Import Geant4 0.0.0 source tree

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Gabriele Cosmo
2016-06-01 15:25:35 +02:00
parent 54d6b71f95
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// This code implementation is the intellectual property of
// the RD44 GEANT4 collaboration.
//
// By copying, distributing or modifying the Program (or any work
// based on the Program) you indicate your acceptance of this statement,
// and all its terms.
//
// $Id: G4TransitionRadiation.cc,v 2.2 1998/11/27 13:37:02 grichine Exp $
// GEANT4 tag $Name: geant4-00 $
//
// G4TransitionRadiation class -- implementation file
// GEANT 4 class implementation file --- Copyright CERN 1995
// CERN Geneva Switzerland
// For information related to this code, please, contact
// CERN, CN Division, ASD Group
// History:
// 1st version 11.09.97 V. Grichine (Vladimir.Grichine@cern.ch )
// 2nd version 16.12.97 V. Grichine
#include <math.h>
// #include "G4ios.hh"
// #include <fstream.h>
// #include <stdlib.h>
#include "G4TransitionRadiation.hh"
#include "G4Material.hh"
// Init gamma array
// Local constants
const G4int G4TransitionRadiation::fSympsonNumber = 100 ;
const G4int G4TransitionRadiation::fGammaNumber = 15 ;
const G4int G4TransitionRadiation::fPointNumber = 100 ;
///////////////////////////////////////////////////////////////////////
//
// Constructor for selected couple of materials
//
G4TransitionRadiation::
G4TransitionRadiation( const G4String& processName )
: G4VDiscreteProcess(processName)
{
// fMatIndex1 = pMat1->GetIndex() ;
// fMatIndex2 = pMat2->GetIndex() ;
}
//////////////////////////////////////////////////////////////////////
//
// Destructor
//
G4TransitionRadiation::~G4TransitionRadiation()
{
;
}
///////////////////////////////////////////////////////////////////
//
// Sympson integral of TR spectral-angle density over energy between
// the limits energy 1 and energy2 at fixed varAngle = 1 - cos(Theta)
G4double
G4TransitionRadiation::IntegralOverEnergy( G4double energy1,
G4double energy2,
G4double varAngle ) const
{
G4int i ;
G4double h , sumEven = 0.0 , sumOdd = 0.0 ;
h = 0.5*(energy2 - energy1)/fSympsonNumber ;
for(i=1;i<fSympsonNumber;i++)
{
sumEven += SpectralAngleTRdensity(energy1 + 2*i*h,varAngle) ;
sumOdd += SpectralAngleTRdensity(energy1 + (2*i - 1)*h,varAngle) ;
}
sumOdd += SpectralAngleTRdensity(energy1 + (2*fSympsonNumber - 1)*h,varAngle) ;
return h*( SpectralAngleTRdensity(energy1,varAngle)
+ SpectralAngleTRdensity(energy2,varAngle)
+ 4.0*sumOdd + 2.0*sumEven )/3.0 ;
}
///////////////////////////////////////////////////////////////////
//
// Sympson integral of TR spectral-angle density over energy between
// the limits varAngle1 and varAngle2 at fixed energy
G4double
G4TransitionRadiation::IntegralOverAngle( G4double energy,
G4double varAngle1,
G4double varAngle2 ) const
{
G4int i ;
G4double h , sumEven = 0.0 , sumOdd = 0.0 ;
h = 0.5*(varAngle2 - varAngle1)/fSympsonNumber ;
for(i=1;i<fSympsonNumber;i++)
{
sumEven += SpectralAngleTRdensity(energy,varAngle1 + 2*i*h) ;
sumOdd += SpectralAngleTRdensity(energy,varAngle1 + (2*i - 1)*h) ;
}
sumOdd += SpectralAngleTRdensity(energy,varAngle1 + (2*fSympsonNumber - 1)*h) ;
return h*( SpectralAngleTRdensity(energy,varAngle1)
+ SpectralAngleTRdensity(energy,varAngle2)
+ 4.0*sumOdd + 2.0*sumEven )/3.0 ;
}
///////////////////////////////////////////////////////////////////
//
// The number of transition radiation photons generated in the
// angle interval between varAngle1 and varAngle2
//
G4double G4TransitionRadiation::
AngleIntegralDistribution( G4double varAngle1,
G4double varAngle2 ) const
{
G4int i ;
G4double h , sumEven = 0.0 , sumOdd = 0.0 ;
h = 0.5*(varAngle2 - varAngle1)/fSympsonNumber ;
for(i=1;i<fSympsonNumber;i++)
{
sumEven += IntegralOverEnergy(fMinEnergy,
fMinEnergy +0.3*(fMaxEnergy-fMinEnergy),
varAngle1 + 2*i*h)
+ IntegralOverEnergy(fMinEnergy + 0.3*(fMaxEnergy - fMinEnergy),
fMaxEnergy,
varAngle1 + 2*i*h);
sumOdd += IntegralOverEnergy(fMinEnergy,
fMinEnergy + 0.3*(fMaxEnergy - fMinEnergy),
varAngle1 + (2*i - 1)*h)
+ IntegralOverEnergy(fMinEnergy + 0.3*(fMaxEnergy - fMinEnergy),
fMaxEnergy,
varAngle1 + (2*i - 1)*h) ;
}
sumOdd += IntegralOverEnergy(fMinEnergy,
fMinEnergy + 0.3*(fMaxEnergy - fMinEnergy),
varAngle1 + (2*fSympsonNumber - 1)*h)
+ IntegralOverEnergy(fMinEnergy + 0.3*(fMaxEnergy - fMinEnergy),
fMaxEnergy,
varAngle1 + (2*fSympsonNumber - 1)*h) ;
return h*(IntegralOverEnergy(fMinEnergy,
fMinEnergy + 0.3*(fMaxEnergy - fMinEnergy),
varAngle1)
+ IntegralOverEnergy(fMinEnergy + 0.3*(fMaxEnergy - fMinEnergy),
fMaxEnergy,
varAngle1)
+ IntegralOverEnergy(fMinEnergy,
fMinEnergy + 0.3*(fMaxEnergy - fMinEnergy),
varAngle2)
+ IntegralOverEnergy(fMinEnergy + 0.3*(fMaxEnergy - fMinEnergy),
fMaxEnergy,
varAngle2)
+ 4.0*sumOdd + 2.0*sumEven )/3.0 ;
}
///////////////////////////////////////////////////////////////////
//
// The number of transition radiation photons, generated in the
// energy interval between energy1 and energy2
//
G4double G4TransitionRadiation::
EnergyIntegralDistribution( G4double energy1,
G4double energy2 ) const
{
G4int i ;
G4double h , sumEven = 0.0 , sumOdd = 0.0 ;
h = 0.5*(energy2 - energy1)/fSympsonNumber ;
for(i=1;i<fSympsonNumber;i++)
{
sumEven += IntegralOverAngle(energy1 + 2*i*h,0.0,0.01*fMaxTheta )
+ IntegralOverAngle(energy1 + 2*i*h,0.01*fMaxTheta,fMaxTheta);
sumOdd += IntegralOverAngle(energy1 + (2*i - 1)*h,0.0,0.01*fMaxTheta)
+ IntegralOverAngle(energy1 + (2*i - 1)*h,0.01*fMaxTheta,fMaxTheta) ;
}
sumOdd += IntegralOverAngle(energy1 + (2*fSympsonNumber - 1)*h,
0.0,0.01*fMaxTheta)
+ IntegralOverAngle(energy1 + (2*fSympsonNumber - 1)*h,
0.01*fMaxTheta,fMaxTheta) ;
return h*(IntegralOverAngle(energy1,0.0,0.01*fMaxTheta)
+ IntegralOverAngle(energy1,0.01*fMaxTheta,fMaxTheta)
+ IntegralOverAngle(energy2,0.0,0.01*fMaxTheta)
+ IntegralOverAngle(energy2,0.01*fMaxTheta,fMaxTheta)
+ 4.0*sumOdd + 2.0*sumEven )/3.0 ;
}
// end of G4TransitionRadiation implementation file --------------------------