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0001 // 0002 // ******************************************************************** 0003 // * License and Disclaimer * 0004 // * * 0005 // * The Geant4 software is copyright of the Copyright Holders of * 0006 // * the Geant4 Collaboration. It is provided under the terms and * 0007 // * conditions of the Geant4 Software License, included in the file * 0008 // * LICENSE and available at http://cern.ch/geant4/license . These * 0009 // * include a list of copyright holders. * 0010 // * * 0011 // * Neither the authors of this software system, nor their employing * 0012 // * institutes,nor the agencies providing financial support for this * 0013 // * work make any representation or warranty, express or implied, * 0014 // * regarding this software system or assume any liability for its * 0015 // * use. Please see the license in the file LICENSE and URL above * 0016 // * for the full disclaimer and the limitation of liability. * 0017 // * * 0018 // * This code implementation is the result of the scientific and * 0019 // * technical work of the GEANT4 collaboration. * 0020 // * By using, copying, modifying or distributing the software (or * 0021 // * any work based on the software) you agree to acknowledge its * 0022 // * use in resulting scientific publications, and indicate your * 0023 // * acceptance of all terms of the Geant4 Software license. * 0024 // ******************************************************************** 0025 // 0026 //////////////////////////////////////////////////////////////////////////////// 0027 // Class: G4AdjointBremsstrahlungModel 0028 // Author: L. Desorgher 0029 // Organisation: SpaceIT GmbH 0030 //////////////////////////////////////////////////////////////////////////////// 0031 // 0032 // Adjoint Model for e- Bremsstrahlung.Adapted from G4eBremsstrahlungModel 0033 // Use of a simple biased differential cross section (C(Z)/Egamma) allowing a 0034 // rapid computation of adjoint CS and rapid sampling of adjoint secondaries. 0035 // In this way cross section matrices are not used anymore, avoiding a long 0036 // computation of adjoint brem cross section matrices for each material 0037 // at initialisation. This mode can be switched on/off by selecting 0038 // SetUseMatrix(false)/ SetUseMatrix(true) in the constructor. 0039 // 0040 //------------------------------------------------------------- 0041 0042 #ifndef G4AdjointBremsstrahlungModel_h 0043 #define G4AdjointBremsstrahlungModel_h 1 0044 0045 #include "globals.hh" 0046 #include "G4VEmAdjointModel.hh" 0047 0048 class G4AdjointCSManager; 0049 class G4EmModelManager; 0050 class G4ParticleDefinition; 0051 0052 class G4AdjointBremsstrahlungModel : public G4VEmAdjointModel 0053 { 0054 public: 0055 explicit G4AdjointBremsstrahlungModel(G4VEmModel* aModel); 0056 0057 G4AdjointBremsstrahlungModel(); 0058 0059 ~G4AdjointBremsstrahlungModel() override; 0060 0061 void SampleSecondaries(const G4Track& aTrack, G4bool isScatProjToProj, 0062 G4ParticleChange* fParticleChange) override; 0063 0064 void RapidSampleSecondaries(const G4Track& aTrack, G4bool isScatProjToProj, 0065 G4ParticleChange* fParticleChange); 0066 0067 G4double DiffCrossSectionPerVolumePrimToSecond( 0068 const G4Material* aMaterial, 0069 G4double kinEnergyProj, // kinetic energy of the primary particle before 0070 // the interaction 0071 G4double kinEnergyProd // kinetic energy of the secondary particle 0072 ) override; 0073 0074 G4double AdjointCrossSection(const G4MaterialCutsCouple* aCouple, 0075 G4double primEnergy, 0076 G4bool isScatProjToProj) override; 0077 0078 G4AdjointBremsstrahlungModel(G4AdjointBremsstrahlungModel&) = delete; 0079 G4AdjointBremsstrahlungModel& operator=( 0080 const G4AdjointBremsstrahlungModel& right) = delete; 0081 0082 private: 0083 void Initialize(); 0084 0085 G4EmModelManager* fEmModelManagerForFwdModels; 0086 G4AdjointCSManager* fCSManager; 0087 G4ParticleDefinition* fElectron; 0088 G4ParticleDefinition* fGamma; 0089 0090 G4double fLastCZ = 0.; 0091 0092 G4bool fIsDirectModelInitialised = false; 0093 }; 0094 0095 #endif
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