source: trunk/source/processes/electromagnetic/adjoint/include/G4AdjointCSMatrix.hh@ 1192

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1//
2// ********************************************************************
3// * License and Disclaimer *
4// * *
5// * The Geant4 software is copyright of the Copyright Holders of *
6// * the Geant4 Collaboration. It is provided under the terms and *
7// * conditions of the Geant4 Software License, included in the file *
8// * LICENSE and available at http://cern.ch/geant4/license . These *
9// * include a list of copyright holders. *
10// * *
11// * Neither the authors of this software system, nor their employing *
12// * institutes,nor the agencies providing financial support for this *
13// * work make any representation or warranty, express or implied, *
14// * regarding this software system or assume any liability for its *
15// * use. Please see the license in the file LICENSE and URL above *
16// * for the full disclaimer and the limitation of liability. *
17// * *
18// * This code implementation is the result of the scientific and *
19// * technical work of the GEANT4 collaboration. *
20// * By using, copying, modifying or distributing the software (or *
21// * any work based on the software) you agree to acknowledge its *
22// * use in resulting scientific publications, and indicate your *
23// * acceptance of all terms of the Geant4 Software license. *
24// ********************************************************************
25//
26/////////////////////////////////////////////////////////////////////////////////
27// Module: G4AdjointCSMatrix.hh
28// Author: L. Desorgher
29// Date: 1st April 2007
30// Organisation: SpaceIT GmbH
31// Customer: ESA/ESTEC
32/////////////////////////////////////////////////////////////////////////////////
33//
34// CHANGE HISTORY
35// --------------
36// ChangeHistory:
37// 1st April 2007 creation by L. Desorgher
38//
39//-------------------------------------------------------------
40// Documentation:
41// An adjoint CS matrix is used by the model of a reverse process to sample an adjoint secondary (being equivalent to a forward primary).
42// It represents the integration over the energy of the adjoint secondary (therefore the forward primary) of the differential cross section
43// of the equiavlent forward discrete process (Ionisation, Brem, PE effect, Compton,..) . Each reverse model has its own cross section matrix for a given cut,
44// material couple. It is therefore recompute after a modification of the cuts by the user.
45//
46//
47//
48
49#ifndef G4AdjointCSMatrix_h
50#define G4AdjointCSMatrix_h 1
51
52#include"globals.hh"
53#include<vector>
54#include"G4ParticleDefinition.hh"
55
56////////////////////////////////////////////////////////////////////////////////
57//
58class G4AdjointCSMatrix
59{
60 ////////////////////////////////
61 // Constructors and Destructor
62 ////////////////////////////////
63public:
64 G4AdjointCSMatrix(G4bool aBool);
65 ~G4AdjointCSMatrix();
66
67 ////////////
68 // Methods
69 ////////////
70 void Clear();
71 void AddData(G4double aPrimEnergy,G4double aCS, std::vector< G4double>* aLogSecondEnergyVector,
72 std::vector< G4double>* aLogProbVector,size_t n_pro_decade=0);
73
74 bool GetData(unsigned int i, G4double& aPrimEnergy,G4double& aCS,G4double& log0, std::vector< G4double>*& aLogSecondEnergyVector,
75 std::vector< G4double>*& aLogProbVector,
76 std::vector< size_t>*& aLogProbVectorIndex);
77
78 inline std::vector< G4double >* GetLogPrimEnergyVector(){return &theLogPrimEnergyVector;}
79 inline std::vector< G4double >* GetLogCrossSectionvector(){return &theLogCrossSectionVector;}
80 inline G4double GetDlog(){return dlog;}
81 inline G4bool IsScatProjToProjCase(){return is_scat_proj_to_proj_case;}
82 void Write(G4String file_name);
83 void Read(G4String file_name);
84
85private:
86
87 // we did first try to use G4PhysicsOrderedVector but they are not general enough for our purpose
88
89 std::vector< G4double > theLogPrimEnergyVector;
90 std::vector< G4double > theLogCrossSectionVector; //Adjoint Cross sections in function of primary energy
91 std::vector< std::vector< G4double >* > theLogSecondEnergyMatrix;
92 std::vector< std::vector< G4double >* > theLogProbMatrix; //Each column represents the integrated probability of getting a secondary
93 // in function of their energy
94 std::vector< std::vector< size_t >* > theLogProbMatrixIndex; //index of euqidistant LogProb
95 std::vector< G4double > log0Vector;
96
97 unsigned int nb_of_PrimEnergy;
98 G4bool is_scat_proj_to_proj_case;
99 G4double dlog;
100
101
102};
103#endif
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