source: trunk/source/processes/electromagnetic/lowenergy/include/G4hQAOModel.hh @ 1350

Last change on this file since 1350 was 819, checked in by garnier, 16 years ago

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1//
2// ********************************************************************
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24// ********************************************************************
25//
26//
27// -------------------------------------------------------------------
28//
29// GEANT4 Class file
30//
31//
32// File name:     G4hQAOModel
33//
34// Author:        V.Ivanchenko (Vladimir.Ivanchenko@cern.ch)
35//
36// Creation date: 27 April 2004
37//
38// Modifications:
39//
40// Class Description:
41//
42// Electronic stopping power for negative heavy partiles
43// Further documentation available from http://www.ge.infn.it/geant4/lowE//
44
45// -------------------------------------------------------------------
46//
47
48#ifndef G4hQAOModel_h
49#define G4hQAOModel_h 1
50
51#include "globals.hh"
52#include "G4VhElectronicStoppingPower.hh"
53
54class G4Material;
55class G4Element;
56
57class G4hQAOModel : public G4VhElectronicStoppingPower
58{
59
60public:
61
62  G4hQAOModel();
63
64  ~G4hQAOModel();
65
66  G4bool HasMaterial(const G4Material*) {return true;};
67
68  G4double StoppingPower(const G4Material* material,
69                               G4double kineticEnergy);
70
71  G4double ElectronicStoppingPower(G4double z,
72                                   G4double kineticEnergy) const;
73
74private:
75
76  // get number of shell, energy and oscillator strenghts for material
77  G4int GetNumberOfShell(G4int z) const;
78
79  G4double GetShellEnergy(G4int z, G4int nbOfTheShell) const;
80  G4double GetOscillatorEnergy(G4int z, G4int nbOfTheShell) const;
81  G4double GetShellStrength(G4int z, G4int nbOfTheShell) const;
82  G4double GetOccupationNumber(G4int z, G4int ShellNb) const;
83
84  // calculate stopping number for L's term
85  G4double GetL0(G4double normEnergy) const;
86  // terms in Z^2
87  G4double GetL1(G4double normEnergy) const;
88  // terms in Z^3
89  G4double GetL2(G4double normEnergy) const;
90  // terms in Z^4
91 
92  // hide assignment operator
93  G4hQAOModel & operator=(const  G4hQAOModel &right);
94  G4hQAOModel(const  G4hQAOModel&);
95
96  // Z of element at now avaliable for the model
97  static const G4int materialAvailable[6];
98
99  // number, energy and oscillator strenghts
100  // for an harmonic oscillator model of material
101  static const  G4int nbofShellForMaterial[6];
102  static const  G4double alShellEnergy[3];
103  static const  G4double alShellStrength[3];
104  static const  G4double siShellEnergy[3];
105  static const  G4double siShellStrength[3];
106  static const  G4double cuShellEnergy[4];
107  static const  G4double cuShellStrength[4];
108  static const  G4double taShellEnergy[6];
109  static const  G4double taShellStrength[6];
110  static const  G4double auShellEnergy[6];
111  static const  G4double auShellStrength[6];
112  static const  G4double ptShellEnergy[6];
113  static const  G4double ptShellStrength[6];
114
115
116  //  variable for calculation of stopping number of L's term
117  static const G4double L0[67][2];
118  static const G4double L1[22][2];
119  static const G4double L2[14][2];
120  static const G4int nbOfElectronPerSubShell[1540];
121  static const G4int fNumberOfShells[101];
122
123  G4int numberOfMaterials;
124  G4int sizeL0;
125  G4int sizeL1;
126  G4int sizeL2;
127
128  const G4Material* currentMaterial;
129  const G4Element*  currentElement;
130
131  G4double theZieglerFactor;
132  G4double thePlasmonFactor;
133};
134
135#endif
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