G4Mag_SpinEqRhs.hh

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//
// 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.
 
// Created: J.Apostolakis, P.Gumplinger - 08.02.1999
// --------------------------------------------------------------------
#ifndef G4MAG_SPIN_EQRHS_HH
#define G4MAG_SPIN_EQRHS_HH
 
#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=0.0, mass=0.0, magMoment=0.0, spin=0.0;
     G4double omegac=0.0, anomaly=0.0011659208;
     G4double beta=0.0, gamma=0.0;
};
 
#endif