Design strategy for devices under high radiation field in J-PARC muon facility

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Title: Design strategy for devices under high radiation field in J-PARC muon facility
Authors: Kawamura, Naritoshi nari.kawamura@kek.jp, Makimura, Shunsuke1, Strasser, Patrick1, Koda, Akihiro1, Fujimori, Hiroshi1, Nishiyama, Kusuo1, Miyake, Yasuhiro1, Muon section, M.L.F1
Source: Nuclear Instruments & Methods in Physics Research Section A. Feb2009, Vol. 600 Issue 1, p114-116. 3p.
Subjects: Radiation shielding for proton accelerators, Nuclear facilities, Monte Carlo method, Spallation (Nuclear physics), Muons
Geographic Terms: Tōkai Region (Japan), Japan
Abstract: Abstract: The intensity of proton accelerator has attained the order of mega-watt, and several MW-class proton accelerators have started operating in the world. In comparison with the other MW-class accelerators, Japan Proton Accelerator Research Complex (J-PARC) is unique due to the muon facility. Materials and Life Science Facility, J-PARC, has not only the mercury target but also the graphite target to provide spallation neutrons and muons, respectively. The muon target is inserted upstream of the neutron target in the proton beam line. Full use of several mutually linking Monte-Carlo codes enables the design work of devices in the muon facility, which has to be operated under high radiation field from the muon target. [Copyright &y& Elsevier]
Copyright of Nuclear Instruments & Methods in Physics Research Section A is the property of Elsevier B.V. and its content may not be copied or emailed to multiple sites without the copyright holder's express written permission. Additionally, content may not be used with any artificial intelligence tools or machine learning technologies. However, users may print, download, or email articles for individual use. This abstract may be abridged. No warranty is given about the accuracy of the copy. Users should refer to the original published version of the material for the full abstract. (Copyright applies to all Abstracts.)
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  Data: Design strategy for devices under high radiation field in J-PARC muon facility
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  Data: <searchLink fieldCode="AR" term="%22Kawamura%2C+Naritoshi%22">Kawamura, Naritoshi</searchLink><i> nari.kawamura@kek.jp</i><br /><searchLink fieldCode="AR" term="%22Makimura%2C+Shunsuke%22">Makimura, Shunsuke</searchLink><relatesTo>1</relatesTo><br /><searchLink fieldCode="AR" term="%22Strasser%2C+Patrick%22">Strasser, Patrick</searchLink><relatesTo>1</relatesTo><br /><searchLink fieldCode="AR" term="%22Koda%2C+Akihiro%22">Koda, Akihiro</searchLink><relatesTo>1</relatesTo><br /><searchLink fieldCode="AR" term="%22Fujimori%2C+Hiroshi%22">Fujimori, Hiroshi</searchLink><relatesTo>1</relatesTo><br /><searchLink fieldCode="AR" term="%22Nishiyama%2C+Kusuo%22">Nishiyama, Kusuo</searchLink><relatesTo>1</relatesTo><br /><searchLink fieldCode="AR" term="%22Miyake%2C+Yasuhiro%22">Miyake, Yasuhiro</searchLink><relatesTo>1</relatesTo><br /><searchLink fieldCode="AR" term="%22Muon+section%2C+M%2EL%2EF%22">Muon section, M.L.F</searchLink><relatesTo>1</relatesTo>
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  Data: <searchLink fieldCode="JN" term="%22Nuclear+Instruments+%26+Methods+in+Physics+Research+Section+A%22">Nuclear Instruments & Methods in Physics Research Section A</searchLink>. Feb2009, Vol. 600 Issue 1, p114-116. 3p.
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  Data: <searchLink fieldCode="DE" term="%22Radiation+shielding+for+proton+accelerators%22">Radiation shielding for proton accelerators</searchLink><br /><searchLink fieldCode="DE" term="%22Nuclear+facilities%22">Nuclear facilities</searchLink><br /><searchLink fieldCode="DE" term="%22Monte+Carlo+method%22">Monte Carlo method</searchLink><br /><searchLink fieldCode="DE" term="%22Spallation+%28Nuclear+physics%29%22">Spallation (Nuclear physics)</searchLink><br /><searchLink fieldCode="DE" term="%22Muons%22">Muons</searchLink>
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  Data: Abstract: The intensity of proton accelerator has attained the order of mega-watt, and several MW-class proton accelerators have started operating in the world. In comparison with the other MW-class accelerators, Japan Proton Accelerator Research Complex (J-PARC) is unique due to the muon facility. Materials and Life Science Facility, J-PARC, has not only the mercury target but also the graphite target to provide spallation neutrons and muons, respectively. The muon target is inserted upstream of the neutron target in the proton beam line. Full use of several mutually linking Monte-Carlo codes enables the design work of devices in the muon facility, which has to be operated under high radiation field from the muon target. [Copyright &y& Elsevier]
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  Data: <i>Copyright of Nuclear Instruments & Methods in Physics Research Section A is the property of Elsevier B.V. and its content may not be copied or emailed to multiple sites without the copyright holder's express written permission. Additionally, content may not be used with any artificial intelligence tools or machine learning technologies. However, users may print, download, or email articles for individual use. This abstract may be abridged. No warranty is given about the accuracy of the copy. Users should refer to the original published version of the material for the full abstract.</i> (Copyright applies to all Abstracts.)
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        Value: 10.1016/j.nima.2008.11.073
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      – SubjectFull: Nuclear facilities
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      – SubjectFull: Monte Carlo method
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      – SubjectFull: Spallation (Nuclear physics)
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      – SubjectFull: Muons
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      – SubjectFull: Tōkai Region (Japan)
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              Text: Feb2009
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