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Takahashi, Hiroki*; Kato, Toru*; Yamashita, Meguru*; Doi, Akio*; Imabuchi, Takashi
Artificial Life and Robotics, 13 Pages, 2026/00
Kato, Toru*; Takahashi, Hiroki*; Yamashita, Meguru*; Doi, Akio*; Imabuchi, Takashi
Artificial Life and Robotics, 30(1), p.126 - 135, 2025/02
Takahashi, Hiroki*; Kato, Toru*; Yamashita, Meguru*; Doi, Akio*; Imabuchi, Takashi
Proceedings of 29th International Symposium on Artificial Life and Robotics (AROB 29th 2024) (Internet), p.1093 - 1096, 2024/01
Kato, Toru*; Takahashi, Hiroki*; Yamashita, Meguru*; Doi, Akio*; Imabuchi, Takashi
Proceedings of 29th International Symposium on Artificial Life and Robotics (AROB 29th 2024) (Internet), p.1097 - 1100, 2024/01
Takasaki, Koji; Yasumune, Takashi; Yamaguchi, Yukako; Hashimoto, Makoto; Maeda, Koji; Kato, Masato
Journal of Nuclear Science and Technology, 60(11), p.1437 - 1446, 2023/11
Times Cited Count:2 Percentile:31.60(Nuclear Science & Technology)The aerodynamic radioactive median diameter (AMAD) is necessary information to assess the internal exposure. On June 6, 2017, at a plutonium handling facility in Oarai site of Japan Atomic Energy Agency (JAEA), during the inspection work of a storage container that contains nuclear fuel materials, accidental contamination occurred and five workers inhaled radioactive materials including plutonium. Some smear papers and an air sampling filter were measured with the imaging plate, and we conservatively estimated minimum AMADs for two cases, plutonium nitrate and plutonium dioxide. As a result of AMAD estimation, even excluding a giant particle of a smear sample, the minimum AMADs of plutonium nitrate from smear papers were 4.3 - 11.3
m and those of plutonium dioxide were 5.6 - 14.1
m. Also, the minimum AMAD of plutonium nitrate from an air sampling filter was 3.0
m and that of plutonium dioxide was 3.9
m.
Abe, Shinichiro; Hashimoto, Masanori*; Liao, W.*; Kato, Takashi*; Asai, Hiroaki*; Shimbo, Kenichi*; Matsuyama, Hideya*; Sato, Tatsuhiko; Kobayashi, Kazutoshi*; Watanabe, Yukinobu*
IEEE Transactions on Nuclear Science, 70(8, Part 1), p.1652 - 1657, 2023/08
Times Cited Count:7 Percentile:79.14(Engineering, Electrical & Electronic)Single event upsets (SEUs) caused by neutrons is a reliability problem for microelectronic devices in the terrestrial environment. Acceleration tests using white neutron beam provide realistic soft error rates (SERs), but only a few facilities can provide white neutron beam in the world. If single-source irradiation applicable to diverse neutron source can be utilized for the evaluation of the SER in the terrestrial environment, it contributes to solve the shortage of beam time. In this study, we investigated the feasibility of the SER estimation in the terrestrial environment by any one of these measured data with the SEU cross sections obtained by PHITS simulation. It was found that the SERs estimated by our proposed method are within a factor of 2.7 of that estimated by the Weibull function. We also investigated the effect of simplification which reduce the computational cost in simulation to the SER estimation.
Ohshima, Hiroyuki; Morishita, Masaki*; Aizawa, Kosuke; Ando, Masanori; Ashida, Takashi; Chikazawa, Yoshitaka; Doda, Norihiro; Enuma, Yasuhiro; Ezure, Toshiki; Fukano, Yoshitaka; et al.
Sodium-cooled Fast Reactors; JSME Series in Thermal and Nuclear Power Generation, Vol.3, 631 Pages, 2022/07
This book is a collection of the past experience of design, construction, and operation of two reactors, the latest knowledge and technology for SFR designs, and the future prospects of SFR development in Japan. It is intended to provide the perspective and the relevant knowledge to enable readers to become more familiar with SFR technology.
Takasaki, Koji; Yasumune, Takashi; Hashimoto, Makoto; Maeda, Koji; Kato, Masato; Yoshizawa, Michio; Momose, Takumaro
JAEA-Review 2019-003, 48 Pages, 2019/03
June 6, 2017, at Plutonium Fuel Research Facility in Oarai Research and Development Center of JAEA, when five workers were inspecting storage containers containing plutonium and uranium, resin bags in a storage container ruptured, and radioactive dust spread. Though they were wearing a half face mask respirator, they inhaled radioactive materials. In the evaluation of the internal exposure dose, the aerodynamic radioactive median diameter (AMAD) is an important parameter. We measured 14 smear samples and a dust filter paper with imaging plates, and estimated the AMAD by image analysis. As a result of estimating the AMAD, from the 14 smear samples, the AMADs are 4.3 to 11
m or more in the case of nitrate plutonium, and the AMADs are 5.6 to 14
m or more in the case of the oxidized plutonium. Also, from the dust filter paper, the AMAD is 3.0
m or more in the case of nitrate plutonium, and the AMAD is 3.9
m or more in the case of the oxidized plutonium.
Abe, Shinichiro; Sato, Tatsuhiko; Kato, Takashi*; Matsuyama, Hideya*
no journal, ,
Radiation-induced charges in semiconductor device cause temporary and non-destructive faults (the so-called soft errors) in microelectronic devices. The model which estimates charges collected in the storage node of a memory element quickly and accurately is necessary to evaluate soft error rate by simulation. In our previous study, it was found that charge collection efficiency in FinFET change with the position and the amount of deposited charge. In this study, we construct the multiple sensitive volume model to estimate collected charge for FinFET. We obtained arbitrary charge deposition events by PHITS and analyzed charge collection of these events for by 3-D TCAD simulator HyENEXSS, the simple sensitive volume model and the multiple sensitive volume model. From the comparisons of the collected charges, it is found that the accuracy of collected charge calculation is improved by considering the variations of charge collection efficiency accompanying the position and the amount of deposited charge.
Doi, Akio*; Yamashita, Meguru*; Takahashi, Hiroki*; Kato, Toru*; Imabuchi, Takashi; Hanari, Toshihide; Tanifuji, Yuta; Ito, Rintaro
no journal, ,
no abstracts in English
Doi, Akio*; Yamashita, Meguru*; Takahashi, Hiroki*; Kato, Toru*; Imabuchi, Takashi; Hanari, Toshihide; Tanifuji, Yuta; Ito, Rintaro
no journal, ,
no abstracts in English
Ashida, Takashi; Takamatsu, Misao; Kawahara, Hirotaka; Maeda, Shigetaka; Maeda, Yukimoto; Hara, Masahide*; Kato, Jungo*
no journal, ,
no abstracts in English
Abe, Shinichiro; Hashimoto, Masanori*; Liao, W.*; Kato, Takashi*; Asai, Hiroaki*; Shimbo, Kenichi*; Matsuyama, Hideya*; Sato, Tatsuhiko; Kobayashi, Kazutoshi*; Watanabe, Yukinobu*
no journal, ,
Single event upset (SEU) induced by secondary cosmic-ray neutrons is one of the causes of non-destructive faults (the so-called soft errors) in microelectronics. We have proposed a method to estimate the terrestrial soft error rates (SERs) based on simulation coupled with one-time neutron irradiation testing which can be applied to various kinds of neutron sources. The validity of our method has been investigated for 65-nm bulk SRAMs with the measured data using various neutron sources. This result will be reviewed on the organized session of the 67th Space Sciences and Technology Conference.
Itagaki, Wataru; Noguchi, Koichi; Endo, Norio; Nakamura, Toshiyuki; Ashida, Takashi; Saito, Takakazu; Someya, Hiroyuki*; Tomine, Hiroshi*; Kato, Jun*; Gunji, Masakatsu*
no journal, ,
no abstracts in English
Abe, Shinichiro; Sato, Tatsuhiko; Kato, Takashi*; Matsuyama, Hideya*
no journal, ,
Radiation-induced charges in semiconductor device cause temporary and non-destructive faults (the so-called soft errors) in microelectronic devices. The model which estimates charges collected in the storage node of a memory element quickly and accurately is necessary to evaluate soft error rate by simulation. It is predicted that charge collection process in FinFET is differs from that in planar process due to differences in their structures. In this study, we perform systematic investigation of charge collection caused by radiation using 3-D TCAD simulator HyENEXSS in order to construct the charge collection model for FinFET. As a result of that investigation, it is found that temporal conduction between source node and drain node arises at few psec. It is also clarified that the temporal conduction has a major impact on charge collection process when charges deposited only near fin. Meanwhile, it is found that diffusion process is the main cause of charge collection when charges deposited in the substrate.
Kato, Yoshinari; Hashimoto, Makoto; Miyauchi, Hideaki; Yasumune, Takashi; Ogawa, Ryuichiro; Goto, Shingo; Ochiai, Yukihiro*; Matsui, Junki
no journal, ,
no abstracts in English
Kato, Toru*; Takahashi, Hiroki*; Yamashita, Meguru*; Doi, Akio*; Imabuchi, Takashi
no journal, ,
Yamashita, Meguru*; Takahashi, Hiroki*; Kato, Toru*; Doi, Akio*; Imabuchi, Takashi
no journal, ,
Takahashi, Hiroki*; Kato, Toru*; Yamashita, Meguru*; Doi, Akio*; Imabuchi, Takashi
no journal, ,
Doi, Akio*; Yamashita, Meguru*; Takahashi, Hiroki*; Kato, Toru*; Imabuchi, Takashi
no journal, ,