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| author | tlatorre <tlatorre@uchicago.edu> | 2018-11-28 09:46:52 -0600 |
|---|---|---|
| committer | tlatorre <tlatorre@uchicago.edu> | 2018-11-28 09:46:52 -0600 |
| commit | f93d19b96093cdd498639868700e0f722b7eb9b0 (patch) | |
| tree | 64891421c89e0d2b2f77618993c2444a35cc2eda /src/path.c | |
| parent | 22090220988bd7d5631481c5b4cbfa2f95c11131 (diff) | |
| download | sddm-f93d19b96093cdd498639868700e0f722b7eb9b0.tar.gz sddm-f93d19b96093cdd498639868700e0f722b7eb9b0.tar.bz2 sddm-f93d19b96093cdd498639868700e0f722b7eb9b0.zip | |
update sno_charge.c
This commit adds lots of comments to sno_charge.c and makes a couple of other
changes:
- use interp1d() instead of the GSL interpolation routines
- increase MAX_PE to 100
I increased MAX_PE because I determined that it had a rather large impact on
the likelihood function for 500 MeV electrons. This unfortunately slows down
the initialization by a lot. I think I could speed this up by convolving the
single PE charge distribution with a gaussian *before* convolving the charge
distributions to compute the charge distributions for multiple PE.
Diffstat (limited to 'src/path.c')
0 files changed, 0 insertions, 0 deletions