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File indexing completed on 2026-09-18 09:14:01
0001 // 0002 // ******************************************************************** 0003 // * License and Disclaimer * 0004 // * * 0005 // * The Geant4 software is copyright of the Copyright Holders of * 0006 // * the Geant4 Collaboration. It is provided under the terms and * 0007 // * conditions of the Geant4 Software License, included in the file * 0008 // * LICENSE and available at http://cern.ch/geant4/license . These * 0009 // * include a list of copyright holders. * 0010 // * * 0011 // * Neither the authors of this software system, nor their employing * 0012 // * institutes,nor the agencies providing financial support for this * 0013 // * work make any representation or warranty, express or implied, * 0014 // * regarding this software system or assume any liability for its * 0015 // * use. Please see the license in the file LICENSE and URL above * 0016 // * for the full disclaimer and the limitation of liability. * 0017 // * * 0018 // * This code implementation is the result of the scientific and * 0019 // * technical work of the GEANT4 collaboration. * 0020 // * By using, copying, modifying or distributing the software (or * 0021 // * any work based on the software) you agree to acknowledge its * 0022 // * use in resulting scientific publications, and indicate your * 0023 // * acceptance of all terms of the Geant4 Software license. * 0024 // ******************************************************************** 0025 // 0026 // G4Mag_SpinEqRhs 0027 // 0028 // Class description: 0029 // 0030 // This is the equation of motion for a particle with spin in a pure 0031 // magnetic field. The three components of the particle's spin are 0032 // treated utilising BMT equation. 0033 0034 // Authors: John Apostolakis (CERN) & Peter Gumplinger (TRIUMF), 08.02.1999 0035 // -------------------------------------------------------------------- 0036 #ifndef G4MAG_SPIN_EQRHS_HH 0037 #define G4MAG_SPIN_EQRHS_HH 0038 0039 #include "G4Types.hh" 0040 #include "G4Mag_EqRhs.hh" 0041 #include "G4ChargeState.hh" 0042 0043 class G4MagneticField; 0044 0045 /** 0046 * @brief G4Mag_SpinEqRhs defines the equation of motion for a particle with 0047 * spin in a pure magnetic field. The three components of the particle's spin 0048 * are treated utilising BMT equation. 0049 */ 0050 0051 class G4Mag_SpinEqRhs : public G4Mag_EqRhs 0052 { 0053 public: 0054 0055 /** 0056 * Constructor for G4Mag_SpinEqRhs. 0057 * @param[in] MagField Pointer to the associated magnetic field. 0058 */ 0059 G4Mag_SpinEqRhs( G4MagneticField* MagField ); 0060 0061 /** 0062 * Default Destructor. 0063 */ 0064 ~G4Mag_SpinEqRhs() override = default; 0065 0066 /** 0067 * Sets the charge momentum mass value. 0068 */ 0069 void SetChargeMomentumMass(G4ChargeState particleCharge, 0070 G4double MomentumXc, 0071 G4double mass) override; 0072 0073 /** 0074 * Calculates the value of the derivative, given the value of the field. 0075 * @param[in] y Coefficients array. 0076 * @param[in] B Field value. 0077 * @param[out] dydx Derivatives array. 0078 */ 0079 void EvaluateRhsGivenB( const G4double y[], 0080 const G4double B[3], 0081 G4double dydx[] ) const override; 0082 0083 /** 0084 * Setter and getter for the magnetic anomaly. 0085 */ 0086 inline void SetAnomaly(G4double a) { anomaly = a; } 0087 inline G4double GetAnomaly() const { return anomaly; } 0088 0089 /** 0090 * Returns the equation of motion type ID, i.e. "kEqMagneticWithSpin". 0091 */ 0092 inline G4EquationType GetEquationType() const override { return kEqMagneticWithSpin; } 0093 0094 private: 0095 0096 G4double charge=0.0, mass=0.0, magMoment=0.0, spin=0.0; 0097 G4double omegac=0.0, anomaly=0.0011659208; 0098 G4double beta=0.0, gamma=0.0; 0099 }; 0100 0101 #endif
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