// // ******************************************************************** // * 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: G4AdjointCSMatrix // Author: L. Desorgher // Organisation: SpaceIT GmbH // // An adjoint CS matrix is used by the model of a reverse process to sample // an adjoint secondary (being equivalent to a forward primary). It represents // the integration over the energy of the adjoint secondary (therefore the // forward primary) of the differential cross section of the equivalent forward // discrete process (Ionisation, Brem, PE effect, Compton,..). Each reverse // model has its own cross section matrix for a given cut, material couple. It // is therefore recomputed after a modification of the cuts by the user. // //////////////////////////////////////////////////////////////////////////////// #ifndef G4AdjointCSMatrix_h #define G4AdjointCSMatrix_h 1 #include "globals.hh" #include "G4ParticleDefinition.hh" #include class G4AdjointCSMatrix { public: G4AdjointCSMatrix(G4bool aBool); ~G4AdjointCSMatrix(); void Clear(); void AddData(G4double aPrimEnergy, G4double aCS, std::vector* aLogSecondEnergyVector, std::vector* aLogProbVector, std::size_t n_pro_decade = 0); G4bool GetData(unsigned int i, G4double& aPrimEnergy, G4double& aCS, G4double& log0, std::vector*& aLogSecondEnergyVector, std::vector*& aLogProbVector, std::vector*& aLogProbVectorIndex); inline std::vector* GetLogPrimEnergyVector() { return &fLogPrimEnergyVector; } inline std::vector* GetLogCrossSectionvector() { return &fLogCrossSectionVector; } inline G4bool IsScatProjToProj() { return fScatProjToProj; } void Write(const G4String& file_name); void Read(const G4String& file_name); private: std::vector fLogPrimEnergyVector; // Adjoint Cross sections as functions of primary energy std::vector fLogCrossSectionVector; std::vector*> fLogSecondEnergyMatrix; std::vector*> fLogProbMatrix; // Each column represents the integrated probability of // getting a secondary // index of equidistant LogProb std::vector*> fLogProbMatrixIndex; std::vector fLog0Vector; std::size_t fNbPrimEnergy = 0; G4bool fScatProjToProj; }; #endif