G4LElastic.cc

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// Physics model class G4LElastic
// G4 Model: Low-energy Elastic scattering
// F.W. Jones, TRIUMF, 04-JUN-96
//
// use -scheme for elastic scattering: HPW, 20th June 1997
// most of the code comes from the old Low-energy Elastic class
//
// 25-JUN-98 FWJ: replaced missing Initialize for ParticleChange.
// 14-DEC-05 V.Ivanchenko: restore 1.19 version (7.0)
// 23-JAN-07 V.Ivanchenko: add protection inside sqrt
 
#include <iostream>
 
#include "G4LElastic.hh"
#include "globals.hh"
#include "G4PhysicalConstants.hh"
#include "G4SystemOfUnits.hh"
#include "Randomize.hh"
#include "G4ParticleTable.hh"
#include "G4IonTable.hh"
 
G4LElastic::G4LElastic(const G4String& name)
 :G4HadronicInteraction(name)
{
  SetMinEnergy(0.0);
  SetMaxEnergy(DBL_MAX);
}
 
 
void G4LElastic::ModelDescription(std::ostream& outFile) const
{
  outFile << "G4LElastic is one of the Low Energy Parameterized (LEP)\n"
          << "models used to implement elastic hadron scattering from nuclei.\n"
          << "It is a re-engineered version of the GHEISHA code of\n"
          << "H. Fesefeldt.  It performs simplified two-body elastic\n"
          << "scattering for all long-lived hadronic projectiles by using\n"
          << "a two-exponential parameterization in momentum transfer.\n"
          << "It is valid for incident hadrons of all energies.\n";
}
 
 
G4HadFinalState*
G4LElastic::ApplyYourself(const G4HadProjectile& aTrack, G4Nucleus& targetNucleus)
{
  if(getenv("debug_LElastic")) verboseLevel = 5;
  theParticleChange.Clear();
  const G4HadProjectile* aParticle = &aTrack;
  G4double atno2 = targetNucleus.GetA_asInt();
  G4double zTarget = targetNucleus.GetZ_asInt();
  theParticleChange.SetEnergyChange(aTrack.GetKineticEnergy());
  theParticleChange.SetMomentumChange(aTrack.Get4Momentum().vect().unit());
 
  // Elastic scattering off Hydrogen
 
  G4DynamicParticle* aSecondary = 0;
  if (atno2 < 1.5) {
    const G4ParticleDefinition* aParticleType = aParticle->GetDefinition();
    if (aParticleType == G4PionPlus::PionPlus())
       aSecondary = LightMedia.PionPlusExchange(aParticle, targetNucleus);
    else if (aParticleType == G4PionMinus::PionMinus())
       aSecondary = LightMedia.PionMinusExchange(aParticle, targetNucleus);
    else if (aParticleType == G4KaonPlus::KaonPlus())
       aSecondary = LightMedia.KaonPlusExchange(aParticle, targetNucleus);
    else if (aParticleType == G4KaonZeroShort::KaonZeroShort())
       aSecondary = LightMedia.KaonZeroShortExchange(aParticle,targetNucleus);
    else if (aParticleType == G4KaonZeroLong::KaonZeroLong())
       aSecondary = LightMedia.KaonZeroLongExchange(aParticle, targetNucleus);
    else if (aParticleType == G4KaonMinus::KaonMinus())
       aSecondary = LightMedia.KaonMinusExchange(aParticle, targetNucleus);
    else if (aParticleType == G4Proton::Proton())
       aSecondary = LightMedia.ProtonExchange(aParticle, targetNucleus);
    else if (aParticleType == G4AntiProton::AntiProton())
       aSecondary = LightMedia.AntiProtonExchange(aParticle, targetNucleus);
    else if (aParticleType == G4Neutron::Neutron())
       aSecondary = LightMedia.NeutronExchange(aParticle, targetNucleus);
    else if (aParticleType == G4AntiNeutron::AntiNeutron())
       aSecondary = LightMedia.AntiNeutronExchange(aParticle, targetNucleus);
    else if (aParticleType == G4Lambda::Lambda())
       aSecondary = LightMedia.LambdaExchange(aParticle, targetNucleus);
    else if (aParticleType == G4AntiLambda::AntiLambda())
       aSecondary = LightMedia.AntiLambdaExchange(aParticle, targetNucleus);
    else if (aParticleType == G4SigmaPlus::SigmaPlus())
       aSecondary = LightMedia.SigmaPlusExchange(aParticle, targetNucleus);
    else if (aParticleType == G4SigmaMinus::SigmaMinus())
       aSecondary = LightMedia.SigmaMinusExchange(aParticle, targetNucleus);
    else if (aParticleType == G4AntiSigmaPlus::AntiSigmaPlus())
       aSecondary = LightMedia.AntiSigmaPlusExchange(aParticle,targetNucleus);
    else if (aParticleType == G4AntiSigmaMinus::AntiSigmaMinus())
       aSecondary= LightMedia.AntiSigmaMinusExchange(aParticle,targetNucleus);
    else if (aParticleType == G4XiZero::XiZero())
       aSecondary = LightMedia.XiZeroExchange(aParticle, targetNucleus);
    else if (aParticleType == G4XiMinus::XiMinus())
       aSecondary = LightMedia.XiMinusExchange(aParticle, targetNucleus);
    else if (aParticleType == G4AntiXiZero::AntiXiZero())
       aSecondary = LightMedia.AntiXiZeroExchange(aParticle, targetNucleus);
    else if (aParticleType == G4AntiXiMinus::AntiXiMinus())
       aSecondary = LightMedia.AntiXiMinusExchange(aParticle, targetNucleus);
    else if (aParticleType == G4OmegaMinus::OmegaMinus())
       aSecondary = LightMedia.OmegaMinusExchange(aParticle, targetNucleus);
    else if (aParticleType == G4AntiOmegaMinus::AntiOmegaMinus())
       aSecondary= LightMedia.AntiOmegaMinusExchange(aParticle,targetNucleus);
    else if (aParticleType == G4KaonPlus::KaonPlus())
       aSecondary = LightMedia.KaonPlusExchange(aParticle, targetNucleus);
  }
 
  // Has a charge or strangeness exchange occurred?
   if (aSecondary) {
      aSecondary->SetMomentum(aParticle->Get4Momentum().vect());
      theParticleChange.SetStatusChange(stopAndKill);
      theParticleChange.AddSecondary(aSecondary);
   }
   // G4cout << "Entering elastic scattering 1"<<G4endl;
 
   G4double p = aParticle->GetTotalMomentum()/GeV;
   if (verboseLevel > 1)
      G4cout << "G4LElastic::DoIt: Incident particle p=" << p << " GeV" << G4endl;
 
   if (p < 0.01) return &theParticleChange;
 
   // G4cout << "Entering elastic scattering 2"<<G4endl;
// Compute the direction of elastic scattering.
// It is planned to replace this code with a method based on
// parameterized functions and a Monte Carlo method to invert the CDF.
 
   G4double ran = G4UniformRand();
   G4double aa, bb, cc, dd, rr;
   if (atno2 <= 62.) {
      aa = std::pow(atno2, 1.63);
      bb = 14.5*std::pow(atno2, 0.66);
      cc = 1.4*std::pow(atno2, 0.33);
      dd = 10.;
   }
   else {
      aa = std::pow(atno2, 1.33);
      bb = 60.*std::pow(atno2, 0.33);
      cc = 0.4*std::pow(atno2, 0.40);
      dd = 10.;
   }
   aa = aa/bb;
   cc = cc/dd;
   rr = (aa + cc)*ran;
   if (verboseLevel > 1) {
      G4cout << "DoIt: aa,bb,cc,dd,rr" << G4endl;
      G4cout << aa << " " << bb << " " << cc << " " << dd << " " << rr << G4endl;
   }
   G4double t1 = -std::log(ran)/bb;
   G4double t2 = -std::log(ran)/dd;
   if (verboseLevel > 1) {
      G4cout << "t1,Fctcos " << t1 << " " << Fctcos(t1, aa, bb, cc, dd, rr) << 
              G4endl;
      G4cout << "t2,Fctcos " << t2 << " " << Fctcos(t2, aa, bb, cc, dd, rr) << 
              G4endl;
   }
   G4double eps = 0.001;
   G4int ind1 = 10;
   G4double t;
   G4int ier1;
   ier1 = Rtmi(&t, t1, t2, eps, ind1,
               aa, bb, cc, dd, rr);
   if (verboseLevel > 1) {
      G4cout << "From Rtmi, ier1=" << ier1 << G4endl;
      G4cout << "t, Fctcos " << t << " " << Fctcos(t, aa, bb, cc, dd, rr) << 
              G4endl;
   }
   if (ier1 != 0) t = 0.25*(3.*t1 + t2);
   if (verboseLevel > 1) {
      G4cout << "t, Fctcos " << t << " " << Fctcos(t, aa, bb, cc, dd, rr) << 
              G4endl;
   }
   G4double phi = G4UniformRand()*twopi;
   rr = 0.5*t/(p*p);
   if (rr > 1.) rr = 0.;
   if (verboseLevel > 1)
      G4cout << "rr=" << rr << G4endl;
   G4double cost = 1. - rr;
   G4double sint = std::sqrt(std::max(rr*(2. - rr), 0.));
   if (sint == 0.) return &theParticleChange;
   // G4cout << "Entering elastic scattering 3"<<G4endl;
   if (verboseLevel > 1)
     G4cout << "cos(t)=" << cost << "  std::sin(t)=" << sint << G4endl;
 
   // Scattered particle referred to axis of incident particle
   G4double mass1 = aParticle->GetDefinition()->GetPDGMass();
   G4int Z=static_cast<G4int>(zTarget+.5);
   G4int A=static_cast<G4int>(atno2);
   if(G4UniformRand()<atno2-A) A++;
   //G4cout << " ion info "<<atno2 << " "<<A<<" "<<Z<<" "<<zTarget<<G4endl;
   G4double mass2 =
     G4ParticleTable::GetParticleTable()->FindIon(Z,A,0,Z)->GetPDGMass();
 
   // non relativistic approximation
   G4double a = 1 + mass2/mass1;
   G4double b = -2.*p*cost;
   G4double c = p*p*(1 - mass2/mass1);
   G4double p1 = (-b+std::sqrt(std::max(0.0,b*b-4.*a*c)))/(2.*a);
   G4double px = p1*sint*std::sin(phi);
   G4double py = p1*sint*std::cos(phi);
   G4double pz = p1*cost;
 
// relativistic calculation
   G4double etot = std::sqrt(mass1*mass1+p*p)+mass2;
   a = etot*etot-p*p*cost*cost;
   b = 2*p*p*(mass1*cost*cost-etot);
   c = p*p*p*p*sint*sint;
   
   G4double de = (-b-std::sqrt(std::max(0.0,b*b-4.*a*c)))/(2.*a);
   G4double e1 = std::sqrt(p*p+mass1*mass1)-de;
   G4double p12=e1*e1-mass1*mass1;
   p1 = std::sqrt(std::max(1.*eV*eV,p12));
   px = p1*sint*std::sin(phi);
   py = p1*sint*std::cos(phi);
   pz = p1*cost;
 
   if (verboseLevel > 1) 
   {
     G4cout << "Relevant test "<<p<<" "<<p1<<" "<<cost<<" "<<de<<G4endl;
     G4cout << "p1/p = "<<p1/p<<" "<<mass1<<" "<<mass2<<" "<<a<<" "<<b<<" "<<c<<G4endl;
     G4cout << "rest = "<< b*b<<" "<<4.*a*c<<" "<<G4endl;
     G4cout << "make p1 = "<< p12<<" "<<e1*e1<<" "<<mass1*mass1<<" "<<G4endl;
   }
// Incident particle
   G4double pxinc = p*aParticle->Get4Momentum().vect().unit().x();
   G4double pyinc = p*aParticle->Get4Momentum().vect().unit().y();
   G4double pzinc = p*aParticle->Get4Momentum().vect().unit().z();
   if (verboseLevel > 1) {
      G4cout << "NOM SCAT " << px << " " << py << " " << pz << G4endl;
      G4cout << "INCIDENT " << pxinc << " " << pyinc << " " << pzinc << G4endl;
   }
  
// Transform scattered particle to reflect direction of incident particle
   G4double pxnew, pynew, pznew;
   Defs1(p, px, py, pz, pxinc, pyinc, pzinc, &pxnew, &pynew, &pznew);
// Normalize:
   G4double pxre=pxinc-pxnew;
   G4double pyre=pyinc-pynew;
   G4double pzre=pzinc-pznew;
   G4ThreeVector it0(pxnew*GeV, pynew*GeV, pznew*GeV);
   if(p1>0)
   {
     pxnew = pxnew/p1;
     pynew = pynew/p1;
     pznew = pznew/p1;
   }
   else
   {
     //G4double pphi = 2*pi*G4UniformRand();
     //G4double ccth = 2*G4UniformRand()-1;
     pxnew = 0;//std::sin(std::acos(ccth))*std::sin(pphi);
     pynew = 0;//std::sin(std::acos(ccth))*std::cos(phi);
     pznew = 1;//ccth;
   }
   if (verboseLevel > 1) {
      G4cout << "DoIt: returning new momentum vector" << G4endl;
      G4cout << "DoIt: "<<pxinc << " " << pyinc << " " << pzinc <<" "<<p<< G4endl;
      G4cout << "DoIt: "<<pxnew << " " << pynew << " " << pznew <<" "<<p<< G4endl;
   }
 
   if (aSecondary) {
     aSecondary->SetMomentumDirection(pxnew, pynew, pznew);
   } else {
     try
     {
       theParticleChange.SetMomentumChange(pxnew, pynew, pznew);
       theParticleChange.SetEnergyChange(std::sqrt(mass1*mass1+it0.mag2())-mass1);
     }
     catch(G4HadronicException)
     {
       std::cerr << "GHADException originating from components of G4LElastic"<<std::cout;
       throw;
     }
     G4ParticleDefinition * theDef = G4ParticleTable::GetParticleTable()->FindIon(Z,A,0,Z);
     G4ThreeVector it(pxre*GeV, pyre*GeV, pzre*GeV);
     G4DynamicParticle * aSec = 
       new G4DynamicParticle(theDef, it.unit(), it.mag2()/(2.*mass2));
     theParticleChange.AddSecondary(aSec);
     // G4cout << "Final check ###### "<<p<<" "<<it.mag()<<" "<<p1<<G4endl;
   }
   return &theParticleChange;
}
 
 
// The following is a "translation" of a root-finding routine
// from GEANT3.21/GHEISHA.  Some of the labelled block structure has
// been retained for clarity.  This routine will not be needed after
// the planned revisions to DoIt().
 
G4int
G4LElastic::Rtmi(G4double* x, G4double xli, G4double xri, G4double eps, 
                 G4int iend, 
                 G4double aa, G4double bb, G4double cc, G4double dd, 
                 G4double rr)
{
   G4int ier = 0;
   G4double xl = xli;
   G4double xr = xri;
   *x = xl;
   G4double tol = *x;
   G4double f = Fctcos(tol, aa, bb, cc, dd, rr);
   if (f == 0.) return ier;
   G4double fl, fr;
   fl = f;
   *x = xr;
   tol = *x;
   f = Fctcos(tol, aa, bb, cc, dd, rr);
   if (f == 0.) return ier;
   fr = f;
 
// Error return in case of wrong input data
   if (fl*fr >= 0.) {
      ier = 2;
      return ier;
   }
 
// Basic assumption fl*fr less than 0 is satisfied.
// Generate tolerance for function values.
   G4int i = 0;
   G4double tolf = 100.*eps;
 
// Start iteration loop
label4:
   i++;
 
// Start bisection loop
   for (G4int k = 1; k <= iend; k++) {
      *x = 0.5*(xl + xr);
      tol = *x;
      f = Fctcos(tol, aa, bb, cc, dd, rr);
      if (f == 0.) return 0;
      if (f*fr < 0.) {      // Interchange xl and xr in order to get the
         tol = xl;          // same Sign in f and fr
         xl = xr;
         xr = tol;
         tol = fl;
         fl = fr;
         fr = tol;
      }
      tol = f - fl;
      G4double a = f*tol;
      a = a + a;
      if (a < fr*(fr - fl) && i <= iend) goto label17;
      xr = *x;
      fr = f;
 
// Test on satisfactory accuracy in bisection loop
      tol = eps;
      a = std::abs(xr);
      if (a > 1.) tol = tol*a;
      if (std::abs(xr - xl) <= tol && std::abs(fr - fl) <= tolf) goto label14;
   }
// End of bisection loop
 
// No convergence after iend iteration steps followed by iend
// successive steps of bisection or steadily increasing function
// values at right bounds.  Error return.
   ier = 1;
 
label14:
   if (std::abs(fr) > std::abs(fl)) {
      *x = xl;
      f = fl;
   }
   return ier;
 
// Computation of iterated x-value by inverse parabolic interp
label17:
   G4double a = fr - f;
   G4double dx = (*x - xl)*fl*(1. + f*(a - tol)/(a*(fr - fl)))/tol;
   G4double xm = *x;
   G4double fm = f;
   *x = xl - dx;
   tol = *x;
   f = Fctcos(tol, aa, bb, cc, dd, rr);
   if (f == 0.) return ier;
 
// Test on satisfactory accuracy in iteration loop
   tol = eps;
   a = std::abs(*x);
   if (a > 1) tol = tol*a;
   if (std::abs(dx) <= tol && std::abs(f) <= tolf) return ier;
 
// Preparation of next bisection loop
   if (f*fl < 0.) {
      xr = *x;
      fr = f;
   }
   else {
      xl = *x;
      fl = f;
      xr = xm;
      fr = fm;
   }
   goto label4;
}
 
 
// Test function for root-finder
 
G4double
G4LElastic::Fctcos(G4double t, 
                   G4double aa, G4double bb, G4double cc, G4double dd, 
                   G4double rr)
{
   const G4double expxl = -82.;
   const G4double expxu = 82.;
 
   G4double test1 = -bb*t;
   if (test1 > expxu) test1 = expxu;
   if (test1 < expxl) test1 = expxl;
 
   G4double test2 = -dd*t;
   if (test2 > expxu) test2 = expxu;
   if (test2 < expxl) test2 = expxl;
 
   return aa*std::exp(test1) + cc*std::exp(test2) - rr;
}
 
 
void
G4LElastic::Defs1(G4double p, G4double px, G4double py, G4double pz, 
                  G4double pxinc, G4double pyinc, G4double pzinc, 
                  G4double* pxnew, G4double* pynew, G4double* pznew)
{
// Transform scattered particle to reflect direction of incident particle
   G4double pt2 = pxinc*pxinc + pyinc*pyinc;
   if (pt2 > 0.) {
      G4double cost = pzinc/p;
      G4double sint1 = std::sqrt(std::abs((1. - cost )*(1.+cost)));
      G4double sint2 = std::sqrt(pt2)/p;
      G4double sint = 0.5*(sint1 + sint2);
      G4double ph = pi*0.5;
      if (pyinc < 0.) ph = pi*1.5;
      if (std::abs(pxinc) > 1.e-6) ph = std::atan2(pyinc, pxinc);
      G4double cosp = std::cos(ph);
      G4double sinp = std::sin(ph);
      if (verboseLevel > 1) {
         G4cout << "cost sint " << cost << " " << sint << G4endl;
         G4cout << "cosp sinp " << cosp << " " << sinp << G4endl;
      }
      *pxnew = cost*cosp*px - sinp*py + sint*cosp*pz;
      *pynew = cost*sinp*px + cosp*py + sint*sinp*pz;
      *pznew =     -sint*px                 +cost*pz;
   }
   else {
       G4double cost=pzinc/p;
       *pxnew = cost*px;
       *pynew = py;
       *pznew = cost*pz;
   }
}
 
const std::pair<G4double, G4double> G4LElastic::GetFatalEnergyCheckLevels() const
{
    return std::pair<G4double, G4double>(5*perCent,250*GeV);  // max energy non-conservation is mass of heavy nucleus
}