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Sato, Hiroshi; Aso, Tomokazu; Kogawa, Hiroyuki; Teshigawara, Makoto; Hino, Ryutaro
JAERI-Tech 2004-018, 23 Pages, 2004/03
The Japan Atomic Energy Research Institute is constructing a mega-watt class spallation neutron source in cooperation with the High Energy Accelerator Research Organization. A cold moderator using liquid hydrogen is one of the key components in the system, which directly affects the neutronic performance both in intensity and pulse time structure. Since a hydrogen temperature rise in the moderator vessel affects the neutronic performance, it is necessary to suppress the recirculation and stagnant regions which would cause hot spots. A cold moderator with a poison plate (poisoned decoupled moderator) has a high possibility to generate the stagnant region on and near the poison plate. Thermal-hydraulic analyses were carried out with proposed inner structure of the poisoned cold moderator. The stagnant and recirculation regions could be reduced by making a gap between the poison plate end and the vessel bottom surface, and the local temperature rise also could be kept under the required design value.
Kobayashi, Kaoru*; Kaminaga, Masanori; Haga, Katsuhiro; Kinoshita, Hidetaka; Aso, Tomokazu; Hino, Ryutaro
JAERI-Review 2002-010, 52 Pages, 2002/05
no abstracts in English
Aso, Tomokazu; Kaminaga, Masanori; Terada, Atsuhiko*; Hino, Ryutaro
Nihon Genshiryoku Gakkai-Shi, 43(11), p.1149 - 1158, 2001/11
Times Cited Count:0 Percentile:0.01(Nuclear Science & Technology)no abstracts in English
Aso, Tomokazu; Kaminaga, Masanori; Terada, Atsuhiko*; Hino, Ryutaro
JAERI-Tech 2001-051, 22 Pages, 2001/08
no abstracts in English
Islam, M. S.*; Terada, Atsuhiko*; Kinoshita, Hidetaka; Hino, Ryutaro; Monde, Masanori*
JAERI-Tech 2001-044, 49 Pages, 2001/07
no abstracts in English
Aso, Tomokazu; Kaminaga, Masanori; Terada, Atsuhiko*; Hino, Ryutaro
JAERI-Conf 2001-002, p.893 - 903, 2001/03
no abstracts in English
Aso, Tomokazu; Kaminaga, Masanori; Terada, Atsuhiko*; Hino, Ryutaro
Kashika Joho Gakkai-Shi, 20(Suppl.2), p.175 - 178, 2000/10
no abstracts in English
Aso, Tomokazu; Kaminaga, Masanori; Terada, Atsuhiko*; Hino, Ryutaro
JAERI-Tech 2000-018, p.49 - 0, 2000/03
no abstracts in English
Aso, Tomokazu; Kaminaga, Masanori; Terada, Atsuhiko*; Ishikura, Shuichi*; Hino, Ryutaro
JAERI-Tech 2000-011, p.23 - 0, 2000/02
no abstracts in English
Aso, Tomokazu; Kaminaga, Masanori; Terada, Atsuhiko; Hino, Ryutaro
JAERI-Tech 99-049, 45 Pages, 1999/06
no abstracts in English
Aso, Tomokazu; Kaminaga, Masanori; Terada, Atsuhiko; Hino, Ryutaro
JAERI-Tech 99-014, 113 Pages, 1999/03
no abstracts in English
Kinoshita, Hidetaka; Kaminaga, Masanori; Hino, Ryutaro
JAERI-Tech 98-061, 55 Pages, 1999/01
no abstracts in English
Aso, Tomokazu; Kaminaga, Masanori; Terada, Atsuhiko*; Hino, Ryutaro
Kashika Joho Gakkai-Shi, 19(Suppl.2), p.127 - 130, 1999/00
no abstracts in English
Kamiya, Tomihiro; Yuto, Hidenori; Tanaka, Ryuichi
Dai-5-Kai Tandemu Kasokuki Oyobi Sono Shuhen Gijutsu No Kenkyukai Hokokushu, p.116 - 119, 1992/07
no abstracts in English
Meigo, Shinichiro; Oi, Motoki; Fujimori, Hiroshi*; Sakamoto, Shinichi*
no journal, ,
Since the damage of the neutron target depends on the beam current density, the beam current density on the target is required to be minimized for the stable operation. Using linear optics, the current density can be reduced by expanding the beamwidth, forbidden by the increase of heat at the vicinities. Because the beam shape cannot be changed from Gaussian by linear optics, a new technique changing the beam shape was required. The beam can be shaped flatly by nonlinear optics using an octupole magnet having a cubic magnetic field. It was known that the beam loss arose by the nonlinear optics. Therefore, a detailed technique is required. Solving the transport calculation exactly, we found that the beam shape can be specified by only two parameters and the optimum parameter to achieve both the flat distribution and the minimized beam loss. From this result, we succeeded in reducing the current density on the target by about 30% compared to the previous case without significant beam loss.
Meigo, Shinichiro
no journal, ,
A high-intensity proton beam transport facility (3NBT) at J-PARC provides the proton beam accelerated at 3 GeV synchrotron accelerator to the neutron source facility and muon facility installed at the Materials and Life Science Experimental Facility (MLF) supplying the secondary beam of neutron and muons to the users. A talk regarding the development of the instruments for high-intensity beam transport, and the beam flattening technology based on nonlinear beam optics will be given at the annual meeting of the Physical Society of Japan,