source: trunk/source/processes/hadronic/models/pre_equilibrium/exciton_model/include/G4PreCompoundFragmentVector.icc @ 978

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// $Id: G4PreCompoundFragmentVector.icc,v 1.4 2008/09/22 10:18:36 ahoward Exp $
// GEANT4 tag $Name: geant4-09-02-ref-02 $
//
// Hadronic Process: Nuclear Preequilibrium
// by V. Lara 
//
// Modif (03 September 2008) by J. M. Quesada for external choice of inverse 
// cross section option
// JMQ (06 September 2008) Also external choice has been added for:
//                      - superimposed Coulomb barrier (if useSICB=true) 

inline G4PreCompoundFragmentVector::G4PreCompoundFragmentVector(pcfvector * avector) :
  theChannels(avector), TotalEmissionProbability(0.0)
{
}


inline G4PreCompoundFragmentVector::~G4PreCompoundFragmentVector()
{
}

inline void G4PreCompoundFragmentVector::SetVector(pcfvector * avector)
{
  theChannels = avector;
}

inline void 
G4PreCompoundFragmentVector::
Initialize(const G4Fragment & aFragment)
{
    TotalEmissionProbability = 0.0;
    for (pcfvector::iterator i=theChannels->begin(); 
         i != theChannels->end(); i++) (*i)->Initialize(aFragment);
    return;
}

inline void G4PreCompoundFragmentVector::
ResetStage()
{
  for (pcfvector::iterator i=theChannels->begin(); i != theChannels->end(); i++)
    (*i)->ResetStage();
  return;
}

//for inverse cross section choice
inline void G4PreCompoundFragmentVector::
SetOPTxs(G4int opt)
{    
  for (pcfvector::iterator i = theChannels->begin(); i != theChannels->end(); ++i) 
    (*i)->SetOPTxs(opt);
  return;
}

//for superimposed Coulomb Barrier for inverse  cross sections 
inline void G4PreCompoundFragmentVector::
UseSICB(G4bool use)
{    
  for (pcfvector::iterator i = theChannels->begin(); i != theChannels->end(); ++i) 
    (*i)->UseSICB(use);
  return;
}