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Stress contribution of B2 phase in Al$$_{0.7}$$CoCrFeNi eutectic high entropy alloy

Yun, D.*; Chae, H.*; Lee, T.*; Lee, D.-H.*; Ryu, H. J.*; Banerjee, R.*; Harjo, S.; 川崎 卓郎; Lee, S. Y.*

Journal of Alloys and Compounds, 918, p.165673_1 - 165673_7, 2022/10


In this study, the deformation behavior and strengthening contribution of the FCC phase and B2 phase in Al$$_{0.7}$$CoCrFeNi eutectic high entropy alloys (HEAs) were investigated using in-situ neutron diffraction. An FCC matrix phase exhibited a slip-dominant deformation scheme, while twinning hardly contributed to deformation. Applied macroscopic stresses were rarely redistributed to the BCC A2 phase dispersed within the B2 phase, whereas the stress contribution of the B2 phase, which was initially lower than that of the FCC phase, increased significantly with an increase in plastic strain; hence, its contribution to tensile deformation became predominant. This study allows us to postulate a target value of each phase by microstructural tunning to achieve the desired properties of multicomponent phase HEAs.


Square and rhombic lattices of magnetic skyrmions in a centrosymmetric binary compound

高木 里奈*; 松山 直文*; Ukleev, V.*; Yu, L.*; White, J. S.*; Francoual, S.*; Mardegan, J. R. L.*; 速水 賢*; 齋藤 開*; 金子 耕士; et al.

Nature Communications (Internet), 13(1), p.1472_1 - 1472_7, 2022/03

 被引用回数:5 パーセンタイル:93.91(Multidisciplinary Sciences)

Magnetic skyrmions are topologically stable swirling spin textures with particle-like character, and have been intensively studied as a candidate of high-density information bit. While magnetic skyrmions were originally discovered in noncentrosymmetric systems, recently a nanometric skyrmion lattice has also been reported for centrosymmetric rare-earth compounds. For the latter systems, a novel skyrmion formation mechanism mediated by itinerant electrons has been proposed, and the search of a simpler model system allowing for a better understanding of their intricate magnetic phase diagram is highly demanded. Here, we report the discovery of square and rhombic lattices of nanometric skyrmions in a centrosymmetric binary compound EuAl$$_4$$, by performing small-angle neutron and resonant elastic X-ray scattering experiments. Unlike previously reported centrosymmetric skyrmion-hosting materials, EuAl$$_4$$ shows multiple-step reorientation of the fundamental magnetic modulation vector as a function of magnetic field, probably reflecting a delicate balance of associated itinerant-electron-mediated interactions. The present results demonstrate that a variety of distinctive skyrmion orders can be derived even in a simple centrosymmetric binary compound, which highlights rare-earth intermetallic systems as a promising platform to realize/control the competition of multiple topological magnetic phases in a single material.


Gapless spin liquid in a square-kagome lattice antiferromagnet

藤原 理賀*; 森田 克洋*; Mole, R.*; 満田 節生*; 遠山 貴巳*; 矢野 真一郎*; Yu, D.*; 曽田 繁利*; 桑井 智彦*; 幸田 章宏*; et al.

Nature Communications (Internet), 11(1), p.3429_1 - 3429_7, 2020/07

 被引用回数:14 パーセンタイル:85.72(Multidisciplinary Sciences)

Observation of a quantum spin liquid (QSL) state is one of the most important goals in condensed-matter physics, as well as the development of new spintronic devices that support next-generation industries. The QSL in two-dimensional quantum spin systems is expected to be due to geometrical magnetic frustration, and thus a kagome-based lattice is the most probable playground for QSL. Here, we report the first experimental results of the QSL state on a square-kagome quantum antiferromagnet, KCu$$_6$$AlBiO$$_4$$(SO$$_4$$)$$_5$$Cl. Comprehensive experimental studies via magnetic susceptibility, magnetisation, heat capacity, muon spin relaxation, and inelastic neutron scattering measurements reveal the formation of a gapless QSL at very low temperatures close to the ground state. The QSL behavior cannot be explained fully by a frustrated Heisenberg model with nearest-neighbor exchange interactions, providing a theoretical challenge to unveil the nature of the QSL state.


Colossal barocaloric effects in plastic crystals

Li, B.*; 川北 至信; 河村 聖子; 菅原 武*; Wang, H.*; Wang, J.*; Chen, Y.*; 河口 沙織*; 河口 彰吾*; 尾原 幸治*; et al.

Nature, 567(7749), p.506 - 510, 2019/03

 被引用回数:135 パーセンタイル:99.3(Multidisciplinary Sciences)



Liquid-like thermal conduction in intercalated layered crystalline solids

Li, B.; Wang, H.*; 川北 至信; Zhang, Q.*; Feygenson, M.*; Yu, H. L.*; Wu, D.*; 尾原 幸治*; 菊地 龍弥*; 柴田 薫; et al.

Nature Materials, 17(3), p.226 - 230, 2018/03

 被引用回数:86 パーセンタイル:96.84(Chemistry, Physical)

As a generic property, all substances transfer heat through microscopic collisions of constituent particles. A solid conducts heat through both transverse and longitudinal acoustic phonons, but a liquid employs only longitudinal vibrations. As a result, a solid is usually thermally more conductive than a liquid. In canonical viewpoints, such a difference also serves as the dynamic signature distinguishing a solid from a liquid. Here, we report liquid-like thermal conduction observed in the crystalline AgCrSe$$_{2}$$. The transverse acoustic phonons are completely suppressed by the ultrafast dynamic disorder while the longitudinal acoustic phonons are strongly scattered but survive, and are thus responsible for the intrinsically ultralow thermal conductivity. This scenario is applicable to a wide variety of layered compounds with heavy intercalants in the van der Waals gaps, manifesting a broad implication on suppressing thermal conduction. These microscopic insights might reshape the fundamental understanding on thermal transport properties of matter and open up a general opportunity to optimize performances of thermoelectrics.


Melting of Pb charge glass and simultaneous Pb-Cr charge transfer in PbCrO$$_{3}$$ as the origin of volume collapse

Yu, R.*; 北條 元*; 綿貫 徹; 水牧 仁一朗*; 溝川 貴司*; 岡 研吾*; Kim, H.*; 町田 晃彦; 榊 浩司*; 中村 優美子*; et al.

Journal of the American Chemical Society, 137(39), p.12719 - 12728, 2015/10

 被引用回数:28 パーセンタイル:69.07(Chemistry, Multidisciplinary)



New PbTiO$$_{3}$$-type giant tetragonal compound Bi$$_{2}$$ZnVO$$_{6}$$ and its stability under pressure

Yu, R.*; 北條 元*; 岡 研吾*; 綿貫 徹; 町田 晃彦; 清水 啓佑*; 中野 紀穂*; 東 正樹*

Chemistry of Materials, 27(6), p.2012 - 2017, 2015/03

 被引用回数:24 パーセンタイル:65.31(Chemistry, Physical)



Origin of dramatic oxygen solute strengthening effect in titanium

Yu, Q.*; Qi, L.*; 都留 智仁; Traylor, R.*; Rugg, D.*; Morris, J. W. Jr.*; Asta, M.*; Chrzan, D. C.*; Minor, A. M.*

Science, 347(6222), p.635 - 639, 2015/02

 被引用回数:182 パーセンタイル:98.07(Multidisciplinary Sciences)



Development of a GEM-TPC for H-dibaryon search experiment at J-PARC

佐甲 博之; Ahn, J. K.*; Baek, K. H.*; Bassalleck, B.*; Fujioka, H.*; Guo, L.*; 長谷川 勝一; Hicks, K.*; Honda, R.*; Hwang, S. H.*; et al.

Journal of Instrumentation (Internet), 9(4), p.C04009_1 - C04009_10, 2014/04

 被引用回数:3 パーセンタイル:17.73(Instruments & Instrumentation)

($$K^+$$,$$K^-$$)反応によるHダイバリオン探索実験(J-PARC E42)のためのTPCの開発を行っている。TPCにおいてHが2個の$$pi^{-}$$と2個の$$p$$に崩壊する事象を測定する。TPCのドリフト体積は50cm直径、55cmドリフト長を持つ8角柱構造をしておりAr-CH$$_4$$ガスを使用する。増幅部には3層のGEMを使用する。荷電粒子の運動量測定のためTPCにはドリフト電場と平行に鉛直方向の1Tの双極磁場を超伝導ヘルムホルツ型磁石によりかける。H崩壊のアクセプタンスを最大にするためダイアモンド標的がTPC内部の筒状の穴に設置される。さらに、超高レートの$$K^-$$ビームをTPCに直接照射するため陽イオンフィードバックを極力抑制必要がある。このためTPCにGEMとgating gridを採用した。


Diluted ferromagnetic semiconductor Li(Zn,Mn)P with decoupled charge and spin doping

Deng, Z.*; Zhao, K.*; Gu, B.; Han, W.*; Zhu, J. L.*; Wang, X. C.*; Li, X.*; Liu, Q. Q.*; Yu, R. C.*; 後神 達郎*; et al.

Physical Review B, 88(8), p.081203_1 - 081203_5, 2013/08

 被引用回数:69 パーセンタイル:92.57(Materials Science, Multidisciplinary)

We report the discovery of a diluted magnetic semiconductor, Li(Zn,Mn)P, in which charge and spin are introduced independently via lithium off-stoichiometry and the isovalent substitution of Mn$$^{2+}$$ for Zn$$^{2+}$$, respectively. Isostructural to (Ga,Mn)As, Li(Zn,Mn)P was found to be a ${it p}$-type ferromagnetic semiconductor with excess lithium providing charge doping. First-principles calculations indicate that excess Li is favored to partially occupy the Zn site, leading to hole doping. Ferromagnetism with Curie temperature up to 34 K is achieved while the system still shows semiconducting transport behavior.


Benchmarking of mechanical test facilities related to ITER CICC steel jackets

Vostner, A.*; Pong, I.*; Bessette, D.*; Devred, A.*; Sgobba, S.*; Jung, A.*; Weiss, K.-P.*; Jewell, M. C.*; Liu, S.*; Yu, W.*; et al.

IEEE Transactions on Applied Superconductivity, 23(3), p.9500705_1 - 9500705_5, 2013/06

 被引用回数:11 パーセンタイル:53.27(Engineering, Electrical & Electronic)



Test results of ITER conductors in the SULTAN facility

Bruzzone, P.*; Stepanov, B.*; Wesche, R.*; Mitchell, N.*; Devred, A.*; 布谷 嘉彦; Tronza, V.*; Kim, K.*; Boutboul, T.*; Martovetsky, N.*; et al.

Proceedings of 24th IAEA Fusion Energy Conference (FEC 2012) (CD-ROM), 8 Pages, 2013/03



Positron annihilation study of 4H-SiC by Ge$$^+$$ implantation and subsequent thermal annealing

Yu, R. S.*; 前川 雅樹; 河裾 厚男; Wang, B. Y.*; Wei, L.*

Nuclear Instruments and Methods in Physics Research B, 270, p.47 - 49, 2012/01

 被引用回数:5 パーセンタイル:40.95(Instruments & Instrumentation)

Positron annihilation in 800 keV Ge$$^+$$ implanted hexagonal SiC was studied by thermal annealing at temperatures ranging from 800 to 1400 $$^{circ}$$C. The variation in Doppler broadening $$S$$ values as a function of the incident positron energy suggests a broad distribution in the depth of vacancy defects in the implanted samples. Increasing the annealing temperature triggers the accumulation of vacancies into vacancy clusters. After annealing at 1400 $$^{circ}$$C, defects in the deep region of SiC are eliminated, and Ge precipitation is believed to appear in the sample at the same time. Though Ge has a much more negative positron affinity than SiC, positron annihilation coincidence Doppler broadening measurement reveals that a preferential trapping of positrons in Ge seems impossible.


Li(Zn,Mn)As as a new generation ferromagnet based on a I-II-V semiconductor

Deng, Z.*; Jin, C. Q.*; Liu, Q. Q.*; Wang, X. C.*; Zhu, J. L.*; Feng, S. M.*; Chen, L. C.*; Yu, R. C.*; Arguello, C.*; 後神 達郎*; et al.

Nature Communications (Internet), 2, p.1425_1 - 1425_5, 2011/08

 被引用回数:142 パーセンタイル:93.78(Multidisciplinary Sciences)



Validation of on- and off-axis neutral beam current drive against experiment in DIII-D

Park, J. M.*; 村上 和功*; Petty, C. C.*; Heidbrink, W. W.*; Osborne, T. H.*; Holcomb, C. T.*; Van Zeeland, M. A.*; Prater, R.*; Luce, T. C.*; Wade, M. R.*; et al.

Physics of Plasmas, 16(9), p.092508_1 - 092508_10, 2009/09

 被引用回数:20 パーセンタイル:62.73(Physics, Fluids & Plasmas)

DIII-Dにおいてプラズマを垂直方向に変位させることで、プラズマ周辺部(off-axis)での中性粒子ビーム電流駆動(NBCD)を実証した。モーショナルシュタルク効果計測により測定した磁力線ピッチ角の時間変化からポロイダル磁束の時間変化を評価し、小半径の半分程度にピークを持ち空間的に広がったoff-axis NBCD分布を示す結果を得た。多くの場合、測定したoff-axis NBCD分布は有限軌道効果を考慮した軌道追跡モンテカルロコードによる高速イオンの減速計算によるものと一致する。中性化した高速イオンが発するD$$alpha$$光の2次元イメージング計測によるとビームイオン密度分布は凹状になっており古典的な減速の描像と一致する。NB駆動電流の大きさはビームと磁力線のなす角と関係しており、両者のなす角が小さくなるように選ぶことでoff-axis NBCDの効率は中心部(on-axis)NBCDと同程度によくすることができる。測定したoff-axis NBCDは入射パワーとともに増加するが、高パワーにおいて測定と計算が合うためには計算に適度な高速イオン拡散を入れる必要がある。


Off-axis neutral beam current drive for advanced scenario development in DIII-D

村上 和功*; Park, J. M.*; Petty, C. C.*; Luce, T. C.*; Heidbrink, W. W.*; Osborne, T. H.*; Prater, R.*; Wade, M. R.*; Anderson, P. M.*; Austin, M. E.*; et al.

Nuclear Fusion, 49(6), p.065031_1 - 065031_8, 2009/06

 被引用回数:40 パーセンタイル:83.22(Physics, Fluids & Plasmas)



New method to measure the rise time of a fast pulse slicer for laser ion acceleration research

森 道昭; 余語 覚文; 桐山 博光; 西内 満美子; 小倉 浩一; 織茂 聡; Ma, J.*; 匂坂 明人; 金沢 修平; 近藤 修司; et al.

IEEE Transactions on Plasma Science, 36(4), p.1872 - 1877, 2008/08

 被引用回数:7 パーセンタイル:29.91(Physics, Fluids & Plasmas)



Positron microscopic analysis of crack failure in stainless steels

Yu, R.; 前川 雅樹; 三輪 幸夫; 平出 哲也; 西村 昭彦; 河裾 厚男

Physica Status Solidi (C), 4(10), p.3577 - 3580, 2007/09

 被引用回数:4 パーセンタイル:74.4



Design of a positron microprobe using magnetic lenses

前川 雅樹; Yu, R.; 河裾 厚男

Physica Status Solidi (C), 4(10), p.4016 - 4019, 2007/09

 被引用回数:4 パーセンタイル:74.4



Characterization of ion beam-induced SiC-OI structures by positron annihilation spectroscopy

前川 雅樹; Yu, R.; 河裾 厚男

Physica Status Solidi (C), 4(10), p.3680 - 3683, 2007/09

 被引用回数:0 パーセンタイル:0.07

陽電子消滅法を用い、イオン注入法によって作成した埋め込み酸化膜層を有する炭化ケイ素(SiC)基板の評価を行った。試料は200keVの酸素イオンをSiCに打ち込み作成した。注入量は1$$times$$10$$^{18}$$cm$$^{-2}$$とした。注入時の照射損傷の残留を避け酸素イオンの反応を促すために、照射温度を変化させて注入した。注入後、1400$$^{circ}$$Cまでの熱アニールを行った。室温注入時には現れなかった酸素打ち込み領域におけるSパラメータ変化は、600$$^{circ}$$C, 800$$^{circ}$$Cと高温になるにつれ明瞭になった。これは注入酸素が反応し、SiO$$_2$$が形成していることを示していると思われる。しかしながら陽電子寿命は石英から期待されるSiO$$_2$$の値よりも短くなった。また運動量分布を詳細に測定したところ、この領域の結晶構造はSiO$$_2$$に至る前の不完全酸化状態にあることがわかり、十分な品質を保持していないことが示唆された。表層SiC層に関してはマイクロボイドのような欠陥が生成し、熱アニールによっても除去できないことがわかった。高品質な埋め込み酸化膜を有するSiC基板の作成のためには、従来法よりもより効果的な処理手法が必要であると思われる。

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