// // ******************************************************************** // * License and Disclaimer * // * * // * The Geant4 software is copyright of the Copyright Holders of * // * the Geant4 Collaboration. It is provided under the terms and * // * conditions of the Geant4 Software License, included in the file * // * LICENSE and available at http://cern.ch/geant4/license . These * // * include a list of copyright holders. * // * * // * Neither the authors of this software system, nor their employing * // * institutes,nor the agencies providing financial support for this * // * work make any representation or warranty, express or implied, * // * regarding this software system or assume any liability for its * // * use. Please see the license in the file LICENSE and URL above * // * for the full disclaimer and the limitation of liability. * // * * // * This code implementation is the result of the scientific and * // * technical work of the GEANT4 collaboration. * // * By using, copying, modifying or distributing the software (or * // * any work based on the software) you agree to acknowledge its * // * use in resulting scientific publications, and indicate your * // * acceptance of all terms of the Geant4 Software license. * // ******************************************************************** // //////////////////////////////////////////////////////////////////////////////// // Class: G4AdjointPhotoElectricModel // Author: L. Desorgher // Organisation: SpaceIT GmbH // // Model for the adjoint photo electric process. // 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 occurrence by weight // correction in the StepDoIt method is not statistically sufficient at small // energy. The problem is partially solved by setting a 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 weights 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 rare cases but does give a weight that is outside // the normal distribution. (Very Tricky!) // //////////////////////////////////////////////////////////////////////////////// #ifndef G4AdjointPhotoElectricModel_h #define G4AdjointPhotoElectricModel_h 1 #include "globals.hh" #include "G4VEmAdjointModel.hh" class G4AdjointPhotoElectricModel : public G4VEmAdjointModel { public: G4AdjointPhotoElectricModel(); ~G4AdjointPhotoElectricModel() override; void SampleSecondaries(const G4Track& aTrack, G4bool isScatProjToProj, G4ParticleChange* fParticleChange) override; G4double AdjointCrossSection(const G4MaterialCutsCouple* aCouple, G4double primEnergy, G4bool isScatProjToProj) override; G4double AdjointCrossSectionPerAtom(const G4Element* anElement, G4double electronEnergy); G4AdjointPhotoElectricModel(G4AdjointPhotoElectricModel&) = delete; G4AdjointPhotoElectricModel& operator=( const G4AdjointPhotoElectricModel& right) = delete; protected: void CorrectPostStepWeight(G4ParticleChange* fParticleChange, G4double old_weight, G4double adjointPrimKinEnergy, G4double projectileKinEnergy, G4bool isScatProjToProj) override; private: void DefineCurrentMaterialAndElectronEnergy( const G4MaterialCutsCouple* aCouple, G4double eEnergy); G4double fShellProb[40][40]; G4double fXsec[40]; G4double fTotAdjointCS = 0.; G4double fFactorCSBiasing = 1.; G4double fPreStepAdjointCS = 0.; G4double fPostStepAdjointCS = 0.; G4double fCurrenteEnergy = 0.; size_t fIndexElement = 0; }; #endif