Import Geant4 9.1.0 source tree

This commit is contained in:
Gabriele Cosmo
2016-06-09 15:37:50 +02:00
parent a8e9364cea
commit 96c8bcd0af
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//
// ********************************************************************
// * License and Disclaimer *
// * *
// * The Geant4 software is copyright of the Copyright Holders of *
// * the Geant4 Collaboration. It is provided under the terms and *
// * conditions of the Geant4 Software License, included in the file *
// * LICENSE and available at http://cern.ch/geant4/license . These *
// * include a list of copyright holders. *
// * *
// * Neither the authors of this software system, nor their employing *
// * institutes,nor the agencies providing financial support for this *
// * work make any representation or warranty, express or implied, *
// * regarding this software system or assume any liability for its *
// * use. Please see the license in the file LICENSE and URL above *
// * for the full disclaimer and the limitation of liability. *
// * *
// * This code implementation is the result of the scientific and *
// * technical work of the GEANT4 collaboration. *
// * By using, copying, modifying or distributing the software (or *
// * any work based on the software) you agree to acknowledge its *
// * use in resulting scientific publications, and indicate your *
// * acceptance of all terms of the Geant4 Software license. *
// ********************************************************************
//
//
// $Id: G4EqEMFieldWithSpin.cc,v 1.1 2007/08/30 23:34:19 gum Exp $
// GEANT4 tag $Name: geant4-09-01 $
//
//
// This is the standard right-hand side for equation of motion.
//
// The only case another is required is when using a moving reference
// frame ... or extending the class to include additional Forces,
// eg an electric field
//
// 30.08.2007 Chris Gong, Peter Gumplinger
//
// -------------------------------------------------------------------
#include "G4EqEMFieldWithSpin.hh"
#include "G4ThreeVector.hh"
#include "globals.hh"
G4EqEMFieldWithSpin::G4EqEMFieldWithSpin(G4ElectroMagneticField *emField )
: G4EquationOfMotion( emField ) { anomaly = 1.165923e-3; }
void
G4EqEMFieldWithSpin::SetChargeMomentumMass(G4double particleCharge, // e+ units
G4double MomentumXc,
G4double particleMass)
{
fElectroMagCof = eplus*particleCharge*c_light ;
fMassCof = particleMass*particleMass ;
omegac = 0.105658387*GeV/particleMass * 2.837374841e-3*(rad/cm/kilogauss);
ParticleCharge = particleCharge;
E = std::sqrt(sqr(MomentumXc)+sqr(particleMass));
beta = MomentumXc/E;
gamma = E/particleMass;
}
void
G4EqEMFieldWithSpin::EvaluateRhsGivenB(const G4double y[],
const G4double Field[],
G4double dydx[] ) const
{
// Components of y:
// 0-2 dr/ds,
// 3-5 dp/ds - momentum derivatives
G4double pSquared = y[3]*y[3] + y[4]*y[4] + y[5]*y[5] ;
G4double Energy = std::sqrt( pSquared + fMassCof );
G4double cof2 = Energy/c_light ;
G4double pModuleInverse = 1.0/std::sqrt(pSquared) ;
// G4double inverse_velocity = Energy * c_light * pModuleInverse;
G4double inverse_velocity = Energy * pModuleInverse / c_light;
G4double cof1 = fElectroMagCof*pModuleInverse ;
// G4double vDotE = y[3]*Field[3] + y[4]*Field[4] + y[5]*Field[5] ;
dydx[0] = y[3]*pModuleInverse ;
dydx[1] = y[4]*pModuleInverse ;
dydx[2] = y[5]*pModuleInverse ;
dydx[3] = cof1*(cof2*Field[3] + (y[4]*Field[2] - y[5]*Field[1])) ;
dydx[4] = cof1*(cof2*Field[4] + (y[5]*Field[0] - y[3]*Field[2])) ;
dydx[5] = cof1*(cof2*Field[5] + (y[3]*Field[1] - y[4]*Field[0])) ;
// Lab Time of flight
dydx[7] = inverse_velocity;
G4ThreeVector BField(Field[0],Field[1],Field[2]);
G4ThreeVector u(y[3], y[4], y[5]);
u *= pModuleInverse;
G4double udb = anomaly*beta*gamma/(1.+gamma) * (BField * u);
G4double ucb = (anomaly+1./gamma)/beta;
G4ThreeVector Spin(y[9],y[10],y[11]);
G4ThreeVector dSpin;
dSpin = ParticleCharge*omegac*(ucb*(Spin.cross(BField))-udb*(Spin.cross(u)));
dydx[ 9] = dSpin.x();
dydx[10] = dSpin.y();
dydx[11] = dSpin.z();
return ;
}