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geant4/source/processes/electromagnetic/standard/include/G4PhotoElectricEffect.hh
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//
// ********************************************************************
// * DISCLAIMER *
// * *
// * The following disclaimer summarizes all the specific disclaimers *
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// * work make any representation or warranty, express or implied, *
// * regarding this software system or assume any liability for its *
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// * This code implementation is the intellectual property of the *
// * GEANT4 collaboration. *
// * By copying, distributing or modifying the Program (or any work *
// * based on the Program) you indicate your acceptance of this *
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//
//
// $Id: G4PhotoElectricEffect.hh,v 1.18 2005/05/04 16:16:12 vnivanch Exp $
// GEANT4 tag $Name: geant4-08-00 $
//
//
//------------------ G4PhotoElectricEffect physics process ------------------
// by Michel Maire, 24 May 1996
//
// 12-06-96, Added SelectRandomAtom() method and new data member
// for cumulative total cross section, by M.Maire
// 21-06-96, SetCuts implementation, M.Maire
// 17-09-96, Dynamic array PartialSumSigma
// split ComputeBindingEnergy(), M.Maire
// 08-01-97, crossection table + meanfreepath table, M.Maire
// 13-03-97, adapted for the new physics scheme, M.Maire
// 13-08-98, new methods SetBining() PrintInfo()
// 17-11-98, use table of atomic shells in PostStepDoIt, mma
// 06-01-99, Sandia crossSection below 50 keV, V.Grichine mma
// 03-08-01, new methods Store/Retrieve PhysicsTable (mma)
// 06-08-01, BuildThePhysicsTable() called from constructor (mma)
// 19-09-01, come back to previous process name "phot"
// 20-09-01, DoIt: fminimalEnergy = 1*eV (mma)
// 01-10-01, come back to BuildPhysicsTable(const G4ParticleDefinition&)
// 10-01-02, moved few function from icc to cc
// 17-04-02, Keep only Sandia crossSections. Remove BuildPhysicsTables.
// Simplify public interface (mma)
// 29-04-02, Generate theta angle of the photoelectron from Sauter-Gavrila
// distribution (mma)
// 13-08-04, suppress icc file; make public ComputeCrossSectionPerAtom() (mma)
// 21-04-05, Redesign - use G4VEmProcess interface (V.Ivanchenko)
// 02-05-05, move ParticleChange actions in model (mma)
// 04-05-05, Make class to be default (V.Ivanchenko)
// -----------------------------------------------------------------------------
// class description
//
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
#ifndef G4PhotoElectricEffect_h
#define G4PhotoElectricEffect_h 1
#include "globals.hh"
#include "G4VEmProcess.hh"
#include "G4Gamma.hh"
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
class G4ParticleDefinition;
class G4VEmModel;
class G4MaterialCutsCouple;
class G4DynamicParticle;
class G4PhotoElectricEffect : public G4VEmProcess
{
public: // with description
G4PhotoElectricEffect(const G4String& processName ="phot",
G4ProcessType type = fElectromagnetic);
virtual ~G4PhotoElectricEffect();
// true for Gamma only.
G4bool IsApplicable(const G4ParticleDefinition&);
// Print few lines of informations about the process: validity range,
void PrintInfo();
protected:
void InitialiseProcess(const G4ParticleDefinition*);
std::vector<G4DynamicParticle*>* SecondariesPostStep(
G4VEmModel*,
const G4MaterialCutsCouple*,
const G4DynamicParticle*);
private:
G4bool isInitialised;
};
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
inline G4bool G4PhotoElectricEffect::IsApplicable(const G4ParticleDefinition& p)
{
return (&p == G4Gamma::Gamma());
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
inline std::vector<G4DynamicParticle*>* G4PhotoElectricEffect::SecondariesPostStep(
G4VEmModel* model,
const G4MaterialCutsCouple* couple,
const G4DynamicParticle* dp)
{
return model->SampleSecondaries(couple, dp);
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
#endif