G4Mag_SpinEqRhs.hh

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// $Id: G4Mag_SpinEqRhs.hh 69699 2013-05-13 08:50:30Z gcosmo $
//
//
// 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"
#include "G4ChargeState.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(G4ChargeState particleCharge,
                                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 charge, mass, magMoment, spin;

     G4double omegac, anomaly;

     G4double beta, gamma;

};

#endif /* G4MAG_SPIN_EQRHS */