source: trunk/source/processes/hadronic/models/de_excitation/gem_evaporation/src/G4C15GEMProbability.cc @ 1340

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// $Id: G4C15GEMProbability.cc,v 1.6 2009/09/15 12:54:16 vnivanch Exp $
// GEANT4 tag $Name: geant4-09-03-ref-09 $
//
// Hadronic Process: Nuclear De-excitations
// by V. Lara (Nov 1999)
//


#include "G4C15GEMProbability.hh"

G4C15GEMProbability::G4C15GEMProbability() :
  G4GEMProbability(15,6,1.0/2.0) // A,Z,Spin
{

  ExcitEnergies.push_back(740.0*keV);
  ExcitSpins.push_back(5.0/2.0);
  ExcitLifetimes.push_back(2.61e-9*s);

  ExcitEnergies.push_back(3105*keV);
  ExcitSpins.push_back(1.0/2.0);
  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(40*keV));

  ExcitEnergies.push_back(4221*keV);
  ExcitSpins.push_back(5.0/2.0);
  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(14*keV));

  ExcitEnergies.push_back(6370*keV);
  ExcitSpins.push_back(9.0/2.0);
  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(20*keV));

  ExcitEnergies.push_back(6429*keV);
  ExcitSpins.push_back(7.0/2.0);
  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(50*keV));

  ExcitEnergies.push_back(6461*keV);
  ExcitSpins.push_back(11.0/2.0);
  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(14*keV));

  ExcitEnergies.push_back(6639*keV);
  ExcitSpins.push_back(3.0/2.0);
  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(20*keV));

  ExcitEnergies.push_back(6845*keV);
  ExcitSpins.push_back(11.0/2.0);
  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(14*keV));

  ExcitEnergies.push_back(6884*keV);
  ExcitSpins.push_back(9.0/2.0);
  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(20*keV));

  ExcitEnergies.push_back(7098*keV);
  ExcitSpins.push_back(3.0/2.0);
  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(15*keV));

  ExcitEnergies.push_back(7352*keV);
  ExcitSpins.push_back(11.0/2.0);
  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(20*keV));

  ExcitEnergies.push_back(8470*keV);
  ExcitSpins.push_back(13.0/2.0);
  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(40*keV));

  ExcitEnergies.push_back(8559*keV);
  ExcitSpins.push_back(13.0/2.0);
  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(40*keV));

  ExcitEnergies.push_back(9789*keV);
  ExcitSpins.push_back(15.0/2.0);
  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(20*keV));

  ExcitEnergies.push_back(10248*keV);
  ExcitSpins.push_back(9.0/2.0);
  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(20*keV));

  ExcitEnergies.push_back(11123*keV);
  ExcitSpins.push_back(19.0/2.0);
  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(30*keV));

  ExcitEnergies.push_back(11825*keV);
  ExcitSpins.push_back(13.0/2.0);
  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(70*keV));

  SetExcitationEnergiesPtr(&ExcitEnergies);
  SetExcitationSpinsPtr(&ExcitSpins);
  SetExcitationLifetimesPtr(&ExcitLifetimes);
}


G4C15GEMProbability::G4C15GEMProbability(const G4C15GEMProbability &) : G4GEMProbability()
{
  throw G4HadronicException(__FILE__, __LINE__, "G4C15GEMProbability::copy_constructor meant to not be accessable");
}




const G4C15GEMProbability & G4C15GEMProbability::
operator=(const G4C15GEMProbability &)
{
  throw G4HadronicException(__FILE__, __LINE__, "G4C15GEMProbability::operator= meant to not be accessable");
  return *this;
}


G4bool G4C15GEMProbability::operator==(const G4C15GEMProbability &) const
{
  return false;
}

G4bool G4C15GEMProbability::operator!=(const G4C15GEMProbability &) const
{
  return true;
}