// // ******************************************************************** // * 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. * // ******************************************************************** // // 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. // Authors: John Apostolakis (CERN) & Peter Gumplinger (TRIUMF), 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; /** * @brief G4Mag_SpinEqRhs defines 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. */ class G4Mag_SpinEqRhs : public G4Mag_EqRhs { public: /** * Constructor for G4Mag_SpinEqRhs. * @param[in] MagField Pointer to the associated magnetic field. */ G4Mag_SpinEqRhs( G4MagneticField* MagField ); /** * Default Destructor. */ ~G4Mag_SpinEqRhs() override = default; /** * Sets the charge momentum mass value. */ void SetChargeMomentumMass(G4ChargeState particleCharge, G4double MomentumXc, G4double mass) override; /** * Calculates the value of the derivative, given the value of the field. * @param[in] y Coefficients array. * @param[in] B Field value. * @param[out] dydx Derivatives array. */ void EvaluateRhsGivenB( const G4double y[], const G4double B[3], G4double dydx[] ) const override; /** * Setter and getter for the magnetic anomaly. */ inline void SetAnomaly(G4double a) { anomaly = a; } inline G4double GetAnomaly() const { return anomaly; } /** * Returns the equation of motion type ID, i.e. "kEqMagneticWithSpin". */ inline G4EquationType GetEquationType() const override { return kEqMagneticWithSpin; } 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