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geant4/source/processes/hadronic/models/binary_cascade/src/G4KM_OpticalEqRhs.cc
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// -------------------------------------------------------------------
// GEANT 4 class implementation file
//
// CERN, Geneva, Switzerland
//
// File name: G4KM_OpticalEqRhs.cc
//
// Author: Alessandro Brunengo (Alessandro.Brunengo@ge.infn.it)
//
// Creation date: 5 June 2000
// -------------------------------------------------------------------
#include "G4KM_OpticalEqRhs.hh"
#include "G4PhysicalConstants.hh"
#include "G4NucleiProperties.hh"
#include "G4VNuclearDensity.hh"
#include "G4HadTmpUtil.hh"
G4KM_OpticalEqRhs::G4KM_OpticalEqRhs(G4KM_DummyField *field,
G4V3DNucleus * nucleus) :
G4Mag_EqRhs(field), theNucleus(nucleus)
{
theFactor = 0;
theMass = 0;
}
void G4KM_OpticalEqRhs::SetFactor(G4double mass, G4double opticalParameter)
{
G4double A = theNucleus->GetMassNumber();
G4double Z = theNucleus->GetCharge();
G4double bindingEnergy = G4NucleiProperties::GetBindingEnergy(G4lrint(A), G4lrint(Z));
G4double nucleusMass = Z*proton_mass_c2+(A-Z)*neutron_mass_c2+bindingEnergy;
G4double reducedMass = mass*nucleusMass/(mass+nucleusMass);
G4double nucleonMass = (proton_mass_c2+neutron_mass_c2)/2;
// _factor in (MeV*fermi)*fermi/MeV = fermi*fermi -- need to have A as density normalized to 1
theFactor = 2*pi*hbarc*hbarc*(1+mass/nucleonMass)* opticalParameter/reducedMass * A;
theMass = mass;
}
void G4KM_OpticalEqRhs::EvaluateRhsGivenB(const G4double y[], const G4double *,
G4double dydx[]) const
{
G4double yMod = std::sqrt(y[0]*y[0]+y[1]*y[1]+y[2]*y[2]);
G4double e = std::sqrt(theMass*theMass+y[3]*y[3]+y[4]*y[4]+y[5]*y[5]);
dydx[0] = c_light*y[3]/e; //
dydx[1] = c_light*y[4]/e; // dq/dt=dH/dp = c*p/e
dydx[2] = c_light*y[5]/e; //
// V=K*rho(r) ==> dydx[3] = -dV/dr*dr/dx = -K*d(rho)/dr*dr/dx.
// Idem for dydx[4] and dydx[5]
const G4VNuclearDensity * nuclearDensity=theNucleus->GetNuclearDensity();
G4ThreeVector pos(y[0],y[1],y[2]);
G4double deriv = theFactor*nuclearDensity->GetDeriv(pos);
dydx[3] = yMod == 0 ? 0 : -deriv*y[0]/yMod*c_light;
dydx[4] = yMod == 0 ? 0 : -deriv*y[1]/yMod*c_light;
dydx[5] = yMod == 0 ? 0 : -deriv*y[2]/yMod*c_light;
}
// Here by design, but it is unnecessary for nuclear fields
void G4KM_OpticalEqRhs::SetChargeMomentumMass(G4ChargeState,G4double ,G4double )
{
}