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dc.contributor.authorBlyth, S. C.en_US
dc.contributor.authorChan, Y. L.en_US
dc.contributor.authorChen, X. C.en_US
dc.contributor.authorChu, M. C.en_US
dc.contributor.authorCui, K. X.en_US
dc.contributor.authorHahn, R. L.en_US
dc.contributor.authorHo, T. H.en_US
dc.contributor.authorHsiung, Y. B.en_US
dc.contributor.authorHu, B. Z.en_US
dc.contributor.authorKwan, K. K.en_US
dc.contributor.authorKwok, M. W.en_US
dc.contributor.authorKwok, T.en_US
dc.contributor.authorLau, Y. P.en_US
dc.contributor.authorLeung, J. K. C.en_US
dc.contributor.authorLeung, K. Y.en_US
dc.contributor.authorLin, G. L.en_US
dc.contributor.authorLin, Y. C.en_US
dc.contributor.authorLuk, K. B.en_US
dc.contributor.authorLuk, W. H.en_US
dc.contributor.authorNgai, H. Y.en_US
dc.contributor.authorNgan, S. Y.en_US
dc.contributor.authorPun, C. S. J.en_US
dc.contributor.authorShih, K.en_US
dc.contributor.authorTam, Y. H.en_US
dc.contributor.authorTsang, R. H. M.en_US
dc.contributor.authorWang, C. H.en_US
dc.contributor.authorWong, C. M.en_US
dc.contributor.authorWong, H. L.en_US
dc.contributor.authorWong, K. K.en_US
dc.contributor.authorYeh, M.en_US
dc.contributor.authorZhang, B. J.en_US
dc.date.accessioned2017-04-21T06:50:09Z-
dc.date.available2017-04-21T06:50:09Z-
dc.date.issued2016-04-06en_US
dc.identifier.issn2405-6014en_US
dc.identifier.urihttp://dx.doi.org/10.1016/j.nuclphysbps.2015.10.027en_US
dc.identifier.urihttp://hdl.handle.net/11536/134299-
dc.description.abstractMuon-induced neutrons are one of the major backgrounds to various underground experiments, such as dark matter searches, low-energy neutrino oscillation experiments and neutrino-less double beta-decay experiments. Previous experiments on the underground production rate of muon-induced neutrons were mostly carried out either at shallow sites or at very deep sites. The Aberdeen Tunnel experiment aims to measure the neutron production rate at a moderate depth of 611 meters water equivalent. Our apparatus comprises of six layers of plastic-scintillator hodoscopes for tracking the incident cosmic-ray muons, and 760 L of gadolinium-doped liquid-scintillator for both neutron production and detection targets. In this paper, we describe the design and the performance of the apparatus. The preliminary result on the measurement of neutron production rate is also presented.en_US
dc.language.isoen_USen_US
dc.subjectCosmic-ray muonen_US
dc.subjectSpallation neutronen_US
dc.subjectAberdeen Tunnelen_US
dc.subjectUnderground laboratoryen_US
dc.titleMeasurement of Cosmic-ray Muon-induced Spallation Neutrons in the Aberdeen Tunnel Underground Laboratoryen_US
dc.typeProceedings Paperen_US
dc.identifier.doi10.1016/j.nuclphysbps.2015.10.027en_US
dc.identifier.journalNUCLEAR AND PARTICLE PHYSICS PROCEEDINGSen_US
dc.citation.volume273en_US
dc.citation.spage2675en_US
dc.citation.epage2677en_US
dc.contributor.department物理研究所zh_TW
dc.contributor.departmentInstitute of Physicsen_US
dc.identifier.wosnumberWOS:000390295200492en_US
dc.citation.woscount0en_US
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