G4AdjointCSMatrix.hh

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// $Id: G4AdjointCSMatrix.hh 66892 2013-01-17 10:57:59Z gunter $
//
/////////////////////////////////////////////////////////////////////////////////
//      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