// // ******************************************************************** // * 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. * // ******************************************************************** // // G4ScreeningMottCrossSection.hh //------------------------------------------------------------------- // // GEANT4 Class header file // // File name: G4ScreeningMottCrossSection // // Author: Cristina Consolandi // // Creation date: 20.10.2011 // // Modifications: // 27-05-2012 Added Analytic Fitting to the Mott Cross Section by means of G4MottCoefficients class. // // // Class Description: // Computation of electron Coulomb Scattering Cross Section. // Suitable for high energy electrons and light target materials. // // Reference: // M.J. Boschini et al. // "Non Ionizing Energy Loss induced by Electrons in the Space Environment" // Proc. of the 13th International Conference on Particle Physics and Advanced Technology // (13th ICPPAT, Como 3-7/10/2011), World Scientific (Singapore). // Available at: http://arxiv.org/abs/1111.4042v4 // // 1) Mott Differential Cross Section Approximation: // For Target material up to Z=92 (U): // As described in http://arxiv.org/abs/1111.4042v4 // par. 2.1 , eq. (16)-(17) // Else (Z>92): // W. A. McKinley and H. Fashbach, Phys. Rev. 74, (1948) 1759. // 2) Screening coefficient: // vomn G. Moliere, Z. Naturforsh A2 (1947), 133-145; A3 (1948), 78. // 3) Nuclear Form Factor: // A.V. Butkevich et al. Nucl. Instr. and Meth. in Phys. Res. A 488 (2002), 282-294. // // ---------------------------------------------------------------------------------------- // #ifndef G4ScreeningMottCrossSection_h #define G4ScreeningMottCrossSection_h 1 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo...... #include "G4MottCoefficients.hh" #include "globals.hh" #include "G4Material.hh" #include "G4Element.hh" #include "G4ElementVector.hh" #include "G4NistManager.hh" #include "G4ThreeVector.hh" #include "G4Pow.hh" #include "G4LossTableManager.hh" class G4ParticleDefinition; //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo...... class G4ScreeningMottCrossSection { public: G4ScreeningMottCrossSection(); virtual ~G4ScreeningMottCrossSection(); void Initialise(const G4ParticleDefinition*, G4double cosThetaLim); G4double GetScreeningAngle(); void SetScreeningCoefficient(); inline void SetupParticle(const G4ParticleDefinition*); void SetupKinematic(G4double kinEnergy ,G4double Z); G4double NuclearCrossSection(); G4ThreeVector GetNewDirection(); inline G4double GetMom2CM()const; inline G4double GetMom2Lab()const; inline G4double GetTrec() const; inline G4double GetScreeningCoefficient() const; inline G4double GetTotalCross() const; G4double McFcorrection(G4double); G4double RatioMottRutherford(G4double);//.....new G4double FormFactor2ExpHof(G4double); G4double GetScatteringAngle(); G4double AngleDistribution(G4double); private: G4ScreeningMottCrossSection & operator=(const G4ScreeningMottCrossSection &right); G4ScreeningMottCrossSection(const G4ScreeningMottCrossSection&); G4NistManager* fNistManager; G4MottCoefficients * mottcoeff; G4double TotalCross; //cost - min - max G4double cosThetaMin;// def 1.0 G4double cosThetaMax;// def -1.0 G4double cosTetMinNuc; G4double cosTetMaxNuc; //energy cut G4double ecut; G4double etag; // projectile........................ const G4ParticleDefinition* particle; G4double spin; G4double mass; //lab of incedent particle G4double tkinLab; G4double momLab2; G4double invbetaLab2; //relative system with nucleus G4double mu_rel; G4double tkin; G4double mom2; G4double invbeta2; G4double beta; G4double gamma; // target nucleus G4double targetZ; G4double targetA; G4double targetMass; G4double Trec; G4double As; G4double coeffb[5][6]; //constants G4double alpha; G4double htc2; G4double e2; }; //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... inline void G4ScreeningMottCrossSection::SetupParticle(const G4ParticleDefinition* p) { particle = p; mass = particle->GetPDGMass(); spin = particle->GetPDGSpin(); if(0.0 != spin) { spin = 0.5; } tkin = 0.0; } //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... inline G4double G4ScreeningMottCrossSection::GetMom2CM() const { return mom2; } //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... inline G4double G4ScreeningMottCrossSection::GetMom2Lab() const { return momLab2; } //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... inline G4double G4ScreeningMottCrossSection::GetTrec() const { return Trec; } //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... inline G4double G4ScreeningMottCrossSection::GetScreeningCoefficient() const { return As; } //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... inline G4double G4ScreeningMottCrossSection::GetTotalCross() const { return TotalCross; } //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... #endif