Geant4: Electromagnetic Processes 2

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Presentation transcript:

Geant4: Electromagnetic Processes 2 Geant4 cuts Stopping powers and ranges Fluctuations Multiple scattering V.Ivanchenko 16.07.02 Salamanca

Electromagnetic processes Energy spectrum of -electrons  1/T2 Energy spectrum of Bremsstahlung  1/ Huge number of low energy e- and gammas cannot be tracked by any Monte Carlo Cuts should be used V.Ivanchenko 16.07.02 Salamanca

Geant4 cuts No tracking cuts, only production thresholds Cuts can be established to any particle but mandatory cuts on gamma and electrons Thresholds for production secondaries are expressed in range, universal for all media, Range 10 keV gamma in Si  2 cm Range of 10 keV electron in Si  2 microns Energy thresholds for a material is calculated from this cut in range. In 2002 a possibility to set a cut by logical volume will be implemented V.Ivanchenko 16.07.02 Salamanca

G4 cuts Production cuts for a typical G4Ionisation Tc subdivides continues and discrete part: Energy loss -electron production Energy loss can be used for generation of -electrons under the threshold (subcutoff) and for fluorescence and Auger–electrons emission V.Ivanchenko 16.07.02 Salamanca

G3/G4 cuts in Pb/Ar calorimeter Protons 500 MeV G3 Cut 450 keV Ar Pb Ar G4 1.5 mm - 450 keV LAr 2 MeV Pb V.Ivanchenko 16.07.02 Salamanca

Geant4 validation Everyday task for Geant4 team is the validation of the toolkit Comparison with data G3/G4 comparisons Comparison experiments (BaBar, SLAC, Stanford; ATLAS, CERN, Geneve; others) Testing procedures V.Ivanchenko 16.07.02 Salamanca

G3/G4/Data comparison V.Ivanchenko 16.07.02 Salamanca

Remarks about G4 cuts The use of production threshold is mandatory only for ionisation and bremsstahlung process Other processes can use or ignore G4 cuts Alternative mechanism is UserLimits, which can be defined in a given G4LogicalVolume: Maximum step size; Maximum track length; Maximum track time; Minimun kinetic energy; Minimum range; V.Ivanchenko 16.07.02 Salamanca

Stopping powers and ranges At initialization stage dE/dx, R(E), and E(R) tables are calculated for all materials and basic particles e-, e+, -, +, p, pbar At run time dE/dx, R(T), T(R) for hadrons and ions are calculated using scaling Tp=T·mp/m Deuterons V.Ivanchenko 16.07.02 Salamanca

Stopping powers and ranges Scaling is applicable to all types of ions Initialization should be redone if run conditions are changed: New basic particle New material New cut V.Ivanchenko 16.07.02 Salamanca

Straggling At each step of charged particle after calculation of average energy deposition the sampling of energy is performed Three fluctuation models are used Bohr fluctuations Vavilov fluctuations Landau fluctuations V.Ivanchenko 16.07.02 Salamanca

Multiple Scattering Provides step limit Sample transverse displacement at end point of the step Sample scattering angle Model is used in which scattering angles are not small V.Ivanchenko 16.07.02 Salamanca

Conclusion remarks Geant4 electromagnetic model based on new conception: universal cut in range Geant4 is not a frozen program – it is a free toolkit, which allows to implement any variant of cuts and thresholds Geant4 electromagnetic physics is well tested and demonstrates a good quality for HEP applications In some cases Geant4 provide physics which is absent in Geant3, in others – more precise models V.Ivanchenko 16.07.02 Salamanca