G4Be11GEMProbability.cc

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//
// $Id$
//
// Hadronic Process: Nuclear De-excitations
// by V. Lara (Nov 1999)
//
 
#include "G4Be11GEMProbability.hh"
#include "G4SystemOfUnits.hh"
 
G4Be11GEMProbability::G4Be11GEMProbability() :
  G4GEMProbability(11,4,1.0/2.0) // A,Z,Spin
{
  ExcitEnergies.push_back(320.04*keV);
  ExcitSpins.push_back(1.0/2);
  ExcitLifetimes.push_back(115.0e-15*s);
 
  ExcitEnergies.push_back(1778.0*keV);
  ExcitSpins.push_back(5.0/2.0);
  ExcitLifetimes.push_back(fPlanck/(100.0*keV));
 
  ExcitEnergies.push_back(2.69e3*keV);
  ExcitSpins.push_back(3.0/2.0);
  ExcitLifetimes.push_back(fPlanck/(200.0*keV));
 
  ExcitEnergies.push_back(3.41e3*keV);
  ExcitSpins.push_back(3.0/2.0);
  ExcitLifetimes.push_back(fPlanck/(125.0*keV));
 
  ExcitEnergies.push_back(3887.0*keV);
  ExcitSpins.push_back(7.0/2.0);
  ExcitLifetimes.push_back(fPlanck/(10.0*keV));
 
  ExcitEnergies.push_back(3956.0*keV);
  ExcitSpins.push_back(3.0/2.0);
  ExcitLifetimes.push_back(fPlanck/(15.0*keV));
 
  ExcitEnergies.push_back(5240.0*keV);
  ExcitSpins.push_back(0.0);
  ExcitLifetimes.push_back(fPlanck/(45.0*keV));
 
  ExcitEnergies.push_back(5.86e3*keV);
  ExcitSpins.push_back(0.0);
  ExcitLifetimes.push_back(fPlanck/(300.0*keV));
 
  ExcitEnergies.push_back(6.51e3*keV);
  ExcitSpins.push_back(0.0);
  ExcitLifetimes.push_back(fPlanck/(120.0*keV));
 
  ExcitEnergies.push_back(6705.0*keV);
  ExcitSpins.push_back(0.0);
  ExcitLifetimes.push_back(fPlanck/(40.0*keV));
 
  ExcitEnergies.push_back(7.03e3*keV);
  ExcitSpins.push_back(0.0);
  ExcitLifetimes.push_back(fPlanck/(300.0*keV));
 
  ExcitEnergies.push_back(8816.0*keV);
  ExcitSpins.push_back(0.0);
  ExcitLifetimes.push_back(fPlanck/(300.0*keV));
 
  ExcitEnergies.push_back(10.59e3*keV);
  ExcitSpins.push_back(0.0);
  ExcitLifetimes.push_back(fPlanck/(210.0*keV));
}
 
G4Be11GEMProbability::~G4Be11GEMProbability() 
{}