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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: G4AdjointCSMatrix 28 // Author: L. Desorgher 29 // Organisation: SpaceIT GmbH 30 // 31 // An adjoint CS matrix is used by the model of a reverse process to sample 32 // an adjoint secondary (being equivalent to a forward primary). It represents 33 // the integration over the energy of the adjoint secondary (therefore the 34 // forward primary) of the differential cross section of the equivalent forward 35 // discrete process (Ionisation, Brem, PE effect, Compton,..). Each reverse 36 // model has its own cross section matrix for a given cut, material couple. It 37 // is therefore recomputed after a modification of the cuts by the user. 38 // 39 //////////////////////////////////////////////////////////////////////////////// 40 41 #ifndef G4AdjointCSMatrix_h 42 #define G4AdjointCSMatrix_h 1 43 44 #include "globals.hh" 45 #include "G4ParticleDefinition.hh" 46 47 #include <vector> 48 49 class G4AdjointCSMatrix 50 { 51 public: 52 G4AdjointCSMatrix(G4bool aBool); 53 ~G4AdjointCSMatrix(); 54 55 void Clear(); 56 57 void AddData(G4double aPrimEnergy, G4double aCS, 58 std::vector<G4double>* aLogSecondEnergyVector, 59 std::vector<G4double>* aLogProbVector, std::size_t n_pro_decade = 0); 60 61 G4bool GetData(unsigned int i, G4double& aPrimEnergy, G4double& aCS, 62 G4double& log0, std::vector<G4double>*& aLogSecondEnergyVector, 63 std::vector<G4double>*& aLogProbVector, 64 std::vector<std::size_t>*& aLogProbVectorIndex); 65 66 inline std::vector<G4double>* GetLogPrimEnergyVector() 67 { 68 return &fLogPrimEnergyVector; 69 } 70 71 inline std::vector<G4double>* GetLogCrossSectionvector() 72 { 73 return &fLogCrossSectionVector; 74 } 75 76 inline G4bool IsScatProjToProj() { return fScatProjToProj; } 77 78 void Write(const G4String& file_name); 79 80 void Read(const G4String& file_name); 81 82 private: 83 std::vector<G4double> fLogPrimEnergyVector; 84 // Adjoint Cross sections as functions of primary energy 85 std::vector<G4double> fLogCrossSectionVector; 86 87 std::vector<std::vector<G4double>*> fLogSecondEnergyMatrix; 88 std::vector<std::vector<G4double>*> fLogProbMatrix; 89 // Each column represents the integrated probability of 90 // getting a secondary 91 92 // index of equidistant LogProb 93 std::vector<std::vector<std::size_t>*> fLogProbMatrixIndex; 94 std::vector<G4double> fLog0Vector; 95 96 std::size_t fNbPrimEnergy = 0; 97 98 G4bool fScatProjToProj; 99 }; 100 #endif 101