source: trunk/source/processes/hadronic/models/pre_equilibrium/exciton_model/include/G4PreCompoundEmission.icc @ 1337

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// $Id: G4PreCompoundEmission.icc,v 1.5 2009/02/10 16:01:37 vnivanch Exp $
// GEANT4 tag $Name: geant4-09-04-beta-01 $
//
//
// Author:         V.Lara
//
// Modified:  
// 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 void G4PreCompoundEmission::Initialize(const G4Fragment & aFragment) 
{
  theFragmentsVector->Initialize(aFragment);
  return;
}

inline G4double G4PreCompoundEmission::GetTotalProbability(const G4Fragment & aFragment) 
{
  return theFragmentsVector->CalculateProbabilities(aFragment);
}

inline void G4PreCompoundEmission::SetUp(const G4Fragment & aFragment)
{
  // This should be the projectile energy. If I would know which is the projectile (proton, neutron)
  // I could remove the binding energy. But, what happens if INC precedes precompound? This approximation
  // seems to work well enough
  ProjEnergy = aFragment.GetExcitationEnergy();
  theIncidentDirection = aFragment.GetMomentum().vect().unit();
  theFragmentsVector->ResetStage();
  return;
}

//for inverse cross section choice
inline void G4PreCompoundEmission::SetOPTxs(G4int opt)
{
  theFragmentsVector->SetOPTxs(opt);
  return;
}
//for superimposed Coumlomb Barrier for inverse cross sections 
inline void G4PreCompoundEmission::UseSICB(G4bool use)
{
  theFragmentsVector->UseSICB(use);
  return;
}