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geant4/source/processes/hadronic/stopping/src/G4PiMinusStopCo.cc
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//
// ********************************************************************
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// * *
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// * This code implementation is the result of the scientific and *
// * technical work of the GEANT4 collaboration. *
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// ********************************************************************
//
// File name: G4PiMinusStopCo
//
// Author: Maria Grazia Pia (pia@genova.infn.it)
//
// Creation date: 8 May 1998
//
// -------------------------------------------------------------------
#include "G4ios.hh"
#include "G4PiMinusStopCo.hh"
#include <vector>
#include "globals.hh"
#include "Randomize.hh"
#include "G4Proton.hh"
#include "G4Neutron.hh"
#include "G4ParticleTypes.hh"
#include "G4ReactionKinematics.hh"
#include "G4DynamicParticleVector.hh"
#include "G4LorentzVector.hh"
#include "G4PiMinusStopMaterial.hh"
#include "G4DistributionGenerator.hh"
// np/pp production ratio
// Experimental values:
// R(np/pp) (E. Gadioli et al., Phys Rev C36 (1987) 741
G4double G4PiMinusStopCo::npRatio = 2.5;
// Average numbers of final nucleons detected, for N-pair absorption
// (Hartmann et al., Nucl. Phys. A300 (1978) 345
G4double G4PiMinusStopCo::nFinalNucleons = 1.38;
// Kinetic energy (MeV) distributions measured for coincident nucleon
// emission
// P. Heusi et al., Nucl. Phys. A407(1983) 429
G4int G4PiMinusStopCo::eKinEntries = 11;
G4double G4PiMinusStopCo::eKinData[11] = {0.085, 0.09, 0.09, 0.15,
0.1, 0.09, 0.08,
0.04, 0.03, 0.02, 0.01};
G4double G4PiMinusStopCo::eKin[12] = { 15., 17.5, 25., 33.,
42., 52., 62.,
75., 85., 95., 105. };
// Opening angle distributions measured for coincident nucleon emission
// (P.Heusi et al., Nucl. Phys. A407 (1983) 429
G4int G4PiMinusStopCo::angleEntries = 7;
G4double G4PiMinusStopCo::angleData[7] =
{6., 8., 9., 10., 25., 40., 45. };
G4double G4PiMinusStopCo::angle[8] = { 0.5, 0.7, 0.87, 1.4, 2.1,
2.44, 2.8, 3.1415927 };
// Constructor
G4PiMinusStopCo::G4PiMinusStopCo()
{
// Cluster size: nucleon pair, alpha, triton etc.
// First implementation: interaction with nucleon pair only
_clusterSize = 2;
// R ratio
theR = 1. / (1. + npRatio);
_definitions = new std::vector<G4ParticleDefinition*>();
_momenta = new std::vector<G4LorentzVector*>();
std::vector<double> eKinVector;
std::vector<double> eKinDataVector;
int i;
for (i=0; i<eKinEntries; i++)
{
eKinVector.push_back(eKin[i]);
eKinDataVector.push_back(eKinData[i]);
}
eKinVector.push_back(eKin[eKinEntries]);
_distributionE = new G4DistributionGenerator(eKinVector,eKinDataVector);
std::vector<double> angleVector;
std::vector<double> angleDataVector;
for (i=0; i<angleEntries; i++)
{
angleVector.push_back(angle[i]);
angleDataVector.push_back(angleData[i]);
}
angleVector.push_back(angle[angleEntries]);
_distributionAngle = new G4DistributionGenerator(angleVector,angleDataVector);
}
// Destructor
G4PiMinusStopCo::~G4PiMinusStopCo()
{}
G4double G4PiMinusStopCo::FinalNucleons()
{
return nFinalNucleons;
}