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26 ////////////////////////////////////////////// << 26 // $Id: G4AdjointCSMatrix.hh 66892 2013-01-17 10:57:59Z gunter $
27 // Class: G4AdjointCSMatrix <<
28 // Author: L. Desorgher <<
29 // Organisation: SpaceIT GmbH <<
30 // 27 //
31 // An adjoint CS matrix is used by the model << 28 /////////////////////////////////////////////////////////////////////////////////
32 // an adjoint secondary (being equivalent to << 29 // Class: G4AdjointCSMatrix.hh
33 // the integration over the energy of the adj << 30 // Author: L. Desorgher
34 // forward primary) of the differential cross << 31 // Organisation: SpaceIT GmbH
35 // discrete process (Ionisation, Brem, PE eff << 32 // Contract: ESA contract 21435/08/NL/AT
36 // model has its own cross section matrix for << 33 // Customer: ESA/ESTEC
37 // is therefore recomputed after a modificati << 34 /////////////////////////////////////////////////////////////////////////////////
>> 35 //
>> 36 // CHANGE HISTORY
>> 37 // --------------
>> 38 // ChangeHistory:
>> 39 // 1st April 2007 creation by L. Desorgher
>> 40 //
>> 41 //-------------------------------------------------------------
>> 42 // Documentation:
>> 43 // An adjoint CS matrix is used by the model of a reverse process to sample an adjoint secondary (being equivalent to a forward primary).
>> 44 // It represents the integration over the energy of the adjoint secondary (therefore the forward primary) of the differential cross section
>> 45 // of the equiavlent forward discrete process (Ionisation, Brem, PE effect, Compton,..) . Each reverse model has its own cross section matrix for a given cut,
>> 46 // material couple. It is therefore recompute after a modification of the cuts by the user.
>> 47 //
>> 48 //
38 // 49 //
39 ////////////////////////////////////////////// <<
40 50
41 #ifndef G4AdjointCSMatrix_h 51 #ifndef G4AdjointCSMatrix_h
42 #define G4AdjointCSMatrix_h 1 52 #define G4AdjointCSMatrix_h 1
43 53
44 #include "globals.hh" << 54 #include"globals.hh"
45 #include "G4ParticleDefinition.hh" << 55 #include<vector>
46 << 56 #include"G4ParticleDefinition.hh"
47 #include <vector> <<
48 57
>> 58 ////////////////////////////////////////////////////////////////////////////////
>> 59 //
49 class G4AdjointCSMatrix 60 class G4AdjointCSMatrix
50 { 61 {
51 public: << 62 ////////////////////////////////
52 G4AdjointCSMatrix(G4bool aBool); << 63 // Constructors and Destructor
53 ~G4AdjointCSMatrix(); << 64 ////////////////////////////////
54 << 65 public:
55 void Clear(); << 66 G4AdjointCSMatrix(G4bool aBool);
56 << 67 ~G4AdjointCSMatrix();
57 void AddData(G4double aPrimEnergy, G4double << 68
58 std::vector<G4double>* aLogSeco << 69 //////////////
59 std::vector<G4double>* aLogProb << 70 // Methods //
60 << 71 //////////////
61 G4bool GetData(unsigned int i, G4double& aPr << 72 void Clear();
62 G4double& log0, std::vector<G << 73 void AddData(G4double aPrimEnergy,G4double aCS, std::vector< double>* aLogSecondEnergyVector,
63 std::vector<G4double>*& aLogP << 74 std::vector< double>* aLogProbVector,size_t n_pro_decade=0);
64 std::vector<std::size_t>*& aL << 75
65 << 76 G4bool GetData(unsigned int i, G4double& aPrimEnergy,G4double& aCS,G4double& log0, std::vector< double>*& aLogSecondEnergyVector,
66 inline std::vector<G4double>* GetLogPrimEner << 77 std::vector< double>*& aLogProbVector,
67 { << 78 std::vector< size_t>*& aLogProbVectorIndex);
68 return &fLogPrimEnergyVector; << 79
69 } << 80 inline std::vector< double>* GetLogPrimEnergyVector(){return &theLogPrimEnergyVector;}
70 << 81 inline std::vector< double>* GetLogCrossSectionvector(){return &theLogCrossSectionVector;}
71 inline std::vector<G4double>* GetLogCrossSec << 82 inline G4double GetDlog(){return dlog;}
72 { << 83 inline G4bool IsScatProjToProjCase(){return is_scat_proj_to_proj_case;}
73 return &fLogCrossSectionVector; << 84 void Write(G4String file_name);
74 } << 85 void Read(G4String file_name);
75 << 86
76 inline G4bool IsScatProjToProj() { return fS << 87 private:
77 << 88
78 void Write(const G4String& file_name); << 89 // we did first try to use G4PhysicsOrderedVector but they are not general enough for our purpose
79 << 90
80 void Read(const G4String& file_name); << 91 std::vector< double> theLogPrimEnergyVector;
81 << 92 std::vector< double> theLogCrossSectionVector; //Adjoint Cross sections in function of primary energy
82 private: << 93 std::vector< std::vector< double>* > theLogSecondEnergyMatrix;
83 std::vector<G4double> fLogPrimEnergyVector; << 94 std::vector< std::vector< double>* > theLogProbMatrix; //Each column represents the integrated probability of getting a secondary
84 // Adjoint Cross sections as functions of pr << 95 // in function of their energy
85 std::vector<G4double> fLogCrossSectionVector << 96 std::vector< std::vector< size_t >* > theLogProbMatrixIndex; //index of equidistant LogProb
86 << 97 std::vector< double> log0Vector;
87 std::vector<std::vector<G4double>*> fLogSeco << 98
88 std::vector<std::vector<G4double>*> fLogProb << 99 unsigned int nb_of_PrimEnergy;
89 // Each column represents the integrated pro << 100 G4bool is_scat_proj_to_proj_case;
90 // getting a secondary << 101 G4double dlog;
91 << 102
92 // index of equidistant LogProb <<
93 std::vector<std::vector<std::size_t>*> fLogP <<
94 std::vector<G4double> fLog0Vector; <<
95 <<
96 std::size_t fNbPrimEnergy = 0; <<
97 103
98 G4bool fScatProjToProj; <<
99 }; 104 };
100 #endif 105 #endif
101 106