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//
// $Id: G4B10GEMProbability.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 "G4B10GEMProbability.hh"

G4B10GEMProbability::G4B10GEMProbability() :
  G4GEMProbability(10,5,3.0) // A,Z,Spin
{
    ExcitEnergies.push_back(718.35*keV);
    ExcitSpins.push_back(1.0);
    ExcitLifetimes.push_back(0.707e-9*s);

    ExcitEnergies.push_back(1740.15*keV);
    ExcitSpins.push_back(0.0);
    ExcitLifetimes.push_back(5.0e-15*s);

    ExcitEnergies.push_back(2154.3*keV);
    ExcitSpins.push_back(1.0);
    ExcitLifetimes.push_back(1.48e-12*s);

    ExcitEnergies.push_back(3587.1*keV);
    ExcitSpins.push_back(2.0);
    ExcitLifetimes.push_back(106.0e-15*s);

    ExcitEnergies.push_back(4774.0*keV);
    ExcitSpins.push_back(3.0);
    ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(8.7*keV));

    ExcitEnergies.push_back(5110.3*keV);
    ExcitSpins.push_back(2.0);
    ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(0.98*keV));

    ExcitEnergies.push_back(5163.9*keV);
    ExcitSpins.push_back(2.0);
    ExcitLifetimes.push_back(4.2e-15*s);

    ExcitEnergies.push_back(5180.0*keV);
    ExcitSpins.push_back(1.0);
    ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(110.0*keV));

    ExcitEnergies.push_back(5919.5*keV);
    ExcitSpins.push_back(2.0);
    ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(6.0*keV));

    ExcitEnergies.push_back(6025.0*keV);
    ExcitSpins.push_back(4.0);
    ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(0.05*keV));

    ExcitEnergies.push_back(6127.2*keV);
    ExcitSpins.push_back(3.0);
    ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(2.36*keV));

    ExcitEnergies.push_back(6561.0*keV);
    ExcitSpins.push_back(4.0);
    ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(25.1*keV));

    ExcitEnergies.push_back(6873.0*keV);
    ExcitSpins.push_back(1.0);
    ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(120.0*keV));

    ExcitEnergies.push_back(7002.0*keV);
    ExcitSpins.push_back(2.0);
    ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(100.0*keV));

    ExcitEnergies.push_back(7430.0*keV);
    ExcitSpins.push_back(2.0);
    ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(100.0*keV));

    ExcitEnergies.push_back(7467.0*keV);
    ExcitSpins.push_back(1.0);
    ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(65.0*keV));

    ExcitEnergies.push_back(7479.0*keV);
    ExcitSpins.push_back(2.0);
    ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(74.0*keV));

    ExcitEnergies.push_back(7560.7*keV);
    ExcitSpins.push_back(0.0);
    ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(2.65*keV));

    ExcitEnergies.push_back(7670.0*keV);
    ExcitSpins.push_back(1.0);
    ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(250.0*keV));

    ExcitEnergies.push_back(7819.0*keV);
    ExcitSpins.push_back(1.0);
    ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(260.0*keV));

    ExcitEnergies.push_back(8070.0*keV);
    ExcitSpins.push_back(2.0);
    ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(800.0*keV));

    ExcitEnergies.push_back(8700.0*keV);
    ExcitSpins.push_back(1.0);
    ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(200.0*keV));

    ExcitEnergies.push_back(8889.0*keV);
    ExcitSpins.push_back(3.0);
    ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(84.0*keV));

    ExcitEnergies.push_back(8895.0*keV);
    ExcitSpins.push_back(2.0);
    ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(40.0*keV));

    ExcitEnergies.push_back(9700.0*keV);
    ExcitSpins.push_back(0.0);
    ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(700.0*keV));

    ExcitEnergies.push_back(10840.0*keV);
    ExcitSpins.push_back(4.0);
    ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(300.0*keV));

    ExcitEnergies.push_back(11520.0*keV);
    ExcitSpins.push_back(0.0);
    ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(500.0*keV));

    ExcitEnergies.push_back(12560.0*keV);
    ExcitSpins.push_back(2.0);
    ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(100.0*keV));

    ExcitEnergies.push_back(13490.0*keV);
    ExcitSpins.push_back(2.0);
    ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(300.0*keV));

    ExcitEnergies.push_back(14.4e3*keV);
    ExcitSpins.push_back(0.0);
    ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(800.0*keV));

    ExcitEnergies.push_back(18.2e3*keV);
    ExcitSpins.push_back(0.0);
    ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(1500.0*keV));

    ExcitEnergies.push_back(18430.0*keV);
    ExcitSpins.push_back(2.0);
    ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(340.0*keV));

    ExcitEnergies.push_back(18800.0*keV);
    ExcitSpins.push_back(1.0);
    ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(600.0*keV));

    ExcitEnergies.push_back(19290.0*keV);
    ExcitSpins.push_back(2.0);
    ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(190.0*keV));


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


G4B10GEMProbability::G4B10GEMProbability(const G4B10GEMProbability &) : G4GEMProbability()
{
  throw G4HadronicException(__FILE__, __LINE__, "G4B10GEMProbability::copy_constructor meant to not be accessable");}




const G4B10GEMProbability & G4B10GEMProbability::
operator=(const G4B10GEMProbability &)
{
  throw G4HadronicException(__FILE__, __LINE__, "G4B10GEMProbability::operator= meant to not be accessable");
  return *this;
}


G4bool G4B10GEMProbability::operator==(const G4B10GEMProbability &) const
{
  return false;
}

G4bool G4B10GEMProbability::operator!=(const G4B10GEMProbability &) const
{
  return true;
}



