Geant4 9.6.0
Toolkit for the simulation of the passage of particles through matter
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G4TransitionRadiation.hh
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1//
2// ********************************************************************
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6// * the Geant4 Collaboration. It is provided under the terms and *
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14// * regarding this software system or assume any liability for its *
15// * use. Please see the license in the file LICENSE and URL above *
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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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24// ********************************************************************
25//
26// $Id$
27//
28// G4TransitionRadiation -- header file
29//
30// Class for description of transition radiation generated
31// by charged particle crossed interface between material 1
32// and material 2 (1 -> 2). Transition radiation could be of kind:
33// - optical back
34// - optical forward
35// - X-ray forward (for relativistic case Tkin/mass >= 10^2)
36//
37// GEANT 4 class header file --- Copyright CERN 1995
38// CERB Geneva Switzerland
39//
40// for information related to this code, please, contact
41// CERN, CN Division, ASD Group
42// History:
43// 18.12.97, V. Grichine ([email protected])
44// 02.02.00, V.Grichine, new data fEnergy and fVarAngle for double
45// numerical integration in inherited classes
46// 03.06.03, V.Ivanchenko fix compilation warnings
47// 28.07.05, P.Gumplinger add G4ProcessType to constructor
48
49#ifndef G4TransitionRadiation_h
50#define G4TransitionRadiation_h
51
52
53#include "G4VDiscreteProcess.hh"
54#include "G4Material.hh"
55// #include "G4OpBoundaryProcess.hh"
56
58{
59public:
60
61 G4TransitionRadiation( const G4String& processName = "TR",
63
64 virtual ~G4TransitionRadiation() ;
65
66 // Methods
67
68 G4bool IsApplicable(const G4ParticleDefinition& aParticleType);
69
72
74
75 virtual
77 G4double varAngle ) const = 0 ;
78
80 G4double energy2,
81 G4double varAngle ) const ;
82
84 G4double varAngle1,
85 G4double varAngle2 ) const ;
86
88 G4double varAngle2 ) const ;
89
91 G4double energy2 ) const ;
92
93
94
95 // Access functions
96
97protected :
98
99 G4int fMatIndex1 ; // index of the 1st material
100 G4int fMatIndex2 ; // index of the 2nd material
101
102 // private :
103
107
108 // Local constants
109 static const G4int fSympsonNumber ; // Accuracy of Sympson integration 10
110 static const G4int fGammaNumber ; // = 15
111 static const G4int fPointNumber ; // = 100
112
113 G4double fMinEnergy ; // min TR energy
114 G4double fMaxEnergy ; // max TR energy
115 G4double fMaxTheta ; // max theta of TR quanta
116
117 G4double fSigma1 ; // plasma energy Sq of matter1
118 G4double fSigma2 ; // plasma energy Sq of matter2
119
120private:
121
122// Operators
124 G4TransitionRadiation& operator=(const G4TransitionRadiation& right) ;
125
126};
127
128#endif // G4TransitionRadiation_h
G4double condition(const G4ErrorSymMatrix &m)
G4ForceCondition
G4ProcessType
@ fElectromagnetic
double G4double
Definition: G4Types.hh:64
int G4int
Definition: G4Types.hh:66
bool G4bool
Definition: G4Types.hh:67
Definition: G4Step.hh:78
static const G4int fGammaNumber
G4double EnergyIntegralDistribution(G4double energy1, G4double energy2) const
G4double GetMeanFreePath(const G4Track &, G4double, G4ForceCondition *condition)
static const G4int fPointNumber
G4double IntegralOverAngle(G4double energy, G4double varAngle1, G4double varAngle2) const
virtual G4double SpectralAngleTRdensity(G4double energy, G4double varAngle) const =0
G4double IntegralOverEnergy(G4double energy1, G4double energy2, G4double varAngle) const
G4bool IsApplicable(const G4ParticleDefinition &aParticleType)
G4VParticleChange * PostStepDoIt(const G4Track &, const G4Step &)
static const G4int fSympsonNumber
G4double AngleIntegralDistribution(G4double varAngle1, G4double varAngle2) const