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authortlatorre <tlatorre@uchicago.edu>2018-11-28 09:46:52 -0600
committertlatorre <tlatorre@uchicago.edu>2018-11-28 09:46:52 -0600
commitf93d19b96093cdd498639868700e0f722b7eb9b0 (patch)
tree64891421c89e0d2b2f77618993c2444a35cc2eda /src/likelihood.c
parent22090220988bd7d5631481c5b4cbfa2f95c11131 (diff)
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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/likelihood.c')
-rw-r--r--src/likelihood.c4
1 files changed, 2 insertions, 2 deletions
diff --git a/src/likelihood.c b/src/likelihood.c
index 40261f9..93740a0 100644
--- a/src/likelihood.c
+++ b/src/likelihood.c
@@ -944,9 +944,9 @@ double nll_muon(event *ev, int id, double T0, double *pos, double *dir, double t
if (ev->pmt_hits[i].hit) {
for (j = 1; j < MAX_PE; j++) {
if (fast)
- logp[j] = log_pq(ev->pmt_hits[i].qhs,j) - mu[i] + j*log_mu - lnfact(j) + log_pt_fast;
+ logp[j] = get_log_pq(ev->pmt_hits[i].qhs,j) - mu[i] + j*log_mu - lnfact(j) + log_pt_fast;
else
- logp[j] = log_pq(ev->pmt_hits[i].qhs,j) - mu[i] + j*log_mu - lnfact(j) + log_pt(ev->pmt_hits[i].t, j, mu_noise, mu_indirect, &mu_direct[i], &mu_shower[i], 1, &ts[i], &ts_shower[i], ts[i], PMT_TTS, &ts_sigma[i]);
+ logp[j] = get_log_pq(ev->pmt_hits[i].qhs,j) - mu[i] + j*log_mu - lnfact(j) + log_pt(ev->pmt_hits[i].t, j, mu_noise, mu_indirect, &mu_direct[i], &mu_shower[i], 1, &ts[i], &ts_shower[i], ts[i], PMT_TTS, &ts_sigma[i]);
if (j == 1 || logp[j] > max_logp) max_logp = logp[j];