G4NuMuNucleusCcModel.cc

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// $Id: G4NuMuNucleusCcModel.cc 91806 2015-08-06 12:20:45Z gcosmo $
//
// Geant4 Header : G4NuMuNucleusCcModel
//
// Author : V.Grichine 12.2.19
//  

#include <iostream>
#include <fstream>
#include <sstream>

#include "G4NuMuNucleusCcModel.hh"
// #include "G4NuMuNuclCcDistrKR.hh" 

// #include "G4NuMuResQX.hh" 

#include "G4SystemOfUnits.hh"
#include "G4ParticleTable.hh"
#include "G4ParticleDefinition.hh"
#include "G4IonTable.hh"
#include "Randomize.hh"
#include "G4RandomDirection.hh"
// #include "G4Threading.hh"

// #include "G4Integrator.hh"
#include "G4DataVector.hh"
#include "G4PhysicsTable.hh"
/*
#include "G4CascadeInterface.hh"
// #include "G4BinaryCascade.hh"
#include "G4TheoFSGenerator.hh"
#include "G4LundStringFragmentation.hh"
#include "G4ExcitedStringDecay.hh"
#include "G4FTFModel.hh"
// #include "G4BinaryCascade.hh"
#include "G4HadFinalState.hh"
#include "G4HadSecondary.hh"
#include "G4HadronicInteractionRegistry.hh"
// #include "G4INCLXXInterface.hh"
#include "G4QGSModel.hh"
#include "G4QGSMFragmentation.hh"
#include "G4QGSParticipants.hh"
*/
#include "G4KineticTrack.hh"
#include "G4DecayKineticTracks.hh"
#include "G4KineticTrackVector.hh"
#include "G4Fragment.hh"
#include "G4NucleiProperties.hh"
#include "G4ReactionProductVector.hh"

#include "G4GeneratorPrecompoundInterface.hh"
#include "G4PreCompoundModel.hh"
#include "G4ExcitationHandler.hh"


#include "G4MuonMinus.hh"
#include "G4MuonPlus.hh"
#include "G4Nucleus.hh"
#include "G4LorentzVector.hh"

using namespace std;
using namespace CLHEP;

const G4int G4NuMuNucleusCcModel::fResNumber = 6;

const G4double G4NuMuNucleusCcModel::fResMass[6] = // [fResNumber] = 
  {2190., 1920., 1700., 1600., 1440., 1232. };

const G4int G4NuMuNucleusCcModel::fClustNumber = 4;

const G4double G4NuMuNucleusCcModel::fMesMass[4] = {1260., 980., 770., 139.57};
const G4int    G4NuMuNucleusCcModel::fMesPDG[4]  = {20213, 9000211, 213, 211};

// const G4double G4NuMuNucleusCcModel::fBarMass[4] = {1905., 1600., 1232., 939.57};
// const G4int    G4NuMuNucleusCcModel::fBarPDG[4]  = {2226, 32224, 2224, 2212};

const G4double G4NuMuNucleusCcModel::fBarMass[4] = {1700., 1600., 1232., 939.57};
const G4int    G4NuMuNucleusCcModel::fBarPDG[4]  = {12224, 32224, 2224, 2212};

const G4double  G4NuMuNucleusCcModel::fNuMuEnergyLogVector[50] = {
115.603, 133.424, 153.991, 177.729, 205.126, 236.746, 273.24, 315.361, 363.973, 420.08, 484.836, 559.573, 645.832, 
745.387, 860.289, 992.903, 1145.96, 1322.61, 1526.49, 1761.8, 2033.38, 2346.83, 2708.59, 3126.12, 3608.02, 4164.19, 
4806.1, 5546.97, 6402.04, 7388.91, 8527.92, 9842.5, 11359.7, 13110.8, 15131.9, 17464.5, 20156.6, 23263.8, 26849.9, 
30988.8, 35765.7, 41279, 47642.2, 54986.3, 63462.4, 73245.2, 84536, 97567.2, 112607, 129966 };


G4double G4NuMuNucleusCcModel::fNuMuXarrayKR[50][51] = {{1.0}};
G4double G4NuMuNucleusCcModel::fNuMuXdistrKR[50][50] = {{1.0}};
G4double G4NuMuNucleusCcModel::fNuMuQarrayKR[50][51][51] = {{{1.0}}};
G4double G4NuMuNucleusCcModel::fNuMuQdistrKR[50][51][50] = {{{1.0}}};

#ifdef G4MULTITHREADED
    G4Mutex G4NuMuNucleusCcModel::numuNucleusModel = G4MUTEX_INITIALIZER;
#endif     


G4NuMuNucleusCcModel::G4NuMuNucleusCcModel(const G4String& name) 
  : G4NeutrinoNucleusModel(name)
{
  fData = fMaster = false;
  InitialiseModel();  
}


G4NuMuNucleusCcModel::~G4NuMuNucleusCcModel()
{}


void G4NuMuNucleusCcModel::ModelDescription(std::ostream& outFile) const
{

    outFile << "G4NuMuNucleusCcModel is a neutrino-nucleus (charge 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 G4NuMuNucleusCcModel::InitialiseModel()
{
  G4String pName  = "nu_mu";
  
  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 << "/xarraycckr";

    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 << "/xdistrcckr";
    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 << "/q2arraycckr";
    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 << "/q2distrcckr";
    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 G4NuMuNucleusCcModel::IsApplicable(const G4HadProjectile & aPart, 
                 G4Nucleus & targetNucleus)
{
  G4bool result  = false;
  G4String pName = aPart.GetDefinition()->GetParticleName();
  G4double energy = aPart.GetTotalEnergy();
  
  if(  pName == "nu_mu" // || pName == "anti_nu_mu"   ) 
        &&
        energy > fMinNuEnergy                                )
  {
    result = true;
  }
  G4int Z = targetNucleus.GetZ_asInt();
        Z *= 1;

  return result;
}

//
//

G4HadFinalState* G4NuMuNucleusCcModel::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 < fMu ) // ~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.), massX(0.), massR(0.), eCut(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()  ) // && 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-fMu*fMu);
    muMom = sqrt(fEmu*fEmu-fMu*fMu);

    eP *= muMom;

    // lv2 = G4LorentzVector( eP, fEmuPi );
    // lv2 = G4LorentzVector( eP, fEmu );
    lv2 = fLVl;

    // lvX = lvsum - lv2;
    lvX = fLVh;
    massX2 = lvX.m2();
    massX = lvX.m();
    massR = fLVt.m();
    
    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;

    if(  pName == "nu_mu" )         aLept = new G4DynamicParticle( theMuonMinus, lv2 );  
    else if( pName == "anti_nu_mu") aLept = new G4DynamicParticle( theMuonPlus,  lv2 );
    else
    {
      theParticleChange.SetEnergyChange(energy);
      theParticleChange.SetMomentumChange(aTrack.Get4Momentum().vect().unit());
      return &theParticleChange;
    }
    if( pName == "nu_mu" ) pdgP =  211;
    else                   pdgP = -211;

    // eCut = fMpi + 0.5*(fMpi*fMpi-massX2)/mTarg; // massX -> fMpi

    eCut = (fMpi + mTarg)*(fMpi + mTarg) - (massX + massR)*(massX + massR);
    eCut /= 2.*massR;
    eCut += massX;

    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-fMu*fMu);

    eP *= muMom;

    lv2 = G4LorentzVector( eP, fEmu );
    lv2 = fLVl;
    lvX = lvsum - lv2;
    lvX = fLVh;
    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;

    if(  pName == "nu_mu" )         aLept = new G4DynamicParticle( theMuonMinus, lv2 );  
    else if( pName == "anti_nu_mu") aLept = new G4DynamicParticle( theMuonPlus,  lv2 );
    else
    {
      theParticleChange.SetEnergyChange(energy);
      theParticleChange.SetMomentumChange(aTrack.Get4Momentum().vect().unit());
      return &theParticleChange;
    }
    theParticleChange.AddSecondary( aLept );
  }

  // hadron part

  fRecoil  = nullptr;
  fCascade = false;
  fString  = false;
  
  if( A == 1 )
  {
    if( pName == "nu_mu" ) qB = 2;
    else                   qB = 0;

    // if( G4UniformRand() > 0.1 ) //  > 0.9999 ) // > 0.0001 ) //
    {
      ClusterDecay( lvX, qB );
    }
    return &theParticleChange;
  }
    /*
    // else
    {
      if( pName == "nu_mu" ) pdgP =  211;
      else                   pdgP = -211;


      if ( fQtransfer < 0.95*GeV ) // < 0.35*GeV ) //
      {
  if( lvX.m() > mSum ) CoherentPion( lvX, pdgP, targetNucleus);
      }
    }
    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);

    if( pName == "nu_mu" ) // (++) state -> p + pi+
    { 
      fMt = G4ParticleTable::GetParticleTable()->FindParticle(2212)->GetPDGMass()
          + G4ParticleTable::GetParticleTable()->FindParticle(211)->GetPDGMass();
    }
    else // (0) state -> p + pi-, n + pi0
    {
      fMt = G4ParticleTable::GetParticleTable()->FindParticle(2212)->GetPDGMass()
          + G4ParticleTable::GetParticleTable()->FindParticle(-211)->GetPDGMass();
    } 
  }
  else // excited neutron
  {
    fProton = false;
    recoil = G4Nucleus(A-1,Z);
    fRecoil = &recoil;
    rM = recoil.AtomicMass(A-1,Z);

    if( pName == "nu_mu" ) // (+) state -> n + pi+
    {      
      fMt = G4ParticleTable::GetParticleTable()->FindParticle(2112)->GetPDGMass()
          + G4ParticleTable::GetParticleTable()->FindParticle(211)->GetPDGMass();
    }
    else // (-) state -> n + pi-, // n + pi0
    {
      fMt = G4ParticleTable::GetParticleTable()->FindParticle(2112)->GetPDGMass()
          + G4ParticleTable::GetParticleTable()->FindParticle(-211)->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);
  // G4double pX   = sqrt( eX*eX - mX*mX );
  // G4double sumE = eX + rM;

  if( qeTotRat > G4UniformRand() || mX <= fMt ) // || eX <= 1232.*MeV) // QE
  {  
    fString = false;

    if( pName == "nu_mu" ) 
    {  
      fPDGencoding = 2212;
      fMr =  proton_mass_c2;
      recoil = G4Nucleus(A-1,Z);
      fRecoil = &recoil;
      rM = recoil.AtomicMass(A-1,Z);
    } 
    else // if( pName == "anti_nu_mu" ) 
    {  
      fPDGencoding = 2112;
      fMr =   G4ParticleTable::GetParticleTable()->
  FindParticle(fPDGencoding)->GetPDGMass(); // 939.5654133*MeV;
      recoil = G4Nucleus(A-1,Z-1);
      fRecoil = &recoil;
      rM = recoil.AtomicMass(A-1,Z-1);
    } 
    // sumE = eX + rM;   
    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( fLVh, 0, fPDGencoding ); // p(n)+deexcited recoil
  }
  else if ( eX < 95000.*GeV ) // <  25.*GeV) // < 95.*GeV ) // < 2.5*GeV ) //cluster decay
  {  
    if     (  fProton && pName == "nu_mu" )      qB =  2;
    else if(  fProton && pName == "anti_nu_mu" ) qB =  0;
    else if( !fProton && pName == "nu_mu" )      qB =  1;
    else if( !fProton && pName == "anti_nu_mu" ) qB = -1;

    // if( G4UniformRand() > 0.1 )
    {
      ClusterDecay( lvX, qB );
    }
    // else
    {
      if( pName == "nu_mu" ) pdgP =  211;
      else                   pdgP = -211;

      if ( fQtransfer < 0.95*GeV )  // < 0.99*GeV )  //
      {
        // if( lvX.m() > mSum ) CoherentPion( lvX, pdgP, targetNucleus);
      }
    }
  }
  else // string
  {  
    return &theParticleChange;
  } 
  return &theParticleChange;
}



//
// sample x, then Q2

void G4NuMuNucleusCcModel::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 Ex(0.), ei(0.), nm2(0.);
  G4double cost(1.), sint(0.), phi(0.), muMom(0.); 
  G4ThreeVector eP, bst;
  const G4HadProjectile* aParticle = &aTrack;
  G4LorentzVector lvp1 = aParticle->Get4Momentum();

  if( A == 1 ) // 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;
    
      pMu2 = fEmu*fEmu - fMu*fMu;
      pX2  = e3*e3 - fW2;

      fCosTheta  = fNuEnergy*fNuEnergy  + pMu2 - pX2;
      fCosTheta /= 2.*fNuEnergy*sqrt(pMu2);
      iTer++;
    }
    while( ( abs(fCosTheta) > 1. || fEmu < fMu ) && 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-fMu*fMu);
    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
  {
    G4Nucleus recoil1( A-1, Z );
    rM = recoil1.AtomicMass(A-1,Z);   
    do
    {
      // nMom = NucleonMomentumBR( targetNucleus ); // BR
      nMom = GgSampleNM( targetNucleus ); // Gg
      Ex = GetEx(A-1, fProton);
      ei = tM - sqrt( (rM + Ex)*(rM + Ex) + nMom*nMom );
      //   ei = 0.5*( tM - s2M - 2*eX );
    
      nm2 = ei*ei - nMom*nMom;
      iTer++;
    }
    while( nm2 < 0. && iTer < iTerMax ); 

    if( iTer >= iTerMax ) { fBreak = true; return; }
    
    G4ThreeVector nMomDir = nMom*G4RandomDirection();

    if( !f2p2h ) // 1p1h
    {
      // hM = tM - rM;

      fLVt = G4LorentzVector( -nMomDir, sqrt( (rM + Ex)*(rM + Ex) + nMom*nMom ) ); // rM ); //
      fLVh = G4LorentzVector(  nMomDir, ei ); // hM); //
    }
    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();

    lvp1.boost(-bst); // -> nucleon rest system, where Q2 transfer is ???

    fNuEnergy  = lvp1.e();
    G4double mN = fLVh.m();
    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
        fW2 = mN*mN - 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 - fMu*fMu;
      pX2  = e3*e3 - fW2;

      if(pMu2 < 0.)
      {
        fBreak = true;
  return;
      }
      fCosTheta  = fNuEnergy*fNuEnergy  + pMu2 - pX2;
      fCosTheta /= 2.*fNuEnergy*sqrt(pMu2);
      iTer++;
    }
    while( ( abs(fCosTheta) > 1. || fEmu < fMu ) && 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., mN ); // 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-fMu*fMu);
    eP *= muMom;
    fLVl = G4LorentzVector( eP, fEmu );
    fLVh = lvsum - fLVl;
    // back to lab system
    fLVl.boost(bst);
    fLVh.boost(bst);
  }
  //G4cout<<iTer<<", "<<fBreak<<"; ";
}


G4double G4NuMuNucleusCcModel::SampleXkr(G4double energy)
{
  G4int i(0), nBin(50);
  G4double xx(0.), prob = G4UniformRand();

  for( i = 0; i < nBin; ++i ) 
  {
    if( energy <= fNuMuEnergyLogVector[i] ) break;
  }
  if( i <= 0)          // E-edge
  {
    fEindex = 0;
    xx = GetXkr( 0, prob);  
  }
  else if ( i >= nBin) 
  {
    fEindex = nBin-1;  
    xx = GetXkr( nBin-1, prob); 
  }
  else
  {
    fEindex = i;
    G4double x1 = GetXkr(i-1,prob);
    G4double x2 = GetXkr(i,prob);

    G4double e1 = G4Log(fNuMuEnergyLogVector[i-1]);
    G4double e2 = G4Log(fNuMuEnergyLogVector[i]);
    G4double e  = G4Log(energy);

    if( e2 <= e1) xx = x1 + G4UniformRand()*(x2-x1);
    else          xx = x1 + (e-e1)*(x2-x1)/(e2-e1);  // lin in energy log-scale
  }
  return xx;
}

//
// sample X according to prob (xmin,1) at a given energy index iEnergy

G4double G4NuMuNucleusCcModel::GetXkr(G4int iEnergy, G4double prob)
{
  G4int i(0), nBin=50; 
  G4double xx(0.);

  for( i = 0; i < nBin; ++i ) 
  {
    if( prob <= fNuMuXdistrKR[iEnergy][i] ) 
      break;
  }
  if(i <= 0 )  // X-edge
  {
    fXindex = 0;
    xx = fNuMuXarrayKR[iEnergy][0];
  }
  if ( i >= nBin ) 
  {
    fXindex = nBin;
    xx = fNuMuXarrayKR[iEnergy][nBin];
  }  
  else
  {
    fXindex = i;
    G4double x1 = fNuMuXarrayKR[iEnergy][i];
    G4double x2 = fNuMuXarrayKR[iEnergy][i+1];

    G4double p1 = 0.;

    if( i > 0 ) p1 = fNuMuXdistrKR[iEnergy][i-1];

    G4double p2 = fNuMuXdistrKR[iEnergy][i];  

    if( p2 <= p1 ) xx = x1 + G4UniformRand()*(x2-x1);
    else           xx = x1 + (prob-p1)*(x2-x1)/(p2-p1);
  }
  return xx;
}

//
// Sample fQtransfer at a given Enu and fX

G4double G4NuMuNucleusCcModel::SampleQkr( G4double energy, G4double xx)
{
  G4int nBin(50), iE=fEindex, jX=fXindex;
  G4double qq(0.), qq1(0.), qq2(0.);
  G4double prob = G4UniformRand();

  // first E

  if( iE <= 0 )          
  {
    qq1 = GetQkr( 0, jX, prob);  
  }
  else if ( iE >= nBin-1) 
  {
    qq1 = GetQkr( nBin-1, jX, prob); 
  }
  else
  {
    G4double q1 = GetQkr(iE-1,jX, prob);
    G4double q2 = GetQkr(iE,jX, prob);

    G4double e1 = G4Log(fNuMuEnergyLogVector[iE-1]);
    G4double e2 = G4Log(fNuMuEnergyLogVector[iE]);
    G4double e  = G4Log(energy);

    if( e2 <= e1) qq1 = q1 + G4UniformRand()*(q2-q1);
    else          qq1 = q1 + (e-e1)*(q2-q1)/(e2-e1);  // lin in energy log-scale
  }

  // then X

  if( jX <= 0 )          
  {
    qq2 = GetQkr( iE, 0, prob);  
  }
  else if ( jX >= nBin) 
  {
    qq2 = GetQkr( iE, nBin, prob); 
  }
  else
  {
    G4double q1 = GetQkr(iE,jX-1, prob);
    G4double q2 = GetQkr(iE,jX, prob);

    G4double e1 = G4Log(fNuMuXarrayKR[iE][jX-1]);
    G4double e2 = G4Log(fNuMuXarrayKR[iE][jX]);
    G4double e  = G4Log(xx);

    if( e2 <= e1) qq2 = q1 + G4UniformRand()*(q2-q1);
    else          qq2 = q1 + (e-e1)*(q2-q1)/(e2-e1);  // lin in energy log-scale
  }
  qq = 0.5*(qq1+qq2);

  return qq;
}

//
// sample Q according to prob (qmin,qmax) at a given energy index iE and X index jX

G4double G4NuMuNucleusCcModel::GetQkr( G4int iE, G4int jX, G4double prob )
{
  G4int i(0), nBin=50; 
  G4double qq(0.);

  for( i = 0; i < nBin; ++i ) 
  {
    if( prob <= fNuMuQdistrKR[iE][jX][i] ) 
      break;
  }
  if(i <= 0 )  // Q-edge
  {
    fQindex = 0;
    qq = fNuMuQarrayKR[iE][jX][0];
  }
  if ( i >= nBin ) 
  {
    fQindex = nBin;
    qq = fNuMuQarrayKR[iE][jX][nBin];
  }  
  else
  {
    fQindex = i;
    G4double q1 = fNuMuQarrayKR[iE][jX][i];
    G4double q2 = fNuMuQarrayKR[iE][jX][i+1];

    G4double p1 = 0.;

    if( i > 0 ) p1 = fNuMuQdistrKR[iE][jX][i-1];

    G4double p2 = fNuMuQdistrKR[iE][jX][i];  

    if( p2 <= p1 ) qq = q1 + G4UniformRand()*(q2-q1);
    else           qq = q1 + (prob-p1)*(q2-q1)/(p2-p1);
  }
  return qq;
}

//
//