-
Notifications
You must be signed in to change notification settings - Fork 4
New issue
Have a question about this project? Sign up for a free GitHub account to open an issue and contact its maintainers and the community.
By clicking “Sign up for GitHub”, you agree to our terms of service and privacy statement. We’ll occasionally send you account related emails.
Already on GitHub? Sign in to your account
phys: investigate symbolic Dalitz Plot Decomposition #133
Conversation
Allows displaying free symbols in a more concise way
I'm having a look at the code now, it may be a bit difficult to rewrite the notebook to a generic form. I think ideally you need some data structure that contains all the info you need for each decay, like LS values in the production node and in the decay node and parent spin. There's some info on developing with notebooks here. Feedback is welcome. If you have the installed a virtual environment with tox -e nb docs/report/018.ipynb # run the notebook in terminal
tox -e doc # fast documentation build
tox -e docnb # build documentation with cell outputs For editing metadata in notebooks, it's best to work with Jupyter Lab. That also renders the myst syntax a bit better jupyter lab |
Certaintly. |
yes, that is what I did before with my julia code.
|
for more information, see https://pre-commit.ci
Do you mean
not sure I installed the |
Yep. Or to be even safer: pip install -e .[dev] -c .constraints/py3.8.txt # your python version here |
Saves CI time. Will be added through ComPWA#129
88725fb encapsulates that info as a (mutable) class. Could be rewritten by nesting for instance. I didn't push more modifications to avoid merge conflicts. |
TR-018 is already reserved for polarization sensitivity
…ompwa-org into dalitzdistribution
…litzdistribution
This PR has become superseded by https://github.com/ComPWA/ampform-dpd and https://lc2pkpi-polarimetry.docs.cern.ch. |
Preview can be viewed here.
The notebook is extended from the TR-018 (#129) to provide a different angle to the three-body decay distribution.
The unpolarized matrix element is casted to a bilinear form on dynamic function$R$ for every LS coupling.
Parity conservation is assumed.
To-do list