// // ******************************************************************** // * 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. * // ******************************************************************** // // // Author: Mathieu Karamitros // The code is developed in the framework of the ESA AO7146 // // We would be very happy hearing from you, send us your feedback! :) // // In order for Geant4-DNA to be maintained and still open-source, // article citations are crucial. // If you use Geant4-DNA chemistry and you publish papers about your software, // in addition to the general paper on Geant4-DNA: // // Int. J. Model. Simul. Sci. Comput. 1 (2010) 157–178 // // we would be very happy if you could please also cite the following // reference papers on chemistry: // // J. Comput. Phys. 274 (2014) 841-882 // Prog. Nucl. Sci. Tec. 2 (2011) 503-508 #ifndef G4DNAOneStepThermalizationModel_hh #define G4DNAOneStepThermalizationModel_hh #include #include "G4VEmModel.hh" class G4ITNavigator; class G4Navigator; namespace DNA{ namespace Penetration{ //----------------------- /* * Article: Jintana Meesungnoen, Jean-Paul Jay-Gerin, * Abdelali Filali-Mouhim, and Samlee Mankhetkorn (2002) * Low-Energy Electron Penetration Range in Liquid Water. * Radiation Research: November 2002, Vol. 158, No. 5, pp.657-660. */ struct Meesungnoen2002{ static void GetPenetration(G4double energy, G4ThreeVector& displacement); static double GetRmean(double energy); //----- // Polynomial fit of Meesungnoen, 2002 static const double gCoeff[13]; }; struct Meesungnoen2002_amorphous{ static void GetPenetration(G4double energy, G4ThreeVector& displacement); static double GetRmean(double energy); //----- // Polynomial fit of Meesungnoen, 2002 static const double gCoeff[7]; }; //----------------------- /* * Article: Kreipl M S, Friedland W, Paretzke H G (2009) Time- and * space-resolved Monte Carlo study of water radiolysis * for photon, electron and ion irradiation. * Radiat Environ Biophys 48:11-20 */ struct Kreipl2009{ static void GetPenetration(G4double energy, G4ThreeVector& displacement); }; //----------------------- /* * Article: Terrissol M, Beaudre A (1990) Simulation of space and time * evolution of radiolytic species induced by electrons in water. * Radiat Prot Dosimetry 31:171–175 */ struct Terrisol1990{ static void GetPenetration(G4double energy, G4ThreeVector& displacement); static double GetRmean(double energy); static double Get3DStdDeviation(double energy); //----- // Terrisol, 1990 static const double gEnergies_T1990[11]; static const double gStdDev_T1990[11]; }; //----------------------- /* * Article: Ritchie RH, Hamm RN, Turner JE, Bolch WE (1994) Interaction of * low-energy electrons with condensed matter: relevance for track * structure. * Computational approaches in molecular radiation biology, Plenum, * New York, Vol. 63, pp. 155–166 * Note: also used in Ballarini et al., 2000 */ struct Ritchie1994{ static void GetPenetration(G4double energy, G4ThreeVector& displacement); static double GetRmean(double energy); }; } } /** * When an electron reaches the highest energy domain of * G4DNAOneStepThermalizationModel, * it is then automatically converted into a solvated electron and displace * from its original position using a published thermalization statistic. */ template class G4TDNAOneStepThermalizationModel : public G4VEmModel { public: using Model = MODEL; G4TDNAOneStepThermalizationModel(const G4ParticleDefinition* p = nullptr, const G4String& nam = "DNAOneStepThermalizationModel"); ~G4TDNAOneStepThermalizationModel() override; void Initialise(const G4ParticleDefinition*, const G4DataVector&) override; G4double CrossSectionPerVolume(const G4Material* material, const G4ParticleDefinition* p, G4double ekin, G4double emin, G4double emax) override; void SampleSecondaries(std::vector*, const G4MaterialCutsCouple*, const G4DynamicParticle*, G4double tmin, G4double maxEnergy) override; inline void SetVerbose(int flag){ fVerboseLevel = flag; } void GetPenetration(G4double energy, G4ThreeVector& displacement); double GetRmean(double energy); protected: const std::vector* fpWaterDensity; G4ParticleChangeForGamma* fpParticleChangeForGamma; G4bool fIsInitialised{false}; G4int fVerboseLevel; std::unique_ptr fpNavigator; private: G4TDNAOneStepThermalizationModel& operator=(const G4TDNAOneStepThermalizationModel &right); G4TDNAOneStepThermalizationModel(const G4TDNAOneStepThermalizationModel&); }; #include "G4DNAOneStepThermalizationModel.hpp" using G4DNAOneStepThermalizationModel = G4TDNAOneStepThermalizationModel; // typedef G4TDNAOneStepThermalizationModel G4DNAOneStepThermalizationModel; // Note: if you use the above distribution, it would be // better to follow the electrons down to 6 eV and only then apply // the one step thermalization class G4DNASolvationModelFactory { public: /// @param penetrationType Available options: /// Meesungnoen2002, Terrisol1990, Ritchie1994 static G4VEmModel* Create(const G4String& penetrationModel); /// \brief One step thermalization model can be chosen via macro using /// /process/dna/e-SolvationSubType Ritchie1994 /// \return Create the model defined via the command macro /// /process/dna/e-SolvationSubType /// In case the command is unused, it returns the default model set in /// G4EmParameters. static G4VEmModel* GetMacroDefinedModel(); }; #endif