// // ******************************************************************** // * 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. * // ******************************************************************** // /// \file G4ScreenedNuclearRecoil.hh /// \brief Definition of the G4ScreenedNuclearRecoil class // G4ScreenedNuclearRecoil.hh,v 1.24 2008/05/01 19:58:59 marcus Exp // GEANT4 tag // // // // Class Description // Process for screened electromagnetic nuclear elastic scattering; // Physics comes from: // Marcus H. Mendenhall and Robert A. Weller, // "Algorithms for the rapid computation of classical cross sections // for screened Coulomb collisions " // Nuclear Instruments and Methods in Physics Research B58 (1991) 11-17 // The only input required is a screening function phi(r/a) which is the ratio // of the actual interatomic potential for two atoms with atomic numbers Z1 and // Z2, // to the unscreened potential Z1*Z2*e^2/r where e^2 is elm_coupling in Geant4 // units // the actual screening tables are computed externally in a python module // "screened_scattering.py" // to allow very specific screening functions to be added if desired, without // messing with the insides of this code. // // First version, April 2004, Marcus H. Mendenhall, Vanderbilt University // May 1, 2008 -- Added code to allow process to have zero cross section above // max energy, to coordinate with G4MSC. -- mhm // // Class Description - End #ifndef G4ScreenedNuclearRecoil_h #define G4ScreenedNuclearRecoil_h 1 #include "c2_function.hh" #include "G4ParticleChange.hh" #include "G4PhysicalConstants.hh" #include "G4SystemOfUnits.hh" #include "G4VDiscreteProcess.hh" #include "globals.hh" #include #include class G4VNIELPartition; typedef c2_const_ptr G4_c2_const_ptr; typedef c2_ptr G4_c2_ptr; typedef c2_function G4_c2_function; typedef struct G4ScreeningTables { G4double z1, z2, m1, m2, au, emin; G4_c2_const_ptr EMphiData; } G4ScreeningTables; // A class for loading ScreenedCoulombCrossSections class G4ScreenedCoulombCrossSectionInfo { public: G4ScreenedCoulombCrossSectionInfo() {} ~G4ScreenedCoulombCrossSectionInfo() {} static const char* CVSHeaderVers() { return "G4ScreenedNuclearRecoil.hh,v 1.24 2008/05/01 19:58:59 marcus Exp GEANT4 tag "; } static const char* CVSFileVers(); }; // A class for loading ScreenedCoulombCrossSections class G4ScreenedCoulombCrossSection : public G4ScreenedCoulombCrossSectionInfo { public: G4ScreenedCoulombCrossSection() : verbosity(1) {} G4ScreenedCoulombCrossSection(const G4ScreenedCoulombCrossSection& src) : G4ScreenedCoulombCrossSectionInfo(), verbosity(src.verbosity) {} virtual ~G4ScreenedCoulombCrossSection(); typedef std::map ScreeningMap; // a local, fast-access mapping of a particle's Z to its full definition typedef std::map ParticleCache; // LoadData is called by G4ScreenedNuclearRecoil::GetMeanFreePath // It loads the data tables, builds the elemental cross-section tables. virtual void LoadData(G4String screeningKey, G4int z1, G4double m1, G4double recoilCutoff) = 0; // BuildMFPTables is called by G4ScreenedNuclearRecoil::GetMeanFreePath // to build the MFP tables for each material void BuildMFPTables(void); // scan the MaterialsTable and construct MFP // tables virtual G4ScreenedCoulombCrossSection* create() = 0; // a 'virtual constructor' which clones the class const G4ScreeningTables* GetScreening(G4int Z) { return &(screeningData[Z]); } void SetVerbosity(G4int v) { verbosity = v; } // this process needs element selection weighted only by number density G4ParticleDefinition* SelectRandomUnweightedTarget(const G4MaterialCutsCouple* couple); enum { nMassMapElements = 116 }; G4double standardmass(G4int z1) { return z1 <= nMassMapElements ? massmap[z1] : 2.5 * z1; } // get the mean-free-path table for the indexed material const G4_c2_function* operator[](G4int materialIndex) { return MFPTables.find(materialIndex) != MFPTables.end() ? &(MFPTables[materialIndex].get()) : (G4_c2_function*)0; } protected: ScreeningMap screeningData; // screening tables for each element ParticleCache targetMap; G4int verbosity; std::map sigmaMap; // total cross section for each element std::map MFPTables; // MFP for each material private: static const G4double massmap[nMassMapElements + 1]; }; typedef struct G4CoulombKinematicsInfo { G4double impactParameter; G4ScreenedCoulombCrossSection* crossSection; G4double a1, a2, sinTheta, cosTheta, sinZeta, cosZeta, eRecoil; G4ParticleDefinition* recoilIon; const G4Material* targetMaterial; } G4CoulombKinematicsInfo; class G4ScreenedCollisionStage { public: virtual void DoCollisionStep(class G4ScreenedNuclearRecoil* master, const class G4Track& aTrack, const class G4Step& aStep) = 0; virtual ~G4ScreenedCollisionStage() {} }; class G4ScreenedCoulombClassicalKinematics : public G4ScreenedCoulombCrossSectionInfo, public G4ScreenedCollisionStage { public: G4ScreenedCoulombClassicalKinematics(); virtual void DoCollisionStep(class G4ScreenedNuclearRecoil* master, const class G4Track& aTrack, const class G4Step& aStep); G4bool DoScreeningComputation(class G4ScreenedNuclearRecoil* master, const G4ScreeningTables* screen, G4double eps, G4double beta); virtual ~G4ScreenedCoulombClassicalKinematics() {} protected: // the c2_functions we need to do the work. c2_const_plugin_function_p& phifunc; c2_linear_p& xovereps; G4_c2_ptr diff; }; class G4SingleScatter : public G4ScreenedCoulombCrossSectionInfo, public G4ScreenedCollisionStage { public: G4SingleScatter() {} virtual void DoCollisionStep(class G4ScreenedNuclearRecoil* master, const class G4Track& aTrack, const class G4Step& aStep); virtual ~G4SingleScatter() {} }; /** \brief A process which handles screened Coulomb collisions between nuclei */ class G4ScreenedNuclearRecoil : public G4ScreenedCoulombCrossSectionInfo, public G4VDiscreteProcess { public: friend class G4ScreenedCollisionStage; /// \param processName the name to assign the process /// \param ScreeningKey the name of a screening function to use. /// The default functions are "zbl" (recommended for soft scattering), /// "lj" (recommended for backscattering) and "mol" (Moliere potential) /// \param GenerateRecoils if frue, ions struck by primary are converted /// into new moving particles. /// If false, energy is deposited, but no new moving ions are created. /// \param RecoilCutoff energy below which no new moving particles will be /// created, even if a GenerateRecoils is true. /// Also, a moving primary particle will be stopped if its energy falls /// below this limit. /// \param PhysicsCutoff the energy transfer to which screening tables are /// calucalted. /// There is no really /// compelling reason to change it from the 10.0 eV default. /// However, see the paper on running this /// in thin targets for further discussion, and its interaction /// with SetMFPScaling() G4ScreenedNuclearRecoil(const G4String& processName = "ScreenedElastic", const G4String& ScreeningKey = "zbl", G4bool GenerateRecoils = 1, G4double RecoilCutoff = 100.0 * eV, G4double PhysicsCutoff = 10.0 * eV); virtual ~G4ScreenedNuclearRecoil(); virtual G4double GetMeanFreePath(const G4Track&, G4double, G4ForceCondition*); virtual G4VParticleChange* PostStepDoIt(const G4Track& aTrack, const G4Step& aStep); /// \param aParticleType the particle to test virtual G4bool IsApplicable(const G4ParticleDefinition& aParticleType); /// \param aParticleType the type of particle to build tables for virtual void BuildPhysicsTable(const G4ParticleDefinition& aParticleType); /// \param aParticleType the type of particle to build tables for virtual void DumpPhysicsTable(const G4ParticleDefinition& aParticleType); /// range of the selected nucleus /// \param A the nucleon number of the beam /// \param A1 the nucleon number of the target /// \param apsis the distance of closest approach virtual G4bool CheckNuclearCollision(G4double A, G4double A1, G4double apsis); // return true if hard collision virtual G4ScreenedCoulombCrossSection* GetNewCrossSectionHandler(void); G4double GetNIEL() const { return NIEL; } void ResetTables(); // clear all data tables to allow changing energy cutoff, materials, etc. /// cross section /// /// This funciton is used to coordinate this process with G4MSC. /// Typically, G4MSC should /// not be allowed to operate in a range which overlaps that of this /// process. The criterion which is most reasonable /// is that the transition should be somewhere in the modestly /// relativistic regime (500 MeV/u for example). /// param energy energy per nucleon for the cutoff void SetMaxEnergyForScattering(G4double energy) { processMaxEnergy = energy; } std::string GetScreeningKey() const { return screeningKey; } /// \param flag if true, enable deposition of energy (the default). /// If false, disable deposition. void AllowEnergyDeposition(G4bool flag) { registerDepositedEnergy = flag; } G4bool GetAllowEnergyDeposition() const { return registerDepositedEnergy; } /// If recoils are disabled, the energy they would have received is just /// deposited. /// param flag if true, create recoil ions in cases in which the energy /// is above the recoilCutoff. /// If false, just deposit the energy. void EnableRecoils(G4bool flag) { generateRecoils = flag; } G4bool GetEnableRecoils() const { return generateRecoils; } /// \param scale the factor by which the default MFP will be scaled. /// Set to less than 1 for very thin films, typically, /// to sample multiple scattering, /// or to greater than 1 for quick simulations with a very long flight path void SetMFPScaling(G4double scale) { MFPScale = scale; } G4double GetMFPScaling() const { return MFPScale; } /// which are close enough they need hadronic phsyics. /// Default is true (skip close collisions). /// Disabling this results in excess nuclear stopping power. /// \param flag true results in hard collisions being skipped. /// false allows hard collisions. void AvoidNuclearReactions(G4bool flag) { avoidReactions = flag; } G4bool GetAvoidNuclearReactions() const { return avoidReactions; } /// be generated, /// and the energy (per nucleon) below which all ions are stopped. /// \param energy energy per nucleon void SetRecoilCutoff(G4double energy) { recoilCutoff = energy; } G4double GetRecoilCutoff() const { return recoilCutoff; } /// Typically, this is 10 eV or so, and not often changed. /// \param energy the cutoff energy void SetPhysicsCutoff(G4double energy) { physicsCutoff = energy; ResetTables(); } G4double GetPhysicsCutoff() const { return physicsCutoff; } void SetNIELPartitionFunction(const G4VNIELPartition* part); /// backscattering /// \param fraction the fraction of particles to have their cross section /// boosted. /// \param HardeningFactor the factor by which to boost the scattering /// cross section. void SetCrossSectionHardening(G4double fraction, G4double HardeningFactor) { hardeningFraction = fraction; hardeningFactor = HardeningFactor; } G4double GetHardeningFraction() const { return hardeningFraction; } G4double GetHardeningFactor() const { return hardeningFactor; } G4double GetCurrentInteractionLength() const { return currentInteractionLength; } /// if the user needs non-standard behavior. /// \param cs a class which constructs the screening tables. void SetExternalCrossSectionHandler(G4ScreenedCoulombCrossSection* cs) { externalCrossSectionConstructor = cs; } G4int GetVerboseLevel() const { return verboseLevel; } std::map& GetCrossSectionHandlers() { return crossSectionHandlers; } void ClearStages(void); void AddStage(G4ScreenedCollisionStage* stage) { collisionStages.push_back(stage); } G4CoulombKinematicsInfo& GetKinematics() { return kinematics; } void SetValidCollision(G4bool flag) { validCollision = flag; } G4bool GetValidCollision() const { return validCollision; } /// for internal use, primarily. class G4ParticleChange& GetParticleChange() { return static_cast(*pParticleChange); } /// to partition it into NIEL and ionizing energy. void DepositEnergy(G4int z1, G4double a1, const G4Material* material, G4double energy); protected: G4double highEnergyLimit; G4double lowEnergyLimit; /// to cross over to G4MSC G4double processMaxEnergy; G4String screeningKey; G4bool generateRecoils, avoidReactions; G4double recoilCutoff, physicsCutoff; G4bool registerDepositedEnergy; G4double IonizingLoss, NIEL; G4double MFPScale; G4double hardeningFraction, hardeningFactor; G4ScreenedCoulombCrossSection* externalCrossSectionConstructor; std::vector collisionStages; std::map crossSectionHandlers; G4bool validCollision; G4CoulombKinematicsInfo kinematics; const G4VNIELPartition* NIELPartitionFunction; }; // A customized G4CrossSectionHandler which gets its data from // an external program class G4NativeScreenedCoulombCrossSection : public G4ScreenedCoulombCrossSection { public: G4NativeScreenedCoulombCrossSection(); G4NativeScreenedCoulombCrossSection(const G4NativeScreenedCoulombCrossSection& src) : G4ScreenedCoulombCrossSection(src), phiMap(src.phiMap) {} G4NativeScreenedCoulombCrossSection(const G4ScreenedCoulombCrossSection& src) : G4ScreenedCoulombCrossSection(src) {} virtual ~G4NativeScreenedCoulombCrossSection(); virtual void LoadData(G4String screeningKey, G4int z1, G4double m1, G4double recoilCutoff); virtual G4ScreenedCoulombCrossSection* create() { return new G4NativeScreenedCoulombCrossSection(*this); } // get a list of available keys std::vector GetScreeningKeys() const; typedef G4_c2_function& (*ScreeningFunc)(G4int z1, G4int z2, size_t nPoints, G4double rMax, G4double* au); void AddScreeningFunction(G4String name, ScreeningFunc fn) { phiMap[name] = fn; } private: // this is a map used to look up screening function generators std::map phiMap; }; G4_c2_function& ZBLScreening(G4int z1, G4int z2, size_t npoints, G4double rMax, G4double* auval); G4_c2_function& MoliereScreening(G4int z1, G4int z2, size_t npoints, G4double rMax, G4double* auval); G4_c2_function& LJScreening(G4int z1, G4int z2, size_t npoints, G4double rMax, G4double* auval); G4_c2_function& LJZBLScreening(G4int z1, G4int z2, size_t npoints, G4double rMax, G4double* auval); #endif