- oleg's home page
- Posts
- 2024
- 2023
- February (1)
- 2022
- 2021
- 2020
- 2019
- 2018
- 2017
- 2016
- December (2)
- November (1)
- October (2)
- August (1)
- July (1)
- June (3)
- May (2)
- April (3)
- March (4)
- January (1)
- 2015
- 2014
- December (2)
- October (2)
- September (1)
- August (1)
- July (3)
- June (1)
- May (3)
- April (2)
- March (2)
- February (1)
- January (1)
- 2013
- My blog
- Post new blog entry
- All blogs
Parameters for FMS /w preshower in fast MC
Preshower layers PS1 & PS2 with a cut on maximum light yield (for photon/hadron separation):
Electromagnetic shower E_em from n_i hadron interactions in the FMS:
photon_survival = 0.98 hadron_survival = 0.05Preshower layer PS3 with a cut on maximum light yield (for electron/hadron separation):
electron_survival = 0.10 hadron_survival = 0.80
Electromagnetic shower E_em from n_i hadron interactions in the FMS:
E_em = 1. - pow(2./3., n_i) * energy_of_hadronwith the cumulative probability for n_i nuclear interactions in FMS (length = 1.8 lambda_int):
TRandom3 *my_random = new TRandom3(); p_i = my_random->Rndm(); if(p_i > 0.162) n_i=1; if(p_i > 0.457) n_i=2; if(p_i > 0.725) n_i=3; if(p_i > 0.888) n_i=4; if(p_i > 0.962) n_i=5; if(p_i > 0.989) n_i=6; if(p_i > 0.997) n_i=7; if(p_i > 0.999) n_i=8;
(*) Anything above 8 is largely diluted by the stochastic term in the shower.
Energy resolution in FMS (also applies to hadronic energy deposit above):
sigma_PbGl_rootE = 0.10; // stochastic term / sqrt(E) sigma_PbGl_const = 0.005; // constant term
(*) The stochastic term for PbGl detectors are usually on the order of less than 8%/sqrt(E), but previous studies with the FMS were as large as 14%. Since we include the converter in the preshower, we assume 10% for now.
Groups:
- oleg's blog
- Login or register to post comments