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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: G4AdjointCSMatrix 0028 // Author: L. Desorgher 0029 // Organisation: SpaceIT GmbH 0030 // 0031 // An adjoint CS matrix is used by the model of a reverse process to sample 0032 // an adjoint secondary (being equivalent to a forward primary). It represents 0033 // the integration over the energy of the adjoint secondary (therefore the 0034 // forward primary) of the differential cross section of the equivalent forward 0035 // discrete process (Ionisation, Brem, PE effect, Compton,..). Each reverse 0036 // model has its own cross section matrix for a given cut, material couple. It 0037 // is therefore recomputed after a modification of the cuts by the user. 0038 // 0039 //////////////////////////////////////////////////////////////////////////////// 0040 0041 #ifndef G4AdjointCSMatrix_h 0042 #define G4AdjointCSMatrix_h 1 0043 0044 #include "globals.hh" 0045 #include "G4ParticleDefinition.hh" 0046 0047 #include <vector> 0048 0049 class G4AdjointCSMatrix 0050 { 0051 public: 0052 G4AdjointCSMatrix(G4bool aBool); 0053 ~G4AdjointCSMatrix(); 0054 0055 void Clear(); 0056 0057 void AddData(G4double aPrimEnergy, G4double aCS, 0058 std::vector<double>* aLogSecondEnergyVector, 0059 std::vector<double>* aLogProbVector, size_t n_pro_decade = 0); 0060 0061 G4bool GetData(unsigned int i, G4double& aPrimEnergy, G4double& aCS, 0062 G4double& log0, std::vector<double>*& aLogSecondEnergyVector, 0063 std::vector<double>*& aLogProbVector, 0064 std::vector<size_t>*& aLogProbVectorIndex); 0065 0066 inline std::vector<double>* GetLogPrimEnergyVector() 0067 { 0068 return &fLogPrimEnergyVector; 0069 } 0070 0071 inline std::vector<double>* GetLogCrossSectionvector() 0072 { 0073 return &fLogCrossSectionVector; 0074 } 0075 0076 inline G4bool IsScatProjToProj() { return fScatProjToProj; } 0077 0078 void Write(G4String file_name); 0079 0080 void Read(G4String file_name); 0081 0082 private: 0083 std::vector<double> fLogPrimEnergyVector; 0084 // Adjoint Cross sections as functions of primary energy 0085 std::vector<double> fLogCrossSectionVector; 0086 0087 std::vector<std::vector<double>*> fLogSecondEnergyMatrix; 0088 std::vector<std::vector<double>*> fLogProbMatrix; 0089 // Each column represents the integrated probability of 0090 // getting a secondary 0091 0092 // index of equidistant LogProb 0093 std::vector<std::vector<size_t>*> fLogProbMatrixIndex; 0094 std::vector<double> fLog0Vector; 0095 0096 size_t fNbPrimEnergy = 0; 0097 0098 G4bool fScatProjToProj; 0099 }; 0100 #endif
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