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Journal Articles

sparse-ir; Optimal compression and sparse sampling of many-body propagators

Wallerberger, M.*; Badr, S.*; Hoshino, Shintaro*; Huber, S.*; Kakizawa, Fumiya*; Koretsune, Takashi*; Nagai, Yuki; Nogaki, Kosuke*; Nomoto, Takuya*; Mori, Hitoshi*; et al.

Software X (Internet), 21, p.101266_1 - 101266_7, 2023/02

 Times Cited Count:10 Percentile:88.45(Computer Science, Software Engineering)

no abstracts in English

Journal Articles

Erosion of $$N$$=20 shell in $$^{33}$$Al investigated through the ground-state electric quadrupole moment

Shimada, Kenji*; Ueno, Hideki*; Neyens, G.*; Asahi, Koichiro*; Balabanski, D. L.*; Daugas, J. M.*; Depuydt, M.*; De Rydt, M.*; Gaudefroy, L.*; Gr$'e$vy, S.*; et al.

Physics Letters B, 714(2-5), p.246 - 250, 2012/08

 Times Cited Count:7 Percentile:41.35(Astronomy & Astrophysics)

no abstracts in English

Journal Articles

Precision measurement of the electric quadrupole moment of $$^{31}$$Al and determination of the effective proton charge in the sd-shell

De Rydt, M.*; Neyens, G.*; Asahi, Koichiro*; Balabanski, D. L.*; Daugas, J. M.*; Depuydt, M.*; Gaudefroy, L.*; Gr$'e$vy, S.*; Hasama, Yuka*; Ichikawa, Yuichi*; et al.

Physics Letters B, 678(4), p.344 - 349, 2009/07

 Times Cited Count:17 Percentile:69.95(Astronomy & Astrophysics)

no abstracts in English

Journal Articles

Status of extened performance tests for blanket remote maintenance in the ITER L6 project

Kakudate, Satoshi; Oka, Kiyoshi; Yoshimi, Takashi*; Hiyama, Masayuki; Taguchi, Ko*; Shibanuma, Kiyoshi; Koizumi, Koichi; Matsumoto, Yasuhiro*; Honda, Tsutomu*; Haange, R.*

Nuclear Fusion, 42(3), p.243 - 246, 2002/03

 Times Cited Count:3 Percentile:10.69(Physics, Fluids & Plasmas)

no abstracts in English

Journal Articles

Development of a control system for a heavy object handling manipulator; Application to a remote maintenance system for ITER blanket module

Yoshimi, Takashi*; Kakudate, Satoshi; Tada, Eisuke; Tsuji, Koichi*; Miyagawa, Shinichi*; Kubo, Tomomi*

Nihon Robotto Gakkai-Shi, 19(6), p.766 - 774, 2001/09

no abstracts in English

Journal Articles

Mechanical characteristics and position control of vehicle/manipulator for ITER blanket remote maintenance

Kakudate, Satoshi; Oka, Kiyoshi; Yoshimi, Takashi*; Taguchi, Ko*; Nakahira, Masataka; Takeda, Nobukazu; Shibanuma, Kiyoshi; Obara, Kenjiro; Tada, Eisuke; Matsumoto, Yasuhiro*; et al.

Fusion Engineering and Design, 51-52(1-4), p.993 - 999, 2000/11

 Times Cited Count:9 Percentile:54.14(Nuclear Science & Technology)

no abstracts in English

Journal Articles

Position measurement method for blanket maintenance

Hiyama, Masayuki; Oka, Kiyoshi; Kakudate, Satoshi; Yoshimi, Takashi*; Shibanuma, Kiyoshi; Koizumi, Koichi

Robotikusu, Mekatoronikusu Koenkai '00 Koen Rombunshu, (2P2-11-008), p.1 - 2, 2000/05

no abstracts in English

Journal Articles

Basic experiments for the mechanically attached blanket module installation by the ITER remote vehicle-type manipulator

Yoshimi, Takashi*; Kakudate, Satoshi; Oka, Kiyoshi; Hiyama, Masayuki; Taguchi, Ko*; Shibanuma, Kiyoshi; Koizumi, Koichi

Robotikusu, Mekatoronikusu Koenkai '00 Koen Rombunshu, (2P2-11-006), p.1 - 2, 2000/05

no abstracts in English

Oral presentation

Electric quadrupole moment measurement using a new RF-application system

Nagae, Daisuke; Takemuara, Makoto*; Ueno, Hideki*; Kameda, Daisuke*; Asahi, Koichiro*; Yoshimi, Akihiro*; Sugimoto, Takashi*; Nagatomo, Takashi*; Kobayashi, Yoshio*; Uchida, Makoto*; et al.

no journal, , 

An electric quadrupole moment ($$Q$$ moment) is sensitive to collective aspects of nuclear structure. In the $$Q$$-moment measurement for unstable nuclei, we employ the $$beta$$-detected nuclear-quadrupole resonance method. In this method, we need to supply $$2I$$ resonance frequencies, where $$I$$ denotes the nuclear spin. We have developed a new RF-application system to induced all of the $$2I$$ transitions. The application of the $$2I$$ frequencies may be pursued in two different ways; the sequential RF pulse method and the mixed-wave RF pulse method. We confirmed the reversal of polarization for the both methods, from measurements of $$beta$$-ray asymmetry change for polarized $$^{12}$$B. Using this system, the $$Q$$ moments of $$^{31,32}$$Al have been measured to be $$|Q(^{31}{rm Al})| = 104(9)$$ $$e$$$$cdot$$mb and $$|Q(^{32}{rm Al})| = 24(2)$$ $$e$$$$cdot$$mb by the sequential RF pulse method.

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