-C29 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.00155 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c29-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c29-e/current - type: pyaml.magnet.quadrupole name: QF1A-C30 + description: "QF1A-C30 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.998271 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c30-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c30-a/current - type: pyaml.magnet.quadrupole name: QF1E-C30 + description: "QF1E-C30 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.999702 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c30-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c30-e/current - type: pyaml.magnet.quadrupole name: QF1A-C31 + description: "QF1A-C31 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.998005 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c31-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c31-a/current - type: pyaml.magnet.quadrupole name: QF1E-C31 + description: "QF1E-C31 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.999463 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c31-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c31-e/current - type: pyaml.magnet.quadrupole name: QF1A-C32 + description: "QF1A-C32 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.997794 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c32-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c32-a/current - type: pyaml.magnet.quadrupole name: QF1E-C32 + description: "QF1E-C32 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.00203 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c32-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c32-e/current - type: pyaml.magnet.quadrupole name: QF1A-C01 + description: "QF1A-C01 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.00504 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c01-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c01-a/current - type: pyaml.magnet.quadrupole name: QF1E-C01 + description: "QF1E-C01 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.998212 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c01-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c01-e/current - type: pyaml.magnet.quadrupole name: QF1A-C02 + description: "QF1A-C02 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.0037 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c02-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c02-a/current - type: pyaml.magnet.quadrupole name: QF1E-C02 + description: "QF1E-C02 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.00093 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c02-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c02-e/current - type: pyaml.magnet.quadrupole name: QF1A-C03 + description: "QF1A-C03 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.0025 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qf1/c03-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qf1/c03-a/current - type: pyaml.magnet.quadrupole name: QD2E-C04 + description: "QD2E-C04 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.999305341 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c04-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c04-e/current - type: pyaml.magnet.quadrupole name: QD2A-C05 + description: "QD2A-C05 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.997452918 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c05-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c05-a/current - type: pyaml.magnet.quadrupole name: QD2E-C05 + description: "QD2E-C05 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.997993208 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c05-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c05-e/current - type: pyaml.magnet.quadrupole name: QD2A-C06 + description: "QD2A-C06 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.006031322 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c06-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c06-a/current - type: pyaml.magnet.quadrupole name: QD2E-C06 + description: "QD2E-C06 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.998547233 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c06-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c06-e/current - type: pyaml.magnet.quadrupole name: QD2A-C07 + description: "QD2A-C07 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.002327856 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c07-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c07-a/current - type: pyaml.magnet.quadrupole name: QD2E-C07 + description: "QD2E-C07 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.000154369 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c07-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c07-e/current - type: pyaml.magnet.quadrupole name: QD2A-C08 + description: "QD2A-C08 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.009580478 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c08-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c08-a/current - type: pyaml.magnet.quadrupole name: QD2E-C08 + description: "QD2E-C08 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.00447669 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c08-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c08-e/current - type: pyaml.magnet.quadrupole name: QD2A-C09 + description: "QD2A-C09 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.0015563 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c09-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c09-a/current - type: pyaml.magnet.quadrupole name: QD2E-C09 + description: "QD2E-C09 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.997221365 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c09-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c09-e/current - type: pyaml.magnet.quadrupole name: QD2A-C10 + description: "QD2A-C10 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.005954167 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c10-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c10-a/current - type: pyaml.magnet.quadrupole name: QD2E-C10 + description: "QD2E-C10 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.006725723 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c10-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c10-e/current - type: pyaml.magnet.quadrupole name: QD2A-C11 + description: "QD2A-C11 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.994535144 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c11-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c11-a/current - type: pyaml.magnet.quadrupole name: QD2E-C11 + description: "QD2E-C11 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.999550256 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c11-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c11-e/current - type: pyaml.magnet.quadrupole name: QD2A-C12 + description: "QD2A-C12 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.001479145 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c12-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c12-a/current - type: pyaml.magnet.quadrupole name: QD2E-C12 + description: "QD2E-C12 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.000321811 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c12-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c12-e/current - type: pyaml.magnet.quadrupole name: QD2A-C13 + description: "QD2A-C13 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.006715036 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c13-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c13-a/current - type: pyaml.magnet.quadrupole name: QD2E-C13 + description: "QD2E-C13 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.0036395 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c13-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c13-e/current - type: pyaml.magnet.quadrupole name: QD2A-C14 + description: "QD2A-C14 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.997684471 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c14-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c14-a/current - type: pyaml.magnet.quadrupole name: QD2E-C14 + description: "QD2E-C14 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.000385922 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c14-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c14-e/current - type: pyaml.magnet.quadrupole name: QD2A-C15 + description: "QD2A-C15 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.999010167 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c15-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c15-a/current - type: pyaml.magnet.quadrupole name: QD2E-C15 + description: "QD2E-C15 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.998392922 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c15-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c15-e/current - type: pyaml.magnet.quadrupole name: QD2A-C16 + description: "QD2A-C16 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.999318789 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c16-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c16-a/current - type: pyaml.magnet.quadrupole name: QD2E-C16 + description: "QD2E-C16 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.996926967 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c16-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c16-e/current - type: pyaml.magnet.quadrupole name: QD2A-C17 + description: "QD2A-C17 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.000849027 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c17-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c17-a/current - type: pyaml.magnet.quadrupole name: QD2E-C17 + description: "QD2E-C17 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.003392444 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c17-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c17-e/current - type: pyaml.magnet.quadrupole name: QD2A-C18 + description: "QD2A-C18 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.001312133 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c18-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c18-a/current - type: pyaml.magnet.quadrupole name: QD2E-C18 + description: "QD2E-C18 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.005402902 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c18-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c18-e/current - type: pyaml.magnet.quadrupole name: QD2A-C19 + description: "QD2A-C19 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.995846789 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c19-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c19-a/current - type: pyaml.magnet.quadrupole name: QD2E-C19 + description: "QD2E-C19 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.005877011 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c19-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c19-e/current - type: pyaml.magnet.quadrupole name: QD2A-C20 + description: "QD2A-C20 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.001016211 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c20-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c20-a/current - type: pyaml.magnet.quadrupole name: QD2E-C20 + description: "QD2E-C20 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.999010167 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c20-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c20-e/current - type: pyaml.magnet.quadrupole name: QD2A-C21 + description: "QD2A-C21 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.007265811 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c21-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c21-a/current - type: pyaml.magnet.quadrupole name: QD2E-C21 + description: "QD2E-C21 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.998238611 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c21-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c21-e/current - type: pyaml.magnet.quadrupole name: QD2A-C22 + description: "QD2A-C22 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.998161456 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c22-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c22-a/current - type: pyaml.magnet.quadrupole name: QD2E-C22 + description: "QD2E-C22 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.004642522 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c22-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c22-e/current - type: pyaml.magnet.quadrupole name: QD2A-C23 + description: "QD2A-C23 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.001479145 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c23-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c23-a/current - type: pyaml.magnet.quadrupole name: QD2E-C23 + description: "QD2E-C23 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.001942078 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c23-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c23-e/current - type: pyaml.magnet.quadrupole name: QD2A-C24 + description: "QD2A-C24 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.999087322 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c24-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c24-a/current - type: pyaml.magnet.quadrupole name: QD2E-C24 + description: "QD2E-C24 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.998547233 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c24-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c24-e/current - type: pyaml.magnet.quadrupole name: QD2A-C25 + description: "QD2A-C25 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.001698055 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c25-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c25-a/current - type: pyaml.magnet.quadrupole name: QD2E-C25 + description: "QD2E-C25 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.999704567 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c25-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c25-e/current - type: pyaml.magnet.quadrupole name: QD2A-C26 + description: "QD2A-C26 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.999164478 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c26-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c26-a/current - type: pyaml.magnet.quadrupole name: QD2E-C26 + description: "QD2E-C26 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.000694659 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c26-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c26-e/current - type: pyaml.magnet.quadrupole name: QD2A-C27 + description: "QD2A-C27 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.99945971 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c27-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c27-a/current - type: pyaml.magnet.quadrupole name: QD2E-C27 + description: "QD2E-C27 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.999922816 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c27-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c27-e/current - type: pyaml.magnet.quadrupole name: QD2A-C28 + description: "QD2A-C28 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.999922816 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c28-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c28-a/current - type: pyaml.magnet.quadrupole name: QD2E-C28 + description: "QD2E-C28 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.997838839 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c28-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c28-e/current - type: pyaml.magnet.quadrupole name: QD2A-C29 + description: "QD2A-C29 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.003318926 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c29-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c29-a/current - type: pyaml.magnet.quadrupole name: QD2E-C29 + description: "QD2E-C29 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.004179589 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c29-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c29-e/current - type: pyaml.magnet.quadrupole name: QD2A-C30 + description: "QD2A-C30 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.999010167 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c30-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c30-a/current - type: pyaml.magnet.quadrupole name: QD2E-C30 + description: "QD2E-C30 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.9987787 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c30-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c30-e/current - type: pyaml.magnet.quadrupole name: QD2A-C31 + description: "QD2A-C31 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.004411056 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c31-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c31-a/current - type: pyaml.magnet.quadrupole name: QD2E-C31 + description: "QD2E-C31 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.0029451 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c31-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c31-e/current - type: pyaml.magnet.quadrupole name: QD2A-C32 + description: "QD2A-C32 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.009426167 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c32-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c32-a/current - type: pyaml.magnet.quadrupole name: QD2E-C32 + description: "QD2E-C32 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.0050283 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c32-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c32-e/current - type: pyaml.magnet.quadrupole name: QD2A-C01 + description: "QD2A-C01 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 0.998533498 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c01-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c01-a/current - type: pyaml.magnet.quadrupole name: QD2E-C01 + description: "QD2E-C01 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.003485189 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c01-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c01-e/current - type: pyaml.magnet.quadrupole name: QD2A-C02 + description: "QD2A-C02 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.001389318 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c02-a/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c02-a/current - type: pyaml.magnet.quadrupole name: QD2E-C02 + description: "QD2E-C02 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.006108478 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c02-e/current - unit: A + hardware_unit: A + powerconverter: srmag/vps-qd2/c02-e/current - type: pyaml.magnet.quadrupole name: QD2A-C03 + description: "QD2A-C03 quadrupole" model: type: pyaml.magnet.linear_model calibration_factor: 1.002096389 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/vps-qd2/c03-a/current - unit: A -- type: pyaml.diagnostics.tune_monitor - name: BETATRON_TUNE - tune_h: - type: tango.pyaml.attribute_read_only - attribute: srdiag/beam-tune/main/Qh - unit: mm - tune_v: - type: tango.pyaml.attribute_read_only - attribute: srdiag/beam-tune/main/Qv - unit: mm -- type: pyaml.tuning_tools.tune - name: DEFAULT_TUNE_CORRECTION - quad_array_name: QForTune - betatron_tune_name: BETATRON_TUNE - response_matrix: file:tune_response.json -- type: pyaml.tuning_tools.tune_response_matrix - name: DEFAULT_TUNE_RESPONSE_MATRIX - quad_array_name: QForTune - betatron_tune_name: BETATRON_TUNE - quad_delta: 1e-4 + hardware_unit: A + powerconverter: srmag/vps-qd2/c03-a/current diff --git a/tests/config/EBSTuneOATango.yaml b/tests/config/EBSTuneOATango.yaml index adb7be831..dae87e8d6 100644 --- a/tests/config/EBSTuneOATango.yaml +++ b/tests/config/EBSTuneOATango.yaml @@ -147,7 +147,7 @@ devices: calibration_factor: 1.00054 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m powerconverter: @@ -162,7 +162,7 @@ devices: calibration_factor: 0.996841 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m powerconverter: @@ -177,7 +177,7 @@ devices: calibration_factor: 1.00191 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m powerconverter: @@ -192,7 +192,7 @@ devices: calibration_factor: 1.0003 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m powerconverter: @@ -207,7 +207,7 @@ devices: calibration_factor: 0.997615 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m powerconverter: @@ -222,7 +222,7 @@ devices: calibration_factor: 0.998152 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m powerconverter: @@ -237,7 +237,7 @@ devices: calibration_factor: 1.00262 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m powerconverter: @@ -252,7 +252,7 @@ devices: calibration_factor: 1.00319 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m powerconverter: @@ -267,7 +267,7 @@ devices: calibration_factor: 0.996180929 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m powerconverter: @@ -282,7 +282,7 @@ devices: calibration_factor: 1.00206 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m powerconverter: @@ -297,7 +297,7 @@ devices: calibration_factor: 0.999285 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m powerconverter: @@ -312,7 +312,7 @@ devices: calibration_factor: 1.00232 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m powerconverter: @@ -327,7 +327,7 @@ devices: calibration_factor: 0.998212 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m powerconverter: @@ -342,7 +342,7 @@ devices: calibration_factor: 0.999225 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m powerconverter: @@ -357,7 +357,7 @@ devices: calibration_factor: 0.998033 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m powerconverter: @@ -372,7 +372,7 @@ devices: calibration_factor: 0.998748 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m powerconverter: @@ -387,7 +387,7 @@ devices: calibration_factor: 1.0023 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m powerconverter: @@ -402,7 +402,7 @@ devices: calibration_factor: 1.00337 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m powerconverter: @@ -417,7 +417,7 @@ devices: calibration_factor: 1.00403 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m powerconverter: @@ -432,7 +432,7 @@ devices: calibration_factor: 1.00182 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m powerconverter: @@ -447,7 +447,7 @@ devices: calibration_factor: 0.998303 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m powerconverter: @@ -462,7 +462,7 @@ devices: calibration_factor: 0.998748 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m powerconverter: @@ -477,7 +477,7 @@ devices: calibration_factor: 0.994098 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m powerconverter: @@ -492,7 +492,7 @@ devices: calibration_factor: 1.00232 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m powerconverter: @@ -507,7 +507,7 @@ devices: calibration_factor: 0.99884 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m powerconverter: @@ -522,7 +522,7 @@ devices: calibration_factor: 1.0079 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m powerconverter: @@ -537,7 +537,7 @@ devices: calibration_factor: 0.999523 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m powerconverter: @@ -552,7 +552,7 @@ devices: calibration_factor: 1 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m powerconverter: @@ -567,7 +567,7 @@ devices: calibration_factor: 0.999854 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m powerconverter: @@ -582,7 +582,7 @@ devices: calibration_factor: 0.99845 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m powerconverter: @@ -597,7 +597,7 @@ devices: calibration_factor: 1 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m powerconverter: @@ -612,7 +612,7 @@ devices: calibration_factor: 1.00095 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m powerconverter: @@ -627,7 +627,7 @@ devices: calibration_factor: 0.996753 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m powerconverter: @@ -642,7 +642,7 @@ devices: calibration_factor: 1.00334 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m powerconverter: @@ -657,7 +657,7 @@ devices: calibration_factor: 0.997707 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m powerconverter: @@ -672,7 +672,7 @@ devices: calibration_factor: 1.00152 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m powerconverter: @@ -687,7 +687,7 @@ devices: calibration_factor: 0.998124 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m powerconverter: @@ -702,7 +702,7 @@ devices: calibration_factor: 0.996662 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m powerconverter: @@ -717,7 +717,7 @@ devices: calibration_factor: 1.0017 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m powerconverter: @@ -732,7 +732,7 @@ devices: calibration_factor: 0.999642 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m powerconverter: @@ -747,7 +747,7 @@ devices: calibration_factor: 1.00042 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m powerconverter: @@ -762,7 +762,7 @@ devices: calibration_factor: 1.00471 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m powerconverter: @@ -777,7 +777,7 @@ devices: calibration_factor: 1.00393 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m powerconverter: @@ -792,7 +792,7 @@ devices: calibration_factor: 0.992906 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m powerconverter: @@ -807,7 +807,7 @@ devices: calibration_factor: 1.00268 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m powerconverter: @@ -822,7 +822,7 @@ devices: calibration_factor: 1.00248 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m powerconverter: @@ -837,7 +837,7 @@ devices: calibration_factor: 1.00203 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m powerconverter: @@ -852,7 +852,7 @@ devices: calibration_factor: 0.998030791 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m powerconverter: @@ -867,7 +867,7 @@ devices: calibration_factor: 1.00232 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m powerconverter: @@ -882,7 +882,7 @@ devices: calibration_factor: 0.995052 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m powerconverter: @@ -897,7 +897,7 @@ devices: calibration_factor: 1.00155 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m powerconverter: @@ -912,7 +912,7 @@ devices: calibration_factor: 0.998271 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m powerconverter: @@ -927,7 +927,7 @@ devices: calibration_factor: 0.999702 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m powerconverter: @@ -942,7 +942,7 @@ devices: calibration_factor: 0.998005 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m powerconverter: @@ -957,7 +957,7 @@ devices: calibration_factor: 0.999463 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m powerconverter: @@ -972,7 +972,7 @@ devices: calibration_factor: 0.997794 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m powerconverter: @@ -987,7 +987,7 @@ devices: calibration_factor: 1.00203 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m powerconverter: @@ -1002,7 +1002,7 @@ devices: calibration_factor: 1.00504 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m powerconverter: @@ -1017,7 +1017,7 @@ devices: calibration_factor: 0.998212 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m powerconverter: @@ -1032,7 +1032,7 @@ devices: calibration_factor: 1.0037 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m powerconverter: @@ -1047,7 +1047,7 @@ devices: calibration_factor: 1.00093 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m powerconverter: @@ -1062,7 +1062,7 @@ devices: calibration_factor: 1.0025 crosstalk: 1.0 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv unit: 1/m powerconverter: @@ -1077,7 +1077,7 @@ devices: calibration_factor: 0.999305341 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m powerconverter: @@ -1092,7 +1092,7 @@ devices: calibration_factor: 0.997452918 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m powerconverter: @@ -1107,7 +1107,7 @@ devices: calibration_factor: 0.997993208 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m powerconverter: @@ -1122,7 +1122,7 @@ devices: calibration_factor: 1.006031322 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m powerconverter: @@ -1137,7 +1137,7 @@ devices: calibration_factor: 0.998547233 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m powerconverter: @@ -1152,7 +1152,7 @@ devices: calibration_factor: 1.002327856 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m powerconverter: @@ -1167,7 +1167,7 @@ devices: calibration_factor: 1.000154369 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m powerconverter: @@ -1182,7 +1182,7 @@ devices: calibration_factor: 1.009580478 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m powerconverter: @@ -1197,7 +1197,7 @@ devices: calibration_factor: 1.00447669 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m powerconverter: @@ -1212,7 +1212,7 @@ devices: calibration_factor: 1.0015563 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m powerconverter: @@ -1227,7 +1227,7 @@ devices: calibration_factor: 0.997221365 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m powerconverter: @@ -1242,7 +1242,7 @@ devices: calibration_factor: 1.005954167 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m powerconverter: @@ -1257,7 +1257,7 @@ devices: calibration_factor: 1.006725723 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m powerconverter: @@ -1272,7 +1272,7 @@ devices: calibration_factor: 0.994535144 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m powerconverter: @@ -1287,7 +1287,7 @@ devices: calibration_factor: 0.999550256 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m powerconverter: @@ -1302,7 +1302,7 @@ devices: calibration_factor: 1.001479145 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m powerconverter: @@ -1317,7 +1317,7 @@ devices: calibration_factor: 1.000321811 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m powerconverter: @@ -1332,7 +1332,7 @@ devices: calibration_factor: 1.006715036 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m powerconverter: @@ -1347,7 +1347,7 @@ devices: calibration_factor: 1.0036395 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m powerconverter: @@ -1362,7 +1362,7 @@ devices: calibration_factor: 0.997684471 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m powerconverter: @@ -1377,7 +1377,7 @@ devices: calibration_factor: 1.000385922 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m powerconverter: @@ -1392,7 +1392,7 @@ devices: calibration_factor: 0.999010167 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m powerconverter: @@ -1407,7 +1407,7 @@ devices: calibration_factor: 0.998392922 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m powerconverter: @@ -1422,7 +1422,7 @@ devices: calibration_factor: 0.999318789 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m powerconverter: @@ -1437,7 +1437,7 @@ devices: calibration_factor: 0.996926967 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m powerconverter: @@ -1452,7 +1452,7 @@ devices: calibration_factor: 1.000849027 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m powerconverter: @@ -1467,7 +1467,7 @@ devices: calibration_factor: 1.003392444 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m powerconverter: @@ -1482,7 +1482,7 @@ devices: calibration_factor: 1.001312133 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m powerconverter: @@ -1497,7 +1497,7 @@ devices: calibration_factor: 1.005402902 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m powerconverter: @@ -1512,7 +1512,7 @@ devices: calibration_factor: 0.995846789 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m powerconverter: @@ -1527,7 +1527,7 @@ devices: calibration_factor: 1.005877011 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m powerconverter: @@ -1542,7 +1542,7 @@ devices: calibration_factor: 1.001016211 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m powerconverter: @@ -1557,7 +1557,7 @@ devices: calibration_factor: 0.999010167 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m powerconverter: @@ -1572,7 +1572,7 @@ devices: calibration_factor: 1.007265811 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m powerconverter: @@ -1587,7 +1587,7 @@ devices: calibration_factor: 0.998238611 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m powerconverter: @@ -1602,7 +1602,7 @@ devices: calibration_factor: 0.998161456 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m powerconverter: @@ -1617,7 +1617,7 @@ devices: calibration_factor: 1.004642522 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m powerconverter: @@ -1632,7 +1632,7 @@ devices: calibration_factor: 1.001479145 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m powerconverter: @@ -1647,7 +1647,7 @@ devices: calibration_factor: 1.001942078 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m powerconverter: @@ -1662,7 +1662,7 @@ devices: calibration_factor: 0.999087322 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m powerconverter: @@ -1677,7 +1677,7 @@ devices: calibration_factor: 0.998547233 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m powerconverter: @@ -1692,7 +1692,7 @@ devices: calibration_factor: 1.001698055 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m powerconverter: @@ -1707,7 +1707,7 @@ devices: calibration_factor: 0.999704567 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m powerconverter: @@ -1722,7 +1722,7 @@ devices: calibration_factor: 0.999164478 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m powerconverter: @@ -1737,7 +1737,7 @@ devices: calibration_factor: 1.000694659 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m powerconverter: @@ -1752,7 +1752,7 @@ devices: calibration_factor: 0.99945971 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m powerconverter: @@ -1767,7 +1767,7 @@ devices: calibration_factor: 0.999922816 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m powerconverter: @@ -1782,7 +1782,7 @@ devices: calibration_factor: 0.999922816 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m powerconverter: @@ -1797,7 +1797,7 @@ devices: calibration_factor: 0.997838839 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m powerconverter: @@ -1812,7 +1812,7 @@ devices: calibration_factor: 1.003318926 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m powerconverter: @@ -1827,7 +1827,7 @@ devices: calibration_factor: 1.004179589 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m powerconverter: @@ -1842,7 +1842,7 @@ devices: calibration_factor: 0.999010167 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m powerconverter: @@ -1857,7 +1857,7 @@ devices: calibration_factor: 0.9987787 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m powerconverter: @@ -1872,7 +1872,7 @@ devices: calibration_factor: 1.004411056 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m powerconverter: @@ -1887,7 +1887,7 @@ devices: calibration_factor: 1.0029451 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m powerconverter: @@ -1902,7 +1902,7 @@ devices: calibration_factor: 1.009426167 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m powerconverter: @@ -1917,7 +1917,7 @@ devices: calibration_factor: 1.0050283 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m powerconverter: @@ -1932,7 +1932,7 @@ devices: calibration_factor: 0.998533498 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m powerconverter: @@ -1947,7 +1947,7 @@ devices: calibration_factor: 1.003485189 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m powerconverter: @@ -1962,7 +1962,7 @@ devices: calibration_factor: 1.001389318 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m powerconverter: @@ -1977,7 +1977,7 @@ devices: calibration_factor: 1.006108478 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m powerconverter: @@ -1992,7 +1992,7 @@ devices: calibration_factor: 1.002096389 crosstalk: 0.99912 curve: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv unit: 1/m powerconverter: diff --git a/tests/config/EBS_chromaticity.yaml b/tests/config/EBS_chromaticity.yaml deleted file mode 100644 index d7e45bcff..000000000 --- a/tests/config/EBS_chromaticity.yaml +++ /dev/null @@ -1,3892 +0,0 @@ -type: pyaml.accelerator -facility: ESRF -machine: sr -energy: 6e9 -alphac: 8.623614679299252e-05 -simulators: - - type: pyaml.lattice.simulator - lattice: sr/lattices/ebs.mat - name: design -controls: - - type: tango.pyaml.controlsystem - tango_host: ebs-simu-2:10000 - name: live -data_folder: /data/store -arrays: - - type: pyaml.arrays.bpm - name: BPM - elements: - - BPM* -devices: -- type: pyaml.diagnostics.tune_monitor - name: BETATRON_TUNE - tune_h: - type: tango.pyaml.attribute_read_only - attribute: srdiag/beam-tune/main/Qh - unit: "1" - tune_v: - type: tango.pyaml.attribute_read_only - attribute: srdiag/beam-tune/main/Qv - unit: "1" -- type: pyaml.diagnostics.chromaticity_monitor - name: CHROMATICITY_MONITOR - betatron_tune_name: BETATRON_TUNE - rf_plant_name: RF - bpm_array_name: BPM - n_step: 5 -- type: pyaml.rf.rf_plant - name: RF - masterclock: - type: tango.pyaml.attribute - attribute: sy/ms/1/Frequency - unit: Hz - transmitters: - - type: pyaml.rf.rf_transmitter - name: RFTRA - cavities: [CAV_C05_01,CAV_C05_02,CAV_C05_03,CAV_C05_04,CAV_C05_05,CAV_C07_01,CAV_C07_02,CAV_C07_03,CAV_C07_04,CAV_C07_05,CAV_C25_01,CAV_C25_02,CAV_C25_03] - harmonic: 1 - distribution: 1 - voltage: - type: tango.pyaml.attribute - attribute: sys/ringsimulator/ebs/RfVoltage - unit: V -- type: pyaml.bpm.bpm - name: BPM_C04-01 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c04-01/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c04-01/SA_VPosition - unit: m -- type: pyaml.bpm.bpm - name: BPM_C04-02 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c04-02/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c04-02/SA_VPosition - unit: m -- type: pyaml.bpm.bpm - name: BPM_C04-03 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c04-03/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c04-03/SA_VPosition - unit: m -- type: pyaml.bpm.bpm - name: BPM_C04-04 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c04-04/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c04-04/SA_VPosition - unit: m -- type: pyaml.bpm.bpm - name: BPM_C04-05 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c04-05/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c04-05/SA_VPosition - unit: m -- type: pyaml.bpm.bpm - name: BPM_C04-06 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c04-06/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c04-06/SA_VPosition - unit: m -- type: pyaml.bpm.bpm - name: BPM_C04-07 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c04-07/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c04-07/SA_VPosition - unit: m -- type: pyaml.bpm.bpm - name: BPM_C04-08 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c04-08/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c04-08/SA_VPosition - unit: m -- type: pyaml.bpm.bpm - name: BPM_C04-09 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c04-09/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c04-09/SA_VPosition - unit: m -- type: pyaml.bpm.bpm - name: BPM_C04-10 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c04-10/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c04-10/SA_VPosition - unit: m -- type: pyaml.bpm.bpm - name: BPM_C05-01 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c05-01/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c05-01/SA_VPosition - unit: m -- type: pyaml.bpm.bpm - name: BPM_C05-02 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c05-02/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c05-02/SA_VPosition - unit: m -- type: pyaml.bpm.bpm - name: BPM_C05-03 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c05-03/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c05-03/SA_VPosition - unit: m -- type: pyaml.bpm.bpm - name: BPM_C05-04 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c05-04/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c05-04/SA_VPosition - unit: m -- type: pyaml.bpm.bpm - name: BPM_C05-05 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c05-05/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c05-05/SA_VPosition - unit: m -- type: pyaml.bpm.bpm - name: BPM_C05-06 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c05-06/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c05-06/SA_VPosition - unit: m -- type: pyaml.bpm.bpm - name: BPM_C05-07 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c05-07/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c05-07/SA_VPosition - unit: m -- type: pyaml.bpm.bpm - name: BPM_C05-08 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c05-08/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c05-08/SA_VPosition - unit: m -- type: pyaml.bpm.bpm - name: BPM_C05-09 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c05-09/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c05-09/SA_VPosition - unit: m -- type: pyaml.bpm.bpm - name: BPM_C05-10 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c05-10/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c05-10/SA_VPosition - unit: m -- type: pyaml.bpm.bpm - name: BPM_C06-01 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c06-01/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c06-01/SA_VPosition - unit: m -- type: pyaml.bpm.bpm - name: BPM_C06-02 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c06-02/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c06-02/SA_VPosition - unit: m -- type: pyaml.bpm.bpm - name: BPM_C06-03 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c06-03/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c06-03/SA_VPosition - unit: m -- type: pyaml.bpm.bpm - name: BPM_C06-04 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c06-04/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c06-04/SA_VPosition - unit: m -- type: pyaml.bpm.bpm - name: BPM_C06-05 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c06-05/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c06-05/SA_VPosition - unit: m -- type: pyaml.bpm.bpm - name: BPM_C06-06 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c06-06/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c06-06/SA_VPosition - unit: m -- type: pyaml.bpm.bpm - name: BPM_C06-07 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c06-07/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c06-07/SA_VPosition - unit: m -- type: pyaml.bpm.bpm - name: BPM_C06-08 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c06-08/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c06-08/SA_VPosition - unit: m -- type: pyaml.bpm.bpm - name: BPM_C06-09 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c06-09/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c06-09/SA_VPosition - unit: m -- type: pyaml.bpm.bpm - name: BPM_C06-10 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c06-10/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c06-10/SA_VPosition - unit: m -- type: pyaml.bpm.bpm - name: BPM_C07-01 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c07-01/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c07-01/SA_VPosition - unit: m -- type: pyaml.bpm.bpm - name: BPM_C07-02 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c07-02/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c07-02/SA_VPosition - unit: m -- type: pyaml.bpm.bpm - name: BPM_C07-03 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c07-03/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c07-03/SA_VPosition - unit: m -- type: pyaml.bpm.bpm - name: BPM_C07-04 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c07-04/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c07-04/SA_VPosition - unit: m -- type: pyaml.bpm.bpm - name: BPM_C07-05 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c07-05/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c07-05/SA_VPosition - unit: m -- type: pyaml.bpm.bpm - name: BPM_C07-06 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c07-06/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c07-06/SA_VPosition - unit: m -- type: pyaml.bpm.bpm - name: BPM_C07-07 - model: - type: 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unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c07-10/SA_VPosition - unit: m -- type: pyaml.bpm.bpm - name: BPM_C08-01 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c08-01/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c08-01/SA_VPosition - unit: m -- type: pyaml.bpm.bpm - name: BPM_C08-02 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c08-02/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c08-02/SA_VPosition - unit: m -- type: pyaml.bpm.bpm - name: BPM_C08-03 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c08-03/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c08-03/SA_VPosition - unit: m -- type: 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tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c08-07/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c08-07/SA_VPosition - unit: m -- type: pyaml.bpm.bpm - name: BPM_C08-08 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c08-08/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c08-08/SA_VPosition - unit: m -- type: pyaml.bpm.bpm - name: BPM_C08-09 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c08-09/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c08-09/SA_VPosition - unit: m -- type: pyaml.bpm.bpm - name: BPM_C08-10 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c08-10/SA_HPosition - unit: m - y_pos: - type: 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pyaml.bpm.bpm - name: BPM_C32-07 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c32-07/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c32-07/SA_VPosition - unit: m -- type: pyaml.bpm.bpm - name: BPM_C32-08 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c32-08/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c32-08/SA_VPosition - unit: m -- type: pyaml.bpm.bpm - name: BPM_C32-09 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c32-09/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c32-09/SA_VPosition - unit: m -- type: pyaml.bpm.bpm - name: BPM_C32-10 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c32-10/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c32-10/SA_VPosition - unit: m -- type: pyaml.bpm.bpm - name: BPM_C01-01 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c01-01/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c01-01/SA_VPosition - unit: m -- type: pyaml.bpm.bpm - name: BPM_C01-02 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c01-02/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c01-02/SA_VPosition - unit: m -- type: pyaml.bpm.bpm - name: BPM_C01-03 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c01-03/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c01-03/SA_VPosition - unit: m -- type: pyaml.bpm.bpm - name: BPM_C01-04 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c01-04/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c01-04/SA_VPosition - unit: m -- type: pyaml.bpm.bpm - name: BPM_C01-05 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c01-05/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c01-05/SA_VPosition - unit: m -- type: pyaml.bpm.bpm - name: BPM_C01-06 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c01-06/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c01-06/SA_VPosition - unit: m -- type: pyaml.bpm.bpm - name: BPM_C01-07 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c01-07/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c01-07/SA_VPosition - unit: m -- type: pyaml.bpm.bpm - name: BPM_C01-08 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c01-08/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c01-08/SA_VPosition - unit: m -- type: pyaml.bpm.bpm - name: BPM_C01-09 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c01-09/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c01-09/SA_VPosition - unit: m -- type: pyaml.bpm.bpm - name: BPM_C01-10 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c01-10/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c01-10/SA_VPosition - unit: m -- type: pyaml.bpm.bpm - name: BPM_C02-01 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c02-01/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c02-01/SA_VPosition - unit: m -- type: pyaml.bpm.bpm - name: BPM_C02-02 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c02-02/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c02-02/SA_VPosition - unit: m -- type: pyaml.bpm.bpm - name: BPM_C02-03 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c02-03/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c02-03/SA_VPosition - unit: m -- type: pyaml.bpm.bpm - name: BPM_C02-04 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c02-04/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c02-04/SA_VPosition - unit: m -- type: pyaml.bpm.bpm - name: BPM_C02-05 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c02-05/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c02-05/SA_VPosition - unit: m -- type: pyaml.bpm.bpm - name: BPM_C02-06 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c02-06/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c02-06/SA_VPosition - unit: m -- type: pyaml.bpm.bpm - name: BPM_C02-07 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c02-07/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c02-07/SA_VPosition - unit: m -- type: pyaml.bpm.bpm - name: BPM_C02-08 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c02-08/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c02-08/SA_VPosition - unit: m -- type: pyaml.bpm.bpm - name: BPM_C02-09 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c02-09/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c02-09/SA_VPosition - unit: m -- type: pyaml.bpm.bpm - name: BPM_C02-10 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c02-10/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c02-10/SA_VPosition - unit: m -- type: pyaml.bpm.bpm - name: BPM_C03-01 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c03-01/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c03-01/SA_VPosition - unit: m -- type: pyaml.bpm.bpm - name: BPM_C03-02 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c03-02/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c03-02/SA_VPosition - unit: m -- type: pyaml.bpm.bpm - name: BPM_C03-03 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c03-03/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c03-03/SA_VPosition - unit: m -- type: pyaml.bpm.bpm - name: BPM_C03-04 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c03-04/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c03-04/SA_VPosition - unit: m -- type: pyaml.bpm.bpm - name: BPM_C03-05 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c03-05/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c03-05/SA_VPosition - unit: m -- type: pyaml.bpm.bpm - name: BPM_C03-06 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c03-06/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c03-06/SA_VPosition - unit: m -- type: pyaml.bpm.bpm - name: BPM_C03-07 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c03-07/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c03-07/SA_VPosition - unit: m -- type: pyaml.bpm.bpm - name: BPM_C03-08 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c03-08/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c03-08/SA_VPosition - unit: m -- type: pyaml.bpm.bpm - name: BPM_C03-09 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c03-09/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c03-09/SA_VPosition - unit: m -- type: pyaml.bpm.bpm - name: BPM_C03-10 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c03-10/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c03-10/SA_VPosition - unit: m diff --git a/tests/config/EBS_rf.yaml b/tests/config/EBS_rf.yaml index 5094d3553..52b40210f 100644 --- a/tests/config/EBS_rf.yaml +++ b/tests/config/EBS_rf.yaml @@ -13,18 +13,12 @@ controls: data_folder: /data/store devices: - type: pyaml.rf.rf_plant - name: RF - masterclock: - type: tango.pyaml.attribute - attribute: sy/ms/1/Frequency - unit: Hz + name: DEFAULT_RF_PLANT + masterclock: sy/ms/1/Frequency transmitters: - type: pyaml.rf.rf_transmitter name: RFTRA cavities: [CAV_C05_01,CAV_C05_02,CAV_C05_03,CAV_C05_04,CAV_C05_05,CAV_C07_01,CAV_C07_02,CAV_C07_03,CAV_C07_04,CAV_C07_05,CAV_C25_01,CAV_C25_02,CAV_C25_03] harmonic: 1 distribution: 1 - voltage: - type: tango.pyaml.attribute - attribute: sys/ringsimulator/ebs/RfVoltage - unit: V + voltage: sys/ringsimulator/ebs/RfVoltage diff --git a/tests/config/EBS_rf_multi.yaml b/tests/config/EBS_rf_multi.yaml index 1d6d42993..d3c7133be 100644 --- a/tests/config/EBS_rf_multi.yaml +++ b/tests/config/EBS_rf_multi.yaml @@ -10,38 +10,27 @@ controls: - type: tango.pyaml.controlsystem tango_host: ebs-simu-3:10000 name: live + catalog: catalogs/ebs_catalogs.yaml data_folder: /data/store devices: - type: pyaml.rf.rf_plant - name: RF - masterclock: - type: tango.pyaml.attribute - attribute: sy/ms/1/Frequency - unit: Hz + name: DEFAULT_RF_PLANT + masterclock: sy/ms/1/Frequency transmitters: - type: pyaml.rf.rf_transmitter name: RFTRA1 cavities: [CAV_C05_01,CAV_C05_02,CAV_C05_03,CAV_C05_04,CAV_C05_05,CAV_C07_01,CAV_C07_02,CAV_C07_03,CAV_C07_04,CAV_C07_05] harmonic: 1 distribution: 0.83333333333 - voltage: - type: tango.pyaml.attribute - attribute: sr/tra/1/RfVoltage - unit: V + voltage: sr/tra/1/RfVoltage - type: pyaml.rf.rf_transmitter name: RFTRA2 cavities: [CAV_C25_01,CAV_C25_02] harmonic: 1 distribution: 0.16666666666 - voltage: - type: tango.pyaml.attribute - attribute: sr/tra/2/RfVoltage - unit: V + voltage: sr/tra/2/RfVoltage - type: pyaml.rf.rf_transmitter name: RFTRA_HARMONIC cavities: [CAV_C25_03] harmonic: 4 - voltage: - type: tango.pyaml.attribute - attribute: sr/tra/harm/RfVoltage - unit: V + voltage: sr/tra/harm/RfVoltage diff --git a/tests/config/EBS_rf_notrans.yaml b/tests/config/EBS_rf_notrans.yaml index d6cb3ee69..1306d8c28 100644 --- a/tests/config/EBS_rf_notrans.yaml +++ b/tests/config/EBS_rf_notrans.yaml @@ -10,11 +10,9 @@ controls: - type: tango.pyaml.controlsystem tango_host: ebs-simu-3:10000 name: live + catalog: catalogs/ebs_catalogs.yaml data_folder: /data/store devices: - type: pyaml.rf.rf_plant - name: RF - masterclock: - type: tango.pyaml.attribute - attribute: sy/ms/1/Frequency - unit: Hz + name: DEFAULT_RF_PLANT + masterclock: sy/ms/1/Frequency diff --git a/tests/config/bad_catalog_duplicate_key.yaml b/tests/config/bad_catalog_duplicate_key.yaml new file mode 100644 index 000000000..ddf320b9c --- /dev/null +++ b/tests/config/bad_catalog_duplicate_key.yaml @@ -0,0 +1,21 @@ +type: pyaml.accelerator +facility: ESRF +machine: sr +energy: 6e9 +data_folder: /data/store +devices: [] +catalogs: + - type: tango.pyaml.static_catalog + entries: + - type: tango.pyaml.static_catalog_entry + key: duplicated/key + device: + type: tango.pyaml.attribute + attribute: sr/test/one + unit: A + - type: tango.pyaml.static_catalog_entry + key: duplicated/key + device: + type: tango.pyaml.attribute + attribute: sr/test/two + unit: A diff --git a/tests/config/bad_conf_duplicate_2.yaml b/tests/config/bad_conf_duplicate_2.yaml index 7282bdafd..346957aa8 100644 --- a/tests/config/bad_conf_duplicate_2.yaml +++ b/tests/config/bad_conf_duplicate_2.yaml @@ -10,6 +10,7 @@ controls: - type: tango.pyaml.controlsystem tango_host: ebs-simu-3:10000 name: live + catalog: catalogs/sr_catalogs.yaml data_folder: /data/store arrays: - type: pyaml.arrays.bpm @@ -22,37 +23,13 @@ arrays: devices: - type: pyaml.bpm.bpm name: BPM_C04-04 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c04-04/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c04-04/SA_VPosition - unit: m + x_pos: srdiag/bpm/c04-04/SA_HPosition + y_pos: srdiag/bpm/c04-04/SA_VPosition - type: pyaml.bpm.bpm name: BPM_C04-05 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c04-05/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c04-05/SA_VPosition - unit: m + x_pos: srdiag/bpm/c04-05/SA_HPosition + y_pos: srdiag/bpm/c04-05/SA_VPosition - type: pyaml.bpm.bpm name: BPM_C04-06 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c04-06/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c04-06/SA_VPosition - unit: m + x_pos: srdiag/bpm/c04-06/SA_HPosition + y_pos: srdiag/bpm/c04-06/SA_VPosition diff --git a/tests/config/bad_conf_duplicate_3.yaml b/tests/config/bad_conf_duplicate_3.yaml index 6e9c7b926..9149009fb 100644 --- a/tests/config/bad_conf_duplicate_3.yaml +++ b/tests/config/bad_conf_duplicate_3.yaml @@ -10,6 +10,9 @@ controls: - type: tango.pyaml.controlsystem tango_host: ebs-simu-3:10000 name: live + catalog: bpm-catalog +catalogs: + - catalogs/sr_catalogs.yaml data_folder: /data/store arrays: - type: pyaml.arrays.bpm @@ -21,49 +24,17 @@ arrays: devices: - type: pyaml.bpm.bpm name: BPM_C04-04 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c04-04/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c04-04/SA_VPosition - unit: m + x_pos: srdiag/bpm/c04-04/SA_HPosition + y_pos: srdiag/bpm/c04-04/SA_VPosition - type: pyaml.bpm.bpm name: BPM_C04-05 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c04-05/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c04-05/SA_VPosition - unit: m + x_pos: srdiag/bpm/c04-05/SA_HPosition + y_pos: srdiag/bpm/c04-05/SA_VPosition - type: pyaml.bpm.bpm name: BPM_C04-06 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c04-06/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c04-06/SA_VPosition - unit: m + x_pos: srdiag/bpm/c04-06/SA_HPosition + y_pos: srdiag/bpm/c04-06/SA_VPosition - type: pyaml.bpm.bpm # duplicate device name: BPM_C04-06 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c04-06/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c04-06/SA_VPosition - unit: m + x_pos: srdiag/bpm/c04-06/SA_HPosition + y_pos: srdiag/bpm/c04-06/SA_VPosition diff --git a/tests/config/bpms.yaml b/tests/config/bpms.yaml index e0efafec5..07caf59af 100644 --- a/tests/config/bpms.yaml +++ b/tests/config/bpms.yaml @@ -10,70 +10,28 @@ controls: - type: tango.pyaml.controlsystem tango_host: ebs-simu-3:10000 name: live + catalog: catalogs/sr_catalogs.yaml data_folder: /data/store devices: - type: pyaml.bpm.bpm name: BPM_C01-01 - model: - type: pyaml.bpm.bpm_tiltoffset_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c01-01/SA_HPosition - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c01-01/SA_VPosition - unit: mm - x_offset: - type: tango.pyaml.attribute - attribute: srdiag/bpm/c01-01/HOffset - unit: mm - y_offset: - type: tango.pyaml.attribute - attribute: srdiag/bpm/c01-01/VOffset - unit: mm - tilt: - type: tango.pyaml.attribute - attribute: srdiag/bpm/c01-01/Tilt_Angle - unit: rad + x_pos: srdiag/bpm/c01-01/SA_HPosition + y_pos: srdiag/bpm/c01-01/SA_VPosition + x_offset: srdiag/bpm/c01-01/HOffset + y_offset: srdiag/bpm/c01-01/VOffset + tilt: srdiag/bpm/c01-01/Tilt_Angle - type: pyaml.bpm.bpm name: BPM_C01-02 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c01-02/SA_HPosition - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c01-02/SA_VPosition - unit: mm + x_pos: srdiag/bpm/c01-02/SA_HPosition + y_pos: srdiag/bpm/c01-02/SA_VPosition - type: pyaml.bpm.bpm name: BPM_C01-03 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c01-03/SA_HPosition - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c01-03/SA_VPosition - unit: mm + x_pos: srdiag/bpm/c01-03/SA_HPosition + y_pos: srdiag/bpm/c01-03/SA_VPosition - type: pyaml.bpm.bpm name: BPM_C01-04 - model: - type: pyaml.bpm.bpm_simple_model - x_pos_index: 0 - y_pos_index: 1 - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c01-04/Position - unit: mm - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c01-04/Position - unit: mm + x_pos: srdiag/bpm/c01-04/SA_HPosition + y_pos: srdiag/bpm/c01-04/SA_VPosition - type: pyaml.magnet.cfm_magnet name: SH1A-C01 #Name of the element in the lattice model mapping: diff --git a/tests/config/catalogs/ebs_bpm_catalogs.yaml b/tests/config/catalogs/ebs_bpm_catalogs.yaml new file mode 100644 index 000000000..ced75f81c --- /dev/null +++ b/tests/config/catalogs/ebs_bpm_catalogs.yaml @@ -0,0 +1,3852 @@ +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c04-01/SA_HPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c04-01/SA_HPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c04-01/SA_VPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c04-01/SA_VPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c04-02/SA_HPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c04-02/SA_HPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c04-02/SA_VPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c04-02/SA_VPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c04-03/SA_HPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c04-03/SA_HPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c04-03/SA_VPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c04-03/SA_VPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c04-04/SA_HPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c04-04/SA_HPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c04-04/SA_VPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c04-04/SA_VPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c04-04/HOffset + device: + type: tango.pyaml.attribute + attribute: srdiag/bpm/c04-04/HOffset + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c04-04/VOffset + device: + type: tango.pyaml.attribute + attribute: srdiag/bpm/c04-04/VOffset + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c04-05/SA_HPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c04-05/SA_HPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c04-05/SA_VPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c04-05/SA_VPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c04-06/SA_HPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c04-06/SA_HPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c04-06/SA_VPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c04-06/SA_VPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c04-07/SA_HPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c04-07/SA_HPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c04-07/SA_VPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c04-07/SA_VPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c04-08/SA_HPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c04-08/SA_HPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c04-08/SA_VPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c04-08/SA_VPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c04-09/SA_HPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c04-09/SA_HPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c04-09/SA_VPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c04-09/SA_VPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c04-10/SA_HPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c04-10/SA_HPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c04-10/SA_VPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c04-10/SA_VPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c05-01/SA_HPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c05-01/SA_HPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c05-01/SA_VPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c05-01/SA_VPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c05-02/SA_HPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c05-02/SA_HPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c05-02/SA_VPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c05-02/SA_VPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c05-03/SA_HPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c05-03/SA_HPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c05-03/SA_VPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c05-03/SA_VPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c05-04/SA_HPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c05-04/SA_HPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c05-04/SA_VPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c05-04/SA_VPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c05-05/SA_HPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c05-05/SA_HPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c05-05/SA_VPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c05-05/SA_VPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c05-06/SA_HPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c05-06/SA_HPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c05-06/SA_VPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c05-06/SA_VPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c05-07/SA_HPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c05-07/SA_HPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c05-07/SA_VPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c05-07/SA_VPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c05-08/SA_HPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c05-08/SA_HPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c05-08/SA_VPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c05-08/SA_VPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c05-09/SA_HPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c05-09/SA_HPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c05-09/SA_VPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c05-09/SA_VPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c05-10/SA_HPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c05-10/SA_HPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c05-10/SA_VPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c05-10/SA_VPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c06-01/SA_HPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c06-01/SA_HPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c06-01/SA_VPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c06-01/SA_VPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c06-02/SA_HPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c06-02/SA_HPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c06-02/SA_VPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c06-02/SA_VPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c06-03/SA_HPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c06-03/SA_HPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c06-03/SA_VPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c06-03/SA_VPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c06-04/SA_HPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c06-04/SA_HPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c06-04/SA_VPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c06-04/SA_VPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c06-05/SA_HPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c06-05/SA_HPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c06-05/SA_VPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c06-05/SA_VPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c06-06/SA_HPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c06-06/SA_HPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c06-06/SA_VPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c06-06/SA_VPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c06-07/SA_HPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c06-07/SA_HPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c06-07/SA_VPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c06-07/SA_VPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c06-08/SA_HPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c06-08/SA_HPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c06-08/SA_VPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c06-08/SA_VPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c06-09/SA_HPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c06-09/SA_HPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c06-09/SA_VPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c06-09/SA_VPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c06-10/SA_HPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c06-10/SA_HPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c06-10/SA_VPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c06-10/SA_VPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c07-01/SA_HPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c07-01/SA_HPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c07-01/SA_VPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c07-01/SA_VPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c07-02/SA_HPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c07-02/SA_HPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c07-02/SA_VPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c07-02/SA_VPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c07-03/SA_HPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c07-03/SA_HPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c07-03/SA_VPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c07-03/SA_VPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c07-04/SA_HPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c07-04/SA_HPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c07-04/SA_VPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c07-04/SA_VPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c07-05/SA_HPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c07-05/SA_HPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c07-05/SA_VPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c07-05/SA_VPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c07-06/SA_HPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c07-06/SA_HPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c07-06/SA_VPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c07-06/SA_VPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c07-07/SA_HPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c07-07/SA_HPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c07-07/SA_VPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c07-07/SA_VPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c07-08/SA_HPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c07-08/SA_HPosition + unit: m +- type: 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+ type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c01-07/SA_HPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c01-07/SA_VPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c01-07/SA_VPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c01-08/SA_HPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c01-08/SA_HPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c01-08/SA_VPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c01-08/SA_VPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c01-09/SA_HPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c01-09/SA_HPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c01-09/SA_VPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c01-09/SA_VPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c01-10/SA_HPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c01-10/SA_HPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c01-10/SA_VPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c01-10/SA_VPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c02-01/SA_HPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c02-01/SA_HPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c02-01/SA_VPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c02-01/SA_VPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c02-02/SA_HPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c02-02/SA_HPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c02-02/SA_VPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c02-02/SA_VPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c02-03/SA_HPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c02-03/SA_HPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c02-03/SA_VPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c02-03/SA_VPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c02-04/SA_HPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c02-04/SA_HPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c02-04/SA_VPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c02-04/SA_VPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c02-05/SA_HPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c02-05/SA_HPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c02-05/SA_VPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c02-05/SA_VPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c02-06/SA_HPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c02-06/SA_HPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c02-06/SA_VPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c02-06/SA_VPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c02-07/SA_HPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c02-07/SA_HPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c02-07/SA_VPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c02-07/SA_VPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c02-08/SA_HPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c02-08/SA_HPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c02-08/SA_VPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c02-08/SA_VPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c02-09/SA_HPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c02-09/SA_HPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c02-09/SA_VPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c02-09/SA_VPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c02-10/SA_HPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c02-10/SA_HPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c02-10/SA_VPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c02-10/SA_VPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c03-01/SA_HPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c03-01/SA_HPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c03-01/SA_VPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c03-01/SA_VPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c03-02/SA_HPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c03-02/SA_HPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c03-02/SA_VPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c03-02/SA_VPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c03-03/SA_HPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c03-03/SA_HPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c03-03/SA_VPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c03-03/SA_VPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c03-04/SA_HPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c03-04/SA_HPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c03-04/SA_VPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c03-04/SA_VPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c03-05/SA_HPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c03-05/SA_HPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c03-05/SA_VPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c03-05/SA_VPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c03-06/SA_HPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c03-06/SA_HPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c03-06/SA_VPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c03-06/SA_VPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c03-07/SA_HPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c03-07/SA_HPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c03-07/SA_VPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c03-07/SA_VPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c03-08/SA_HPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c03-08/SA_HPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c03-08/SA_VPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c03-08/SA_VPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c03-09/SA_HPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c03-09/SA_HPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c03-09/SA_VPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c03-09/SA_VPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c03-10/SA_HPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c03-10/SA_HPosition + unit: m +- type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c03-10/SA_VPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c03-10/SA_VPosition + unit: m diff --git a/tests/config/catalogs/ebs_catalogs.yaml b/tests/config/catalogs/ebs_catalogs.yaml new file mode 100644 index 000000000..d15349d6f --- /dev/null +++ b/tests/config/catalogs/ebs_catalogs.yaml @@ -0,0 +1,8 @@ +type: tango.pyaml.static_catalog +entries: + - catalogs/ebs_bpm_catalogs.yaml + - catalogs/ebs_rf_catalogs.yaml + - catalogs/ebs_diag_catalogs.yaml + - catalogs/ebs_magnets_catalogs.yaml + - catalogs/ebs_sh_catalogs.yaml + - catalogs/ebs_sext_catalogs.yaml diff --git a/tests/config/catalogs/ebs_diag_catalogs.yaml b/tests/config/catalogs/ebs_diag_catalogs.yaml new file mode 100644 index 000000000..84e820625 --- /dev/null +++ b/tests/config/catalogs/ebs_diag_catalogs.yaml @@ -0,0 +1,12 @@ +- type: tango.pyaml.static_catalog_entry + key: srdiag/beam-tune/main/Qh + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/beam-tune/main/Qh + unit: "" +- type: tango.pyaml.static_catalog_entry + key: srdiag/beam-tune/main/Qv + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/beam-tune/main/Qv + unit: "" diff --git a/tests/config/catalogs/ebs_magnets_catalogs.yaml b/tests/config/catalogs/ebs_magnets_catalogs.yaml new file mode 100644 index 000000000..79923fd6c --- /dev/null +++ b/tests/config/catalogs/ebs_magnets_catalogs.yaml @@ -0,0 +1,875 @@ +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qf1/c04-e/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qf1/c04-e/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qf1/c05-a/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qf1/c05-a/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qf1/c05-e/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qf1/c05-e/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qf1/c06-a/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qf1/c06-a/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qf1/c06-e/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qf1/c06-e/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qf1/c07-a/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qf1/c07-a/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qf1/c07-e/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qf1/c07-e/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qf1/c08-a/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qf1/c08-a/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qf1/c08-e/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qf1/c08-e/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qf1/c09-a/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qf1/c09-a/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qf1/c09-e/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qf1/c09-e/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qf1/c10-a/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qf1/c10-a/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qf1/c10-e/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qf1/c10-e/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qf1/c11-a/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qf1/c11-a/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qf1/c11-e/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qf1/c11-e/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qf1/c12-a/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qf1/c12-a/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qf1/c12-e/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qf1/c12-e/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qf1/c13-a/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qf1/c13-a/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qf1/c13-e/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qf1/c13-e/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qf1/c14-a/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qf1/c14-a/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qf1/c14-e/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qf1/c14-e/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qf1/c15-a/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qf1/c15-a/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qf1/c15-e/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qf1/c15-e/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qf1/c16-a/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qf1/c16-a/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qf1/c16-e/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qf1/c16-e/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qf1/c17-a/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qf1/c17-a/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qf1/c17-e/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qf1/c17-e/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qf1/c18-a/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qf1/c18-a/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qf1/c18-e/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qf1/c18-e/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qf1/c19-a/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qf1/c19-a/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qf1/c19-e/current + device: + type: tango.pyaml.attribute + 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type: tango.pyaml.static_catalog_entry + key: srmag/vps-qf1/c22-e/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qf1/c22-e/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qf1/c23-a/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qf1/c23-a/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qf1/c23-e/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qf1/c23-e/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qf1/c24-a/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qf1/c24-a/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qf1/c24-e/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qf1/c24-e/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: 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attribute: srmag/vps-qd2/c04-e/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qd2/c05-a/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qd2/c05-a/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qd2/c05-e/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qd2/c05-e/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qd2/c06-a/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qd2/c06-a/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qd2/c06-e/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qd2/c06-e/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qd2/c07-a/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qd2/c07-a/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qd2/c07-e/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qd2/c07-e/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qd2/c08-a/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qd2/c08-a/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qd2/c08-e/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qd2/c08-e/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qd2/c09-a/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qd2/c09-a/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qd2/c09-e/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qd2/c09-e/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qd2/c10-a/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qd2/c10-a/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qd2/c10-e/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qd2/c10-e/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qd2/c11-a/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qd2/c11-a/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qd2/c11-e/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qd2/c11-e/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qd2/c12-a/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qd2/c12-a/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qd2/c12-e/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qd2/c12-e/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qd2/c13-a/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qd2/c13-a/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qd2/c13-e/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qd2/c13-e/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qd2/c14-a/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qd2/c14-a/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qd2/c14-e/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qd2/c14-e/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qd2/c15-a/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qd2/c15-a/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qd2/c15-e/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qd2/c15-e/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qd2/c16-a/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qd2/c16-a/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qd2/c16-e/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qd2/c16-e/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qd2/c17-a/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qd2/c17-a/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qd2/c17-e/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qd2/c17-e/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: 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attribute: srmag/vps-qd2/c20-e/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qd2/c21-a/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qd2/c21-a/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qd2/c21-e/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qd2/c21-e/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qd2/c22-a/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qd2/c22-a/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qd2/c22-e/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qd2/c22-e/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qd2/c23-a/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qd2/c23-a/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qd2/c23-e/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qd2/c23-e/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qd2/c24-a/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qd2/c24-a/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qd2/c24-e/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qd2/c24-e/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qd2/c25-a/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qd2/c25-a/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qd2/c25-e/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qd2/c25-e/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qd2/c26-a/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qd2/c26-a/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qd2/c26-e/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qd2/c26-e/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qd2/c27-a/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qd2/c27-a/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qd2/c27-e/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qd2/c27-e/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qd2/c28-a/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qd2/c28-a/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qd2/c28-e/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qd2/c28-e/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qd2/c29-a/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qd2/c29-a/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qd2/c29-e/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qd2/c29-e/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qd2/c30-a/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qd2/c30-a/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qd2/c30-e/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qd2/c30-e/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qd2/c31-a/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qd2/c31-a/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qd2/c31-e/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qd2/c31-e/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qd2/c32-a/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qd2/c32-a/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qd2/c32-e/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qd2/c32-e/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qd2/c01-a/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qd2/c01-a/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qd2/c01-e/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qd2/c01-e/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qd2/c02-a/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qd2/c02-a/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qd2/c02-e/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qd2/c02-e/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qd2/c03-a/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qd2/c03-a/current + range: [10,109] + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/vps-qf6/c04-b/current + device: + type: tango.pyaml.attribute + attribute: srmag/vps-qf6/c04-b/current + range: [10,109] + unit: A diff --git a/tests/config/catalogs/ebs_rf_catalogs.yaml b/tests/config/catalogs/ebs_rf_catalogs.yaml new file mode 100644 index 000000000..0739d3526 --- /dev/null +++ b/tests/config/catalogs/ebs_rf_catalogs.yaml @@ -0,0 +1,30 @@ +- type: tango.pyaml.static_catalog_entry + key: sys/ringsimulator/ebs/RfVoltage + device: + type: tango.pyaml.attribute + attribute: sys/ringsimulator/ebs/RfVoltage + unit: V +- type: tango.pyaml.static_catalog_entry + key: sy/ms/1/Frequency + device: + type: tango.pyaml.attribute + attribute: sy/ms/1/Frequency + unit: Hz +- type: tango.pyaml.static_catalog_entry + key: sr/tra/1/RfVoltage + device: + type: tango.pyaml.attribute + attribute: sr/tra/1/RfVoltage + unit: V +- type: tango.pyaml.static_catalog_entry + key: sr/tra/2/RfVoltage + device: + type: tango.pyaml.attribute + attribute: sr/tra/2/RfVoltage + unit: V +- type: tango.pyaml.static_catalog_entry + key: sr/tra/harm/RfVoltage + device: + type: tango.pyaml.attribute + attribute: sr/tra/harm/RfVoltage + unit: V diff --git a/tests/config/catalogs/ebs_sext_catalogs.yaml b/tests/config/catalogs/ebs_sext_catalogs.yaml new file mode 100644 index 000000000..d62c07305 --- /dev/null +++ b/tests/config/catalogs/ebs_sext_catalogs.yaml @@ -0,0 +1,4608 @@ +- type: tango.pyaml.static_catalog_entry + key: srmag/m-sd1/c04-a/Strength_H + device: + type: tango.pyaml.attribute + attribute: srmag/m-sd1/c04-a/Strength_H + unit: rad +- type: tango.pyaml.static_catalog_entry + key: srmag/m-sd1/c04-a/Strength_V + device: + type: tango.pyaml.attribute + attribute: srmag/m-sd1/c04-a/Strength_V + unit: rad +- type: tango.pyaml.static_catalog_entry + key: srmag/m-sd1/c04-a/Strength_SQ + device: + type: tango.pyaml.attribute + attribute: srmag/m-sd1/c04-a/Strength_SQ + unit: m-1 +- type: tango.pyaml.static_catalog_entry + key: srmag/m-sd1/c04-a/Strength + device: + type: tango.pyaml.attribute + attribute: srmag/m-sd1/c04-a/Strength + unit: m-2 +- type: tango.pyaml.static_catalog_entry + key: srmag/m-sf2/c04-a/Strength_H + device: + type: tango.pyaml.attribute + attribute: srmag/m-sf2/c04-a/Strength_H + unit: rad +- type: tango.pyaml.static_catalog_entry + key: srmag/m-sf2/c04-a/Strength_V + device: + type: tango.pyaml.attribute + attribute: 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tango.pyaml.static_catalog_entry + key: srmag/m-sd1/c03-d/Strength + device: + type: tango.pyaml.attribute + attribute: srmag/m-sd1/c03-d/Strength + unit: m-2 +- type: tango.pyaml.static_catalog_entry + key: srmag/m-sf2/c03-e/Strength_H + device: + type: tango.pyaml.attribute + attribute: srmag/m-sf2/c03-e/Strength_H + unit: rad +- type: tango.pyaml.static_catalog_entry + key: srmag/m-sf2/c03-e/Strength_V + device: + type: tango.pyaml.attribute + attribute: srmag/m-sf2/c03-e/Strength_V + unit: rad +- type: tango.pyaml.static_catalog_entry + key: srmag/m-sf2/c03-e/Strength_SQ + device: + type: tango.pyaml.attribute + attribute: srmag/m-sf2/c03-e/Strength_SQ + unit: m-1 +- type: tango.pyaml.static_catalog_entry + key: srmag/m-sf2/c03-e/Strength + device: + type: tango.pyaml.attribute + attribute: srmag/m-sf2/c03-e/Strength + unit: m-2 +- type: tango.pyaml.static_catalog_entry + key: srmag/m-sd1/c03-e/Strength_H + device: + type: tango.pyaml.attribute + attribute: srmag/m-sd1/c03-e/Strength_H + unit: rad +- type: tango.pyaml.static_catalog_entry + key: srmag/m-sd1/c03-e/Strength_V + device: + type: tango.pyaml.attribute + attribute: srmag/m-sd1/c03-e/Strength_V + unit: rad +- type: tango.pyaml.static_catalog_entry + key: srmag/m-sd1/c03-e/Strength_SQ + device: + type: tango.pyaml.attribute + attribute: srmag/m-sd1/c03-e/Strength_SQ + unit: m-1 +- type: tango.pyaml.static_catalog_entry + key: srmag/m-sd1/c03-e/Strength + device: + type: tango.pyaml.attribute + attribute: srmag/m-sd1/c03-e/Strength + unit: m-2 diff --git a/tests/config/catalogs/ebs_sh_catalogs.yaml b/tests/config/catalogs/ebs_sh_catalogs.yaml new file mode 100644 index 000000000..72282b1d7 --- /dev/null +++ b/tests/config/catalogs/ebs_sh_catalogs.yaml @@ -0,0 +1,1752 @@ +- type: tango.pyaml.static_catalog_entry + key: srmag/ps-corr-sh1/c04-a-ch1/current + device: + type: tango.pyaml.attribute + attribute: srmag/ps-corr-sh1/c04-a-ch1/current + unit: A +- type: 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srmag/ps-corr-sh1/c03-a-ch3/current + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/ps-corr-sh2/c03-b-ch1/current + device: + type: tango.pyaml.attribute + attribute: srmag/ps-corr-sh2/c03-b-ch1/current + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/ps-corr-sh2/c03-b-ch2/current + device: + type: tango.pyaml.attribute + attribute: srmag/ps-corr-sh2/c03-b-ch2/current + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/ps-corr-sh2/c03-b-ch3/current + device: + type: tango.pyaml.attribute + attribute: srmag/ps-corr-sh2/c03-b-ch3/current + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/ps-corr-sh3/c03-e-ch1/current + device: + type: tango.pyaml.attribute + attribute: srmag/ps-corr-sh3/c03-e-ch1/current + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/ps-corr-sh3/c03-e-ch2/current + device: + type: tango.pyaml.attribute + attribute: srmag/ps-corr-sh3/c03-e-ch2/current + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/ps-corr-sh3/c03-e-ch3/current + device: + type: tango.pyaml.attribute + attribute: srmag/ps-corr-sh3/c03-e-ch3/current + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/ps-corr-sh3/c03-e-ch5/current + device: + type: tango.pyaml.attribute + attribute: srmag/ps-corr-sh3/c03-e-ch5/current + unit: A +- type: tango.pyaml.static_catalog_entry + key: srmag/ps-corr-sh3/c03-e-ch6/current + device: + type: tango.pyaml.attribute + attribute: srmag/ps-corr-sh3/c03-e-ch6/current + unit: A diff --git a/tests/config/catalogs/sr_catalogs.yaml b/tests/config/catalogs/sr_catalogs.yaml new file mode 100644 index 000000000..dc3bc686d --- /dev/null +++ b/tests/config/catalogs/sr_catalogs.yaml @@ -0,0 +1,204 @@ +type: tango.pyaml.static_catalog +entries: + - type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c01-01/SA_HPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c01-01/SA_HPosition + unit: mm + - type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c01-01/SA_VPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c01-01/SA_VPosition + unit: mm + - type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c01-01/HOffset + device: + type: tango.pyaml.attribute + attribute: srdiag/bpm/c01-01/HOffset + unit: mm + - type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c01-01/VOffset + device: + type: tango.pyaml.attribute + attribute: srdiag/bpm/c01-01/VOffset + unit: mm + - type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c01-01/Tilt_Angle + device: + type: tango.pyaml.attribute + attribute: srdiag/bpm/c01-01/Tilt_Angle + unit: rad + - type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c01-02/SA_HPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c01-02/SA_HPosition + unit: mm + - type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c01-02/SA_VPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c01-02/SA_VPosition + unit: mm + - type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c01-03/SA_HPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c01-03/SA_HPosition + unit: mm + - type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c01-03/SA_VPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c01-03/SA_VPosition + unit: mm + - type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c01-04/SA_HPosition + device: + type: tango.pyaml.attribute + attribute: srdiag/bpm/c01-04/Position + index: 0 + unit: mm + - type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c01-04/SA_VPosition + device: + type: tango.pyaml.attribute + attribute: srdiag/bpm/c01-04/Position + index: 1 + unit: mm + - type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c04-01/SA_HPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c04-01/SA_HPosition + unit: m + - type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c04-01/SA_VPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c04-01/SA_VPosition + unit: m + - type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c04-02/SA_HPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c04-02/SA_HPosition + unit: m + - type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c04-02/SA_VPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c04-02/SA_VPosition + unit: m + - type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c04-04/SA_HPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c04-04/SA_HPosition + unit: m + - type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c04-04/SA_VPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c04-04/SA_VPosition + unit: m + - type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c04-05/SA_HPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c04-05/SA_HPosition + unit: m + - type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c04-05/SA_VPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c04-05/SA_VPosition + unit: m + - type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c04-06/SA_HPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c04-06/SA_HPosition + unit: m + - type: tango.pyaml.static_catalog_entry + key: srdiag/bpm/c04-06/SA_VPosition + device: + type: tango.pyaml.attribute_read_only + attribute: srdiag/bpm/c04-06/SA_VPosition + unit: m + + - type: tango.pyaml.static_catalog_entry + key: srmag/m-qf1/c01-a/strength + device: + type: tango.pyaml.attribute + attribute: srmag/m-qf1/c01-a/strength + unit: m-1 + + - type: tango.pyaml.static_catalog_entry + key: sr/ps-qf1/c01-a/current + device: + type: tango.pyaml.attribute + attribute: sr/ps-qf1/c01-a/current + unit: A + + - type: tango.pyaml.static_catalog_entry + key: srmag/hst-sh1/c01-a/strength + device: + type: tango.pyaml.attribute + attribute: srmag/hst-sh1/c01-a/strength + unit: rad + - type: tango.pyaml.static_catalog_entry + key: srmag/vst-sh1/c01-a/strength + device: + type: tango.pyaml.attribute + attribute: srmag/vst-sh1/c01-a/strength + unit: rad + - type: tango.pyaml.static_catalog_entry + key: srmag/sqp-sh1/c01-a/strength + device: + type: tango.pyaml.attribute + attribute: srmag/sqp-sh1/c01-a/strength + unit: m-1 + + - type: tango.pyaml.static_catalog_entry + key: srmag/ps-corr-sh1/c01-a-ch1/current + device: + type: tango.pyaml.attribute + attribute: srmag/ps-corr-sh1/c01-a-ch1/current + unit: A + range: [-1.5, 1.5] + - type: tango.pyaml.static_catalog_entry + key: srmag/ps-corr-sh1/c01-a-ch2/current + device: + type: tango.pyaml.attribute + attribute: srmag/ps-corr-sh1/c01-a-ch2/current + unit: A + range: [null, 1.5] + - type: tango.pyaml.static_catalog_entry + key: srmag/ps-corr-sh1/c01-a-ch3/current + device: + type: tango.pyaml.attribute + attribute: srmag/ps-corr-sh1/c01-a-ch3/current + unit: A + range: [-1.5, null] + + - type: tango.pyaml.static_catalog_entry + key: srmag/ps-corr-sh1/c02-a-ch1/current + device: + type: tango.pyaml.attribute + attribute: srmag/ps-corr-sh1/c02-a-ch1/current + unit: A + - type: tango.pyaml.static_catalog_entry + key: srmag/ps-corr-sh1/c02-a-ch2/current + device: + type: tango.pyaml.attribute + attribute: srmag/ps-corr-sh1/c02-a-ch2/current + unit: A + - type: tango.pyaml.static_catalog_entry + key: srmag/ps-corr-sh1/c02-a-ch3/current + device: + type: tango.pyaml.attribute + attribute: srmag/ps-corr-sh1/c02-a-ch3/current + unit: A diff --git a/tests/config/config_manager_sr_base.yaml b/tests/config/config_manager_sr_base.yaml index 914739fa4..c842221ac 100644 --- a/tests/config/config_manager_sr_base.yaml +++ b/tests/config/config_manager_sr_base.yaml @@ -10,4 +10,5 @@ controls: - type: tango.pyaml.controlsystem tango_host: ebs-simu-3:10000 name: live + catalog: catalogs/sr_catalogs.yaml data_folder: /data/store diff --git a/tests/config/config_manager_sr_catalogs.yaml b/tests/config/config_manager_sr_catalogs.yaml new file mode 100644 index 000000000..2a0f93347 --- /dev/null +++ b/tests/config/config_manager_sr_catalogs.yaml @@ -0,0 +1,2 @@ +catalogs: + - catalogs/sr_catalogs.yaml diff --git a/tests/config/config_manager_sr_devices.yaml b/tests/config/config_manager_sr_devices.yaml index e02a64b95..c6d3e2124 100644 --- a/tests/config/config_manager_sr_devices.yaml +++ b/tests/config/config_manager_sr_devices.yaml @@ -3,25 +3,9 @@ devices: - sr/correctors/SH1AC01-C02.yaml - type: pyaml.bpm.bpm name: BPM_C04-01 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c04-01/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c04-01/SA_VPosition - unit: m + x_pos: srdiag/bpm/c04-01/SA_HPosition + y_pos: srdiag/bpm/c04-01/SA_VPosition - type: pyaml.bpm.bpm name: BPM_C04-02 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c04-02/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c04-02/SA_VPosition - unit: m + x_pos: srdiag/bpm/c04-02/SA_HPosition + y_pos: srdiag/bpm/c04-02/SA_VPosition diff --git a/tests/config/config_manager_tune_monitor_devices.yaml b/tests/config/config_manager_tune_monitor_devices.yaml index 8b330a534..0f532c98d 100644 --- a/tests/config/config_manager_tune_monitor_devices.yaml +++ b/tests/config/config_manager_tune_monitor_devices.yaml @@ -1,11 +1,5 @@ devices: - type: pyaml.diagnostics.tune_monitor name: BETATRON_TUNE - tune_h: - type: tango.pyaml.attribute_read_only - attribute: srdiag/tune/tune_h - unit: mm - tune_v: - type: tango.pyaml.attribute_read_only - attribute: srdiag/tune/tune_v - unit: mm + tune_h: srdiag/tune/tune_h + tune_v: srdiag/tune/tune_v diff --git a/tests/config/sr-ident-cfm.yaml b/tests/config/sr-ident-cfm.yaml index 0608ca5d3..7bc833fdf 100644 --- a/tests/config/sr-ident-cfm.yaml +++ b/tests/config/sr-ident-cfm.yaml @@ -10,6 +10,7 @@ controls: - type: tango.pyaml.controlsystem tango_host: ebs-simu-3:10000 name: live + catalog: catalogs/sr_catalogs.yaml data_folder: /data/store arrays: - type: pyaml.arrays.magnet diff --git a/tests/config/sr-ident-hw-only.yaml b/tests/config/sr-ident-hw-only.yaml deleted file mode 100644 index 4e85b109c..000000000 --- a/tests/config/sr-ident-hw-only.yaml +++ /dev/null @@ -1,20 +0,0 @@ -type: pyaml.accelerator -facility: ESRF -machine: sr -energy: 6e9 -simulators: - - type: pyaml.lattice.simulator - lattice: sr/lattices/ebs.mat - name: design -data_folder: /data/store -devices: - - type: pyaml.magnet.quadrupole - name: QF1A-C01 - model: - type: pyaml.magnet.identity_model - unit: A - powerconverter: - type: pyaml.control.device - setpoint: srmag/vps-qf1/c05-a/current - readback: srmag/vps-qf1/c05-a/current - unit: A diff --git a/tests/config/sr-ident-strgth-only.yaml b/tests/config/sr-ident-strgth-only.yaml deleted file mode 100644 index 225bfab9d..000000000 --- a/tests/config/sr-ident-strgth-only.yaml +++ /dev/null @@ -1,20 +0,0 @@ -type: pyaml.accelerator -facility: ESRF -machine: sr -energy: 6e9 -simulators: - - type: pyaml.lattice.simulator - lattice: sr/lattices/ebs.mat - name: design -data_folder: /data/store -devices: - - type: pyaml.magnet.quadrupole - name: QF1A-C01 - model: - type: pyaml.magnet.identity_model - unit: 1/m - physics: - type: pyaml.control.device - setpoint: srmag/m-qf1/c05-a/strength - readback: srmag/m-qf1/c05-a/strength - unit: 1/m diff --git a/tests/config/sr-range-cfm.yaml b/tests/config/sr-range-cfm.yaml index ae4fd7f45..fc1b37217 100644 --- a/tests/config/sr-range-cfm.yaml +++ b/tests/config/sr-range-cfm.yaml @@ -10,6 +10,7 @@ controls: - type: tango.pyaml.controlsystem tango_host: ebs-simu-3:10000 name: live + catalog: catalogs/sr_catalogs.yaml data_folder: /data/store arrays: - type: pyaml.arrays.magnet diff --git a/tests/config/sr.yaml b/tests/config/sr.yaml index e2f6ac2e4..3e9561e81 100644 --- a/tests/config/sr.yaml +++ b/tests/config/sr.yaml @@ -10,6 +10,7 @@ controls: - type: tango.pyaml.controlsystem tango_host: ebs-simu-3:10000 name: live + catalog: catalogs/sr_catalogs.yaml data_folder: /data/store arrays: - type: pyaml.arrays.magnet @@ -44,25 +45,9 @@ devices: - sr/correctors/SH1AC01-C02.yaml - type: pyaml.bpm.bpm name: BPM_C04-01 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c04-01/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c04-01/SA_VPosition - unit: m + x_pos: srdiag/bpm/c04-01/SA_HPosition + y_pos: srdiag/bpm/c04-01/SA_VPosition - type: pyaml.bpm.bpm name: BPM_C04-02 - model: - type: pyaml.bpm.bpm_simple_model - x_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c04-02/SA_HPosition - unit: m - y_pos: - type: tango.pyaml.attribute_read_only - attribute: srdiag/bpm/c04-02/SA_VPosition - unit: m + x_pos: srdiag/bpm/c04-02/SA_HPosition + y_pos: srdiag/bpm/c04-02/SA_VPosition diff --git a/tests/config/sr/custom_magnets/hidcorr.yaml b/tests/config/sr/custom_magnets/hidcorr.yaml index 90bc97ea7..513e57bf6 100644 --- a/tests/config/sr/custom_magnets/hidcorr.yaml +++ b/tests/config/sr/custom_magnets/hidcorr.yaml @@ -3,7 +3,4 @@ name: IDCORR model: type: pyaml_external.external_magnet_model param: my random param - powersupply: - type: tango.pyaml.attribute - attribute: sr/ps-qf1/c01-a/current - unit: A + powersupply: sr/ps-qf1/c01-a/current diff --git a/tests/config/sr/magnet_models/QF1AC01.json b/tests/config/sr/magnet_models/QF1AC01.json index b6651a7aa..b9b4e8abd 100644 --- a/tests/config/sr/magnet_models/QF1AC01.json +++ b/tests/config/sr/magnet_models/QF1AC01.json @@ -4,9 +4,6 @@ "calibration_offset": 0.0, "curve": "sr/magnet_models/quadcurve.json", "unit": "1/m", - "powerconverter": { - "type": "tango.pyaml.attribute", - "attribute": "sr/ps-qf1/c01-a/current", - "unit": "A" - } + "hardware_unit": "A", + "powerconverter": "sr/ps-qf1/c01-a/current" } diff --git a/tests/config/sr/magnet_models/QF1AC01.yaml b/tests/config/sr/magnet_models/QF1AC01.yaml index 07701268a..c2f1ac30c 100644 --- a/tests/config/sr/magnet_models/QF1AC01.yaml +++ b/tests/config/sr/magnet_models/QF1AC01.yaml @@ -3,7 +3,5 @@ calibration_factor: 1.00504 calibration_offset: 0.0 curve: sr/magnet_models/quadcurve.yaml unit: 1/m -powerconverter: - type: tango.pyaml.attribute - attribute: sr/ps-qf1/c01-a/current - unit: A +hardware_unit: A +powerconverter: sr/ps-qf1/c01-a/current diff --git a/tests/config/sr/magnet_models/QF6_strength.csv b/tests/config/sr/magnet_models/QF6_strength.csv new file mode 100755 index 000000000..6331415ea --- /dev/null +++ b/tests/config/sr/magnet_models/QF6_strength.csv @@ -0,0 +1,101 @@ + 0, 0 + 10, 4.8381057 +11.01010101, 5.309790224 +12.02020202, 5.781444181 +13.03030303, 6.253037002 +14.04040404, 6.72453812 +15.05050505, 7.195916967 +16.06060606, 7.667150484 +17.07070707, 8.138241462 +18.08080808, 8.609198255 +19.09090909, 9.080029216 + 20.1010101, 9.5507427 +21.11111111, 10.02134783 +22.12121212, 10.49185598 +23.13131313, 10.96227898 +24.14141414, 11.43262864 +25.15151515, 11.90291672 +26.16161616, 12.37313684 +27.17171717, 12.84323594 +28.18181818, 13.31315356 +29.19191919, 13.78282926 + 30.2020202, 14.25220272 +31.21212121, 14.7212447 +32.22222222, 15.18999532 +33.23232323, 15.65850402 +34.24242424, 16.12682031 +35.25252525, 16.59499334 +36.26262626, 17.06303632 +37.27272727, 17.53089254 +38.28282828, 17.99849728 +39.29292929, 18.46578582 + 40.3030303, 18.93269377 +41.31313131, 19.39918272 +42.32323232, 19.86525832 +43.33333333, 20.33093051 +44.34343434, 20.79620918 +45.35353535, 21.26110358 +46.36363636, 21.72558595 +47.37373737, 22.18957373 +48.38383838, 22.65297993 +49.39393939, 23.11571754 + 50.4040404, 23.57770039 +51.41414141, 24.03887417 +52.42424242, 24.49922597 +53.43434343, 24.95874566 +54.44444444, 25.4174231 +55.45454545, 25.87522826 +56.46464646, 26.33154575 +57.47474747, 26.7850931 +58.48484848, 27.2345516 +59.49494949, 27.6786025 +60.50505051, 28.11592527 +61.51515152, 28.54515768 +62.52525253, 28.96489584 +63.53535354, 29.37373405 +64.54545455, 29.7702666 +65.55555556, 30.15310646 +66.56565657, 30.52120955 +67.57575758, 30.87383285 +68.58585859, 31.21024353 + 69.5959596, 31.52970877 +70.60606061, 31.83155581 +71.61616162, 32.11601021 +72.62626263, 32.38398911 +73.63636364, 32.63642744 +74.64646465, 32.87426012 +75.65656566, 33.09843152 +76.66666667, 33.31000256 +77.67676768, 33.51011278 +78.68686869, 33.69990319 + 79.6969697, 33.8805148 +80.70707071, 34.05306116 +81.71717172, 34.21837218 +82.72727273, 34.37711048 +83.73737374, 34.52993649 +84.74747475, 34.67751066 +85.75757576, 34.82045497 +86.76767677, 34.95905659 +87.77777778, 35.09343031 +88.78787879, 35.22368951 + 89.7979798, 35.34994755 +90.80808081, 35.47232532 +91.81818182, 35.59099919 +92.82828283, 35.70617041 +93.83838384, 35.81804036 +94.84848485, 35.92681041 +95.85858586, 36.03267776 +96.86868687, 36.13581324 +97.87878788, 36.23637744 +98.88888889, 36.33453092 + 99.8989899, 36.43043424 +100.9090909, 36.52421516 +101.9191919, 36.6158239 +102.9292929, 36.70515097 +103.9393939, 36.7920868 +104.9494949, 36.87652186 + 105.959596, 36.95843775 + 106.969697, 37.03823987 + 107.979798, 37.11645666 + 108.989899, 37.19361655 + 110, 37.270248 diff --git a/tests/config/sr/magnet_models/SH1AC01-ident.yaml b/tests/config/sr/magnet_models/SH1AC01-ident.yaml index 206754b84..0a701dba5 100644 --- a/tests/config/sr/magnet_models/SH1AC01-ident.yaml +++ b/tests/config/sr/magnet_models/SH1AC01-ident.yaml @@ -2,12 +2,6 @@ multipoles: [B0,A0,A1] units: [rad,rad,m-1] physics: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c01-a-ch1/strength - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c01-a-ch2/strength - unit: rad - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c01-a-ch3/strength - unit: m-1 + - srmag/hst-sh1/c01-a/strength + - srmag/vst-sh1/c01-a/strength + - srmag/sqp-sh1/c01-a/strength diff --git a/tests/config/sr/magnet_models/SH1AC01-range.yaml b/tests/config/sr/magnet_models/SH1AC01-range.yaml index 2c96a3b82..dbb494eff 100644 --- a/tests/config/sr/magnet_models/SH1AC01-range.yaml +++ b/tests/config/sr/magnet_models/SH1AC01-range.yaml @@ -1,27 +1,19 @@ type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: [A,A,A] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c01-a-ch1/current - unit: A - range: [-1.5, 1.5] - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c01-a-ch2/current - unit: A - range: [null, 1.5] - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c01-a-ch3/current - unit: A - range: [-1.5, null] + - srmag/ps-corr-sh1/c01-a-ch1/current + - srmag/ps-corr-sh1/c01-a-ch2/current + - srmag/ps-corr-sh1/c01-a-ch3/current diff --git a/tests/config/sr/magnet_models/SH1AC01.yaml b/tests/config/sr/magnet_models/SH1AC01.yaml index d8eb8fa40..dbb494eff 100644 --- a/tests/config/sr/magnet_models/SH1AC01.yaml +++ b/tests/config/sr/magnet_models/SH1AC01.yaml @@ -1,24 +1,19 @@ type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: [A,A,A] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c01-a-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c01-a-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c01-a-ch3/current - unit: A + - srmag/ps-corr-sh1/c01-a-ch1/current + - srmag/ps-corr-sh1/c01-a-ch2/current + - srmag/ps-corr-sh1/c01-a-ch3/current diff --git a/tests/config/sr/magnet_models/SH1AC02.yaml b/tests/config/sr/magnet_models/SH1AC02.yaml index 5c0664b62..ed3482a33 100644 --- a/tests/config/sr/magnet_models/SH1AC02.yaml +++ b/tests/config/sr/magnet_models/SH1AC02.yaml @@ -1,24 +1,19 @@ type: pyaml.magnet.linear_cfm_model multipoles: [B0,A0,A1] units: [rad,rad,m-1] + hardware_units: [A,A,A] pseudo_factors: [1.0,-1.0,-1.0] curves: - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_h_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_v_strength.csv - - type: pyaml.configuration.csvcurve + - type: pyaml.magnet.csvcurve file: sr/magnet_models/SH1_SH3_sq_strength.csv matrix: - type: pyaml.configuration.csvmatrix + type: pyaml.magnet.csvmatrix file: sr/magnet_models/SH_matrix.csv powerconverters: - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c02-a-ch1/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c02-a-ch2/current - unit: A - - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c02-a-ch3/current - unit: A + - srmag/ps-corr-sh1/c02-a-ch1/current + - srmag/ps-corr-sh1/c02-a-ch2/current + - srmag/ps-corr-sh1/c02-a-ch3/current diff --git a/tests/config/sr/magnet_models/quadcurve.json b/tests/config/sr/magnet_models/quadcurve.json index 9920711b4..f4d181968 100644 --- a/tests/config/sr/magnet_models/quadcurve.json +++ b/tests/config/sr/magnet_models/quadcurve.json @@ -1,4 +1,4 @@ { - "type": "pyaml.configuration.csvcurve", + "type": "pyaml.magnet.csvcurve", "file": "sr/magnet_models/QF1_strength.csv" } diff --git a/tests/config/sr/magnet_models/quadcurve.yaml b/tests/config/sr/magnet_models/quadcurve.yaml index a536a9f65..267184559 100644 --- a/tests/config/sr/magnet_models/quadcurve.yaml +++ b/tests/config/sr/magnet_models/quadcurve.yaml @@ -1,2 +1,2 @@ -type: pyaml.configuration.csvcurve +type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv diff --git a/tests/config/sr/quadrupoles/QF1AC01-IDENT-HW.yaml b/tests/config/sr/quadrupoles/QF1AC01-IDENT-HW.yaml index d77cdcf33..4ab7c69f8 100644 --- a/tests/config/sr/quadrupoles/QF1AC01-IDENT-HW.yaml +++ b/tests/config/sr/quadrupoles/QF1AC01-IDENT-HW.yaml @@ -3,7 +3,4 @@ name: QF1A-C01 model: type: pyaml.magnet.identity_model unit: A - powerconverter: - type: tango.pyaml.attribute - attribute: sr/ps-qf1/c01-a/strength - unit: 1/m + powerconverter: sr/ps-qf1/c01-a/current diff --git a/tests/config/sr/quadrupoles/QF1AC01-IDENT-STRGTH.yaml b/tests/config/sr/quadrupoles/QF1AC01-IDENT-STRGTH.yaml index 02f3de35c..7612dfd67 100644 --- a/tests/config/sr/quadrupoles/QF1AC01-IDENT-STRGTH.yaml +++ b/tests/config/sr/quadrupoles/QF1AC01-IDENT-STRGTH.yaml @@ -3,7 +3,4 @@ name: QF1A-C01 model: type: pyaml.magnet.identity_model unit: 1/m - physics: - type: tango.pyaml.attribute - attribute: sr/ps-qf1/c01-a/strength - unit: 1/m + physics: srmag/m-qf1/c01-a/strength diff --git a/tests/config/sr/quadrupoles/QF1C01A_2.yaml b/tests/config/sr/quadrupoles/QF1C01A_2.yaml index 3ada2ab13..6ab7f120d 100644 --- a/tests/config/sr/quadrupoles/QF1C01A_2.yaml +++ b/tests/config/sr/quadrupoles/QF1C01A_2.yaml @@ -6,7 +6,5 @@ model: calibration_offset: 0.0034 curve: sr/magnet_models/quadcurve.yaml unit: 1/m - powerconverter: - type: tango.pyaml.attribute - attribute: sr/ps-qf1/c01-a/current - unit: A + hardware_unit: A + powerconverter: sr/ps-qf1/c01-a/current diff --git a/tests/config/sr_serialized_magnets.yaml b/tests/config/sr_serialized_magnets.yaml index 19058d3e4..a8a3c486d 100644 --- a/tests/config/sr_serialized_magnets.yaml +++ b/tests/config/sr_serialized_magnets.yaml @@ -32,13 +32,11 @@ devices: calibration_factors: 1.00504 calibration_offsets: 0.0 unit: m-1 + hardware_unit: A curves: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/serialized_strength.csv - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c01-a-ch1/current - unit: A + powerconverter: srmag/ps-corr-sh1/c01-a-ch1/current - type: pyaml.magnet.serialized_magnet name: QF1A function: B1 @@ -79,13 +77,11 @@ devices: calibration_factors: 1 calibration_offsets: 0.0 unit: m-1 + hardware_unit: A curves: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c01-a-ch1/current - unit: A + powerconverter: srmag/ps-corr-sh1/c01-a-ch1/current - type: pyaml.magnet.serialized_magnet name: QF1E function: B1 @@ -126,13 +122,11 @@ devices: calibration_factors: 1 calibration_offsets: 0.0 unit: m-1 + hardware_unit: A curves: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QF1_strength.csv - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c01-a-ch1/current - unit: A + powerconverter: srmag/ps-corr-sh1/c01-a-ch1/current - type: pyaml.magnet.serialized_magnet name: QD2A function: B1 @@ -173,13 +167,11 @@ devices: calibration_factors: 1 calibration_offsets: 0.0 unit: m-1 + hardware_unit: A curves: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c01-a-ch1/current - unit: A + powerconverter: srmag/ps-corr-sh1/c01-a-ch1/current - type: pyaml.magnet.serialized_magnet name: QD2E function: B1 @@ -220,28 +212,20 @@ devices: calibration_factors: 1 calibration_offsets: 0.0 unit: m-1 + hardware_unit: A curves: - type: pyaml.configuration.csvcurve + type: pyaml.magnet.csvcurve file: sr/magnet_models/QD2_strength.csv - powerconverter: - type: tango.pyaml.attribute - attribute: srmag/ps-corr-sh1/c01-a-ch1/current - unit: A + powerconverter: srmag/ps-corr-sh1/c01-a-ch1/current - type: pyaml.diagnostics.tune_monitor name: BETATRON_TUNE - tune_h: - type: tango.pyaml.attribute_read_only - attribute: srdiag/beam-tune/main/Qh - unit: mm - tune_v: - type: tango.pyaml.attribute_read_only - attribute: srdiag/beam-tune/main/Qv - unit: mm + tune_h: srdiag/beam-tune/main/Qh + tune_v: srdiag/beam-tune/main/Qv - type: pyaml.tuning_tools.tune name: DEFAULT_TUNE_CORRECTION quad_array_name: QForTune betatron_tune_name: BETATRON_TUNE - response_matrix: file:tune_response.json + response_matrix: ${path:tune_response.json} - type: pyaml.tuning_tools.tune_response_matrix name: DEFAULT_TUNE_RESPONSE_MATRIX quad_array_name: QForTune diff --git a/tests/config/tune_monitor.yaml b/tests/config/tune_monitor.yaml index c6b00b8f9..f782a2c1c 100644 --- a/tests/config/tune_monitor.yaml +++ b/tests/config/tune_monitor.yaml @@ -11,22 +11,14 @@ controls: - type: tango.pyaml.controlsystem tango_host: ebs-simu-3:10000 name: live + catalog: catalogs/ebs_catalogs.yaml data_folder: /data/store devices: - type: pyaml.diagnostics.tune_monitor name: BETATRON_TUNE - tune_h: - type: tango.pyaml.attribute_read_only - attribute: srdiag/beam-tune/main/Qh - unit: mm - tune_v: - type: tango.pyaml.attribute_read_only - attribute: srdiag/beam-tune/main/Qv - unit: mm + tune_h: srdiag/beam-tune/main/Qh + tune_v: srdiag/beam-tune/main/Qv rf_plant_name: RF - type: pyaml.rf.rf_plant name: RF - masterclock: - type: tango.pyaml.attribute - attribute: sy/ms/1/Frequency - unit: Hz + masterclock: sy/ms/1/Frequency diff --git a/tests/config/tune_response.json b/tests/config/tune_response.json new file mode 100644 index 000000000..f6ce892ec --- /dev/null +++ b/tests/config/tune_response.json @@ -0,0 +1,387 @@ +{ + "type": "pyaml.tuning_tools.response_matrix_data", + "matrix": [ + [ + 0.1785305247425928, + 0.17890863159841786, + 0.17917913766291038, + 0.1784299133444911, + 0.17932003613274627, + 0.17884801681883333, + 0.17868922050995328, + 0.17950160845769947, + 0.178363425837047, + 0.17902822605941893, + 0.17907164949343413, + 0.17845271143679398, + 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"QF1E-C28", + "QF1A-C29", + "QF1E-C29", + "QF1A-C30", + "QF1E-C30", + "QF1A-C31", + "QF1E-C31", + "QF1A-C32", + "QF1E-C32", + "QF1A-C01", + "QF1E-C01", + "QF1A-C02", + "QF1E-C02", + "QF1A-C03" + ], + "observable_names": [ + "BETATRON_TUNE.x", + "BETATRON_TUNE.y" + ] +} diff --git a/tests/test_configuration_manager.py b/tests/configuration/test_configuration_manager.py similarity index 89% rename from tests/test_configuration_manager.py rename to tests/configuration/test_configuration_manager.py index f5ee6b4f3..f36c37dd1 100644 --- a/tests/test_configuration_manager.py +++ b/tests/configuration/test_configuration_manager.py @@ -103,7 +103,7 @@ def test_configuration_manager_clear_category_and_settings( result = manager.clear() assert result is None - assert manager.to_dict() == {"type": "pyaml.accelerator"} + assert manager.to_dict() == {"class_path": "pyaml.accelerator.Accelerator"} def test_configuration_manager_settings_follow_accelerator_config_model_order(): @@ -121,7 +121,7 @@ def test_configuration_manager_settings_follow_accelerator_config_model_order(): ) assert list(manager.settings()) == [ - "type", + "class_path", "facility", "machine", "energy", @@ -187,10 +187,10 @@ def test_configuration_manager_accumulates_multiple_device_fragments( assert manager.has("devices", "BPM_C04-01") assert manager.has("devices", "BPM_C04-02") assert manager.has("devices", "BETATRON_TUNE") - assert manager.get("devices", "QF1A-C01")["type"] == "pyaml.magnet.quadrupole" - assert manager.get("devices", "SH1A-C01")["type"] == "pyaml.magnet.cfm_magnet" - assert manager.get("devices", "BPM_C04-01")["type"] == "pyaml.bpm.bpm" - assert manager.get("devices", "BETATRON_TUNE")["type"] == "pyaml.diagnostics.tune_monitor" + assert manager.get("devices", "QF1A-C01")["class_path"] == "pyaml.magnet.quadrupole.Quadrupole" + assert manager.get("devices", "SH1A-C01")["class_path"] == "pyaml.magnet.cfm_magnet.CombinedFunctionMagnet" + assert manager.get("devices", "BPM_C04-01")["class_path"] == "pyaml.bpm.bpm.BPM" + assert manager.get("devices", "BETATRON_TUNE")["class_path"] == "pyaml.diagnostics.tune_monitor.BetatronTuneMonitor" def test_accelerator_load_stays_compatible(config_manager_base_config): @@ -270,10 +270,10 @@ def test_configuration_manager_repr_is_yellow_pages_like( assert "Simulators:" in output assert "Arrays:" in output assert "Devices:" in output - assert "live (tango.pyaml.controlsystem) source=config_manager_sr_base.yaml" in output - assert "design (pyaml.lattice.simulator) source=config_manager_sr_base.yaml" in output - assert "HCORR (pyaml.arrays.magnet) patterns=1 source=config_manager_sr_arrays.yaml" in output - assert "BPM_C04-01 (pyaml.bpm.bpm) source=config_manager_sr_devices.yaml" in output + assert "live (tango.pyaml.controlsystem.TangoControlSystem) source=config_manager_sr_base.yaml" in output + assert "design (pyaml.lattice.simulator.Simulator) source=config_manager_sr_base.yaml" in output + assert "HCORR (pyaml.arrays.magnet.Magnet) patterns=1 source=config_manager_sr_arrays.yaml" in output + assert "BPM_C04-01 (pyaml.bpm.bpm.BPM) source=config_manager_sr_devices.yaml" in output assert " ." in output @@ -288,5 +288,5 @@ def test_configuration_manager_yellow_pages_like_shortcuts( manager.add(sr_devices_fragment) assert manager["BPM_C04*"] == ["BPM_C04-01", "BPM_C04-02"] - assert manager.HCORR["type"] == "pyaml.arrays.magnet" + assert manager.HCORR["class_path"] == "pyaml.arrays.magnet.Magnet" assert manager.simulators == ["design"] diff --git a/tests/configuration/test_factory.py b/tests/configuration/test_factory.py new file mode 100644 index 000000000..692706bc4 --- /dev/null +++ b/tests/configuration/test_factory.py @@ -0,0 +1,30 @@ +import pytest + +from pyaml import PyAMLConfigException, PyAMLException +from pyaml.accelerator import Accelerator +from pyaml.configuration import ROOT +from pyaml.configuration.factory import Factory +from pyaml.configuration.fileloader import load +from tests.conftest import MockElement + + +def test_factory_build_default(): + """Test default PyAML module loading.""" + data = {"type": "mock_module", "name": "simple"} + obj = Factory.build(data, False) + assert isinstance(obj, MockElement) + assert obj.name == "simple" + + +@pytest.mark.parametrize( + "test_file", + [ + "tests/config/bad_conf_cycles.yml", + "tests/config/bad_conf_cycles.json", + ], +) +def test_error_cycles(test_file): + with pytest.raises(PyAMLException) as exc: + ml: Accelerator = Accelerator.load(test_file) + + assert "Circular file inclusion of " in str(exc.value) diff --git a/tests/configuration/test_fileloader.py b/tests/configuration/test_fileloader.py new file mode 100644 index 000000000..53b234a66 --- /dev/null +++ b/tests/configuration/test_fileloader.py @@ -0,0 +1,292 @@ +import json + +import pytest + +from pyaml import PyAMLException +from pyaml.configuration.fileloader import ( + FIELD_LOCATIONS_KEY, + LOCATION_KEY, + ROOT, + LoadContext, + RootFolder, + _is_supported_file, + load, +) + + +def test_rootfolder_uses_current_working_directory_when_no_path(monkeypatch, tmp_path): + monkeypatch.chdir(tmp_path) + + root = RootFolder() + + assert root.get() == tmp_path.resolve() + + +def test_rootfolder_sets_explicit_path(tmp_path): + root = RootFolder(tmp_path) + + assert root.get() == tmp_path.resolve() + + +def test_rootfolder_expands_relative_paths(tmp_path): + root = RootFolder(tmp_path) + + assert root.expand_path("config.yaml") == (tmp_path / "config.yaml").resolve() + + +def test_rootfolder_expands_absolute_paths(tmp_path): + root = RootFolder(tmp_path) + absolute = (tmp_path / "nested" / "config.yaml").resolve() + + assert root.expand_path(absolute) == absolute + + +def test_rootfolder_set_updates_root(tmp_path): + root = RootFolder(tmp_path) + new_root = tmp_path / "other" + + before = root.expand_path("config.yaml") + root.set(new_root) + after = root.expand_path("config.yaml") + + assert root.get() == new_root.resolve() + assert before == (tmp_path / "config.yaml").resolve() + assert after == (new_root / "config.yaml").resolve() + + +def test_is_supported_file(): + assert _is_supported_file("config.yaml") + assert _is_supported_file("config.yml") + assert _is_supported_file("config.json") + + assert not _is_supported_file("config.txt") + assert not _is_supported_file(1) + assert not _is_supported_file(None) + + +def test_load_context_adds_and_removes_paths(tmp_path): + ctx = LoadContext() + path = tmp_path / "config.yaml" + + with ctx.loading(path): + assert ctx.include_stack == [path] + + assert ctx.include_stack == [] + + +def test_load_context_cleans_up_after_exception(tmp_path): + ctx = LoadContext() + path = tmp_path / "config.yaml" + + with pytest.raises(RuntimeError): + with ctx.loading(path): + raise RuntimeError + + assert ctx.include_stack == [] + + +def test_load_yaml(tmp_path): + ROOT.set(tmp_path) + + config = tmp_path / "config.yaml" + config.write_text("a: 1\nb: hello\n") + + result = load("config.yaml") + + assert result["a"] == 1 + assert result["b"] == "hello" + + +def test_load_json(tmp_path): + ROOT.set(tmp_path) + + config = tmp_path / "config.json" + config.write_text(json.dumps({"a": 1, "b": "hello"})) + + result = load("config.json") + + assert result == {"a": 1, "b": "hello"} + + +def test_load_nested_yaml(tmp_path): + ROOT.set(tmp_path) + + (tmp_path / "child.yaml").write_text("answer: 42\n") + + (tmp_path / "parent.yaml").write_text("child: child.yaml\n") + + result = load("parent.yaml") + + assert result["child"]["answer"] == 42 + + +def test_load_nested_json(tmp_path): + ROOT.set(tmp_path) + + (tmp_path / "child.json").write_text(json.dumps({"answer": 42})) + + (tmp_path / "parent.json").write_text(json.dumps({"child": "child.json"})) + + result = load("parent.json") + + assert result["child"]["answer"] == 42 + + +def test_load_file_resolver_loads_nested_file(tmp_path): + ROOT.set(tmp_path) + + (tmp_path / "subdir").mkdir() + (tmp_path / "subdir" / "child.yaml").write_text("answer: 42\n") + (tmp_path / "parent.yaml").write_text('target: "${file:subdir/child.yaml}"\n') + + result = load("parent.yaml") + + assert result["target"]["answer"] == 42 + + +def test_load_env_resolver_resolves_environment_variable(tmp_path, monkeypatch): + ROOT.set(tmp_path) + + monkeypatch.setenv("TANGO_HOST", "localhost:10000") + (tmp_path / "config.yaml").write_text("host: ${env:TANGO_HOST}\n") + + result = load("config.yaml") + + assert result["host"] == "localhost:10000" + + +def test_load_env_resolver_missing_variable_raises(tmp_path, monkeypatch): + ROOT.set(tmp_path) + + monkeypatch.delenv("TANGO_HOST", raising=False) + (tmp_path / "config.yaml").write_text("host: ${env:TANGO_HOST}\n") + + with pytest.raises(PyAMLException, match="Environment variable 'TANGO_HOST' is not set"): + load("config.yaml") + + +def test_interpolates_env_inside_string(tmp_path, monkeypatch): + ROOT.set(tmp_path) + monkeypatch.setenv("HOST", "localhost") + monkeypatch.setenv("PORT", "5432") + + (tmp_path / "config.yaml").write_text("url: http://${env:HOST}:${env:PORT}\n") + + result = load("config.yaml") + + assert result["url"] == "http://localhost:5432" + + +def test_load_interpolates_env_multiple_times_in_one_string(tmp_path, monkeypatch): + ROOT.set(tmp_path) + + monkeypatch.setenv("USER", "alice") + + (tmp_path / "config.yaml").write_text("message: hello ${env:USER}, ${env:USER}!\n") + + result = load("config.yaml") + + assert result["message"] == "hello alice, alice!" + + +def test_load_path_resolver_resolves_without_loading_file(tmp_path): + ROOT.set(tmp_path) + + (tmp_path / "config.yaml").write_text("target: ${path:subdir/missing.json}\n") + + result = load("config.yaml") + + assert result["target"] == str((tmp_path / "subdir" / "missing.json").resolve()) + + +def test_load_interpolated_file_resolver_inside_string_raises(tmp_path): + ROOT.set(tmp_path) + + (tmp_path / "child.yaml").write_text("answer: 42\n") + (tmp_path / "config.yaml").write_text('value: "prefix-${file:child.yaml}-suffix"\n') + + with pytest.raises(PyAMLException, match="cannot be interpolated into a string"): + load("config.yaml") + + +def test_load_interpolation_unknown_resolver_raises(tmp_path): + ROOT.set(tmp_path) + + (tmp_path / "config.yaml").write_text("value: prefix-${missing:VALUE}-suffix\n") + + with pytest.raises(PyAMLException, match="Unknown resolver 'missing'"): + load("config.yaml") + + +def test_load_list_include_extends_list(tmp_path): + ROOT.set(tmp_path) + + (tmp_path / "items.yaml").write_text("- one\n- two\n") + + (tmp_path / "parent.yaml").write_text( + """ + values: + - start + - items.yaml + - end + """.strip() + ) + + result = load("parent.yaml") + + assert result["values"] == [ + "start", + "one", + "two", + "end", + ] + + +def test_load_yaml_omits_locations_by_default(tmp_path): + ROOT.set(tmp_path) + + (tmp_path / "config.yaml").write_text("a: 1\n") + + result = load("config.yaml") + + assert LOCATION_KEY not in result + assert FIELD_LOCATIONS_KEY not in result + + +def test_load_yaml_includes_locations_when_enables(tmp_path): + ROOT.set(tmp_path) + + (tmp_path / "config.yaml").write_text("a: 1\n") + + result = load("config.yaml", include_locations=True) + + assert LOCATION_KEY in result + assert FIELD_LOCATIONS_KEY in result + + +def test_load_invalid_yaml_raises_pyaml_exception(tmp_path): + ROOT.set(tmp_path) + + (tmp_path / "bad.yaml").write_text("a:\n - 1\n - 2\n") + + with pytest.raises(PyAMLException, match="bad.yaml"): + load("bad.yaml") + + +def test_load_invalid_json_raises_pyaml_exception(tmp_path): + ROOT.set(tmp_path) + + (tmp_path / "bad.json").write_text('{"a": }') + + with pytest.raises(PyAMLException, match="bad.json"): + load("bad.json") + + +def test_load_circular_include_raises_pyaml_exception(tmp_path): + ROOT.set(tmp_path) + + (tmp_path / "a.yaml").write_text("b: b.yaml\n") + (tmp_path / "b.yaml").write_text("a: a.yaml\n") + + with pytest.raises(PyAMLException, match="Circular file inclusion"): + load("a.yaml") diff --git a/tests/conftest.py b/tests/conftest.py index 030cb61f5..a39aef1d8 100644 --- a/tests/conftest.py +++ b/tests/conftest.py @@ -1,5 +1,6 @@ import importlib import importlib.machinery +import os import pathlib import sys import types @@ -215,6 +216,10 @@ def _installed_test_packages( @pytest.fixture(scope="session", autouse=True) def install_default_test_packages(): + if os.environ.get("PYAML_DT4ACC_INTEGRATION") == "1": + yield + return + package_paths = [spec.local_path.resolve() for spec in _TEST_PACKAGES.values()] with _installed_test_packages( package_paths, diff --git a/tests/control/test_aggregator.py b/tests/control/test_aggregator.py new file mode 100644 index 000000000..9efd31f07 --- /dev/null +++ b/tests/control/test_aggregator.py @@ -0,0 +1,35 @@ +import numpy as np +import pytest + +from pyaml.accelerator import Accelerator + + +@pytest.mark.parametrize( + "install_test_package", + [{"name": "tango-pyaml", "path": "tests/dummy_cs/tango-pyaml"}], + indirect=True, +) +def test_aggregator(install_test_package): + sr = Accelerator.load("tests/config/sr.yaml") + agg = sr.live.get_aggregator() + agg.add_devices(sr.live.get_device_access("srdiag/bpm/c04-01/SA_HPosition")) + agg.add_devices(sr.live.get_device_access("srdiag/bpm/c04-01/SA_VPosition")) + agg.add_devices(sr.live.get_device_access("srdiag/bpm/c04-02/SA_HPosition")) + agg.add_devices(sr.live.get_device_access("srdiag/bpm/c04-02/SA_VPosition")) + + # Iterator and index + assert agg.len() == 4 + + for idx, d in enumerate(agg): + plane = "H" if idx % 2 == 0 else "V" + assert f"c04-{(idx >> 1) + 1:02d}/SA_{plane}" in repr(d) + + assert "srdiag/bpm/c04-02/SA_HPosition" in repr(agg[2]) + + # Immutable behavior + with pytest.raises(TypeError, match="does not support item assignment"): + agg[1] = sr.live.get_device_access("srdiag/bpm/c04-01/SA_HPosition") + + # Values + assert np.shape(agg.get()) == (4,) + assert agg.unit() == ["m", "m", "m", "m"] diff --git a/tests/test_dummy_tango_attributes.py b/tests/control/test_dummy_tango_attributes.py similarity index 97% rename from tests/test_dummy_tango_attributes.py rename to tests/control/test_dummy_tango_attributes.py index 20747e298..ac3454819 100644 --- a/tests/test_dummy_tango_attributes.py +++ b/tests/control/test_dummy_tango_attributes.py @@ -66,5 +66,5 @@ def test_dummy_tango_read_only_attribute_can_be_initialized(install_test_package assert attribute.get() == 0.37 assert attribute.unit() == "1" - with pytest.raises(Exception, match="read only attribute"): + with pytest.raises(Exception, match="not writable"): attribute.set(0.38) diff --git a/tests/test_ranges.py b/tests/control/test_ranges.py similarity index 100% rename from tests/test_ranges.py rename to tests/control/test_ranges.py diff --git a/tests/test_values.py b/tests/control/test_values.py similarity index 100% rename from tests/test_values.py rename to tests/control/test_values.py diff --git a/tests/dummy_cs/tango-pyaml/tango/pyaml/attribute.py b/tests/dummy_cs/tango-pyaml/tango/pyaml/attribute.py index cc19566f6..053ab8fbc 100644 --- a/tests/dummy_cs/tango-pyaml/tango/pyaml/attribute.py +++ b/tests/dummy_cs/tango-pyaml/tango/pyaml/attribute.py @@ -1,5 +1,8 @@ +from typing import Optional + from pydantic import BaseModel, ConfigDict +from pyaml.common.exception import PyAMLException from pyaml.control.deviceaccess import DeviceAccess from pyaml.control.readback_value import Value @@ -13,85 +16,77 @@ class ConfigModel(BaseModel): attribute: str unit: str = "" - range: tuple[float | None, float | None] | None = None + range: Optional[tuple[Optional[float], Optional[float]]] = None + index: Optional[int] = None class Attribute(DeviceAccess): """ - Class that implements a default device class that just prints out - values (Debugging purpose) + Dummy attribute backed by a shared in-memory state store. + + When ``index`` is set the attribute presents a read-only scalar view of + one element of a vector attribute; writes are rejected and the underlying + store is automatically marked as an array. """ - def __init__(self, cfg: ConfigModel, is_array=False): + def __init__(self, cfg: ConfigModel): super().__init__() self._cfg = cfg - self._setpoint = cfg.attribute - self._readback = cfg.attribute - # Register metadata early. The value may already have been initialized - # by a test before the accelerator configuration is loaded. - get_state(cfg.attribute, unit=cfg.unit, range=self._range()) + self._index = cfg.index + state = get_state(cfg.attribute, unit=cfg.unit, range=cfg.range) + if self._index is not None: + state.is_array = True def set_array(self, is_array: bool): """Mark the shared value as array-like without initializing it.""" - get_state( - self._cfg.attribute, - unit=self._cfg.unit, - range=self._range(), - ).is_array = is_array + get_state(self._cfg.attribute, unit=self._cfg.unit, range=self._cfg.range).is_array = is_array def name(self) -> str: - return self._setpoint + if self._index is not None: + return f"{self._cfg.attribute}[{self._index}]" + return self._cfg.attribute def measure_name(self) -> str: - return self._readback + return self.name() def set(self, value): - print(f"{self._cfg.attribute}:{value}") - state = get_state(self._cfg.attribute, unit=self._cfg.unit, range=self._range()) + if self._index is not None: + raise PyAMLException( + f"Indexed attribute '{self._cfg.attribute}[{self._index}]' does not support individual element writes." + ) + state = get_state(self._cfg.attribute, unit=self._cfg.unit, range=self._cfg.range) state.value = value def set_and_wait(self, value): self.set(value) def get(self): - state = get_state(self._cfg.attribute, unit=self._cfg.unit, range=self._range()) + state = get_state(self._cfg.attribute, unit=self._cfg.unit, range=self._cfg.range) + if self._index is not None: + return state.value[self._index] return state.value def readback(self): """Return readback from shared state, preserving scalar/array shape.""" - state = get_state( - self._cfg.attribute, - unit=self._cfg.unit, - range=self._range(), - ) + state = get_state(self._cfg.attribute, unit=self._cfg.unit, range=self._cfg.range) value = state.value if state.readback is None else state.readback + if self._index is not None: + return Value(value[self._index]) if state.is_array: return [Value(v) for v in value] return Value(value) def unit(self) -> str: - state = get_state(self._cfg.attribute, unit=self._cfg.unit, range=self._range()) - return state.unit + return get_state(self._cfg.attribute, unit=self._cfg.unit, range=self._cfg.range).unit def __repr__(self): return repr(self._cfg).replace("ConfigModel", self.__class__.__name__) def get_range(self) -> list[float]: - state = get_state( - self._cfg.attribute, - unit=self._cfg.unit, - range=self._range(), - ) + state = get_state(self._cfg.attribute, unit=self._cfg.unit, range=self._cfg.range) if state.range is None: return [None, None] - return [ - state.range[0] if state.range[0] is not None else None, - state.range[1] if state.range[1] is not None else None, - ] + return [state.range[0], state.range[1]] def check_device_availability(self) -> bool: return True - - def _range(self): - """Return optional range metadata for models that define it.""" - return getattr(self._cfg, "range", None) diff --git a/tests/dummy_cs/tango-pyaml/tango/pyaml/attribute_read_only.py b/tests/dummy_cs/tango-pyaml/tango/pyaml/attribute_read_only.py index b42b54467..5c5809dde 100644 --- a/tests/dummy_cs/tango-pyaml/tango/pyaml/attribute_read_only.py +++ b/tests/dummy_cs/tango-pyaml/tango/pyaml/attribute_read_only.py @@ -1,39 +1,19 @@ -from pydantic import BaseModel, ConfigDict +from pyaml.common.exception import PyAMLException -from pyaml.control.readback_value import Value - -from .attribute import Attribute +from .attribute import Attribute, ConfigModel PYAMLCLASS: str = "AttributeReadOnly" -class ConfigModel(BaseModel): - model_config = ConfigDict(arbitrary_types_allowed=True, extra="forbid") - - attribute: str - unit: str = "" - - class AttributeReadOnly(Attribute): - """ - Class that implements a default device class that just prints out - values (Debugging purpose) - """ - def __init__(self, cfg: ConfigModel): super().__init__(cfg) def set(self, value): - raise Exception(f"{self._cfg.attribute} is read only attribute") + raise PyAMLException(f"Tango attribute {self._cfg.attribute} is not writable.") def set_and_wait(self, value): - raise Exception(f"{self._cfg.attribute} is read only attribute") - - def unit(self) -> str: - return super().unit() - - def get_range(self) -> list[float]: - return super().get_range() + raise PyAMLException(f"Tango attribute {self._cfg.attribute} is not writable.") - def check_device_availability(self) -> bool: - return True + def get(self): + return self.readback().value diff --git a/tests/dummy_cs/tango-pyaml/tango/pyaml/attribute_with_tango_powersupply_mocking_behaviour.py b/tests/dummy_cs/tango-pyaml/tango/pyaml/attribute_with_tango_powersupply_mocking_behaviour.py index c336b1835..e0c37a513 100644 --- a/tests/dummy_cs/tango-pyaml/tango/pyaml/attribute_with_tango_powersupply_mocking_behaviour.py +++ b/tests/dummy_cs/tango-pyaml/tango/pyaml/attribute_with_tango_powersupply_mocking_behaviour.py @@ -5,9 +5,9 @@ from scipy.constants import speed_of_light from pyaml.configuration import get_root_folder -from pyaml.configuration.curve import Curve from pyaml.control.deviceaccess import DeviceAccess from pyaml.control.readback_value import Value +from pyaml.magnet.curve import Curve PYAMLCLASS: str = "AttributeWithTangoMockingBehaviour" diff --git a/tests/dummy_cs/tango-pyaml/tango/pyaml/catalog.py b/tests/dummy_cs/tango-pyaml/tango/pyaml/catalog.py new file mode 100644 index 000000000..c71444b4b --- /dev/null +++ b/tests/dummy_cs/tango-pyaml/tango/pyaml/catalog.py @@ -0,0 +1,43 @@ +"""Configuration helpers for backend-provided catalogs.""" + +from abc import ABCMeta, abstractmethod + +from pydantic import BaseModel, ConfigDict + +from pyaml.control.deviceaccess import DeviceAccess + + +class CatalogConfigModel(BaseModel): + r""" + Base configuration model for named catalogs. + + Parameters + ---------- + name : str + Unique catalog identifier used in accelerator and control-system + configuration. + """ + + model_config = ConfigDict(arbitrary_types_allowed=True, extra="forbid") + + +class Catalog(metaclass=ABCMeta): + r""" + Abstract class for backend catalog configuration objects. + + Notes + ----- + Concrete catalogs live in each control-system package. They may expose + backend-specific resolution APIs, but those APIs are not called by the + PyAML core. + """ + + def __init__(self, cfg: CatalogConfigModel): + self._cfg = cfg + + @abstractmethod + def resolve(self, key: str) -> DeviceAccess: + """ + Return + """ + pass diff --git a/tests/dummy_cs/tango-pyaml/tango/pyaml/controlsystem.py b/tests/dummy_cs/tango-pyaml/tango/pyaml/controlsystem.py index 68fee777c..0955d9c0e 100644 --- a/tests/dummy_cs/tango-pyaml/tango/pyaml/controlsystem.py +++ b/tests/dummy_cs/tango-pyaml/tango/pyaml/controlsystem.py @@ -1,10 +1,15 @@ import copy -import os +from typing import Any from pydantic import BaseModel, ConfigDict +from pyaml import PyAMLException from pyaml.control.controlsystem import ControlSystem from pyaml.control.deviceaccess import DeviceAccess +from pyaml.control.deviceaccesslist import DeviceAccessList + +from .catalog import Catalog +from .multi_attribute import MultiAttribute PYAMLCLASS: str = "TangoControlSystem" @@ -13,38 +18,63 @@ class ConfigModel(BaseModel): model_config = ConfigDict(arbitrary_types_allowed=True, extra="forbid") name: str - tango_host: str - debug_level: str = None + tango_host: str | None = None + catalog: Catalog | None = None + debug_level: str | None = None + lazy_devices: bool = True + timeout_ms: int = 3000 class TangoControlSystem(ControlSystem): def __init__(self, cfg: ConfigModel): super().__init__() self._cfg = cfg - print(f"Creating dummy TangoControlSystem: {cfg.name}") - self.__DEVICES = {} + self.__devices = {} - def attach_array(self, devs: list[DeviceAccess]) -> list[DeviceAccess]: + def attach_array(self, devs: list[DeviceAccess | None]) -> list[DeviceAccess | None]: return self._attach(devs, True) - def attach(self, devs: list[DeviceAccess]) -> list[DeviceAccess]: + def attach(self, devs: list[DeviceAccess | None]) -> list[DeviceAccess | None]: return self._attach(devs, False) - def _attach(self, devs: list[DeviceAccess], is_array: bool) -> list[DeviceAccess]: + def get_device_access(self, ref: str | BaseModel | None) -> DeviceAccess | None: + if ref is None: + return None + + if isinstance(ref, str): + if self._cfg.catalog is None: + raise PyAMLException(f"Control system '{self.name()}' has no catalog configured for key '{ref}'") + try: + dev = self._cfg.catalog.resolve(ref) + except AttributeError as exc: + raise PyAMLException(f"Control system '{self.name()}' catalog cannot resolve key '{ref}'") from exc + return self._attach([dev], False)[0] + + from .attribute import Attribute + from .attribute import ConfigModel as AttributeConfigModel + + if isinstance(ref, AttributeConfigModel): + return self._attach([Attribute(ref)], False)[0] + + raise PyAMLException(f"Control system '{self.name()}' cannot build a device from {type(ref).__name__}") + + def _attach(self, devs: list[DeviceAccess | None], is_array: bool) -> list[DeviceAccess | None]: newDevs = [] for d in devs: if d is not None: - full_name = "//" + self._cfg.tango_host + "/" + d._cfg.attribute - if full_name not in self.__DEVICES: - # Shallow copy the object + if self._cfg.tango_host: + full_name = "//" + self._cfg.tango_host + "/" + d._cfg.attribute + else: + full_name = d._cfg.attribute + index = getattr(d._cfg, "index", None) + cache_key = full_name if index is None else f"{full_name}[{index}]" + if cache_key not in self.__devices: newDev = copy.copy(d) - # Shallow copy the config object - # to allow a new attribute name newDev._cfg = copy.copy(d._cfg) newDev._cfg.attribute = full_name newDev.set_array(is_array) - self.__DEVICES[full_name] = newDev - newDevs.append(self.__DEVICES[full_name]) + self.__devices[cache_key] = newDev + newDevs.append(self.__devices[cache_key]) else: newDevs.append(None) return newDevs @@ -52,11 +82,8 @@ def _attach(self, devs: list[DeviceAccess], is_array: bool) -> list[DeviceAccess def name(self) -> str: return self._cfg.name - def scalar_aggregator(self) -> str | None: - return "tango.pyaml.multi_attribute" - - def vector_aggregator(self) -> str | None: - return None + def get_aggregator(self) -> str | None: + return MultiAttribute() def __repr__(self): return repr(self._cfg).replace("ConfigModel", self.__class__.__name__) diff --git a/tests/dummy_cs/tango-pyaml/tango/pyaml/multi_attribute.py b/tests/dummy_cs/tango-pyaml/tango/pyaml/multi_attribute.py index 8fd8619f7..9235fd4a1 100644 --- a/tests/dummy_cs/tango-pyaml/tango/pyaml/multi_attribute.py +++ b/tests/dummy_cs/tango-pyaml/tango/pyaml/multi_attribute.py @@ -1,44 +1,18 @@ import numpy as np from numpy import typing as npt -from pydantic import BaseModel import pyaml from pyaml.control.deviceaccess import DeviceAccess from pyaml.control.deviceaccesslist import DeviceAccessList from .attribute import Attribute -from .attribute import ConfigModel as AttributeConfigModel - -PYAMLCLASS: str = "MultiAttribute" LAST_NB_WRITTEN = 0 -class ConfigModel(BaseModel): - """ - Configuration model for a list of DeviceAccess. - - Attributes - ---------- - attributes : list of str - List of Tango attribute paths. - name : str, optional - Group name. - unit : str, optional - Unit of the attributes. - """ - - attributes: list[str] = [] - name: str = "" - - class MultiAttribute(DeviceAccessList): - def __init__(self, cfg: ConfigModel = None): - super().__init__() - self._cfg = cfg - if cfg.attributes: - for name in cfg.attributes: - self.add_devices(Attribute(AttributeConfigModel(name, cfg.unit))) + def __init__(self): + self._items = [] def add_devices(self, devices: DeviceAccess | list[DeviceAccess]): if isinstance(devices, list): @@ -49,7 +23,7 @@ def add_devices(self, devices: DeviceAccess | list[DeviceAccess]): (tango.pyaml.attribute) but got ({device.__class__.__name__})""" ) - super().extend(devices) + self._items.extend(devices) else: if not isinstance(devices, Attribute): raise pyaml.PyAMLException( @@ -57,46 +31,46 @@ def add_devices(self, devices: DeviceAccess | list[DeviceAccess]): (tango.pyaml.attribute) but got ({devices.__class__.__name__})""" ) - super().append(devices) + self._items.append(devices) - def get_devices(self) -> DeviceAccess | list[DeviceAccess]: - if len(self) == 1: - return self[0] - else: - return self + def len(self) -> int: + return len(self._items) + + def get_device_at(self, index: int) -> DeviceAccess: + return self._items[index] def set(self, value: npt.NDArray[np.float64]): print(f"MultiAttribute.set({len(value)} values)") global LAST_NB_WRITTEN LAST_NB_WRITTEN += len(value) - for idx, a in enumerate(self): + for idx, a in enumerate(self._items): a.set(value[idx]) def set_and_wait(self, value: npt.NDArray[np.float64]): pass def get(self) -> npt.NDArray[np.float64]: - print(f"MultiAttribute.get({len(self)} values)") - return np.array([a.get() for a in self]) + print(f"MultiAttribute.get({len(self._items)} values)") + return np.array([a.get() for a in self._items]) def readback(self) -> np.array: return np.array([]) def unit(self) -> list[str]: - return [a.unit() for a in self] + return [a.unit() for a in self._items] def get_last_nb_written(self) -> int: return self.__last_nb_written def get_range(self) -> list[float]: attr_range: list[float] = [] - for device in self: + for device in self._items: attr_range.extend(device.get_range()) return attr_range def check_device_availability(self) -> bool: available = False - for device in self: + for device in self._items: available = device.check_device_availability() if not available: break diff --git a/tests/dummy_cs/tango-pyaml/tango/pyaml/static_catalog.py b/tests/dummy_cs/tango-pyaml/tango/pyaml/static_catalog.py new file mode 100644 index 000000000..093a04cd3 --- /dev/null +++ b/tests/dummy_cs/tango-pyaml/tango/pyaml/static_catalog.py @@ -0,0 +1,34 @@ +from pydantic import ConfigDict + +from pyaml import PyAMLException +from pyaml.control.deviceaccess import DeviceAccess + +from .catalog import Catalog, CatalogConfigModel +from .static_catalog_entry import StaticCatalogEntry + +PYAMLCLASS = "StaticCatalog" + + +class ConfigModel(CatalogConfigModel): + model_config = ConfigDict(arbitrary_types_allowed=True, extra="forbid") + + entries: list[StaticCatalogEntry] + + +class StaticCatalog(Catalog): + def __init__(self, cfg: ConfigModel): + super().__init__(cfg) + if len(cfg.entries) == 0: + raise PyAMLException("StaticCatalog.entries must contain at least one entry") + self._refs: dict[str, DeviceAccess] = {} + for entry in cfg.entries: + key = entry.get_key() + if key in self._refs: + raise PyAMLException(f"StaticCatalog.entries contains duplicate key '{key}'") + self._refs[key] = entry.get_device() + + def resolve(self, key: str) -> DeviceAccess: + try: + return self._refs[key] + except KeyError as exc: + raise PyAMLException(f"Catalog cannot resolve key '{key}'") from exc diff --git a/tests/dummy_cs/tango-pyaml/tango/pyaml/static_catalog_entry.py b/tests/dummy_cs/tango-pyaml/tango/pyaml/static_catalog_entry.py new file mode 100644 index 000000000..b9ed8c92b --- /dev/null +++ b/tests/dummy_cs/tango-pyaml/tango/pyaml/static_catalog_entry.py @@ -0,0 +1,23 @@ +from pydantic import BaseModel, ConfigDict + +from pyaml.control.deviceaccess import DeviceAccess + +PYAMLCLASS = "StaticCatalogEntry" + + +class ConfigModel(BaseModel): + model_config = ConfigDict(arbitrary_types_allowed=True, extra="forbid") + + key: str + device: DeviceAccess + + +class StaticCatalogEntry: + def __init__(self, cfg: ConfigModel): + self._cfg = cfg + + def get_key(self) -> str: + return self._cfg.key + + def get_device(self) -> DeviceAccess: + return self._cfg.device diff --git a/tests/dummy_cs/tango-pyaml/tango/pyaml/tango_catalog.py b/tests/dummy_cs/tango-pyaml/tango/pyaml/tango_catalog.py new file mode 100644 index 000000000..59f546e07 --- /dev/null +++ b/tests/dummy_cs/tango-pyaml/tango/pyaml/tango_catalog.py @@ -0,0 +1,51 @@ +from pydantic import ConfigDict + +from pyaml.common.exception import PyAMLException +from pyaml.control.deviceaccess import DeviceAccess + +from .catalog import Catalog, CatalogConfigModel + +PYAMLCLASS = "TangoCatalog" + + +class ConfigModel(CatalogConfigModel): + model_config = ConfigDict(arbitrary_types_allowed=True, extra="forbid") + + disconnected: bool = False + + +class TangoCatalog(Catalog): + def __init__(self, cfg: ConfigModel): + super().__init__(cfg) + self._refs: dict[str, DeviceAccess] = {} + + def resolve(self, key: str) -> DeviceAccess: + if key not in self._refs: + attr_path, index = self._parse_key(key) + from .attribute import Attribute + from .attribute import ConfigModel as AttributeConfigModel + + self._refs[key] = Attribute(AttributeConfigModel(attribute=attr_path, index=index)) + return self._refs[key] + + def _parse_key(self, key: str) -> tuple[str, int | None]: + if not isinstance(key, str): + raise PyAMLException(f"Tango catalog '{self.get_name()}' expects string keys, got {type(key).__name__}") + if "@" in key: + attr_path, idx_str = key.rsplit("@", 1) + try: + index = int(idx_str) + except ValueError: + raise PyAMLException(f"Tango catalog '{self.get_name()}' invalid index '{idx_str}' in key '{key}'.") from None + else: + attr_path = key + index = None + + parts = attr_path.split("/") + if len(parts) != 4 or any(part == "" for part in parts): + raise PyAMLException( + f"Tango catalog '{self.get_name()}' cannot resolve invalid Tango attribute " + f"reference '{key}'. Expected 'domain/family/member/attribute' or " + f"'domain/family/member/attribute@index'." + ) + return attr_path, index diff --git a/tests/external/pyaml_external/external_magnet_model.py b/tests/external/pyaml_external/external_magnet_model.py index 14e83b89a..43d1411de 100644 --- a/tests/external/pyaml_external/external_magnet_model.py +++ b/tests/external/pyaml_external/external_magnet_model.py @@ -16,7 +16,7 @@ class ConfigModel(BaseModel): model_config = ConfigDict(arbitrary_types_allowed=True, extra="forbid") - powersupply: DeviceAccess + powersupply: str param: str = None @@ -30,7 +30,7 @@ class ExternalMagnetModel(MagnetModel): """ def __init__(self, cfg: ConfigModel): - print("ExternalMagnetModel:\n powersupply:%s\n param:%s" % (cfg.powersupply.name(), cfg.param)) + print("ExternalMagnetModel:\n powersupply:%s\n param:%s" % (cfg.powersupply, cfg.param)) self._cfg = cfg # Implementation of the MagnetModel abstract class @@ -53,7 +53,7 @@ def get_strength_units(self) -> list[str]: def get_hardware_units(self) -> list[str]: return ["A"] - def get_devices(self) -> list[DeviceAccess]: + def get_device_names(self) -> list[DeviceAccess]: return [self._cfg.powersupply] def has_hardware(self) -> bool: diff --git a/tests/integration/start_dt4acc_twin.sh b/tests/integration/start_dt4acc_twin.sh new file mode 100644 index 000000000..eea0bff3d --- /dev/null +++ b/tests/integration/start_dt4acc_twin.sh @@ -0,0 +1,329 @@ +#!/usr/bin/env bash +set -Eeuo pipefail + +DEFAULT_IMAGE_URI="oras://registry.synchrotron-soleil.fr/software_control_system_public/dt4acc-soleil-twin:latest" +READY_PATTERN="Calculation heartbeat: simulator/ringsimulator/ringsimulator reachable" + +usage() { + cat <<'EOF' +Usage: + start_dt4acc_twin.sh --accelerator-setup-file FILE --lattice-file FILE [options] + start_dt4acc_twin.sh FILE.json FILE.m [options] + +Required simulator input data: + --accelerator-setup-file FILE Accelerator setup JSON file passed to the twin. + --lattice-file FILE Lattice file passed to the twin. + +Options: + --tango-host HOST Tango database host. Default: localhost. + --tango-port PORT Tango database port. If omitted, the twin may choose it. + --image-uri URI Apptainer image URI. Default: dt4acc latest ORAS image. + --sif FILE Use a local SIF file instead of --image-uri. + --log-file FILE Log file path. Default: mktemp under /tmp. + --pid-file FILE Write the Apptainer process PID to FILE. + --timeout SECONDS Readiness timeout. Default: 900. + --detach Exit after readiness and leave the twin running. + -h, --help Show this help. + +The script prints "Ready to use" when the twin reaches the same heartbeat used by +the dt4acc-integration CI workflow. Keep this process running; press Ctrl-C to +stop the twin. With --detach, the script exits after readiness; use --pid-file +so a later step can stop the twin. +EOF +} + +accelerator_setup_file="" +lattice_file="" +tango_host="localhost" +tango_port="" +image_uri="${DEFAULT_IMAGE_URI}" +sif_file="" +log_file="" +pid_file="" +timeout_seconds="900" +detach="0" +positionals=() + +while (($#)); do + case "$1" in + --accelerator-setup-file|--setup-file) + accelerator_setup_file="${2:-}" + shift 2 + ;; + --lattice-file) + lattice_file="${2:-}" + shift 2 + ;; + --tango-host) + tango_host="${2:-}" + shift 2 + ;; + --tango-port) + tango_port="${2:-}" + shift 2 + ;; + --image-uri) + image_uri="${2:-}" + shift 2 + ;; + --sif) + sif_file="${2:-}" + shift 2 + ;; + --log-file) + log_file="${2:-}" + shift 2 + ;; + --pid-file) + pid_file="${2:-}" + shift 2 + ;; + --timeout) + timeout_seconds="${2:-}" + shift 2 + ;; + --detach) + detach="1" + shift + ;; + -h|--help) + usage + exit 0 + ;; + --) + shift + while (($#)); do + positionals+=("$1") + shift + done + ;; + -*) + echo "Unknown option: $1" >&2 + usage >&2 + exit 2 + ;; + *) + positionals+=("$1") + shift + ;; + esac +done + +if [[ -z "${accelerator_setup_file}" && ${#positionals[@]} -ge 1 ]]; then + accelerator_setup_file="${positionals[0]}" +fi + +if [[ -z "${lattice_file}" && ${#positionals[@]} -ge 2 ]]; then + lattice_file="${positionals[1]}" +fi + +if [[ ${#positionals[@]} -gt 2 ]]; then + echo "Too many positional arguments." >&2 + usage >&2 + exit 2 +fi + +if [[ -z "${accelerator_setup_file}" || -z "${lattice_file}" ]]; then + echo "Missing required simulator input data." >&2 + usage >&2 + exit 2 +fi + +if ! command -v apptainer >/dev/null 2>&1; then + echo "apptainer is required but was not found in PATH." >&2 + exit 127 +fi + +if ! command -v setsid >/dev/null 2>&1; then + echo "setsid is required but was not found in PATH." >&2 + exit 127 +fi + +if [[ ! "${timeout_seconds}" =~ ^[0-9]+$ || "${timeout_seconds}" -eq 0 ]]; then + echo "--timeout must be a positive integer." >&2 + exit 2 +fi + +if [[ -n "${tango_port}" && ! "${tango_port}" =~ ^[0-9]+$ ]]; then + echo "--tango-port must be an integer." >&2 + exit 2 +fi + +accelerator_setup_file="$(realpath "${accelerator_setup_file}")" +lattice_file="$(realpath "${lattice_file}")" + +if [[ ! -f "${accelerator_setup_file}" ]]; then + echo "Accelerator setup file not found: ${accelerator_setup_file}" >&2 + exit 2 +fi + +if [[ ! -f "${lattice_file}" ]]; then + echo "Lattice file not found: ${lattice_file}" >&2 + exit 2 +fi + +if [[ -n "${sif_file}" ]]; then + sif_file="$(realpath "${sif_file}")" + if [[ ! -f "${sif_file}" ]]; then + echo "SIF file not found: ${sif_file}" >&2 + exit 2 + fi + image_ref="${sif_file}" +else + image_ref="${image_uri}" +fi + +if [[ -z "${log_file}" ]]; then + log_file="$(mktemp -t dt4acc-twin.XXXXXX.log)" +else + log_file="$(realpath -m "${log_file}")" + mkdir -p "$(dirname "${log_file}")" + : >"${log_file}" +fi + +if [[ -n "${pid_file}" ]]; then + pid_file="$(realpath -m "${pid_file}")" + mkdir -p "$(dirname "${pid_file}")" +fi + +setup_dir="$(dirname "${accelerator_setup_file}")" +setup_base="$(basename "${accelerator_setup_file}")" +lattice_dir="$(dirname "${lattice_file}")" +lattice_base="$(basename "${lattice_file}")" + +bind_args=() +if [[ "${setup_dir}" == "${lattice_dir}" ]]; then + bind_args+=(--bind "${setup_dir}:/data:ro") + accelerator_setup_container="/data/${setup_base}" + lattice_container="/data/${lattice_base}" +else + bind_args+=(--bind "${setup_dir}:/accelerator-setup:ro") + bind_args+=(--bind "${lattice_dir}:/lattice:ro") + accelerator_setup_container="/accelerator-setup/${setup_base}" + lattice_container="/lattice/${lattice_base}" +fi + +if [[ -n "${tango_port}" ]]; then + requested_tango_host="${tango_host}:${tango_port}" +else + requested_tango_host="${tango_host}" +fi + +detected_tango_port="" +twin_pid="" + +cleanup() { + if [[ -n "${twin_pid}" ]] && kill -0 "${twin_pid}" 2>/dev/null; then + kill -- "-${twin_pid}" 2>/dev/null || kill "${twin_pid}" 2>/dev/null || true + for _ in {1..10}; do + if ! kill -0 "${twin_pid}" 2>/dev/null; then + return + fi + sleep 1 + done + kill -KILL -- "-${twin_pid}" 2>/dev/null || kill -KILL "${twin_pid}" 2>/dev/null || true + fi +} + +detect_tango_port() { + if [[ -n "${tango_port}" ]]; then + printf '%s\n' "${tango_port}" + return 0 + fi + + if [[ ! -s "${log_file}" ]]; then + return 1 + fi + + local detected + # The twin also logs an Mexec port for internal IPC; only the Tango host line is relevant here. + detected="$( + grep -Eai 'TANGO_HOST|tango[-_ ]host' "${log_file}" \ + | sed -nE 's/.*:([0-9]{2,5}).*/\1/p' \ + | tail -n 1 \ + || true + )" + + if [[ -n "${detected}" ]]; then + printf '%s\n' "${detected}" + return 0 + fi + + return 1 +} + +echo "Starting dt4acc twin" +echo " accelerator setup: ${accelerator_setup_file}" +echo " lattice file: ${lattice_file}" +echo " tango host: ${tango_host}" +echo " tango port: ${tango_port:-auto}" +echo " requested TANGO_HOST: ${requested_tango_host}" +echo " image: ${image_ref}" +echo " log file: ${log_file}" +if [[ -n "${pid_file}" ]]; then + echo " pid file: ${pid_file}" +fi + +trap cleanup INT TERM EXIT + +setsid env TANGO_HOST="${requested_tango_host}" apptainer run \ + "${bind_args[@]}" \ + "${image_ref}" \ + tango-db-embedded \ + --force-kill-db \ + --tango-host "${requested_tango_host}" \ + --accelerator-setup-file "${accelerator_setup_container}" \ + --lattice-file "${lattice_container}" \ + >"${log_file}" 2>&1 & + +twin_pid="$!" +if [[ -n "${pid_file}" ]]; then + echo "${twin_pid}" >"${pid_file}" +fi +start_epoch="$(date +%s)" + +while true; do + if ! kill -0 "${twin_pid}" 2>/dev/null; then + echo "dt4acc twin exited before becoming ready. Last log lines:" >&2 + tail -n 200 "${log_file}" >&2 || true + exit 1 + fi + + if [[ -z "${detected_tango_port}" ]]; then + if detected_tango_port="$(detect_tango_port)"; then + echo "Detected Tango database port: ${detected_tango_port}" + echo "Effective TANGO_HOST: ${tango_host}:${detected_tango_port}" + else + detected_tango_port="" + fi + fi + + if grep -q "${READY_PATTERN}" "${log_file}"; then + if [[ -z "${detected_tango_port}" ]]; then + if detected_tango_port="$(detect_tango_port)"; then + echo "Detected Tango database port: ${detected_tango_port}" + echo "Effective TANGO_HOST: ${tango_host}:${detected_tango_port}" + else + echo "Warning: ready heartbeat found, but Tango database port was not detected in logs." >&2 + fi + fi + echo "Ready to use" + if [[ "${detach}" == "1" ]]; then + trap - EXIT + disown "${twin_pid}" 2>/dev/null || true + exit 0 + fi + break + fi + + now_epoch="$(date +%s)" + if (( now_epoch - start_epoch >= timeout_seconds )); then + echo "Timed out after ${timeout_seconds}s waiting for dt4acc twin readiness. Last log lines:" >&2 + tail -n 200 "${log_file}" >&2 || true + exit 1 + fi + + sleep 2 +done + +wait "${twin_pid}" diff --git a/tests/integration/test_dt4acc_twin_smoke.py b/tests/integration/test_dt4acc_twin_smoke.py new file mode 100644 index 000000000..549bdb4e7 --- /dev/null +++ b/tests/integration/test_dt4acc_twin_smoke.py @@ -0,0 +1,212 @@ +import os +from pathlib import Path + +import numpy as np +import pytest +import yaml +from pyaml_test_lattice import configurations, lattices + +from pyaml.accelerator import Accelerator +from pyaml.configuration import ConfigurationManager + +QF_001 = "QF_001" +QF_001_STRENGTH = "AN01-AR/EM-QP/QF.01/magnetic_strength" +RF_REFERENCE_FREQUENCY = "simulator/ringsimulator/ringsimulator/reference_frequency" +EXAMPLES_ROOT = Path(__file__).parent.parent.parent / "examples" / "use_cases" / "config" + +FODO_LATTICE_KEY = "fodo_1gev_6d.json" +FODO_1GEV_6D_TANGO_PYAML_CONFIG_KEY = "pyaml/tango/tango-pyaml/fodo_1gev_6d_pyaml.yaml" +FODO_1GEV_6D_CS_OA_CONFIG_KEY = "pyaml/tango/pyaml-cs-oa/fodo_1gev_6d_pyaml-oa.yaml" +FODO_1GEV_6D_CONFIGS = [ + FODO_1GEV_6D_TANGO_PYAML_CONFIG_KEY, + FODO_1GEV_6D_CS_OA_CONFIG_KEY, +] +pytestmark = [ + pytest.mark.integration, + pytest.mark.skipif( + os.environ.get("PYAML_DT4ACC_INTEGRATION") != "1", + reason="dt4acc Apptainer integration test is opt-in", + ), +] + + +def _readback_value(device_access): + return float(device_access.readback()) + + +def _load_fragment(config_key: str) -> dict: + """Load one pyaml-test-lattice merged config fragment as a plain dict. + + Bypasses pyaml's own YAML loader (which auto-loads any bare + ``*.yaml``/``*.json`` string value as a nested file relative to the + parent file's directory) since the lattice file ships under a different + package subtree (``data/lattice``) than the config fragment + (``data/configuration``). The ``lattice`` and ``catalog`` references are + resolved explicitly instead. + """ + config_path = Path(configurations[config_key]) + fragment = yaml.safe_load(config_path.read_text()) + + fragment["simulators"][0]["lattice"] = str(Path(lattices[FODO_LATTICE_KEY])) + + catalog_name = fragment["controls"][0]["catalog"] + catalog_path = config_path.parent / catalog_name + fragment["controls"][0]["catalog"] = yaml.safe_load(catalog_path.read_text()) + + return fragment + + +def _build_accelerator(config_key: str): + configuration_manager: ConfigurationManager = ConfigurationManager() + configuration_manager.add(_load_fragment(config_key)) + + return Accelerator.from_dict(configuration_manager.to_dict()) + + +@pytest.mark.parametrize("config_key", FODO_1GEV_6D_CONFIGS, ids=["tango-pyaml", "pyaml-cs-oa"]) +def test_dt4acc_twin_accelerator_instantiates_and_reads_live_values(config_key: str): + accelerator = _build_accelerator(config_key) + + assert accelerator.live is not None + assert "live" in accelerator.controls() + + accelerator.live.rf.get("RF") + + reference_frequency = _readback_value(accelerator.live.get_device_access(RF_REFERENCE_FREQUENCY)) + + assert np.isfinite(reference_frequency), f"RF reference frequency is not finite: {reference_frequency!r}" + assert reference_frequency > 0.0, f"RF reference frequency should be positive, got {reference_frequency!r}" + + accelerator.live.magnet.get(QF_001) + magnetic_strength = _readback_value(accelerator.live.get_device_access(QF_001_STRENGTH)) + + assert np.isfinite(magnetic_strength), f"{QF_001} magnetic strength is not finite: {magnetic_strength!r}" + assert magnetic_strength > 0.0, f"{QF_001} magnetic strength should be positive, got {magnetic_strength!r}" + + +@pytest.mark.parametrize("config_key", FODO_1GEV_6D_CONFIGS, ids=["tango-pyaml", "pyaml-cs-oa"]) +def test_dt4acc_twin_reads_all_declared_magnetic_strengths(config_key: str): + accelerator = _build_accelerator(config_key) + magnets = [magnet for magnet in accelerator.live.magnets.get() if magnet.get_model_name() == magnet.get_name()] + combined_function_magnets = accelerator.live.combined_function_magnet.all() + + assert magnets or combined_function_magnets + + failures = [] + for magnet in magnets: + try: + value = float(magnet.strength.get()) + except Exception as exc: # noqa: BLE001 - report all unavailable Tango attributes at once. + failures.append(f"{magnet.get_name()}: {type(exc).__name__}: {exc}") + continue + + if not np.isfinite(value): + failures.append(f"{magnet.get_name()}: non-finite value {value!r}") + + for magnet in combined_function_magnets: + try: + values = np.asarray(magnet.strengths.get(), dtype=float) + except Exception as exc: # noqa: BLE001 - report all unavailable Tango attributes at once. + failures.append(f"{magnet.get_name()}: {type(exc).__name__}: {exc}") + continue + + if not np.all(np.isfinite(values)): + failures.append(f"{magnet.get_name()}: non-finite values {values!r}") + + assert not failures, "Magnetic strength readback failures:\n" + "\n".join(failures) + + +@pytest.mark.parametrize( + ("root_folder", "config_file"), + [ + (EXAMPLES_ROOT / "bessy2", "bessy2.yaml"), + (EXAMPLES_ROOT / "soleil_ii", "p.yaml"), + ], + ids=["bessy_ii", "soleil_ii"], +) +def test_examples_can_be_loaded(root_folder: Path, config_file: str): + accelerator: Accelerator = Accelerator.load(str(root_folder / config_file)) + assert accelerator.yellow_pages is not None + + +@pytest.mark.parametrize("config_key", [FODO_1GEV_6D_TANGO_PYAML_CONFIG_KEY]) +def deactivated_test_orbit_correction(config_key: str): + try: + accelerator = _build_accelerator(config_key) + control_mode = accelerator.live + bpms = control_mode.bpms.get("bpms") + orbit_response_matrix = control_mode.get_orm_tuning("DEFAULT_ORBIT_RESPONSE_MATRIX") + orbit_correction = control_mode.get_orbit_tuning("DEFAULT_ORBIT_CORRECTION") + orbit_response_matrix.measure() + ormdata = orbit_response_matrix.get() + orbit_response_matrix.save("orm.json") + orbit_correction.load("orm.json") + std_kick = 1e-6 + hcorr = control_mode.magnets.get("hcorrectors") + vcorr = control_mode.magnets.get("vcorrectors") + print(f"HCORR={hcorr.strengths.get()}") + print(f"VCORR={vcorr.strengths.get()}") + ref_h, ref_v = bpms.positions.get().T + reference = np.concat((ref_h, ref_v)) + # mangle orbit + hcorr.strengths.set(hcorr.strengths.get() + std_kick * np.random.normal(size=len(hcorr))) + vcorr.strengths.set(vcorr.strengths.get() + std_kick * np.random.normal(size=len(vcorr))) + positions_bc = bpms.positions.get() + std_bc = np.std(positions_bc, axis=0) + print(f"R.m.s. orbit before correction H: {1e6 * std_bc[0]: .1f} µm, V: {1e6 * std_bc[1]: .1f} µm.") + orbit_correction.correct(reference=reference) + finally: + import time + + from tango import DevFailed, DeviceProxy + + simulator = DeviceProxy("simulator/ringsimulator/ringsimulator") + try: + print("Reset the simulator") + simulator.Reinit() + print("Reset done") + except DevFailed: + time.sleep(3) + + +@pytest.mark.parametrize("config_key", [FODO_1GEV_6D_TANGO_PYAML_CONFIG_KEY]) +def deactivated_test_chromaticity_measurement(config_key: str): + # Deactivated like test_orbit_correction above: pyaml-test-lattice's current fixture + # (as of commit 9d753c73) does not yet define BPMs/correctors or tuning tools + # (chromaticity/orbit/tune response matrix), which this test requires. + try: + from pyaml.common.constants import Action + + accelerator = _build_accelerator(config_key) + control_mode = accelerator.live + chromaticity_measurement = control_mode.get_chromaticity_monitor("DEFAULT_CHROMATICITY_MEASUREMENT") + + def chroma_callback(action: int, cb_data: dict): + if action == Action.MEASURE: + print(f"Chromaticy measurement: #{cb_data['step']} RF={cb_data['rf']} Tune={cb_data['tune']}") + return True + + accelerator.design.get_lattice().disable_6d() + alphac = accelerator.design.get_lattice().get_mcf() + accelerator.design.get_lattice().enable_6d() + chromaticity_measurement.measure( + callback=chroma_callback, + do_plot=True, + alphac=alphac, + fit_order=2, + n_step=5, + sleep_between_meas=2.0, + sleep_between_step=2.0, + ) + finally: + import time + + from tango import DevFailed, DeviceProxy + + simulator = DeviceProxy("simulator/ringsimulator/ringsimulator") + try: + print("Reset the simulator") + simulator.Reset() + print("Reset done") + except DevFailed: + time.sleep(3) diff --git a/tests/lattice_info.py b/tests/lattice/lattice_info.py similarity index 100% rename from tests/lattice_info.py rename to tests/lattice/lattice_info.py diff --git a/tests/test_linkers.py b/tests/lattice/test_linkers.py similarity index 81% rename from tests/test_linkers.py rename to tests/lattice/test_linkers.py index 9e8734bb9..75585da74 100644 --- a/tests/test_linkers.py +++ b/tests/lattice/test_linkers.py @@ -2,9 +2,6 @@ from pyaml import PyAMLException from pyaml.accelerator import Accelerator -from pyaml.lattice.attribute_linker import ( - ConfigModel as AttrConfigModel, -) from pyaml.lattice.attribute_linker import ( PyAtAttributeElementsLinker, PyAtAttributeIdentifier, @@ -28,7 +25,7 @@ def get_name(self) -> str: def test_conf_with_linker(): sr: Accelerator = Accelerator.load("tests/config/sr-attribute-linker.yaml") assert sr is not None - magnet = sr.design.get_magnet("SH1A-C01-H") + magnet = sr.design.magnet.get("SH1A-C01-H") assert magnet is not None @@ -40,7 +37,7 @@ def test_conf_with_linker(): def test_attribute_identifier_from_pyaml_name(lattice_with_custom_attr): """We bind to AT element attribute 'Tag'; identifier value comes from PyAML element .name""" - linker = PyAtAttributeElementsLinker(AttrConfigModel(attribute_name="Tag")) + linker = PyAtAttributeElementsLinker(attribute_name="Tag") linker.set_lattice(lattice_with_custom_attr) pyaml_elem = DummyPyAMLElement(name="QF") # identifier="QF" ident = linker.get_element_identifier(pyaml_elem) @@ -50,7 +47,7 @@ def test_attribute_identifier_from_pyaml_name(lattice_with_custom_attr): def test_attribute_get_at_elements_all_matches(lattice_with_custom_attr): - linker = PyAtAttributeElementsLinker(AttrConfigModel(attribute_name="Tag")) + linker = PyAtAttributeElementsLinker(attribute_name="Tag") linker.set_lattice(lattice_with_custom_attr) ident = PyAtAttributeIdentifier("Tag", "QF") matches = linker.get_at_elements(ident) @@ -60,7 +57,7 @@ def test_attribute_get_at_elements_all_matches(lattice_with_custom_attr): def test_attribute_get_at_element_first_match(lattice_with_custom_attr): - linker = PyAtAttributeElementsLinker(AttrConfigModel(attribute_name="Tag")) + linker = PyAtAttributeElementsLinker(attribute_name="Tag") linker.set_lattice(lattice_with_custom_attr) ident = PyAtAttributeIdentifier("Tag", "QD") first = linker.get_at_element(ident) @@ -73,7 +70,7 @@ def test_attribute_get_at_element_first_match(lattice_with_custom_attr): def test_attribute_no_match_raises(lattice_with_custom_attr): - linker = PyAtAttributeElementsLinker(AttrConfigModel(attribute_name="Tag")) + linker = PyAtAttributeElementsLinker(attribute_name="Tag") linker.set_lattice(lattice_with_custom_attr) ident = PyAtAttributeIdentifier("Tag", "ZZ") with pytest.raises(PyAMLException): @@ -83,7 +80,7 @@ def test_attribute_no_match_raises(lattice_with_custom_attr): def test_attribute_multiple_identifiers_accumulate(lattice_with_custom_attr): - linker = PyAtAttributeElementsLinker(AttrConfigModel(attribute_name="Tag")) + linker = PyAtAttributeElementsLinker(attribute_name="Tag") linker.set_lattice(lattice_with_custom_attr) ids = [PyAtAttributeIdentifier("Tag", "QF"), PyAtAttributeIdentifier("Tag", "QD")] res = linker.get_at_elements(ids) @@ -101,7 +98,7 @@ def test_various_naming_addressing(): sr = Accelerator.load("tests/config/EBSNames.yaml", ignore_external=True) ring = sr.design.get_lattice() - elts = sr.design.get_magnet("QF1E").strength._RWStrengthScalar__elements + elts = sr.design.magnet.get("QF1E").strength._elements assert len(elts) == 31 check_index( ring, @@ -141,7 +138,7 @@ def test_various_naming_addressing(): ], ) - elts = sr.design.get_magnet("QF1E-ALL").strength._RWStrengthScalar__elements + elts = sr.design.magnet.get("QF1E-ALL").strength._elements assert len(elts) == 32 check_index( ring, @@ -182,18 +179,18 @@ def test_various_naming_addressing(): ], ) - elts = sr.design.get_magnet("QF1E-C05").strength._RWStrengthScalar__elements + elts = sr.design.magnet.get("QF1E-C05").strength._elements assert len(elts) == 1 check_index(ring, elts, [290]) - elts = sr.design.get_magnet("QF1E-C04-C05-C06").strength._RWStrengthScalar__elements + elts = sr.design.magnet.get("QF1E-C04-C05-C06").strength._elements assert len(elts) == 3 check_index(ring, elts, [140, 290, 424]) - elts = sr.design.get_magnet("QF1E-C04-C05-C06-2").strength._RWStrengthScalar__elements + elts = sr.design.magnet.get("QF1E-C04-C05-C06-2").strength._elements assert len(elts) == 3 check_index(ring, elts, [140, 290, 424]) - elts = sr.design.get_magnet("QF1E-C04-C05-C06-3").strength._RWStrengthScalar__elements + elts = sr.design.magnet.get("QF1E-C04-C05-C06-3").strength._elements assert len(elts) == 3 check_index(ring, elts, [140, 290, 424]) diff --git a/tests/test_curve.py b/tests/magnet/test_curve.py similarity index 66% rename from tests/test_curve.py rename to tests/magnet/test_curve.py index 39cf66932..cf8597d19 100644 --- a/tests/test_curve.py +++ b/tests/magnet/test_curve.py @@ -1,13 +1,12 @@ import numpy as np -from pyaml.configuration import set_root_folder -from pyaml.configuration.csvcurve import ConfigModel, CSVCurve -from pyaml.configuration.curve import Curve +from pyaml.configuration import ROOT +from pyaml.magnet.csvcurve import CSVCurve +from pyaml.magnet.curve import Curve def curve_test(file: str, current: float, strength: float): - curveConfig = ConfigModel(file=file) - curve = CSVCurve(curveConfig) + curve = CSVCurve(file=file) curveData = curve.get_curve() icurveData = Curve.inverse(curveData) x1 = np.interp(current, curveData[:, 0], curveData[:, 1]) @@ -17,6 +16,6 @@ def curve_test(file: str, current: float, strength: float): def test_curve(config_root_dir): - set_root_folder(config_root_dir) + ROOT.set(config_root_dir) curve_test("sr/magnet_models/QF1_strength.csv", 85, 16.618788) curve_test("sr/magnet_models/QD2_strength.csv", 87, -12.319894) diff --git a/tests/test_ident_models.py b/tests/magnet/test_ident_models.py similarity index 80% rename from tests/test_ident_models.py rename to tests/magnet/test_ident_models.py index 03582404d..7fa5f0d2e 100644 --- a/tests/test_ident_models.py +++ b/tests/magnet/test_ident_models.py @@ -20,14 +20,14 @@ def test_cfm_magnets(magnet_file, install_test_package): sr: Accelerator = Accelerator.load(magnet_file) sr.design.get_lattice().disable_6d() - # magnet_design = sr.design.get_magnet("SH1A-C01") - # magnet_live = sr.live.get_magnet("SH1A-C01") + # magnet_design = sr.design.magnet.get("SH1A-C01") + # magnet_live = sr.live.magnet.get("SH1A-C01") # assert isinstance(magnet_design, CombinedFunctionMagnet) # assert isinstance(magnet_live, CombinedFunctionMagnet) - magnet_h_design = sr.design.get_magnet("SH1A-C01-H") - magnet_v_design = sr.design.get_magnet("SH1A-C01-V") - magnet_h_live = sr.live.get_magnet("SH1A-C01-H") - magnet_v_live = sr.live.get_magnet("SH1A-C01-V") + magnet_h_design = sr.design.magnet.get("SH1A-C01-H") + magnet_v_design = sr.design.magnet.get("SH1A-C01-V") + magnet_h_live = sr.live.magnet.get("SH1A-C01-H") + magnet_v_live = sr.live.magnet.get("SH1A-C01-V") assert isinstance(magnet_h_design, HCorrector) assert isinstance(magnet_v_design, VCorrector) assert isinstance(magnet_h_live, HCorrector) diff --git a/tests/test_load_quad.py b/tests/magnet/test_load_quad.py similarity index 84% rename from tests/test_load_quad.py rename to tests/magnet/test_load_quad.py index ac64605eb..386382b49 100644 --- a/tests/test_load_quad.py +++ b/tests/magnet/test_load_quad.py @@ -4,9 +4,7 @@ import pytest from scipy.constants import speed_of_light -from pyaml import PyAMLException -from pyaml.accelerator import Accelerator -from pyaml.configuration import Factory, get_root_folder, set_root_folder +from pyaml.configuration import ROOT, Factory from pyaml.configuration.fileloader import load from pyaml.control.abstract_impl import ( RWHardwareArray, @@ -32,17 +30,18 @@ indirect=True, ) def test_quad_external_model(install_test_package, config_root_dir): - set_root_folder(config_root_dir) + ROOT.set(config_root_dir) cfg_hcorr_yaml = load("sr/custom_magnets/hidcorr.yaml") - cs = Factory.build_object( + cs = Factory.build( { "type": "tango.pyaml.controlsystem", "name": "live", "tango_host": "ebs-simu-3:10000", + "catalog": Factory.build(load("catalogs/sr_catalogs.yaml"), False), } ) - hcorr_with_external_model: HCorrector = Factory.depth_first_build(cfg_hcorr_yaml, False) - dev = cs.attach(hcorr_with_external_model.model.get_devices())[0] + hcorr_with_external_model: HCorrector = Factory.build(cfg_hcorr_yaml, False) + dev = cs.get_device_access(hcorr_with_external_model.model.get_device_names()[0]) strength = RWStrengthScalar(hcorr_with_external_model.model, dev) hardware = RWHardwareScalar(hcorr_with_external_model.model, dev) ref_corr = hcorr_with_external_model.attach(cs, strength, hardware) @@ -72,18 +71,19 @@ def test_quad_external_model(install_test_package, config_root_dir): indirect=["install_test_package"], ) def test_quad_linear(magnet_file, install_test_package, config_root_dir): - set_root_folder(config_root_dir) + ROOT.set(config_root_dir) cfg_quad = load(magnet_file) print(f"Current file: {config_root_dir}/{magnet_file}") - cs = Factory.build_object( + cs = Factory.build( { "type": "tango.pyaml.controlsystem", "name": "live", "tango_host": "ebs-simu-3:10000", + "catalog": Factory.build(load("catalogs/sr_catalogs.yaml"), False), } ) - quad: Quadrupole = Factory.depth_first_build(cfg_quad, False) - dev = cs.attach(quad.model.get_devices())[0] + quad: Quadrupole = Factory.build(cfg_quad, False) + dev = cs.get_device_access(quad.model.get_device_names()[0]) hardware = RWHardwareScalar(quad.model, dev) if quad.model.has_hardware() else None strength = RWStrengthScalar(quad.model, dev) if quad.model.has_physics() else None ref_quad = quad.attach(cs, strength, hardware) @@ -121,18 +121,19 @@ def test_quad_linear(magnet_file, install_test_package, config_root_dir): ], ) def test_combined_function_magnets(magnet_file, config_root_dir): - set_root_folder(config_root_dir) + ROOT.set(config_root_dir) cfg_sh = load(magnet_file) - cs = Factory.build_object( + cs = Factory.build( { "type": "tango.pyaml.controlsystem", "name": "live", "tango_host": "ebs-simu-3:10000", + "catalog": Factory.build(load("catalogs/sr_catalogs.yaml"), False), } ) - sh: CombinedFunctionMagnet = Factory.depth_first_build(cfg_sh, False) + sh: CombinedFunctionMagnet = Factory.build(cfg_sh, False) sh.model.set_magnet_rigidity(6e9 / speed_of_light) - devs = cs.attach(sh.model.get_devices()) + devs = cs.get_devices_access(sh.model.get_device_names()) currents = RWHardwareArray(sh.model, devs) strengths = RWStrengthArray(sh.model, devs) sUnits = sh.model.get_strength_units() diff --git a/tests/test_ranges_cfm_deviceaccess.py b/tests/magnet/test_ranges_cfm_deviceaccess.py similarity index 92% rename from tests/test_ranges_cfm_deviceaccess.py rename to tests/magnet/test_ranges_cfm_deviceaccess.py index d8e09faca..6316cc940 100644 --- a/tests/test_ranges_cfm_deviceaccess.py +++ b/tests/magnet/test_ranges_cfm_deviceaccess.py @@ -38,10 +38,10 @@ def test_cfm_ranges_from_yaml_are_propagated_and_enforced(magnet_file, install_t sr.design.get_lattice().disable_6d() # Parent CFM magnet (the one defined in SH1AC01-range.yaml) - m = sr.live.get_cfm_magnet("SH1A-C01") + m = sr.live.combined_function_magnet.get("SH1A-C01") - devs = m.model.get_devices() - assert len(devs) == 3 + dev_names = m.model.get_device_names() + assert len(dev_names) == 3 # Exact ranges coming from the YAML configuration file (powerconverters[*].range) expected_ranges = [ @@ -50,6 +50,8 @@ def test_cfm_ranges_from_yaml_are_propagated_and_enforced(magnet_file, install_t [-1.5, None], ] + devs = sr.live.get_devices_access(dev_names) + got_ranges = [d.get_range() for d in devs] assert got_ranges == expected_ranges diff --git a/tests/test_serialized_magnets.py b/tests/magnet/test_serialized_magnets.py similarity index 86% rename from tests/test_serialized_magnets.py rename to tests/magnet/test_serialized_magnets.py index 20506f79e..1e95ca706 100644 --- a/tests/test_serialized_magnets.py +++ b/tests/magnet/test_serialized_magnets.py @@ -24,7 +24,7 @@ def check_no_diff(array: list[np.float64]) -> bool: ], ) def test_config_load(sr_file): - sr: Accelerator = Accelerator.load(sr_file, use_fast_loader=True, ignore_external=True) + sr: Accelerator = Accelerator.load(sr_file, include_locations=False, ignore_external=True) assert sr is not None magnets = [ sr.design.get_element("QF8B-C04"), @@ -55,11 +55,11 @@ def test_config_load(sr_file): ], ) def test_magnet_modification(sr_file): - sr = Accelerator.load(sr_file, use_fast_loader=True, ignore_external=True) + sr = Accelerator.load(sr_file, include_locations=False, ignore_external=True) print(sr.yellow_pages) - sm: SerializedMagnets = sr.design.get_serialized_magnet("mySeriesOfMagnets") + sm: SerializedMagnets = sr.design.serialized_magnet.get("mySeriesOfMagnets") element_names = sm._SerializedMagnets__elements lattice = sr.design.get_lattice() @@ -107,14 +107,14 @@ def test_magnet_modification(sr_file): ], ) def test_tune(sr_file): - sr = Accelerator.load(sr_file, use_fast_loader=True, ignore_external=True) + sr = Accelerator.load(sr_file, include_locations=False, ignore_external=True) sr.design.get_lattice().disable_6d() - m = sr.design.get_serialized_magnet("QF1A") + m = sr.design.serialized_magnet.get("QF1A") print(f"m.strength.get()={m.strength.get()}") assert len(m.get_magnets()) == m.get_nb_magnets() - quadForTuneDesign = sr.design.get_serialized_magnets("QForTune") + quadForTuneDesign = sr.design.serialized_magnets.get("QForTune") tune_monitor = sr.design.get_betatron_tune_monitor("BETATRON_TUNE") # Build tune response matrix tunemat = np.zeros((len(quadForTuneDesign), 2)) @@ -160,14 +160,14 @@ def test_tune(sr_file): "tests/config/sr_serialized_magnets.yaml", ], ) -def test_get_devices(sr_file): - sr: Accelerator = Accelerator.load(sr_file, use_fast_loader=True, ignore_external=True) - sm: SerializedMagnets = sr.design.get_serialized_magnet("QF1A") +def test_get_device_names(sr_file): + sr: Accelerator = Accelerator.load(sr_file, include_locations=False, ignore_external=True) + sm: SerializedMagnets = sr.design.serialized_magnet.get("QF1A") - devices = sm.get_devices() + device_names = sm.get_device_names() # Serialized magnets share a single power converter: exactly 1 device - assert len(devices) == 1 + assert len(device_names) == 1 # Strength and hardware computation must remain consistent after the fix initial_strength = sm.strength.get() sm.strength.set(initial_strength * 1.01) @@ -191,8 +191,8 @@ def get_strengths_from_lattice(sr: Accelerator, sm: SerializedMagnets) -> list: ], ) def test_strength_computation(sr_file): - sr: Accelerator = Accelerator.load(sr_file, use_fast_loader=True, ignore_external=True) - sm: SerializedMagnets = sr.design.get_serialized_magnet("QF1A") + sr: Accelerator = Accelerator.load(sr_file, include_locations=False, ignore_external=True) + sm: SerializedMagnets = sr.design.serialized_magnet.get("QF1A") assert sm.get_nb_magnets() == 31 sm.strength.set(24.0) assert abs(sm.strength.get() - 24.0) < 1e-3 diff --git a/tests/test_rf.py b/tests/rf/test_rf.py similarity index 70% rename from tests/test_rf.py rename to tests/rf/test_rf.py index 5752d4d07..1d8b5a570 100644 --- a/tests/test_rf.py +++ b/tests/rf/test_rf.py @@ -7,9 +7,8 @@ def test_rf(): sr: Accelerator = Accelerator.load("tests/config/EBS_rf.yaml", ignore_external=True) - RF = sr.design.get_rf_plant("RF") - RF.frequency.set(3.523e8) + sr.design.rf.frequency.set(3.523e8) # Check that frequency has been applied on all cavities ring = sr.design.get_lattice() @@ -17,7 +16,7 @@ def test_rf(): if e.FamName.startswith("CAV"): assert e.Frequency == 3.523e8 - RF.voltage.set(10.0e6) + sr.design.rf.voltage.set(10.0e6) # Check that voltage has been applied on all cavities ring = sr.design.get_lattice() @@ -26,11 +25,10 @@ def test_rf(): assert np.isclose(e.Voltage, 10.0e6 / 13.0) if False: - RF = sr.live.get_rf_plant("RF") - RF.frequency.set(3.523721693993786e8) - RF.voltage.set(6.5e6) - assert np.isclose(RF.frequency.get(), 3.523721693993786e8) - assert np.isclose(RF.voltage.get(), 6.5e6) + sr.live.rf.frequency.set(3.523721693993786e8) + sr.live.rf.voltage.set(6.5e6) + assert np.isclose(sr.live.rf.frequency.get(), 3.523721693993786e8) + assert np.isclose(sr.live.rf.voltage.get(), 6.5e6) @pytest.mark.parametrize( @@ -42,9 +40,8 @@ def test_rf_multi(install_test_package): sr: Accelerator = Accelerator.load("tests/config/EBS_rf_multi.yaml") # Simulator - RF = sr.design.get_rf_plant("RF") - RF.frequency.set(3.523e8) + sr.design.rf.frequency.set(3.523e8) # Check that frequency has been applied on all cavities ring = sr.design.get_lattice() @@ -56,9 +53,9 @@ def test_rf_multi(install_test_package): else: assert e.Frequency == 3.523e8 - RFTRA_HARMONIC = sr.design.get_rf_trasnmitter("RFTRA_HARMONIC") + RFTRA_HARMONIC = sr.design.rf.transmitter.get("RFTRA_HARMONIC") RFTRA_HARMONIC.voltage.set(300e3) - RF.voltage.set(12e6) + sr.design.rf.voltage.set(12e6) for e in ring: if e.FamName.startswith("CAV"): @@ -69,14 +66,13 @@ def test_rf_multi(install_test_package): assert np.isclose(e.Voltage, 1e6) # Control system - RF = sr.live.get_rf_plant("RF") - RF1 = sr.live.get_rf_trasnmitter("RFTRA1") - RF2 = sr.live.get_rf_trasnmitter("RFTRA2") - RFTRA_HARMONIC = sr.live.get_rf_trasnmitter("RFTRA_HARMONIC") + RF1 = sr.live.rf.transmitter.get("RFTRA1") + RF2 = sr.live.rf.transmitter.get("RFTRA2") + RFTRA_HARMONIC = sr.live.rf.transmitter.get("RFTRA_HARMONIC") - RF.frequency.set(3.523e8) + sr.live.rf.frequency.set(3.523e8) RFTRA_HARMONIC.voltage.set(300e3) - RF.voltage.set(12e6) + sr.live.rf.voltage.set(12e6) assert np.isclose(RF1.voltage.get(), 10e6) assert np.isclose(RF2.voltage.get(), 2e6) @@ -92,9 +88,8 @@ def test_rf_multi_notrans(install_test_package): sr: Accelerator = Accelerator.load("tests/config/EBS_rf_notrans.yaml") # Simulator - RF = sr.design.get_rf_plant("RF") - RF.frequency.set(3.523e8) - RF.voltage.set(10e6) + sr.design.rf.frequency.set(3.523e8) + sr.design.rf.voltage.set(10e6) # Check that frequency and voltage has been applied on all cavities ring = sr.design.get_lattice() for e in ring: @@ -103,11 +98,10 @@ def test_rf_multi_notrans(install_test_package): assert np.isclose(e.Voltage, 10e6 / 13.0) # Control system - RF = sr.live.get_rf_plant("RF") - RF.frequency.set(3.523e8) + sr.live.rf.frequency.set(3.523e8) with pytest.raises(PyAMLException) as exc: - RF.voltage.set(10e6) - assert "has no trasmitter device defined" in str(exc) + sr.live.rf.voltage.set(10e6) + assert "has no transmitter device defined" in str(exc) # Check that frequency and voltage has been applied on the masterclock device - assert np.isclose(RF.frequency.get(), 3.523e8) + assert np.isclose(sr.live.rf.frequency.get(), 3.523e8) diff --git a/tests/test_accelerator_load.py b/tests/test_accelerator_load.py index 326f0a337..f30a68e39 100644 --- a/tests/test_accelerator_load.py +++ b/tests/test_accelerator_load.py @@ -1,7 +1,7 @@ import pytest from pydantic import BaseModel, ConfigDict -from pyaml import PyAMLConfigException +from pyaml import PyAMLConfigException, set_repr_options from pyaml.accelerator import Accelerator, ElementHolder from pyaml.common.element import Element, ElementConfigModel, __pyaml_repr__ from pyaml.control.controlsystem import ControlSystemAdapter @@ -17,6 +17,45 @@ def test_peer(): assert isinstance(tm.peer, ElementHolder) +def test_repr_is_informative_and_bounded(): + sr = Accelerator.load("tests/config/EBSOrbit.yaml") + bpm = sr.design.bpm.get("BPM_C04-04") + bpms = sr.design.bpms.get("BPM") + + assert repr(bpm) == ( + "BPM(name='BPM_C04-04', lattice_names='BPM_C04-04', " + + "peer=Simulator:design, x_pos='srdiag/bpm/c04-04/SA_HPosition', " + + "y_pos='srdiag/bpm/c04-04/SA_VPosition', " + + "x_offset='srdiag/bpm/c04-04/HOffset', " + + "y_offset='srdiag/bpm/c04-04/VOffset', " + + "tilt_name=None)" + ) + + assert repr(sr.design) == ( + f"Simulator(name='design', lattice={sr.design.lattice!r}, mat_key=None, n_elements={len(sr.design.ring)})" + ) + assert repr(sr) == "Accelerator(facility='ESRF', machine='sr', simulators=['design'], controls=['live'])" + assert len(repr(bpms)) < 250 + assert f"size={len(bpms)}" in repr(bpms) + assert f"... +{len(bpms) - 3} more ..." in repr(bpms) + + +def test_repr_options_limit_sequences(): + original = set_repr_options() + try: + set_repr_options(max_items=1) + sr = Accelerator.load("tests/config/EBSOrbit.yaml") + + bpms = sr.design.bpms.get("BPM") + assert f"... +{len(bpms) - 1} more ..." in repr(bpms) + finally: + set_repr_options( + max_items=original.max_items, + max_depth=original.max_depth, + max_length=original.max_length, + ) + + def test_accelerator_load_rejects_non_accelerator_root(tmp_path): config_file = tmp_path / "quadrupole.yaml" config_file.write_text("type: pyaml.magnet.quadrupole\nname: QF1A-C01\n", encoding="utf-8") diff --git a/tests/test_catalogs.py b/tests/test_catalogs.py new file mode 100644 index 000000000..828627aa5 --- /dev/null +++ b/tests/test_catalogs.py @@ -0,0 +1,190 @@ +import numpy as np +import pytest + +from pyaml import PyAMLConfigException +from pyaml.accelerator import Accelerator + + +@pytest.mark.parametrize( + "install_test_package", + [{"name": "tango-pyaml", "path": "tests/dummy_cs/tango-pyaml"}], + indirect=True, +) +def test_inline_catalog_is_supported(install_test_package): + sr = Accelerator.from_dict( + { + "type": "pyaml.accelerator", + "facility": "ESRF", + "machine": "sr", + "energy": 6e9, + "data_folder": "/data/store", + "controls": [ + { + "type": "tango.pyaml.controlsystem", + "tango_host": "ebs-simu-3:10000", + "name": "live", + "catalog": { + "type": "tango.pyaml.static_catalog", + "entries": [ + { + "type": "tango.pyaml.static_catalog_entry", + "key": "BPM_C02-01/x", + "device": { + "type": "tango.pyaml.attribute_read_only", + "attribute": "srdiag/bpm/c02-01/SA_HPosition", + "unit": "mm", + }, + }, + { + "type": "tango.pyaml.static_catalog_entry", + "key": "BPM_C02-01/y", + "device": { + "type": "tango.pyaml.attribute_read_only", + "attribute": "srdiag/bpm/c02-01/SA_VPosition", + "unit": "mm", + }, + }, + ], + }, + } + ], + "devices": [ + { + "type": "pyaml.bpm.bpm", + "name": "BPM_C02-01", + "x_pos": "BPM_C02-01/x", + "y_pos": "BPM_C02-01/y", + } + ], + } + ) + + bpm = sr.live.bpm.get("BPM_C02-01") + assert np.allclose(bpm.positions.get(), np.array([0.0, 0.0])) + + +@pytest.mark.parametrize( + "install_test_package", + [{"name": "tango-pyaml", "path": "tests/dummy_cs/tango-pyaml"}], + indirect=True, +) +def test_unresolved_catalog_key_raises_runtime_error(install_test_package): + with pytest.raises( + PyAMLConfigException, + match="Catalog cannot resolve key 'BPM_C03-01/y'", + ): + Accelerator.from_dict( + { + "type": "pyaml.accelerator", + "facility": "ESRF", + "machine": "sr", + "energy": 6e9, + "data_folder": "/data/store", + "controls": [ + { + "type": "tango.pyaml.controlsystem", + "tango_host": "ebs-simu-3:10000", + "name": "live", + "catalog": { + "type": "tango.pyaml.static_catalog", + "entries": [ + { + "type": "tango.pyaml.static_catalog_entry", + "key": "BPM_C03-01/x", + "device": { + "type": "tango.pyaml.attribute_read_only", + "attribute": "srdiag/bpm/c03-01/SA_HPosition", + "unit": "mm", + }, + } + ], + }, + } + ], + "devices": [ + { + "type": "pyaml.bpm.bpm", + "name": "BPM_C03-01", + "x_pos": "BPM_C03-01/x", + "y_pos": "BPM_C03-01/y", + } + ], + } + ) + + +def test_duplicate_static_catalog_entry_keys_raise_config_error(): + with pytest.raises(PyAMLConfigException, match="duplicate key 'duplicated/key'"): + Accelerator.load("tests/config/bad_catalog_duplicate_key.yaml") + + +@pytest.mark.parametrize( + "install_test_package", + [{"name": "tango-pyaml", "path": "tests/dummy_cs/tango-pyaml"}], + indirect=True, +) +def test_indexed_catalog_entry_extracts_scalar_from_vector_attribute(install_test_package): + """ + Verify that a catalog can map two keys to different indices of the same + vector attribute. The BPM sees two independent scalar DeviceAccess objects + (one per axis) even though the hardware exposes a single position vector. + The indexing is fully transparent to pyAML — it happens in the CS backend. + """ + from tango.pyaml.attribute_store import set_attribute + + set_attribute("srdiag/bpm/c01-04/Position", [1.5, -0.3], unit="mm") + + sr = Accelerator.from_dict( + { + "type": "pyaml.accelerator", + "facility": "ESRF", + "machine": "sr", + "energy": 6e9, + "data_folder": "/data/store", + "controls": [ + { + "type": "tango.pyaml.controlsystem", + "tango_host": "ebs-simu-3:10000", + "name": "live", + "catalog": { + "type": "tango.pyaml.static_catalog", + "entries": [ + { + "type": "tango.pyaml.static_catalog_entry", + "key": "bpm/SA_HPosition", + "device": { + "type": "tango.pyaml.attribute", + "attribute": "srdiag/bpm/c01-04/Position", + "index": 0, + "unit": "mm", + }, + }, + { + "type": "tango.pyaml.static_catalog_entry", + "key": "bpm/SA_VPosition", + "device": { + "type": "tango.pyaml.attribute", + "attribute": "srdiag/bpm/c01-04/Position", + "index": 1, + "unit": "mm", + }, + }, + ], + }, + } + ], + "devices": [ + { + "type": "pyaml.bpm.bpm", + "name": "BPM_TEST", + "x_pos": "bpm/SA_HPosition", + "y_pos": "bpm/SA_VPosition", + } + ], + } + ) + + bpm = sr.live.bpm.get("BPM_TEST") + positions = bpm.positions.get() + assert np.isclose(positions[0], 1.5) + assert np.isclose(positions[1], -0.3) diff --git a/tests/test_factory.py b/tests/test_factory.py deleted file mode 100644 index e60afad55..000000000 --- a/tests/test_factory.py +++ /dev/null @@ -1,53 +0,0 @@ -import pytest - -from pyaml import PyAMLConfigException, PyAMLException -from pyaml.accelerator import Accelerator -from pyaml.configuration import get_root_folder, set_root_folder -from pyaml.configuration.factory import Factory -from pyaml.configuration.fileloader import load -from tests.conftest import MockElement - - -def test_factory_build_default(): - """Test default PyAML module loading.""" - data = {"type": "mock_module", "name": "simple"} - obj = Factory.depth_first_build(data, False) - assert isinstance(obj, MockElement) - assert obj.name == "simple" - - -@pytest.mark.parametrize( - "test_file", - [ - "tests/config/bad_conf.yml", - ], -) -def test_error_location(test_file): - previous_root = get_root_folder() - try: - with pytest.raises(PyAMLConfigException) as exc: - set_root_folder("tests/config") - cfg = load("bad_conf.yml") - Factory.depth_first_build(cfg, False) - finally: - set_root_folder(previous_root) - print(str(exc.value)) - test_file_names = test_file.split("/") - test_file_name = test_file_names[len(test_file_names) - 1] - assert f"{test_file_name} at line 6, column 5" in str(exc.value) - - -@pytest.mark.parametrize( - "test_file", - [ - "tests/config/bad_conf_cycles.yml", - "tests/config/bad_conf_cycles.json", - ], -) -def test_error_cycles(test_file): - with pytest.raises(PyAMLException) as exc: - ml: Accelerator = Accelerator.load(test_file) - - assert "Circular file inclusion of " in str(exc.value) - if not test_file.endswith(".json"): - assert "at line 22" in str(exc.value) diff --git a/tests/test_load_conf_with_code.py b/tests/test_load_conf_with_code.py index ceb4747d0..de4761023 100644 --- a/tests/test_load_conf_with_code.py +++ b/tests/test_load_conf_with_code.py @@ -8,6 +8,11 @@ def test_load_conf_with_code(): config_path = parent_folder.joinpath("config", "EBSOrbit.yaml").resolve() sr: Accelerator = Accelerator.load(config_path) - bpms = sr.live.get_bpms("BPM") + bpms = sr.live.bpms.get("BPM") assert bpms is not None assert len(bpms) == 320 + + assert sr.live[bpms[0].get_name()] is bpms[0] + assert sr.live["BPM*"].names() == bpms.names() + assert sr.live[:].names() == [element.get_name() for element in sr.live.get_all_elements()] + assert sr.design["BPM*"].names() == sr.design.bpms.get("BPM").names() diff --git a/tests/test_yellow_pages_basic.py b/tests/test_yellow_pages_basic.py index c3e84057d..80413e6f3 100644 --- a/tests/test_yellow_pages_basic.py +++ b/tests/test_yellow_pages_basic.py @@ -17,10 +17,15 @@ VCorr (pyaml.arrays.magnet_array) size=288 Skews (pyaml.arrays.magnet_array) size=288 Sext (pyaml.arrays.magnet_array) size=180 + QForTune (pyaml.arrays.magnet_array) size=124 . Tools: - CHROMATICITY_MONITOR (pyaml.diagnostics.chromaticity_monitor) + BBA-BPM_C04-04 (pyaml.tuning_tools.bba) + BBA2-BPM_C04-04 (pyaml.tuning_tools.bba2) + CHROMATICITY_MONITOR (pyaml.tuning_tools.chromaticity_monitor) + DEFAULT_TUNE_CORRECTION (pyaml.tuning_tools.tune) + DEFAULT_TUNE_RESPONSE_MATRIX (pyaml.tuning_tools.tune_response_matrix) DEFAULT_CHROMATICITY_RESPONSE_MATRIX (pyaml.tuning_tools.chromaticity_response_matrix) DEFAULT_CHROMATICITY_CORRECTION (pyaml.tuning_tools.chromaticity) DEFAULT_ORBIT_CORRECTION (pyaml.tuning_tools.orbit) diff --git a/tests/tuning_tools/test_bba.py b/tests/tuning_tools/test_bba.py new file mode 100644 index 000000000..330c8118f --- /dev/null +++ b/tests/tuning_tools/test_bba.py @@ -0,0 +1,27 @@ +import numpy as np +import pytest + +from pyaml.accelerator import Accelerator + + +def test_bba(): + sr = Accelerator.load("tests/config/EBSOrbit.yaml") + SR = sr.design + + # Add a misalignement + SR.bpm.get("BPM_C04-04").offset.set([20e-6, -15e-6]) + + # BBA (standard bow tie, model independant) + bba = SR.get_bba("BBA-BPM_C04-04") + bba.measure() + assert np.abs(bba.h_offset() - 20e-6) < 1e-6 + assert np.abs(bba.v_offset() + 15e-6) < 1e-6 + + # BBA (model dependant method) + bba = SR.get_bba("BBA2-BPM_C04-04") + bba.minicycle_sleep_time = 0 + bba.measure() + assert np.abs(bba.h_offset() - 20e-6) < 1e-6 + assert np.abs(bba.v_offset() + 15e-6) < 1e-6 + assert np.abs(bba.h_offset_error() - 3.425616879733572e-07) < 1e-10 + assert np.abs(bba.v_offset_error() - 2.593196843945284e-07) < 1e-10 diff --git a/tests/test_chromaticity_monitor.py b/tests/tuning_tools/test_chromaticity_monitor.py similarity index 91% rename from tests/test_chromaticity_monitor.py rename to tests/tuning_tools/test_chromaticity_monitor.py index 5f296ea9e..d9b816b6f 100644 --- a/tests/test_chromaticity_monitor.py +++ b/tests/tuning_tools/test_chromaticity_monitor.py @@ -10,7 +10,7 @@ def callback(action: int, data: dict): def test_simulator_chromaticity_monitor(): - sr: Accelerator = Accelerator.load("tests/config/EBS_chromaticity.yaml", ignore_external=True) + sr: Accelerator = Accelerator.load("tests/config/EBSOrbit.yaml", ignore_external=True) sr.design.get_lattice().enable_6d() chromaAT = sr.design.get_lattice().get_chrom()[:-1] chromaticity_monitor = sr.design.get_chromaticity_monitor("CHROMATICITY_MONITOR") @@ -40,7 +40,7 @@ def test_simulator_chromaticity_monitor(): indirect=True, ) def test_controlsystem_chromaticity_monitor(install_test_package): - sr: Accelerator = Accelerator.load("tests/config/EBS_chromaticity.yaml") + sr: Accelerator = Accelerator.load("tests/config/EBSOrbit.yaml") chromaticity_monitor = sr.live.get_chromaticity_monitor("CHROMATICITY_MONITOR") assert chromaticity_monitor.chromaticity.get() is None chromaticity_monitor.measure( diff --git a/tests/test_tune.py b/tests/tuning_tools/test_tune.py similarity index 88% rename from tests/test_tune.py rename to tests/tuning_tools/test_tune.py index 0ff9f2ac0..a114230cf 100644 --- a/tests/test_tune.py +++ b/tests/tuning_tools/test_tune.py @@ -5,15 +5,15 @@ def test_tune(): - sr: Accelerator = Accelerator.load("tests/config/EBSTune.yaml", ignore_external=True) + sr: Accelerator = Accelerator.load("tests/config/EBSTune.yaml", ignore_external=False) assert sr.get_description() == "Accelerator configuration for EBS storage ring" - assert sr.design.get_magnet("QF1E-C04").get_description() == "QF1E-C04 quadrupole" + assert sr.design.magnet.get("QF1E-C04").get_description() == "QF1E-C04 quadrupole" assert sr.design.get_description() == "EBS lattice" sr.design.get_lattice().disable_6d() - quadForTuneDesign = sr.design.get_magnets("QForTune") + quadForTuneDesign = sr.design.magnets.get("QForTune") tune_monitor = sr.design.get_betatron_tune_monitor("BETATRON_TUNE") # Build tune response matrix tune = tune_monitor.tune.get() @@ -47,7 +47,7 @@ def test_tune(): if False: # Correct the tune on live (need a Virutal Accelerator) - quadForTuneLive = sr.live.get_magnets("QForTune") + quadForTuneLive = sr.live.magnets.get("QForTune") strs = quadForTuneLive.strengths.get() strs += np.matmul(correctionmat, [0.1, 0.05]) # Ask for correction [dqx,dqy] quadForTuneLive.strengths.set(strs) diff --git a/tests/test_tune_hardware.py b/tests/tuning_tools/test_tune_hardware.py similarity index 95% rename from tests/test_tune_hardware.py rename to tests/tuning_tools/test_tune_hardware.py index 638bc8397..8e83197df 100644 --- a/tests/test_tune_hardware.py +++ b/tests/tuning_tools/test_tune_hardware.py @@ -8,7 +8,7 @@ def test_tune(): sr: Accelerator = Accelerator.load("tests/config/EBSTune.yaml", ignore_external=True) sr.design.get_lattice().disable_6d() - quadForTuneDesign = sr.design.get_magnets("QForTune") + quadForTuneDesign = sr.design.magnets.get("QForTune") # Build tune response matrix (hardware units) diff --git a/tests/test_tune_monitor.py b/tests/tuning_tools/test_tune_monitor.py similarity index 100% rename from tests/test_tune_monitor.py rename to tests/tuning_tools/test_tune_monitor.py diff --git a/tests/test_tuning_dispersion.py b/tests/tuning_tools/test_tuning_dispersion.py similarity index 81% rename from tests/test_tuning_dispersion.py rename to tests/tuning_tools/test_tuning_dispersion.py index b96b414b2..16d2cd397 100644 --- a/tests/test_tuning_dispersion.py +++ b/tests/tuning_tools/test_tuning_dispersion.py @@ -8,7 +8,7 @@ def test_tuning_orm(): logging.getLogger("pyaml.tuning_tools").setLevel(logging.WARNING) parent_folder = Path(__file__).parent - config_path = parent_folder.joinpath("config", "EBSOrbit.yaml").resolve() + config_path = parent_folder.joinpath("..", "config", "EBSOrbit.yaml").resolve() sr = Accelerator.load(config_path) element_holder = sr.design @@ -17,7 +17,7 @@ def test_tuning_orm(): dispersion.measure() dispersion_data = dispersion.get() - bpms = element_holder.get_bpms("BPM") + bpms = element_holder.bpms.get("BPM") assert len(dispersion_data["frequency_response_x"]) == len(bpms) assert len(dispersion_data["frequency_response_y"]) == len(bpms) diff --git a/tests/test_tuning_orbit_correction.py b/tests/tuning_tools/test_tuning_orbit_correction.py similarity index 92% rename from tests/test_tuning_orbit_correction.py rename to tests/tuning_tools/test_tuning_orbit_correction.py index 447bea50c..d2648c7a4 100644 --- a/tests/test_tuning_orbit_correction.py +++ b/tests/tuning_tools/test_tuning_orbit_correction.py @@ -12,16 +12,16 @@ def test_tuning_orbit_correction(): logging.getLogger("pyaml.tuning_tools").setLevel(logging.WARNING) parent_folder = Path(__file__).parent - config_path = parent_folder.joinpath("config", "EBSOrbit.yaml").resolve() + config_path = parent_folder.joinpath("..", "config", "EBSOrbit.yaml").resolve() sr = Accelerator.load(config_path) element_holder = sr.design ## generate some orbit np.random.seed(42) std_kick = 1e-6 - hcorr = element_holder.get_magnets("HCorr") - vcorr = element_holder.get_magnets("VCorr") - bpms = element_holder.get_bpms("BPM") + hcorr = element_holder.magnets.get("HCorr") + vcorr = element_holder.magnets.get("VCorr") + bpms = element_holder.bpms.get("BPM") x, y = bpms.positions.get().T # get reference orbit reference = np.concat((x, y)) @@ -183,9 +183,8 @@ def test_tuning_orbit_correction(): x, y = bpms.positions.get().T # get reference orbit reference_before_rf = np.concat((x, y)) - plant = element_holder.get_rf_plant("RF") - frf = plant.frequency.get() - plant.frequency.set(frf + 100) + frf = element_holder.rf.frequency.get() + element_holder.rf.frequency.set(frf + 100) for _ in range(3): element_holder.orbit.correct( reference=reference_before_rf, @@ -195,7 +194,7 @@ def test_tuning_orbit_correction(): gain_H=0, ) - frf_after = plant.frequency.get() + frf_after = element_holder.rf.frequency.get() assert np.isclose(frf, frf_after, rtol=0, atol=1e-16) # no need to mangle orbit again, test rf @@ -204,9 +203,8 @@ def test_tuning_orbit_correction(): rf_weight = element_holder.orbit.get_rf_weight() element_holder.orbit.set_rf_weight(1.1 * rf_weight) - plant = element_holder.get_rf_plant("RF") - frf = plant.frequency.get() - plant.frequency.set(frf + 100) + frf = element_holder.rf.frequency.get() + element_holder.rf.frequency.set(frf + 100) for _ in range(8): element_holder.orbit.correct( reference=reference_before_rf, @@ -216,7 +214,7 @@ def test_tuning_orbit_correction(): gain_H=0, ) - frf_after = plant.frequency.get() + frf_after = element_holder.rf.frequency.get() assert np.isclose(frf, frf_after, rtol=0, atol=1e-16) element_holder.orbit.set_rf_weight(rf_weight) @@ -237,7 +235,7 @@ def test_tuning_orbit_correction_config(): "singular_values": "162", "response_matrix": "file:does_not_exist.json", } - orbit_cor = Factory.depth_first_build(config_dict, ignore_external=False) + orbit_cor = Factory.build(config_dict, ignore_external=False) Factory.clear() config_dict = { @@ -250,7 +248,7 @@ def test_tuning_orbit_correction_config(): "response_matrix": "file:does_not_exist.json", } try: - orbit_cor = Factory.depth_first_build(config_dict, ignore_external=False) + orbit_cor = Factory.build(config_dict, ignore_external=False) except PyAMLConfigException as exc: # failed successfully! Factory.clear() @@ -265,5 +263,5 @@ def test_tuning_orbit_correction_config(): "singular_values_V": "162", "response_matrix": "file:does_not_exist.json", } - orbit_cor = Factory.depth_first_build(config_dict, ignore_external=False) + orbit_cor = Factory.build(config_dict, ignore_external=False) Factory.clear() diff --git a/tests/test_tuning_orm.py b/tests/tuning_tools/test_tuning_orm.py similarity index 52% rename from tests/test_tuning_orm.py rename to tests/tuning_tools/test_tuning_orm.py index 4eac3428f..553bce161 100644 --- a/tests/test_tuning_orm.py +++ b/tests/tuning_tools/test_tuning_orm.py @@ -1,4 +1,5 @@ import logging +import tempfile from pathlib import Path import numpy as np @@ -10,17 +11,24 @@ def test_tuning_orm(): logging.getLogger("pyaml.tuning_tools").setLevel(logging.WARNING) parent_folder = Path(__file__).parent - config_path = parent_folder.joinpath("config", "EBSOrbit.yaml").resolve() + config_path = parent_folder.joinpath("..", "config", "EBSOrbit.yaml").resolve() sr = Accelerator.load(config_path) element_holder = sr.design orm = element_holder.orm - bpms = element_holder.get_bpms("BPM") - hcorr_names = element_holder.get_magnets("HCorr").names()[:4] - vcorr_names = element_holder.get_magnets("VCorr").names()[:4] + bpms = element_holder.bpms.get("BPM") + hcorr_names = element_holder.magnets.get("HCorr").names()[:4] + vcorr_names = element_holder.magnets.get("VCorr").names()[:4] orm.measure(corrector_names=hcorr_names + vcorr_names) orm_data = orm.get() orm_shape = np.array(orm_data["matrix"]).shape assert orm_shape == (2 * len(bpms), 8) + + with tempfile.NamedTemporaryFile(mode="w", suffix=".json", prefix="orm_") as f: + # save file + orm.save(save_path=f.name) + + # load saved file + element_holder.orbit.load(f.name) diff --git a/tests/test_tuning_tools.py b/tests/tuning_tools/test_tuning_tools.py similarity index 88% rename from tests/test_tuning_tools.py rename to tests/tuning_tools/test_tuning_tools.py index 72fdc5d3b..5c748b003 100644 --- a/tests/test_tuning_tools.py +++ b/tests/tuning_tools/test_tuning_tools.py @@ -10,7 +10,7 @@ def callback(action: Action, data: dict): def test_tune_tool(): - sr = Accelerator.load("tests/config/EBSTune.yaml", use_fast_loader=True) + sr = Accelerator.load("tests/config/EBSTune.yaml", include_locations=False) sr.design.get_lattice().disable_6d() sr.design.trm.measure(callback=callback) sr.design.trm.save("tunemat.json") @@ -22,7 +22,7 @@ def test_tune_tool(): def test_tune_add(): - sr = Accelerator.load("tests/config/EBSTune.yaml", use_fast_loader=True) + sr = Accelerator.load("tests/config/EBSTune.yaml", include_locations=False) sr.design.get_lattice().disable_6d() sr.design.tune.load("tunemat.json") tune_initial = sr.design.tune.readback() @@ -33,7 +33,7 @@ def test_tune_add(): def test_chroma_tool(): - sr: Accelerator = Accelerator.load("tests/config/EBSOrbit.yaml", use_fast_loader=True) + sr: Accelerator = Accelerator.load("tests/config/EBSOrbit.yaml", include_locations=False) sr.design.get_lattice().enable_6d() sr.design.chromaticity.set([8.0, 5.0], iter=2) QpAT = sr.design.get_lattice().get_chrom()[:-1] @@ -45,7 +45,7 @@ def test_chroma_tool(): def test_chroma_add(): - sr: Accelerator = Accelerator.load("tests/config/EBSOrbit.yaml", use_fast_loader=True) + sr: Accelerator = Accelerator.load("tests/config/EBSOrbit.yaml", include_locations=False) sr.design.get_lattice().enable_6d() chromaAT = sr.design.get_lattice().get_chrom()[:-1] sr.design.chromaticity.add([0.5, 0.4]) diff --git a/tests/validation/test_generator.py b/tests/validation/test_generator.py new file mode 100644 index 000000000..b3d8917c5 --- /dev/null +++ b/tests/validation/test_generator.py @@ -0,0 +1,233 @@ +"""Tests of the schema generator.""" + +import json +import re +from collections.abc import Generator +from pathlib import Path + +import pytest +from pydantic import Field + +from pyaml.validation import ( + ConfigurationSchema, + SchemaGenerator, + SchemaRegistry, +) +from pyaml.validation.generator import RegistryJsonSchema + +# ========================================================== +# Dummy schemas +# ========================================================== + + +class DummySchema(ConfigurationSchema): + pass + + +class OtherSchema(ConfigurationSchema): + pass + + +class ParentSchema(ConfigurationSchema): + """Parent schema used to test inheritance.""" + + pass + + +class ChildSchemaA(ParentSchema): + a: int = 1 + + +class ChildSchemaB(ParentSchema): + b: str = "x" + + +class VirtualChildSchema(ConfigurationSchema): + b: str = "x" + + +class ContainerSchema(ConfigurationSchema): + model: ChildSchemaA | None = Field( + default=None, + description="Container schema used for testing.", + ) + + +# ========================================================== +# Fixtures +# ========================================================== + + +@pytest.fixture(autouse=True) +def clear_registry() -> Generator[None, None, None]: + """Ensure the registry is empty for each test.""" + + registry = SchemaRegistry() + registry.clear() + yield + registry.clear() + + +@pytest.fixture +def registry() -> SchemaRegistry: + return SchemaRegistry() + + +# ========================================================== +# Generate +# ========================================================== + + +def test_generate_raises_clean_keyerror_for_missing_schema(registry: SchemaRegistry): + class_path = "pkg.module.Class" + + with pytest.raises( + KeyError, + match=re.escape(f"No schema registered for '{class_path}'"), + ): + SchemaGenerator.generate(class_path) + + +def test_generate_returns_schema_for_registered_class(registry: SchemaRegistry): + class_path = "pkg.module.Class" + + registry.register(class_path, DummySchema) + + schema = SchemaGenerator.generate(class_path) + + assert schema["title"] == "DummySchema" + + +# ========================================================== +# Save +# ========================================================== + + +def test_save_writes_schema_to_file(registry: SchemaRegistry, tmp_path: Path): + class_path = "pkg.module.Class" + registry.register(class_path, DummySchema) + + filename = tmp_path / "schema.json" + + result = SchemaGenerator.save(class_path, filename, indent=2) + + assert result == filename + assert json.loads(filename.read_text(encoding="utf-8")) == SchemaGenerator.generate(class_path) + + +# ========================================================== +# Registry-aware polymorphism +# ========================================================== + + +def test_generate_replaces_parent_schema_with_registered_subclasses( + registry: SchemaRegistry, +): + registry.register("pkg.module.Parent", ParentSchema) + registry.register("pkg.module.ChildA", ChildSchemaA) + registry.register("pkg.module.ChildB", ChildSchemaB) + + schema = SchemaGenerator.generate("pkg.module.Parent") + + oneof = schema.get("oneOf", []) + refs = {item["$ref"] for item in oneof if "$ref" in item} + if refs: + assert "#/$defs/ChildSchemaA" in refs + assert "#/$defs/ChildSchemaB" in refs + else: + class_paths = {item["properties"]["class"]["const"] for item in oneof if "properties" in item} + assert "pkg.module.ChildA" in class_paths + assert "pkg.module.ChildB" in class_paths + + +def test_generate_includes_real_and_virtual_subclasses( + registry: SchemaRegistry, +): + registry.register("pkg.module.Parent", ParentSchema) + registry.register("pkg.module.ChildA", ChildSchemaA) + registry.register("pkg.module.VirtualChild", VirtualChildSchema) + + ParentSchema.register_virtual_subclass(VirtualChildSchema) + + schema = SchemaGenerator.generate("pkg.module.Parent") + + oneof = schema.get("oneOf", []) + refs = {item["$ref"] for item in oneof if "$ref" in item} + if refs: + assert "#/$defs/ChildSchemaA" in refs + assert "#/$defs/VirtualChildSchema" in refs + else: + class_paths = {item["properties"]["class"]["const"] for item in oneof if "properties" in item} + assert "pkg.module.ChildA" in class_paths + assert "pkg.module.VirtualChild" in class_paths + + +def test_model_schema_preserves_metadata_from_parent_schema( + registry: SchemaRegistry, +): + registry.register("pkg.module.Parent", ParentSchema) + registry.register("pkg.module.ChildA", ChildSchemaA) + registry.register("pkg.module.ChildB", ChildSchemaB) + + schema = ParentSchema.model_json_schema(schema_generator=RegistryJsonSchema) + + assert schema["title"] == "ParentSchema" + assert schema["description"] == "Parent schema used to test inheritance." + + +# ========================================================== +# Literals +# ========================================================== + + +def test_add_literals_to_class_path_ignores_empty_literal_list(): + schema = {"type": "string"} + + RegistryJsonSchema._add_literals_to_class_path(schema, []) + + assert schema == {"type": "string"} + + +def test_add_literals_to_class_path_replaces_single_value_with_const(): + schema = {"type": "string"} + + RegistryJsonSchema._add_literals_to_class_path( + schema, + ["pkg.module.Parent"], + ) + + assert schema["const"] == "pkg.module.Parent" + assert "enum" not in schema + + +def test_add_literals_to_class_path_merges_existing_enum_and_removes_duplicates(): + schema = {"type": "string", "enum": ["pkg.module.Parent", "pkg.module.ChildA"]} + + RegistryJsonSchema._add_literals_to_class_path( + schema, + ["pkg.module.ChildA", "pkg.module.ChildB", "pkg.module.Parent"], + ) + + assert schema["enum"] == [ + "pkg.module.Parent", + "pkg.module.ChildA", + "pkg.module.ChildB", + ] + assert "const" not in schema + + +def test_add_literals_to_class_path_does_not_modify_non_string_schema_without_enum(): + schema = {"type": "integer"} + + RegistryJsonSchema._add_literals_to_class_path(schema, ["pkg.module.Parent"]) + + assert schema == {"type": "integer"} + + +def test_add_literals_to_class_path_updates_existing_enum_even_without_string_type(): + schema = {"enum": ["pkg.module.Parent"]} + + RegistryJsonSchema._add_literals_to_class_path(schema, ["pkg.module.ChildA"]) + + assert schema["enum"] == ["pkg.module.Parent", "pkg.module.ChildA"] + assert "const" not in schema diff --git a/tests/validation/test_models.py b/tests/validation/test_models.py new file mode 100644 index 000000000..7913fa7c4 --- /dev/null +++ b/tests/validation/test_models.py @@ -0,0 +1,445 @@ +"""Tests of the configuration models.""" + +import inspect +import json +from dataclasses import dataclass + +import pytest +from pydantic import BaseModel, ValidationError +from pydantic.errors import PydanticSchemaGenerationError + +from pyaml.common.exception import PyAMLConfigException +from pyaml.validation import ConfigurationSchema, DynamicValidation, StaticValidation +from pyaml.validation.configuration_models import PyAMLBaseModel +from pyaml.validation.validation_models import ValidationModel + +# ========================================================== +# PyAMLBaseModel +# ========================================================== + + +def test_model_dump_serializes_subclass_fields(): + class Device(PyAMLBaseModel): + name: str + + class Magnet(Device): + type: str + + class Accelerator(PyAMLBaseModel): + device: Device + + accelerator = Accelerator(device=Magnet(name="QF", type="Quadrupole")) + + dumped = accelerator.model_dump() + + assert dumped == {"device": {"name": "QF", "type": "Quadrupole"}} + + +def test_model_dump_json_serializes_subclass_fields(): + class Device(PyAMLBaseModel): + name: str + + class Magnet(Device): + type: str + + class Accelerator(PyAMLBaseModel): + device: Device + + accelerator = Accelerator(device=Magnet(name="QF", type="Quadrupole")) + + dumped_json = accelerator.model_dump_json() + dumped = json.loads(dumped_json) + + assert dumped == {"device": {"name": "QF", "type": "Quadrupole"}} + + +# ========================================================== +# ConfigurationSchema +# ========================================================== + + +def test_configuration_schema_accepts_alias_class(): + schema = ConfigurationSchema.model_validate({"class": "pkg.module.Class"}) + + assert schema.class_path == "pkg.module.Class" + + +def test_configuration_schema_accepts_field_name_class_path(): + schema = ConfigurationSchema.model_validate({"class_path": "pkg.module.Class"}) + + assert schema.class_path == "pkg.module.Class" + + +def test_configuration_schema_forbids_extra_fields(): + with pytest.raises(ValidationError) as exc_info: + ConfigurationSchema.model_validate( + { + "class": "pkg.module.Class", + "unexpected": "value", + } + ) + + assert "extra_forbidden" in str(exc_info.value) + + +def test_configuration_schema_do_not_allow_arbitrary_types(): + class ArbitraryType: + pass + + with pytest.raises(PydanticSchemaGenerationError): + + class TestModel(ConfigurationSchema): + value: ArbitraryType + + +def test_configuration_schema_dump_uses_alias_when_requested(): + schema = ConfigurationSchema.model_validate({"class": "pkg.module.Class"}) + + dumped = schema.model_dump(by_alias=True) + + assert dumped == {"class": "pkg.module.Class"} + + +def test_configuration_schema_registers_virtual_subclass(): + class Curve(ConfigurationSchema): + pass + + class Curve1(ConfigurationSchema): + pass + + Curve.register_virtual_subclass(Curve1) + + assert Curve1 in Curve.virtual_subclasses() + assert Curve1.is_virtual_subclass_of(Curve) + + +def test_configuration_schema_is_virtual_subclass_of_is_transitive(): + class Curve(ConfigurationSchema): + pass + + class Curve1(ConfigurationSchema): + pass + + class Curve2(ConfigurationSchema): + pass + + Curve.register_virtual_subclass(Curve1) + Curve1.register_virtual_subclass(Curve2) + + assert Curve1.is_virtual_subclass_of(Curve) + assert Curve2.is_virtual_subclass_of(Curve) + assert Curve2.is_virtual_subclass_of(Curve1) + assert Curve.is_virtual_subclass_of(Curve) + assert not Curve.is_virtual_subclass_of(Curve1) + assert not Curve1.is_virtual_subclass_of(Curve2) + + +def test_configuration_schema_virtual_subclasses_are_per_class(): + class Curve(ConfigurationSchema): + pass + + class Curve1(ConfigurationSchema): + pass + + class Curve2(ConfigurationSchema): + pass + + Curve.register_virtual_subclass(Curve1) + Curve1.register_virtual_subclass(Curve2) + + assert Curve.virtual_subclasses() == {Curve1} + assert Curve1.virtual_subclasses() == {Curve2} + assert Curve2.virtual_subclasses() == set() + + +def test_configuration_schema_virtual_subclasses_returns_copy(): + class Curve(ConfigurationSchema): + pass + + class Curve1(ConfigurationSchema): + pass + + Curve.register_virtual_subclass(Curve1) + + subclasses = Curve.virtual_subclasses() + subclasses.clear() + + assert Curve.virtual_subclasses() == {Curve1} + + +def test_configuration_schema_register_virtual_subclass_rejects_non_schema(): + class Curve(ConfigurationSchema): + pass + + with pytest.raises(TypeError, match="is not a ConfigurationSchema subclass"): + Curve.register_virtual_subclass(int) # type: ignore[arg-type] + + +def test_configuration_schema_is_virtual_subclass_of_rejects_non_schema(): + class Curve(ConfigurationSchema): + pass + + with pytest.raises(TypeError, match="is not a ConfigurationSchema"): + Curve.is_virtual_subclass_of(int) # type: ignore[arg-type] + + +# ========================================================== +# ValidationModel +# ========================================================== + + +class DummyDevice: + pass + + +class DummyModel(ValidationModel): + device: DummyDevice + + +def test_validation_model_allows_arbitrary_types(): + device = DummyDevice() + + schema = DummyModel.model_validate({"device": device}) + + assert schema.device is device + + +def test_validation_model_forbids_extra_fields(): + with pytest.raises(ValidationError): + DummyModel.model_validate({"device": DummyDevice(), "extra_field": 123}) + + +# ========================================================== +# DynamicValidation +# ========================================================== + + +def test_dynamic_validation_builds_model_from_init_signature(): + class MyClass(DynamicValidation): + def __init__(self, name: str, count: int = 0): + self.name = name + self.count = count + + assert issubclass(MyClass.validation_model, ValidationModel) + assert list(MyClass.validation_model.model_fields) == ["name", "count"] + + name_field = MyClass.validation_model.model_fields["name"] + count_field = MyClass.validation_model.model_fields["count"] + + assert name_field.annotation is str + assert name_field.is_required() + + assert count_field.annotation is int + assert count_field.default == 0 + + +def test_dynamic_validation_accepts_positional_and_keyword_arguments(): + class MyClass(DynamicValidation): + def __init__(self, name: str, count: int = 0): + self.name = name + self.count = count + + obj1 = MyClass("test", 1) + obj2 = MyClass(name="test", count=1) + obj3 = MyClass("test") + + assert obj1.name == "test" + assert obj1.count == 1 + + assert obj2.name == "test" + assert obj2.count == 1 + + assert obj3.name == "test" + assert obj3.count == 0 + + +def test_dynamic_validation_coerces_and_rejects_invalid_input(): + class MyClass(DynamicValidation): + def __init__(self, name: str, count: int): + self.name = name + self.count = count + + obj = MyClass(name="test", count="12") + assert obj.count == 12 + + with pytest.raises(PyAMLConfigException): + MyClass(name="test", count="not-an-int") + + +def test_dynamic_validation_rejects_manual_validation_model(): + class ManualModel(BaseModel): + name: str + + with pytest.raises(TypeError, match="may not define validation_model manually"): + + class Broken(DynamicValidation): + validation_model = ManualModel + + def __init__(self, name: str): + self.name = name + + +def test_dynamic_validation_can_be_disabled_per_instance(): + class MyClass(DynamicValidation): + def __init__(self, name: str, count: int): + self.name = name + self.count = count + + obj = MyClass(name="test", count="12", validate=False) + + assert obj.name == "test" + assert obj.count == "12" + + +# ========================================================== +# StaticValidation +# ========================================================== + + +def test_static_validation_accepts_explicit_basemodel(): + class ExampleModel(BaseModel): + name: str + count: int = 0 + + class Example(StaticValidation): + validation_model = ExampleModel + + def __init__(self, name: str, count: int = 0): + self.name = name + self.count = count + + obj1 = Example("test", 1) + obj2 = Example(name="test", count=1) + obj3 = Example("test") + + assert obj1.name == "test" + assert obj1.count == 1 + + assert obj2.name == "test" + assert obj2.count == 1 + + assert obj3.name == "test" + assert obj3.count == 0 + + +def test_static_validation_validates_and_coerces_input(): + class ExampleModel(BaseModel): + name: str + count: int + + class Example(StaticValidation): + validation_model = ExampleModel + + def __init__(self, name: str, count: int): + self.name = name + self.count = count + + obj = Example(name="test", count="12") + assert obj.count == 12 + + with pytest.raises(PyAMLConfigException): + Example(name="test", count="not-an-int") + + +def test_static_validation_inherits_validation_model(): + class ParentModel(BaseModel): + name: str + + class Parent(StaticValidation): + validation_model = ParentModel + + def __init__(self, name: str): + self.name = name + + class Child(Parent): + def __init__(self, name: str): + super().__init__(name) + + obj = Child("test") + assert obj.name == "test" + assert Child.validation_model is ParentModel + + +def test_static_validation_requires_a_validation_model(): + with pytest.raises(TypeError, match="must define validation_model"): + + class Broken(StaticValidation): + def __init__(self, name: str): + self.name = name + + +# ========================================================== +# ValidationMeta signatures +# ========================================================== + + +def test_dynamic_validation_exposes_constructor_signature(): + class MyClass(DynamicValidation): + def __init__(self, name: str, count: int = 0): + self.name = name + self.count = count + + signature = inspect.signature(MyClass) + + assert list(signature.parameters) == ["name", "count"] + assert signature.parameters["count"].default == 0 + assert signature.return_annotation is inspect.Signature.empty + + +def test_static_validation_exposes_constructor_signature(): + class ExampleModel(BaseModel): + name: str + + class Example(StaticValidation): + validation_model = ExampleModel + + def __init__(self, name: str): + self.name = name + + assert list(inspect.signature(Example).parameters) == ["name"] + + +def test_validation_signature_excludes_validate_keyword(): + class MyClass(DynamicValidation): + def __init__(self, name: str): + self.name = name + + assert "validate" not in inspect.signature(MyClass).parameters + + +def test_validation_signature_uses_inherited_constructor(): + class Parent(DynamicValidation): + def __init__(self, name: str, count: int = 0): + self.name = name + self.count = count + + class Child(Parent): + pass + + assert list(inspect.signature(Child).parameters) == ["name", "count"] + + +def test_validation_signature_of_class_without_constructor_is_empty(): + class MyClass(DynamicValidation): + pass + + assert inspect.signature(MyClass) == inspect.Signature() + + +def test_validation_signature_matches_dataclass_fields(): + @dataclass + class MyClass(DynamicValidation): + name: str + count: int = 0 + + assert list(inspect.signature(MyClass).parameters) == ["name", "count"] + + +def test_validation_signature_not_visible_on_instances(): + class MyClass(DynamicValidation): + def __init__(self, name: str): + self.name = name + + obj = MyClass("test") + + assert not hasattr(obj, "__signature__") diff --git a/tests/validation/test_registry.py b/tests/validation/test_registry.py new file mode 100644 index 000000000..df5b68e6f --- /dev/null +++ b/tests/validation/test_registry.py @@ -0,0 +1,378 @@ +"""Tests of the schema registry.""" + +import re +from collections.abc import Generator + +import pytest + +from pyaml.validation import ConfigurationSchema, SchemaRegistry, register_schema + +# ========================================================== +# Dummy schemas +# ========================================================== + + +class DummySchema(ConfigurationSchema): + pass + + +class OtherSchema(ConfigurationSchema): + pass + + +# ========================================================== +# Fixtures +# ========================================================== + + +@pytest.fixture(autouse=True) +def clear_registry() -> Generator[None, None, None]: + """Ensure the registry is empty for each test.""" + + registry = SchemaRegistry() + registry.clear() + yield + registry.clear() + + +@pytest.fixture +def registry() -> SchemaRegistry: + return SchemaRegistry() + + +# ========================================================== +# Singleton behaviour +# ========================================================== + + +def test_singleton_returns_same_instance(): + assert SchemaRegistry() is SchemaRegistry() + + +# ========================================================== +# Registration +# ========================================================== + + +def test_register_stores_schema(registry: SchemaRegistry): + registry.register("pkg.module.Class", DummySchema) + + assert registry["pkg.module.Class"] is DummySchema + + +def test_register_allows_same_schema_for_existing_class_path(registry: SchemaRegistry): + class_path = "pkg.module.Class" + + registry.register(class_path, DummySchema) + registry.register(class_path, DummySchema) + + assert registry[class_path] is DummySchema + assert len(registry) == 1 + + +def test_register_raises_valueerror_for_different_schema(registry: SchemaRegistry): + class_path = "pkg.module.Class" + + registry.register(class_path, DummySchema) + + with pytest.raises( + ValueError, + match=re.escape(f"{class_path} already registered with a different schema."), + ): + registry.register(class_path, OtherSchema) + + +def test_register_raises_typeerror_for_invalid_schema(registry: SchemaRegistry): + with pytest.raises( + TypeError, + match=re.escape("must inherit from ConfigurationSchema"), + ): + registry.register( + "pkg.module.Class", + object, # type: ignore[arg-type] + ) + + +# ========================================================== +# Unregistering +# ========================================================== + + +def test_unregister_removes_registered_schema(registry: SchemaRegistry): + class_path = "pkg.module.Class" + + registry.register(class_path, DummySchema) + + registry.unregister(class_path) + + assert class_path not in registry + + +def test_unregister_raises_clean_keyerror_for_missing_schema( + registry: SchemaRegistry, +): + class_path = "pkg.module.Class" + + with pytest.raises( + KeyError, + match=re.escape(f"No schema registered for '{class_path}'"), + ): + registry.unregister(class_path) + + +def test_unregister_removes_only_requested_schema(registry: SchemaRegistry): + registry.register("pkg.module.ClassA", DummySchema) + registry.register("pkg.module.ClassB", OtherSchema) + + registry.unregister("pkg.module.ClassA") + + assert "pkg.module.ClassA" not in registry + assert registry["pkg.module.ClassB"] is OtherSchema + assert len(registry) == 1 + + +# ========================================================== +# Clearing +# ========================================================== + + +def test_clear_removes_all_registered_schemas(registry: SchemaRegistry): + registry.register("pkg.module.ClassA", DummySchema) + registry.register("pkg.module.ClassB", OtherSchema) + + registry.clear() + + assert len(registry) == 0 + assert "pkg.module.ClassA" not in registry + assert "pkg.module.ClassB" not in registry + + +def test_clear_on_empty_registry_keeps_registry_empty( + registry: SchemaRegistry, +): + registry.clear() + + assert len(registry) == 0 + + +def test_clear_allows_new_registrations_afterwards( + registry: SchemaRegistry, +): + registry.register("pkg.module.Class", DummySchema) + + registry.clear() + + registry.register("pkg.module.OtherClass", OtherSchema) + + assert len(registry) == 1 + assert registry["pkg.module.OtherClass"] is OtherSchema + + +# ========================================================== +# Lookup +# ========================================================== + + +def test_getitem_raises_clean_keyerror_for_missing_schema(registry: SchemaRegistry): + with pytest.raises(KeyError, match=r"No schema registered for 'pkg\.module\.Class.'"): + _ = registry["pkg.module.Class"] + + +def test_get_returns_registered_schema(registry: SchemaRegistry): + registry.register("pkg.module.Class", DummySchema) + + assert registry.get("pkg.module.Class") is DummySchema + + +def test_get_returns_none_for_missing_schema(registry: SchemaRegistry): + assert registry.get("pkg.module.Class") is None + + +# ========================================================== +# Contents +# ========================================================== + + +def test_items_returns_registered_items(registry: SchemaRegistry): + registry.register("pkg.module.ClassA", DummySchema) + registry.register("pkg.module.ClassB", OtherSchema) + + items = registry.items() + + assert ("pkg.module.ClassA", DummySchema) in items + assert ("pkg.module.ClassB", OtherSchema) in items + assert len(items) == 2 + + +def test_keys_returns_registered_class_paths(registry: SchemaRegistry): + registry.register("pkg.module.ClassA", DummySchema) + registry.register("pkg.module.ClassB", OtherSchema) + + keys = registry.keys() + + assert "pkg.module.ClassA" in keys + assert "pkg.module.ClassB" in keys + assert len(keys) == 2 + + +def test_values_returns_registered_schemas(registry: SchemaRegistry): + registry.register("pkg.module.ClassA", DummySchema) + registry.register("pkg.module.ClassB", OtherSchema) + + values = registry.values() + + assert DummySchema in values + assert OtherSchema in values + assert len(values) == 2 + + +def test_iter_returns_registered_class_paths(registry: SchemaRegistry): + registry.register("pkg.module.ClassA", DummySchema) + registry.register("pkg.module.ClassB", OtherSchema) + + class_paths = list(iter(registry)) + + assert "pkg.module.ClassA" in class_paths + assert "pkg.module.ClassB" in class_paths + assert len(class_paths) == 2 + + +# ========================================================== +# Updating +# ========================================================== + + +def test_update_replaces_registered_schema(registry: SchemaRegistry): + registry.register("pkg.module.Class", DummySchema) + + registry.update("pkg.module.Class", OtherSchema) + + assert registry["pkg.module.Class"] is OtherSchema + + +def test_update_raises_keyerror_for_missing_schema(registry: SchemaRegistry): + class_path = "pkg.module.Class" + + with pytest.raises( + KeyError, + match=re.escape(f"{class_path} is not registered."), + ): + registry.update(class_path, DummySchema) + + +def test_update_raises_typeerror_for_invalid_schema(registry: SchemaRegistry): + with pytest.raises( + TypeError, + match=r"must inherit from ConfigurationSchema", + ): + registry.update( + "pkg.module.Class", + object, # type: ignore[arg-type] + ) + + +# ========================================================== +# Representation +# ========================================================== + + +def test_repr_returns_empty_registry_representation( + registry: SchemaRegistry, +): + assert repr(registry) == "SchemaRegistry({})" + + +def test_repr_returns_registered_schemas( + registry: SchemaRegistry, +): + registry.register("pkg.module.ClassA", DummySchema) + registry.register("pkg.module.ClassB", OtherSchema) + + result = repr(registry) + + assert result.startswith("SchemaRegistry(") + assert "'pkg.module.ClassA'" in result + assert "'pkg.module.ClassB'" in result + + assert f"{DummySchema.__module__}.{DummySchema.__name__}" in result + assert f"{OtherSchema.__module__}.{OtherSchema.__name__}" in result + + assert result.endswith(")") + + +def test_repr_sorts_registered_class_paths( + registry: SchemaRegistry, +): + registry.register("pkg.module.ZClass", DummySchema) + registry.register("pkg.module.AClass", OtherSchema) + + result = repr(registry) + + assert result.index("'pkg.module.AClass'") < result.index("'pkg.module.ZClass'") + + +# ========================================================== +# Register schema decorator +# ========================================================== + + +def test_register_schema_registers_the_decorated_class( + registry: SchemaRegistry, +): + @register_schema(DummySchema) + class DecoratedClass: + pass + + class_path = f"{DecoratedClass.__module__}.{DecoratedClass.__name__}" + + assert registry[class_path] is DummySchema + + +def test_register_schema_can_register_multiple_classes_with_same_schema( + registry: SchemaRegistry, +): + @register_schema(DummySchema) + class FirstClass: + pass + + @register_schema(DummySchema) + class SecondClass: + pass + + first_path = f"{FirstClass.__module__}.{FirstClass.__name__}" + second_path = f"{SecondClass.__module__}.{SecondClass.__name__}" + + assert registry[first_path] is DummySchema + assert registry[second_path] is DummySchema + assert len(registry) == 2 + + +def test_register_schema_generates_and_registers_schema_for_class(registry: SchemaRegistry): + @register_schema + class DecoratedClass: + def __init__(self, value: int): + pass + + class_path = f"{DecoratedClass.__module__}.{DecoratedClass.__name__}" + + schema = registry[class_path] + assert schema.__name__ == "DecoratedClassConfigurationSchema" + assert "value" in schema.model_fields + + +def test_register_schema_with_empty_call_generates_and_registers_schema( + registry: SchemaRegistry, +): + @register_schema() + class DecoratedClass: + def __init__(self, value: int): + pass + + class_path = f"{DecoratedClass.__module__}.{DecoratedClass.__name__}" + + assert class_path in registry + + +def test_register_schema_rejects_non_schema_explicit_argument(): + with pytest.raises(TypeError): + register_schema(123) diff --git a/tests/validation/test_schema_builder.py b/tests/validation/test_schema_builder.py new file mode 100644 index 000000000..796fdbfd0 --- /dev/null +++ b/tests/validation/test_schema_builder.py @@ -0,0 +1,256 @@ +"""Tests of the schema builder.""" + +import inspect +from abc import ABC +from collections.abc import Generator +from enum import Enum +from typing import Annotated, Any, Literal, get_args, get_origin + +import pytest +from pydantic import BaseModel, Field + +from pyaml.validation.configuration_models import ConfigurationSchema +from pyaml.validation.registry import SchemaRegistry +from pyaml.validation.schema_builder import ( + EXCLUDED_TYPES, + _configuration_schema_from_basemodel, + _field_definition_from_field_info, + _fields_from_constructor_signature, + _generate_schema_name, + _resolve_annotation, + generate_configuration_schema, +) + + +@pytest.fixture(autouse=True) +def clear_registry() -> Generator[None, None, None]: + """Ensure the registry is empty for each test.""" + + registry = SchemaRegistry() + registry.clear() + yield + registry.clear() + + +class Color(Enum): + RED = "red" + + +def test_generate_schema_name(): + class Magnet: + pass + + assert _generate_schema_name(Magnet) == "MagnetConfigurationSchema" + + +def test_generate_configuration_schema_requires_class(): + with pytest.raises(TypeError, match="Source must be a class"): + generate_configuration_schema(1) + + +def test_generate_configuration_schema_from_validation_model(): + class ValidationModel(BaseModel): + strength: int + name: str = "Q1" + + class Magnet: + validation_model = ValidationModel + + schema = generate_configuration_schema(Magnet) + + assert issubclass(schema, ConfigurationSchema) + assert schema.__name__ == "MagnetConfigurationSchema" + assert schema.model_fields["strength"].annotation is int + assert schema.model_fields["name"].default == "Q1" + + registry = SchemaRegistry() + assert registry.get(f"{Magnet.__module__}.{Magnet.__name__}") is schema + + +def test_generate_configuration_schema_from_constructor(): + class Magnet: + def __init__(self, strength: int, name: str = "Q1"): + pass + + schema = generate_configuration_schema(Magnet) + + assert issubclass(schema, ConfigurationSchema) + assert schema.model_fields["strength"].annotation is int + assert schema.model_fields["name"].default == "Q1" + + registry = SchemaRegistry() + assert registry.get(f"{Magnet.__module__}.{Magnet.__name__}") is schema + + +def test_generate_configuration_schema_is_cached(): + class Magnet: + def __init__(self, strength: int): + pass + + schema1 = generate_configuration_schema(Magnet) + schema2 = generate_configuration_schema(Magnet) + + assert schema1 is schema2 + + +def test_configuration_schema_from_basemodel_rejects_reserved_field(): + class ValidationModel(BaseModel): + class_path: str + + with pytest.raises(ValueError, match="reserved field"): + _configuration_schema_from_basemodel( + ValidationModel, + "BadConfigurationSchema", + __name__, + ) + + +def test_generate_configuration_schema_registers_parent_chain(): + class Curve: + pass + + class Curve1(Curve): + pass + + class Curve2(Curve1): + pass + + curve2_schema = generate_configuration_schema(Curve2) + + registry = SchemaRegistry() + curve_path = f"{Curve.__module__}.{Curve.__name__}" + curve1_path = f"{Curve1.__module__}.{Curve1.__name__}" + curve2_path = f"{Curve2.__module__}.{Curve2.__name__}" + + curve_schema = registry.get(curve_path) + curve1_schema = registry.get(curve1_path) + curve2_schema_from_registry = registry.get(curve2_path) + + assert curve_schema is not None + assert curve1_schema is not None + assert curve2_schema_from_registry is curve2_schema + + assert curve1_schema.is_virtual_subclass_of(curve_schema) + assert curve2_schema.is_virtual_subclass_of(curve1_schema) + assert curve2_schema.is_virtual_subclass_of(curve_schema) + assert not curve_schema.is_virtual_subclass_of(curve1_schema) + + +def test_generate_configuration_schema_registers_multiple_inheritance(): + class Curve: + pass + + class Monitor: + pass + + class Curve1(Curve): + pass + + class Curve2(Curve1, Monitor): + pass + + curve2_schema = generate_configuration_schema(Curve2) + + registry = SchemaRegistry() + curve_schema = registry.get(f"{Curve.__module__}.{Curve.__name__}") + monitor_schema = registry.get(f"{Monitor.__module__}.{Monitor.__name__}") + curve1_schema = registry.get(f"{Curve1.__module__}.{Curve1.__name__}") + curve2_schema_from_registry = registry.get(f"{Curve2.__module__}.{Curve2.__name__}") + + assert curve_schema is not None + assert monitor_schema is not None + assert curve1_schema is not None + assert curve2_schema_from_registry is curve2_schema + + assert curve1_schema.is_virtual_subclass_of(curve_schema) + assert curve2_schema.is_virtual_subclass_of(curve1_schema) + assert curve2_schema.is_virtual_subclass_of(curve_schema) + assert curve2_schema.is_virtual_subclass_of(monitor_schema) + + +def test_fields_from_constructor_signature(): + class Example: + def __init__(self, x: int, y: str = "a", *args, **kwargs): + pass + + fields = _fields_from_constructor_signature(Example) + + assert fields["x"] == (int, ...) + assert fields["y"] == (str, "a") + assert set(fields) == {"x", "y"} + + +def test_fields_from_constructor_signature_rejects_reserved_parameter(): + class Example: + def __init__(self, class_path: str): + pass + + with pytest.raises(ValueError, match="reserved parameter"): + _fields_from_constructor_signature(Example) + + +def test_resolve_annotation(): + assert _resolve_annotation(inspect._empty) is Any + assert _resolve_annotation(Any) is Any + assert _resolve_annotation(None) is type(None) + assert _resolve_annotation(int) is int + assert _resolve_annotation(Color) is Color + assert _resolve_annotation(list[int]) == list[int] + assert _resolve_annotation(dict[str, int]) == dict[str, int] + assert _resolve_annotation(tuple[int, ...]) == tuple[int, ...] + assert _resolve_annotation(tuple[int, str]) == tuple[int, str] + assert _resolve_annotation(set[int]) == set[int] + assert _resolve_annotation(frozenset[int]) == frozenset[int] + assert _resolve_annotation(int | str) == (int | str) + assert _resolve_annotation(Literal["a", "b"]) == Literal["a", "b"] + + annotated = _resolve_annotation(Annotated[int, "meta"]) + assert get_origin(annotated) is Annotated + assert get_args(annotated) == (int, "meta") + + +def test_excluded_framework_bases_are_not_registered(): + class FrameworkConfig(ABC): + pass + + class UserConfig(FrameworkConfig): + pass + + EXCLUDED_TYPES.add(FrameworkConfig) + try: + generate_configuration_schema(UserConfig) + registry = SchemaRegistry() + assert f"{FrameworkConfig.__module__}.{FrameworkConfig.__name__}" not in registry + assert f"{UserConfig.__module__}.{UserConfig.__name__}" in registry + finally: + EXCLUDED_TYPES.remove(FrameworkConfig) + + +def test_resolve_annotation_rejects_forward_reference(): + with pytest.raises(TypeError, match="Forward references"): + _resolve_annotation("SomeClass") + + +def test_field_definition_from_field_info(): + class Model(BaseModel): + x: int = Field( + default_factory=lambda: 5, + description="desc", + title="title", + examples=[1], + deprecated=True, + alias="alias", + ) + + annotation, field = _field_definition_from_field_info( + "x", + Model.model_fields["x"], + ) + + assert annotation is int + assert field.default_factory is not None + assert field.alias == "alias" + assert field.description == "desc" + assert field.title == "title" + assert field.examples == [1] + assert field.deprecated is True diff --git a/tests/validation/test_validation_errors.py b/tests/validation/test_validation_errors.py new file mode 100644 index 000000000..4dd3f0c66 --- /dev/null +++ b/tests/validation/test_validation_errors.py @@ -0,0 +1,105 @@ +"""Tests of validation errors.""" + +import pytest +from pydantic import BaseModel, ValidationError + +from pyaml.common.exception import PyAMLConfigException +from pyaml.validation.errors import ( + Location, + LocationMetadata, + extract_location_metadata, + raise_validation_error, +) + + +def test_location_str_formats_readably(): + loc = Location(file="config.yaml", line=12, column=4) + assert str(loc) == "config.yaml: line 12, column 4" + + +def test_extract_location_metadata_removes_metadata_and_converts_values(): + data = { + "__location__": ("config.yaml", 22, 3), + "__fieldlocations__": { + "class": ("config.yaml", 22, 10), + "name": ("config.yaml", 23, 9), + }, + "class": "pkg.module.Class", + "name": "test_device", + } + + cleaned, metadata = extract_location_metadata(data) + + assert cleaned == { + "class": "pkg.module.Class", + "name": "test_device", + } + assert metadata.location == Location("config.yaml", 22, 3) + assert metadata.field_locations == { + "class": Location("config.yaml", 22, 10), + "name": Location("config.yaml", 23, 9), + } + + +def test_extract_location_metadata_without_metadata_returns_clean_data(): + data = {"class": "pkg.module.Class", "name": "test_device"} + + cleaned, metadata = extract_location_metadata(data) + + assert cleaned == data + assert metadata.location is None + assert metadata.field_locations is None + + +class SimpleModel(BaseModel): + age: int + + +class DeepNestedModel(BaseModel): + items: list[SimpleModel] + + +def get_validation_error(model: type[BaseModel], payload: dict) -> ValidationError: + with pytest.raises(ValidationError) as exc: + model.model_validate(payload) + return exc.value + + +def test_raise_validation_error_formats_error_with_location_metadata(): + exc = get_validation_error(SimpleModel, {"age": "not-an-int"}) + + metadata = LocationMetadata( + location=Location("config.yaml", 20, 1), + field_locations={ + "age": Location("config.yaml", 21, 7), + }, + ) + + with pytest.raises(PyAMLConfigException) as err: + raise_validation_error( + exc, + class_path="pkg.module.Class", + location_metadata=metadata, + ) + + message = str(err.value) + + assert "'age'" in message + assert "for class: 'pkg.module.Class'" in message + assert "config.yaml: line 21, column 7" in message + assert "config.yaml: line 20, column 1." in message + + +def test_raise_validation_error_formats_deep_nested_error_tuple_repr(): + exc = get_validation_error(DeepNestedModel, {"items": [{"age": "nope"}]}) + + with pytest.raises(PyAMLConfigException) as err: + raise_validation_error( + exc, + class_path="demo.DeepNestedModel", + ) + + message = str(err.value) + print(message) + assert "items[0].age" in message + assert "for class: 'demo.DeepNestedModel'" in message diff --git a/tests/validation/test_validator.py b/tests/validation/test_validator.py new file mode 100644 index 000000000..3f357209d --- /dev/null +++ b/tests/validation/test_validator.py @@ -0,0 +1,263 @@ +"""Tests of the schema validator.""" + +import sys +from collections.abc import Generator +from types import ModuleType + +import pytest + +from pyaml.common.exception import PyAMLConfigException +from pyaml.validation import ( + ConfigurationSchema, + SchemaRegistry, + SchemaValidator, +) + +# ========================================================== +# Dummy schemas +# ========================================================== + + +class DummySchema(ConfigurationSchema): + value: int | None = None + + +class OtherSchema(ConfigurationSchema): + name: str | None = None + children: list[DummySchema] | None = None + + +# ========================================================== +# Fixtures +# ========================================================== + + +@pytest.fixture(autouse=True) +def clear_registry() -> Generator[None, None, None]: + """Ensure the registry is empty for each test.""" + + registry = SchemaRegistry() + registry.clear() + yield + registry.clear() + + +@pytest.fixture +def registry() -> SchemaRegistry: + return SchemaRegistry() + + +# ========================================================== +# Recursive validation +# ========================================================== + + +def test_recursive_validate_returns_validated_schema( + registry: SchemaRegistry, +): + registry.register("pkg.module.Class", DummySchema) + + data = { + "class_path": "pkg.module.Class", + "value": 42, + } + + result = SchemaValidator._recursive_validate(data) + + assert isinstance(result, DummySchema) + assert result.class_path == "pkg.module.Class" + assert result.value == 42 + + +def test_recursive_validate_recurses_through_nested_lists_and_dicts( + registry: SchemaRegistry, +): + registry.register("pkg.module.ClassA", DummySchema) + registry.register("pkg.module.ClassB", OtherSchema) + + data = { + "class_path": "pkg.module.ClassB", + "name": "dummy", + "children": [ + { + "class_path": "pkg.module.ClassA", + "value": "42", + }, + { + "class_path": "pkg.module.ClassA", + "value": "73", + }, + ], + } + + result = SchemaValidator._recursive_validate(data) + + assert isinstance(result, OtherSchema) + + assert isinstance(result.children[0], DummySchema) + assert result.children[0].value == 42 + + assert isinstance(result.children[1], DummySchema) + assert result.children[1].value == 73 + + +def test_recursive_validate_leaves_plain_dicts_unchanged(): + data = { + "plain": "dict", + } + + result = SchemaValidator._recursive_validate(data) + + assert result == data + + +def test_recursive_validate_leaves_non_container_values_unchanged(): + assert SchemaValidator._recursive_validate("text") == "text" + assert SchemaValidator._recursive_validate(123) == 123 + assert SchemaValidator._recursive_validate(True) is True + assert SchemaValidator._recursive_validate(None) is None + + +def test_recursive_validate_warns_for_unknown_schema( + registry: SchemaRegistry, +): + data = { + "class_path": "pkg.module.Unknown", + "value": 42, + } + + with pytest.warns( + UserWarning, + match=r"Unknown schema for 'pkg\.module\.Unknown' so cannot validate\. Leaving data as raw dict\.", + ): + result = SchemaValidator._recursive_validate(data) + + assert result == data + + +# ========================================================== +# Configuration parsing +# ========================================================== + + +def test_parse_configuration_returns_none_for_non_configuration_dict(): + data = { + "plain": "dict", + } + + result = SchemaValidator._parse_configuration(data) + + assert result is None + + +def test_parse_configuration_accepts_modern_configuration() -> None: + data = { + "class_path": "pkg.module.Class", + "value": 42, + } + + result = SchemaValidator._parse_configuration(data) + + assert result == data + + +def test_parse_configuration_translates_legacy_module_configuration( + monkeypatch: pytest.MonkeyPatch, +) -> None: + module_name = "legacy_test_module" + + module = ModuleType(module_name) + module.PYAMLCLASS = "LegacyClass" + monkeypatch.setitem(sys.modules, module_name, module) + + data = { + "module": module_name, + "value": 42, + } + + result = SchemaValidator._parse_configuration(data) + + assert result == { + "class_path": f"{module_name}.LegacyClass", + "value": 42, + } + + +# ========================================================== +# Top-level validation +# ========================================================== + + +def test_validate_returns_validated_configuration_schema( + registry: SchemaRegistry, +): + registry.register("pkg.module.Class", DummySchema) + + data = { + "class_path": "pkg.module.Class", + "value": 42, + } + + result = SchemaValidator.validate(data) + + assert isinstance(result, DummySchema) + assert result.class_path == "pkg.module.Class" + assert result.value == 42 + + +# def test_validate_raises_typeerror_for_non_configuration_dict(): +# data = { +# "plain": "dict", +# } + +# with pytest.raises( +# TypeError, +# match=r"Top-level configuration did not validate to a ConfigurationSchema\.", +# ): +# SchemaValidator.validate(data) + + +def test_validate_to_dict_returns_dict(registry: SchemaRegistry) -> None: + registry.register("pkg.module.Class", DummySchema) + + data = { + "class_path": "pkg.module.Class", + "value": 42, + } + + result = SchemaValidator.validate_to_dict(data) + + assert result == { + "class_path": "pkg.module.Class", + "value": 42, + } + + +# ========================================================== +# Error handling +# ========================================================== + + +def test_recursive_validate_includes_location_metadata_in_error( + registry: SchemaRegistry, +) -> None: + registry.register("pkg.module.Class", DummySchema) + + data = { + "__location__": ("config.yaml", 10, 4), + "__fieldlocations__": { + "value": ("config.yaml", 11, 8), + }, + "class_path": "pkg.module.Class", + "value": "not-an-int", + } + + with pytest.raises(PyAMLConfigException) as exc_info: + SchemaValidator._recursive_validate(data) + + message = str(exc_info.value) + + assert "pkg.module.Class" in message + assert "config.yaml: line 10, column 4." in message + assert "config.yaml: line 11, column 8" in message + assert "'value'" in message