// // ******************************************************************** // * 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. * // ******************************************************************** // // G4EqEMFieldWithEDM // // Class description: // // This is the right-hand side of equation of motion in a combined // electric and magnetic field, with spin tracking for both MDM and // EDM terms. // Author: Kevin Lynch (Boston Univ.), 19.02.2009 - Based on G4EqEMFieldWithSpin // ------------------------------------------------------------------- #ifndef G4EQEMFIELDWITHEDM_HH #define G4EQEMFIELDWITHEDM_HH #include "G4ChargeState.hh" #include "G4EquationOfMotion.hh" class G4ElectroMagneticField; /** * @brief G4EqEMFieldWithEDM implements the right-hand side of equation of * motion in a combined electric and magnetic field, with spin tracking for * both MDM and EDM terms. */ class G4EqEMFieldWithEDM : public G4EquationOfMotion { public: /** * Constructor for G4EqEMFieldWithEDM. * @param[in] emField Pointer to the electromagnetic field. */ G4EqEMFieldWithEDM(G4ElectroMagneticField* emField); /** * Default Destructor. */ ~G4EqEMFieldWithEDM() 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 * electromagnetic 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 magnetic anomaly. */ inline void SetAnomaly(G4double a) { anomaly = a; } inline G4double GetAnomaly() const { return anomaly; } /** * Setter and getter for EDM eta parameter. */ inline void SetEta(G4double n) { eta = n; } inline G4double GetEta() const { return eta; } /** * Returns the equation type-ID, "kEqEMfieldWithEDM". */ inline G4EquationType GetEquationType() const override { return kEqEMfieldWithEDM; } private: G4double charge{0.}, mass{0.}, magMoment{0.}, spin{0.}; G4double fElectroMagCof{0.} ; G4double fMassCof{0.}; G4double omegac{0.}, anomaly{0.0011659208}, eta{0.}; G4double beta{0.}, gamma{0.}; }; #endif