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論文

Spin density wave and van Hove singularity in the kagome metal CeTi$$_3$$Bi$$_4$$

Park, P.*; Ortiz, B. R.*; Spargue, M.*; Sakuya, A. P.*; Chen, S. A.*; Frontzek, M. D.*; Tian, W.*; Sibille, R.*; Mazzone, D. G.*; 田端 千紘; et al.

Nature Communications (Internet), 16, p.4384_1 - 4384_9, 2025/05

 被引用回数:0

Kagome metals with van Hove singularities (VHSs) near the Fermi level can host intriguing quantum phenomena, including chiral loop currents, electronic nematicity, and unconventional superconductivity. However, unconventional magnetic states driven by VHSs, such as spin-density waves (SDWs), have yet to be observed experimentally in kagome metals. Here, we present a comprehensive investigation of the magnetic and electronic structure of the layered kagome metal CeTi$$_3$$Bi$$_4$$, where the Ti kagome electronic structure interacts with a magnetic sublattice of Ce$$^{3+}$$ $$J_{rm eff}$$ = 1/2 moments. Our findings establish the rare-earth Kagome metals LnTi3Bi4 as a model platform where characteristic electronic structure of the kagome lattice plays a pivotal role in magnetic order.

論文

Spin-singlet ground state with spin gap in $$S_{rm eff}$$ = $$frac{1}{2}$$ antiferromagnetic tetramer compound Yb$$_2$$SiO$$_5$$

長谷 正司*; 金子 耕士; 田端 千紘; 山内 宏樹; 辻井 直人*; D$"o$nni, A.*

Physical Review B, 111(9), p.094403_1 - 094403_9, 2025/03

 被引用回数:0 パーセンタイル:0.00(Materials Science, Multidisciplinary)

We studied magnetic properties of Yb$$_2$$SiO$$_5$$ having pseudospins of $$S_{rm eff}$$ = $$frac{1}{2}$$ using magnetization, specific heat, and inelastic neutron scattering (INS) measurements. We observed cluster-like excitations in the INS measurements. We determined that the spin system in Yb$$_2$$SiO$$_5$$ is the $$S_{rm eff}$$ = $$frac{1}{2}$$ AFM tetramer with two exchange interactions of $$J_1 = 0.74$$ and $$J_2 = 0.95$$~meV. The spin tetramer can explain the excitation energies, $$chi (T)$$, magnetic specific heat at $$T < 15$$~K, and the magnitude of the scattering vector ($$Q$$) dependence of the intensity [$$I(Q)$$] at 0.7 and 1.2 meV. The spin tetramer, however, cannot explain well $$I(Q)$$ at 1.9 meV and $$I(T)$$ of the three excitations probably due to effects of weak inter-tetramer interactions.

論文

Physical properties of intergrowth compound Eu$$_{2}$$CuZn$$_{2}$$P$$_{3}$$

May, A. F.*; 田端 千紘; Okamoto, Satoshi*; Ortiz, B. R.*; Christianson, A. D.*; Yan, J.*; 金子 耕士; McGuire, M. A.*

Physical Review Materials (Internet), 9(2), p.024406_1 - 024406_13, 2025/02

 被引用回数:0 パーセンタイル:0.00(Materials Science, Multidisciplinary)

The physical properties of single crystalline Eu$$_{2}$$CuZn$$_{2}$$P$$_{3}$$ were inspected via thermodynamic, transport, and neutron diffraction measurements. Eu$$_{2}$$CuZn$$_{2}$$P$$_{3}$$ is composed of EuCuP and EuZn$$_{2}$$P$$_{2}$$ motifs stacked in a one-to-one ratio. The magnetic response of Eu$$_{2}$$CuZn$$_{2}$$P$$_{3}$$ is similar to that of EuZn$$_{2}$$P$$_{2}$$ in its A-type antiferromagnetic (semiconducting) form.

論文

Large spontaneous Hall effect with flexible domain control in the antiferromagnetic material TaMnP

小手川 恒*; 中村 彰良*; Huyen, V. T. N.*; 新井 祐樹*; 藤 秀樹*; 菅原 仁*; 林 純一*; 武田 圭生*; 田端 千紘; 金子 耕士; et al.

Physical Review B, 110(21), p.214417_1 - 214417_8, 2024/12

 被引用回数:0 パーセンタイル:0.00(Materials Science, Multidisciplinary)

In this study, we show that the orthorhombic system TaMnP exhibits a large anomalous Hall conductivity (AHC) in spite of the small net magnetization. Neutron scattering experiment and the observation of the AH effect comprehensively suggest a dominant AF structure in TaMnP is represented by $$B_{3g}$$. The AHC is one of the largest among those observed in AF materials at zero fields. First-principles calculations suggest that the spin-orbit interaction originating in nonmagnetic Ta-5$$d$$ electrons significantly contributes to the enhancement of Berry curvatures in the momentum space. We found that the AF domain switching is triggered by the magnetic fields along all the crystal axes. This indicates that the AF domain determining the sign of the Hall response can be controlled even through the small net magnetization symmetrically different.

論文

Single helicity of the triple-$$q$$ triangular skyrmion lattice state in the cubic chiral helimagnet EuPtSi

松村 武*; 田端 千紘; 金子 耕士; 中尾 裕則*; 垣花 将司*; 辺土 正人*; 仲間 隆男*; 大貫 惇睦*

Physical Review B, 109(17), p.174437_1 - 174437_8, 2024/05

 被引用回数:4 パーセンタイル:74.90(Materials Science, Multidisciplinary)

We investigated the magnetic helicity of the triple-$$q$$ magnetic structure of the triangular skyrmion lattice in the A-phase of EuPtSi for a magnetic field along the [111] axis by resonant X-ray diffraction using a circularly polarized beam. We show that all three Fourier components of the triple-$$q$$ structure are perpendicular to the respective $$q$$ vectors and have the same helicity. They are connected by the rotation operations about the [111] axis. The helicity is the same as that of the single-$$q$$ helimagnetic phase at low fields, suggesting that the antisymmetric exchange interaction inherent in the chiral structure supports the formation of the triangular skyrmion lattice. We also observe that the helical plane in the helimagnetic phase is tilted to the magnetic field to form a conical structure before the first-order transition to the skyrmion lattice phase.

論文

Polarized neutron diffraction study on UPt$$_{2}$$Si$$_{2}$$

今 布咲子*; 田端 千紘; 齋藤 開*; 中島 多朗*; 日高 宏之*; 柳澤 達也*; 網塚 浩*

Journal of the Physical Society of Japan, 93(4), p.044701_1 - 044701_11, 2024/04

 被引用回数:0 パーセンタイル:0.00(Physics, Multidisciplinary)

We investigated the magnetic structure of the antiferromagnetic (AFM) ordered state ($$T_{rm N}$$ $$sim$$ 34 K) in tetragonal UPt$$_{2}$$Si$$_{2}$$ using polarized and unpolarized neutron diffraction. Previous neutron scattering studies reported that this system possesses a simple AFM structure with a propagation vector, Q= 0, and the ordered magnetic moments aligned along the c-axis. By contrast, our latest resonant X-ray scattering (RXS) experiments have revealed that the magnetic structure is modulated by the charge-density-wave (CDW) order, which emerges in one of the two Pt atomic layers in the unit cell below $$sim$$320 K. The modulation is characterized by a transverse wave in the c-plane, with the propagation vector of the CDW order, q$$_{rm CDW}$$ = ($$sim$$0.42, 0, 0). In this study using neutron scattering, we observed that the superlattice reflections specified by q$$_{rm CDW}$$ develop below $$T_{rm N}$$, in addition to the magnetic reflections with Q= 0, thereby further confirming the presence of modulation in the AFM structure of this system. From detailed analyses, we revealed that the amplitude of the transverse-wave magnetic modulation is 0.72(2)$$mu$$$$_{rm B}$$/U, which is quantitative information that can not be obtained through RXS experiments. This implies that the CDW drives the ordered magnetic moments to be tilted up to 20$$^{circ}$$ in the AFM state. The observations strongly suggest that the magnetism of UPt$$_{2}$$Si$$_{2}$$ is heavily influenced by the hybridization effects between the $$5f$$ electrons of U and the 5d electrons of Pt.

論文

Magnetic order in honeycomb layered U$$_2$$Pt$$_6$$Ga$$_{15}$$ studied by resonant X-ray and neutron scattering

田端 千紘; 今 布咲子*; 太田 玖吾*; 日比野 瑠央*; 松本 裕司*; 網塚 浩*; 中尾 裕則*; 芳賀 芳範; 金子 耕士

Physical Review B, 109(13), p.134403_1 - 134403_7, 2024/04

 被引用回数:2 パーセンタイル:40.97(Materials Science, Multidisciplinary)

Antiferromagnetic (AF) order of U$$_2$$Pt$$_6$$Ga$$_{15}$$ with the ordering temperature $$T$$$$_{rm N}$$ = 26 K was investigated by resonant X-ray scattering and neutron diffraction on single crystals. This compound possesses a unique crystal structure in which uranium ions form honeycomb layers and then stacks along the c-axis with slight offset, which gives rise to a stacking disorder. The AF order can be described with the propagation vector of q = (1/6, 1/6, 0) in the hexagonal notation. The ordered magnetic moments orient perpendicular to the honeycomb layers, indicating a collinear spin structure consistent with Ising-like anisotropy. The magnetic reflections are found to be broadened along c$$^{*}$$ indicating that the stacking disorder results in anisotropic correlation lengths. The semiquantitative analysis of neutron diffraction intensity, combined with group theory considerations based on the crystallographic symmetry, suggests a zig-zag type magnetic structure for the AF ground state, in which the AF coupling runs perpendicular to the stacking offset, characterized as q = (1, 0, 0). The realization of the zig-zag magnetic structure implies the presence of frustrating intralayer exchange interactions involving both ferromagnetic (FM) first-neighbor and AF second and third-neighbor interactions in this compound.

論文

New standard for low temperature sample environment at JAEA/JRR-3

金子 耕士; 田端 千紘; 萩原 雅人; 山内 宏樹; 大場 洋次郎; 熊田 高之; 久保田 正人; 児島 佑樹*; 生田目 望; 佐々木 未来; et al.

JPS Conference Proceedings (Internet), 41, p.011015_1 - 011015_6, 2024/03

We will introduce our recent update on low temperature system for neutron diffraction experiments. This is characterized by advantages such as liquid He free and sophisticated automatic temperature control functions, which can be a new standard for low temperature and high magnetic field experiments of neutron scattering.

論文

Neutron scattering study of antiferromagnet U$$_{2}$$Pt$$_{6}$$Al$$_{15}$$

太田 玖吾*; 松本 裕司*; 渡部 悠貴*; 金子 耕士; 田端 千紘; 芳賀 芳範

New Physics; Sae Mulli, 73(12), p.1170 - 1173, 2023/12

ハニカム格子を持つ反強磁性体U$$_{2}$$Pt$$_{6}$$Al$$_{15}$$の磁気構造を決定するために中性子散乱実験を行った。U$$_{2}$$Pt$$_{6}$$Al$$_{15}$$$$T_{rm m1}$$=9Kと$$T_{rm m2}$$=26Kで二つの相転移を示す。$$T_{rm m1}$$ $$<$$ $$T$$ $$<$$ $$T_{rm m2}$$の第一相では、$$kappa$$$$_{rm I}$$=(1/3, 0, 0)の伝搬ベクトルで記述される磁気反射が観測された。$$T$$$$<$$$$T_{rm m1}$$のフェーズIIでは、$$kappa$$$$_{rm I}$$=(1/3, 0, 0)と$$kappa$$$$_{rm II}$$=(1/2, 0, 0)の磁気反射が観測され、$$kappa$$$$_{rm I}$$=(1/3, 0, 0)の磁気反射強度は弱いが有限であった。温度依存強度のヒステリシスは$$T_{rm m1}$$での相転移にまたがって観測され、$$T_{rm m1}$$での転移が1次転移であることを示唆している。

論文

Incommensurate nature of the antiferromagnetic order in GdCu$$_2$$

金子 耕士; 田端 千紘; 萩原 雅人; 山内 宏樹; 久保田 正人; 長壁 豊隆; 大貫 惇睦*

Journal of the Physical Society of Japan, 92(8), p.085001_1 - 085001_2, 2023/08

 被引用回数:0 パーセンタイル:0.00(Physics, Multidisciplinary)

A magnetic order in orthorhombic GdCu$$_2$$ was investigated by a single crystal neutron diffraction with thermal neutron. Magnetic peaks were observed at incommensurate positions described by the ordering vector $$q$$=($${delta}$$~1~0) with $${delta}$$=0.678 at 4~K. This ordering vector is close to the commensurate one with $$q_c$$=(2/3~1~0) reported earlier, but clearly deviates. The incommensurate nature of the magnetic order in GdCu$$_2$$ is further corroborated by the peak shift with temperature below $$T_{rm N}$$.

論文

Crystallographic and/or magnetic properties of neutral and cationic uranium(IV) sandwiched phthalocyanine complexes

田端 千紘; 渡邊 博仁*; 白崎 謙次*; 砂賀 彩光*; 福田 貴光*; Li, D.*; 山村 朝雄*

Journal of Molecular Structure, 1277, p.134870_1 - 134870_8, 2023/04

 被引用回数:4 パーセンタイル:20.92(Chemistry, Physical)

中性およびカチオンのU(IV)サンドイッチ型フタロシアニン(Pc)錯体を調製した。中性種であるUPc$$_{2}$$はUCl$$_{4}$$とフタロニトリルの反応によって得られ、[UPc$$_{2}$$][BF$$_{4}$$]]の結晶は電解によって成長させた。これらの錯体の構造は、結晶学的に決定された。U(IV)イオンは2個の$$5f$$電子を持ち、この電子はUサイトに局在する磁気モーメントを担うため、この錯体は磁気的に活性である。UPc$$_{2}$$の帯磁率測定から、この系は2Kまで局所的な磁気モーメントを持つ常磁性であるが、配位子磁場効果により、その磁気モーメントが抑制されている可能性があることがわかった。また、ヒステリシスのない磁化曲線から常磁性であることが確認された。カチオン性錯体である[UPc$$_{2}$$][BF$$_{4}$$]は空間群$$P4nc$$の正方形構造で結晶化し、UPc$$_{2}$$分子は正方形の$$c$$軸に沿って積み重なっていることがわかった。この構造は[LnPc$$_{2}$$][BF$$_{4}$$]と似ているが、積層面には明瞭な乱れがあった。アクチノイド元素の多配位性を考慮した第一原理計算により、UPc$$_{2}$$と[UPc$$_{2}$$][BF$$_{4}$$]の結晶構造、分子構造の安定性と電子配置を評価した。

論文

Influence of additives on low-temperature hydrothermal synthesis of UO$$_{2+x}$$ and ThO$$_2$$

田端 千紘; 白崎 謙次*; 酒井 宏典; 砂賀 彩光*; Li, D.*; 小中 真理子*; 山村 朝雄*

CrystEngComm (Internet), 24(19), p.3637 - 3648, 2022/05

 被引用回数:2 パーセンタイル:30.55(Chemistry, Multidisciplinary)

Hydrothermal reactions of uranium(IV) nitrate solutions in the presence of aldehydes yielded microparticles of UO$$_{2+x}$$, at temperatures as low as 100$$^{circ}$$C. The synthesized products contained residual organic matter originating from aldehydes used as an additive, unless the synthesis temperature was 390$$^{circ}$$C. Additionally, the residual matter could be separated from the product by heat treatment at $$>$$ 300$$^{circ}$$C. The valence of uranium ions in the UO$$_{2+x}$$ products was found to be higher than that reported for UO$$_{2}$$. Low synthesis temperatures resulted in the suppression of the magnetic moments of uranium ions and the occurrence of the spin interaction among the ions. Therefore, the oxidation number of uranium averaged over the entire product could become higher than 4+. A comparative study with ThO$$_2$$ suggested that the redox reaction could be closely related to the hydrothermal synthesis reaction and particle growth of UO$$_{2+x}$$.

論文

Homogeneity of (U, $$M$$)O$$_2$$ ($$M$$ = Th, Np) prepared by supercritical hydrothermal synthesis

白崎 謙次*; 田端 千紘*; 砂賀 彩光*; 酒井 宏典; Li, D.*; 小中 真理子*; 山村 朝雄*

Journal of Nuclear Materials, 563, p.153608_1 - 153608_11, 2022/05

 被引用回数:4 パーセンタイル:53.26(Materials Science, Multidisciplinary)

添加剤を変えながらウラン酸化物(U, $$M$$)O$$_2$$ ($$M$$=Th, Np)固溶体を超臨界水熱合成で調製した。それらの試料の均質性をVegard則に基づいた結晶構造解析や、(U, Np, Na)O$$_2$$固溶体については、$$^{23}$$Na核核磁気共鳴(NMR)によって調べた。その結果、(i) (U, Th)O$$_{2+x}$$固溶体の場合は、炭酸アンモニウムを添加剤として、IV価ウランから出発し、(ii) (U, Np)O$$_{2+x}$$の場合は、エタノールを添加剤として、VI価ウランから出発すると、均質な試料が得られることがわかった。

論文

Supercritical hydrothermal synthesis of UO$$_{2+x}$$; Stoichiometry, crystal shape and size, and homogeneity observed using $$^{23}$$Na-NMR spectroscopy of (U, Na)O$$_{2+x}$$

田端 千紘*; 白崎 謙次*; 砂賀 彩光*; 酒井 宏典; Li, D.*; 小中 真理子*; 山村 朝雄*

CrystEngComm (Internet), 23(48), p.8660 - 8672, 2021/12

 被引用回数:7 パーセンタイル:63.97(Chemistry, Multidisciplinary)

超臨界水下においてウラン酸化物UO$$_2$$の水熱合成について調べた。得られたUO$$_{2+x}$$粒子について、その化学組成,結晶形,サイズ,均一性などを調べた結果、超臨界水熱合成法は、化学的に制御された均一なUO$$_{2+x}$$を合成するのに有効である可能性がある。

論文

Magnetic field induced triple-$$q$$ magnetic order in trillium lattice antiferromagnet EuPtSi studied by resonant X-ray scattering

田端 千紘*; 松村 武*; 中尾 裕則*; 道村 真司*; 垣花 将司*; 稲見 俊哉*; 金子 耕士; 辺土 正人*; 仲間 隆男*; 大貫 惇睦*

Journal of the Physical Society of Japan, 88(9), p.093704_1 - 093704_5, 2019/09

 被引用回数:44 パーセンタイル:88.96(Physics, Multidisciplinary)

The magnetic order in the magnetic-fild-induced so-called A phase of cubic chiral antiferromagnet EuPtSi was investigated by resonant X-ray scattering (RXS) near the Eu $$L_{2}$$ edge. The high flux RXS signal under the magnetic field applied along [111] revealed the first and second order satellite magnetic reflections, indicating that the A phase is a triple-$$q$$ magnetic ordered state that is described by three propagation vectors lying in the plane normal to the magnetic field direction; $$q_1$$, $$q_2$$, and $$q_3$$. With the high resolution in the reciprocal space achieved in the RXS measurement, it is suggested that the triple-$$q$$ order strongly couples with the underlying crystal lattice. The triple-$$q$$ magnetic order is discussed in the context of a magnetic skyrmion lattice on which the geometrical frustration may play a crucial role.

論文

X-ray backscattering study of crystal lattice distortion in hidden order of URu$$_2$$Si$$_2$$

田端 千紘*; 稲見 俊哉; 道村 真司*; 横山 淳*; 日高 宏之*; 柳澤 達也*; 網塚 浩*

Philosophical Magazine, 94(32-33), p.3691 - 3701, 2014/00

 被引用回数:16 パーセンタイル:56.89(Materials Science, Multidisciplinary)

We performed synchrotron X-ray diffraction measurements on a small single crystal of URu$$_2$$Si$$_2$$. A backscattering diffraction setup (2$$thetasim179.81^circ$$) in combination with a Si(6 6 0) monochromator ensures a high instrumental resolution of $$Delta d/d sim 7.3 times 10^{-6}$$, where $$d$$ denotes a lattice-plane spacing and $$Delta d$$ is its spread expressed as the full width at half maximum (FWHM). We carefully measured the (5 5 0) Bragg peak in the temperature range between 5 and 25 K, and found it to show no signature of broadening and splitting when "Hidden Order (HO)" sets in below 17.5 K. Temperature variation of the peak position closely follows the behaviour of the known linear thermal expansion coefficient. Detailed analysis of the peak width reveals that the tetragonal fourfold rotational symmetry of URu$$_2$$Si$$_2$$ is conserved in HO within the experimental accuracy of the orthorhombicity of $$|b-a|/(b+a)leq3.0times10^{-5}$$.

報告書

JMTR改良LEU炉心の熱水力解析

田畑 俊夫; 長尾 美春; 小向 文作; 那珂 通裕; 武田 卓士*; 藤木 和男

JAERI-Tech 2002-100, 108 Pages, 2003/01

JAERI-Tech-2002-100.pdf:4.44MB

JMTRの燃料の最高燃焼度を増加させて燃料をより有効に使用し、年間運転日数の増加を図れるよう、炉心構成の改良を検討した結果、改良LEU炉心として、従来のLEU炉心中央部の反射体要素2体に代えて燃料要素2体を追加した新しい炉心構成を決定した。本報告書は改良LEU炉心の安全評価にかかわる熱水力解析の結果をまとめたものである。解析の範囲は、熱設計にかかわる定常解析,運転時の異常な過渡変化及び事故について、それぞれ原子炉設置変更許可申請書の添付書類八,同十に記載された事象である。解析条件は核計算によって得られた熱水路係数等に基づいて保守的に定めた。解析により燃料温度,DNBR,一次系冷却水温度に関する安全上の判断基準を満足することを確認し、これらの結果は原子炉設置変更許可申請に使用された。改良LEU炉心についての設置許可は平成13年3月27日に取得し、同年11月の第142サイクルより同炉心による運転を開始した。

報告書

JMTR改良LEU炉心の核特性解析

小向 文作; 那珂 通裕; 田畑 俊夫; 長尾 美春; 武田 卓士*; 藤木 和男

JAERI-Tech 2002-067, 75 Pages, 2002/08

JAERI-Tech-2002-067.pdf:3.41MB

JMTRでは、燃料の燃焼度を増加させてより有効に利用することによって運転日数を大幅に増加させる検討を行った結果、従来のLEU炉心に対して標準燃料要素を新たに2体追加して燃料要素29体で構成された改良LEU炉心を考案した。本炉心の核特性をSRACコードシステムを用いて解析した結果、LEU炉心と比べて運転サイクル開始時の過剰反応度が若干大きくなるなどの違いはあるものの、JMTRの安全設計における核特性の設計方針を満足することを確認した。また、本炉心では1サイクル当たり最長32日までの運転が可能であり、燃料要素平均の燃焼度を最高約54%まで増加できることから、従来の4サイクル分の燃料要素消費数で年間180日以上の運転が可能なことがわかった。

論文

Feasibility study for improvement of efficient irradiation with LEU core in JMTR

那珂 通裕; 長尾 美春; 小向 文作; 田畑 俊夫

Proceedings of 7th Meeting of the International Group on Research Reactors (IGORR-7) (CD-ROM), 7 Pages, 1999/10

現在、JMTRはLEUとMEU燃料を使用した炉心により、年間4~5サイクル、1サイクル当たり約25日間の運転を行っているが、来年からはLEU燃料のみの炉心による運転が予定されている。また最近、年間の運転日数の増加による高フルエンス照射の要望が高まっている。そこでLEU燃料の燃焼度向上による運転日数の増加を図れる炉心構成について検討し、核・熱水力学的解析を行った。その結果、標準燃料数を現在の22本から24本に増加し、現在の2サイクル使用(燃料フォロワは1サイクル使用)から、3サイクル(燃料フォロワは2サイクル使用)とする8-8-8炉心により、年間180日の運転が可能であること、50%を越える燃料平均燃焼度が達成できることが示された。この変更による照射場の中性子フラックスはほとんど変わらず、また、安全評価上の基準も十分満たせる見通しを得た。したがって、本炉心構成によって今後のJMTRの照射効率と燃料経済性の向上が可能であることがわかった。

口頭

Resonant X-ray scattering study of the nonmagnetic order of 5f electrons in a pseudo-Kagome layered system URhSn

田端 千紘; 今 布咲子*; 網塚 浩*; 清水 悠晴*; 青木 大*; 中尾 裕則*

no journal, , 

Magnetic materials with no inversion center at the magnetic site have attracted much attention from the viewpoints of chiral magnetic orders and electromagnetic effects in recent years. URhSn has a crystal structure without spatial inversion symmetry (hexagonal, space group P-62m) consisting of distorted Kagome layers, and according to previous reports on polycrystalline samples, it undergoes a two-step phase transition at To = 54 K and TC = 16 K. While the low-temperature phase is considered a ferromagnetic phase with spontaneous magnetization along the c-axis, the order parameter of the high-temperature phase has remained unknown for decades. No symmetry breaking has been detected for this mysterious phase by microscopic measurements such as powder neutron diffraction and Mossbauer spectroscopy. We recently succeeded in growing high-quality single crystals of this compound and clarified its detailed bulk properties (specific heat, magnetization, electrical resistivity, and thermal expansion). Interestingly, the high-temperature phase below To isstabilized by a magnetic field parallel to the c-axis, despite the absence of a c-axis spontaneous magnetization component. This peculiar behavior indicates neither a simple ferromagnetic nor antiferromagnetic scenario. We investigated the order parameter of this unknown phase using a resonant X-ray scattering (RXS) technique. On the resonance condition at the M4 absorption edge of U, we observed a slight increase in the intensity of a fundamental Bragg reflection below To, suggesting an order parameter with q = 0 that does not break the translational symmetry of the crystal. The observed RXS signal can be interpreted by either case of order parameters of magnetic dipoles and electric quadrupoles. Given the Sn-Mossbauer and Sn-NMR reports of no internal magnetic field associated with the order, an electric quadrupolar order is more plausible.

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