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Kosugi, Mioko*; Kikkawa, Takashi; Saito, Eiji; 10 of others*
ACS Applied Materials & Interfaces, 16(46), p.64190 - 64196, 2024/11
Times Cited Count：0 Percentile：0.00(Nanoscience & Nanotechnology)Kiliyankil, V. A.*; Fukutani, Katsuyuki; 10 of others*
Journal of Materials Chemistry A, 12(42), p.28731 - 28743, 2024/10
Times Cited Count：0 Percentile：0.00(Chemistry, Physical)
= 82 shell closureZhang, W. Q.*; Andreyev, A. N.; 10 of others*
Physical Review C, 110(4), p.044301_1 - 044301_7, 2024/10
Times Cited Count：0 Percentile：0.00(Physics, Nuclear)
Mo, 
Mo, and 
MoKumar, V.*; Chapman, R.*; Ollier, J.*; Orlandi, R.; Smith, J. F.*; Spohr, K.-M.*; Torres, D. A.*; Wady, P.*; 10 of others*
Physical Review C, 110(4), p.044308_1 - 044308_18, 2024/10
Times Cited Count：0 Percentile：0.00(Physics, Nuclear)
U and 
ThFilipescu, D.*; Gheorghe, I.*; Goriely, S.*; Nishio, Katsuhisa; Utsunomiya, Hiroaki*; Suzaki, Fumi; Hirose, Kentaro; 10 of others*
Physical Review C, 109(4), p.044602_1 - 044602_23, 2024/04
Times Cited Count：2 Percentile：84.76(Physics, Nuclear)Ahn, J. K.*; Hasegawa, Shoichi; Imai, Kenichi*; Sako, Hiroyuki; Sato, Susumu; Tanida, Kiyoshi; 10 of others*
Nuclear Instruments and Methods in Physics Research A, 1047, p.167775_1 - 167775_13, 2023/02
Times Cited Count：1 Percentile：0.00(Instruments & Instrumentation)
nuclear modification at backward and forward rapidity in 
, Al, and Au collisions at 
GeVAcharya, U. A.*; Hasegawa, Shoichi; Imai, Kenichi*; Sako, Hiroyuki; Sato, Susumu; Tanida, Kiyoshi; PHENIX Collaboration*; 310 of others*
Physical Review C, 105(6), p.064912_1 - 064912_15, 2022/06
Times Cited Count：14 Percentile：88.43(Physics, Nuclear)Oset, E.*; 10 of others*; Oka, Makoto
Acta Physica Polonica B, 47(2), p.357 - 365, 2016/02
Times Cited Count：3 Percentile：26.07(Physics, Multidisciplinary)We review results from studies with unconventional many-hadron systems containing mesons: systems with two mesons and one baryon, three mesons, some novel systems with two baryons and one meson, and finally, systems with many vector mesons, up to six, with their spins aligned forming states of increasing spin. We show that in many cases, one has experimental counterparts for the states found, while in some other cases, they remain as predictions, which we suggest to be searched in BESIII, Belle, LHCb, FAIR and other facilities.
Thalmeier, R.*; Tanida, Kiyoshi; 102 of others*
Journal of Instrumentation (Internet), 11(1), p.C01044_1 - C01044_10, 2016/01
Times Cited Count：2 Percentile：10.25(Instruments & Instrumentation)Tsuru, Tomohito; Lobzenko, I.; Shiihara, Yoshinori*; Wei, D.*; Yamashita, Shinichiro; Itakura, Mitsuhiro; 10 of others*
no journal, ,
High entropy alloys (HEAs) are chemically complex single- or multi-phase alloys with crystal structures. There are no major components but five or more elements are included with near equiatomic fraction. In such a situation, deformation behavior can no longer be described by conventional solid solution strengthening model. Some HEAs, indeed, show higher strengthening behavior and anomalous slip. However, the mechanisms of these features have yet to be understood. Dislocation structure and motion should be the key to identify the unique feature of mechanical properties of HEAs. In the present study, we investigated the core structure of dislocations in body centered cubic (BCC) HEAs using density functional theory (DFT) calculations. The Random structure and ZrNbTaTiHf and the SRO structure obtained from the 800 K MC calculation in two BCC-HEA MoNbTaVW was prepared. Then, the energy distribution when the dislocation dipoles were introduced at 135 sites were calculated. We found that the dislocation formation energy is smaller in ZrNbTaTiHf, which has a large difference in MSAD and a large lattice distortion.
