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authortlatorre <tlatorre@uchicago.edu>2018-08-27 10:59:31 -0500
committertlatorre <tlatorre@uchicago.edu>2018-08-27 10:59:31 -0500
commita84cfbe584580f08ca0a88f176cb49cdf801665e (patch)
tree9e51ec936b02e6bcdbe48fce43c1a70fcaf1b63e /src/muon.c
parent779266ec72a5c76ee52043ab3ae17479ba6a9788 (diff)
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fix how multiple Coulomb scattering is treated
Previously I had been assuming that a particle undergoing many small angle Coulomb scatters had a track direction whose polar angle was a Gaussian. However, this was just due to a misunderstanding of the PDG section "Multiple scattering through small angles" in the "Passage of particles through matter" article. In fact, what is described by a Gaussian is the polar angle projected onto a plane. Therefore the distribution of the polar angle is actually: (1/(sqrt(2*pi)*theta0**2))*theta*exp(-theta**2/(2*theta0)) This commit updates the code in scattering.c to correctly calculate the probability that a photon is emitted at a particular angle. I also updated test-likelihood.c to simulate a track correctly.
Diffstat (limited to 'src/muon.c')
-rw-r--r--src/muon.c2
1 files changed, 1 insertions, 1 deletions
diff --git a/src/muon.c b/src/muon.c
index 9a539de..7012214 100644
--- a/src/muon.c
+++ b/src/muon.c
@@ -262,5 +262,5 @@ double get_expected_charge(double x, double T, double T0, double *pos, double *d
theta0 = get_scattering_rms(x,p0,beta0,z,rho);
/* FIXME: add angular response and scattering/absorption. */
- return 2*omega*2*M_PI*FINE_STRUCTURE_CONSTANT*z*z*(1-(1/(beta*beta*n*n)))*get_probability(beta, cos_theta, theta0)/(sqrt(2*M_PI)*theta0);
+ return omega*FINE_STRUCTURE_CONSTANT*z*z*(1-(1/(beta*beta*n*n)))*get_probability(beta, cos_theta, theta0);
}