source: trunk/source/processes/electromagnetic/lowenergy/include/G4PenelopeIonisationModel.hh@ 1141

Last change on this file since 1141 was 1055, checked in by garnier, 17 years ago

maj sur la beta de geant 4.9.3

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[966]1//
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18// * This code implementation is the result of the scientific and *
19// * technical work of the GEANT4 collaboration. *
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25//
26// $Id: G4PenelopeIonisationModel.hh,v 1.1 2008/12/04 14:12:09 pandola Exp $
[1055]27// GEANT4 tag $Name: geant4-09-03-beta-cand-00 $
[966]28//
29// Author: Luciano Pandola
30//
31// History:
32// -----------
33// 26 Nov 2008 L. Pandola 1st implementation. Migration from EM process
34// to EM model. Physics is unchanged.
35//
36// -------------------------------------------------------------------
37//
38// Class description:
39// Low Energy Electromagnetic Physics, e+ and e- ionisation
40// with Penelope Model
41// -------------------------------------------------------------------
42
43#ifndef G4PENELOPEIONISATIONMODEL_HH
44#define G4PENELOPEIONISATIONMODEL_HH 1
45
46#include "globals.hh"
47#include "G4VEmModel.hh"
48#include "G4DataVector.hh"
49#include "G4ParticleChangeForLoss.hh"
50#include "G4VCrossSectionHandler.hh"
51#include "G4PhysicsLogVector.hh"
52#include "G4AtomicDeexcitation.hh"
53
54class G4ParticleDefinition;
55class G4DynamicParticle;
56class G4MaterialCutsCouple;
57class G4Material;
58class G4VEMDataSet;
59
60class G4PenelopeIonisationModel : public G4VEmModel
61{
62
63public:
64
65 G4PenelopeIonisationModel(const G4ParticleDefinition* p=0,
66 const G4String& processName ="PenelopeIoni");
67
68 virtual ~G4PenelopeIonisationModel();
69
70 virtual void Initialise(const G4ParticleDefinition*, const G4DataVector&);
71
72 virtual G4double CrossSectionPerVolume(const G4Material* material,
73 const G4ParticleDefinition* theParticle,
74 G4double kineticEnergy,
75 G4double cutEnergy,
76 G4double maxEnergy = DBL_MAX);
77
78 virtual void SampleSecondaries(std::vector<G4DynamicParticle*>*,
79 const G4MaterialCutsCouple*,
80 const G4DynamicParticle*,
81 G4double tmin,
82 G4double maxEnergy);
83
84 virtual G4double ComputeDEDXPerVolume(const G4Material*,
85 const G4ParticleDefinition*,
86 G4double kineticEnergy,
87 G4double cutEnergy);
88
89
90 void SetUseAtomicDeexcitation(G4bool value){fUseAtomicDeexcitation = value;};
91 G4bool GetUseAtomicDeexcitation(){return fUseAtomicDeexcitation;};
92
93 void SetVerbosityLevel(G4int lev){verboseLevel = lev;};
94 G4int GetVerbosityLevel(){return verboseLevel;};
95
96
97protected:
98 G4ParticleChangeForLoss* fParticleChange;
99
100private:
101
102 G4PenelopeIonisationModel & operator=(const G4PenelopeIonisationModel &right);
103 G4PenelopeIonisationModel(const G4PenelopeIonisationModel&);
104
105
106 //Intrinsic energy limits of the model: cannot be extended by the parent process
107 G4double fIntrinsicLowEnergyLimit;
108 G4double fIntrinsicHighEnergyLimit;
109
110 G4bool fUseAtomicDeexcitation;
111
112 G4int verboseLevel;
113
114 G4bool isInitialised;
115
116 G4double CalculateDeltaFermi(G4double kinEnergy ,G4int Z,
117 G4double electronVolumeDensity);
118
119 //Methods and variables to calculate final state
120 void CalculateDiscreteForElectrons(G4double kinEnergy,G4double cutoffEnergy,
121 G4int Z,G4double electronVolumeDensity);
122 void CalculateDiscreteForPositrons(G4double kinEnergy,G4double cutoffEnergy,
123 G4int Z,G4double electronVolumeDensity);
124
125 G4AtomicDeexcitation deexcitationManager;
126 G4double kineticEnergy1;
127 G4double cosThetaPrimary;
128 G4double energySecondary;
129 G4double cosThetaSecondary;
130 G4int iOsc;
131
132 //These methods are used to calculate the hard-cross section (namely they
133 //return the hard/total cross section)
134 G4double CalculateCrossSectionsRatio(G4double kinEnergy,
135 G4double cutoffEnergy,
136 G4int Z,
137 G4double electronVolumeDensity,
138 const G4ParticleDefinition*);
139 //In fact the total cross section (hard+soft) is read from file
140 //The following methods give the cross section contribution (hard and soft) from each
141 //individual oscillator
142 std::pair<G4double,G4double> CrossSectionsRatioForElectrons(G4double kineticEnergy,
143 G4double resEnergy,
144 G4double densityCorrection,
145 G4double cutoffEnergy);
146
147 std::pair<G4double,G4double> CrossSectionsRatioForPositrons(G4double kineticEnergy,
148 G4double resEnergy,
149 G4double densityCorrection,
150 G4double cutoffEnergy);
151
152 G4VCrossSectionHandler* crossSectionHandler;
153
154 //These methods are used to calculate the stopping power up to the cutoff
155 //for each individual oscillator
156 G4double ComputeStoppingPowerForElectrons(G4double kinEnergy,
157 G4double cutEnergy,
158 G4double deltaFermi,
159 G4double resEnergy);
160
161 G4double ComputeStoppingPowerForPositrons(G4double kinEnergy,
162 G4double cutEnergy,
163 G4double deltaFermi,
164 G4double resEnergy);
165
166
167 //Parameters of atomic shells
168 void ReadData();
169 std::map<G4int,G4DataVector*> *ionizationEnergy;
170 std::map<G4int,G4DataVector*> *resonanceEnergy;
171 std::map<G4int,G4DataVector*> *occupationNumber;
172 std::map<G4int,G4DataVector*> *shellFlag;
173
174 //Mean free path table. This will become obsolete! For now I need something to store
175 //cross sections and to sample a random atom
176 std::vector<G4VEMDataSet*>* theXSTable;
177 std::vector<G4VEMDataSet*>* BuildCrossSectionTable(const G4ParticleDefinition*);
178 G4int SampleRandomAtom(const G4MaterialCutsCouple*,G4double energy) const;
179
180};
181
182#endif
183
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