G4ANuElNucleusNcModel.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.          *
// ********************************************************************
//
// $Id: G4ANuElNucleusNcModel.cc 91806 2015-08-06 12:20:45Z gcosmo $
//
// Geant4 Header : G4ANuElNucleusNcModel
//
// Author : V.Grichine 12.2.19
//  
 
#include "G4ANuElNucleusNcModel.hh"
#include "G4NeutrinoNucleusModel.hh" 
 
// #include "G4NuMuResQX.hh" 
 
#include "G4SystemOfUnits.hh"
#include "G4ParticleTable.hh"
#include "G4ParticleDefinition.hh"
#include "G4IonTable.hh"
#include "Randomize.hh"
#include "G4RandomDirection.hh"
 
// #include "G4Integrator.hh"
#include "G4DataVector.hh"
#include "G4PhysicsTable.hh"
#include "G4KineticTrack.hh"
#include "G4DecayKineticTracks.hh"
#include "G4KineticTrackVector.hh"
#include "G4Fragment.hh"
#include "G4ReactionProductVector.hh"
 
 
#include "G4NeutrinoE.hh"
// #include "G4AntiNeutrinoMu.hh"
#include "G4Nucleus.hh"
#include "G4LorentzVector.hh"
 
using namespace std;
using namespace CLHEP;
 
#ifdef G4MULTITHREADED
    G4Mutex G4ANuElNucleusNcModel::numuNucleusModel = G4MUTEX_INITIALIZER;
#endif     
 
 
G4ANuElNucleusNcModel::G4ANuElNucleusNcModel(const G4String& name) 
  : G4NeutrinoNucleusModel(name)
{
  SetMinEnergy( 0.0*GeV );
  SetMaxEnergy( 100.*TeV );
  SetMinEnergy(1.e-6*eV);
 
  theNuE =  G4NeutrinoE::NeutrinoE();
 
  fMnumu = 0.; 
  fData = fMaster = false;
  InitialiseModel();  
     
}
 
 
G4ANuElNucleusNcModel::~G4ANuElNucleusNcModel()
{}
 
 
void G4ANuElNucleusNcModel::ModelDescription(std::ostream& outFile) const
{
 
    outFile << "G4ANuElNucleusNcModel is a neutrino-nucleus (neutral current) scattering\n"
            << "model which uses the standard model \n"
            << "transfer parameterization.  The model is fully relativistic\n";
 
}
 
/////////////////////////////////////////////////////////
//
// Read data from G4PARTICLEXSDATA (locally PARTICLEXSDATA)
 
void G4ANuElNucleusNcModel::InitialiseModel()
{
  G4String pName  = "anti_nu_e";
  
  G4int nSize(0), i(0), j(0), k(0);
 
  if(!fData)
  { 
#ifdef G4MULTITHREADED
    G4MUTEXLOCK(&numuNucleusModel);
    if(!fData)
    { 
#endif     
      fMaster = true;
#ifdef G4MULTITHREADED
    }
    G4MUTEXUNLOCK(&numuNucleusModel);
#endif
  }
 
  if(fMaster)
  {  
    char* path = getenv("G4PARTICLEXSDATA");
    std::ostringstream ost1, ost2, ost3, ost4;
    ost1 << path << "/" << "neutrino" << "/" << pName << "/xarraynckr";
 
    std::ifstream filein1( ost1.str().c_str() );
 
    // filein.open("$PARTICLEXSDATA/");
 
    filein1>>nSize;
 
    for( k = 0; k < fNbin; ++k )
    {
      for( i = 0; i <= fNbin; ++i )
      {
        filein1 >> fNuMuXarrayKR[k][i];
        // G4cout<< fNuMuXarrayKR[k][i] << "  ";
      }
    }
    // G4cout<<G4endl<<G4endl;
 
    ost2 << path << "/" << "neutrino" << "/" << pName << "/xdistrnckr";
    std::ifstream  filein2( ost2.str().c_str() );
 
    filein2>>nSize;
 
    for( k = 0; k < fNbin; ++k )
    {
      for( i = 0; i < fNbin; ++i )
      {
        filein2 >> fNuMuXdistrKR[k][i];
        // G4cout<< fNuMuXdistrKR[k][i] << "  ";
      }
    }
    // G4cout<<G4endl<<G4endl;
 
    ost3 << path << "/" << "neutrino" << "/" << pName << "/q2arraynckr";
    std::ifstream  filein3( ost3.str().c_str() );
 
    filein3>>nSize;
 
    for( k = 0; k < fNbin; ++k )
    {
      for( i = 0; i <= fNbin; ++i )
      {
        for( j = 0; j <= fNbin; ++j )
        {
          filein3 >> fNuMuQarrayKR[k][i][j];
          // G4cout<< fNuMuQarrayKR[k][i][j] << "  ";
        }
      }
    }
    // G4cout<<G4endl<<G4endl;
 
    ost4 << path << "/" << "neutrino" << "/" << pName << "/q2distrnckr";
    std::ifstream  filein4( ost4.str().c_str() );
 
    filein4>>nSize;
 
    for( k = 0; k < fNbin; ++k )
    {
      for( i = 0; i <= fNbin; ++i )
      {
        for( j = 0; j < fNbin; ++j )
        {
          filein4 >> fNuMuQdistrKR[k][i][j];
          // G4cout<< fNuMuQdistrKR[k][i][j] << "  ";
        }
      }
    }
    fData = true;
  }
}
 
/////////////////////////////////////////////////////////
 
G4bool G4ANuElNucleusNcModel::IsApplicable(const G4HadProjectile & aPart, 
                           G4Nucleus & targetNucleus)
{
  G4bool result  = false;
  G4String pName = aPart.GetDefinition()->GetParticleName();
  G4double energy = aPart.GetTotalEnergy();
  fMinNuEnergy = GetMinNuElEnergy();
  
  if(  pName == "anti_nu_e"
        &&
        energy > fMinNuEnergy                                )
  {
    result = true;
  }
  G4int Z = targetNucleus.GetZ_asInt();
        Z *= 1;
 
  return result;
}
 
/////////////////////////////////////////// ClusterDecay ////////////////////////////////////////////////////////////
//
//
 
G4HadFinalState* G4ANuElNucleusNcModel::ApplyYourself(
         const G4HadProjectile& aTrack, G4Nucleus& targetNucleus)
{
  theParticleChange.Clear();
  fProton = f2p2h = fBreak = false;
  const G4HadProjectile* aParticle = &aTrack;
  G4double energy = aParticle->GetTotalEnergy();
 
  G4String pName  = aParticle->GetDefinition()->GetParticleName();
 
  if( energy < fMinNuEnergy ) 
  {
    theParticleChange.SetEnergyChange(energy);
    theParticleChange.SetMomentumChange(aTrack.Get4Momentum().vect().unit());
    return &theParticleChange;
  }
  SampleLVkr( aTrack, targetNucleus);
 
  if( fBreak == true || fEmu < fMnumu ) // ~5*10^-6
  {
    // G4cout<<"ni, ";
    theParticleChange.SetEnergyChange(energy);
    theParticleChange.SetMomentumChange(aTrack.Get4Momentum().vect().unit());
    return &theParticleChange;
  }
 
  // LVs of initial state
 
  G4LorentzVector lvp1 = aParticle->Get4Momentum();
  G4LorentzVector lvt1( 0., 0., 0., fM1 );
  G4double mPip = G4ParticleTable::GetParticleTable()->FindParticle(211)->GetPDGMass();
 
  // 1-pi by fQtransfer && nu-energy
  G4LorentzVector lvpip1( 0., 0., 0., mPip );
  G4LorentzVector lvsum, lv2, lvX;
  G4ThreeVector eP;
  G4double cost(1.), sint(0.), phi(0.), muMom(0.), massX2(0.);
  G4DynamicParticle* aLept = nullptr; // lepton lv
 
  G4int Z = targetNucleus.GetZ_asInt();
  G4int A = targetNucleus.GetA_asInt();
  G4double  mTarg = targetNucleus.AtomicMass(A,Z);
  G4int pdgP(0), qB(0);
  // G4double mSum = G4ParticleTable::GetParticleTable()->FindParticle(2212)->GetPDGMass() + mPip;
 
  G4int iPi     = GetOnePionIndex(energy);
  G4double p1pi = GetNuMuOnePionProb( iPi, energy);
 
  if( p1pi > G4UniformRand() && fCosTheta > 0.9  ) // && fQtransfer < 0.95*GeV ) // mu- & coherent pion + nucleus
  {
    // lvsum = lvp1 + lvpip1;
    lvsum = lvp1 + lvt1;
    // cost = fCosThetaPi;
    cost = fCosTheta;
    sint = std::sqrt( (1.0 - cost)*(1.0 + cost) );
    phi  = G4UniformRand()*CLHEP::twopi;
    eP   = G4ThreeVector( sint*std::cos(phi), sint*std::sin(phi), cost );
 
    // muMom = sqrt(fEmuPi*fEmuPi-fMnumu*fMnumu);
    muMom = sqrt(fEmu*fEmu-fMnumu*fMnumu);
 
    eP *= muMom;
 
    // lv2 = G4LorentzVector( eP, fEmuPi );
    lv2 = G4LorentzVector( eP, fEmu );
    lv2 = fLVl;
 
    lvX = lvsum - lv2;
    lvX = fLVh;
    massX2 = lvX.m2();
    G4double massX = lvX.m();
    G4double massR = fLVt.m();
 
    // if ( massX2 <= 0. ) // vmg: very rarely ~ (1-4)e-6 due to big Q2/x, to be improved
    if ( massX2 <= fM1*fM1 ) // 9-3-20 vmg: very rarely ~ (1-4)e-6 due to big Q2/x, to be improved
      if ( lvX.e() <= fM1 ) // 9-3-20 vmg: very rarely ~ (1-4)e-6 due to big Q2/x, to be improved
    {
      theParticleChange.SetEnergyChange(energy);
      theParticleChange.SetMomentumChange(aTrack.Get4Momentum().vect().unit());
      return &theParticleChange;
    }
    fW2 = massX2;
 
    if(  pName == "anti_nu_e" )         aLept = new G4DynamicParticle( theNuE, lv2 );  
    // else if( pName == "anti_nu_mu") aLept = new G4DynamicParticle( theANuMu,  lv2 );
    else
    {
      theParticleChange.SetEnergyChange(energy);
      theParticleChange.SetMomentumChange(aTrack.Get4Momentum().vect().unit());
      return &theParticleChange;
    } 
 
    pdgP = 111;
 
    G4double eCut; // = fMpi + 0.5*(fMpi*fMpi - massX2)/mTarg; // massX -> fMpi
 
    if( A > 1 )
    {
      eCut = (fMpi + mTarg)*(fMpi + mTarg) - (massX + massR)*(massX + massR);
      eCut /= 2.*massR;
      eCut += massX;
    }
    else  eCut = fM1 + fMpi;
 
    if ( lvX.e() > eCut ) // && sqrt( GetW2() ) < 1.4*GeV ) // 
    {
      CoherentPion( lvX, pdgP, targetNucleus);
    }
    else
    {
      theParticleChange.SetEnergyChange(energy);
      theParticleChange.SetMomentumChange(aTrack.Get4Momentum().vect().unit());
      return &theParticleChange;
    } 
    theParticleChange.AddSecondary( aLept );
 
    return &theParticleChange;
  }
  else // lepton part in lab
  { 
    lvsum = lvp1 + lvt1;
    cost = fCosTheta;
    sint = std::sqrt( (1.0 - cost)*(1.0 + cost) );
    phi  = G4UniformRand()*CLHEP::twopi;
    eP   = G4ThreeVector( sint*std::cos(phi), sint*std::sin(phi), cost );
 
    muMom = sqrt(fEmu*fEmu-fMnumu*fMnumu);
 
    eP *= muMom;
 
    lv2 = G4LorentzVector( eP, fEmu );
 
    lvX = lvsum - lv2;
 
    massX2 = lvX.m2();
 
    if ( massX2 <= 0. ) // vmg: very rarely ~ (1-4)e-6 due to big Q2/x, to be improved
    {
      theParticleChange.SetEnergyChange(energy);
      theParticleChange.SetMomentumChange(aTrack.Get4Momentum().vect().unit());
      return &theParticleChange;
    }
    fW2 = massX2;
 
    aLept = new G4DynamicParticle( theNuE, lv2 );  
    
    theParticleChange.AddSecondary( aLept );
  }
 
  // hadron part
 
  fRecoil  = nullptr;
  fCascade = false;
  fString  = false;
  
  if( A == 1 )
  {
    qB = 1;
 
    // if( G4UniformRand() > 0.1 ) //  > 0.9999 ) // > 0.0001 ) //
    {
      ClusterDecay( lvX, qB );
    }
    return &theParticleChange;
  }
  G4Nucleus recoil;
  G4double rM(0.), ratio = G4double(Z)/G4double(A);
 
  if( ratio > G4UniformRand() ) // proton is excited
  {
    fProton = true;
    recoil = G4Nucleus(A-1,Z-1);
    fRecoil = &recoil;
    rM = recoil.AtomicMass(A-1,Z-1);
 
    fMt = G4ParticleTable::GetParticleTable()->FindParticle(2212)->GetPDGMass()
          + G4ParticleTable::GetParticleTable()->FindParticle(111)->GetPDGMass();
  }
  else // excited neutron
  {
    fProton = false;
    recoil = G4Nucleus(A-1,Z);
    fRecoil = &recoil;
    rM = recoil.AtomicMass(A-1,Z);
 
    fMt = G4ParticleTable::GetParticleTable()->FindParticle(2112)->GetPDGMass()
          + G4ParticleTable::GetParticleTable()->FindParticle(111)->GetPDGMass(); 
  }
  G4int       index = GetEnergyIndex(energy);
  G4double qeTotRat = GetNuMuQeTotRat(index, energy);
 
  G4ThreeVector dX = (lvX.vect()).unit();
  G4double eX   = lvX.e();  // excited nucleon
  G4double mX   = sqrt(massX2);
 
  if( qeTotRat > G4UniformRand() || mX <= fMt ) // || eX <= 1232.*MeV) // QE
  {  
    fString = false;
 
    if( fProton ) 
    {  
      fPDGencoding = 2212;
      fMr =  proton_mass_c2;
      recoil = G4Nucleus(A-1,Z-1);
      fRecoil = &recoil;
      rM = recoil.AtomicMass(A-1,Z-1);
    } 
    else
    {  
      fPDGencoding = 2112;
      fMr =   G4ParticleTable::GetParticleTable()->
    FindParticle(fPDGencoding)->GetPDGMass(); // 939.5654133*MeV;
      recoil = G4Nucleus(A-1,Z);
      fRecoil = &recoil;
      rM = recoil.AtomicMass(A-1,Z);
    } 
    G4double eTh = fMr+0.5*(fMr*fMr-mX*mX)/rM;
 
    if(eX <= eTh) // vmg, very rarely out of kinematics
    {
      theParticleChange.SetEnergyChange(energy);
      theParticleChange.SetMomentumChange(aTrack.Get4Momentum().vect().unit());
      return &theParticleChange;
    } 
    FinalBarion( lvX, 0, fPDGencoding ); // p(n)+deexcited recoil
  }
  else // if ( eX < 9500000.*GeV ) // < 25.*GeV) //  < 95.*GeV ) // < 2.5*GeV ) //cluster decay
  {  
    if     (  fProton && pName == "anti_nu_e" )      qB =  1;
    else if( !fProton && pName == "anti_nu_e" )      qB =  0;
 
    ClusterDecay( lvX, qB );
  }
  return &theParticleChange;
}
 
 
/////////////////////////////////////////////////////////////////////
////////////////////////////////////////////////////////////////////
///////////////////////////////////////////////////////////////////
 
/////////////////////////////////////////////////
//
// sample x, then Q2
 
void G4ANuElNucleusNcModel::SampleLVkr(const G4HadProjectile & aTrack, G4Nucleus& targetNucleus)
{
  fBreak = false;
  G4int A = targetNucleus.GetA_asInt(), iTer(0), iTerMax(100); 
  G4int Z = targetNucleus.GetZ_asInt(); 
  G4double e3(0.), pMu2(0.), pX2(0.), nMom(0.), rM(0.), hM(0.), tM = targetNucleus.AtomicMass(A,Z);
  G4double cost(1.), sint(0.), phi(0.), muMom(0.); 
  G4ThreeVector eP, bst;
  const G4HadProjectile* aParticle = &aTrack;
  G4LorentzVector lvp1 = aParticle->Get4Momentum();
  nMom = NucleonMomentum( targetNucleus );
 
  if( A == 1 || nMom == 0. ) // hydrogen, no Fermi motion ???
  {
    fNuEnergy = aParticle->GetTotalEnergy();
    iTer = 0;
 
    do
    {
      fXsample = SampleXkr(fNuEnergy);
      fQtransfer = SampleQkr(fNuEnergy, fXsample);
      fQ2 = fQtransfer*fQtransfer;
 
     if( fXsample > 0. )
      {
        fW2 = fM1*fM1 - fQ2 + fQ2/fXsample; // sample excited hadron mass
        fEmu = fNuEnergy - fQ2/2./fM1/fXsample;
      }
      else
      {
        fW2 = fM1*fM1;
        fEmu = fNuEnergy;
      }
      e3 = fNuEnergy + fM1 - fEmu;
 
      // if( e3 < sqrt(fW2) )  G4cout<<"energyX = "<<e3/GeV<<", fW = "<<sqrt(fW2)/GeV<<G4endl; // vmg ~10^-5 for NC
    
      pMu2 = fEmu*fEmu - fMnumu*fMnumu;
      pX2  = e3*e3 - fW2;
 
      fCosTheta  = fNuEnergy*fNuEnergy  + pMu2 - pX2;
      fCosTheta /= 2.*fNuEnergy*sqrt(pMu2);
      iTer++;
    }
    while( ( abs(fCosTheta) > 1. || fEmu < fMnumu ) && iTer < iTerMax );
 
    if( iTer >= iTerMax ) { fBreak = true; return; }
 
    if( abs(fCosTheta) > 1.) // vmg: due to big Q2/x values. To be improved ...
    { 
      G4cout<<"H2: fCosTheta = "<<fCosTheta<<", fEmu = "<<fEmu<<G4endl;
      // fCosTheta = -1. + 2.*G4UniformRand(); 
      if(fCosTheta < -1.) fCosTheta = -1.;
      if(fCosTheta >  1.) fCosTheta =  1.;
    }
    // LVs
 
    G4LorentzVector lvt1  = G4LorentzVector( 0., 0., 0., fM1 );
    G4LorentzVector lvsum = lvp1 + lvt1;
 
    cost = fCosTheta;
    sint = std::sqrt( (1.0 - cost)*(1.0 + cost) );
    phi  = G4UniformRand()*CLHEP::twopi;
    eP   = G4ThreeVector( sint*std::cos(phi), sint*std::sin(phi), cost );
    muMom = sqrt(fEmu*fEmu-fMnumu*fMnumu);
    eP *= muMom;
    fLVl = G4LorentzVector( eP, fEmu );
 
    fLVh = lvsum - fLVl;
    fLVt = G4LorentzVector( 0., 0., 0., 0. ); // no recoil
  }
  else // Fermi motion, Q2 in nucleon rest frame
  {
    G4ThreeVector nMomDir = nMom*G4RandomDirection();
 
    if( !f2p2h ) // 1p1h
    {
      G4Nucleus recoil(A-1,Z);
      rM = sqrt( recoil.AtomicMass(A-1,Z)*recoil.AtomicMass(A-1,Z) + nMom*nMom );
      hM = tM - rM;
 
      fLVt = G4LorentzVector( nMomDir, sqrt( rM*rM+nMom*nMom ) );
      fLVh = G4LorentzVector(-nMomDir, sqrt( hM*hM+nMom*nMom ) ); 
    }
    else // 2p2h
    {
      G4Nucleus recoil(A-2,Z-1);
      rM = recoil.AtomicMass(A-2,Z-1)+sqrt(nMom*nMom+fM1*fM1);
      hM = tM - rM;
 
      fLVt = G4LorentzVector( nMomDir, sqrt( rM*rM+nMom*nMom ) );
      fLVh = G4LorentzVector(-nMomDir, sqrt( hM*hM+nMom*nMom ) ); 
    }
    // G4cout<<hM<<", ";
    // bst = fLVh.boostVector(); // 9-3-20
 
    // lvp1.boost(-bst); // 9-3-20 -> nucleon rest system, where Q2 transfer is ???
 
    fNuEnergy  = lvp1.e();
    iTer = 0;
 
    do
    {
      fXsample = SampleXkr(fNuEnergy);
      fQtransfer = SampleQkr(fNuEnergy, fXsample);
      fQ2 = fQtransfer*fQtransfer;
 
      if( fXsample > 0. )
      {
        fW2 = fM1*fM1 - fQ2 + fQ2/fXsample; // sample excited hadron mass
        fEmu = fNuEnergy - fQ2/2./fM1/fXsample;
      }
      else
      {
        fW2 = fM1*fM1;
        fEmu = fNuEnergy;
      }
 
      // if(fEmu < 0.) G4cout<<"fEmu = "<<fEmu<<" hM = "<<hM<<G4endl;
 
      e3 = fNuEnergy + fM1 - fEmu;
 
      // if( e3 < sqrt(fW2) )  G4cout<<"energyX = "<<e3/GeV<<", fW = "<<sqrt(fW2)/GeV<<G4endl;
    
      pMu2 = fEmu*fEmu - fMnumu*fMnumu;
      pX2  = e3*e3 - fW2;
 
      fCosTheta  = fNuEnergy*fNuEnergy  + pMu2 - pX2;
      fCosTheta /= 2.*fNuEnergy*sqrt(pMu2);
      iTer++;
    }
    while( ( abs(fCosTheta) > 1. || fEmu < fMnumu ) && iTer < iTerMax );
 
    if( iTer >= iTerMax ) { fBreak = true; return; }
 
    if( abs(fCosTheta) > 1.) // vmg: due to big Q2/x values. To be improved ...
    { 
      G4cout<<"FM: fCosTheta = "<<fCosTheta<<", fEmu = "<<fEmu<<G4endl;
      // fCosTheta = -1. + 2.*G4UniformRand(); 
      if(fCosTheta < -1.) fCosTheta = -1.;
      if(fCosTheta >  1.) fCosTheta =  1.;
    }
    // LVs
    G4LorentzVector lvt1  = G4LorentzVector( 0., 0., 0., fM1 );
    G4LorentzVector lvsum = lvp1 + lvt1;
 
    cost = fCosTheta;
    sint = std::sqrt( (1.0 - cost)*(1.0 + cost) );
    phi  = G4UniformRand()*CLHEP::twopi;
    eP   = G4ThreeVector( sint*std::cos(phi), sint*std::sin(phi), cost );
    muMom = sqrt(fEmu*fEmu-fMnumu*fMnumu);
    eP *= muMom;
    fLVl = G4LorentzVector( eP, fEmu );
    fLVh = lvsum - fLVl;
    // back to lab system
    // fLVl.boost(bst); // 9-3-20
    // fLVh.boost(bst); // 9-3-20
  }
  //G4cout<<iTer<<", "<<fBreak<<"; ";
}
 
//
//
///////////////////////////