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25 //
26 // G4EqEMFieldWithSpin implementation
27 //
28 // Created: Chris Gong & Peter Gumplinger, 30.
29 // -------------------------------------------
30
31 #include "G4EqEMFieldWithSpin.hh"
32 #include "G4ElectroMagneticField.hh"
33 #include "G4ThreeVector.hh"
34 #include "globals.hh"
35 #include "G4PhysicalConstants.hh"
36 #include "G4SystemOfUnits.hh"
37
38 G4EqEMFieldWithSpin::G4EqEMFieldWithSpin(G4Ele
39 : G4EquationOfMotion( emField )
40 {
41 }
42
43 G4EqEMFieldWithSpin::~G4EqEMFieldWithSpin() =
44
45 void
46 G4EqEMFieldWithSpin::SetChargeMomentumMass(G4C
47 G4d
48 G4d
49 {
50 charge = particleCharge.GetCharge();
51 mass = particleMass;
52 magMoment = particleCharge.GetMagneticDipol
53 spin = particleCharge.GetSpin();
54
55 fElectroMagCof = eplus*charge*c_light ;
56 fMassCof = mass*mass;
57
58 omegac = (eplus/mass)*c_light;
59
60 G4double muB = 0.5*eplus*hbar_Planck/(mass/
61
62 G4double g_BMT;
63 if ( spin != 0. )
64 {
65 g_BMT = (std::abs(magMoment)/muB)/spin;
66 }
67 else
68 {
69 g_BMT = 2.;
70 }
71
72 anomaly = (g_BMT - 2.)/2.;
73
74 G4double E = std::sqrt(sqr(MomentumXc)+sqr(
75 beta = MomentumXc/E;
76 gamma = E/mass;
77 }
78
79 void
80 G4EqEMFieldWithSpin::EvaluateRhsGivenB(const G
81 const G
82 G
83 {
84
85 // Components of y:
86 // 0-2 dr/ds,
87 // 3-5 dp/ds - momentum derivatives
88 // 9-11 dSpin/ds = (1/beta) dSpin/dt - s
89
90 // The BMT equation, following J.D.Jackson,
91 // Electrodynamics, Second Edition,
92 // dS/dt = (e/mc) S \cross
93 // [ (g/2-1 +1/\gamma) B
94 // -(g/2-1)\gamma/(\gamma+1)
95 // -(g/2-\gamma/(\gamma+1) \b
96 // where
97 // S = \vec{s}, where S^2 = 1
98 // B = \vec{B}
99 // \beta = \vec{\beta} = \beta \vec{u} with
100 // E = \vec{E}
101
102 G4double pSquared = y[3]*y[3] + y[4]*y[4] +
103
104 G4double Energy = std::sqrt( pSquared + f
105 G4double cof2 = Energy/c_light ;
106
107 G4double pModuleInverse = 1.0/std::sqrt(pS
108
109 G4double inverse_velocity = Energy * pModul
110
111 G4double cof1 = fElectroMagCof*pModuleInver
112
113 dydx[0] = y[3]*pModuleInverse ;
114 dydx[1] = y[4]*pModuleInverse ;
115 dydx[2] = y[5]*pModuleInverse ;
116
117 dydx[3] = cof1*(cof2*Field[3] + (y[4]*Field
118
119 dydx[4] = cof1*(cof2*Field[4] + (y[5]*Field
120
121 dydx[5] = cof1*(cof2*Field[5] + (y[3]*Field
122
123 dydx[6] = dydx[8] = 0.;//not used
124
125 // Lab Time of flight
126 dydx[7] = inverse_velocity;
127
128 G4ThreeVector BField(Field[0],Field[1],Fiel
129 G4ThreeVector EField(Field[3],Field[4],Fiel
130
131 EField /= c_light;
132
133 G4ThreeVector u(y[3], y[4], y[5]);
134 u *= pModuleInverse;
135
136 G4double udb = anomaly*beta*gamma/(1.+gamma
137 G4double ucb = (anomaly+1./gamma)/beta;
138 G4double uce = anomaly + 1./(gamma+1.);
139
140 G4ThreeVector Spin(y[9],y[10],y[11]);
141
142 G4double pcharge;
143 if (charge == 0.)
144 {
145 pcharge = 1.;
146 }
147 else
148 {
149 pcharge = charge;
150 }
151
152 G4ThreeVector dSpin(0.,0.,0.);
153 if (Spin.mag2() != 0.)
154 {
155 dSpin = pcharge*omegac*( ucb*(Spin.cross
156 // from Jackson
157 // -uce*Spin.cross(
158 // but this form ha
159 - uce*(u*(Spin*EField) -
160 }
161
162 dydx[ 9] = dSpin.x();
163 dydx[10] = dSpin.y();
164 dydx[11] = dSpin.z();
165
166 return;
167 }
168