Difference between revisions of "Background"
(Created 06/23/11(Zwzhao), Last modified 11/08/17(Zwzhao)) |
(Created 06/23/11(Zwzhao), Last modified 11/08/17(Zwzhao)) |
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== PVDIS Geant4 modeled background from Target == | == PVDIS Geant4 modeled background from Target == | ||
| − | Rates and flux from GEMC for PVDIS follow. Validation against GEANT3 can be found here: [ | + | Rates and flux from GEMC for PVDIS follow. Validation against GEANT3 can be found here: [https://hallaweb.jlab.org/wiki/index.php/Compare_to_geant3_result]. |
Rates on GEMs for 50uA on LH2. Solid lines are unbaffled, dashed are with lead baffles: | Rates on GEMs for 50uA on LH2. Solid lines are unbaffled, dashed are with lead baffles: | ||
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== <math>\pi</math>/e Ratio == | == <math>\pi</math>/e Ratio == | ||
| − | See [[ | + | See [[pi e ratio| here]] |
Latest revision as of 11:24, 4 December 2020
Contents
rate
The result is at /work/halla/solid/evgen
SIDIS e and hadron rate
generated by "collider", the code and script for analyzing result are at https://jlabsvn.jlab.org/svnroot/solid/evgen/collider
The result is here
single particle rate
various particle from vertex is estimated by "eicRate" in our event generator repository. The code and script for analyzing result are at https://jlabsvn.jlab.org/svnroot/solid/evgen/eicRate_20101102 https://jlabsvn.jlab.org/svnroot/solid/evgen/eicRate_20101102/output
rate study
pdf Comparison with 6GeV transversity data by Xin Qian
pptx pdf event generator rate comparison, study by Zhiwen Zhao and Zhihong Ye
pdf study by Nguyen Ton and Xiaochao Zheng (outdated)
other staff
PVDIS Geant4 modeled background from Target
Rates and flux from GEMC for PVDIS follow. Validation against GEANT3 can be found here: [1].
Rates on GEMs for 50uA on LH2. Solid lines are unbaffled, dashed are with lead baffles:
Flux in EM calorimeter for 50uA on LH2. Solid lines are unbaffled, dashed are with lead baffles. The true rate should be taken from the black lines.
SIDIS Geant4 modeled background from Target
<math>\pi</math>/e Ratio
See here
