Validation of EM Part of Geant4
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1 Validation of EM Part of Geant4 February 22, Geant4 Work Shop Tsuneyoshi Kamae/Tsunefumi Mizuno 1
2 Purpose and Plan of this Talk We have validated EM processes in Geant4 important for gamma-ray satellite GLAST. Energy range of GLAST is 20 MeV GeV. So we need to validate physics processed down to ~10 MeV and lower. Particle Ionization Energy Loss in Matters Bethe-Bloch Formula (pp. 3-5) Landau Distribution (pp. 3-5) Range (p. 6) Processed related to electromagnetic shower Pair creation (pp. 8-9) Bremsstrahlung (p. 10) Moller scattering/bhabha scattering (pp ) Comparison of shower profile with experimental data (pp ) Comparison of shower profile with EGS4 (pp ) We use Geant4 2.0 Tracker (Si, Pb) Calorimeter (CsI) 2
3 Ionization Energy loss in matters Shoot proton/electron in Pb and Si. Cutoff Length: 0.4mm(e-), 0.1mm(others) Thick absorber: Bethe-Bloch formula Thin absorber: Landau distribution Check mean energy loss (thick absorber), shape and 3 most probable energy loss (thin absorber).
4 Bethe-Bloch formula for protons Geant4 well reproduces ionization energy loss in thick Si and Pb of proton down to 10 MeV 4
5 Landau Distribution for protons and electrons protons electrons Fluctuation of energy loss and the most probable value in thin Si and Pb are appropriate. 5
6 Range of protons Shoot protons of 200 MeV and 1 GeV in CsI, Pb and W Compare the results with NIST data: ( ysrefdata/star/text/conte nts.html) Show good agreement within 0.6%. 6
7 Processes related to EM shower Pair creation (pp. 8-9) (and compton scattering and photo-electric effect) Bremsstrahlung (p. 10) Moller scattering (pp ) Bhabha scattering (pp ) e- Cutoff 0.04mm(e-) 0.01mm(others) We need to validate these processes, especially in low-energy, since Pair creation and EM shower are key processes to determine gamma-ray energy and direction in the GLAST. Low energy electrons may suffer large-angle scattering and cause trigger in the GLAST. Tracker (Si-Strip detectors) Calorimeter (CsI scintillator) 7
8 Pair creation cross section Compare the cross section in Pb calculated by Geant4 with that of a reference ( srefdata/xcom/text) Geant4 correctly calculates cross section down to ~100 kev 8
9 Pair creation-angular distribution of emitted electrons Shoot 20 MeV gammas into Pb absorber (10% RL) Compare the angular distribution of generated e- with that of theoretical formula Events/Bin e- 4 MeV Theta [rad] e- 18 MeV We found discrepancies for low energy electrons and fixed the code Events/Bin Theta [rad]
10 Bremsstrahlung -- angular distribution of generated photons Shoot 20 MeV e- into Pb absorber (10% RL) Compare the angular distribution of generated photons with that of theoretical formula gamma 2 MeV gamma 6 MeV Geant4 well reproduces the angular distribution of photons generated via bremsstrahlung down to ~1 MeV gamma 10 MeV 10
11 Moller/Bhabha scattering (scattering with e-/e+) Shoot e- of 20 MeV and 100 MeV into Pb absorber (1% RL) Compare the angular distribution of scattered electrons with that of theoretical formula 11
12 Moller scattering (with e-) Bhabha scattering (with e+) Theoretical furmula Geant4 20 MeV 20 MeV 100 MeV 100 MeV G4 well reproduces the theoretical formula down to MeV
13 EM shower profile Crannell experiment (1) Cranell experimtns: Carol Jo Crannell, et al., Phys. Rev. 184 (1969) 426 shoot 1GeV e- into water tank (10 rings and 11 layers) Compare the G4 results with that of experimental data and EGS4 (Professor Nelthon and Liu). 13
14 EM shower profile Crannell experiment (2) longitudinal profile lateral profiles Shower profile of G4 is narrower than that of experiment and EGS4 14
15 EM shower in Pb layers (1) To investigate the EM shower profile in the GLAST Tracker, we constructed 10 Pb layers(0.1rl each) with air (3cm). The radius is 0.2 Moliere radius (core of shower) Geant4 EGS4 20 MeV, longitudinal profile Pb air lateral profiles 15
16 EM shower in Pb and air (2) Geant4 EGS4 500 MeV, longitudinal profile Geant4 EGS4 5 GeV, longitudinal profile lateral profiles lateral profiles Energy deposition is higher in Geant4 (low energy region) Geant4 shows narrower shower profile (and could not be solved by fixing the angular distribution of pair creation) 16
17 Effect of cutoff energy (length) 0.4mm, 0.04mm (e-), 0.1mm, 0.01mm(others) Geant4 EGS4 The discrepancy can not be attributed to cutoff length (energy) The reason of the narrower shower profile is unrevealed. 17
18 Summary We have validated EM part of Geant4 (2.0). Energy loss in matters is well simulated down to ~10 MeV. Angular distribution of pair-created e- was found to be inappropriate and fixed. Cross section of pair creation, angular distribution of bremsstrahlung/moller scattering/bhabha scattering were validated down to ~10 MeV. Shower profile of G4 is slightly narrower than that of experimental data and EGS4. The reason of this is unknown. 18
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