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Naito, Fujio*; Anami, Shozo*; Ikegami, Kiyoshi*; Uota, Masahiko*; Ouchi, Toshikatsu*; Onishi, Takahiro*; Oba, Toshiyuki*; Obina, Takashi*; Kawamura, Masato*; Kumada, Hiroaki*; et al.
Proceedings of 13th Annual Meeting of Particle Accelerator Society of Japan (Internet), p.1244 - 1246, 2016/11
The proton linac installed in the Ibaraki Neutron Medical Research Center is used for production of the intense neutron flux for the Boron Neutron Capture Therapy (BNCT). The linac consists of the 3-MeV RFQ and the 8-MeV DTL. Design average beam current is 10mA. Target is made of Beryllium. First neutron production from the Beryllium target was observed at the end of 2015 with the low intensity beam as a demonstration. After the observation of neutron production, a lot of improvement s was carried out in order to increase the proton beam intensity for the real beam commissioning. The beam commissioning has been started on May 2016. The status of the commissioning is summarized in this report.
Sako, Hiroyuki; Imai, Kenichi; Sato, Susumu; Sugimura, Hitoshi; Miura, Akihiko; Maruta, Tomofumi; Kikuzawa, Nobuhiro
Proceedings of 8th Annual Meeting of Particle Accelerator Society of Japan (Internet), 3 Pages, 2011/08
J-PARC linac has been operated at 7.2 kW since Nov. 2007. The most serious problem from SDTL (Separated-type Drift-Tube Linac) to ACS (Annular-Coupled Structure) sections is how to suppress the highest beam loss due to 
which have been generated by interactions between 
and remnant gas. Although beam loss has been measured with proportional counters, we have not succeeded to estimate absolute amplitude of . We have succeeded to reconstruct proton tracks which are generated from using scintillating fiber hodoscopes which were installed in the ACS section.
Miura, Akihiko; Sako, Hiroyuki; Yamamoto, Kazami; Kikuzawa, Nobuhiro; Maruta, Tomofumi; Sato, Susumu; Imai, Kenichi; Adachi, Satoshi; Sugimura, Hitoshi; Igarashi, Zenei*; et al.
Proceedings of 25th International Linear Accelerator Conference (LINAC 2010) (CD-ROM), p.590 - 592, 2010/09
Ar-CO
gas proportional counters are employed for the measurement of beam loss in the current linac operation, but they are also sensitive to background noise of X-ray emitted from RF cavities. In SDTL section, protons, secondary hadrons and 
rays would be mainly generated as a beam loss, but it is not easy to estimate real beam loss using the proportional counter. The plastic scintillation counters with less X-ray sensitivity and 
He proportional counters with high thermal neutron sensitivity will be also employed to measure the beam loss. This paper reports the signals obtained during the beam operation using the Ar-CO gas proportional counter and the plastic scintillation counter. Finally, a measurement of emission position and angle distributions of protons due to negative hydrogen ion (H
) beam loss is being planed. This plan is introduced and this result would lead to clarify the source of beam loss.
Ogawa, Hiroaki; Ogawa, Toshihide; Tsuzuki, Kazuhiro; Kawashima, Hisato; Kasai, Satoshi*; Kashiwa, Yoshitoshi; Hasegawa, Koichi; Suzuki, Sadaaki; Shibata, Takatoshi; Miura, Yukitoshi; et al.
Fusion Science and Technology, 49(2), p.209 - 224, 2006/02
Times Cited Count：3 Percentile：24.11(Nuclear Science & Technology)no abstracts in English
Shiraiwa, Shunichi*; Ide, Shunsuke; Ito, Satoshi*; Mitarai, Osamu*; Naito, Osamu; Ozeki, Takahisa; Sakamoto, Yoshiteru; Suzuki, Takahiro; Takase, Yuichi*; Tanaka, Shigetoshi*; et al.
Physical Review Letters, 92(3), p.035001_1 - 035001_4, 2004/01
Times Cited Count：46 Percentile：82.94(Physics, Multidisciplinary)no abstracts in English
Ogawa, Toshihide; Ogawa, Hiroaki; Miura, Yukitoshi; Niimi, Hironobu*; Kimura, Haruyuki; Kashiwa, Yoshitoshi; Shibata, Takatoshi; Yamamoto, Masahiro; Fukumoto, Naoyuki*; Nagata, Masayoshi*; et al.
Journal of Nuclear Materials, 290-293, p.454 - 458, 2001/03
Times Cited Count：7 Percentile：48.68(Materials Science, Multidisciplinary)no abstracts in English
Miura, Yukitoshi; *; *; Hoshino, Katsumichi; *; *; Kasai, Satoshi; Kawakami, Tomohide; Kawashima, Hisato; Maeda, M.*; et al.
Fusion Energy 1996, p.167 - 175, 1997/05
no abstracts in English
*; *; *; *; *; *; *; Oikawa, Toshihiro; *; *; et al.
Fusion Energy 1996, p.885 - 890, 1997/05
no abstracts in English
Miura, Akihiko; Nakajima, Masayoshi; Yamashita, Teruo; Sakai, Takaaki; Shiotsuki, Masao; Sato, Akihiro*; Kawahara, Hitoshi*
no journal, ,
no abstracts in English
Nakajima, Masayoshi; Miura, Akihiko; Yamashita, Teruo; Sakai, Takaaki; Shiotsuki, Masao; Kawahara, Hitoshi*; Sato, Akihiro*
no journal, ,
no abstracts in English
Seino, Takeshi*; Miura, Satoshi*; Tamaki, Hitoshi
no journal, ,
no abstracts in English
Ijiri, Yuji*; Shindo, Akihisa*; Miura, Hitoshi*; Kamemura, Katsumi*; Tomoe, Naoto*; Nagai, Norihisa*; Abe, Akimasa*; Fujita, Tomoo; Izumi, Atsushi
no journal, ,
no abstracts in English
Sako, Hiroyuki; Kikuzawa, Nobuhiro; Miura, Akihiko; Maruta, Tomofumi; Adachi, Satoshi; Imai, Kenichi; Sato, Susumu; Sugimura, Hitoshi
no journal, ,
At Annular Coupled Structure linac (ACS) in J-PARC linac, high residual radiation due to beam loss has been observed. Since the beam loss is approximately proportional to the residual gas pressure, the observed beam loss may be caused by the H
's which are generated by the electron stripping by the residual gas. We are going to evaluate beam loss by counting H
's emitted outside the beam duct. We have developed hodoscopes with the sensitive area of 64 mm 
64 mm, which consists of 16 fibers of 4 mm 4 mm 64 mm. Scintillation photons are measured by the multi-anode photo-multipliers. We report beam loss measurements by the hodoscopes.
Ozawa, Yusuke*; Kubota, Hitoshi*; Miura, Kenta*; Hanaizumi, Osamu*; Noguchi, Katsuya*; Sato, Takahiro; Ishii, Yasuyuki; Koka, Masashi; Takano, Katsuyoshi*; Okubo, Takeru; et al.
no journal, ,
