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//
// $Id: G4Be9GEMProbability.cc,v 1.6 2009/09/15 12:54:16 vnivanch Exp $
// GEANT4 tag $Name: geant4-09-03 $
//
// Hadronic Process: Nuclear De-excitations
// by V. Lara (Nov 1999)
//


#include "G4Be9GEMProbability.hh"

G4Be9GEMProbability::G4Be9GEMProbability() :
  G4GEMProbability(9,4,3.0/2.0) // A,Z,Spin
{
  ExcitEnergies.push_back(1685.0*keV);
  ExcitSpins.push_back(1.0/2.0);
  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(150.0*keV));

  ExcitEnergies.push_back(2429.4*keV);
  ExcitSpins.push_back(5.0/2.0);
  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(0.77*keV));

  ExcitEnergies.push_back(2.78e3*keV);
  ExcitSpins.push_back(1.0/2.0);
  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(1080.0*keV));

  ExcitEnergies.push_back(3049.0*keV);
  ExcitSpins.push_back(5.0/2.0);
  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(282.0*keV));

  ExcitEnergies.push_back(4704.0*keV);
  ExcitSpins.push_back(3.0/2.0);
  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(743.0*keV));

  ExcitEnergies.push_back(6760.0*keV);
  ExcitSpins.push_back(7.0/2.0);
  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(1540.0*keV));

  ExcitEnergies.push_back(7940.0*keV);
  ExcitSpins.push_back(1.0/2.0);
  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(1000.0*keV));

  ExcitEnergies.push_back(11283.0*keV);
  ExcitSpins.push_back(3.0/2.0);
  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(575.0*keV));

  ExcitEnergies.push_back(11810.0*keV);
  ExcitSpins.push_back(0.0);
  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(400.0*keV));

  ExcitEnergies.push_back(13790.0*keV);
  ExcitSpins.push_back(0.0);
  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(590.0*keV));

  ExcitEnergies.push_back(14392.9*keV);
  ExcitSpins.push_back(3.0/2.0);
  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(0.381*keV));

  ExcitEnergies.push_back(14.4e3*keV);
  ExcitSpins.push_back(0.0);
  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(800*keV));

  ExcitEnergies.push_back(15970.0*keV);
  ExcitSpins.push_back(0.0);
  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(300.0*keV));

  ExcitEnergies.push_back(16671.0*keV);
  ExcitSpins.push_back(0.0);
  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(41.0*keV));

  ExcitEnergies.push_back(16975.0*keV);
  ExcitSpins.push_back(1.0/2.0);
  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(0.47*keV));

  ExcitEnergies.push_back(17298.0*keV);
  ExcitSpins.push_back(5.0/2.0);
  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(200.0*keV));

  ExcitEnergies.push_back(17493.0*keV);
  ExcitSpins.push_back(7.0/2.0);
  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(47.0*keV));

  ExcitEnergies.push_back(19200.0*keV);
  ExcitSpins.push_back(0.0);
  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(310.0*keV));

  ExcitEnergies.push_back(20740.0*keV);
  ExcitSpins.push_back(0.0);
  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(1000.0*keV));

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


G4Be9GEMProbability::G4Be9GEMProbability(const G4Be9GEMProbability &) : G4GEMProbability()
{
  throw G4HadronicException(__FILE__, __LINE__, "G4Be9GEMProbability::copy_constructor meant to not be accessable");
}




const G4Be9GEMProbability & G4Be9GEMProbability::
operator=(const G4Be9GEMProbability &)
{
  throw G4HadronicException(__FILE__, __LINE__, "G4Be9GEMProbability::operator= meant to not be accessable");
  return *this;
}


G4bool G4Be9GEMProbability::operator==(const G4Be9GEMProbability &) const
{
  return false;
}

G4bool G4Be9GEMProbability::operator!=(const G4Be9GEMProbability &) const
{
  return true;
}



