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geant4/source/processes/electromagnetic/dna/models/include/G4DNAPTBElasticModel.hh
2023-12-08 10:43:34 +01:00

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//
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// Authors: S. Meylan and C. Villagrasa (IRSN, France)
// Models come from
// M. Bug et al, Rad. Phys and Chem. 130, 459-479 (2017)
//
#ifndef G4DNAPTBElasticModel_h
#define G4DNAPTBElasticModel_h 1
#include "G4DNACrossSectionDataSet.hh"
#include "G4Electron.hh"
#include "G4LogLogInterpolation.hh"
#include "G4NistManager.hh"
#include "G4ParticleChangeForGamma.hh"
#include "G4ProductionCutsTable.hh"
#include "G4VDNAModel.hh"
#include <map>
/*!
* \brief The G4DNAPTBElasticModel class
* This class implements the elastic model for the DNA materials and precursors.
*/
class G4DNAPTBElasticModel : public G4VDNAModel
{
public:
using TriDimensionMap = std::map<std::size_t,
std::map<const G4ParticleDefinition*, std::map<G4double, std::map<G4double, G4double>>>>;
using VecMap = std::map<std::size_t,
std::map<const G4ParticleDefinition*, std::map<G4double, std::vector<G4double>>>>;
/*!
* \brief G4DNAPTBElasticModel
* Constructor
* \param applyToMaterial
* \param p
* \param nam
*/
G4DNAPTBElasticModel(const G4String& applyToMaterial = "all",
const G4ParticleDefinition* p = nullptr, const G4String& nam = "DNAPTBElasticModel");
/*!
* \brief ~G4DNAPTBElasticModel
* Destructor
*/
~G4DNAPTBElasticModel() override = default;
// copy constructor and hide assignment operator
G4DNAPTBElasticModel(G4DNAPTBElasticModel&) = delete; // prevent copy-construction
G4DNAPTBElasticModel& operator=(
const G4DNAPTBElasticModel& right) = delete; // prevent assignement
/*!
* \brief Initialise
* Mandatory method for every model class. The material/particle for which the model
* can be used have to be added here through the AddCrossSectionData method.
* Then the LoadCrossSectionData method must be called to trigger the load process.
* Scale factors to be applied to the cross section can be defined here.
*/
void Initialise(const G4ParticleDefinition* particle, const G4DataVector&) override;
/*!
* \brief CrossSectionPerVolume
* This method is mandatory for any model class. It finds and return the cross section value
* for the current material, particle and energy values.
* The number of molecule per volume is not used here but in the G4DNAModelInterface class.
* \param material
* \param materialName
* \param p
* \param ekin
* \param emin
* \param emax
* \return the cross section value
*/
G4double CrossSectionPerVolume(const G4Material* material, const G4ParticleDefinition* p,
G4double ekin, G4double emin, G4double emax) override;
/*!
* \brief SampleSecondaries
* Method called after CrossSectionPerVolume if the process is the one which is selected
* (according to the sampling on the calculated path length). Here, the characteristics of the
* incident and created (if any) particle(s) are set (energy, momentum ...). \param materialName
* \param particleChangeForGamma
* \param tmin
* \param tmax
*/
void SampleSecondaries(std::vector<G4DynamicParticle*>*, const G4MaterialCutsCouple*,
const G4DynamicParticle*, G4double tmin, G4double tmax) override;
protected:
G4ParticleChangeForGamma* fParticleChangeForGamma = nullptr;
private:
G4int verboseLevel = 0; ///< verbose level
// Verbosity scale:
// 0 = nothing
// 1 = warning for energy non-conservation
// 2 = details of energy budget
// 3 = calculation of cross sections, file openings, sampling of atoms
// 4 = entering in methods
G4double fKillBelowEnergy = 0.;
///< energy kill limit
TriDimensionMap diffCrossSectionData;
///< A map: [materialName][particleName]=DiffCrossSectionTable
VecMap eValuesVect;
/*!< map with vectors containing all the output energy (E) of the diff. file */
std::map<std::size_t, std::map<const G4ParticleDefinition*, std::vector<G4double>>> tValuesVec;
///< map with vectors containing all the incident (T) energy of the dif. file
G4Material* fpGuanine_PU = nullptr;
G4Material* fpTHF = nullptr;
G4Material* fpPY = nullptr;
G4Material* fpPU = nullptr;
G4Material* fpTMP = nullptr;
G4Material* fpG4_WATER = nullptr;
G4Material* fpBackbone_THF = nullptr;
G4Material* fpCytosine_PY = nullptr;
G4Material* fpThymine_PY = nullptr;
G4Material* fpAdenine_PU = nullptr;
G4Material* fpBackbone_TMP = nullptr;
G4Material* fpN2 = nullptr;
G4DNAPTBElasticModel* fpModelData = nullptr;
/*!
* \brief ReadDiffCSFile
* Method to read the differential cross section files. This method is not standard yet so every
* model must implement its own. \param materialName \param particleName \param file
*/
void ReadDiffCSFile(const std::size_t& materialID, const G4ParticleDefinition* particleName,
const G4String& file, const G4double&) override;
/*!
* \brief Theta
* To return an angular theta value from the differential file. This method uses interpolations to
* calculate the theta value. \param fParticleDefinition \param k \param integrDiff \param
* materialName \return a theta value
*/
G4double Theta(
const G4ParticleDefinition* p, G4double k, G4double integrDiff, const std::size_t& materialID);
/*!
* \brief LinLinInterpolate
* \param e1
* \param e2
* \param e
* \param xs1
* \param xs2
* \return
*/
G4double LinLinInterpolate(G4double e1, G4double e2, G4double e, G4double xs1, G4double xs2);
/*!
* \brief LinLogInterpolate
* \param e1
* \param e2
* \param e
* \param xs1
* \param xs2
* \return
*/
G4double LinLogInterpolate(G4double e1, G4double e2, G4double e, G4double xs1, G4double xs2);
/*!
* \brief LogLogInterpolate
* \param e1
* \param e2
* \param e
* \param xs1
* \param xs2
* \return
*/
G4double LogLogInterpolate(G4double e1, G4double e2, G4double e, G4double xs1, G4double xs2);
/*!
* \brief QuadInterpolator
* \param e11
* \param e12
* \param e21
* \param e22
* \param x11
* \param x12
* \param x21
* \param x22
* \param t1
* \param t2
* \param t
* \param e
* \return
*/
G4double QuadInterpolator(G4double e11, G4double e12, G4double e21, G4double e22, G4double x11,
G4double x12, G4double x21, G4double x22, G4double t1, G4double t2, G4double t, G4double e);
/*!
* \brief RandomizeCosTheta
* \param k
* \param materialName
* \return
*/
G4double RandomizeCosTheta(const G4double& k, const std::size_t& materialName);
};
#endif