// // ******************************************************************** // * 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. * // ******************************************************************** // // G4RepleteEofM // // Class description: // // This is the right-hand side of equation of motion in a combined // field, including: magnetic, electric, gravity, and gradient B field, // as well as spin tracking. // Author: Peter Gumplinger (TRIUMF), 08.04.2013 // ------------------------------------------------------------------- #ifndef G4EOFM_HH #define G4EOFM_HH #include "G4ChargeState.hh" #include "G4EquationOfMotion.hh" class G4Field; /** * @brief G4RepleteEofM is the right-hand side of equation of motion in a * combined field, including: magnetic, electric, gravity, and gradient * B field, as well as spin tracking. */ class G4RepleteEofM : public G4EquationOfMotion { public: /** * Constructor for G4EquationOfMotion. * @param[in] field Pointer to the field. * @param[in] nvar The number of integration variables. */ G4RepleteEofM(G4Field* field, G4int nvar = 8); /** * Default Destructor. */ ~G4RepleteEofM() override = default; /** * Sets the charge, momentum and mass of the current particle. * Used to set the equation's coefficients. * @param[in] particleCharge Magnetic charge and moments in e+ units. * @param[in] MomentumXc Particle momentum. * @param[in] mass Particle mass. */ void SetChargeMomentumMass(G4ChargeState particleCharge, // in e+ units G4double MomentumXc, G4double mass) override; /** * Calculates the value of the derivative, given the value of the field. * @param[in] y Coefficients array. * @param[in] Field Field value. * @param[out] dydx Derivatives array. */ void EvaluateRhsGivenB(const G4double y[], const G4double Field[], G4double dydx[] ) const override; /** * Setter and getter for the magnetic anomaly. */ inline void SetAnomaly(G4double a) { anomaly = a; } inline G4double GetAnomaly() const { return anomaly; } /** * Modifiers. */ inline void SetBField() { fBfield = true; } inline void SetEField() { fEfield = true; } inline void SetgradB() { fgradB = true; } inline void SetSpin() { fSpin = true; } private: G4int fNvar = 0; G4bool fBfield=false, fEfield=false, fGfield=false, fgradB=false, fSpin=false; G4double charge=0.0, mass=0.0, magMoment=0.0, spin=0.0; G4double ElectroMagCof=0.0; G4double omegac=0.0, anomaly=0.0; G4double beta=0.0, gamma=0.0; }; #endif