source: trunk/source/processes/electromagnetic/xrays/src/G4RegularXTRadiator.cc@ 1066

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//
// $Id: G4RegularXTRadiator.cc,v 1.9 2006/06/29 19:56:09 gunter Exp $
// GEANT4 tag $Name: geant4-09-02 $
//

#include <complex>

#include "G4RegularXTRadiator.hh"
#include "Randomize.hh"

#include "G4Gamma.hh"

using namespace std;

////////////////////////////////////////////////////////////////////////////
//
// Constructor, destructor

G4RegularXTRadiator::G4RegularXTRadiator(G4LogicalVolume *anEnvelope,
                                         G4Material* foilMat,G4Material* gasMat, 
                                         G4double a, G4double b, G4int n,
                                         const G4String& processName) :
  G4VXTRenergyLoss(anEnvelope,foilMat,gasMat,a,b,n,processName)
{
  G4cout<<"Regular X-ray TR  radiator EM process is called"<<G4endl ;

  // Build energy and angular integral spectra of X-ray TR photons from
  // a radiator

  fAlphaPlate = 10000;
  fAlphaGas   = 1000;
  G4cout<<"fAlphaPlate = "<<fAlphaPlate<<" ; fAlphaGas = "<<fAlphaGas<<G4endl ;

  // BuildTable() ;
}

///////////////////////////////////////////////////////////////////////////

G4RegularXTRadiator::~G4RegularXTRadiator()
{
  ;
}



///////////////////////////////////////////////////////////////////////////
//
// Approximation for radiator interference factor for the case of
// fully Regular radiator. The plate and gas gap thicknesses are fixed .
// The mean values of the plate and gas gap thicknesses 
// are supposed to be about XTR formation zones but much less than 
// mean absorption length of XTR photons in coresponding material.

G4double 
G4RegularXTRadiator::GetStackFactor( G4double energy, 
                                         G4double gamma, G4double varAngle )
{

  // some gamma (10000/1000) like algorithm

  G4double result, Za, Zb, Ma, Mb;
  
  Za = GetPlateFormationZone(energy,gamma,varAngle);
  Zb = GetGasFormationZone(energy,gamma,varAngle);

  Ma = GetPlateLinearPhotoAbs(energy);
  Mb = GetGasLinearPhotoAbs(energy);


  G4complex Ca(1.0+0.5*fPlateThick*Ma/fAlphaPlate,fPlateThick/Za/fAlphaPlate); 
  G4complex Cb(1.0+0.5*fGasThick*Mb/fAlphaGas,fGasThick/Zb/fAlphaGas); 

  G4complex Ha = pow(Ca,-fAlphaPlate);  
  G4complex Hb = pow(Cb,-fAlphaGas);
  G4complex H  = Ha*Hb;
  
  G4complex F1 =   (1.0 - Ha)*(1.0 - Hb )/(1.0 - H)
                 * G4double(fPlateNumber);

  G4complex F2 =   (1.0-Ha)*(1.0-Ha)*Hb/(1.0-H)/(1.0-H)
                 * (1.0 - pow(H,fPlateNumber));

  G4complex R  = (F1 + F2)*OneInterfaceXTRdEdx(energy,gamma,varAngle);
  
  result       = 2.0*real(R);
  
  return      result;
  
  /*
   // numerically stable but slow algorithm

  G4double result, Qa, Qb, Q, aZa, bZb, aMa, bMb;   // , D; 
 
  aZa = fPlateThick/GetPlateFormationZone(energy,gamma,varAngle);
  bZb = fGasThick/GetGasFormationZone(energy,gamma,varAngle);
  aMa = fPlateThick*GetPlateLinearPhotoAbs(energy);
  bMb = fGasThick*GetGasLinearPhotoAbs(energy);
  Qa = exp(-aMa);
  Qb = exp(-bMb);
  Q  = Qa*Qb;
  G4complex Ha( exp(-0.5*aMa)*cos(aZa),
               -exp(-0.5*aMa)*sin(aZa)   );  
  G4complex Hb( exp(-0.5*bMb)*cos(bZb),
               -exp(-0.5*bMb)*sin(bZb)    );
  G4complex H  = Ha*Hb;
  
  G4complex Hs = conj(H);
  D            = 1.0 /( (1 - sqrt(Q))*(1 - sqrt(Q)) + 
                  4*sqrt(Q)*sin(0.5*(aZa+bZb))*sin(0.5*(aZa+bZb)) );
  G4complex F1 = (1.0 - Ha)*(1.0 - Hb)*(1.0 - Hs)
                 * G4double(fPlateNumber)*D;
  G4complex F2 = (1.0-Ha)*(1.0-Ha)*Hb*(1.0-Hs)*(1.0-Hs)
                 * (1.0 - pow(H,fPlateNumber)) * D*D;
  G4complex R  = (F1 + F2)*OneInterfaceXTRdEdx(energy,gamma,varAngle);
  

  G4complex S(0.,0.), c(1.,0.);
  G4int k;
  for(k = 1; k < fPlateNumber; k++)
  {
    c *= H;
    S += ( G4double(fPlateNumber) - G4double(k) )*c; 
  }
  G4complex R  = (2.- Ha - 1./Ha)*S + (1. - Ha)*G4double(fPlateNumber);
            R *= OneInterfaceXTRdEdx(energy,gamma,varAngle);
  result       = 2.0*real(R); 
  return      result;
  */
}


//
//
////////////////////////////////////////////////////////////////////////////