source: trunk/source/processes/hadronic/models/de_excitation/fermi_breakup/src/G4FermiConfigurationList.cc @ 1199

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//
// Hadronic Process: Nuclear De-excitations
// by V. Lara (Nov 1998)

#include "G4FermiConfigurationList.hh"
#include "G4FermiSplitter.hh"
#include "G4HadronicException.hh"

G4FermiFragmentsPool & G4FermiConfigurationList::GetFragmentsPoolInstance()
{
  static G4FermiFragmentsPool theFragmentsPool;
  return theFragmentsPool;
}

G4FermiConfigurationList::G4FermiConfigurationList()
{
}

G4FermiConfigurationList::G4FermiConfigurationList(const G4FermiConfigurationList &)
{
  throw G4HadronicException(__FILE__, __LINE__, "G4FermiConfigurationList::copy_constructor meant to not be accessable");
}


const G4FermiConfigurationList & G4FermiConfigurationList::
operator=(const G4FermiConfigurationList &)
{
  throw G4HadronicException(__FILE__, __LINE__, "G4FermiConfigurationList::operator= meant to not be accessable");
  return *this;
}


G4bool G4FermiConfigurationList::operator==(const G4FermiConfigurationList &) const
{
  return false;
}

G4bool G4FermiConfigurationList::operator!=(const G4FermiConfigurationList &) const
{
  return true;
}



G4bool G4FermiConfigurationList::
Initialize(const G4int A, const G4int Z, const G4double TotalEnergyRF)
{
  //
  // let's split nucleus into k = 2,...,A fragments
  //
  Configurations.clear();
  NormalizedWeights.clear();
  G4FermiSplitter aSplitter(&GetFragmentsPoolInstance());
  G4double NormStatWeight = 0.0;
  for (G4int k = 2; k <= A; k++) 
    {
      // Initialize Configuration for k fragments
      aSplitter.Initialize(A,Z,k);
      for (G4int i = 0; i < aSplitter.GetNumberOfSplits(); i++)
        {
          // Create a configuration from a split
          G4FermiConfiguration * aConfiguration = new G4FermiConfiguration(aSplitter.GetSplit(i));

          // Store configuration
          Configurations.push_back(aConfiguration);
                    
          // Non-Normalized statistical weight for given channel with k fragments
          G4double StatWeight = aConfiguration->DecayProbability(A,TotalEnergyRF);
          NormStatWeight += StatWeight;
          // Statistical weights (it will be normalized...)
          NormalizedWeights.push_back(StatWeight);      
        } 
    }
  
  if (NormStatWeight > 0.0) 
    {
      // Let's normalize statistical weights of channels
      std::transform(NormalizedWeights.begin(), NormalizedWeights.end(), 
                     NormalizedWeights.begin(),
                     std::bind2nd(std::divides<G4double>(),NormStatWeight));
      return true;
    }

  return false;
}



G4FermiConfiguration G4FermiConfigurationList::ChooseConfiguration(void)
{
  G4double RandomWeight =  G4UniformRand();
  G4double AcumWeight = 0.0;
  std::vector<G4double>::iterator thisConfig;
  for (thisConfig = NormalizedWeights.begin(); thisConfig != NormalizedWeights.end(); ++thisConfig)
    {
      // We are adding the prob. of each configuration
      AcumWeight += *thisConfig; 
      if (AcumWeight >= RandomWeight) break;
    } 
  if (thisConfig == NormalizedWeights.end())
    {
      throw G4HadronicException(__FILE__, __LINE__, "G4FermiConfigurationList::ChooseConfigration: Cannot choose a configuration");
      G4FermiConfiguration dummy;
      return dummy;
    }
  else 
    {
#ifdef G4NO_ISO_VECDIST
      std::vector<G4double>::difference_type n = 0;
      std::distance(NormalizedWeights.begin(),thisConfig,n);
      return *(Configurations[n]);
#else
      return *(Configurations[std::distance(NormalizedWeights.begin(),thisConfig)]);
#endif
    }
}