Publication:
Monte Carlo simulation of the neutron monitor yield function

dc.contributor.authorP. S. Mangearden_US
dc.contributor.authorD. Ruffoloen_US
dc.contributor.authorA. Sáizen_US
dc.contributor.authorS. Madleeen_US
dc.contributor.authorT. Nutaroen_US
dc.contributor.otherNational Astronomical Research Institute of Thailanden_US
dc.contributor.otherMahidol Universityen_US
dc.contributor.otherUniversity of Delawareen_US
dc.contributor.otherUbon Rajathanee Universityen_US
dc.date.accessioned2018-12-11T01:57:13Z
dc.date.accessioned2019-03-14T08:04:35Z
dc.date.available2018-12-11T01:57:13Z
dc.date.available2019-03-14T08:04:35Z
dc.date.issued2016-08-01en_US
dc.description.abstract©2016. American Geophysical Union. All Rights Reserved. Neutron monitors (NMs) are ground-based detectors that measure variations of the Galactic cosmic ray flux at GV range rigidities. Differences in configuration, electronics, surroundings, and location induce systematic effects on the calculation of the yield functions of NMs worldwide. Different estimates of NM yield functions can differ by a factor of 2 or more. In this work, we present new Monte Carlo simulations to calculate NM yield functions and perform an absolute (not relative) comparison with the count rate of the Princess Sirindhorn Neutron Monitor (PSNM) at Doi Inthanon, Thailand, both for the entire monitor and for individual counter tubes. We model the atmosphere using profiles from the Global Data Assimilation System database and the Naval Research Laboratory Mass Spectrometer, Incoherent Scatter Radar Extended model. Using FLUKA software and the detailed geometry of PSNM, we calculated the PSNM yield functions for protons and alpha particles. An agreement better than 9% was achieved between the PSNM observations and the simulated count rate during the solar minimum of December 2009. The systematic effect from the electronic dead time was studied as a function of primary cosmic ray rigidity at the top of the atmosphere up to 1 TV. We show that the effect is not negligible and can reach 35% at high rigidity for a dead time >1 ms. We analyzed the response function of each counter tube at PSNM using its actual dead time, and we provide normalization coefficients between count rates for various tube configurations in the standard NM64 design that are valid to within ∼1% for such stations worldwide.en_US
dc.identifier.citationJournal of Geophysical Research: Space Physics. Vol.121, No.8 (2016), 7435-7448en_US
dc.identifier.doi10.1002/2016JA022638en_US
dc.identifier.issn21699402en_US
dc.identifier.issn21699380en_US
dc.identifier.other2-s2.0-84983535098en_US
dc.identifier.urihttps://repository.li.mahidol.ac.th/handle/123456789/43532
dc.rightsMahidol Universityen_US
dc.rights.holderSCOPUSen_US
dc.source.urihttps://www.scopus.com/inward/record.uri?partnerID=HzOxMe3b&scp=84983535098&origin=inwarden_US
dc.subjectAgricultural and Biological Sciencesen_US
dc.subjectEarth and Planetary Sciencesen_US
dc.subjectEnvironmental Scienceen_US
dc.titleMonte Carlo simulation of the neutron monitor yield functionen_US
dc.typeArticleen_US
dspace.entity.typePublication
mu.datasource.scopushttps://www.scopus.com/inward/record.uri?partnerID=HzOxMe3b&scp=84983535098&origin=inwarden_US

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