完整後設資料紀錄
DC 欄位 | 值 | 語言 |
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dc.contributor.author | Blyth, S. C. | en_US |
dc.contributor.author | Chan, Y. L. | en_US |
dc.contributor.author | Chen, X. C. | en_US |
dc.contributor.author | Chu, M. C. | en_US |
dc.contributor.author | Cui, K. X. | en_US |
dc.contributor.author | Hahn, R. L. | en_US |
dc.contributor.author | Ho, T. H. | en_US |
dc.contributor.author | Hsiung, Y. B. | en_US |
dc.contributor.author | Hu, B. Z. | en_US |
dc.contributor.author | Kwan, K. K. | en_US |
dc.contributor.author | Kwok, M. W. | en_US |
dc.contributor.author | Kwok, T. | en_US |
dc.contributor.author | Lau, Y. P. | en_US |
dc.contributor.author | Leung, J. K. C. | en_US |
dc.contributor.author | Leung, K. Y. | en_US |
dc.contributor.author | Lin, G. L. | en_US |
dc.contributor.author | Lin, Y. C. | en_US |
dc.contributor.author | Luk, K. B. | en_US |
dc.contributor.author | Luk, W. H. | en_US |
dc.contributor.author | Ngai, H. Y. | en_US |
dc.contributor.author | Ngan, S. Y. | en_US |
dc.contributor.author | Pun, C. S. J. | en_US |
dc.contributor.author | Shih, K. | en_US |
dc.contributor.author | Tam, Y. H. | en_US |
dc.contributor.author | Tsang, R. H. M. | en_US |
dc.contributor.author | Wang, C. H. | en_US |
dc.contributor.author | Wong, C. M. | en_US |
dc.contributor.author | Wong, H. L. | en_US |
dc.contributor.author | Wong, K. K. | en_US |
dc.contributor.author | Yeh, M. | en_US |
dc.contributor.author | Zhang, B. J. | en_US |
dc.date.accessioned | 2018-08-21T05:56:35Z | - |
dc.date.available | 2018-08-21T05:56:35Z | - |
dc.date.issued | 2016-04-01 | en_US |
dc.identifier.issn | 2405-6014 | en_US |
dc.identifier.uri | http://dx.doi.org/10.1016/j.nuclphysbps.2015.10.027 | en_US |
dc.identifier.uri | http://hdl.handle.net/11536/146376 | - |
dc.description.abstract | Muon-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.iso | en_US | en_US |
dc.subject | Cosmic-ray muon | en_US |
dc.subject | Spallation neutron | en_US |
dc.subject | Aberdeen Tunnel | en_US |
dc.subject | Underground laboratory | en_US |
dc.title | Measurement of Cosmic-ray Muon-induced Spallation Neutrons in the Aberdeen Tunnel Underground Laboratory | en_US |
dc.type | Proceedings Paper | en_US |
dc.identifier.doi | 10.1016/j.nuclphysbps.2015.10.027 | en_US |
dc.identifier.journal | NUCLEAR AND PARTICLE PHYSICS PROCEEDINGS | en_US |
dc.citation.volume | 273 | en_US |
dc.citation.spage | 2675 | en_US |
dc.citation.epage | 2677 | en_US |
dc.contributor.department | 物理研究所 | zh_TW |
dc.contributor.department | Institute of Physics | en_US |
dc.identifier.wosnumber | WOS:000390295200492 | en_US |
顯示於類別: | 會議論文 |