Neutron background expectation
Simon JM Peeters s.j.m.peeters@sussex.ac.uk JT DAQ Physics Performance WG 2019.11.21
Neutron background expectation Simon JM Peeters - - PowerPoint PPT Presentation
Neutron background expectation Simon JM Peeters s.j.m.peeters@sussex.ac.uk JT DAQ Physics Performance WG 2019.11.21 In G4: ENDF Data Base, Neutron capture in LAr slightly different (worse) n + 40 Ar 41 Ar * : dominant n + 36 Ar 37 Ar *
Simon JM Peeters s.j.m.peeters@sussex.ac.uk JT DAQ Physics Performance WG 2019.11.21
Hardell, R. and Beer, C., 1970. Thermal Neutron Capture in Natural Argon. Physica Scripta, 1(2-3), p.85.
n + 40Ar 41Ar* : dominant n + 36Ar 37Ar* Radiative neutron capture on Argon results in an excited atom
isotope. The excited argon isotopes de- excite with very specific total energy: 6.1 MeV for 41Ar, 8.8 MeV for 37Ar. This energy is carried away by at least one photon on the case of
37Ar and at least two photons in
the case of 41Ar.
=0.978 In G4: ENDF Data Base, slightly different (worse)
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Neutron capture
(Compton) See Pierre’s talk last time (and at/around CM): https://indico.fnal.gov/event/22378/contribution/0/material/slides/0.pdf e CC events
Aran, Tyler & Pierre – more details & motivation, see (amongst other talks): https://indico.fnal.gov/event/21861/session/6/contribution/20/material/slides/0.pdf
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Effective neutron mean free path could be ~30 m! (ENDF: as currently in GEANT4)
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arXiv:1902.00596
https://indico.fnal.gov/event/20996/other-view?view=standard Report by review committee has been distributed but not published yet (?)
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2019.11.21 Simon JM Peeters | Neutrons in DUNE | DAQ PPWG 8
Dominant (large mass):
(238U/232Th/56Fe(,n)/54Fe(,n)) Subdominant (low mass/activity):
40Ar(,n)
(238U/232Th)
(238U/232Th,56Fe(,n)/54Fe(,n))
Also: cosmogenically-generated neutrons. Subdominant in rate, but possibly high- multiplicity events! Arxiv:1811.07912
Today / tomorrow https://agenda.ciemat.es/event/1127/overview Vidyo: https://agenda.ciemat.es/event/1127/page/14-remote-connection Code: 232238
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DarkSide simulation (Paola Sala) (200 events / year / ton) * 10 * 10^3 tons / (3e7 sec / year) * • 18 [flux factor] * 10 [fiducialization factor] * • 3 [PUF foam moderation] * 3 [dead LAr shell extinction] = 108 neutrons / sec captured
(J Reichenbacher @ CM https://indico.fnal.gov/event/21445/session/16/contribution/172/material/slides/0.pdf)
in good agreement with: 104 Hz Aran Borkum, DUNE LArSoft (Geant4) 81 Hz Beacom et al (FLUKA) We expect a factor 3 shielding from insulation, so around: 30 n/s
protoDUNE sample: 4.15 1.59 Bq/kg in 238U
(J Reichenbacher, SDSM&T, https://indico.fnal.gov/event/21625/contribution/0/material/slides/0.pdf)
238U fission, 56Fe(,n) & 54Fe(,n):
O(10) Hz
(J Reichenbacher, SDSM&T, https://indico.fnal.gov/event/22323/contribution/0/material/slides/0.pptx)
Stratification during manufacturing process (226Ra out of equilibrium): sample steel coupons from different heights in smelt
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Vitaly (SOURCES4A): For 238U+235U chains in equlibrium the (,n) yield: 1.46*10-10 n/g/s/ppb Radon and below: 1.37*10-10 n/g/s/ppb For 232Th chain in equilibrium: 8.71*10^(-11) n/g/s/ppb. Even for worst case, we expect: < 1 n/s. ((alpha,gamma) 13 gammas/day)
(J Reichenbacher, SDSM&T, https://indico.fnal.gov/event/22323/contribution/0/material/slides/0.pptx)
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Preliminary measurement at Boulby (David Waters): 3 Bq/kg 616.9 kg in one module. Vitaly (SOURCES4A) has provided expected (,n) yield: again, much below 1 n/s
this in detail, measure the relevant activities in materials, and put in controls where we can.
underway.
effect/use of any shielding.
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