G4LivermoreGammaConversionModelRC.cc

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//
// Author: Sebastien Incerti
//         22 January 2012
//         on base of G4LivermoreGammaConversionModelRC (original version)
//         and G4LivermoreRayleighModel (MT version)
 
#include "G4LivermoreGammaConversionModelRC.hh"
#include "G4PhysicalConstants.hh"
#include "G4SystemOfUnits.hh"
#include "G4Log.hh"
#include "G4Electron.hh"                                                           
#include "G4Positron.hh"
#include "G4Gamma.hh"
#include "G4ParticleChangeForGamma.hh"
#include "G4Exp.hh"
                                                           
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using namespace std;
 
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
 
G4int G4LivermoreGammaConversionModelRC::maxZ = 99;
G4LPhysicsFreeVector* G4LivermoreGammaConversionModelRC::data[] = {nullptr};
 
G4LivermoreGammaConversionModelRC::G4LivermoreGammaConversionModelRC
(const G4ParticleDefinition*, const G4String& nam)
:G4VEmModel(nam),isInitialised(false),smallEnergy(2.*MeV)
{
  fParticleChange = nullptr;
 
  lowEnergyLimit = 2.0*electron_mass_c2;
     
  verboseLevel= 0;
  // Verbosity scale for debugging purposes:
  // 0 = nothing 
  // 1 = calculation of cross sections, file openings...
  // 2 = entering in methods
 
  if(verboseLevel > 0) 
  {
    G4cout << "G4LivermoreGammaConversionModelRC is constructed " << G4endl;
  }
}
 
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
 
G4LivermoreGammaConversionModelRC::~G4LivermoreGammaConversionModelRC()
{
  if(IsMaster()) {
    for(G4int i=0; i<maxZ; ++i) {
      if(data[i]) { 
    delete data[i];
    data[i] = 0;
      }
    }
  }
}
 
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
 
void G4LivermoreGammaConversionModelRC::Initialise(
                                const G4ParticleDefinition* particle,
                const G4DataVector& cuts)
{
  if (verboseLevel > 1) 
  {
    G4cout << "Calling Initialise() of G4LivermoreGammaConversionModelRC." 
       << G4endl
       << "Energy range: "
       << LowEnergyLimit() / MeV << " MeV - "
       << HighEnergyLimit() / GeV << " GeV"
       << G4endl;
  }
 
  if(IsMaster()) 
  {
 
    // Initialise element selector
 
    InitialiseElementSelectors(particle, cuts);
 
    // Access to elements
  
    char* path = std::getenv("G4LEDATA");
 
    G4ProductionCutsTable* theCoupleTable =
      G4ProductionCutsTable::GetProductionCutsTable();
  
    G4int numOfCouples = theCoupleTable->GetTableSize();
  
    for(G4int i=0; i<numOfCouples; ++i) 
    {
      const G4Material* material = 
        theCoupleTable->GetMaterialCutsCouple(i)->GetMaterial();
      const G4ElementVector* theElementVector = material->GetElementVector();
      G4int nelm = material->GetNumberOfElements();
    
      for (G4int j=0; j<nelm; ++j) 
      {
        G4int Z = (G4int)(*theElementVector)[j]->GetZ();
        if(Z < 1)          { Z = 1; }
        else if(Z > maxZ)  { Z = maxZ; }
        if(!data[Z]) { ReadData(Z, path); }
      }
    }
  }
  if(isInitialised) { return; }
  fParticleChange = GetParticleChangeForGamma();
  isInitialised = true;
}
 
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
 
void G4LivermoreGammaConversionModelRC::InitialiseLocal(
     const G4ParticleDefinition*, G4VEmModel* masterModel)
{
  SetElementSelectors(masterModel->GetElementSelectors());
}
 
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
 
G4double 
G4LivermoreGammaConversionModelRC::MinPrimaryEnergy(const G4Material*,
                          const G4ParticleDefinition*,
                          G4double)
{
  return lowEnergyLimit;
}
 
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
 
void G4LivermoreGammaConversionModelRC::ReadData(size_t Z, const char* path)
{
  if (verboseLevel > 1) 
  {
    G4cout << "Calling ReadData() of G4LivermoreGammaConversionModelRC" 
       << G4endl;
  }
 
  if(data[Z]) { return; }
  
  const char* datadir = path;
 
  if(!datadir) 
  {
    datadir = std::getenv("G4LEDATA");
    if(!datadir) 
    {
      G4Exception("G4LivermoreGammaConversionModelRC::ReadData()",
          "em0006",FatalException,
          "Environment variable G4LEDATA not defined");
      return;
    }
  }
 
  //
  
  data[Z] = new G4LPhysicsFreeVector();
  
  //
  
  std::ostringstream ost;
  ost << datadir << "/livermore/pair/pp-cs-" << Z <<".dat";
  std::ifstream fin(ost.str().c_str());
  
  if( !fin.is_open()) 
  {
    G4ExceptionDescription ed;
    ed << "G4LivermoreGammaConversionModelRC data file <" << ost.str().c_str()
       << "> is not opened!" << G4endl;
    G4Exception("G4LivermoreGammaConversionModelRC::ReadData()",
        "em0003",FatalException,
        ed,"G4LEDATA version should be G4EMLOW6.27 or later.");
    return;
  } 
  
  else 
  {
    
    if(verboseLevel > 3) { G4cout << "File " << ost.str() 
         << " is opened by G4LivermoreGammaConversionModelRC" << G4endl;}
    
    data[Z]->Retrieve(fin, true);
  } 
 
  // Activation of spline interpolation
  data[Z] ->SetSpline(true);  
  
}
 
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
 
G4double 
G4LivermoreGammaConversionModelRC::ComputeCrossSectionPerAtom(const G4ParticleDefinition*,
                                G4double GammaEnergy,
                                G4double Z, G4double,
                                G4double, G4double)
{
  if (verboseLevel > 1) 
  {
    G4cout << "Calling ComputeCrossSectionPerAtom() of G4LivermoreGammaConversionModelRC" 
       << G4endl;
  }
 
  if (GammaEnergy < lowEnergyLimit) { return 0.0; } 
 
  G4double xs = 0.0;
  
  G4int intZ=G4int(Z);
 
  if(intZ < 1 || intZ > maxZ) { return xs; }
 
  G4LPhysicsFreeVector* pv = data[intZ];
 
  // if element was not initialised
  // do initialisation safely for MT mode
  if(!pv) 
  {
    InitialiseForElement(0, intZ);
    pv = data[intZ];
    if(!pv) { return xs; }
  }
  // x-section is taken from the table
  xs = pv->Value(GammaEnergy); 
 
  if(verboseLevel > 0)
  {
    G4int n = pv->GetVectorLength() - 1;
    G4cout  <<  "****** DEBUG: tcs value for Z=" << Z << " at energy (MeV)=" 
        << GammaEnergy/MeV << G4endl;
    G4cout  <<  "  cs (Geant4 internal unit)=" << xs << G4endl;
    G4cout  <<  "    -> first cs value in EADL data file (iu) =" << (*pv)[0] << G4endl;
    G4cout  <<  "    -> last  cs value in EADL data file (iu) =" << (*pv)[n] << G4endl;
    G4cout  <<  "*********************************************************" << G4endl;
  }
 
  return xs;
 
}
 
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
 
void G4LivermoreGammaConversionModelRC::SampleSecondaries(
                                 std::vector<G4DynamicParticle*>* fvect,
                 const G4MaterialCutsCouple* couple,
                 const G4DynamicParticle* aDynamicGamma,
                 G4double, G4double)
{
 
// The energies of the e+ e- secondaries are sampled using the Bethe - Heitler
// cross sections with Coulomb correction. A modified version of the random
// number techniques of Butcher & Messel is used (Nuc Phys 20(1960),15).
 
// Note 1 : Effects due to the breakdown of the Born approximation at low
// energy are ignored.
// Note 2 : The differential cross section implicitly takes account of
// pair creation in both nuclear and atomic electron fields. However triplet
// prodution is not generated.
 
  if (verboseLevel > 1) {
    G4cout << "Calling SampleSecondaries() of G4LivermoreGammaConversionModelRC" 
       << G4endl;
  }
 
  G4double photonEnergy = aDynamicGamma->GetKineticEnergy();
  G4ParticleMomentum photonDirection = aDynamicGamma->GetMomentumDirection();
 
  G4double epsilon ;
  G4double epsilon0Local = electron_mass_c2 / photonEnergy ;
 
  G4double electronTotEnergy = 0.0;
  G4double positronTotEnergy = 0.0;
  G4double HardPhotonEnergy = 0.0;
  
  
  // Do it fast if photon energy < 2. MeV
  if (photonEnergy < smallEnergy )
    {
      epsilon = epsilon0Local + (0.5 - epsilon0Local) * G4UniformRand();
      if (G4UniformRand() > 0.5)
    {
      electronTotEnergy = (1. - epsilon) * photonEnergy;
      positronTotEnergy = epsilon * photonEnergy;
    }
      else
    {
      positronTotEnergy = (1. - epsilon) * photonEnergy;
      electronTotEnergy = epsilon * photonEnergy;
    }
    }
  else
    {
      // Select randomly one element in the current material
      
      const G4ParticleDefinition* particle =  aDynamicGamma->GetDefinition();
      const G4Element* element = SelectRandomAtom(couple,particle,photonEnergy);
      
      if (element == 0)
    {
      G4cout << "G4LivermoreGammaConversionModelRC::SampleSecondaries - element = 0" 
         << G4endl;
      return;
    }
      G4IonisParamElm* ionisation = element->GetIonisation();
      if (ionisation == 0)
    {
      G4cout << "G4LivermoreGammaConversionModelRC::SampleSecondaries - ionisation = 0" 
         << G4endl;
      return;
    }
      
      // Extract Coulomb factor for this Element
      G4double fZ = 8. * (ionisation->GetlogZ3());
      if (photonEnergy > 50. * MeV) fZ += 8. * (element->GetfCoulomb());
      
      // Limits of the screening variable
      G4double screenFactor = 136. * epsilon0Local / (element->GetIonisation()->GetZ3()) ;
      G4double screenMax = G4Exp ((42.24 - fZ)/8.368) - 0.952 ;
      G4double screenMin = std::min(4.*screenFactor,screenMax) ;
      
      // Limits of the energy sampling
      G4double epsilon1 = 0.5 - 0.5 * std::sqrt(1. - screenMin / screenMax) ;
      G4double epsilonMin = std::max(epsilon0Local,epsilon1);
      G4double epsilonRange = 0.5 - epsilonMin ;
      
      // Sample the energy rate of the created electron (or positron)
      G4double screen;
      G4double gReject ;
      
      G4double f10 = ScreenFunction1(screenMin) - fZ;
      G4double f20 = ScreenFunction2(screenMin) - fZ;
      G4double normF1 = std::max(f10 * epsilonRange * epsilonRange,0.);
      G4double normF2 = std::max(1.5 * f20,0.);
      
      // Method for Radiative corrections 
      
      G4double a=393.3750918, b=115.3070201, c=810.6428451, d=19.96497475, e=1016.874592, f=1.936685510,
    gLocal=751.2140962, h=0.099751048, i=299.9466339, j=0.002057250, k=49.81034926;
      G4double aa=-18.6371131, bb=-1729.95248, cc=9450.971186, dd=106336.0145, ee=55143.09287, ff=-117602.840,
    gg=-721455.467, hh=693957.8635, ii=156266.1085, jj=533209.9347;
      G4double Rechazo = 0.;
      G4double logepsMin = log(epsilonMin);
      G4double NormaRC = a + b*logepsMin + c/logepsMin + d*pow(logepsMin,2.) + e/pow(logepsMin,2.) + f*pow(logepsMin,3.) +
    gLocal/pow(logepsMin,3.) + h*pow(logepsMin,4.) + i/pow(logepsMin,4.) + j*pow(logepsMin,5.) +
    k/pow(logepsMin,5.);
      
      G4double HardPhotonThreshold = 0.08;
      G4double r1, r2, r3, beta=0, gbeta, sigt = 582.068, sigh, rejet;
      // , Pi = 2.*acos(0.);
      G4double cg = (11./2.)/(G4Exp(-11.*HardPhotonThreshold/2.)-G4Exp(-11./2.));
      
      r1 = G4UniformRand();
      sigh = 1028.58*G4Exp(-HardPhotonThreshold/0.09033) + 136.63; // sigma hard
      
      
      if (r1 > 1.- sigh/sigt) {
        r2 = G4UniformRand();
        rejet = 0.;
    while (r2 > rejet) {
          r3 = G4UniformRand();
          beta = (-2./11.)*log(G4Exp(-0.08*11./2.)-r3*11./(2.*cg));
          gbeta = G4Exp(-11.*beta/2.);
          rejet = fbeta(beta)/(8000.*gbeta);
        }
    HardPhotonEnergy = beta * photonEnergy;
      }
      else{
        HardPhotonEnergy = 0.;
      }
      
      photonEnergy -= HardPhotonEnergy;
    
      do
    {
      do 
        {
          if (normF1 / (normF1 + normF2) > G4UniformRand() )
        {
          epsilon = 0.5 - epsilonRange * std::pow(G4UniformRand(), 0.333333) ;
          screen = screenFactor / (epsilon * (1. - epsilon));
          gReject = (ScreenFunction1(screen) - fZ) / f10 ;
        }
          else
        {
          epsilon = epsilonMin + epsilonRange * G4UniformRand();
          screen = screenFactor / (epsilon * (1 - epsilon));
          gReject = (ScreenFunction2(screen) - fZ) / f20 ;
        }
        } while ( gReject < G4UniformRand() );
      
      
      
      if (G4UniformRand()>0.5) epsilon = (1. - epsilon); // Extención de Epsilon hasta 1.
      
      G4double logepsilon = log(epsilon);
      G4double deltaP_R1 = 1. + (a + b*logepsilon + c/logepsilon + d*pow(logepsilon,2.) + e/pow(logepsilon,2.) +
                     f*pow(logepsilon,3.) + gLocal/pow(logepsilon,3.) + h*pow(logepsilon,4.) + i/pow(logepsilon,4.) +
                     j*pow(logepsilon,5.) + k/pow(logepsilon,5.))/100.;
      G4double deltaP_R2 = 1.+((aa + cc*logepsilon +  ee*pow(logepsilon,2.) + gg*pow(logepsilon,3.) + ii*pow(logepsilon,4.))
                   / (1. + bb*logepsilon + dd*pow(logepsilon,2.) + ff*pow(logepsilon,3.) + hh*pow(logepsilon,4.)
                      + jj*pow(logepsilon,5.) ))/100.;
      
      if (epsilon <= 0.5)
        {
          Rechazo = deltaP_R1/NormaRC;
        }
      else
        {
          Rechazo = deltaP_R2/NormaRC;
        }
      //G4cout << Rechazo << " " << NormaRC << " " << epsilon << G4endl;
      
    } while (Rechazo < G4UniformRand() );
      
      electronTotEnergy = (1. - epsilon) * photonEnergy;
      positronTotEnergy = epsilon * photonEnergy;
      
    }   //  End of epsilon sampling
      
  
  // Fix charges randomly
    
  // Scattered electron (positron) angles. ( Z - axis along the parent photon)
  // Universal distribution suggested by L. Urban (Geant3 manual (1993) Phys211),
  // derived from Tsai distribution (Rev. Mod. Phys. 49, 421 (1977)
 
  G4double u;
  const G4double a1 = 0.625;
  G4double a2 = 3. * a1;
  //  G4double d = 27. ;
 
  //  if (9. / (9. + d) > G4UniformRand())
  if (0.25 > G4UniformRand())
    {
      u = - G4Log(G4UniformRand() * G4UniformRand()) / a1 ;
    }
  else
    {
      u = - G4Log(G4UniformRand() * G4UniformRand()) / a2 ;
    }
 
  G4double thetaEle = u*electron_mass_c2/electronTotEnergy;
  G4double thetaPos = u*electron_mass_c2/positronTotEnergy;
  G4double phi  = twopi * G4UniformRand();
 
  G4double dxEle= std::sin(thetaEle)*std::cos(phi),dyEle= std::sin(thetaEle)*std::sin(phi),dzEle=std::cos(thetaEle);
  G4double dxPos=-std::sin(thetaPos)*std::cos(phi),dyPos=-std::sin(thetaPos)*std::sin(phi),dzPos=std::cos(thetaPos);
  
  
  // Kinematics of the created pair:
  // the electron and positron are assumed to have a symetric angular 
  // distribution with respect to the Z axis along the parent photon
  
  G4double electronKineEnergy = std::max(0.,electronTotEnergy - electron_mass_c2) ;
  
  G4ThreeVector electronDirection (dxEle, dyEle, dzEle);
  electronDirection.rotateUz(photonDirection);
      
  G4DynamicParticle* particle1 = new G4DynamicParticle (G4Electron::Electron(),
                            electronDirection,
                            electronKineEnergy);
 
  // The e+ is always created 
  G4double positronKineEnergy = std::max(0.,positronTotEnergy - electron_mass_c2) ;
 
  G4ThreeVector positronDirection (dxPos, dyPos, dzPos);
  positronDirection.rotateUz(photonDirection);   
  
  // Create G4DynamicParticle object for the particle2 
  G4DynamicParticle* particle2 = new G4DynamicParticle(G4Positron::Positron(),
                               positronDirection, 
                               positronKineEnergy);
  // Fill output vector
  fvect->push_back(particle1);
  fvect->push_back(particle2);
   
  if (HardPhotonEnergy > 0.)
    {
      G4double thetaHardPhoton = u*electron_mass_c2/HardPhotonEnergy;
      phi  = twopi * G4UniformRand();
      G4double dxHardP= std::sin(thetaHardPhoton)*std::cos(phi);
      G4double dyHardP= std::sin(thetaHardPhoton)*std::sin(phi);
      G4double dzHardP =std::cos(thetaHardPhoton);
      
      G4ThreeVector hardPhotonDirection (dxHardP, dyHardP, dzHardP);
      hardPhotonDirection.rotateUz(photonDirection);
      G4DynamicParticle* particle3 = new G4DynamicParticle (G4Gamma::Gamma(),
                                hardPhotonDirection,
                                                            HardPhotonEnergy);
      fvect->push_back(particle3);
    }
  
  // kill incident photon
  fParticleChange->SetProposedKineticEnergy(0.);
  fParticleChange->ProposeTrackStatus(fStopAndKill);   
 
}
 
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
 
G4double G4LivermoreGammaConversionModelRC::ScreenFunction1(G4double screenVariable)
{
  // Compute the value of the screening function 3*phi1 - phi2
 
  G4double value;
  
  if (screenVariable > 1.)
    value = 42.24 - 8.368 * G4Log(screenVariable + 0.952);
  else
    value = 42.392 - screenVariable * (7.796 - 1.961 * screenVariable);
  
  return value;
} 
 
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
 
G4double G4LivermoreGammaConversionModelRC::ScreenFunction2(G4double screenVariable)
{
  // Compute the value of the screening function 1.5*phi1 - 0.5*phi2
  
  G4double value;
  
  if (screenVariable > 1.)
    value = 42.24 - 8.368 * G4Log(screenVariable + 0.952);
  else
    value = 41.405 - screenVariable * (5.828 - 0.8945 * screenVariable);
  
  return value;
} 
 
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
 
G4double G4LivermoreGammaConversionModelRC::fbeta(G4double x)
{
   // compute the probabililty distribution for hard photon
   G4double Pi, gamma, eta, d, p1, p2, p3, p4, p5, p6, p7, ffbeta;
   gamma = (1.-x)*(1.-x)/x;
   eta = (1.-x)/(1.+x);
   d = Dilog(1./x)-Dilog(x);
   Pi = 2.*acos(0.);
   p1 = -1.*(25528.*pow(gamma,2) + 116044.* gamma +151556.)/105.;
   p2 = 256.* pow(gamma,3) + 1092.* pow(gamma,2) +1260.*gamma + 420.;
   p3 = (676.*pow(gamma,3) + 9877.*pow(gamma,2) + 58415.*gamma + 62160.)/105.;
   p4 = 64.*pow(gamma,3) + 305.*pow(gamma,2) + 475.*gamma + 269. - 276./gamma;
   p5 = (676.*pow(gamma,3) + 38109.*pow(gamma,2) + 211637.*gamma + 266660. - 53632./gamma)/105.;
   p6 = 32.*pow(gamma,2) + 416.*gamma + 1310. +1184./gamma;
   p7 = 128.*pow(gamma,3) + 802.*pow(gamma,2) + 1028.*gamma - 470. - 1184./gamma;
   ffbeta = (1.-x) * (p1 + p2*Pi*Pi/6. + p3*log(gamma) +
              p4*pow(log(x),2) + (p5 + p6*log(gamma))*eta*log(x) + p7*d*eta);
   return ffbeta;
}
 
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
 
G4double G4LivermoreGammaConversionModelRC::Dilog(G4double y)
{
   G4double fdilog = 0.0;
   G4double Pi = 2.*acos(0.); // serve?
   if (y <= 0.5) {
     fdilog = pow(Pi,2)/6. + (1.-y)*(log(1-y)-1.)+pow((1.-y),2)*((1./2.)*log(1.-y)-1./4.)
       +pow((1.-y),3)*((1./3.)*log(1.-y)-1./9.)+pow((1.-y),4)*((1./4.)*log(1.-y)-1./16.);
   }
   if (0.5 < y && y < 2.) {
     fdilog = 1.-y+pow((1.-y),2)/4.+pow((1.-y),3)/9.+pow((1.-y),4)/16.+
       pow((1.-y),5)/25.+pow((1.-y),6)/36.+pow((1.-y),7)/49.;
   }
   if (y >= 2.) {
     fdilog = -pow(log(y),2)/2. - pow(Pi,2)/6. + (log(y)+1.)/y +
       (log(y)/2.+1./4.)/pow(y,2) + (log(y)/3.+1./9.)/pow(y,3);
   }
   return fdilog;
}
 
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
 
#include "G4AutoLock.hh"
namespace { G4Mutex LivermoreGammaConversionModelRCMutex = G4MUTEX_INITIALIZER; }
 
void G4LivermoreGammaConversionModelRC::InitialiseForElement(
                      const G4ParticleDefinition*, 
                      G4int Z)
{
  G4AutoLock l(&LivermoreGammaConversionModelRCMutex);
  //  G4cout << "G4LivermoreGammaConversionModelRC::InitialiseForElement Z= " 
  //   << Z << G4endl;
  if(!data[Z]) { ReadData(Z); }
  l.unlock();
}
 
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......