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A nton ín Krása, Mitja Majerle for the Energy plus Transmutation collaboration

Neutron Production in Spallation Reactions of p+Pb, d+Pb at GeV Energies (Experiment versus Monte Carlo simula tion ). A nton ín Krása, Mitja Majerle for the Energy plus Transmutation collaboration. Outline. Motivation Performed experiments Energy + Transmutation setup

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A nton ín Krása, Mitja Majerle for the Energy plus Transmutation collaboration

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  1. Neutron Production in Spallation Reactions of p+Pb, d+Pb at GeV Energies(Experiment versus Monte Carlo simulation) Antonín Krása, Mitja Majerlefor the Energy plus Transmutation collaboration

  2. Outline • Motivation • Performed experiments • Energy + Transmutation setup • Monte-Carlo simulations • Neutron spectra • Low-energy region (activation foils) • Intermediate region (activation foils) • High-energy region (SSNTD) • Sources of differences experiment × simulations

  3. Motivation and Tasks • Experimental data for testing the codes for simulation of neutron production and transport in ADT systems • Measurement of neutron field produced in irradiation of: • thick target, • thick target + moderator, • thick target + fissionable blanket + moderator • with relativistic protons and deuterons • Comparison: experimental× Monte-Carlo simulations  check accuracy of nuclear models and x-section libraries

  4. Experiments onthick target (+ moderator) .

  5. Phasotron setup 660 MeV Synchrophasotron setup 885 MeV

  6. Experimentson Energy+Transmutation setup

  7. ENERGY + TRANSMUTATION setup • target: Pb (28.66 kg) • blanket: U (206.4 kg) • shielding: Cd + (CH2)n

  8. Measurement of activated foils • High Purity Germanium -spectrometer

  9. Spatial distributions of yields in Al- and Au-foils • Example of yields at 1.5 GeV proton irradiation of E+T setup

  10. Monte-Carlo simulations • MCNPX 2.6.C • FLUKA Description of U/Pb assemblyin MCNPX

  11. Produced neutron spectrum • Spallation produces neutrons with keV-GeV energies • (n,g)-reaction covers neutrons with energies up to MeV

  12. MCNPX simulation of activation reaction yields

  13. Compilation of total neutron yields for p,d+Pb

  14. SSNTD Activation detectors

  15. Detectors • Activation detectors : • 197Au(n,xn)197-x+1Au • Bi, Al, Co, Ta, In • Gamma spectrometry • Solid State Nuclear Track Detectors : • natPb, natU, 235U + mica foils where fission fragments leave their tracks • Optical microscopy

  16. Results – Phasotron experiment660 MeV, bare, lead target Experiment Experiment/simulation

  17. Energy Plus Transmutation • Au detectors • Longitudinal • Radial in the first gap • SSNTD • Radial in all gaps

  18. Results – EPT, 1 GeV protons

  19. Results – EPT, 1.5 GeV protons

  20. Discrepancies • Disagreement • 1.5 GeV • 2 GeV bigger • 2.52 GeV deuterons – zero ?! • Only in radial direction • Only for threshold detectors, SSNTD are ok • Causes : • Experimental error • Simulations

  21. Experimental error ? • Systematic uncertainties were studied carefully with sets of MCNPX simulations, they are limited to ca. 30% (foil displacement, beam determination) • Transport of activated material out of foil is below 5% • Spectrometry – 5% • … ?

  22. Simulation errors ? • Spallation : • INC (E>160 MeV), • pre-equilibrium (160MeV>E>40MeV), • evaporation(40 MeV>E). • Transport of HE neutrons in uranium blanket • More tests: • Analysis of Yurevich experiments (angular spallation neutron distribution, Ep>1.5 GeV) • EPT experiment without blanket at 1.5 GeV or 2 GeV • Repeat 1 experiment (1.5 GeV or 2 GeV)

  23. Results – EPT, 1.5 GeV protonsFLUKA code - preliminary

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