1 / 15

GEANT4 – Simulations of muon-induced neutrons for the

Experiment. Forschungszentrum Karlsruhe in der Helmholtz-Gemeinschaft. Institut für Kernphysik. GEANT4 – Simulations of muon-induced neutrons for the. EDELWEISS II muon veto, Geant4 physics, muon induced neutrons, muon-nuclear interaction, summary & discussion.

odette
Download Presentation

GEANT4 – Simulations of muon-induced neutrons for the

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript


  1. Experiment Forschungszentrum Karlsruhein der Helmholtz-Gemeinschaft Institut für Kernphysik GEANT4 – Simulations of muon-induced neutronsfor the EDELWEISS II muon veto, Geant4 physics, muon induced neutrons, muon-nuclear interaction, summary & discussion ILIAS-N3, BSNS-working group meeting Valencia, 15.04.2005

  2. EDELWEISS II – muon veto system EDWI (1kg)  EDWII (40kg)  ’total exposure’ ×100  neutron background (Erecoil > 30 keV)main source: muon-induced neutrons from rock and shielding muon veto system 10/2005: 21×320g Ge/NTD thermistor 7 ×400g Ge/NbSi ‘thin film sensors’ sensitivity goal: ×100 Markus Horn: GEANT4 – Simulations of muon-induced neutrons

  3. Tasks: Implement energy and angular distribution of muon flux in underground lab (LSM, Fréjus mountain) Deep Inelastic Scattering (DIS) of high energy muons in rock and shielding material Test & understand Geant4 `muNucl` interaction (energy & angular distribution) Comparison of Geant4 with G3, FLUKA, MCNP, etc. (`benchmarks`) Neutron tracking in the detector area and the surrounding EDELWEISS Geant4 – background simulations Markus Horn: GEANT4 – Simulations of muon-induced neutrons

  4. Geant4 7.0 physics list Inelastic models used: • Muon-photonuclear >1GeV • Photonuclear < 3GeV • QGSP (>12GeV): high energetic hadronic interaction incl. pre-equilibrium-cascade model, nuclear evaporation & multi-fragmentation • BiC (<6GeV): intra-nuclearbinary cascade model • Neutron-HP (<19MeV): data-driven model  details s.a.Geant4- Collab. Markus Horn: GEANT4 – Simulations of muon-induced neutrons

  5. Neutron yield • material: CnH2n • neutron yield in relative good agreement with experimental data • differences toKudryavtsev et al. (hep-ex/0411026) • Why 15% lower yield ?  Physics List, G4version ? • Correction of yield at 10GeV • MC error bars ? Statistics and systematics ? Rare events with high n-multiplicity ~2×105 µ(10-1000GeV), CnH2n, 3200g/cm2 Markus Horn: GEANT4 – Simulations of muon-induced neutrons

  6. Neutron multiplicity • µ-ind. spallation (in most cases only once per event) produces few hadrons • secondary neutrons by hadronic showers on average 4-5 neutrons per event • maximum multiplicity ~100 -1000(depending on material and energy, e.g. Pb, Eµ=1TeV) ~2×105 µ(280GeV), CnH2n, 3200g/cm2 Markus Horn: GEANT4 – Simulations of muon-induced neutrons

  7. material: CnH2n deep inelastic muon-nucleus interaction via virtual photon photonuclearreactions in el.-m. showers triggered by incident muon secondary neutron production (π-N, π-absorption, p-N, etc.) Muon induced neutrons >105 µ(10-1000GeV), CnH2n, 3200g/cm2 Markus Horn: GEANT4 – Simulations of muon-induced neutrons

  8. Diff. energy spectrum of neutrons • material: CnH2n • muon energy: 280 GeV • LVD exp. data(measurement in GranSasso-underground lab) scaled (x6)  neutron detector efficiency • good agreement with FLUKA simulations(Kudryavtsev et al. hep-ex/0411026) ~105 µ(280GeV), CnH2n, 3200g/cm2 Markus Horn: GEANT4 – Simulations of muon-induced neutrons

  9. Neutron yield in different materials • materials: • CnH2n, • Fréjus & LNGS rock, • concrete, • copper, • lead • muon energy: 280 GeV • max. differenceFLUKA ↔ Geant4 less than factor ×2 ~105 µ(280GeV), 3200g/cm2 Markus Horn: GEANT4 – Simulations of muon-induced neutrons

  10. Muon-nucleus interaction I preliminary • energy transfer of muon-nucleus interaction (`muNucl´) 200MeV E 280GeV E´ Etrans ~2×105 µ(280GeV), CnH2n, 3200g/cm2 Markus Horn: GEANT4 – Simulations of muon-induced neutrons

  11. Muon-nucleus interaction II - muons preliminary • angular distribution of muon-nucleus interaction (`muNucl´) µ µ´ θ ~2×105 µ(280GeV), CnH2n, 3200g/cm2 Markus Horn: GEANT4 – Simulations of muon-induced neutrons

  12. Muon-nucleus interaction III - neutrons preliminary • kinetic energy distribution of `muNucl´-neutrons sec. particles µ µ´ n ~2×105 µ(280GeV), CnH2n, 3200g/cm2 Eneutron Markus Horn: GEANT4 – Simulations of muon-induced neutrons

  13. Muon-nucleus interaction IV - neutrons preliminary • angular distribution of muon-nucleus interaction (`muNucl´) sec. particles µ µ´ n θ ~2×105 µ(280GeV), CnH2n, 3200g/cm2 Eneutron Markus Horn: GEANT4 – Simulations of muon-induced neutrons

  14. Muon-nucleus interaction V - neutrons preliminary Markus Horn: GEANT4 – Simulations of muon-induced neutrons

  15. differences to Kudryavtsev et al. (hep-ex/0411026): Due to slightly different physics list ? Or G4 version ? How to correct neutron yield for 10GeV muons ? (benchmarks) neutron multiplicity and statistics Muon-nucleus interaction: Why minimum energy transfer of 200MeV ? Why 1keV – line in neutron spectrum ? Why backward peak in angular distribution ? (Problems with G4 core dump - G4Fragment: pi±) Open questions benchmarks (ü) µ - DIS Markus Horn: GEANT4 – Simulations of muon-induced neutrons

More Related