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論文

Enhancement of domain-wall mobility detected by NMR at the angular momentum compensation temperature

今井 正樹; 中堂 博之; 松尾 衛; 前川 禎通; 齊藤 英治

Physical Review B, 102(1), p.014407_1 - 014407_5, 2020/07

 被引用回数:0 パーセンタイル:100(Materials Science, Multidisciplinary)

The angular momentum compensation temperature $$T_{rm A}$$ of ferrimagnets has attracted much attention because of high-speed magnetic dynamics near $$T_{rm A}$$. We show that NMR can be used to investigate domain wall dynamics near $$T_{rm A}$$ in ferrimagnets. We performed $$^{57}$$Fe-NMR measurements on the ferrimagnet Ho$$_3$$Fe$$_5$$O$$_{12}$$ with $$T_{rm A}$$ = 245 K. In a multi-domain state, the NMR signal is enhanced by domain wall motion. We found that the NMR signal enhancement shows a maximum at $$T_{rm A}$$ in the multi-domain state. The NMR signal enhancement occurs due to increasing domain-wall mobility toward $$T_{rm A}$$. We develop the NMR signal enhancement model involves domain-wall mobility. Our study shows that NMR in multi-domain state is a powerful tool to determine $$T_{rm A}$$, even from a powder sample and it expands the possibility of searching for angular momentum-compensated materials.

論文

Giant spin hydrodynamic generation in laminar flow

高橋 遼*; 中堂 博之; 松尾 衛; 針井 一哉*; 大沼 悠一*; 前川 禎通; 齊藤 英治

Nature Communications (Internet), 11, p.3009_1 - 3009_6, 2020/06

 被引用回数:0 パーセンタイル:100(Multidisciplinary Sciences)

Hydrodynamic motion can generate a flux of electron-spin's angular momentum via the coupling between fluid rotation and electron spins. Such hydrodynamic generation, called spin hydrodynamic generation (SHDG), has recently attracted attention in a wide range of fields, especially in spintronics. Spintronics deals with spin-mediated interconversion taking place on a micro or nano scale because of the spin-diffusion length scale. To be fully incorporated into the interconversion, SHDG physics should also be established in such a minute scale, where most fluids exhibit a laminar flow. Here, we report electric voltage generation due to the SHDG in a laminar flow of a liquid-metal mercury. The experimental results show a scaling rule unique to the laminar-flow SHDG. Furthermore, its energy con- version efficiency turns out to be about 105 greater than of the turbulent one. Our findings reveal that the laminar-flow SHDG is suitable to downsizing and to extend the coverage of fluid spintronics.

論文

Spin Seebeck mechanical force

針井 一哉; Seo, Y.-J.*; 堤 康雅*; 中堂 博之; 大柳 洸一*; 松尾 衛; 塩見 雄毅*; 小野 崇人*; 前川 禎通; 齊藤 英治

Nature Communications (Internet), 10(1), p.2616_1 - 2616_5, 2019/06

 被引用回数:8 パーセンタイル:11.64(Multidisciplinary Sciences)

Electric current has been used to send electricity to far distant places. On the other hand, spin current, a flow of electron spin, can in principle also send angular momentum to distant places. In a magnet, there is a universal spin carrier called a spin wave, a wave-type excitation of magnetization. Since spin waves exhibit a long propagation length, it should be able to send angular momentum that can generate torque and force at a distant place: a new function of magnets. Here we observe mechanical angular momentum transmission and force generation due to spin waves injected into Y$$_3$$Fe$$_5$$O$$_{12}$$ by the spin-Seebeck effect. The spin-wave current, transmitted through a Y$$_3$$Fe$$_5$$O$$_{12}$$ micro cantilever, was found to create a mechanical force on the cantilever as a non-local reaction of the spin-Seebeck effect. Spin-wave current can be generated remotely even in open circuits, and it can be used to drive micro mechanical devices.

論文

Angular momentum compensation manipulation to room temperature of the ferrimagnet Ho$$_{3-x}$$Dy$$_{x}$$Fe$$_5$$O$$_{12}$$ detected by the Barnett effect

今井 正樹; 中堂 博之; 小野 正雄; 針井 一哉; 松尾 衛; 大沼 悠一*; 前川 禎通; 齊藤 英治

Applied Physics Letters, 114(16), p.162402_1 - 162402_4, 2019/04

 被引用回数:6 パーセンタイル:17.09(Physics, Applied)

We demonstrate that the angular momentum compensation temperature $$T_{rm A}$$, at which the net angular momentum in the sample disappears, can be controlled in Ho$$_3$$Fe$$_5$$O$$_{12}$$ by partially substituting Dy for Ho. The $$T_{rm A}$$ can be detected using the Barnett effect, by which mechanical rotation magnetizes an object due to spin-rotation coupling. We found that $$T_{rm A}$$ increases with the Dy content and clarified that the $$T_{rm A}$$ of Ho$$_{1.5}$$Dy$$_{1.5}$$Fe$$_5$$O$$_{12}$$ coincides with room temperature. The Barnett effect enables us to explore materials applicable to magnetic devices utilizing the angular momentum compensation only by rotating the powder sample at room temperature.

論文

Observation of gyromagnetic reversal

今井 正樹; 緒方 裕大*; 中堂 博之; 小野 正雄; 針井 一哉; 松尾 衛*; 大沼 悠一*; 前川 禎通; 齊藤 英治

Applied Physics Letters, 113(5), p.052402_1 - 052402_3, 2018/07

 被引用回数:7 パーセンタイル:33.3(Physics, Applied)

We report direct observation of gyromagnetic reversal, which is the sign change of gyromagnetic ratio in a ferrimagnet Ho$$_3$$Fe$$_5$$O$$_{12}$$, by using the Barnett effect measurement technique at low temperatures. The Barnett effect is a phenomenon in which magnetization is induced by mechanical rotation through the coupling between rotation and total angular momentum $$J$$ of electrons. The magnetization of Ho$$_3$$Fe$$_5$$O$$_{12}$$ induced by mechanical rotation disappears at 135 K and 240 K. The temperatures correspond to the magnetization compensation temperature $$T_{rm M}$$ and the angular momentum compensation temperature $$T_{rm A}$$, respectively. Between $$T_{rm M}$$ and $$T_{rm A}$$, the magnetization flips over to be parallel against the angular momentum due to the sign change of gyromagnetic ratio. This study provides an unprecedented technique to explore the gyromagnetic properties.

論文

Enhanced orbital magnetic moment in FeCo nanogranules observed by Barnett effect

緒方 裕大; 中堂 博之; Gu, B.; 小林 伸聖*; 小野 正雄; 針井 一哉; 松尾 衛; 齊藤 英治; 前川 禎通

Journal of Magnetism and Magnetic Materials, 442, p.329 - 331, 2017/11

 被引用回数:4 パーセンタイル:52.83(Materials Science, Multidisciplinary)

The gyroscopic g factor, $$g'$$, of FeCo nanogranules embedded in a matrix of MgF$$_2$$ (FeCo-MgF$$_2$$) was determined by measuring the magnetic-field generation from a rotating sample due to the Barnett effect. The $$g'$$ value of the FeCo-MgF$$_2$$ is estimated to be 1.76 $$pm$$ 0.11. The orbital contribution to the magnetic moment in the FeCo nanogranules was found to be quite large compared with that in bulk FeCo, being consistent with a density-functional-theory calculation that shows that the orbital magnetic moment may increase at the FeCo/MgF$$_2$$ interfaces. The result suggests that the orbital magnetic moment is enhanced by symmetry breaking at the surface of the FeCo nanogranules.

論文

Fabrication and magnetic control of Y$$_3$$Fe$$_5$$O$$_{12}$$ cantilevers

Seo, Y.-J.*; 針井 一哉; 高橋 遼*; 中堂 博之; 大柳 洸一*; Qiu, Z.*; 小野 崇人*; 塩見 雄毅*; 齊藤 英治

Applied Physics Letters, 110(13), p.132409_1 - 132409_4, 2017/03

 被引用回数:11 パーセンタイル:29.06(Physics, Applied)

フェリ磁性体であるY$$_3$$Fe$$_5$$O$$_{12}$$を用いたサブミクロンカンチレバーを収束イオンビーム法によって作成し、その振動特性を磁場によって制御した。カンチレバーは縦横2つの振動モードを示し、それぞれのモードは外部磁場の印加によって共鳴周波数が減少、増大した。この結果は磁気力の磁場変化を取り扱った数値シミュレーションでよく再現された。周波数変化は数%に及ぶことから、磁場による高効率な振動制御が行われたと結論できる。

論文

Gyroscopic $$g$$ factor of rare earth metals

緒方 裕大; 中堂 博之; 小野 正雄; 針井 一哉; 松尾 衛; 前川 禎通; 齊藤 英治

Applied Physics Letters, 110(7), p.072409_1 - 072409_4, 2017/02

 被引用回数:9 パーセンタイル:35.46(Physics, Applied)

We develop the $$in$$ $$situ$$ magnetization measurement apparatus for observing the Barnett effect consisting of a fluxgate sensor, high speed rotor with frequencies of up to 1.5 kHz, and magnetic shield at room temperature. The effective magnetic field (Barnett field) in a sample arising from rotation magnetizes the sample and is proportional to the rotational frequency. The gyroscopic $$g$$ factor, $$g'$$, of rare earth metals, in particular, Gd, Tb and Dy were estimated to be 2.00$$pm$$0.08, 1.53$$pm$$0.17, and 1.15$$pm$$0.32, respectively, from the slopes of the rotation dependence of the Barnett field. This study provides a technique to determine the $$g'$$ factor even in samples where the spectroscopic method may not be available.

論文

Spin hydrodynamic generation

高橋 遼*; 松尾 衛; 小野 正雄; 針井 一哉; 中堂 博之; 岡安 悟; 家田 淳一; 高橋 三郎*; 前川 禎通; 齊藤 英治

Nature Physics, 12, p.52 - 56, 2016/01

 被引用回数:41 パーセンタイル:6.49(Physics, Multidisciplinary)

Magnetohydrodynamic generation is the conversion of fluid kinetic energy into electricity. Such conversion, which has been applied to various types of electric power generation, is driven by the Lorentz force acting on charged particles and thus a magnetic field is necessary. On the other hand, recent studies of spintronics have revealed the similarity between the function of a magnetic field and that of spin-orbit interactions in condensed matter. This suggests the existence of an undiscovered route to realize the conversion of fluid dynamics into electricity without using magnetic fields. Here we show electric voltage generation from fluid dynamics free from magnetic fields; we excited liquid-metal flows in a narrow channel and observed longitudinal voltage generation in the liquid. This voltage has nothing to do with electrification or thermoelectric effects, but turned out to follow a universal scaling rule based on a spin-mediated scenario. The result shows that the observed voltage is caused by spin-current generation from a fluid motion: spin hydrodynamic generation. The observed phenomenon allows us to make mechanical spin-current and electric generators, opening a door to fluid spintronics.

論文

Barnett effect in paramagnetic states

小野 正雄; 中堂 博之; 針井 一哉; 岡安 悟; 松尾 衛; 家田 淳一; 高橋 遼*; 前川 禎通; 齊藤 英治

Physical Review B, 92(17), p.174424_1 - 174424_4, 2015/11

 被引用回数:14 パーセンタイル:36.69(Materials Science, Multidisciplinary)

We report the observation of the Barnett effect in paramagnetic states by mechanically rotating gadolinium (Gd) metal with a rotational frequency of up to 1.5 kHz above the Curie temperature. An in situ magnetic measurement setup comprising a high-speed rotational system and a fluxgate magnetic sensor was developed for the measurement. Temperature dependence of the observed magnetization follows that of paramagnetic susceptibility, indicating that any emergent magnetic field is proportional to the rotational frequency and is independent of temperature. From the proportionality constant of the emergent field, the gyromagnetic ratio of Gd is calculated to be -29 $$pm$$ 5 GHz/T. This study revisits the primordial issue of magnetism with modern technologies to shed new light on the fundamental spin-rotation coupling.

論文

Line splitting by mechanical rotation in nuclear magnetic resonance

針井 一哉; 中堂 博之; 小野 正雄; 松尾 衛; 家田 淳一; 岡安 悟; 前川 禎通; 齊藤 英治

Japanese Journal of Applied Physics, 54(5), p.050302_1 - 050302_3, 2015/05

 被引用回数:7 パーセンタイル:57.69(Physics, Applied)

Nuclear magnetic resonance (NMR) measurements for a nuclear spin 1/2 system in an external magnet field and mechanical rotation in kHz range are reported. NMR signals are measured by the synchronous rotation of a sample and a detector coil under the condition that the rotation axis is perpendicular to the external field. NMR line splits into two despite the system having a single Zeeman level separation. We analytically show that the splitting originates in the nuclear spin motion under mechanical rotation, and is determined by only the angular velocity of the rotation without any material parameters.

論文

Rotational Doppler effect and Barnett field in spinning NMR

中堂 博之; 針井 一哉; 松尾 衛; 家田 淳一; 小野 正雄; 前川 禎通; 齊藤 英治

Journal of the Physical Society of Japan, 84(4), p.043601_1 - 043601_4, 2015/04

 被引用回数:12 パーセンタイル:27.8(Physics, Multidisciplinary)

We report the observation of the rotational Doppler effect using nuclear magnetic resonance (NMR). We have developed a coil-spinning technique that enables measurements by rotating a detector and fixing a sample. We found that the rotational Doppler effect gives rise to NMR frequency shifts equal to the rotation frequency. We formulate the rotational Doppler effect and the Barnett field using a vector model for the nuclear magnetic moment. This formulation reveals that, with just the sample rotating, both effects cancel each other, thereby explaining the absence of an NMR frequency shift in conventional sample-spinning NMR measurements.

論文

Observation of Barnett fields in solids by nuclear magnetic resonance

中堂 博之; 小野 正雄; 針井 一哉; 松尾 衛; 家田 淳一; 春木 理恵*; 岡安 悟; 前川 禎通; 安岡 弘志; 齊藤 英治

Applied Physics Express, 7(6), p.063004_1 - 063004_4, 2014/06

 被引用回数:30 パーセンタイル:16.64(Physics, Applied)

電気的に中性な物体であっても、回転する物体中の粒子には磁場が生じることが予言されている。この磁場をバーネット磁場という。我々は核磁気共鳴法が固体中に生じたバーネット磁場を測定できることを示す。我々は試料とNMR検出コイルを同じ早さで回転させると核磁気モーメントの符号を反映したNMRシフトが生じることを見いだした。この結果はバーネット磁場の直接的証拠である。NMRを用いたバーネット磁場の測定は未知の核磁気モーメントの符号を決定できる。

論文

Microscopic properties of the heavy-fermion superconductor PuCoIn$$_5$$ explored by nuclear quadrupole resonance

Koutroulakis, G.*; 安岡 弘志; 中堂 博之; Tobash, P. H.*; Mitchell, J. N.*; Bauer, E. D.*; Thompson, J. D.*

New Journal of Physics (Internet), 16, p.053019_1 - 053019_12, 2014/05

 被引用回数:6 パーセンタイル:47.25(Physics, Multidisciplinary)

重い電子系超伝導体PuCoIn$$_5$$において、0.29K $$leq Tleq$$75Kの温度領域で$$^{115}$$In核四重極共鳴(NQR)測定を行ったので報告する。結晶学的に異なるInサイトのNQRパラメーターを決定し、その温度依存性を調べた。超伝導転移温度以下においてNQR周波数が温度に比例してシフトすることを明らかにし、これは複合対形成模型からの予想と一致する。核スピン格子緩和率$$T_1^{-1}(T)$$$$T_c simeq $$2.3Kで超伝導転移を示し、$$T_c$$近傍においてab面内の異方的揺らぎが大きな強結合系超伝導であることを示している。$$T_1^{-1}$$の解析はPuCoIn$$_5$$は強結合系d波超伝導体であることを示している。

論文

Weak itinerant antiferromagnetism in PuIn$$_3$$ explored using $$^{115}$$In nuclear quadrupole resonance

中堂 博之; Koutroulakis, G.*; 安岡 弘志; Bauer, E. D.*; Tobash, P. H.*; Mitchell, J. N.*; Thompson, J. D.*

Journal of Physics; Condensed Matter, 26(3), p.036001_1 - 036001_5, 2014/01

 被引用回数:4 パーセンタイル:74.58(Physics, Condensed Matter)

PuIn$$_3$$における$$^{115}$$In NQR測定の結果について報告する。$$^{115}$$Inの核スピン$$I$$=9/2に期待される4本のNQR共鳴線のうちの3本の共鳴線を観測した。20Kにおいて、それらの共鳴線は等間隔であり、そこからNQR周波数$$nu_{rm Q}=10.45$$MHzと電場勾配の非対称パラメータの$$eta=0$$が導かれた。14Kにおいて、NQR共鳴線の形状と核スピン緩和率1/$$T_1$$は反強磁性転移により変化を生じる。14K以下において、NQRスペクトルより見積もられた内部交番磁化$$M_{rm Q}(T)$$と1/$$T_1$$の温度依存性はスピン揺らぎのSCR理論によりよく説明される。さらに、$$T_1T$$$$M_{rm Q}(T)/M_{rm Q}(0)$$はSCR理論から予言される通りに比例している。これらの結果はPuIn$$_3$$が弱い反強磁性体、すなわち有限温度において反強磁性波数近傍のスピン揺らぎが物性を支配している証拠である。

論文

Anisotropic spin fluctuations in the heavy fermion systems; Case studies of CePd$$_5$$Al$$_2$$ and NpPd$$_5$$Al$$_2$$

酒井 宏典; 中堂 博之; 徳永 陽; 神戸 振作; 芳賀 芳範; Ronning, F.*; Bauer, E. D.*; Thompson, J. D.*; 本間 佳哉*; 青木 大*; et al.

Journal of the Physical Society of Japan, 81(Suppl.B), p.SB003_1 - SB003_6, 2012/12

 被引用回数:5 パーセンタイル:57.5(Physics, Multidisciplinary)

Ce$$T$$In$$_5$$ ($$T$$=Co, Rh, Ir)及び$$An$$$$T$$Ga$$_5$$ ($$An$$=U, Np, Pu)という化学式を持つ一連の化合物(115系と称する)、核磁気共鳴(NMR)測定の結果得られるナイトシフトと緩和率の解析から、反強磁性スピン揺らぎのXY型異方性がd波超伝導発現に有利であるとわかってきた。この仮説を確かめるために、115系化合物と類似の結晶構造を有するCePd$$_5$$Al$$_2$$とNpPd$$_5$$Al$$_2$$においてスピン揺らぎの異方性がどうなっているかを検証した。CePd$$_5$$Al$$_2$$は、イジング異方性を持つ反強磁性体であり、スピン揺らぎも同じくイジング型の異方性を示した。d波超伝導体NpPd$$_5$$Al$$_2$$は、転移温度直上の通常状態においてXY型の反強磁性磁気揺らぎを有していることがわかった。

論文

Observation of $$^{239}$$Pu nuclear magnetic resonance

安岡 弘志; Koutroulakis, G.*; 中堂 博之; Richmond, S.*; Veirs, D. K.*; Smith, A. I.*; Bauer, E. D.*; Thompson, J. D.*; Jarvinen, G. D.*; Clark, D. L.*

Science, 336(6083), p.901 - 904, 2012/05

 被引用回数:40 パーセンタイル:12.71(Multidisciplinary Sciences)

The spin-1/2 plutonium-239 ($$^{239}$$Pu) nucleus should in principle be active in nuclear magnetic resonance spectroscopy. However, its signal has eluded detection for the past fifty years. Here, we report observation of a $$^{239}$$Pu resonance from a solid sample of plutonium dioxide, PuO$$_2$$, subjected to a wide scan of external magnetic field values ($$B_0=3$$ to 8T) at a temperature of 4 Kelvin. By mapping the external field dependence of the measured resonance frequency, we determined the nuclear gyromagnetic ratio $$^{239}$$$$gamma$$$$_{rm n}$$(PuO$$_2$$)/2$$pi$$ to be 2.856 $$pm$$ 0.001 MHz/T. Assuming a free-ion value for the Pu$$^{4+}$$ hyperfine coupling constant, we estimated a bare $$^{239}$$$$gamma$$$$_{rm n}$$/2$$pi$$ value of approximately 2.29 MHz/T, corresponding to a nuclear magnetic moment of $$mu$$$$_{rm n}$$ $${approx}$$ 0.15 $$mu$$$$_{rm N}$$ (where $$mu$$$$_{rm N}$$ is the nuclear magneton).

論文

CeRu$$_2$$Al$$_2$$B; A Local-moment 4$$f$$ magnet with a complex $$T$$-$$H$$ phase diagram

Raumbach, R. E.*; 中堂 博之; 安岡 弘志; Ronning, F.*; Bauer, E. D.*; Thompson, J. D.*

Physical Review B, 85(9), p.094422_1 - 094422_7, 2012/03

 被引用回数:27 パーセンタイル:21.47(Materials Science, Multidisciplinary)

The temperature-magnetic field ($$T$$-$$H$$) phase diagram for the tetragonal compound CeRu$$_2$$Al$$_2$$B, determined from magnetization, specific heat, nuclear magnetic resonance (NMR), and electrical resistivity is reported. This system exhibits localized 4$$f$$ magnetic ordering at high temperatures where antiferromagnetism is observed at a N${'e}$el temperature $$T$$$$_{rm N}$$ = 14.2 K and a first-order ferromagnetic transition is observed at a Curie temperature $$T$$$$_{rm c}$$ = 12.8 K. The application of a magnetic field $$H$$ results in a rich phase diagram that includes three magnetically ordered phase: (1) antiferromagnetic, (2) canted antiferromagnetic, and (3) ferromagnetic, indicating that there are several finely tuned exchange interaction.

論文

Solid-state NMR study of actinide dioxides

徳永 陽; 酒井 宏典; 神戸 振作; 中堂 博之; 逢坂 正彦; 三輪 周平; 西 剛史; 中田 正美; 伊藤 昭憲; 本間 佳哉*

Materials Research Society Symposium Proceedings, Vol.1444, p.149 - 158, 2012/00

 被引用回数:0 パーセンタイル:100

二酸化アクチノイドは原子力燃料としての応用がよく知られているが、アクチノイド化合物の基礎的な電子物性を系統的に理解するうえでも非常に重要な化合物群である。特に低温では$$f$$電子特有の強いスピン-軌道相互作用を起源とした多彩な磁気状態が実現することが知られている。われわれはこれまで$$^{17}$$O酸素核のNMR測定を通じて微視的観点から系統的な研究を行ってきた。最近ではアメリシウム化合物では初めてとなるNMR測定をAmO$$_2$$において成功している。本講演ではこれまでの二酸化アクチノイドのNMR研究結果についての総括的に議論する予定である。

論文

$$^{237}$$Np nuclear relaxation rate in heavy fermion superconductor NpPd$$_5$$ Al$$_2$$

中堂 博之; 徳永 陽; 神戸 振作; 酒井 宏典; 芳賀 芳範; 松田 達磨; 大貫 惇睦; 安岡 弘志; 青木 大*; 本間 佳哉*; et al.

Physical Review B, 84(9), p.094402_1 - 094402_5, 2011/09

 被引用回数:6 パーセンタイル:66.57(Materials Science, Multidisciplinary)

$$^{27}$$Al nuclear spin-lattice relaxation rate 1/$$^{27}$$$$T$$$$_1$$ has been measured in heavy fermion superconductor NpPd$$_5$$Al$$_2$$ for a wide range of external fields between 0.7 and 11 T. We found that 1/$$^{27}$$$$T$$$$_1$$ exhibits a strong, field-dependent behavior at low fields below $$H$$ $$sim$$ 3 T, which is attributed to unlike-spin cross relaxation between $$^{237}$$Np and $$^{27}$$Al. An analysis based on the cross relaxation process allows us to make the first quantitative estimates of the Np nuclear relaxation rate 1/$$^{237}$$$$tau$$ in an itinerant 5$$f$$ electron system. The estimated values of 1/$$^{237}$$$$tau$$ $$sim$$ 6 $$times$$ 10$$^7$$ s$$^{-1}$$, with a weak temperature variation, are below the resolution of NMR relaxation times, indicating that a direct observation of the $$^{237}$$Np NMR signal would be very difficult, at least in the paramagnetic state. It is proposed that a direct observation of $$^{237}$$Np NMR might be possible in the superconducting state at $$T$$ $$sim$$ 1K.

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