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geant4/source/processes/electromagnetic/adjoint/include/G4AdjointPhotoElectricModel.hh
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// $Id: G4AdjointPhotoElectricModel.hh 66892 2013-01-17 10:57:59Z gunter $
//
/////////////////////////////////////////////////////////////////////////////////
// Module: G4AdjointPhotoElectricModel
// Author: L. Desorgher
// Organisation: SpaceIT GmbH
// Contract: ESA contract 21435/08/NL/AT
// Customer: ESA/ESTEC
/////////////////////////////////////////////////////////////////////////////////
//
// CHANGE HISTORY
// --------------
// ChangeHistory:
// -1 September 2007 creation by L. Desorgher
//
// -January 2009. L. Desorgher
// Put a higher limit on the CS to avoid a high rate of Inverse Photo e- effect at low energy. The very high adjoint CS of the reverse
// photo electric reaction produce a high rate of reverse photo electric reaction in the inner side of a shielding for eaxmple, the correction of this occurence
// by weight correction in the StepDoIt method is not statistically sufficient at small energy. The problem is partially solved by setting an higher CS limit
// and compensating it by an extra weight correction factor. However when coupling it with other reverse processes the reverse photo-electric is still
// the source of very occasional high weight that decrease the efficiency of the computation. A way to solve this problemn is still needed but is difficult
// to find as it happens in rarea case but does give a weighrt that is outside the noemal distribution. (Very Tricky!)
//
// -October 2009 Correction of Element sampling. L. Desorgher
//
//-------------------------------------------------------------
// Documentation:
// Model for the adjoint photo electric process
//
#ifndef G4AdjointPhotoElectricModel_h
#define G4AdjointPhotoElectricModel_h 1
#include "globals.hh"
#include "G4VEmAdjointModel.hh"
#include "G4PEEffectFluoModel.hh"
class G4AdjointPhotoElectricModel: public G4VEmAdjointModel
{
public:
G4AdjointPhotoElectricModel();
~G4AdjointPhotoElectricModel();
virtual void SampleSecondaries(const G4Track& aTrack,
G4bool IsScatProjToProjCase,
G4ParticleChange* fParticleChange);
virtual G4double AdjointCrossSection(const G4MaterialCutsCouple* aCouple,
G4double primEnergy,
G4bool IsScatProjToProjCase);
virtual G4double GetAdjointCrossSection(const G4MaterialCutsCouple* aCouple,
G4double primEnergy,
G4bool IsScatProjToProjCase);
G4double AdjointCrossSectionPerAtom(const G4Element* anElement,G4double electronEnergy);
inline void SetTheDirectPEEffectModel(G4PEEffectFluoModel* aModel){theDirectPEEffectModel = aModel;
DefineDirectEMModel(aModel);}
virtual void CorrectPostStepWeight(G4ParticleChange* fParticleChange,
G4double old_weight,
G4double adjointPrimKinEnergy,
G4double projectileKinEnergy,
G4bool IsScatProjToProjCase);
private:
G4double xsec[40];
G4double totAdjointCS;
G4double totBiasedAdjointCS;
G4double factorCSBiasing;
G4double pre_step_AdjointCS;
G4double post_step_AdjointCS;
G4double shell_prob[40][40];
G4PEEffectFluoModel* theDirectPEEffectModel;
size_t index_element;
G4double current_eEnergy;
private:
void DefineCurrentMaterialAndElectronEnergy(const G4MaterialCutsCouple* aCouple,
G4double eEnergy);
};
#endif