gmapy is a Python package to produce nuclear data
evaluations of cross sections including uncertainties
based on the combined data from various experiments.
This package can be regarded as a modernized version of the GMAP code developed by Wolfgang P. Poenitz, which was employed for the evaluation of the neutron data standards. A number of test cases have been created to prove that the latest neutron standards evaluation can be reproduced with gmapy. To learn more about improvements of gmapy over GMAP, please see the respective section below.
This package is still evolving and not well documented yet.
To get a first impression of the usage of gmapy, you can
inspect the Jupyter notebook examples/example-000-basic-usage.ipynb.
You can directly open this notebook in the browser by clicking
here.
gmapy depends on the SuiteSparse library.
Please consults the scikit-sparse GitHub repo for installation instructions.
If you are using the conda package manager, you can install gmapy in this way:
Download or clone this repository on your computer. Let's assume the repo is
stored in the directory gmapy. Then you can execute:
conda create -n gmapy-env python=3.10
conda activate gmapy-env
conda install -c conda-forge scikit-sparse==0.4.14
pip install ./gmapy
Here are the capabilities of gmapy at present that go beyond those of the Fortran GMAP code:
- Exact maximum likelihood optimization based on a custom version of the Levenberg-Marquardt algorithm with convergence checking.
- Adaptive numerical integration by Romberg's method with convergence checking for a precise computation of spectrum averaged cross sections.
- Indidvidual energy meshes for different reactions are possible to account for reaction-specific structures.
- Experimental data need not be aligned perfectly to the the computational mesh thanks to the use of linear interpolation.
- A new data type
ratios of spectrum averaged cross sectionsis available. - Data can be read in the database format used by GMAP as well as in a new JSON format.
- Unknown uncertainties can be introduced and estimated during the estimation of the cross sections and their uncertainties via maximum likelihood estimation.
This code is distributed under the MIT license, see the accompanying license file for more information.
Copyright (c) International Atomic Energy Agency (IAEA)