G4WilsonAbrasionModel.cc

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//
// %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
//
// MODULE:              G4WilsonAbrasionModel.cc
//
// Version:     1.0
// Date:        08/12/2009
// Author:      P R Truscott
// Organisation:    QinetiQ Ltd, UK
// Customer:        ESA/ESTEC, NOORDWIJK
// Contract:        17191/03/NL/LvH
//
// %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
//
// CHANGE HISTORY
// --------------
//
// 6 October 2003, P R Truscott, QinetiQ Ltd, UK
// Created.
//
// 15 March 2004, P R Truscott, QinetiQ Ltd, UK
// Beta release
//
// 18 January 2005, M H Mendenhall, Vanderbilt University, US
// Pointers to theAbrasionGeometry and products generated by the deexcitation 
// handler deleted to prevent memory leaks.  Also particle change of projectile
// fragment previously not properly defined.
//
// 08 December 2009, P R Truscott, QinetiQ Ltd, Ltd
// ver 1.0
// There was originally a possibility of the minimum impact parameter AFTER
// considering Couloumb repulsion, rm, being too large.  Now if:
//     rm >= fradius * (rP + rT)
// where fradius is currently 0.99, then it is assumed the primary track is
// unchanged.  Additional conditions to escape from while-loop over impact
// parameter: if the loop counter evtcnt reaches 1000, the primary track is
// continued.
// Additional clauses have been included in
//    G4WilsonAbrasionModel::GetNucleonInducedExcitation
// Previously it was possible to get sqrt of negative number as Wilson
// algorithm not properly defined if either:
//    rT > rP && rsq < rTsq - rPsq) or (rP > rT && rsq < rPsq - rTsq)
//
// 12 June 2012, A. Ribon, CERN, Switzerland
// Fixing trivial warning errors of shadowed variables. 
//
// 4 August 2015, A. Ribon, CERN, Switzerland
// Replacing std::exp and std::pow with the faster versions G4Exp and G4Pow.
//
// 7 August 2015, A. Ribon, CERN, Switzerland
// Checking of 'while' loops.
//
// %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
///////////////////////////////////////////////////////////////////////////////
 
#include "G4WilsonAbrasionModel.hh"
#include "G4WilsonRadius.hh"
#include "G4NuclearAbrasionGeometry.hh"
#include "G4WilsonAblationModel.hh"
 
#include "G4PhysicalConstants.hh"
#include "G4SystemOfUnits.hh"
#include "G4ExcitationHandler.hh"
#include "G4Evaporation.hh"
#include "G4ParticleDefinition.hh"
#include "G4DynamicParticle.hh"
#include "Randomize.hh"
#include "G4Fragment.hh"
#include "G4ReactionProductVector.hh"
#include "G4LorentzVector.hh"
#include "G4ParticleMomentum.hh"
#include "G4Poisson.hh"
#include "G4ParticleTable.hh"
#include "G4IonTable.hh"
#include "globals.hh"
 
#include "G4Exp.hh"
#include "G4Pow.hh"
 
 
G4WilsonAbrasionModel::G4WilsonAbrasionModel(G4bool useAblation1)
 :G4HadronicInteraction("G4WilsonAbrasion")
{
  // Send message to stdout to advise that the G4Abrasion model is being used.
  PrintWelcomeMessage();
 
  // Set the default verbose level to 0 - no output.
  verboseLevel = 0;
  useAblation  = useAblation1;
  theAblation  = nullptr;
 
  // No de-excitation handler has been supplied - define the default handler.
 
  theExcitationHandler = new G4ExcitationHandler();
  if (useAblation)
  {
    theAblation = new G4WilsonAblationModel;
    theAblation->SetVerboseLevel(verboseLevel);
    theExcitationHandler->SetEvaporation(theAblation, true);
  }
 
  // Set the minimum and maximum range for the model (despite nomanclature,
  // this is in energy per nucleon number).  
 
  SetMinEnergy(70.0*MeV);
  SetMaxEnergy(10.1*GeV);
  isBlocked = false;
 
  // npK, when mutiplied by the nuclear Fermi momentum, determines the range of
  // momentum over which the secondary nucleon momentum is sampled.
 
  r0sq = 0.0;
  npK = 5.0;
  B = 10.0 * MeV;
  third = 1.0 / 3.0;
  fradius = 0.99;
  conserveEnergy = false;
  conserveMomentum = true;
}
 
void G4WilsonAbrasionModel::ModelDescription(std::ostream& outFile) const
{
  outFile << "G4WilsonAbrasionModel is a macroscopic treatment of\n"
          << "nucleus-nucleus collisions using simple geometric arguments.\n"
          << "The smaller projectile nucleus gouges out a part of the larger\n"
          << "target nucleus, leaving a residual nucleus and a fireball\n"
          << "region where the projectile and target intersect.  The fireball"
          << "is then treated as a highly excited nuclear fragment.  This\n"
          << "model is based on the NUCFRG2 model and is valid for all\n"
          << "projectile energies between 70 MeV/n and 10.1 GeV/n. \n";
}
 
G4WilsonAbrasionModel::G4WilsonAbrasionModel(G4ExcitationHandler* aExcitationHandler)
{
// Send message to stdout to advise that the G4Abrasion model is being used.
 
  PrintWelcomeMessage();
 
// Set the default verbose level to 0 - no output.
 
  verboseLevel = 0;
 
  theAblation = nullptr;   //A.R. 26-Jul-2012 Coverity fix.
  useAblation = false;     //A.R. 14-Aug-2012 Coverity fix.
                      
//
// The user is able to provide the excitation handler as well as an argument
// which is provided in this instantiation is used to determine
// whether the spectators of the interaction are free following the abrasion.
//
  theExcitationHandler = aExcitationHandler;
//
//
// Set the minimum and maximum range for the model (despite nomanclature, this
// is in energy per nucleon number).  
//
  SetMinEnergy(70.0*MeV);
  SetMaxEnergy(10.1*GeV);
  isBlocked = false;
//
//
// npK, when mutiplied by the nuclear Fermi momentum, determines the range of
// momentum over which the secondary nucleon momentum is sampled.
//
  r0sq             = 0.0;  //A.R. 14-Aug-2012 Coverity fix. 
  npK              = 5.0;
  B                = 10.0 * MeV;
  third            = 1.0 / 3.0;
  fradius          = 0.99;
  conserveEnergy   = false;
  conserveMomentum = true;
}
////////////////////////////////////////////////////////////////////////////////
//
G4WilsonAbrasionModel::~G4WilsonAbrasionModel()
{
  delete theExcitationHandler;
}
////////////////////////////////////////////////////////////////////////////////
//
G4HadFinalState *G4WilsonAbrasionModel::ApplyYourself (
  const G4HadProjectile &theTrack, G4Nucleus &theTarget)
{
//
//
// The secondaries will be returned in G4HadFinalState &theParticleChange -
// initialise this.  The original track will always be discontinued and
// secondaries followed.
//
  theParticleChange.Clear();
  theParticleChange.SetStatusChange(stopAndKill);
//
//
// Get relevant information about the projectile and target (A, Z, energy/nuc,
// momentum, etc).
//
  const G4ParticleDefinition *definitionP = theTrack.GetDefinition();
  const G4double AP  = definitionP->GetBaryonNumber();
  const G4double ZP  = definitionP->GetPDGCharge();
  G4LorentzVector pP = theTrack.Get4Momentum();
  G4double E         = theTrack.GetKineticEnergy()/AP;
  G4double AT        = theTarget.GetA_asInt();
  G4double ZT        = theTarget.GetZ_asInt();
  G4double TotalEPre = theTrack.GetTotalEnergy() +
    theTarget.AtomicMass(AT, ZT) + theTarget.GetEnergyDeposit();
  G4double TotalEPost = 0.0;
//
//
// Determine the radii of the projectile and target nuclei.
//
  G4WilsonRadius aR;
  G4double rP   = aR.GetWilsonRadius(AP);
  G4double rT   = aR.GetWilsonRadius(AT);
  G4double rPsq = rP * rP;
  G4double rTsq = rT * rT;
  if (verboseLevel >= 2)
  {
    G4cout <<"########################################"
           <<"########################################"
           <<G4endl;
    G4cout.precision(6);
    G4cout <<"IN G4WilsonAbrasionModel" <<G4endl;
    G4cout <<"Initial projectile A=" <<AP 
           <<", Z=" <<ZP
           <<", radius = " <<rP/fermi <<" fm"
           <<G4endl; 
    G4cout <<"Initial target     A=" <<AT
           <<", Z=" <<ZT
           <<", radius = " <<rT/fermi <<" fm"
           <<G4endl;
    G4cout <<"Projectile momentum and Energy/nuc = " <<pP <<" ," <<E <<G4endl;
  }
//
//
// The following variables are used to determine the impact parameter in the
// near-field (i.e. taking into consideration the electrostatic repulsion).
//
  G4double rm   = ZP * ZT * elm_coupling / (E * AP);
  G4double r    = 0.0;
  G4double rsq  = 0.0;
//
//
// Initialise some of the variables which wll be used to calculate the chord-
// length for nucleons in the projectile and target, and hence calculate the
// number of abraded nucleons and the excitation energy.
//
  G4NuclearAbrasionGeometry *theAbrasionGeometry = nullptr;
  G4double CT   = 0.0;
  G4double F    = 0.0;
  G4int Dabr    = 0;
//
//
// The following loop is performed until the number of nucleons which are
// abraded by the process is >1, i.e. an interaction MUST occur.
//
  G4bool skipInteraction = false;  // It will be set true if the two nuclei fail to collide 
  const G4int maxNumberOfLoops = 1000;
  G4int loopCounter = -1;
  while (Dabr == 0 && ++loopCounter < maxNumberOfLoops)  /* Loop checking, 07.08.2015, A.Ribon */
  {
//
//
// Sample the impact parameter.  For the moment, this class takes account of
// electrostatic effects on the impact parameter, but (like HZETRN AND NUCFRG2)
// does not make any correction for the effects of nuclear-nuclear repulsion.
//
    G4double rPT   = rP + rT;
    G4double rPTsq = rPT * rPT;
//
//
// This is a "catch" to make sure we don't go into an infinite loop because the
// energy is too low to overcome nuclear repulsion.  PRT 20091023.  If the
// value of rm < fradius * rPT then we're unlikely to sample a small enough
// impact parameter (energy of incident particle is too low).
//
    if (rm >= fradius * rPT) {
      skipInteraction = true;
    }
//
//
// Now sample impact parameter until the criterion is met that projectile
// and target overlap, but repulsion is taken into consideration.
//
    G4int evtcnt   = 0;
    r              = 1.1 * rPT;
    while (r > rPT && ++evtcnt < 1000)  /* Loop checking, 07.08.2015, A.Ribon */
    {
      G4double bsq = rPTsq * G4UniformRand();
      r            = (rm + std::sqrt(rm*rm + 4.0*bsq)) / 2.0;
    }
//
//
// We've tried to sample this 1000 times, but failed.  
//
    if (evtcnt >= 1000) {
      skipInteraction = true;
    }
 
    rsq = r * r;
//
//
// Now determine the chord-length through the target nucleus.
//
    if (rT > rP)
    {
      G4double x = (rPsq + rsq - rTsq) / 2.0 / r;
      if (x > 0.0) CT = 2.0 * std::sqrt(rTsq - x*x);
      else         CT = 2.0 * std::sqrt(rTsq - rsq);
    }
    else
    {
      G4double x = (rTsq + rsq - rPsq) / 2.0 / r;
      if (x > 0.0) CT = 2.0 * std::sqrt(rTsq - x*x);
      else         CT = 2.0 * rT;
    }
//
//
// Determine the number of abraded nucleons.  Note that the mean number of
// abraded nucleons is used to sample the Poisson distribution.  The Poisson
// distribution is sampled only ten times with the current impact parameter,
// and if it fails after this to find a case for which the number of abraded
// nucleons >1, the impact parameter is re-sampled.
//
    delete theAbrasionGeometry;
    theAbrasionGeometry = new G4NuclearAbrasionGeometry(AP,AT,r);
    F                   = theAbrasionGeometry->F();
    G4double lambda     = 16.6*fermi / G4Pow::GetInstance()->powA(E/MeV,0.26);
    G4double Mabr       = F * AP * (1.0 - G4Exp(-CT/lambda));
    G4long n            = 0;
    for (G4int i = 0; i<10; ++i)
    {
      n = G4Poisson(Mabr);
      if (n > 0)
      {
        if (n>AP) Dabr = (G4int) AP;
        else      Dabr = (G4int) n;
        break;
      }
    }
  }  // End of while loop
 
  if ( loopCounter >= maxNumberOfLoops || skipInteraction ) {
    // Assume nuclei do not collide and return unchanged primary. 
    theParticleChange.SetStatusChange(isAlive);
    theParticleChange.SetEnergyChange(theTrack.GetKineticEnergy());
    theParticleChange.SetMomentumChange(theTrack.Get4Momentum().vect().unit());
    if (verboseLevel >= 2) {
      G4cout <<"Particle energy too low to overcome repulsion." <<G4endl;
      G4cout <<"Event rejected and original track maintained" <<G4endl;
      G4cout <<"########################################"
             <<"########################################"
             <<G4endl;
    }
    delete theAbrasionGeometry;
    return &theParticleChange;
  }
 
  if (verboseLevel >= 2)
  {
    G4cout <<G4endl;
    G4cout <<"Impact parameter    = " <<r/fermi <<" fm" <<G4endl;
    G4cout <<"# Abraded nucleons  = " <<Dabr <<G4endl;
  }
//
//
// The number of abraded nucleons must be no greater than the number of
// nucleons in either the projectile or the target.  If AP - Dabr < 2 or 
// AT - Dabr < 2 then either we have only a nucleon left behind in the
// projectile/target or we've tried to abrade too many nucleons - and Dabr
// should be limited.
//
  if (AP - (G4double) Dabr < 2.0) Dabr = (G4int) AP;
  if (AT - (G4double) Dabr < 2.0) Dabr = (G4int) AT;
//
//
// Determine the abraded secondary nucleons from the projectile.  *fragmentP
// is a pointer to the prefragment from the projectile and nSecP is the number
// of nucleons in theParticleChange which have been abraded.  The total energy
// from these is determined.
//
  G4ThreeVector boost   = pP.findBoostToCM();
  G4Fragment *fragmentP = GetAbradedNucleons (Dabr, AP, ZP, rP); 
  G4int nSecP           = theParticleChange.GetNumberOfSecondaries();
  G4int i               = 0;
  for (i=0; i<nSecP; ++i)
  {
    TotalEPost += theParticleChange.GetSecondary(i)->
      GetParticle()->GetTotalEnergy();
  }
//
//
// Determine the number of spectators in the interaction region for the
// projectile.
//
  G4int DspcP = (G4int) (AP*F) - Dabr;
  if (DspcP <= 0)           DspcP = 0;
  else if (DspcP > AP-Dabr) DspcP = ((G4int) AP) - Dabr;
//
//
// Determine excitation energy associated with excess surface area of the
// projectile (EsP) and the excitation due to scattering of nucleons which are
// retained within the projectile (ExP).  Add the total energy from the excited
// nucleus to the total energy of the secondaries.
//
  G4bool excitationAbsorbedByProjectile = false;
  if (fragmentP != nullptr)
  {
    G4double EsP = theAbrasionGeometry->GetExcitationEnergyOfProjectile();
    G4double ExP = 0.0;
    if (Dabr < AT)
      excitationAbsorbedByProjectile = G4UniformRand() < 0.5;
    if (excitationAbsorbedByProjectile)
      ExP = GetNucleonInducedExcitation(rP, rT, r);
    G4double xP = EsP + ExP;
    if (xP > B*(AP-Dabr)) xP = B*(AP-Dabr);
    G4LorentzVector lorentzVector = fragmentP->GetMomentum();
    lorentzVector.setE(lorentzVector.e()+xP);
    fragmentP->SetMomentum(lorentzVector);
    TotalEPost += lorentzVector.e();
  }
  G4double EMassP = TotalEPost;
//
//
// Determine the abraded secondary nucleons from the target.  Note that it's
// assumed that the same number of nucleons are abraded from the target as for
// the projectile, and obviously no boost is applied to the products. *fragmentT
// is a pointer to the prefragment from the target and nSec is the total number
// of nucleons in theParticleChange which have been abraded.  The total energy
// from these is determined.
//
  G4Fragment *fragmentT = GetAbradedNucleons (Dabr, AT, ZT, rT); 
  G4int nSec = theParticleChange.GetNumberOfSecondaries();
  for (i=nSecP; i<nSec; ++i)
  {
    TotalEPost += theParticleChange.GetSecondary(i)->
      GetParticle()->GetTotalEnergy();
  }
//
//
// Determine the number of spectators in the interaction region for the
// target.
//
  G4int DspcT = (G4int) (AT*F) - Dabr;
  if (DspcT <= 0)           DspcT = 0;
  else if (DspcT > AP-Dabr) DspcT = ((G4int) AT) - Dabr;
//
//
// Determine excitation energy associated with excess surface area of the
// target (EsT) and the excitation due to scattering of nucleons which are
// retained within the target (ExT).  Add the total energy from the excited
// nucleus to the total energy of the secondaries.
//
  if (fragmentT != nullptr)
  {
    G4double EsT = theAbrasionGeometry->GetExcitationEnergyOfTarget();
    G4double ExT = 0.0;
    if (!excitationAbsorbedByProjectile)
      ExT = GetNucleonInducedExcitation(rT, rP, r);
    G4double xT = EsT + ExT;
    if (xT > B*(AT-Dabr)) xT = B*(AT-Dabr);
    G4LorentzVector lorentzVector = fragmentT->GetMomentum();
    lorentzVector.setE(lorentzVector.e()+xT);
    fragmentT->SetMomentum(lorentzVector);
    TotalEPost += lorentzVector.e();
  }
//
//
// Now determine the difference between the pre and post interaction
// energy - this will be used to determine the Lorentz boost if conservation
// of energy is to be imposed/attempted.
//
  G4double deltaE = TotalEPre - TotalEPost;
  if (deltaE > 0.0 && conserveEnergy)
  {
    G4double beta = std::sqrt(1.0 - EMassP*EMassP/G4Pow::GetInstance()->powN(deltaE+EMassP,2));
    boost = boost / boost.mag() * beta;
  }
//
//
// Now boost the secondaries from the projectile.
//
  G4ThreeVector pBalance = pP.vect();
  for (i=0; i<nSecP; ++i)
  {
    G4DynamicParticle *dynamicP = theParticleChange.GetSecondary(i)->
      GetParticle();
    G4LorentzVector lorentzVector = dynamicP->Get4Momentum();
    lorentzVector.boost(-boost);
    dynamicP->Set4Momentum(lorentzVector);
    pBalance -= lorentzVector.vect();
  }
//
//
// Set the boost for the projectile prefragment.  This is now based on the
// conservation of momentum.  However, if the user selected momentum of the
// prefragment is not to be conserved this simply boosted to the velocity of the
// original projectile times the ratio of the unexcited to the excited mass
// of the prefragment (the excitation increases the effective mass of the
// prefragment, and therefore modifying the boost is an attempt to prevent
// the momentum of the prefragment being excessive).
//
  if (fragmentP != nullptr)
  {
    G4LorentzVector lorentzVector = fragmentP->GetMomentum();
    G4double fragmentM            = lorentzVector.m();
    if (conserveMomentum)
      fragmentP->SetMomentum
        (G4LorentzVector(pBalance,std::sqrt(pBalance.mag2()+fragmentM*fragmentM+1.0*eV*eV)));
    else
    {
      G4double fragmentGroundStateM = fragmentP->GetGroundStateMass();
      fragmentP->SetMomentum(lorentzVector.boost(-boost * fragmentGroundStateM/fragmentM));
    }
  }
//
//
// Output information to user if verbose information requested.
//
  if (verboseLevel >= 2)
  {
    G4cout <<G4endl;
    G4cout <<"-----------------------------------" <<G4endl;
    G4cout <<"Secondary nucleons from projectile:" <<G4endl;
    G4cout <<"-----------------------------------" <<G4endl;
    G4cout.precision(7);
    for (i=0; i<nSecP; ++i)
    {
      G4cout <<"Particle # " <<i <<G4endl;
      theParticleChange.GetSecondary(i)->GetParticle()->DumpInfo();
      G4DynamicParticle *dyn = theParticleChange.GetSecondary(i)->GetParticle();
      G4cout <<"New nucleon (P) " <<dyn->GetDefinition()->GetParticleName()
             <<" : "              <<dyn->Get4Momentum()
             <<G4endl;
    }
    G4cout <<"---------------------------" <<G4endl;
    G4cout <<"The projectile prefragment:" <<G4endl;
    G4cout <<"---------------------------" <<G4endl;
    if (fragmentP != nullptr)
      G4cout <<*fragmentP <<G4endl;
    else
      G4cout <<"(No residual prefragment)" <<G4endl;
    G4cout <<G4endl;
    G4cout <<"-------------------------------" <<G4endl;
    G4cout <<"Secondary nucleons from target:" <<G4endl;
    G4cout <<"-------------------------------" <<G4endl;
    G4cout.precision(7);
    for (i=nSecP; i<nSec; ++i)
    {
      G4cout <<"Particle # " <<i <<G4endl;
      theParticleChange.GetSecondary(i)->GetParticle()->DumpInfo();
      G4DynamicParticle *dyn = theParticleChange.GetSecondary(i)->GetParticle();
      G4cout <<"New nucleon (T) " <<dyn->GetDefinition()->GetParticleName()
             <<" : "              <<dyn->Get4Momentum()
             <<G4endl;
    }
    G4cout <<"-----------------------" <<G4endl;
    G4cout <<"The target prefragment:" <<G4endl;
    G4cout <<"-----------------------" <<G4endl;
    if (fragmentT != nullptr)
      G4cout <<*fragmentT <<G4endl;
    else
      G4cout <<"(No residual prefragment)" <<G4endl;
  }
//
//
// Now we can decay the nuclear fragments if present.  The secondaries are
// collected and boosted as well.  This is performed first for the projectile...
//
  if (fragmentP !=nullptr)
  {
    G4ReactionProductVector *products = nullptr;
    //    if (fragmentP->GetZ_asInt() != fragmentP->GetA_asInt())
    products = theExcitationHandler->BreakItUp(*fragmentP);
    // else
    //   products = theExcitationHandlerx->BreakItUp(*fragmentP);      
    delete fragmentP;
    fragmentP = nullptr;
  
    G4ReactionProductVector::iterator iter;
    for (iter = products->begin(); iter != products->end(); ++iter)
    {
      G4DynamicParticle *secondary =
        new G4DynamicParticle((*iter)->GetDefinition(),
        (*iter)->GetTotalEnergy(), (*iter)->GetMomentum());
      theParticleChange.AddSecondary (secondary);  // Added MHM 20050118
      G4String particleName = (*iter)->GetDefinition()->GetParticleName();
      delete (*iter); // get rid of leftover particle def!  // Added MHM 20050118
      if (verboseLevel >= 2 && particleName.find("[",0) < particleName.size())
      {
        G4cout <<"------------------------" <<G4endl;
        G4cout <<"The projectile fragment:" <<G4endl;
        G4cout <<"------------------------" <<G4endl;
        G4cout <<" fragmentP = " <<particleName
               <<" Energy    = " <<secondary->GetKineticEnergy()
               <<G4endl;
      }
    }
    delete products;  // Added MHM 20050118
  }
//
//
// Now decay the target nucleus - no boost is applied since in this
// approximation it is assumed that there is negligible momentum transfer from
// the projectile.
//
  if (fragmentT != nullptr)
  {
    G4ReactionProductVector *products = nullptr;
    //    if (fragmentT->GetZ_asInt() != fragmentT->GetA_asInt())
      products = theExcitationHandler->BreakItUp(*fragmentT);
    // else
    //   products = theExcitationHandlerx->BreakItUp(*fragmentT);      
    // delete fragmentT;
    fragmentT = nullptr;
  
    G4ReactionProductVector::iterator iter;
    for (iter = products->begin(); iter != products->end(); ++iter)
    {
      G4DynamicParticle *secondary =
        new G4DynamicParticle((*iter)->GetDefinition(),
        (*iter)->GetTotalEnergy(), (*iter)->GetMomentum());
      theParticleChange.AddSecondary (secondary);
      G4String particleName = (*iter)->GetDefinition()->GetParticleName();
      delete (*iter); // get rid of leftover particle def!  // Added MHM 20050118
      if (verboseLevel >= 2 && particleName.find("[",0) < particleName.size())
      {
        G4cout <<"--------------------" <<G4endl;
        G4cout <<"The target fragment:" <<G4endl;
        G4cout <<"--------------------" <<G4endl;
        G4cout <<" fragmentT = " <<particleName
               <<" Energy    = " <<secondary->GetKineticEnergy()
               <<G4endl;
      }
    }
    delete products;  // Added MHM 20050118
  }
 
  if (verboseLevel >= 2)
     G4cout <<"########################################"
            <<"########################################"
            <<G4endl;
  
  delete theAbrasionGeometry;
  return &theParticleChange;
}
////////////////////////////////////////////////////////////////////////////////
//
G4Fragment *G4WilsonAbrasionModel::GetAbradedNucleons (G4int Dabr, G4double A,
  G4double Z, G4double r)
{
//
//
// Initialise variables.  tau is the Fermi radius of the nucleus.  The variables
// p..., C... and gamma are used to help sample the secondary nucleon
// spectrum.
//
  
  G4double pK   = hbarc * G4Pow::GetInstance()->A13(9.0 * pi / 4.0 * A) / (1.29 * r);
  if (A <= 24.0) pK *= -0.229*G4Pow::GetInstance()->A13(A) + 1.62;
  G4double pKsq = pK * pK;
  G4double p1sq = 2.0/5.0 * pKsq;
  G4double p2sq = 6.0/5.0 * pKsq;
  G4double p3sq = 500.0 * 500.0;
  G4double C1   = 1.0;
  G4double C2   = 0.03;
  G4double C3   = 0.0002;
  G4double gamma = 90.0 * MeV;
  G4double maxn = C1 + C2 + C3;
//
//
// initialise the number of secondary nucleons abraded to zero, and initially set
// the type of nucleon abraded to proton ... just for now.
//  
  G4double Aabr                     = 0.0;
  G4double Zabr                     = 0.0; 
  G4ParticleDefinition *typeNucleon = G4Proton::ProtonDefinition();
  G4DynamicParticle *dynamicNucleon = nullptr;
  G4ParticleMomentum pabr(0.0, 0.0, 0.0);
//
//
// Now go through each abraded nucleon and sample type, spectrum and angle.
//
  G4bool isForLoopExitAnticipated = false;
  for (G4int i=0; i<Dabr; ++i)
  {
//
//
// Sample the nucleon momentum distribution by simple rejection techniques.  We
// reject values of p == 0.0 since this causes bad behaviour in the sinh term.
//
    G4double p   = 0.0;
    G4bool found = false;
    const G4int maxNumberOfLoops = 100000;
    G4int loopCounter = -1;
    while (!found && ++loopCounter < maxNumberOfLoops)  /* Loop checking, 07.08.2015, A.Ribon */
    {
      while (p <= 0.0) p = npK * pK * G4UniformRand();  /* Loop checking, 07.08.2015, A.Ribon */
      G4double psq = p * p;
      found = maxn * G4UniformRand() < C1*G4Exp(-psq/p1sq/2.0) +
        C2*G4Exp(-psq/p2sq/2.0) + C3*G4Exp(-psq/p3sq/2.0) + p/gamma/(0.5*(G4Exp(p/gamma)-G4Exp(-p/gamma)));
    }
    if ( loopCounter >= maxNumberOfLoops )
    {
      isForLoopExitAnticipated = true;
      break;
    }
//
//
// Determine the type of particle abraded.  Can only be proton or neutron,
// and the probability is determine to be proportional to the ratio as found
// in the nucleus at each stage.
//
    G4double prob = (Z-Zabr)/(A-Aabr);
    if (G4UniformRand()<prob)
    {
      Zabr++;
      typeNucleon = G4Proton::ProtonDefinition();
    }
    else
      typeNucleon = G4Neutron::NeutronDefinition();
    Aabr++;
//
//
// The angular distribution of the secondary nucleons is approximated to an
// isotropic distribution in the rest frame of the nucleus (this will be Lorentz
// boosted later.
//
    G4double costheta = 2.*G4UniformRand()-1.0;
    G4double sintheta = std::sqrt((1.0 - costheta)*(1.0 + costheta));
    G4double phi      = 2.0*pi*G4UniformRand()*rad;
    G4ThreeVector direction(sintheta*std::cos(phi),sintheta*std::sin(phi),costheta);
    G4double nucleonMass = typeNucleon->GetPDGMass();
    G4double E           = std::sqrt(p*p + nucleonMass*nucleonMass)-nucleonMass;
    dynamicNucleon = new G4DynamicParticle(typeNucleon,direction,E);
    theParticleChange.AddSecondary (dynamicNucleon);
    pabr += p*direction;
  }
//
//
// Next determine the details of the nuclear prefragment .. that is if there
// is one or more protons in the residue.  (Note that the 1 eV in the total
// energy is a safety factor to avoid any possibility of negative rest mass
// energy.)
//
  G4Fragment *fragment = nullptr;
  if ( ! isForLoopExitAnticipated && Z-Zabr>=1.0 )
  {
    G4double ionMass = G4ParticleTable::GetParticleTable()->GetIonTable()->
                       GetIonMass(G4lrint(Z-Zabr),G4lrint(A-Aabr));
    G4double E       = std::sqrt(pabr.mag2() + ionMass*ionMass);
    G4LorentzVector lorentzVector = G4LorentzVector(-pabr, E + 1.0*eV);
    fragment =
      new G4Fragment((G4int) (A-Aabr), (G4int) (Z-Zabr), lorentzVector);
  }
 
  return fragment;
}
////////////////////////////////////////////////////////////////////////////////
//
G4double G4WilsonAbrasionModel::GetNucleonInducedExcitation
  (G4double rP, G4double rT, G4double r)
{
//
//
// Initialise variables.
//
  G4double Cl   = 0.0;
  G4double rPsq = rP * rP;
  G4double rTsq = rT * rT;
  G4double rsq  = r * r;
//
//
// Depending upon the impact parameter, a different form of the chord length is
// is used.
//  
  if (r > rT) Cl = 2.0*std::sqrt(rPsq + 2.0*r*rT - rsq - rTsq);
  else        Cl = 2.0*rP;
//
//
// The next lines have been changed to include a "catch" to make sure if the
// projectile and target are too close, Ct is set to twice rP or twice rT.
// Otherwise the standard Wilson algorithm should work fine.
// PRT 20091023.
//
  G4double Ct = 0.0;
  if      (rT > rP && rsq < rTsq - rPsq) Ct = 2.0 * rP;
  else if (rP > rT && rsq < rPsq - rTsq) Ct = 2.0 * rT;
  else {
    G4double bP = (rPsq+rsq-rTsq)/2.0/r;
    G4double x  = rPsq - bP*bP;
    if (x < 0.0) {
      G4cerr <<"########################################"
             <<"########################################"
             <<G4endl;
      G4cerr <<"ERROR IN G4WilsonAbrasionModel::GetNucleonInducedExcitation"
             <<G4endl;
      G4cerr <<"rPsq - bP*bP < 0.0 and cannot be square-rooted" <<G4endl;
      G4cerr <<"Set to zero instead" <<G4endl;
      G4cerr <<"########################################"
             <<"########################################"
             <<G4endl;
    }
    Ct = 2.0*std::sqrt(x);
  }
  
  G4double Ex = 13.0 * Cl / fermi;
  if (Ct > 1.5*fermi)
    Ex += 13.0 * Cl / fermi /3.0 * (Ct/fermi - 1.5);
 
  return Ex;
}
////////////////////////////////////////////////////////////////////////////////
//
void G4WilsonAbrasionModel::SetUseAblation (G4bool useAblation1)
{
  if (useAblation != useAblation1)
  {
    useAblation = useAblation1;
    if (useAblation)
    {
      theAblation = new G4WilsonAblationModel;
      theAblation->SetVerboseLevel(verboseLevel);
      theExcitationHandler->SetEvaporation(theAblation);
    }
    else
    {
      delete theExcitationHandler;
      theAblation                      = nullptr;
      theExcitationHandler  = new G4ExcitationHandler();
    }
  }
  return; 
}
////////////////////////////////////////////////////////////////////////////////
//
void G4WilsonAbrasionModel::PrintWelcomeMessage ()
{
  G4cout <<G4endl;
  G4cout <<" *****************************************************************"
         <<G4endl;
  G4cout <<" Nuclear abrasion model for nuclear-nuclear interactions activated"
         <<G4endl;
  G4cout <<" (Written by QinetiQ Ltd for the European Space Agency)"
         <<G4endl;
  G4cout <<" *****************************************************************"
         <<G4endl;
  G4cout << G4endl;
 
  return;
}
////////////////////////////////////////////////////////////////////////////////
//