// // ******************************************************************** // * 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. * // ******************************************************************** // // Geant4 Class file // // File name: G4PolarizedComptonXS // // Author: Andreas Schaelicke // // Class Description: // determine the polarization of the final state // in a Compton scattering process employing the differential // cross section by F.W.Lipps & H.A.Tolhoek // ( Physica 20 (1954) 395 ) #ifndef G4PolarizedComptonXS_h #define G4PolarizedComptonXS_h 1 #include "globals.hh" #include "G4StokesVector.hh" #include "G4VPolarizedXS.hh" class G4PolarizedComptonXS : public G4VPolarizedXS { public: G4PolarizedComptonXS(); ~G4PolarizedComptonXS() override; // prepares the ingredients for the calculation of a polarization // dependent differential cross section // the kinematics is fixed (X - incoming photon energy in units of electron // mass, eps - outgoing photon energy in unit of incoming photon energy, // and polarization of the incoming particles fixed (p0, p1) // a flag specifies the extent to which polarization is taken into account void Initialize(G4double eps, G4double X, G4double phi, const G4StokesVector& p0, const G4StokesVector& p1, G4int flag = 0) override; // returns the differential cross section for a given polarisation state // of the final state particles to be used in the calculation of the // polarization transfer the calculation has to be initialised by calling // Initialize() prior to the first call of this function (see above) G4double XSection(const G4StokesVector& pol2, const G4StokesVector& pol3) override; // total cross section G4double TotalXSection(G4double xmin, G4double xmax, G4double y, const G4StokesVector& pol0, const G4StokesVector& pol1) override; // return expected mean polarisation G4StokesVector GetPol2() override; G4StokesVector GetPol3() override; G4PolarizedComptonXS& operator=(const G4PolarizedComptonXS& right) = delete; G4PolarizedComptonXS(const G4PolarizedComptonXS&) = delete; private: void DefineCoefficients(const G4StokesVector& pol0, const G4StokesVector& pol1); static constexpr G4double re2 = CLHEP::classic_electr_radius * CLHEP::classic_electr_radius * (4. * CLHEP::pi / CLHEP::hbarc) * (4. * CLHEP::pi / CLHEP::hbarc); // these variables store the information necessary to evaluate the // differential cross section for arbitrary final state // polarizations (used in XSection): // - part depending on the polarization of the final photon G4ThreeVector fPhi2; // - part depending on the polarization of the final electron G4ThreeVector fPhi3; // - polarization independent part G4double fPhi0; // - product of polarizations of initial particles G4double polxx, polyy, polzz, polxz, polzx, polyz, polzy, polxy, polyx; // G4double diffXSFactor, totalXSFactor; G4double fPolXS, fUnpXS; }; #endif