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1 // 2 // ******************************************************************** 3 // * License and Disclaimer * 4 // * * 5 // * The Geant4 software is copyright of the Copyright Holders of * 6 // * the Geant4 Collaboration. It is provided under the terms and * 7 // * conditions of the Geant4 Software License, included in the file * 8 // * LICENSE and available at http://cern.ch/geant4/license . These * 9 // * include a list of copyright holders. * 10 // * * 11 // * Neither the authors of this software system, nor their employing * 12 // * institutes,nor the agencies providing financial support for this * 13 // * work make any representation or warranty, express or implied, * 14 // * regarding this software system or assume any liability for its * 15 // * use. Please see the license in the file LICENSE and URL above * 16 // * for the full disclaimer and the limitation of liability. * 17 // * * 18 // * This code implementation is the result of the scientific and * 19 // * technical work of the GEANT4 collaboration. * 20 // * By using, copying, modifying or distributing the software (or * 21 // * any work based on the software) you agree to acknowledge its * 22 // * use in resulting scientific publications, and indicate your * 23 // * acceptance of all terms of the Geant4 Software license. * 24 // ******************************************************************** 25 // 26 //////////////////////////////////////////////////////////////////////////////// 27 // Class: G4AdjointPhotoElectricModel 28 // Author: L. Desorgher 29 // Organisation: SpaceIT GmbH 30 // 31 // Model for the adjoint photo electric process. 32 // Put a higher limit on the CS to avoid a high rate of Inverse Photo e-effect 33 // at low energy. The very high adjoint CS of the reverse photo electric 34 // reaction produce a high rate of reverse photo electric reaction in the inner 35 // side of a shielding for eaxmple, the correction of this occurrence by weight 36 // correction in the StepDoIt method is not statistically sufficient at small 37 // energy. The problem is partially solved by setting a higher CS limit and 38 // compensating it by an extra weight correction factor. However when coupling 39 // it with other reverse processes the reverse photo-electric is still the 40 // source of very occasional high weights that decrease the efficiency of the 41 // computation. A way to solve this problemn is still needed but is difficult 42 // to find as it happens in rare cases but does give a weight that is outside 43 // the normal distribution. (Very Tricky!) 44 // 45 //////////////////////////////////////////////////////////////////////////////// 46 47 #ifndef G4AdjointPhotoElectricModel_h 48 #define G4AdjointPhotoElectricModel_h 1 49 50 #include "globals.hh" 51 #include "G4VEmAdjointModel.hh" 52 53 class G4AdjointPhotoElectricModel : public G4VEmAdjointModel 54 { 55 public: 56 G4AdjointPhotoElectricModel(); 57 ~G4AdjointPhotoElectricModel() override; 58 59 void SampleSecondaries(const G4Track& aTrack, G4bool isScatProjToProj, 60 G4ParticleChange* fParticleChange) override; 61 62 G4double AdjointCrossSection(const G4MaterialCutsCouple* aCouple, 63 G4double primEnergy, 64 G4bool isScatProjToProj) override; 65 66 G4double AdjointCrossSectionPerAtom(const G4Element* anElement, 67 G4double electronEnergy); 68 69 G4AdjointPhotoElectricModel(G4AdjointPhotoElectricModel&) = delete; 70 G4AdjointPhotoElectricModel& operator=( 71 const G4AdjointPhotoElectricModel& right) = delete; 72 73 protected: 74 void CorrectPostStepWeight(G4ParticleChange* fParticleChange, 75 G4double old_weight, G4double adjointPrimKinEnergy, 76 G4double projectileKinEnergy, 77 G4bool isScatProjToProj) override; 78 79 private: 80 void DefineCurrentMaterialAndElectronEnergy( 81 const G4MaterialCutsCouple* aCouple, G4double eEnergy); 82 83 G4double fShellProb[40][40]; 84 G4double fXsec[40]; 85 G4double fTotAdjointCS = 0.; 86 G4double fFactorCSBiasing = 1.; 87 G4double fPreStepAdjointCS = 0.; 88 G4double fPostStepAdjointCS = 0.; 89 G4double fCurrenteEnergy = 0.; 90 91 size_t fIndexElement = 0; 92 }; 93 94 #endif 95