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update for new wmp library v1.0 - python api and docs
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4 changed files with 111 additions and 320 deletions
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@ -90,7 +90,7 @@ Assuming free-gas thermal motion, cross sections in the multipole form can be
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analytically Doppler broadened to give the form:
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.. math::
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\sigma(E, T) = \frac{1}{2 E \sqrt{\xi}} \sum_j \text{Re} \left[i r_j
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\sigma(E, T) = \frac{1}{2 E \sqrt{\xi}} \sum_j \text{Re} \left[r_j
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\sqrt{\pi} W_i(z) - \frac{r_j}{\sqrt{\pi}} C \left(\frac{p_j}{\sqrt{\xi}},
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\frac{u}{2 \sqrt{\xi}}\right)\right]
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.. math::
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@ -141,7 +141,7 @@ scattering does not occur in the resolved resonance region. This is usually,
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but not always the case. Future library versions may eliminate this issue.
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The data format used by OpenMC to represent windowed multipole data is specified
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in :ref:`io_data_wmp`.
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in :ref:`io_data_wmp` with a publicly available `WMP library`_.
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.. _temperature_treatment:
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@ -270,6 +270,7 @@ or even isotropic scattering.
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https://laws.lanl.gov/vhosts/mcnp.lanl.gov/pdf_files/la-ur-14-24530.pdf
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.. _Hwang: http://www.ans.org/pubs/journals/nse/a_16381
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.. _Josey: http://dx.doi.org/10.1016/j.jcp.2015.08.013
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.. _WMP Library: https://github.com/mit-crpg/WMP_Library
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.. _MCNP: http://mcnp.lanl.gov
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.. _Serpent: http://montecarlo.vtt.fi
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.. _NJOY: http://t2.lanl.gov/codes.shtml
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