source: trunk/source/processes/hadronic/models/pre_equilibrium/exciton_model/src/G4PreCompoundFragment.cc @ 1340

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// $Id: G4PreCompoundFragment.cc,v 1.9 2010/08/28 15:16:55 vnivanch Exp $
// GEANT4 tag $Name: geant4-09-03-ref-09 $
//
// J. M. Quesada (August 2008).  
// Based  on previous work by V. Lara
//
// Modified:
// 06.09.2008 JMQ Also external choice has been added for:
//               - superimposed Coulomb barrier (if useSICB=true) 
// 20.08.2010 V.Ivanchenko cleanup
//

#include "G4PreCompoundFragment.hh"

G4PreCompoundFragment::
G4PreCompoundFragment(const G4ParticleDefinition* part,
                      G4VCoulombBarrier* aCoulombBarrier)
  : G4VPreCompoundFragment(part,aCoulombBarrier)
{}

G4PreCompoundFragment::~G4PreCompoundFragment()
{}

G4double G4PreCompoundFragment::
CalcEmissionProbability(const G4Fragment & aFragment)
{
  //G4cout << theCoulombBarrier << "  " << GetMaximalKineticEnergy() << G4endl;
  // If  theCoulombBarrier effect is included in the emission probabilities
  //if (GetMaximalKineticEnergy() <= 0.0) 
  G4double limit = 0.0;
  if(OPTxs==0 ||  useSICB) { limit = theCoulombBarrier; }
  if (GetMaximalKineticEnergy() <= limit) 
    {
      theEmissionProbability = 0.0;
      return 0.0;
    }    
  // If  theCoulombBarrier effect is included in the emission probabilities
  //  G4double LowerLimit = 0.;
  // Coulomb barrier is the lower limit 
  // of integration over kinetic energy
  G4double LowerLimit = limit;

  // Excitation energy of nucleus after fragment emission is the upper 
  //limit of integration over kinetic energy
  G4double UpperLimit = GetMaximalKineticEnergy();
  
  theEmissionProbability = 
    IntegrateEmissionProbability(LowerLimit,UpperLimit,aFragment);
  /*
  G4cout << "## G4PreCompoundFragment::CalcEmisProb "
         << "Z= " << aFragment.GetZ_asInt() 
         << " A= " << aFragment.GetA_asInt()
         << " Elow= " << LowerLimit/MeV
         << " Eup= " << UpperLimit/MeV
         << " prob= " << theEmissionProbability
         << G4endl;
  */
  return theEmissionProbability;
}

G4double G4PreCompoundFragment::
IntegrateEmissionProbability(G4double Low, G4double Up,
                             const G4Fragment & aFragment)
{
  static const G4int N = 10;
  // 10-Points Gauss-Legendre abcisas and weights
  static const G4double w[N] = {
    0.0666713443086881,
    0.149451349150581,
    0.219086362515982,
    0.269266719309996,
    0.295524224714753,
    0.295524224714753,
    0.269266719309996,
    0.219086362515982,
    0.149451349150581,
    0.0666713443086881
  };
  static const G4double x[N] = {
    -0.973906528517172,
    -0.865063366688985,
    -0.679409568299024,
    -0.433395394129247,
    -0.148874338981631,
    0.148874338981631,
    0.433395394129247,
    0.679409568299024,
    0.865063366688985,
    0.973906528517172
  };
  
  G4double Total = 0.0;

  for (G4int i = 0; i < N; ++i) 
    {
      G4double KineticE = 0.5*((Up-Low)*x[i]+(Up+Low));
      Total += w[i]*ProbabilityDistributionFunction(KineticE, aFragment);
    }
  Total  *= 0.5*(Up-Low);
  return Total;
}

G4double G4PreCompoundFragment::
GetKineticEnergy(const G4Fragment & aFragment) 
{
  //let's keep this way for consistency with CalcEmissionProbability method
  G4double V = 0.0;
  if(OPTxs==0 || useSICB) { V = theCoulombBarrier; }

  G4double Tmax = GetMaximalKineticEnergy();  
  if(Tmax < V) { return 0.0; }
  G4double T(0.0);
  G4double Probability(1.0);
  G4double maxProbability = GetEmissionProbability();
  do 
    {
      T = V + G4UniformRand()*(Tmax-V);
      Probability = ProbabilityDistributionFunction(T,aFragment);      
    }   while (maxProbability*G4UniformRand() > Probability);  
  return T;
}