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9.6.p02
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geant4_9_6_p02
source
processes
electromagnetic
standard
src
G4PhotoElectricEffect.cc
Go to the documentation of this file.
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//
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// ********************************************************************
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// * License and Disclaimer *
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// * *
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// * The Geant4 software is copyright of the Copyright Holders of *
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// * the Geant4 Collaboration. It is provided under the terms and *
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// * conditions of the Geant4 Software License, included in the file *
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// * LICENSE and available at http://cern.ch/geant4/license . These *
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// * include a list of copyright holders. *
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// * *
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// * Neither the authors of this software system, nor their employing *
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// * institutes,nor the agencies providing financial support for this *
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// * work make any representation or warranty, express or implied, *
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// * regarding this software system or assume any liability for its *
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// * use. Please see the license in the file LICENSE and URL above *
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// * for the full disclaimer and the limitation of liability. *
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// * *
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// * This code implementation is the result of the scientific and *
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// * technical work of the GEANT4 collaboration. *
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// * By using, copying, modifying or distributing the software (or *
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// * any work based on the software) you agree to acknowledge its *
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// * use in resulting scientific publications, and indicate your *
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// * acceptance of all terms of the Geant4 Software license. *
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// ********************************************************************
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//
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// $Id$
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//
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//
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//------------------ G4PhotoElectricEffect physics process ---------------------
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// by Michel Maire, 24 May 1996
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//
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// 12-06-96, Added SelectRandomAtom() method, by M.Maire
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// 21-06-96, SetCuts implementation, M.Maire
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// 17-09-96, PartialSumSigma(i)
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// split of ComputeBindingEnergy, M.Maire
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// 08-01-97, crossection table + meanfreepath table, M.Maire
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// 13-03-97, adapted for the new physics scheme, M.Maire
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// 28-03-97, protection in BuildPhysicsTable, M.Maire
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// 04-06-98, in DoIt, secondary production condition:
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// range > std::min(threshold,safety)
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// 13-08-98, new methods SetBining() PrintInfo()
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// 17-11-98, use table of Atomic shells in PostStepDoIt
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// 06-01-99, use Sandia crossSection below 50 keV, V.Grichine mma
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// 20-05-99, protection against very low energy photons ,L.Urban
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// 08-06-99, removed this above protection from the DoIt. mma
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// 21-06-00, in DoIt, killing photon: aParticleChange.SetEnergyChange(0.); mma
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// 22-06-00, in DoIt, absorbe very low energy photon (back to 20-05-99); mma
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// 22-02-01, back to 08-06-99 after correc in SandiaTable (materials-V03-00-05)
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// 28-05-01, V.Ivanchenko minor changes to provide ANSI -wall compilation
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// 13-07-01, DoIt: suppression of production cut of the electron (mma)
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// 06-08-01, new methods Store/Retrieve PhysicsTable (mma)
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// 06-08-01, BuildThePhysicsTable() called from constructor (mma)
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// 17-09-01, migration of Materials to pure STL (mma)
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// 20-09-01, DoIt: fminimalEnergy of generated electron = 1*eV (mma)
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// 01-10-01, come back to BuildPhysicsTable(const G4ParticleDefinition&)
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// 10-01-02, moved few function from icc to cc
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// 17-04-02, Keep only Sandia crossSections. Remove BuildPhysicsTables.
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// Simplify public interface (mma)
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// 29-04-02, Generate theta angle of the photoelectron from Sauter-Gavrila
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// distribution (mma)
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// 15-01-03, photoelectron theta ditribution : return costeta=1 if gamma>5
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// (helmut burkhardt)
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// 21-04-05 Migrate to model interface and inherit
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// from G4VEmProcess (V.Ivanchenko)
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// 04-05-05, Make class to be default (V.Ivanchenko)
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// 09-08-06, add SetModel(G4VEmModel*) (mma)
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// 12-09-06, move SetModel(G4VEmModel*) in G4VEmProcess (mma)
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// -----------------------------------------------------------------------------
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#include "
G4PhotoElectricEffect.hh
"
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#include "
G4SystemOfUnits.hh
"
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#include "
G4PEEffectFluoModel.hh
"
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#include "
G4Electron.hh
"
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//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
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using namespace
std;
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G4PhotoElectricEffect::G4PhotoElectricEffect
(
const
G4String
& processName,
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G4ProcessType
type):
G4VEmProcess
(processName, type),
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isInitialised(false)
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{
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SetBuildTableFlag
(
false
);
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SetSecondaryParticle
(
G4Electron::Electron
());
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SetProcessSubType
(
fPhotoElectricEffect
);
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SetMinKinEnergyPrim
(200*
keV
);
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}
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//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
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G4PhotoElectricEffect::~G4PhotoElectricEffect
()
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{}
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//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
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G4bool
G4PhotoElectricEffect::IsApplicable
(
const
G4ParticleDefinition
&
p
)
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{
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return
(&p ==
G4Gamma::Gamma
());
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}
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//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
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void
G4PhotoElectricEffect::InitialiseProcess
(
const
G4ParticleDefinition
*)
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{
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if
(!isInitialised) {
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isInitialised =
true
;
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if
(!
EmModel
(1)) {
SetEmModel
(
new
G4PEEffectFluoModel
(),1); }
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EmModel
(1)->
SetLowEnergyLimit
(
MinKinEnergy
());
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EmModel
(1)->
SetHighEnergyLimit
(
MaxKinEnergy
());
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AddEmModel
(1,
EmModel
(1));
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}
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}
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//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
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void
G4PhotoElectricEffect::PrintInfo
()
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{}
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//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
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