source: trunk/source/processes/electromagnetic/xrays/include/G4SynchrotronRadiation.hh@ 991

Last change on this file since 991 was 961, checked in by garnier, 17 years ago

update processes

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[819]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 *
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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 *
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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 *
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 *
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24// ********************************************************************
25//
26//
27// $Id: G4SynchrotronRadiation.hh,v 1.4 2006/06/29 19:55:43 gunter Exp $
[961]28// GEANT4 tag $Name: geant4-09-02-ref-02 $
[819]29//
30// ------------------------------------------------------------
31// GEANT 4 class header file
32// CERN Geneva Switzerland
33//
34//
35// History:
36// 21-5-98 1 version , V. Grichine
37// 28-05-01, V.Ivanchenko minor changes to provide ANSI -wall compilation
38// 23-05-06, H. Burkhardt: Energy spectrum from function rather than table
39//
40//
41// ------------------------------------------------------------
42
43#ifndef G4SynchrotronRadiation_h
44#define G4SynchrotronRadiation_h 1
45
46#include "G4ios.hh"
47#include "globals.hh"
48#include "Randomize.hh"
49#include "G4VDiscreteProcess.hh"
50#include "G4TransportationManager.hh"
51#include "G4FieldManager.hh"
52#include "G4Field.hh"
53#include "G4ThreeVector.hh"
54#include "G4PropagatorInField.hh"
55
56#include "G4Track.hh"
57#include "G4Step.hh"
58
59#include "G4Gamma.hh"
60#include "G4Electron.hh"
61#include "G4Positron.hh"
62
63
64class G4SynchrotronRadiation : public G4VDiscreteProcess
65{
66public:
67
68 G4SynchrotronRadiation(const G4String& pName = "SynRad",
69 G4ProcessType type = fElectromagnetic);
70
71 virtual ~G4SynchrotronRadiation();
72
73 G4double GetMeanFreePath( const G4Track& track,
74 G4double previousStepSize,
75 G4ForceCondition* condition );
76
77 G4VParticleChange *PostStepDoIt( const G4Track& track,
78 const G4Step& Step );
79
80 G4double GetPhotonEnergy( const G4Track& trackData,
81 const G4Step& stepData );
82
83 G4double GetRandomEnergySR( G4double, G4double );
84
85 G4double InvSynFracInt(G4double x);
86 G4double Chebyshev(G4double a,G4double b,const G4double c[],G4int m,G4double x);
87 G4bool IsApplicable(const G4ParticleDefinition&);
88 void BuildPhysicsTable(const G4ParticleDefinition& );
89 void PrintInfoDefinition();
90
91private:
92
93 G4SynchrotronRadiation & operator=(const G4SynchrotronRadiation &right);
94 G4SynchrotronRadiation(const G4SynchrotronRadiation&);
95
96 G4ParticleDefinition* theGamma;
97 const G4ParticleDefinition* theElectron;
98 const G4ParticleDefinition* thePositron;
99
100 G4double fLambdaConst;
101 G4double fEnergyConst;
102
103 G4PropagatorInField* fFieldPropagator;
104
105};
106
107////////////////////////// INLINE METHODS /////////////////////////////
108inline G4bool
109G4SynchrotronRadiation::IsApplicable( const G4ParticleDefinition& particle )
110{
111
112 return ( ( &particle == (const G4ParticleDefinition *)theElectron ) ||
113 ( &particle == (const G4ParticleDefinition *)thePositron ) );
114
115 // return ( particle.GetPDGCharge() != 0.0 );
116}
117
118inline G4double G4SynchrotronRadiation::Chebyshev(G4double a,G4double b,const G4double c[],G4int m,G4double x)
119{
120 G4double y;
121 G4double y2=2.0*(y=(2.0*x-a-b)/(b-a)); // Change of variable.
122 G4double d=0,dd=0;
123 for (G4int j=m-1;j>=1;j--) // Clenshaw's recurrence.
124 { G4double sv=d;
125 d=y2*d-dd+c[j];
126 dd=sv;
127 }
128 return y*d-dd+0.5*c[0];
129}
130
131#endif // end of G4SynchrotronRadiation.hh
132
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