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Si and DyCuSiMitsumoto, Keisuke*; Goto, Saori*; Nemoto, Yuichi*; Akatsu, Mitsuhiro*; Goto, Terutaka*; Dung, N. D.*; Matsuda, Tatsuma; Haga, Yoshinori; Takeuchi, Tetsuya*; Sugiyama, Kiyohiro*; et al.
Journal of Physics; Condensed Matter, 25(29), p.296002_1 - 296002_8, 2013/07
Times Cited Count：3 Percentile：13.63(Physics, Condensed Matter)Choi, I. W.*; Kim, C. M.*; Sung, J. H.*; Yu, T. J.*; Lee, S. K.*; Kim, I. J.*; Jin, Y.-Y.*; Jeong, T. M.*; Hafz, N.*; Pae, K. H.*; et al.
Review of Scientific Instruments, 80(5), p.053302_1 - 053302_10, 2009/05
Times Cited Count：24 Percentile：66.06(Instruments & Instrumentation)Nishiuchi, Mamiko; Daido, Hiroyuki; Yogo, Akifumi; Orimo, Satoshi; Ogura, Koichi; Ma, J.-L.; Sagisaka, Akito; Mori, Michiaki; Pirozhkov, A. S.; Kiriyama, Hiromitsu; et al.
Physics of Plasmas, 15(5), p.053104_1 - 053104_10, 2008/05
Times Cited Count：47 Percentile：82.85(Physics, Fluids & Plasmas)High-flux energetic protons whose maximum energies are up to 4 MeV are generated by an intense femtosecond Titanium Sapphire laser pulse interacting with a 7.5, 12.5, and 25
m thick Polyimide tape targets. The laser pulse energy is 1.7 J, duration is 34 fs, and intensity is 3
10
Wcm
. The amplified spontaneous emission (ASE) has the intensity contrast ratio of 410
. The conversion efficiency from laser energy into proton kinetic energies of 
3% is achieved, which is comparable or even higher than those achieved in the previous works with nanometer-thick targets and the ultrahigh contrast laser pulses (10
).
Saido, Masahiro; Fukuda, Mitsuhiro; Arakawa, Kazuo; Tajima, Satoshi; Sunaga, Hiromi; Yotsumoto, Keiichi; Kamiya, Tomihiro; Tanaka, Ryuichi; Hirao, Toshio; Nashiyama, Isamu; et al.
Proceedings of 1999 IEEE Nuclear and Space Radiation Effects Conference, p.117 - 122, 1999/00
no abstracts in English
Hirao, Toshio; ; ; Nashiyama, Isamu; Matsuda, Sumio*; Nemoto, N.*; Onishi, K.*
SDM97-194, p.57 - 63, 1998/02
no abstracts in English
Nemoto, N.*; Shindo, Hiroyuki*; ; Kuboyama, Satoshi*; Oshima, Takeshi; Ito, Hisayoshi; Nashiyama, Isamu; Matsuda, Sumio*
Proceedings of 3rd International Workshop on Radiation Effects on Semiconductor Devices for Space Application, p.154 - 159, 1998/00
no abstracts in English
Yoshikawa, Masahito; Nemoto, N.*; Ito, Hisayoshi; Okumura, Hajime*; ; Yoshida, Sadafumi*; Nashiyama, Isamu
Mater. Sci. Eng., B, 47(3), p.218 - 223, 1997/00
Times Cited Count：1 Percentile：11.35(Materials Science, Multidisciplinary)no abstracts in English
Hirakawa, N.*; Mukaiyama, T.*; Shirakata, K.*; Nemoto, S.*; Hirota, J.*; Matsuno, Y.*; Konishi, T.*
PNC TJ250 70-36T, 69 Pages, 1970/07
The FCA assembly V-1 achieved the first criticality on 28th Feb-ruary, 1970. The assembly V-1 is the first physics mockup of a seriesof assemblies on which the mockup experiments for the JOYO (Japan Ex-perimental Fast Reactor) are programmed. The composition of the corematerial was determined so that the neutron spectrum at the center ofthe core represents the JOYO spectrum as exactly as possible. Atten-tion was payed in the experiment especially on the effects of spontane-ous fission of Pu-240 and -heating of plutonium fuel,because thisis the first experience for plutonium loading in FCA. The critical mass 64.7 0.3kg (Pu-239+Pu-240) and 118.20.6kg (U-235) was experimentally determined after performance ofcorrection experiments on the assembly V-1-B that was established byremoving the hole for the external neutron source. The measured criti-cal mass was compared with the results of one-and two-dimensionaldiffusion calculations and one-dimensional S4 calculation. Diffusioncalculation usi
MeV proton beamNishiuchi, Mamiko; Daito, Izuru; Ikegami, Masahiro; Mori, Michiaki; Orimo, Satoshi; Ogura, Koichi; Sagisaka, Akito; Yogo, Akifumi; Pirozhkov, A. S.; Ma, J.*; et al.
no journal, ,
A laser-driven proton beam with a maximum energy of a few MeV is stably obtained using an ultra-short and high-intensity Titanium Sapphire laser. As compared with the proton beam from the conventional accelerator, this proton beam exhibits peculiar characteristics, such as, more than 10
protons per bunch are produced within a short pulse duration of ps at a source, resulting in a very high peak current. It also exhibits a very low transverse emittance. The proton beam has a divergence angle of 10 degrees and energy spread of 100%. It accompanies electrons and X-rays, which is produced simultaneously. Making the best use of these peculiar characteristics, many possible applications of the laser-driven proton are proposed. In order to make practical laser-driven proton beam for the applications, we carry out series of experiments. We have successfully obtained simultaneous imaging of the target with proton and X-ray or proton and electron beams. In the course of practical use of the proton beam for specific applications, characteristics above should be optimized based on the variations of the applications. For example, in order to apply the laser-driven proton beam for the proton irradiation system, such as used in the medical or the industrial applications, we should obtain focused or parallel proton beam. One of our plans to alter the orbits of the laser-driven protons from the planer tape target is using permanent quadrupole magnets.
Sagisaka, Akito; Pirozhkov, A. S.; Daido, Hiroyuki; Ogura, Koichi; Orimo, Satoshi; Yogo, Akifumi; Daito, Izuru; Nishiuchi, Mamiko; Mori, Michiaki; Nashima, Shigeki*; et al.
no journal, ,
no abstracts in English
Nishiuchi, Mamiko; Daido, Hiroyuki; Yogo, Akifumi; Orimo, Satoshi; Ogura, Koichi; Ma, J.-L.; Sagisaka, Akito; Mori, Michiaki; Pirozhkov, A. S.; Kiriyama, Hiromitsu; et al.
no journal, ,
The efficient proton beam whose maximum energy of up to 4 MeV was produced by the 50TW short pulse intensity Ti:Sap laser irradiated on the polyimide target [(C
H
O
N
)n] with the thicknesses of 7.5m, 12.5m, 25m, which is transparent to the 800 nm laser. The laser parameters are energy of 1.7J, pulse width of 35fs and the intensity of 310 Wcm. The contrast of the ASE component is 410. The conversion efficiency from laser energy into the proton kinetic energy is up to 3%. This conversion efficiency is comparable or even higher than the results obtained with the same level laser ( J energy) interacts with the nano-meter level ultra thin target. In this paper we discuss on the comparison between our results and other experimental results obtained in other facilities.
