source: trunk/source/processes/electromagnetic/adjoint/include/G4AdjointPhotoElectricModel.hh

Last change on this file was 1337, checked in by garnier, 14 years ago

tag geant4.9.4 beta 1 + modifs locales

File size: 4.8 KB
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25//
26// $Id: G4AdjointPhotoElectricModel.hh,v 1.4 2009/11/20 10:31:20 ldesorgh Exp $
27// GEANT4 tag $Name: geant4-09-04-beta-01 $
28//
29/////////////////////////////////////////////////////////////////////////////////
30//      Module:         G4AdjointPhotoElectricModel
31//      Author:         L. Desorgher
32//      Organisation:   SpaceIT GmbH
33//      Contract:       ESA contract 21435/08/NL/AT
34//      Customer:       ESA/ESTEC
35/////////////////////////////////////////////////////////////////////////////////
36//
37// CHANGE HISTORY
38// --------------
39//      ChangeHistory:
40//              -1 September 2007 creation by L. Desorgher 
41//             
42//              -January 2009. L. Desorgher     
43//               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
44//               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
45//               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
46//               and compensating it by an extra weight correction factor. However when  coupling it with other reverse  processes the reverse photo-electric is still
47//               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
48//               to find as it happens in rarea case but does give a weighrt that is outside the noemal distribution. (Very Tricky!) 
49//             
50//              -October 2009   Correction of Element sampling. L. Desorgher           
51//
52//-------------------------------------------------------------
53//      Documentation:
54//              Model for the adjoint photo electric process
55//
56#ifndef G4AdjointPhotoElectricModel_h
57#define G4AdjointPhotoElectricModel_h 1
58
59
60#include "globals.hh"
61#include "G4VEmAdjointModel.hh"
62#include "G4PEEffectModel.hh"
63class G4AdjointPhotoElectricModel: public G4VEmAdjointModel
64
65{
66public:
67
68  G4AdjointPhotoElectricModel();
69  ~G4AdjointPhotoElectricModel();
70 
71 
72 
73  virtual void SampleSecondaries(const G4Track& aTrack,
74                                G4bool IsScatProjToProjCase,
75                                G4ParticleChange* fParticleChange);
76  virtual G4double AdjointCrossSection(const G4MaterialCutsCouple* aCouple,
77                                G4double primEnergy,
78                                G4bool IsScatProjToProjCase);
79                               
80  G4double AdjointCrossSectionPerAtom(const G4Element*  anElement,G4double electronEnergy);
81 
82 
83 
84  inline void SetTheDirectPEEffectModel(G4PEEffectModel* aModel){theDirectPEEffectModel = aModel; 
85                                                       DefineDirectEMModel(aModel);}                                 
86 
87  virtual void CorrectPostStepWeight(G4ParticleChange* fParticleChange, 
88                                     G4double old_weight, 
89                                     G4double adjointPrimKinEnergy, 
90                                     G4double projectileKinEnergy,
91                                     G4bool IsScatProjToProjCase);
92 
93 
94private:
95  G4double  xsec[40];
96  G4double  totAdjointCS;
97  G4double  totBiasedAdjointCS;
98  G4double  factorCSBiasing;
99  G4double  pre_step_AdjointCS;
100  G4double  post_step_AdjointCS;
101 
102 
103  G4double  shell_prob[40][40];
104 
105 
106  G4PEEffectModel* theDirectPEEffectModel;
107  size_t index_element;
108  G4double current_eEnergy;
109 
110 
111private: 
112  void DefineCurrentMaterialAndElectronEnergy(const G4MaterialCutsCouple* aCouple,
113                                G4double eEnergy);
114   
115};
116
117#endif
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