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Magnetism induced by interlayer electrons in the quasi-two-dimensional electride Y$$_{2}$$C; Inelastic neutron scattering study

玉造 博夢; 村上 洋一*; 倉本 義夫*; 佐賀山 基*; 松浦 直人*; 川北 至信; 松石 聡*; 鷲尾 康仁*; 井下 猛*; 浜田 典昭*; et al.

Physical Review B, 102(22), p.224406_1 - 224406_5, 2020/12

Magnetic excitations in layered electride Y$$_{2}$$C have been found by inelastic neutron scattering. We have observed weak but clear magnetic scattering around the wave number $$Q = 0$$, but no magnetic order down to the lowest temperature measured (7 K). The imaginary part of the dynamical susceptibility deduced is well described by the Lorentz function of energy $$E$$ for each momentum $$Q$$. The width $$mathit{Gamma}(Q)$$ of the Lorentzian is proportional to $$Q(Q^2+kappa^{2})$$ with $$kappa^{-1} sim 4{rm AA}$$ at $$T=7$$ K. We have also found that with increasing $$Q$$ the magnetic form factor decays faster than that of a $$4d$$ electron in a single Y atom, which indicates a more extended magnetic moment in Y$$_{2}$$C. These results provide experimental evidence that the itinerant magnetism in Y$$_{2}$$C originates from the anionic electrons that reside in the interlayers. The Curie-Weiss-like behavior of the magnetic susceptibility reported in Y$$_{2}$$C is ascribed to the mode coupling effects of spin fluctuations.


Temporally decoherent and spatially coherent vibrations in metal halide perovskites

Zhang, D.*; Hu, X.*; Chen, T.*; Abernathy, D. L.*; 梶本 亮一; 中村 充孝; 古府 麻衣子; Foley, B. J.*; Yoon, M.*; Choi, J. J.*; et al.

Physical Review B, 102(22), p.224310_1 - 224310_10, 2020/12

The long carrier lifetime and defect tolerance in metal halide perovskites (MHPs) are major contributors to the superb performance of MHP optoelectronic devices. Large polarons were reported to be responsible for the long carrier lifetime. Yet microscopic mechanisms of the large polaron formation, including the so-called phonon melting, are still under debate. Here, time-of-flight inelastic neutron scattering experiments and first-principles density-functional theory calculations were employed to investigate the lattice vibrations (or phonon dynamics) in methylammonium lead iodide, a prototypical example of MHPs. Our findings are that optical phonons lose temporal coherence gradually with increasing temperature which vanishes at the orthorhombic-to-tetragonal structural phase transition. Surprisingly, however, we found that the spatial coherence is still retained throughout the decoherence process. We argue that the temporally decoherent and spatially coherent vibrations contribute to the formation of large polarons in this metal halide perovskite.


Emergence of nearly flat bands through a kagome lattice embedded in an epitaxial two-dimensional Ge layer with a bitriangular structure

Fleurence, A.*; Lee, C.-C.*; Friedlein, R.*; 深谷 有喜; 吉本 真也*; 向井 孝三*; 山根 宏之*; 小杉 信博*; 吉信 淳*; 尾崎 泰助*; et al.

Physical Review B, 102(20), p.201102_1 - 201102_6, 2020/11




Insight into Kondo screening in the intermediate-valence compound SmOs$$_4$$Sb$$_{12}$$ uncovered by soft X-ray magnetic circular dichroism

斎藤 祐児; 藤原 秀紀*; 保井 晃*; 門野 利治*; 菅原 仁*; 菊地 大輔*; 佐藤 英行*; 菅 滋正*; 山崎 篤志*; 関山 明*; et al.

Physical Review B, 102(16), p.165152_1 - 165152_8, 2020/10


Through a high-precision soft X-ray magnetic circular dichroism (XMCD) study of the intermediate-valence compound SmOs$$_4$$Sb$$_{12}$$, we show our successful approach of revealing unprecedented details of Kondo screening below a characteristic temperature of $$ T_{0} sim$$ 20 K in the paramagnetic phase. The multiplet XMCD structure at the Sm $$M_{5}$$ edge sensitive to the 4$$f$$ configuration enabled us to observe a clear difference between the temperature evolution above and below $$T_{0}$$ with one- and two-component behavior, respectively. Our findings are in strong contrast to the conventional Kondo crossover that coincides with the valence transition, but are qualitatively accounted for by theoretical XMCD predictions combined with the two-fluid phenomenology recently proposed. This work contributes to the large context of Kondo physics that is closely related to quantum criticality in heavy fermion systems.


Optomagnonic Barnett effect

仲田 光樹; 高吉 慎太郎*

Physical Review B, 102(9), p.094417_1 - 094417_11, 2020/09

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

いわゆる光学的Barnett効果[A. Rebei and J. Hohlfeld, Phys. Lett. A 372, 1915 (2008); J. Appl. Phys. 103, 07B118 (2008)], i.e., 円偏光レーザー誘起磁化成長[S. Takayoshi et al., Phys. Rev. B 90, 214413 (2014); S. Takayoshi et al., Phys. Rev. B 90, 085150 (2014)]をフェリ磁性絶縁体に応用し、THz領域におけるマグノン凝縮機構を微視的に解明した。これはBose統計に従うマグノンに特有の巨視的量子効果である。本研究が提供するTHzマグノン凝縮体を活用することで、従来の強磁性絶縁体中のものよりはるかに高速のスピン輸送「巨視的量子干渉効果によるJosephsonスピン流」を実現することができる。


Direct measurement of fast ortho-para conversion of molecularly chemisorbed H$$_{2}$$ on Pd(210)

植田 寛和; 笹川 裕矢*; Ivanov, D.*; 大野 哲*; 小倉 正平*; 福谷 克之

Physical Review B, 102(12), p.121407_1 - 121407_5, 2020/09

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



Unveiling spin-dependent unoccupied electronic states of Co$$_{2}$$MnGe (Ga) film via Ge (Ga) $$L_{2,3}$$ absorption spectroscopy

吉川 智己*; Antonov, V. N.*; 河野 嵩*; 鹿子木 将明*; 角田 一樹; 宮本 幸治*; 竹田 幸治; 斎藤 祐児; 後藤 一希*; 桜庭 裕弥*; et al.

Physical Review B, 102(6), p.064428_1 - 064428_7, 2020/08

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

X-ray absorption spectroscopy (XAS) and X-ray magnetic circular dichroism (XMCD) spectroscopy were applied at the Ge (Ga) $$L_{2,3}$$ edge to unravel the spin-resolved unoccupied electronic states of Co$$_{2}$$MnGe (Ga). Complicated spectral features were observed in both XAS and XMCD spectra. For their interpretation, we compared the experimental XAS and XMCD spectra with the calculated Ge (Ga) 4$$s$$ and 4$$d$$ orbital partial density of states. The comparison enabled a qualitative explanation of the XMCD spectra as the difference between the majority and minority-spin unoccupied density of states summed over the 4$$s$$ and 4$$d$$ orbitals. Our finding provides a new approach to uncover the spin-split partial density of states above the Fermi level.


Behavior of Sm in the boron cage of Sm-doped $$R$$B$$_{6}$$ ($$R$$ =Yb, La) observed by multiple-wavelength neutron holography

上地 昇一*; 大山 研司*; 福本 陽平*; 金澤 雄輝*; 八方 直久*; 原田 正英; 稲村 泰弘; 及川 健一; 松浦 航*; 伊賀 文俊*; et al.

Physical Review B, 102(5), p.054104_1 - 054104_10, 2020/08

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

We have succeeded in visualizing the local atomic structures around Sm in $$R$$B$$_{6}$$ ($$R$$ =Yb, La), in which a rareearth atom is located in the boron cage, using the newly developed technique for local structure investigations, multiple-wavelength neutron holography in a pulsed neutron facility. From the local atomic structures, we were able to clarify the behavior of Sm in the boron cage. Doped Sm in YbB$$_6$$ fluctuates within the boron cage with a mean displacement of 0.25(4) ${AA}$, while that of Sm in LaB$$_6$$ is approximately 0.15 ${AA}$. The Sm doping causes the fluctuation of the first-nearest-neighbor B with a mean displacement of 0.28 ${AA}$, while its effect on La, Yb, and the rest of the boron atoms is negligible. These are the first observations of the local behavior of doped rare-earth atoms and B in rare-earth borides with boron cages.


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:1 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.


Self-learning hybrid Monte Carlo; A First-principles approach

永井 佑紀; 奥村 雅彦; 小林 恵太*; 志賀 基之

Physical Review B, 102(4), p.041124_1 - 041124_6, 2020/07

 被引用回数:1 パーセンタイル:31.73(Materials Science, Multidisciplinary)



Fast nuclear-spin conversion of H$$_{2}$$ trapped and polarized in a CO$$_{2}$$ matrix

山川 紘一郎; 石橋 篤季*; 波吉 敏信*; 東 優一*; 荒川 一郎*

Physical Review B, 102(4), p.041401_1 - 041401_5, 2020/07

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

The clear evidence for the nuclear spin conversion of matrix-isolated H$$_{2}$$ is presented. We trapped H$$_{2}$$ in a CO$$_2$$ film at 5.4 K and detected the induced infrared-absorption band including both the components of ortho and para H$$_{2}$$. By analyzing its time-evolution, the conversion rate was determined to be 9.4 $$times$$ 10$$^{-4}$$ s$$^{-1}$$. We confirmed that this fast conversion was induced just by the CO$$_2$$ film with the uniquely unstable structure. We also identified H$$_{2}$$ at another kind of trapping sites, accompanied by higher anisotropy of the confining potential, and estimated its conversion rate to be 6 $$times$$ 10$$^{-3}$$ s$$^{-1}$$.


Two-parameter model for optimizing target beam distribution with an octupole magnet

明午 伸一郎; 大井 元貴; 藤森 寛*

Physical Review Accelerators and Beams (Internet), 23(6), p.062802_1 - 062802_24, 2020/06

 被引用回数:0 パーセンタイル:100(Physics, Nuclear)

加速器駆動の核変換システム(ADS)や核破砕中性子源に用いられる陽子加速器のビーム出力増強につれ、ビーム窓や標的の損傷は深刻な問題となり、損傷緩和のためにビーム電流密度の均一化が重要となる。密度均一化のため比較的よく用いられるラスター磁石には、故障時のビーム集束の重大な問題がある。一方、非線形光学を用いたビーム平坦化にははビーム拡大の問題があることが指摘され、これまで非線形効果導入の八極磁石におけるビームの角度の広がりを無視したフィラメント近似模型による検討が行われた。フィラメント近似模型では、非線形収斂作用を適切に評価できないため、本研究では一般化した非線形モデルの適用により非線形ビーム光学における収斂および発散作用を詳細に検討した。正規化した八極強度$$ K^{*}_8 $$と位相進行$$phi$$における$$cotphi$$の2つのパラメータ導入により、非線形効果を特定な条件によらず一般化できることを明確にした。ビームのピーク密度低減と損失最小化という拮抗する問題の解決には、$$K^{*}_8 sim $$ 1および$$ cotphisim$$ 3とすることにより解決できることが判明した。J-PARCの陽子ビーム輸送系(3NBT)に本検討結果を適用し、核破砕中性子源の水銀標的入口のビーム形状の比較検討した結果、モデル計算によるビーム分布は実験データとよい一致を示し、線形光学においてピーク電流密度を約50%にできることを示した。


Evidence for magnon-phonon coupling in the topological magnet Cu$$_{3}$$TeO$$_{6}$$

Bao, S.*; Cai, Z.*; Si, W.*; Wang, W.*; Wang, X.*; Shangguan, Y.*; Ma, Z.*; Dong, Z.-Y.*; 梶本 亮一; 池内 和彦*; et al.

Physical Review B, 101(21), p.214419_1 - 214419_8, 2020/06

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

We perform thermodynamic and inelastic neutron scattering (INS) measurements to study the lattice dynamics (phonons) of a cubic collinear antiferromagnet Cu$$_{3}$$TeO$$_{6}$$ which hosts topological spin excitations (magnons). While the specific heat and thermal conductivity results show that the thermal transport is dominated by phonons, the deviation of the thermal conductivity from a pure phononic model indicates that there is a strong coupling between magnons and phonons. In the INS measurements, we find a mode in the excitation spectra at 4.5 K, which exhibits a slight downward dispersion around the Brillouin zone center. This mode disappears above the N$'{e}$el temperature and thus cannot be a phonon. Furthermore, the dispersion is distinct from that of a magnon. Instead, it can be explained by the magnon-polaron mode, collective excitations resulting from the hybridization between magnons and phonons. We consider the suppression of the thermal conductivity and emergence of the magnon-polaron mode to be evidence for magnon-phonon coupling in Cu$$_{3}$$TeO$$_{6}$$.


$$q$$=0 long-range magnetic order in centennialite CaCu$$_{3}$$(OD)$$_{6}$$Cl$$_{2}$$ $$cdot$$ 0.6D$$_{2}$$O; A Spin-$$frac{1}{2}$$ perfect kagome antiferromagnet with $$J_{1}$$-$$J_{2}$$-$$J_{d}$$

飯田 一樹*; 吉田 紘行*; 中尾 朗子*; Jeschke, H. O.*; Iqbal, Y.*; 中島 健次; 河村 聖子; 宗像 孝司*; 稲村 泰弘; 村井 直樹; et al.

Physical Review B, 101(22), p.220408_1 - 220408_6, 2020/06

鉱物センテニアライトCaCu$$_{3}$$(OD)$$_{6}$$Cl$$_{2}$$ $$cdot$$ 0.6D$$_{2}$$Oの結晶構造と磁気構造をシンクロトロンX線回折と中性子回折測定に密度汎関数理論(DFT)と疑似フェルミオン汎関数繰り込み群(PFFRG)の計算を組み合わせることで調べた。CaCu$$_{3}$$(OD)$$_{6}$$Cl$$_{2}$$ $$cdot$$ 0.6D$$_{2}$$OではCu$$^{2+}$$イオンは反強磁性$$J_{1}$$と幾何学的に完全なカゴメネットワークを形成する。Cu$$^{2+}$$とCa$$^{2+}$$イオン間のサイト間無秩序は見つからなかった。CaCu$$_{3}$$(OD)$$_{6}$$Cl$$_{2}$$ $$cdot$$ 0.6D$$_{2}$$Oは$$T$$$$_{rm N}$$=7.2K以下で磁気秩序を示し、負のベクトルスピンキラリティーを持つ$$q$$=0の磁気構造が現れる。0.3Kでの秩序モーメントは0.58(2)$$mu$$Bに抑えられている。我々のDFT計算では、この系が量子臨界点の近くにあり、$$J_{1}$$-$$J_{2}$$-$$J_{d}$$カゴメ反強磁性体の優れた実現であることを示唆している。


Magnetically induced electric polarization in Ba$$_{3}$$Fe$$_{2}$$O$$_{5}$$Cl$$_{2}$$ with tunable direction in three dimensions

阿部 伸行*; 塩澤 俊介*; 松浦 慧介*; 佐賀山 基*; 中尾 朗子*; 大原 高志; 徳永 祐介*; 有馬 孝尚*

Physical Review B, 101(18), p.180407_1 - 180407_5, 2020/05

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

The correlation between magnetism and electric polarization in a chiral insulating magnet Ba$$_{3}$$Fe$$_{2}$$O$$_{5}$$Cl$$_{2}$$ has been investigated. The temperature dependence of magnetic susceptibility shows an anomaly at 564 K, suggesting the onset of antiferromagnetic order of Fe$$^{3+}$$ moments. Electric polarization appears in a magnetic field below TN due to the spin-direction-dependent metal-ligand hybridization. The direction of the electric polarization can be controlled in three-dimensional space by changing the direction of an external magnetic field. This compound also shows an antiferromagnetic-to-weak-ferromagnetic transition accompanied by a structural phase transition at 140 K.


Nuclear quantum effect for hydrogen adsorption on Pt(111)

Yan, L.*; 山本 良幸*; 志賀 基之; 杉野 修*

Physical Review B, 101(16), p.165414_1 - 165414_9, 2020/04



Manipulation of saturation magnetization and perpendicular magnetic anisotropy in epitaxial Co$$_{x}$$Mn$$_{4-x}$$N films with ferrimagnetic compensation

伊藤 啓太*; 安富 陽子*; Zhu, S.*; Nurmamat, M.*; 田原 昌樹*; 都甲 薫*; 秋山 了太*; 竹田 幸治; 斎藤 祐児; 小口 多美夫*; et al.

Physical Review B, 101(10), p.104401_1 - 104401_8, 2020/03

 被引用回数:1 パーセンタイル:31.73(Materials Science, Multidisciplinary)

Spintronics devices utilizing a magnetic domain wall motion have attracted increasing attention, and ferrimagentic materials with almost compensated magnetic moments are highly required to realize the fast magnetic domain wall motion. Here, we report a key function for this purpose in anti-perovskite Co$$_{x}$$Mn$$_{4-x}$$N films. Perpendicular magnetization emerges for $$0.8 leq x$$, and the saturation magnetization reaches a minimum value at $$x = 0.8$$.


Majorana corner flat bands in two-dimensional second-order topological superconductors

Kheirkhah, M.*; 永井 佑紀; Chen, C.*; Marsiglio, F.*

Physical Review B, 101(10), p.104502_1 - 104502_9, 2020/03

 被引用回数:2 パーセンタイル:14.76(Materials Science, Multidisciplinary)



Self-learning Monte Carlo method with Behler-Parrinello neural networks

永井 佑紀; 奥村 雅彦; 田中 章詞*

Physical Review B, 101(11), p.115111_1 - 115111_12, 2020/03

 被引用回数:4 パーセンタイル:8.09(Materials Science, Multidisciplinary)



Crystal structure and magnetism of MnO under pressure

Klotz, S.*; 小松 一生*; Polian, A.*; 町田 真一*; 佐野 亜沙美; Iti$'e$, J.-P.*; 服部 高典

Physical Review B, 101(6), p.064105_1 - 064105_6, 2020/02

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

マンガン酸化物(MnO)は、反強磁性モット絶縁体の典型物質である。今回、我々は、高圧下においてネール温度$$T_{N}$$を挟んだ温度域で磁気秩序と格子歪の相互作用を、X線および中性子回折により調べた。その結果、体積歪は圧力に対して鈍感であること、$$T_{N}$$$$T_{N}/dP$$=+4.5(5)K/GPaで上昇すること、格子歪$$alpha$$$$dalpha/dP$$=+0.018$$^{circ}$$/GPaで増大することがわかった。これらの結果は、$$J_{1}$$, $$J_{2}$$相互作用定数の原子間距離への影響を調べることや、また第一原理計算による理論予測と比較を可能にする。反強磁性相互作用に起因する散漫散乱は、$${approx}$$1.2$$T_{N}$$まで観測され、長距離秩序は、室温では42GPaで現れる。

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