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蓬田 匠; Scaria, J.*; Fablet, L.*; 徳永 紘平; 出井 俊太郎; 東 晃太朗*; 河村 直己*; 高橋 嘉夫*; Marsac, R.*
Chemical Communications, 61(91), p.17926 - 17929, 2025/11
本研究では、U(VI)からU(V)およびU(IV)への還元反応において、磁鉄鉱のstoichiometry(0 
R = Fe(II)/Fe(III) 0.5)がUの酸化還元反応に与える影響を明らかにした。磁鉄鉱のRは、構造中のFe(II)の酸化やプロトン/リガンドにより促進される溶解により容易に変化することが知られているが、これまでの研究ではU(V)の生成反応に関するRの影響は評価されていなかった。本研究では、異なるRを持つ磁鉄鉱上におけるUの電子状態を調べるため、U L
端HERFD-XANES分光法を用い、磁鉄鉱上のU(V)による特異的なピーク分裂を観察した。また、異なる条件下で行った吸着実験の結果、U(V)種が広範な条件下で高い安定性を示すことを示し、10日間の反応時間を経た後でも磁鉄鉱上で安定に存在していることが示された。最も重要な知見として、pHと酸化還元条件に依存して存在量が変化する、磁鉄鉱構造中のFe(II)がU(V)の安定化に重要な役割を果たしていることが明らかになった。
Mn
N and Fe
Co
N filmsYin, W.*; 伊藤 啓太*; 坪和 優佑*; 辻川 雅人*; 白井 正文*; 梅津 理恵*; 高梨 弘毅
Journal of Magnetism and Magnetic Materials, 628, p.173157_1 - 173157_8, 2025/09
被引用回数：0 パーセンタイル：0.00(Materials Science, Multidisciplinary)Fe
N exhibits a large anomalous Nernst effect (ANE), which motivates a systematic study of enhancing the anomalous Nernst coefficient (S
) by modulating its electronic and magnetic structures. In this study, Mn and Co substitution effects for Fe in FeN on S
were investigated. FeMnN and FeCoN films in wide ranges of x and y were grown epitaxially on MgO(001) and (LaAlO
)
(Sr
TaAlO
)
(001) substrates, respectively, using molecular beam epitaxy. The S value of the FeN film is suppressed by substituting Fe with Mn or Co. By measuring the ANE, Seebeck effect, and anomalous Hall effect, the transverse thermoelectric conductivity (
) was evaluated. The composition dependence of S was dominated by the change of for both FeMnN and FeCoN films. First-principles calculations were conducted for the transverse electric conductivity (
) and of FeN and Fe
Co
N, and large leading to large S was predicted in FeCoN.
軽部 皓介*; 大貫 惇睦*; 中島 多朗*; Chen, H.-Y.*; 石塚 大晃*; 木俣 基*; 大原 高志; 宗像 孝司*; 野本 拓也*; 有田 亮太郎*; et al.
npj Quantum Materials (Internet), 10, p.55_1 - 55_9, 2025/06
The Hall effect is one of the most fundamental but elusive phenomena in condensed matter physics due to the rich variety of underlying mechanisms. Here we report an exceptionally large Hall effect in a frustrated magnet, GdCu, with high conductivity. The Hall conductivity at the base temperature shows abrupt sign changes under magnetic fields. Our systematic measurements indicate that the unusual Hall effect can be understood in terms of spin-splitting-induced emergence/disappearance of Fermi pockets as well as skew scattering from spin-chiral cluster fluctuations in a field-polarized state. The present study demonstrates a complex interplay among magnetization, spin-dependent electronic structure, and spin fluctuations in producing the giant Hall effect in highly conductive frustrated magnets with a distorted triangular lattice.
玉造 博夢; 内原 猛*; 満田 節生*; 石井 祐太*; 中尾 裕則*; 竹端 寛治*; 今中 康貴*
Physical Review B, 111(13), p.134403_1 - 134403_9, 2025/04
被引用回数：1 パーセンタイル：58.65(Materials Science, Multidisciplinary)In multiferroic CuFe
Al
O, applying uniaxial pressure 
generates a magnetoferroelectric phase distinct from the well-studied spin-driven ferroelectric phase associated with helical magnetic ordering in this system. Using a four-circle neutron diffractometer, the magnetic structure of the -induced magnetoferroelectric phase is determined as the collinear sinusoidal type, which itself does not break the inversion symmetry in this system. Additionally, synchrotron radiation X-ray diffraction experiments are conducted to investigate how the triangular lattice in CuFeAlO is distorted by applied . Although lattice distortion during the magnetic phase transition in CuFeAlO is mitigated by the substitution of nonmagnetic Al
, the application of along the conjugate direction revives the "latent" spin-lattice coupling, causing the triangular lattice to distort during magnetic phase transition. The application of a magnetic filed considerably reduces -induced ferroelectric polarization, but does not affect lattice distortion. These results indicate that -induced ferroelectric polarization is not a consequence of the piezoelectric effect. Instead, the sinusoidal magnetic structure would contribute to the emergence of -induced ferroelectric polarization through spin-lattice coupling.
GeTe
to hydrostatic pressureWang, Y.*; Zeng, X.-T.*; Li, B.*; Su, C.*; 服部 高典; Sheng, X.-L.*; Jin, W.*
Chinese Physics B, 34(4), p.046203_1 - 046203_6, 2025/03
被引用回数：0 パーセンタイル：0.00(Physics, Multidisciplinary)二次元ファンデルワールス強磁性体FeGeTe(FGT)は、その高いキュリー温度、容易な調整性、空気中での優れた構造安定性から、スピントロニクスデバイスへの応用に大きな可能性を秘めている。理論的研究により、外部パラメータとしての圧力が強磁性特性に大きく影響することが示されている。本研究では、5GPaまでの高圧中性子粉末回折(NPD)実験を行い、FGTの静水圧による構造及び磁気特性の変化を調べた。NPDデータは、静水圧による見かけ上の抑制にもかかわらず、FGTにおける強磁性の頑健性を明らかにした。圧力が0から5GPaまで増加すると、キュリー温度は225(5)Kから175(5)Kまで単調減少し、Feの秩序モーメントが劇的に抑制されることがわかった。圧力による構造相転移は5GPaまで観測されなかったが、結合長と結合角の変化を定量的に解析した結果、交換相互作用が大きく変化していることがわかった。
Scaria, J.*; P
drot, M.*; Fablet, L.*; 蓬田 匠; Nguyen, T. T.*; Sivry, Y.*; Catrouillet, C.*; Pradas del Real, A. E.*; Choueikani, F.*; Vantelon, D.*; et al.
Environmental Science & Technology, 59(11), p.5747 - 5755, 2025/03
被引用回数：3 パーセンタイル：95.90(Engineering, Environmental)クロム(Cr)とマグネタイトの相互作用メカニズムを理解し予測することは、環境中のCrの物地球化学的挙動を解明し、最適な土壌浄化および水処理戦略を開発する上で特に重要である。最も毒性の高いCr(VI)がCr(III)に還元されて除去されることは広く報告されているが、Cr(III)のマグネタイトへの吸着に関わる正確なメカニズムは解明されていなかった。本研究では、Cr(III)溶液と10nmサイズのマグネタイトの相互作用を調べた。本研究では、pHとマグネタイトの化学量論の双方がCr(III)吸着メカニズムに及ぼす複合的な影響を調べることで、Cr(III)-(hydr)Oxide沈殿の生成が必ずしも溶液からのCr(III)の除去を駆動するプロセスではないことが明らかになった。これらの結果は、環境中のCrの輸送と終着点の予測、およびマグネタイトを用いたCr浄化プロセスの開発に役立つと期待される。
Chung, J.-H.*; Kwangwoo, S.*; Yokoo, Tetsuya R.; 植田 大地*; 今井 正樹; Kim, H.-S.; Kiem, D. H.; Han, M. J.*; 社本 真一
Scientific Reports (Internet), 15, p.5978_1 - 5978_10, 2025/02
被引用回数：0 パーセンタイル：61.64(Multidisciplinary Sciences)Two dimensional honeycomb ferromagnets host massless Dirac magnons which are a bosonic analogue of Dirac fermions in graphene. The Dirac magnons may become massive and topological when the time-reversal symmetry breaks and an energy gap opens up at the Dirac point, which was experimentally observed in Cr-based van der Waals magnets. Here, we investigate the spin wave excitations in the 
magnetic oxide FeTiO with Fe
electrons (
). Using inelastic neutron scattering, we observe two magnon bands separated by a 1.2-meV gap at the Dirac points indicating that its Dirac magnons are massive. Using the linear spin-wave and density functional theory calculations, we find that the spin-orbit-coupled antisymmetric Dzyaloshinskii-Moriya exchanges can best account for the observed Dirac gap opening. The associated Berry curvature and Chern number (
) indicate that FeTiO hosts topological spin excitations via time-reversal symmetry breaking of Dirac magnons.
前田 瑞穂*; 松田 達磨*; 芳賀 芳範; 白崎 謙次*; 木村 憲彰*
Journal of the Physical Society of Japan, 94(2), p.024707_1 - 024707_6, 2025/01
被引用回数：0 パーセンタイル：0.00(Physics, Multidisciplinary)We investigate the pressure dependence of the magnetoresistivity and Hall resistivity for an itinerant-electron metamagnet UCoAl. The first-order metamagnetic transition point varies as a function of hydrostatic pressure and terminates at the critical pressure 2.0 GPa. The electronic system, however, does not show criticality at this pressure but extends to higher pressures, unlike the usual quantum critical behavior.
井戸村 泰宏
Physics of Plasmas, 31(10), p.102504_1 - 102504_10, 2024/10
被引用回数：0 パーセンタイル：0.00(Physics, Fluids & Plasmas)トカマクプラズマにおける水素同位体混合現象をfull-fジャイロ運動論シミュレーションを用いて解析した。モデルプラズマのパラメータは、重水素(D)ペレットを水素(H)プラズマに入射した後にエネルギー閉じ込め時間スケールで水素同位体混合が発生したJETの水素同位体ペレット実験に基づいて選択した。重水素ペレット入射前後のプラズマ分布を用いて2つの数値実験を行った。どちらの場合も、炉心の乱流揺動はイオン温度勾配駆動乱流によって特徴づけられるが、後者の場合、外側の領域に捕捉電子モード乱流が存在する。前者の場合、バルクHイオンの密度分布は準定常状態に保たれ、その粒子閉じ込め時間はエネルギー閉じ込め時間よりも一桁長い。後者の場合、バルクHイオンとペレットDイオンの密度分布は、エネルギー閉じ込め時間の時間スケールで過渡的な緩和を示し、早い水素同位体混合を示す。トロイダル角運動量バランスから、水素同位体混合はトロイダル電場応力によって駆動されることがわかった。
O and CoFeO nanoparticles for removal of Sr and Cs
from radioactively contaminated water伊藤 あずさ; Thirunavukkarasu, G.*; Hriljac, J. A.*
Frontiers in Environmental Chemistry (Internet), 5, p.1445482_1 - 1445482_19, 2024/09
SiOコートしたFeOとCoFeOの超常磁性ナノ粒子を付加したゼオライトA、ゼオライトX及びNa、K型チャバサイトの開発を行い、それらの結晶構造に関わる分析及びイオン交換試験よって、吸着材としての特性を評価した。これら吸着材の合成は、次の3ステップで行った。まず、ソルボサーマル法でFeOとCoFeOのナノ粒子を合成し、次に、最初に合成したFeOとCoFeOのナノ粒子をゾルゲル法でSiOコートした。最後に、ゼオライト合成過程でMO/SiOをゼオライトに付加した。合成後、これら磁性ゼオライトをX線回析法、蛍光X線分析、ラマン分光法、試料振動型磁力計、走査電子顕微鏡及び透過型電子顕微鏡で分析した。それらの結果から、MO/SiO粒子をゼオライトに付加した後も超常磁性を保っていたことが分かった。また、磁性ゼオライトAとゼオライトXのSr吸着能評価、及び磁性Na、K型チャバザイトのCs吸着能評価をイオン交換試験で行った。これらのイオン交換試験よって、MO/SiO粒子がゼオライトの吸着サイトを塞ぐことなく、また、イオン交換試験後もMO/SiO粒子がゼオライトから脱離していないことを確認した。
Ding, H.*; 伊藤 啓太*; 遠藤 恭*; 高梨 弘毅; 関 剛斎*
Journal of Physics D; Applied Physics, 57(38), p.385002_1 - 385002_10, 2024/09
被引用回数：2 パーセンタイル：56.72(Physics, Applied)This paper reports the systematic study on the structure, magnetic properties and magnetoelastic properties for the Fe
Ga (001) thin films epitaxially grown on the different substrates of GaAs(001) and MgO(001) using the sputtering technique. The alloy composition dependence of effective magnetoelastic coupling coefficient B
along the FeGa [110] direction indicated that the largest magnetoelastic coupling was obtained for the Fe-Ga layer with x = 30 grown on the MgO substrate. Considering the results of structural analysis and magnetization measurement, the different crystallite sizes depending on the kind of substrate may give rise to the different magnetoelastic coupling strengths between the Fe-Ga layers on the MgO and the GaAs. The magnetostriction along the FeGa [111] direction was also estimated with the assumption of plausible elastic property of Fe-Ga, and showed the values comparable to the reported value of bulk Fe-Ga. This means the large magnetostriction can be obtained even for the Fe-Ga thin films epitaxially grown not only on the GaAs(001) but also on the MgO(001). The findings in this work will give a guideline for designing spintronic applications with a Fe-Ga layer exhibiting a large magnetoelastic coupling.
Zhu, L.*; He, H.*; Naeem, M.*; Sun, X.*; Qi, J.*; Liu, P.*; Harjo, S.; 中島 健次; Li, B.*; Wang, X.-L.*
Physical Review Letters, 133(12), p.126701_1 - 126701_6, 2024/09
被引用回数：4 パーセンタイル：77.74(Physics, Multidisciplinary)It has long been suspected that magnetism could play a vital role in the phase stability of multi- component high-entropy alloys. However, the nature of the magnetic order, if any, has remained elusive. Here, by using elastic and inelastic neutron scattering, we demonstrate evidence of antiferromagnetic order below 
80 K and strong spin fluctuations persisting to room temperature in a single-phase face-centered cubic (fcc) CrMnFeCoNi high-entropy alloy. Despite the chemical complexity, the magnetic structure in CrMnFeCoNi can be described as 
-Mn-like, with the magnetic moments confined in alternating (001) planes and pointing toward the 
111
direction. Combined with first-principles calculation results, it is shown that the antiferromagnetic order and spin fluctuations help stabilized the fcc phase in CrMnFeCoNi high-entropy alloy.
Vali
ka, M.*; Haidamak, T.*; Cabala, A.*; Posp
il, J.*; Bastien, G.*; Sechovsk
, V.*; Prokleka, J.*; 柳澤 達也*; Opletal, P.; 酒井 宏典; et al.
Physical Review Materials (Internet), 8(9), p.094415_1 - 094415_9, 2024/09
被引用回数：2 パーセンタイル：25.98(Materials Science, Multidisciplinary)Elastic responses at the metamagnetic transition in UTe are studied at high field. The elastic anomaly becomes the strongest at the critical-end-point. Similar behavior was also observed in another metamagnet UCoAl, suggesting a universal elastic response triggered by critical magnetic fluctuations.
高梨 弘毅; 関 剛斎*
まぐね, 19(3), p.100 - 106, 2024/06
薄膜の垂直磁気異方性は、磁気記録のみならずスピントロニクスにおいても重要な役割を果たしている。本解説記事では、垂直磁気異方性に関して、磁気多層膜、規則合金膜、希土類遷移金属アモルファス合金多層膜、不均一膜やグラニュラー膜など、垂直磁化を持つ具体例を示しながら、基礎からこれまでの研究、そして最近の研究動向を概説する。それぞれの具体例について、構造対称性の破れによる界面磁気異方性、ひずみによる磁気弾性異方性、バルクの結晶磁気異方性、原子の方向性規則配列などの垂直磁気異方性の物理的起源を議論する。
中島 多朗*; 渡辺 真朗; 稲村 泰弘; 玉造 博夢; 他8名*
Physical Review Research (Internet), 6(2), p.023109_1 - 023109_9, 2024/05
We present proof-of-principle experiments of stroboscopic time-of-flight (TOF) neutron diffraction in long pulsed magnetic fields. By utilizing electric double-layer capacitors, we developed a long pulsed magnet for neutron diffraction measurements, which generates pulsed magnetic fields with the full widths at half maximum of more than 100 ms. The field variation is slow enough to be approximated as a steady field within the time scale of a polychromatic neutron pulse passing through a sample placed in a distance of the order of 10 m from the neutron source. This enables us to efficiently explore the reciprocal space using a wide range of neutron wavelength in high magnetic fields. We applied this technique to investigate field-induced magnetic phases in the triangular lattice antiferromagnets CuFe
GaO (x = 0, 0.035).
船引 雄太*; 伊與田 宗慶*; 菖蒲 敬久; 松田 朋己*; 林 雄二郎*; 佐野 智一*; 他8名*
Journal of Manufacturing Processes, 115, p.40 - 55, 2024/04
被引用回数：5 パーセンタイル：67.50(Engineering, Manufacturing)In resistance spot welding (RSW) of Fe and Al alloy, an intermetallic compound (IMC) is formed at the joining interface, and it is known that the joining strength of the joint decreases as the IMC becomes thicker. In this study, the convection behavior in the Al alloy melting zone of an Fe-Al alloy RSW was varied and the effect on the joint characteristics was investigated. For this study, focusing on the electromagnetic force generated in the Al alloy melting zone, the convection behavior in the Al alloy melting zone was changed by adding an external magnetic field using neodymium magnets. In-situ evaluation of the convection behavior using synchrotron radiation and cross-sectional macro-observation of the joint revealed that the addition of an external magnetic field causes a non-axisymmetric change in the convection behavior in the Al alloy melting zone, which results in the deflection of the Al alloy melting zone. The addition of an external magnetic field increases the driving force of convection and homogenizes the temperature field at the joining interface, suggesting that the IMC near the center is formed thin and uniform. Furthermore, from the cross tension test and the observation of the fracture surface of the joint after the test, it was clarified that the CTS of the joint with an external magnetic field was improved by the propagation of cracks into the Al alloy melting zone during the test.
竹内 徹也*; 本多 史憲*; 青木 大*; 芳賀 芳範; 木田 孝則*; 鳴海 康雄*; 萩原 政幸*; 金道 浩一*; 軽部 皓介*; 播磨 尚朝*; et al.
Journal of the Physical Society of Japan, 93(4), p.044708_1 - 044708_10, 2024/04
被引用回数：0 パーセンタイル：0.00(Physics, Multidisciplinary)Electrical and magnetic properties of divalent europium antiferromagnet EuTe are studied on single crystals grown from Te-flux method. Antiferromagnetism occurs at 11 K with an insulating ground state. Application of magnetic field induces a sudden resistance drop leading to a phase transition to metallic state. Energy band calculations reveal the appearance of a Fermi surface pocket with Te-5p character induced by the polarized Eu moments.
-FeNi films with island structures on LaAlO(110) substrates by nitrogen insertion and topotactic extraction西尾 隆宏*; 伊藤 啓太*; 藏 裕彰*; 高梨 弘毅; 柳原 英人*
Journal of Alloys and Compounds, 976, p.172992_1 - 172992_8, 2024/03
被引用回数：3 パーセンタイル：44.62(Chemistry, Physical)Tetrataenite (L1-FeNi) has potential for application in next-generation permanent magnets. This compound is a rare-earth-free material comprising Fe and Ni, which are abundant elements. In addition, an extremely high uniaxial magnetocrystalline anisotropy (
u) is expected for L1-FeNi because of the ordered arrangement of the elements. This study reports the magnetic properties of uniaxially oriented L1-FeNi films with island structures fabricated by a novel method involving the radio-frequency sputter deposition of FeNi alloy films onto a LaAlO(110) substrate, followed by nitrogen insertion and topotactic extraction. FeNiN(110) films are epitaxially grown on the LAO(110) plane by the nitriding and additional annealing process of the FeNi alloy films at high temperatures under ammonia gas to reduce the volume fraction of crystallographic variants. Uniaxially oriented L1-FeNi alloy films with island structures are obtained after the topotactic denitriding of the FeNiN films. The uniaxial magnetic anisotropy of the L1-FeNi films is determined from the magnetization curves and via magnetic torque measurements of the films. The obtained L1-FeNi film exhibiting a relatively high superlattice order parameter of 0.74 yielded a uniaxial magnetocrystalline anisotropy energy of ~0.63 MJ/m
at 300 K, as well as coercivities of 319 and 358 kA/m at 300 and 10 K, respectively. This coercivity is the highest value reported for artificial L1-FeNi to date.
CoSi山内 宏樹; Sari, D. P.*; 安井 幸夫*; 坂倉 輝俊*; 木村 宏之*; 中尾 朗子*; 大原 高志; 本田 孝志*; 樹神 克明; 井川 直樹; et al.
Physical Review Research (Internet), 6(1), p.013144_1 - 013144_9, 2024/02
-Mn-type family alloys Mn
have three-dimensional antiferromagnetic (AFM) corner-shared triangular network. The antiferromagnet MnRhSi shows magnetic short-range order (SRO) over a wide temperature range of approximately 500 K above the N
el temperature 
= 190 K. MnCoSi has the smallest lattice parameter and the lowest in the family compounds. The quantum critical point (QCP) from AFM to the quantum paramagnetic state is expected near a cubic lattice parameter of 6.15 
of MnCoSi is only 140 K, quantum critical behavior is observed in MnCoSi as the enhancement of the electronic specific heat coefficient . We study how the magnetic SRO appears in MnCoSi by using neutron scattering, 
SR, and physical property measurements. The experimental results show that the neutron scattering intensity of the magnetic SRO does not change much regardless of the suppressed magnetic moment in the long-range magnetic ordered state compared to those of MnRhSi. The initial asymmetry drop ratio of SR above becomes small, and the magnetic SRO temperature 
is suppressed to 240 K. The results suggest that the MnCoSi is close to the QCP in the Mn system.
末次 祥大*; 酒井 宏典; Opletal, P.; 常盤 欣文; 芳賀 芳範; 他12名*
Science Advances (Internet), 10(6), p.eadk3772_1 - eadk3772_6, 2024/02
被引用回数：22 パーセンタイル：98.08(Multidisciplinary Sciences)The superconducting gap structure of UTe was determined by the thermal conductivity measurement on ultra-clean UTe single crystals. The result demonstrates the absence of nodes around the 
-axis, contrary to the previous study. The finding reveals that UTe is likely to be a long-sought three-dimensional strong topological superconductor.
