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geant4/source/geometry/magneticfield/include/G4Mag_SpinEqRhs.hh
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//
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// $Id: G4Mag_SpinEqRhs.hh,v 1.11 2006/06/29 18:23:09 gunter Exp $
// GEANT4 tag $Name: geant4-09-01 $
//
//
// class G4Mag_SpinEqRhs
//
// Class description:
//
// This is the equation of motion for a particle with spin in a pure
// magnetic field. The three components of the particle's spin are
// treated utilising BMT equation.
// History:
// - Created: J.Apostolakis, P.Gumplinger - February 8th, 1999.
// --------------------------------------------------------------------
#ifndef G4MAG_SPIN_EQRHS
#define G4MAG_SPIN_EQRHS
#include "G4Types.hh"
#include "G4Mag_EqRhs.hh"
class G4MagneticField;
class G4Mag_SpinEqRhs : public G4Mag_EqRhs
{
public: // with description
G4Mag_SpinEqRhs( G4MagneticField* MagField );
~G4Mag_SpinEqRhs();
// Constructor and destructor. No actions.
void SetChargeMomentumMass(G4double particleCharge, // in e+ units
G4double MomentumXc,
G4double mass);
void EvaluateRhsGivenB( const G4double y[],
const G4double B[3],
G4double dydx[] ) const;
// Given the value of the magnetic field B, this function
// calculates the value of the derivative dydx.
inline void SetAnomaly(G4double a) { anomaly = a; }
inline G4double GetAnomaly() const { return anomaly; }
// set/get magnetic anomaly
private:
G4double omegac;
G4double anomaly;
G4double ParticleCharge;
G4double E;
G4double gamma;
G4double beta;
};
#endif /* G4MAG_SPIN_EQRHS */