source: trunk/source/processes/electromagnetic/adjoint/include/G4AdjointCSMatrix.hh@ 1330

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// $Id: G4AdjointCSMatrix.hh,v 1.4 2009/11/20 10:31:20 ldesorgh Exp $
// GEANT4 tag $Name: geant4-09-03 $
//
/////////////////////////////////////////////////////////////////////////////////
//      Class:          G4AdjointCSMatrix.hh
//      Author:         L. Desorgher
//      Organisation:   SpaceIT GmbH
//      Contract:       ESA contract 21435/08/NL/AT
//      Customer:       ESA/ESTEC
/////////////////////////////////////////////////////////////////////////////////
//
// CHANGE HISTORY
// --------------
//      ChangeHistory: 
//              1st April 2007 creation by L. Desorgher                 
//
//-------------------------------------------------------------
//      Documentation:
//              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 equiavlent 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 recompute after a modification  of the cuts by the user. 
//              
//              
//

#ifndef G4AdjointCSMatrix_h
#define G4AdjointCSMatrix_h 1

#include"globals.hh"
#include<vector>
#include"G4ParticleDefinition.hh"

////////////////////////////////////////////////////////////////////////////////
//
class G4AdjointCSMatrix
{
        ////////////////////////////////
        // Constructors and Destructor
        ////////////////////////////////
public:
        G4AdjointCSMatrix(G4bool aBool);
        ~G4AdjointCSMatrix();

        //////////////
        // Methods  // 
        //////////////
        void Clear();
        void AddData(G4double aPrimEnergy,G4double aCS, std::vector< double>* aLogSecondEnergyVector,
                                                        std::vector< double>* aLogProbVector,size_t n_pro_decade=0);    
        
        G4bool GetData(unsigned int i, G4double& aPrimEnergy,G4double& aCS,G4double& log0, std::vector< double>*& aLogSecondEnergyVector,
                                                                      std::vector< double>*& aLogProbVector,
                                                                      std::vector< size_t>*& aLogProbVectorIndex);
        
        inline std::vector< double>* GetLogPrimEnergyVector(){return &theLogPrimEnergyVector;}
        inline std::vector< double>* GetLogCrossSectionvector(){return &theLogCrossSectionVector;}
        inline G4double GetDlog(){return dlog;}         
        inline G4bool IsScatProjToProjCase(){return is_scat_proj_to_proj_case;} 
        void Write(G4String file_name);
        void Read(G4String file_name);          

private:
        
        // we did first try to use G4PhysicsOrderedVector but they are not general enough for our purpose
        
        std::vector< double> theLogPrimEnergyVector; 
        std::vector< double> theLogCrossSectionVector; //Adjoint Cross sections in function of primary energy
        std::vector< std::vector< double>* > theLogSecondEnergyMatrix;
        std::vector< std::vector< double>* > theLogProbMatrix; //Each column represents the integrated probability of getting a secondary 
                                                                      // in function of their energy 
        std::vector< std::vector< size_t >* > theLogProbMatrixIndex; //index of equidistant LogProb
        std::vector< double> log0Vector;
        
        unsigned int nb_of_PrimEnergy;
        G4bool is_scat_proj_to_proj_case;
        G4double dlog;
        

};
#endif