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//
// Hadronic Process: Low Energy Neutron Inelastic Process
// J.L. Chuma, TRIUMF, 04-Feb-1997
 
#include "G4LENeutronInelastic.hh"
#include "Randomize.hh"
#include "G4Electron.hh"
// #include "DumpFrame.hh"

 G4HadFinalState *
  G4LENeutronInelastic::ApplyYourself( const G4HadProjectile &aTrack,
                                       G4Nucleus &targetNucleus )
  {
    theParticleChange.Clear();
    const G4HadProjectile *originalIncident = &aTrack;
    //
    // create the target particle
    //
    G4DynamicParticle *originalTarget = targetNucleus.ReturnTargetParticle();
    
    if( verboseLevel > 1 )
    {
      const G4Material *targetMaterial = aTrack.GetMaterial();
      G4cout << "G4LENeutronInelastic::ApplyYourself called" << G4endl;
      G4cout << "kinetic energy = " << originalIncident->GetKineticEnergy()/MeV << "MeV, ";
      G4cout << "target material = " << targetMaterial->GetName() << ", ";
      G4cout << "target particle = " << originalTarget->GetDefinition()->GetParticleName()
           << G4endl;
    }
/* not true, for example for Fe56, etc..
    if( originalIncident->GetKineticEnergy()/MeV < 0.000001 )
      throw G4HadronicException(__FILE__, __LINE__, "G4LENeutronInelastic: should be capture process!");
    if( originalIncident->Get4Momentum().vect().mag()/MeV < 0.000001 )
      throw G4HadronicException(__FILE__, __LINE__, "G4LENeutronInelastic: should be capture process!");
*/
    
    G4ReactionProduct modifiedOriginal;
    modifiedOriginal = *originalIncident;
    G4ReactionProduct targetParticle;
    targetParticle = *originalTarget;
    if( originalIncident->GetKineticEnergy()/GeV < 0.01 + 2.*G4UniformRand()/9. )
    {
      SlowNeutron( originalIncident, modifiedOriginal, targetParticle, targetNucleus );
      delete originalTarget;
      return &theParticleChange;
    }
    //
    // Fermi motion and evaporation
    // As of Geant3, the Fermi energy calculation had not been Done
    //
    G4double ek = originalIncident->GetKineticEnergy()/MeV;
    G4double amas = originalIncident->GetDefinition()->GetPDGMass()/MeV;
    
    G4double tkin = targetNucleus.Cinema( ek );
    ek += tkin;
    modifiedOriginal.SetKineticEnergy( ek*MeV );
    G4double et = ek + amas;
    G4double p = std::sqrt( std::abs((et-amas)*(et+amas)) );
    G4double pp = modifiedOriginal.GetMomentum().mag()/MeV;
    if( pp > 0.0 )
    {
      G4ThreeVector momentum = modifiedOriginal.GetMomentum();
      modifiedOriginal.SetMomentum( momentum * (p/pp) );
    }
    //
    // calculate black track energies
    //
    tkin = targetNucleus.EvaporationEffects( ek );
    ek -= tkin;
    modifiedOriginal.SetKineticEnergy( ek*MeV );
    et = ek + amas;
    p = std::sqrt( std::abs((et-amas)*(et+amas)) );
    pp = modifiedOriginal.GetMomentum().mag()/MeV;
    if( pp > 0.0 )
    {
      G4ThreeVector momentum = modifiedOriginal.GetMomentum();
      modifiedOriginal.SetMomentum( momentum * (p/pp) );
    }
    const G4double cutOff = 0.1;
    if( modifiedOriginal.GetKineticEnergy()/MeV <= cutOff )
    {
      SlowNeutron( originalIncident, modifiedOriginal, targetParticle, targetNucleus );
      delete originalTarget;
      return &theParticleChange;
    }
    G4ReactionProduct currentParticle = modifiedOriginal;
    currentParticle.SetSide( 1 ); // incident always goes in forward hemisphere
    targetParticle.SetSide( -1 );  // target always goes in backward hemisphere
    G4bool incidentHasChanged = false;
    G4bool targetHasChanged = false;
    G4bool quasiElastic = false;
    G4FastVector<G4ReactionProduct,GHADLISTSIZE> vec;  // vec will contain the secondary particles
    G4int vecLen = 0;
    vec.Initialize( 0 );
    
    Cascade( vec, vecLen,
             originalIncident, currentParticle, targetParticle,
             incidentHasChanged, targetHasChanged, quasiElastic );
    
    CalculateMomenta( vec, vecLen,
                      originalIncident, originalTarget, modifiedOriginal,
                      targetNucleus, currentParticle, targetParticle,
                      incidentHasChanged, targetHasChanged, quasiElastic );
    
    SetUpChange( vec, vecLen,
                 currentParticle, targetParticle,
                 incidentHasChanged );
    
    delete originalTarget;
    return &theParticleChange;
  }
 
 void
  G4LENeutronInelastic::SlowNeutron(
   const G4HadProjectile *originalIncident,
   G4ReactionProduct &modifiedOriginal,
   G4ReactionProduct &targetParticle,
   G4Nucleus &targetNucleus )
  {        
    const G4double A = targetNucleus.GetN();    // atomic weight
    const G4double Z = targetNucleus.GetZ();    // atomic number
    
    G4double currentKinetic = modifiedOriginal.GetKineticEnergy()/MeV;
    G4double currentMass = modifiedOriginal.GetMass()/MeV;
    if( A < 1.5 )   // Hydrogen
    {
      //
      // very simple simulation of scattering angle and energy
      // nonrelativistic approximation with isotropic angular
      // distribution in the cms system 
      //
      G4double cost1, eka = 0.0;
      while (eka <= 0.0)
      {
        cost1 = -1.0 + 2.0*G4UniformRand();
        eka = 1.0 + 2.0*cost1*A + A*A;
      }
      G4double cost = std::min( 1.0, std::max( -1.0, (A*cost1+1.0)/std::sqrt(eka) ) );
      eka /= (1.0+A)*(1.0+A);
      G4double ek = currentKinetic*MeV/GeV;
      G4double amas = currentMass*MeV/GeV;
      ek *= eka;
      G4double en = ek + amas;
      G4double p = std::sqrt(std::abs(en*en-amas*amas));
      G4double sint = std::sqrt(std::abs(1.0-cost*cost));
      G4double phi = G4UniformRand()*twopi;
      G4double px = sint*std::sin(phi);
      G4double py = sint*std::cos(phi);
      G4double pz = cost;
      targetParticle.SetMomentum( px*GeV, py*GeV, pz*GeV );
      G4double pxO = originalIncident->Get4Momentum().x()/GeV;
      G4double pyO = originalIncident->Get4Momentum().y()/GeV;
      G4double pzO = originalIncident->Get4Momentum().z()/GeV;
      G4double ptO = pxO*pxO + pyO+pyO;
      if( ptO > 0.0 )
      {
        G4double pO = std::sqrt(pxO*pxO+pyO*pyO+pzO*pzO);
        cost = pzO/pO;
        sint = 0.5*(std::sqrt(std::abs((1.0-cost)*(1.0+cost)))+std::sqrt(ptO)/pO);
        G4double ph = pi/2.0;
        if( pyO < 0.0 )ph = ph*1.5;
        if( std::abs(pxO) > 0.000001 )ph = std::atan2(pyO,pxO);
        G4double cosp = std::cos(ph);
        G4double sinp = std::sin(ph);
        px = cost*cosp*px - sinp*py+sint*cosp*pz;
        py = cost*sinp*px + cosp*py+sint*sinp*pz;
        pz = -sint*px     + cost*pz;
      }
      else
      {
        if( pz < 0.0 )pz *= -1.0;
      }
      G4double pu = std::sqrt(px*px+py*py+pz*pz);
      modifiedOriginal.SetMomentum( targetParticle.GetMomentum() * (p/pu) );
      modifiedOriginal.SetKineticEnergy( ek*GeV );
      
      targetParticle.SetMomentum(
       originalIncident->Get4Momentum().vect() - modifiedOriginal.GetMomentum() );
      G4double pp = targetParticle.GetMomentum().mag();
      G4double tarmas = targetParticle.GetMass();
      targetParticle.SetTotalEnergy( std::sqrt( pp*pp + tarmas*tarmas ) );
      
      theParticleChange.SetEnergyChange( modifiedOriginal.GetKineticEnergy() );
      G4DynamicParticle *pd = new G4DynamicParticle;
      pd->SetDefinition( targetParticle.GetDefinition() );
      pd->SetMomentum( targetParticle.GetMomentum() );
      theParticleChange.AddSecondary( pd );
      return;
    }
    G4FastVector<G4ReactionProduct,4> vec;  // vec will contain the secondary particles
    G4int vecLen = 0;
    vec.Initialize( 0 );
    
    G4double theAtomicMass = targetNucleus.AtomicMass( A, Z );
    G4double massVec[9];
    massVec[0] = targetNucleus.AtomicMass( A+1.0, Z     );
    massVec[1] = theAtomicMass;
    massVec[2] = 0.;
    if (Z > 1.0) 
        massVec[2] = targetNucleus.AtomicMass( A    , Z-1.0 );
    massVec[3] = 0.;
    if (Z > 1.0 && A > 1.0) 
        massVec[3] = targetNucleus.AtomicMass( A-1.0, Z-1.0 );
    massVec[4] = 0.;
    if (Z > 1.0 && A > 2.0 && A-2.0 > Z-1.0)
        massVec[4] = targetNucleus.AtomicMass( A-2.0, Z-1.0 );
    massVec[5] = 0.;
    if (Z > 2.0 && A > 3.0 && A-3.0 > Z-2.0)
        massVec[5] = targetNucleus.AtomicMass( A-3.0, Z-2.0 );
    massVec[6] = 0.;
    if (A > 1.0 && A-1.0 > Z) 
        massVec[6] = targetNucleus.AtomicMass( A-1.0, Z     );
    massVec[7] = massVec[3];
    massVec[8] = 0.;
    if (Z > 2.0 && A > 1.0)
        massVec[8] = targetNucleus.AtomicMass( A-1.0, Z-2.0 );
    
    theReactionDynamics.NuclearReaction( vec, vecLen, originalIncident,
                                         targetNucleus, theAtomicMass, massVec );
    
    theParticleChange.SetStatusChange( stopAndKill );
    theParticleChange.SetEnergyChange( 0.0 );
    
    G4DynamicParticle * pd;
    for( G4int i=0; i<vecLen; ++i )
    {
      pd = new G4DynamicParticle();
      pd->SetDefinition( vec[i]->GetDefinition() );
      pd->SetMomentum( vec[i]->GetMomentum() );
      theParticleChange.AddSecondary( pd );
      delete vec[i];
    }
  }
 
 void
  G4LENeutronInelastic::Cascade(
   G4FastVector<G4ReactionProduct,GHADLISTSIZE> &vec,
   G4int& vecLen,
   const G4HadProjectile *originalIncident,
   G4ReactionProduct &currentParticle,
   G4ReactionProduct &targetParticle,
   G4bool &incidentHasChanged,
   G4bool &targetHasChanged,
   G4bool &quasiElastic )
  {
    // derived from original FORTRAN code CASN by H. Fesefeldt (13-Sep-1987)
    //
    // Neutron undergoes interaction with nucleon within a nucleus.  Check if it is
    // energetically possible to produce pions/kaons.  In not, assume nuclear excitation
    // occurs and input particle is degraded in energy. No other particles are produced.
    // If reaction is possible, find the correct number of pions/protons/neutrons
    // produced using an interpolation to multiplicity data.  Replace some pions or
    // protons/neutrons by kaons or strange baryons according to the average
    // multiplicity per Inelastic reaction.
    //
    const G4double mOriginal = originalIncident->GetDefinition()->GetPDGMass()/MeV;
    const G4double etOriginal = originalIncident->GetTotalEnergy()/MeV;
    const G4double targetMass = targetParticle.GetMass()/MeV;
    G4double centerofmassEnergy = std::sqrt( mOriginal*mOriginal +
                                        targetMass*targetMass +
                                        2.0*targetMass*etOriginal );
    G4double availableEnergy = centerofmassEnergy-(targetMass+mOriginal);
    if( availableEnergy <= G4PionPlus::PionPlus()->GetPDGMass()/MeV )
    {
      quasiElastic = true;
      return;
    }
    static G4bool first = true;
    const G4int numMul = 1200;
    const G4int numSec = 60;
    static G4double protmul[numMul], protnorm[numSec]; // proton constants
    static G4double neutmul[numMul], neutnorm[numSec]; // neutron constants
    // np = number of pi+, nm = number of pi-, nz = number of pi0
    G4int counter, nt=0, np=0, nm=0, nz=0;
    const G4double c = 1.25;    
    const G4double b[] = { 0.35, 0.0 };
    if( first )      // compute normalization constants, this will only be Done once
    {
      first = false;
      G4int i;
      for( i=0; i<numMul; ++i )protmul[i] = 0.0;
      for( i=0; i<numSec; ++i )protnorm[i] = 0.0;
      counter = -1;
      for( np=0; np<numSec/3; ++np )
      {
        for( nm=std::max(0,np-1); nm<=(np+1); ++nm )
        {
          for( nz=0; nz<numSec/3; ++nz )
          {
            if( ++counter < numMul )
            {
              nt = np+nm+nz;
              if( nt > 0 )
              {
                protmul[counter] = Pmltpc(np,nm,nz,nt,b[0],c) /
                  ( theReactionDynamics.Factorial(1-np+nm)*
                    theReactionDynamics.Factorial(1+np-nm) );
                protnorm[nt-1] += protmul[counter];
              }
            }
          }
        }
      }
      for( i=0; i<numMul; ++i )neutmul[i] = 0.0;
      for( i=0; i<numSec; ++i )neutnorm[i] = 0.0;
      counter = -1;
      for( np=0; np<(numSec/3); ++np )
      {
        for( nm=np; nm<=(np+2); ++nm )
        {
          for( nz=0; nz<numSec/3; ++nz )
          {
            if( ++counter < numMul )
            {
              nt = np+nm+nz;
              if( (nt>0) && (nt<=numSec) )
              {
                neutmul[counter] = Pmltpc(np,nm,nz,nt,b[1],c) /
                  ( theReactionDynamics.Factorial(nm-np)*
                    theReactionDynamics.Factorial(2-nm+np) );
                neutnorm[nt-1] += neutmul[counter];
              }
            }
          }
        }
      }
      for( i=0; i<numSec; ++i )
      {
        if( protnorm[i] > 0.0 )protnorm[i] = 1.0/protnorm[i];
        if( neutnorm[i] > 0.0 )neutnorm[i] = 1.0/neutnorm[i];
      }
    }   // end of initialization
    
    const G4double expxu = 82.;      // upper bound for arg. of exp
    const G4double expxl = -expxu;        // lower bound for arg. of exp
    G4ParticleDefinition *aNeutron = G4Neutron::Neutron();
    G4ParticleDefinition *aProton = G4Proton::Proton();
    G4int ieab = static_cast<G4int>(availableEnergy*5.0/GeV);
    const G4double supp[] = {0.,0.4,0.55,0.65,0.75,0.82,0.86,0.90,0.94,0.98};
    G4double test, w0, wp, wt, wm;
    if( (availableEnergy < 2.0*GeV) && (G4UniformRand() >= supp[ieab]) )
    {
      // suppress high multiplicity events at low momentum
      // only one pion will be produced

      nm = np = nz = 0;
      if( targetParticle.GetDefinition() == aNeutron )
      {
        test = std::exp( std::min( expxu, std::max( expxl, -(1.0+b[1])*(1.0+b[1])/(2.0*c*c) ) ) );
        w0 = test/2.0;
        wm = test;
        if( G4UniformRand() < w0/(w0+wm) )
          nz = 1;
        else
          nm = 1;
      } else { // target is a proton
        test = std::exp( std::min( expxu, std::max( expxl, -(1.0+b[0])*(1.0+b[0])/(2.0*c*c) ) ) );
        w0 = test;
        wp = test/2.0;        
        test = std::exp( std::min( expxu, std::max( expxl, -(-1.0+b[0])*(-1.0+b[0])/(2.0*c*c) ) ) );
        wm = test/2.0;
        wt = w0+wp+wm;
        wp += w0;
        G4double ran = G4UniformRand();
        if( ran < w0/wt )
          nz = 1;
        else if( ran < wp/wt )
          np = 1;
        else
          nm = 1;
      }
    } else {  // (availableEnergy >= 2.0*GeV) || (random number < supp[ieab])
      G4double n, anpn;
      GetNormalizationConstant( availableEnergy, n, anpn );
      G4double ran = G4UniformRand();
      G4double dum, excs = 0.0;
      if( targetParticle.GetDefinition() == aProton )
      {
        counter = -1;
        for( np=0; np<numSec/3 && ran>=excs; ++np )
        {
          for( nm=std::max(0,np-1); nm<=(np+1) && ran>=excs; ++nm )
          {
            for( nz=0; nz<numSec/3 && ran>=excs; ++nz )
            {
              if( ++counter < numMul )
              {
                nt = np+nm+nz;
                if( nt > 0 )
                {
                  test = std::exp( std::min( expxu, std::max( expxl, -(pi/4.0)*(nt*nt)/(n*n) ) ) );
                  dum = (pi/anpn)*nt*protmul[counter]*protnorm[nt-1]/(2.0*n*n);
                  if( std::fabs(dum) < 1.0 ) {
                    if( test >= 1.0e-10 )excs += dum*test;
                  } else {
                    excs += dum*test;
                  }
                }
              }
            }
          }
        }
        if( ran >= excs )  // 3 previous loops continued to the end
        {
          quasiElastic = true;
          return;
        }
        np--; nm--; nz--;
      } else { // target must be a neutron
        counter = -1;
        for( np=0; np<numSec/3 && ran>=excs; ++np )
        {
          for( nm=np; nm<=(np+2) && ran>=excs; ++nm )
          {
            for( nz=0; nz<numSec/3 && ran>=excs; ++nz )
            {
              if( ++counter < numMul )
              {
                nt = np+nm+nz;
                if( (nt>=1) && (nt<=numSec) )
                {
                  test = std::exp( std::min( expxu, std::max( expxl, -(pi/4.0)*(nt*nt)/(n*n) ) ) );
                  dum = (pi/anpn)*nt*neutmul[counter]*neutnorm[nt-1]/(2.0*n*n);
                  if( std::fabs(dum) < 1.0 ) {
                    if( test >= 1.0e-10 )excs += dum*test;
                  } else {
                    excs += dum*test;
                  }
                }
              }
            }
          }
        }
        if( ran >= excs )  // 3 previous loops continued to the end
        {
          quasiElastic = true;
          return;
        }
        np--; nm--; nz--;
      }
    }
    if( targetParticle.GetDefinition() == aProton )
    {
      switch( np-nm )
      {
       case 0:
         if( G4UniformRand() < 0.33 )
         {
           currentParticle.SetDefinitionAndUpdateE( aProton );
           targetParticle.SetDefinitionAndUpdateE( aNeutron );
           incidentHasChanged = true;
           targetHasChanged = true;
         }
         break;
       case 1:
         targetParticle.SetDefinitionAndUpdateE( aNeutron );
         targetHasChanged = true;
         break;
       default:
         currentParticle.SetDefinitionAndUpdateE( aProton );
         incidentHasChanged = true;
         break;
      }
    } else { // target must be a neutron
      switch( np-nm )
      {
       case -1:                       // changed from +1 by JLC, 7Jul97
         if( G4UniformRand() < 0.5 )
         {
           currentParticle.SetDefinitionAndUpdateE( aProton );
           incidentHasChanged = true;
         } else {
           targetParticle.SetDefinitionAndUpdateE( aProton );
           targetHasChanged = true;
         }
         break;
       case 0:
         break;
       default:
         currentParticle.SetDefinitionAndUpdateE( aProton );
         targetParticle.SetDefinitionAndUpdateE( aProton );
         incidentHasChanged = true;
         targetHasChanged = true;
         break;
      }
    }
    SetUpPions( np, nm, nz, vec, vecLen );
// DEBUG -->    DumpFrames::DumpFrame(vec, vecLen);
    return;
  }

 /* end of file */