G4INCLDeuteronDensity.cc

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//
// INCL++ intra-nuclear cascade model
// Alain Boudard, CEA-Saclay, France
// Joseph Cugnon, University of Liege, Belgium
// Jean-Christophe David, CEA-Saclay, France
// Pekka Kaitaniemi, CEA-Saclay, France, and Helsinki Institute of Physics, Finland
// Sylvie Leray, CEA-Saclay, France
// Davide Mancusi, CEA-Saclay, France
//
#define INCLXX_IN_GEANT4_MODE 1
 
#include "globals.hh"
 
#include "G4INCLDeuteronDensity.hh"
#include "G4INCLGlobals.hh"
// #include <cassert>
#include <algorithm>
 
namespace G4INCL {
 
  namespace DeuteronDensity {
 
    namespace {
 
      const G4int coeffTableSize = 13;
 
      const G4double coeff1[coeffTableSize] = {
        0.88688076e+0,
        -0.34717093e+0,
        -0.30502380e+1,
        0.56207766e+2,
        -0.74957334e+3,
        0.53365279e+4,
        -0.22706863e+5,
        0.60434469e+5,
        -0.10292058e+6,
        0.11223357e+6,
        -0.75925226e+5,
        0.29059715e+5,
        -0.48157368e+4
      };
 
      const G4double coeff2[coeffTableSize] = {
        0.23135193e-1,
        -0.85604572e+0,
        0.56068193e+1,
        -0.69462922e+2,
        0.41631118e+3,
        -0.12546621e+4,
        0.12387830e+4,
        0.33739172e+4,
        -0.13041151e+5,
        0.19512524e+5,
        -0.15634324e+5,
        0.66231089e+4,
        -0.11698185e+4
      };
 
      const G4double normalisationR = std::sqrt(32. * Math::pi) * 0.28212;
 
      const G4double normalisationP = normalisationR / (std::sqrt(4. * Math::pi) * std::pow(PhysicalConstants::hc,1.5));
 
      const G4double al = 0.23162461;
 
    }
 
    G4double densityR(const G4double r) {
      const G4double sWave = wavefunctionR(0, r);
      const G4double dWave = wavefunctionR(2, r);
      return r*r*(sWave*sWave + dWave*dWave);
    }
 
    G4double derivDensityR(const G4double r) {
      const G4double sWave = wavefunctionR(0, r);
      const G4double dWave = wavefunctionR(2, r);
      const G4double sWaveDeriv = derivWavefunctionR(0, r);
      const G4double dWaveDeriv = derivWavefunctionR(2, r);
      return (sWave*sWaveDeriv + dWave*dWaveDeriv) / Math::twoPi;
    }
 
    G4double densityP(const G4double p) {
      const G4double sWave = wavefunctionP(0, p);
      const G4double dWave = wavefunctionP(2, p);
      return p*p*(sWave*sWave + dWave*dWave);
    }
 
    G4double wavefunctionR(const G4int l, const G4double theR) {
// assert(l==0 || l==2); // only s- and d-waves in a deuteron
      const G4double r = 2. * std::max(theR, 1.e-4);
 
      G4double result = 0.;
      G4double fmr;
 
      for(G4int i=0; i<coeffTableSize; ++i) {
        fmr = r * (al+i);
        if(l==0) { // s-wave
          result += coeff1[i] * std::exp(-fmr);
        } else { // d-wave
          result += coeff2[i] * std::exp(-fmr) * (1.+3./fmr+3./(fmr*fmr));
        }
      }
 
      result *= normalisationR/r;
      return result;
    }
 
    G4double derivWavefunctionR(const G4int l, const G4double theR) {
// assert(l==0 || l==2); // only s- and d-waves in a deuteron
      const G4double r = 2. * std::max(theR, 1.e-4);
 
      G4double result = 0.;
      G4double fmr;
 
      for(G4int i=0; i<coeffTableSize; ++i) {
        fmr = r * (al+i);
        if(l==0) { // s-wave
          result += coeff1[i] * std::exp(-fmr) * (fmr + 1.);
        } else { // d-wave
          result += coeff2[i] * std::exp(-fmr) * (fmr + 4. + 9./fmr + 9./(fmr*fmr));
        }
      }
 
      result *= -normalisationR/(r*r);
      return result;
    }
 
    G4double wavefunctionP(const G4int l, const G4double theQ) {
// assert(l==0 || l==2); // only s- and d-waves in a deuteron
      const G4double q = theQ / PhysicalConstants::hc;
      const G4double q2 = q*q;
      G4double result=0.;
      G4double fmq, alPlusI;
      for(G4int i=0; i<coeffTableSize; ++i) {
        alPlusI = al+i;
        fmq = q2 + alPlusI*alPlusI;
        if(l==0) { // s-wave
          result += coeff1[i] / fmq;
        } else { // d-wave
          result += coeff2[i] / fmq;
        }
      }
 
      result *= normalisationP;
      return result;
    }
 
  }
 
}