Geant4-11
G4KM_NucleonEqRhs.cc
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27// -------------------------------------------------------------------
28// GEANT 4 class implementation file
29//
30// CERN, Geneva, Switzerland
31//
32// File name: G4KM_NucleonEqRhs.cc
33//
34// Author: Alessandro Brunengo (Alessandro.Brunengo@ge.infn.it)
35//
36// Creation date: 5 June 2000
37// -------------------------------------------------------------------
38
39#include "G4KM_NucleonEqRhs.hh"
40#include "G4VNuclearDensity.hh"
41
43#include "G4Pow.hh"
44
46 G4V3DNucleus * nucleus) :
47 G4Mag_EqRhs(field), theNucleus(nucleus)
48{
49 theMass = 0.;
52}
53
54
56 const G4double *,
57 G4double dydx[]) const
58{
59 G4double yMod = std::sqrt(y[0]*y[0]+y[1]*y[1]+y[2]*y[2]);
60 G4double e = std::sqrt(theMass*theMass+y[3]*y[3]+y[4]*y[4]+y[5]*y[5]);
61
62// y[0..2] is position
63// y[3..5] is momentum (and not mom.direction)
64
65 dydx[0] = c_light*y[3]/e; //
66 dydx[1] = c_light*y[4]/e; // dq/dt=dH/dp = c*p/e
67 dydx[2] = c_light*y[5]/e; //
68
69/*
70 * // debug
71 * G4cout << " Nucleon RHS : 0..2(dpos/dt) " <<
72 * dydx[0] << " " <<
73 * dydx[1] << " " <<
74 * dydx[2] << " " << G4endl;
75 */
76
77
78// V=K*rho(r) ==> dydx[3] = -dV/dr*dr/dx = -K*d(rho)/dr*dr/dx.
79// GF should be V=K*rho(r) ==> dydx[3] = -dV/dr*dr/dx = -K*d(rho)/dr*dr/dt
80// GF and dV/dt = dE/dt ==> dp/dt = dE/dt * dp/dE = dE/dt *e/p
81// Idem for dydx[4] and dydx[5]
82
83 G4ThreeVector pos(y[0],y[1],y[2]);
84
85 const G4VNuclearDensity * nuclearDensity=theNucleus->GetNuclearDensity();
86
87// do not check for theMass != 0 : it is an error and core dump will signal it
88
89 G4double density= nuclearDensity->GetDensity(pos);
90 G4double deriv(0);
91 if (density > 0 ) deriv = (factor/theMass)/
92 G4Pow::GetInstance()->A13(density)*nuclearDensity->GetDeriv(pos);
93
94// dydx[3] = yMod == 0 ? 0 : -deriv*y[0]/yMod;
95// dydx[4] = yMod == 0 ? 0 : -deriv*y[1]/yMod;
96// dydx[5] = yMod == 0 ? 0 : -deriv*y[2]/yMod;
97 dydx[3] = yMod == 0 ? 0 : deriv*y[0]/yMod*c_light;
98 dydx[4] = yMod == 0 ? 0 : deriv*y[1]/yMod*c_light;
99 dydx[5] = yMod == 0 ? 0 : deriv*y[2]/yMod*c_light;
100
101
102/*
103 * // debug
104 * G4cout << " Nucleon RHS : 3..5(dE/dt) " <<
105 * dydx[3] << " " <<
106 * dydx[4] << " " <<
107 * dydx[5] << " " << G4endl;
108 */
109}
110
111// Here by design, but it is unnecessary for nuclear fields
113{
114}
static const G4double pos
static constexpr double pi2
Definition: G4SIunits.hh:58
double G4double
Definition: G4Types.hh:83
virtual void EvaluateRhsGivenB(const G4double y[], const G4double B[3], G4double dydx[]) const
G4V3DNucleus * theNucleus
virtual void SetChargeMomentumMass(G4ChargeState particleCharge, G4double MomentumXc, G4double MassXc2)
G4KM_NucleonEqRhs(G4KM_DummyField *field, G4V3DNucleus *nucleus)
static G4Pow * GetInstance()
Definition: G4Pow.cc:41
G4double A13(G4double A) const
Definition: G4Pow.cc:120
G4double A23(G4double A) const
Definition: G4Pow.hh:131
virtual const G4VNuclearDensity * GetNuclearDensity() const =0
virtual G4int GetMassNumber()=0
G4double GetDensity(const G4ThreeVector &aPosition) const
virtual G4double GetDeriv(const G4ThreeVector &point) const =0
float c_light
Definition: hepunit.py:256
float hbarc
Definition: hepunit.py:264