High energy muon induced radioactive nuclides in nickel plate and its use for 2-D muon-beam image profile
High energy muon induced radioactive nuclides in nickel plate and its use for 2-D muon-beam image profile
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镍板中高能μ介子诱发放射性核素及其在二维μ介子束图像剖面中的应用
DOI:
10.1016/j.nima.2015.07.021
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发表时间:
2015
期刊:
影响因子:
--
通讯作者:
S. Kunieda
中科院分区:
文献类型:
--
作者:
Y. Kurebayashi;H. Sakurai;Y. Takahashi;N. Doshita;S. Kikuchi;F. Tokanai;K. Horiuchi;Y. Tajima;T. Oe;T. Sato;S. Gunji;E. Inui;K. Kondo;N. Iwata;N. Sasaki;H. Matsuzaki;S. Kunieda
Target materials were exposed to a muon beam with an energy of 160 GeV/c at the COMPASS experiment line in CERN-SPS to measure the production cross-sections for muon-induced radionuclides. A muon imager containing four nickel plates, each measuring 100 mm×100 mm, exposed to the IP plate successfully detected the muon beam image during an irradiation period of 33 days. The contrasting density rate of the nickel plate was (5.2±0.7)×10–9PSL/muon per one-day exposure to IP. The image measured 122 mm and 174 mm in horizontal and vertical lengths, respectively, in relation to the surface of the base, indicating that 50±6% of the muon beam flux is confined to an area of 18% of the whole muon beam. The number of muons estimated from the PSL value in the total beam image area (0.81±0.1)×1013was comparable to the total muon counts of the ion-chamber at the M2 beam line in the CERN-SPS. The production cross-sections of Cr-51, Mn-54, Co-56, Co-57, and Co-58 in nickel were 0.19±0.08, 0.34±0.06, 0.5±0.05, 3.44±0.07, 0.4±0.03 in the unit of mb, respectively, reducing muon associated particles effects. They are approximately 10 times smaller than that a proceeding study by Heisinger et al.