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geant4/source/processes/electromagnetic/adjoint/include/G4AdjointCSMatrix.hh
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//
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//
/////////////////////////////////////////////////////////////////////////////////
// Module: G4AdjointCSMatrix.hh
// Author: L. Desorgher
// Date: 1st April 2007
// Organisation: SpaceIT GmbH
// 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< G4double>* aLogSecondEnergyVector,
std::vector< G4double>* aLogProbVector,size_t n_pro_decade=0);
bool GetData(unsigned int i, G4double& aPrimEnergy,G4double& aCS,G4double& log0, std::vector< G4double>*& aLogSecondEnergyVector,
std::vector< G4double>*& aLogProbVector,
std::vector< size_t>*& aLogProbVectorIndex);
inline std::vector< G4double >* GetLogPrimEnergyVector(){return &theLogPrimEnergyVector;}
inline std::vector< G4double >* 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< G4double > theLogPrimEnergyVector;
std::vector< G4double > theLogCrossSectionVector; //Adjoint Cross sections in function of primary energy
std::vector< std::vector< G4double >* > theLogSecondEnergyMatrix;
std::vector< std::vector< G4double >* > 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 euqidistant LogProb
std::vector< G4double > log0Vector;
unsigned int nb_of_PrimEnergy;
G4bool is_scat_proj_to_proj_case;
G4double dlog;
};
#endif