Highlights in Low Energy Hadronic Physics

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Presentation transcript:

Highlights in Low Energy Hadronic Physics Geant4 Collaboration Meeting 27 September 2017 Dennis Wright

Outline De-excitation and Precompound Low Energy Database Models Radioactive decay Nuclear Resonance Fluorescence Neutrino Physics

Common Developments for Pre-compound/De-excitation G4DeexPrecoParameters scheme introduced in 10.3 is extended Printout of all important parameters values at initialisation Modification of parameters allowed only at G4State_PreInit New booleans added to allow disabling of de-excitation module Only one singleton class G4NuclearDataStore left with static data shared between all threads No longer any thread local data Time and creator model information is propagated to G4HadronicProcess Allowing proper checks of charge and energy conservation Emission of Auger electrons breaks old checks 3

De-excitation Module for 10.4 Evaporation/FermiBreakUp/Photon evaporation updated according to plan for 10.4 Data structure for gamma levels is finalized with G4PhotonEvaporation5.0 Half the size of data in 10.3 Laurent Desorgher produced data files Fixed several bug reports for 10.3 concerning radioactive decay and photon evaporation Optimized data structure: use double, float and integer with maximum compression of data In all classes of the module excited energy of a fragment is taken from the DB directly without any conversion and not computed on-fly Providing reproducibility Isomer production is enabled by default Time limit is taken from G4NuclideTable providing full synkronisation between production and decay

De-excitation Module for 10.4 Correlated gamma decay (Jason Detwiler, University of Washington) Works for several important isotopes (Co60) but provides very long loops if applied in general Triggers non-reproducibility and slow-down in radioactive decay chain sampling Enabled by request or by G4RadiactiveDecayPhysics May be disabled by default also for radioactive decay if problems will not be fixed before 10.4

Double Differential Spectra of Neutrons for 22 MeV Proton Beam The Binary cascade predicts more supressed low-energy part of the spectra than the Bertini cascade There are non-ideal description of the end of the spectra, which means that cascades are not accurate in sampling of quasi-elastic scattering 6

Double Differential Spectra of Neutrons for 256 MeV Proton Beam The Binary cascade predicts more accurately forward neutron spectra The Bertini cascade is more accurate in the backward hemisphere

New Low Energy Photonuclear Model G4LENDorBertModel will use G4LEND models below 20 MeV database has g interaction information on isotopes from D to 241Pu for isotopes with no data, or for Eg > 20 MeV  Bertini cross sections also come from LEND, unless no data, then use G4PhotoNuclearCrossSection as we do now G4LEND gamma models parallel the LEND neutron models: fission, capture, inelastic, elastic to simplify usage in physics lists, fission, capture, inelastic to be combined into one model, elastic in another Existing physics list, ShieldingLEND will be modified to include new model

Geant4/FLUKA Comparison, Quintieri et al. at SATIF 13

Cross Section Comparison, LEND vs. G4PhotoNuclearCrossSection

Thermal Neutron Scattering Validation N.H. Tran @ CEA

Radioactive Decay RDM mini-workshop held at CERN in April 2017 Highlights beta-delayed particle emission works for transitions to discrete levels agreed to refactor RDM code into separate analogue and variance reduction models reduction in number of half-life limits used in code RDM and IT code refactored to include correlated gamma emission photon evaporation and radioactive decay databases now consistent in format and notation (both taken from ENSDF) new example: rdecay03

Radioactive Decay New radioactive decay models Interface changes G4RadioactiveDecayBase (all variance reduction code stripped out) G4Radioactivation (derived from G4RadioactiveDecayBase, only VR code kept) Original class G4RadioactiveDecay kept Interface changes Refactored code contains changes that would break user code – must wait until major release to replace G4RadioactiveDecay two user commands will become obsolete fBeta analogueMC

Validation Example: Bi214 17

Radioactive Decay Tasks Examine possibility of using matrix algebra to implement time evolution of Bateman equations Complete beta-delayed particle emission to continuum Investigate use of Kibedi model of atomic deexcitation Validate new correlated gamma code New examples, including correlated gammas Decide what to do with floating to non-floating transitions

G4NRF: Extending Photonuclear to Lower Energies Nuclear Resonance Fluorescence G4NRF developed by Jayson Vavrek (MIT) 10 keV < Eg < ~10 MeV sharp lines (~few eV or less) uses mostly ENSDF, but also needs extra DB planned for inclusion next year many applications Emitted g Incident g

238U NRF Spectrum from Bremsstrahlung Gammas (endpoint 2.5 MeV)

G4NRF Thin Target Validation

Neutrino Scattering First step: Geant4-to-GENIE interface use Geant4 Bertini cascade to do final state interactions in nucleus after GENIE neutrino vertex is generated complete, committed to GENIE svn validation underway Next step: GENIE-to-Geant4 use GENIE neutrino generators to initiate neutrino interactions in Geant4 need wrapper models to have GENIE models treated as Geant4 models some native Geant4 neutrino cross section classes already exist (V. Grichine)

Neutrino Scattering: NCEL (black: Bertini, blue: GENIE)

Neutrino Scattering: DIS (black: Bertini, Blue: GENIE)

Conclusions Several model extensions ready for 10.4 correlated gamma emission, radioactive decay extensions New models getting close G4LEND-based photonuclear model Neutrino scattering interface Nuclear Resonance Fluorescence