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1 // ******************************************************************** 2 // * License and Disclaimer * 3 // * * 4 // * The Geant4 software is copyright of the Copyright Holders of * 5 // * the Geant4 Collaboration. It is provided under the terms and * 6 // * conditions of the Geant4 Software License, included in the file * 7 // * LICENSE and available at http://cern.ch/geant4/license . These * 8 // * include a list of copyright holders. * 9 // * * 10 // * Neither the authors of this software system, nor their employing * 11 // * institutes,nor the agencies providing financial support for this * 12 // * work make any representation or warranty, express or implied, * 13 // * regarding this software system or assume any liability for its * 14 // * use. Please see the license in the file LICENSE and URL above * 15 // * for the full disclaimer and the limitation of liability. * 16 // * * 17 // * This code implementation is the result of the scientific and * 18 // * technical work of the GEANT4 collaboration. * 19 // * By using, copying, modifying or distributing the software (or * 20 // * any work based on the software) you agree to acknowledge its * 21 // * use in resulting scientific publications, and indicate your * 22 // * acceptance of all terms of the Geant4 Software license. * 23 // ******************************************************************** 24 // 25 // 26 // ------------------------------------------------------------------- 27 // GEANT4 Class file 28 // 29 // File name: G4PolarizationTransition 30 // 31 // Author: Jason Detwiler (jasondet@gmail.com) 32 // 33 // Creation date: Aug 2012 34 // 35 // Description: 36 // Stores and manipulates the statistical tensor describing the nuclear 37 // polarization (see Alder and Winther, "Electromagnetic Excitation" (1975), 38 // Appendix F). Functions are implemented for generating angular correlations 39 // in gamma decays, following Alder and Winther, Appendix G. 40 // This code assumes no polarization will be detected and uses eqs (17-20). 41 // Adding polarization would require using instead (13) and the more generic 42 // form of the statstical tensor after decay described by equation (6) 43 // Could be expanded to also generate e.g. gamma-beta and other 44 // correlations as well. 45 // 46 // ------------------------------------------------------------------- 47 48 #ifndef G4POLARIZATIONTRANSITION_HH 49 #define G4POLARIZATIONTRANSITION_HH 50 51 #include "globals.hh" 52 #include "G4LegendrePolynomial.hh" 53 #include "G4PolynomialPDF.hh" 54 #include "G4Pow.hh" 55 56 class G4NuclearPolarization; 57 58 class G4PolarizationTransition 59 { 60 typedef std::vector< std::vector<G4complex> > POLAR; 61 62 public: 63 G4PolarizationTransition(); 64 ~G4PolarizationTransition() = default; 65 66 void SampleGammaTransition(G4NuclearPolarization* np, 67 G4int twoJ1, G4int twoJ2, 68 G4int L0, G4int Lp, G4double mpRatio, 69 G4double& cosTheta, G4double& phi); 70 71 // generic static functions 72 G4double FCoefficient(G4int K, G4int L, G4int Lprime, 73 G4int twoJ2, G4int twoJ1) const; 74 G4double F3Coefficient(G4int K, G4int K2, G4int K1, G4int L, 75 G4int Lprime, G4int twoJ2, G4int twoJ1) const; 76 77 // transition-specific functions 78 G4double GammaTransFCoefficient(G4int K) const; 79 G4double GammaTransF3Coefficient(G4int K, G4int K2, G4int K1) const; 80 81 void DumpTransitionData(const POLAR& pol) const; 82 83 inline void SetVerbose(G4int val) { fVerbose = val; }; 84 85 private: 86 87 G4PolarizationTransition(const G4PolarizationTransition &right) = delete; 88 const G4PolarizationTransition& operator=(const G4PolarizationTransition &right) = delete; 89 90 // Gamma angle generation and decay: call these functions in this order! 91 // All angles are in the same coordinate system: user may choose any axis 92 G4double GenerateGammaCosTheta(const POLAR&); 93 G4double GenerateGammaPhi(G4double& cosTheta, const POLAR&); 94 95 inline G4double LnFactorial(int k) const { return G4Pow::GetInstance()->logfactorial(k); } 96 97 G4int fVerbose; 98 G4int fTwoJ1, fTwoJ2; 99 G4int fLbar, fL; 100 G4double fDelta; 101 G4double kEps; 102 G4PolynomialPDF kPolyPDF; 103 G4LegendrePolynomial fgLegendrePolys; 104 }; 105 106 107 #endif 108