G4ParticleHPFissionFS.cc

Go to the documentation of this file.

//
// ********************************************************************
// * License and Disclaimer                                           *
// *                                                                  *
// * The  Geant4 software  is  copyright of the Copyright Holders  of *
// * the Geant4 Collaboration.  It is provided  under  the terms  and *
// * conditions of the Geant4 Software License,  included in the file *
// * LICENSE and available at  http://cern.ch/geant4/license .  These *
// * include a list of copyright holders.                             *
// *                                                                  *
// * Neither the authors of this software system, nor their employing *
// * institutes,nor the agencies providing financial support for this *
// * work  make  any representation or  warranty, express or implied, *
// * regarding  this  software system or assume any liability for its *
// * use.  Please see the license in the file  LICENSE  and URL above *
// * for the full disclaimer and the limitation of liability.         *
// *                                                                  *
// * This  code  implementation is the result of  the  scientific and *
// * technical work of the GEANT4 collaboration.                      *
// * By using,  copying,  modifying or  distributing the software (or *
// * any work based  on the software)  you  agree  to acknowledge its *
// * use  in  resulting  scientific  publications,  and indicate your *
// * acceptance of all terms of the Geant4 Software license.          *
// ********************************************************************
//
// neutron_hp -- source file
// J.P. Wellisch, Nov-1996
// A prototype of the low energy neutron transport model.
//
// 12-Apr-06 fix in delayed neutron and photon emission without FS data by T. Koi
// 07-Sep-11 M. Kelsey -- Follow change to G4HadFinalState interface
// P. Arce, June-2014 Conversion neutron_hp to particle_hp
//
 
#include "G4ParticleHPFissionFS.hh"
 
#include "G4DynamicParticleVector.hh"
#include "G4Exp.hh"
#include "G4IonTable.hh"
#include "G4Nucleus.hh"
#include "G4ParticleHPFissionERelease.hh"
#include "G4PhysicalConstants.hh"
#include "G4PhysicsModelCatalog.hh"
 
G4ParticleHPFissionFS::G4ParticleHPFissionFS()
{
  secID = G4PhysicsModelCatalog::GetModelID("model_NeutronHPFission");
  hasXsec = false;
  produceFissionFragments = false;
}
 
void G4ParticleHPFissionFS::Init(G4double A, G4double Z, G4int M, const G4String& dirName,
                                 const G4String& aFSType, G4ParticleDefinition* projectile)
{
  theFS.Init(A, Z, M, dirName, aFSType, projectile);
  theFC.Init(A, Z, M, dirName, aFSType, projectile);
  theSC.Init(A, Z, M, dirName, aFSType, projectile);
  theTC.Init(A, Z, M, dirName, aFSType, projectile);
  theLC.Init(A, Z, M, dirName, aFSType, projectile);
 
  theFF.Init(A, Z, M, dirName, aFSType, projectile);
  if (G4ParticleHPManager::GetInstance()->GetProduceFissionFragments() && theFF.HasFSData()) {
    G4cout << "Fission fragment production is now activated in HP package for "
           << "Z = " << (G4int)Z << ", A = " << (G4int)A << G4endl;
    G4cout << "As currently modeled this option precludes production of delayed neutrons from "
              "fission fragments."
           << G4endl;
    produceFissionFragments = true;
  }
}
 
G4HadFinalState* G4ParticleHPFissionFS::ApplyYourself(const G4HadProjectile& theTrack)
{
  // Because it may change by UI command
  produceFissionFragments = G4ParticleHPManager::GetInstance()->GetProduceFissionFragments();
 
  // prepare neutron
  if (theResult.Get() == nullptr) theResult.Put(new G4HadFinalState);
  theResult.Get()->Clear();
  G4double eKinetic = theTrack.GetKineticEnergy();
  const G4HadProjectile* incidentParticle = &theTrack;
  G4ReactionProduct theNeutron(
    const_cast<G4ParticleDefinition*>(incidentParticle->GetDefinition()));
  theNeutron.SetMomentum(incidentParticle->Get4Momentum().vect());
  theNeutron.SetKineticEnergy(eKinetic);
 
  // prepare target
  G4Nucleus aNucleus;
  G4ReactionProduct theTarget;
  G4double targetMass = theFS.GetMass();
  G4ThreeVector neuVelo =
    (1. / incidentParticle->GetDefinition()->GetPDGMass()) * theNeutron.GetMomentum();
  theTarget =
    aNucleus.GetBiasedThermalNucleus(targetMass, neuVelo, theTrack.GetMaterial()->GetTemperature());
  theTarget.SetDefinition(
    G4IonTable::GetIonTable()->GetIon(G4int(theBaseZ), G4int(theBaseA), 0.0));  // TESTPHP
 
  // set neutron and target in the FS classes
  theFS.SetNeutronRP(theNeutron);
  theFS.SetTarget(theTarget);
  theFC.SetNeutronRP(theNeutron);
  theFC.SetTarget(theTarget);
  theSC.SetNeutronRP(theNeutron);
  theSC.SetTarget(theTarget);
  theTC.SetNeutronRP(theNeutron);
  theTC.SetTarget(theTarget);
  theLC.SetNeutronRP(theNeutron);
  theLC.SetTarget(theTarget);
  theFF.SetNeutronRP(theNeutron);
  theFF.SetTarget(theTarget);
 
  // boost to target rest system and decide on channel.
  theNeutron.Lorentz(theNeutron, -1 * theTarget);
 
  // dice the photons
 
  G4DynamicParticleVector* thePhotons;
  thePhotons = theFS.GetPhotons();
 
  // select the FS in charge
 
  eKinetic = theNeutron.GetKineticEnergy();
  G4double xSec[4];
  xSec[0] = theFC.GetXsec(eKinetic);
  xSec[1] = xSec[0] + theSC.GetXsec(eKinetic);
  xSec[2] = xSec[1] + theTC.GetXsec(eKinetic);
  xSec[3] = xSec[2] + theLC.GetXsec(eKinetic);
  G4int it;
  unsigned int i = 0;
  G4double random = G4UniformRand();
  if (xSec[3] == 0) {
    it = -1;
  }
  else {
    for (i = 0; i < 4; i++) {
      it = i;
      if (random < xSec[i] / xSec[3]) break;
    }
  }
 
  // dice neutron multiplicities, energies and momenta in Lab. @@
  // no energy conservation on an event-to-event basis. we rely on the data to be ok. @@
  // also for mean, we rely on the consistancy of the data. @@
 
  G4int Prompt = 0, delayed = 0, all = 0;
  G4DynamicParticleVector* theNeutrons = nullptr;
  switch (it)  // check logic, and ask, if partials can be assumed to correspond to individual
               // particles @@@
  {
    case 0:
      theFS.SampleNeutronMult(all, Prompt, delayed, eKinetic, 0);
      if (Prompt == 0 && delayed == 0) Prompt = all;
      theNeutrons = theFC.ApplyYourself(Prompt);  // delayed always in FS
      // take 'U' into account explicitly (see 5.4) in the sampling of energy @@@@
      break;
    case 1:
      theFS.SampleNeutronMult(all, Prompt, delayed, eKinetic, 1);
      if (Prompt == 0 && delayed == 0) Prompt = all;
      theNeutrons = theSC.ApplyYourself(Prompt);  // delayed always in FS, off done in FSFissionFS
      break;
    case 2:
      theFS.SampleNeutronMult(all, Prompt, delayed, eKinetic, 2);
      if (Prompt == 0 && delayed == 0) Prompt = all;
      theNeutrons = theTC.ApplyYourself(Prompt);  // delayed always in FS
      break;
    case 3:
      theFS.SampleNeutronMult(all, Prompt, delayed, eKinetic, 3);
      if (Prompt == 0 && delayed == 0) Prompt = all;
      theNeutrons = theLC.ApplyYourself(Prompt);  // delayed always in FS
      break;
    default:
      break;
  }
 
  // dice delayed neutrons and photons, and fallback
  // for Prompt in case channel had no FS data; add all paricles to FS.
 
  if (produceFissionFragments) delayed = 0;
 
  G4double* theDecayConstants;
 
  if (theNeutrons != nullptr) {
    theDecayConstants = new G4double[delayed];
    for (i = 0; i < theNeutrons->size(); ++i) {
      theResult.Get()->AddSecondary(theNeutrons->operator[](i), secID);
    }
    delete theNeutrons;
 
    G4DynamicParticleVector* theDelayed = nullptr;
    theDelayed = theFS.ApplyYourself(0, delayed, theDecayConstants);
    for (i = 0; i < theDelayed->size(); i++) {
      G4double time = -G4Log(G4UniformRand()) / theDecayConstants[i];
      time += theTrack.GetGlobalTime();
      theResult.Get()->AddSecondary(theDelayed->operator[](i), secID);
      theResult.Get()->GetSecondary(theResult.Get()->GetNumberOfSecondaries() - 1)->SetTime(time);
    }
    delete theDelayed;
  }
  else {
    theFS.SampleNeutronMult(all, Prompt, delayed, eKinetic, 0);
    theDecayConstants = new G4double[delayed];
    if (Prompt == 0 && delayed == 0) Prompt = all;
    theNeutrons = theFS.ApplyYourself(Prompt, delayed, theDecayConstants);
    G4int i0;
    for (i0 = 0; i0 < Prompt; ++i0) {
      theResult.Get()->AddSecondary(theNeutrons->operator[](i0), secID);
    }
 
    for (i0 = Prompt; i0 < Prompt + delayed; ++i0) {
      // Protect against the very rare case of division by zero
      G4double time = 0.0;
      if (theDecayConstants[i0 - Prompt] > 1.0e-30) {
        time = -G4Log(G4UniformRand()) / theDecayConstants[i0 - Prompt];
      }
      else {
        G4ExceptionDescription ed;
        ed << " theDecayConstants[i0-Prompt]=" << theDecayConstants[i0 - Prompt]
           << "   -> cannot sample the time : set it to 0.0 !" << G4endl;
        G4Exception("G4ParticleHPFissionFS::ApplyYourself ", "HAD_FISSIONHP_001", JustWarning, ed);
      }
 
      time += theTrack.GetGlobalTime();
      theResult.Get()->AddSecondary(theNeutrons->operator[](i0), secID);
      theResult.Get()->GetSecondary(theResult.Get()->GetNumberOfSecondaries() - 1)->SetTime(time);
    }
    delete theNeutrons;
  }
  delete[] theDecayConstants;
 
  std::size_t nPhotons = 0;
  if (thePhotons != nullptr) {
    nPhotons = thePhotons->size();
    for (i = 0; i < nPhotons; ++i) {
      theResult.Get()->AddSecondary(thePhotons->operator[](i), secID);
    }
    delete thePhotons;
  }
 
  // finally deal with local energy depositions.
 
  G4ParticleHPFissionERelease* theERelease = theFS.GetEnergyRelease();
  G4double eDepByFragments = theERelease->GetFragmentKinetic();
  // theResult.SetLocalEnergyDeposit(eDepByFragments);
  if (!produceFissionFragments) theResult.Get()->SetLocalEnergyDeposit(eDepByFragments);
  // clean up the primary neutron
  theResult.Get()->SetStatusChange(stopAndKill);
 
  if (produceFissionFragments) {
    G4int fragA_Z = 0;
    G4int fragA_A = 0;
    G4int fragA_M = 0;
    // System is traget rest!
    theFF.GetAFissionFragment(eKinetic, fragA_Z, fragA_A, fragA_M);
    if (0 == fragA_A) { return theResult.Get(); }
    G4int fragB_Z = (G4int)theBaseZ - fragA_Z;
    G4int fragB_A = (G4int)theBaseA - fragA_A - Prompt;
 
    G4IonTable* pt = G4IonTable::GetIonTable();
    // Excitation energy is not taken into account
    G4ParticleDefinition* pdA = pt->GetIon(fragA_Z, fragA_A, 0.0);
    G4ParticleDefinition* pdB = pt->GetIon(fragB_Z, fragB_A, 0.0);
 
    // Isotropic Distribution
    G4double phi = twopi * G4UniformRand();
    // Bug #1745 DHW G4double theta = pi*G4UniformRand();
    G4double costheta = 2. * G4UniformRand() - 1.;
    G4double theta = std::acos(costheta);
    G4double sinth = std::sin(theta);
    G4ThreeVector direction(sinth * std::cos(phi), sinth * std::sin(phi), costheta);
 
    // Just use ENDF value for this
    G4double ER = eDepByFragments;
    G4double ma = pdA->GetPDGMass();
    G4double mb = pdB->GetPDGMass();
    G4double EA = ER / (1 + ma / mb);
    G4double EB = ER - EA;
    auto dpA = new G4DynamicParticle(pdA, direction, EA);
    auto dpB = new G4DynamicParticle(pdB, -direction, EB);
    theResult.Get()->AddSecondary(dpA, secID);
    theResult.Get()->AddSecondary(dpB, secID);
  }
 
  return theResult.Get();
}