source: trunk/source/processes/hadronic/models/de_excitation/gem_evaporation/src/G4B12GEMProbability.cc @ 1337

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// $Id: G4B12GEMProbability.cc,v 1.6 2009/09/15 12:54:16 vnivanch Exp $
// GEANT4 tag $Name: geant4-09-04-beta-01 $
//
// Hadronic Process: Nuclear De-excitations
// by V. Lara (Nov 1999)
//


#include "G4B12GEMProbability.hh"

G4B12GEMProbability::G4B12GEMProbability() :
  G4GEMProbability(12,5,1.0) // A,Z,Spin
{
    ExcitEnergies.push_back(953.14*keV);
    ExcitSpins.push_back(2.0);
    ExcitLifetimes.push_back(180.0e-15*s);

    ExcitEnergies.push_back(1673.65*keV);
    ExcitSpins.push_back(2.0);
    ExcitLifetimes.push_back(35.0e-15*s);

    ExcitEnergies.push_back(2620.8*keV);
    ExcitSpins.push_back(1.0);
    ExcitLifetimes.push_back(49.0e-15*s);

    ExcitEnergies.push_back(3388.3*keV);
    ExcitSpins.push_back(3.0);
    ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(3.1*eV));

    ExcitEnergies.push_back(3759.0*keV);
    ExcitSpins.push_back(2.0);
    ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(40*keV));

    ExcitEnergies.push_back(4301*keV);
    ExcitSpins.push_back(1.0);
    ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(9*keV));

    ExcitEnergies.push_back(4518*keV);
    ExcitSpins.push_back(4.0);
    ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(110*keV));

    ExcitEnergies.push_back(5.00E+3*keV);
    ExcitSpins.push_back(1.0);
    ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(50*keV));

    ExcitEnergies.push_back(5612*keV);
    ExcitSpins.push_back(3.0);
    ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(110*keV));

    ExcitEnergies.push_back(5726*keV);
    ExcitSpins.push_back(3.0);
    ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(50*keV));

    ExcitEnergies.push_back(6.6E+3*keV);
    ExcitSpins.push_back(1.0);
    ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(140*keV));

    ExcitEnergies.push_back(7.67E+3*keV);
    ExcitSpins.push_back(2.0);
    ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(45*keV));

    ExcitEnergies.push_back(7836*keV);
    ExcitSpins.push_back(1.0);
    ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(60*keV));

    ExcitEnergies.push_back(7937*keV);
    ExcitSpins.push_back(1.0);
    ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(27*keV));

    ExcitEnergies.push_back(8.24E+3*keV);
    ExcitSpins.push_back(3.0);
    ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(65*keV));

    ExcitEnergies.push_back(8.58E+3*keV);
    ExcitSpins.push_back(3.0);
    ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(75*keV));

    ExcitEnergies.push_back(9040*keV);
    ExcitSpins.push_back(1.0);
    ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(95*keV));

    ExcitEnergies.push_back(9585*keV);
    ExcitSpins.push_back(3.0);
    ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(34*keV));

    ExcitEnergies.push_back(1.275E+4*keV);
    ExcitSpins.push_back(0.0);
    ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(85*keV));

    ExcitEnergies.push_back(1.482E+4*keV);
    ExcitSpins.push_back(2.0);
    ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(200*keV));

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


G4B12GEMProbability::G4B12GEMProbability(const G4B12GEMProbability &) : G4GEMProbability()
{
  throw G4HadronicException(__FILE__, __LINE__, "G4B12GEMProbability::copy_constructor meant to not be accessable");}




const G4B12GEMProbability & G4B12GEMProbability::
operator=(const G4B12GEMProbability &)
{
  throw G4HadronicException(__FILE__, __LINE__, "G4B12GEMProbability::operator= meant to not be accessable");
  return *this;
}


G4bool G4B12GEMProbability::operator==(const G4B12GEMProbability &) const
{
  return false;
}

G4bool G4B12GEMProbability::operator!=(const G4B12GEMProbability &) const
{
  return true;
}