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dc.contributor.authorK. Chaiwongkhoten_US
dc.contributor.authorD. Ruffoloen_US
dc.contributor.authorW. Yamwongen_US
dc.contributor.authorJ. Prabketen_US
dc.contributor.authorP. S. Mangearden_US
dc.contributor.authorA. Sáizen_US
dc.contributor.authorW. Mitthumsirien_US
dc.contributor.authorC. Bangliengen_US
dc.contributor.authorE. Kittiyaen_US
dc.contributor.authorW. Nuntiyakulen_US
dc.contributor.authorU. Tippawanen_US
dc.contributor.authorM. Jitpukdeeen_US
dc.contributor.authorS. Aukkaravittayapunen_US
dc.date.accessioned2022-10-16T07:28:16Z-
dc.date.available2022-10-16T07:28:16Z-
dc.date.issued2021-11-01en_US
dc.identifier.issn09276505en_US
dc.identifier.other2-s2.0-85107805606en_US
dc.identifier.other10.1016/j.astropartphys.2021.102617en_US
dc.identifier.urihttps://www.scopus.com/inward/record.uri?partnerID=HzOxMe3b&scp=85107805606&origin=inwarden_US
dc.identifier.urihttp://cmuir.cmu.ac.th/jspui/handle/6653943832/77332-
dc.description.abstractUsing a setup for testing a prototype for a satellite-borne cosmic-ray ion detector, we have operated a stack of scintillator and silicon detectors on top of the Princess Sirindhorn Neutron Monitor (PSNM), an NM64 detector at 2560-m altitude at Doi Inthanon, Thailand (18.59∘N, 98.49∘E). Monte Carlo simulations have indicated that about 15% of the neutron counts by PSNM are due to interactions (mostly in the lead producer) of GeV-range protons among the atmospheric secondary particles from cosmic ray showers, which can be detected by the scintillator and silicon detectors. Those detectors can provide a timing trigger for measurement of the propagation time distribution of such neutrons as they scatter and propagate through the NM64, processes that are similar whether the interaction was initiated by an energetic proton (for 15% of the count rate) or neutron (for 80% of the count rate). This propagation time distribution underlies the time delay distribution between successive neutron counts, from which we can determine the leader fraction (inverse multiplicity), which has been used to monitor Galactic cosmic ray spectral variations over ∼1-40 GV. Here we have measured and characterized the propagation time distribution from both the experimental setup and Monte Carlo simulations of atmospheric secondary particle detection. We confirm a known propagation time distribution with a peak (at ≈70 μs) and tail over a few ms, dominated by neutron counts. We fit this distribution using an analytic model of neutron diffusion and absorption, for both experimental and Monte Carlo results. In addition we identify a group of prompt neutron monitor pulses that arrive within 20 μs of the charged-particle trigger, of which a substantial fraction can be attributed to charged-particle ionization in a proportional counter, according to both experimental and Monte Carlo results. Prompt pulses, either due to neutrons or charged-particle ionization, are associated with much higher mean multiplicity than typical pulses. These results validate and point the way to some improvements in Monte Carlo simulations and the resulting yield functions used to interpret the neutron monitor count rate and leader fraction.en_US
dc.subjectPhysics and Astronomyen_US
dc.titleMeasurement and simulation of the neutron propagation time distribution inside a neutron monitoren_US
dc.typeJournalen_US
article.title.sourcetitleAstroparticle Physicsen_US
article.volume132en_US
article.stream.affiliationsRajamangala University of Technology Thanyaburi (RMUTT)en_US
article.stream.affiliationsKasetsart Universityen_US
article.stream.affiliationsMahidol Universityen_US
article.stream.affiliationsThailand National Electronics and Computer Technology Centeren_US
article.stream.affiliationsChiang Mai Universityen_US
article.stream.affiliationsThe Bartol Research Instituteen_US
article.stream.affiliationsNational Astronomical Research Institute of Thailanden_US
Appears in Collections:CMUL: Journal Articles

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