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author | tlatorre <tlatorre@uchicago.edu> | 2018-11-28 09:46:52 -0600 |
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committer | tlatorre <tlatorre@uchicago.edu> | 2018-11-28 09:46:52 -0600 |
commit | f93d19b96093cdd498639868700e0f722b7eb9b0 (patch) | |
tree | 64891421c89e0d2b2f77618993c2444a35cc2eda /src/test-charge.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/test-charge.c')
-rw-r--r-- | src/test-charge.c | 4 |
1 files changed, 1 insertions, 3 deletions
diff --git a/src/test-charge.c b/src/test-charge.c index 2fe199b..2373beb 100644 --- a/src/test-charge.c +++ b/src/test-charge.c @@ -70,7 +70,7 @@ int main(int argc, char **argv) for (i = 1; i <= n; i++) { for (j = 0; j < nq; j++) { - fprintf(pipe, "%.10f %.10f\n", x[j], pq(x[j],i)); + fprintf(pipe, "%.10f %.10f\n", x[j], get_pq(x[j],i)); } fprintf(pipe, "\n\n"); } @@ -82,7 +82,5 @@ int main(int argc, char **argv) free(x); - free_charge(); - return 0; } |