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Dimensional reduction by geometrical frustration in a cubic antiferromagnet composed of tetrahedral clusters

大熊 隆太郎*; 古府 麻衣子; 浅井 晋一郎*; Avdeev, M.*; 幸田 章宏*; 岡部 博孝*; 平石 雅俊*; 竹下 聡史*; 小嶋 健児*; 門野 良典*; et al.

Nature Communications (Internet), 12(1), p.4382_1 - 4382_7, 2021/07

 被引用回数:0 パーセンタイル:0(Multidisciplinary Sciences)

Dimensionality is a critical factor in determining the properties of solids and is an apparent built- in character of the crystal structure. However, it can be an emergent and tunable property in geometrically frustrated spin systems. Here, we study the spin dynamics of the tetrahedral cluster antiferromagnet, pharmacosiderite, via muon spin resonance and neutron scattering. We find that the spin correlation exhibits a two-dimensional characteristic despite the isotropic connectivity of tetrahedral clusters made of spin 5/2 Fe$$^{3+}$$ ions in the three-dimensional cubic crystal, which we ascribe to two-dimensionalisation by geometrical frustration based on spin wave calculations. Moreover, we suggest that even one-dimensionalisation occurs in the decoupled layers, generating low-energy and one-dimensional excitation modes, causing large spin fluctuation in the classical spin system.


Quantum dynamics of hydrogen in the iron-based superconductor LaFeAsO$$_{0.9}$$D$$_{0.1}$$ measured with inelastic neutron spectroscopy

山浦 淳一*; 平賀 晴弘*; 飯村 壮史*; 村場 善行*; Bang, J.*; 池内 和彦*; 中村 充孝; 稲村 泰弘; 本田 孝志*; 平石 雅俊*; et al.

Physical Review B, 99(22), p.220505_1 - 220505_6, 2019/06


 被引用回数:1 パーセンタイル:10.83(Materials Science, Multidisciplinary)



New precise measurement of muonium hyperfine structure interval at J-PARC

上野 恭裕*; 青木 正治*; 深尾 祥紀*; 東 芳隆*; 樋口 嵩*; 飯沼 裕美*; 池戸 豊*; 石田 啓一*; 伊藤 孝; 岩崎 雅彦*; et al.

Hyperfine Interactions, 238(1), p.14_1 - 14_6, 2017/11

 被引用回数:3 パーセンタイル:90.77

MuSEUM is an international collaboration aiming at a new precise measurement of the muonium hyperfine structure at J-PARC (Japan Proton Accelerator Research Complex). Utilizing its intense pulsed muon beam, we expect a ten-fold improvement for both measurements at high magnetic field and zero magnetic field. We have developed a sophisticated monitoring system, including a beam profile monitor to measure the 3D distribution of muonium atoms to suppress the systematic uncertainty.


Materials and Life Science Experimental Facility at the Japan Proton Accelerator Research Complex, 4; The Muon Facility

髭本 亘; 門野 良典*; 河村 成肇*; 幸田 章宏*; 小嶋 健児*; 牧村 俊助*; 的場 史郎*; 三宅 康博*; 下村 浩一郎*; Strasser, P.*

Quantum Beam Science (Internet), 1(1), p.11_1 - 11_24, 2017/06

ミュオン科学実験施設はJ-PARCにおいて中性子, ハドロン, ニュートリノ各施設と並ぶ利用施設である。ミュオン施設では、物質生命科学実験棟において中性子実験施設と共有している高エネルギーの陽子により発生させたミュオンを用いて様々な科学研究に用いている。本レビューではミュオン科学実験施設の現状について報告する。


New muonium HFS measurements at J-PARC/MUSE

Strasser, P.*; 青木 正治*; 深尾 祥紀*; 東 芳隆*; 樋口 嵩*; 飯沼 裕美*; 池戸 豊*; 石田 啓一*; 伊藤 孝; 岩崎 雅彦*; et al.

Hyperfine Interactions, 237(1), p.124_1 - 124_9, 2016/12

 被引用回数:6 パーセンタイル:92.96

At the Muon Science Facility (MUSE) of J-PARC (Japan Proton Accelerator Research Complex), the MuSEUM collaboration is planning new measurements of the ground state hyperfine structure (HFS) of muonium both at zero field and at high magnetic field. The previous measurements were performed both at LAMPF (Los Alamos Meson Physics Facility) with experimental uncertainties mostly dominated by statistical errors. The new high intensity muon beam that will soon be available at MUSE H-Line will provide an opportunity to improve the precision of these measurements by one order of magnitude. An overview of the different aspects of these new muonium HFS measurements, the current status of the preparation, and the results of a first commissioning test experiment at zero field are presented.


Tuning of ultra-slow muon transport system

足立 泰平*; 池戸 豊*; 西山 樟生*; 薮内 敦*; 長友 傑*; Strasser, P.*; 伊藤 孝; 髭本 亘; 小嶋 健児*; 牧村 俊助*; et al.

JPS Conference Proceedings (Internet), 8, p.036017_1 - 036017_4, 2015/09

We report on the tuning of the ultra-slow muon beam line at J-PARC MUSE using Li impurities in a tungsten muonium production target in place of positive muons. Li ions were evaporated from the tungsten target by heating it up to 2000K and were transported in the ultra-slow muon beam line. The Li ion beam was monitored by micro channel plates installed at several points in the beam line. The Li beam was successfully transported to the end of the beam line after optimization of beam line parameters.


Bipartite magnetic parent phases in the iron oxypnictide superconductor

平石 雅俊*; 飯村 壮史*; 小嶋 健児*; 山浦 淳一*; 平賀 晴弘*; 池田 一貴*; Miao, P.*; 石川 喜久*; 鳥居 周輝*; 宮崎 正範*; et al.

Nature Physics, 10(4), p.300 - 303, 2014/04

 被引用回数:94 パーセンタイル:96.38(Physics, Multidisciplinary)

High-temperature (high-$$T_{rm c}$$) superconductivity appears as a consequence of the carrier-doping of an undoped parent compound exhibiting antiferromagnetic order; thereby, ground-state properties of the parent compound are closely relevant to the superconducting state. On the basis of the concept, a spin-fluctuation has been addressed as an origin of pairing of the superconducting electrons in cuprates. Whereas, there is growing interest in the pairing mechanism such as an unconventional spin-fluctuation or an advanced orbital-fluctuation due to the characteristic multi-orbital system in iron-pnictides. Here, we report the discovery of an antiferromagnetic order as well as a unique structural transition in electron-overdoped LaFeAsO$$_{1-x}$$H$$_x$$ ($$x sim 0.5$$), whereby another parent phase was uncovered, albeit heavily doped. The unprecedented two-dome superconducting phases observed in this material can be interpreted as a consequence of the carrier-doping starting from the original at $$x sim 0$$ and advanced at $$x sim 0.5$$ parent phases toward the intermediate region. The bipartite parent phases with distinct physical properties in the second magnetic phase provide us with an interesting example to illustrate the intimate interplay among the magnetic interaction, structural change and orbital degree of freedom in iron-pnictides.


Prominent quasiparticle peak in the photoemission spectrum of the metallic phase of V$$_{2}$$O$$_{3}$$

Mo, S.-K.*; Denlinger, J. D.*; Kim, H.-D.*; Park, J.-H.*; Allen, J. W.*; 関山 明*; 山崎 篤志*; 角野 宏治*; 菅 滋正*; 斎藤 祐児; et al.

Physical Review Letters, 90(18), p.186403_1 - 186403_4, 2003/05


 被引用回数:134 パーセンタイル:95.62(Physics, Multidisciplinary)



High-resolution resonance photoemission study of Ce$$MX$$ ($$M$$=Pt, Pd; $$X$$=P, As, Sb)

岩崎 剛之*; 関山 明*; 山崎 篤志*; 岡崎 誠*; 角野 宏治*; 宇都宮 裕*; 今田 真*; 斎藤 祐児; 室 隆桂之*; 松下 智裕*; et al.

Physical Review B, 65(19), p.195109_1 - 195109_9, 2002/05

 被引用回数:23 パーセンタイル:72.01(Materials Science, Multidisciplinary)

低い近藤温度を持つCeMX (M=Pt, Pd; X=P, As, Sb)の Ce 3d-4f共鳴光電子分光を高いエネルギー分解能にて行い、Ce 4d-4f共鳴光電子分光の結果と比較を行った。実験結果は、低い近藤温度の物質においても表面とバルク電子状態が大きく異なることを示した。Ce 4f成分の寄与のない価電子帯スペクトルは、同じ構造をもつLaMXのバンド計算を用いて説明できた。実験で得られたCe 4f成分は、不純物アンダーソンに基づいたNCA(noncrossing approximation)計算によってよく再現でき、表面とバルクのCe 4f電子状態の違いを説明するのにもっと重要な要因がCe 4f準位シフトであることがわかった。さらに、CeMXのCe 4f状は、p-d反結合状態と優先的に混成することがわかった。

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