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Sm synchrotron-radiation-based M
ssbauer spectroscopy of Sm-based heavy fermion compounds筒井 智嗣; 東中 隆二*; 水牧 仁一朗*; 小林 義男*; 中村 仁*; 伊藤 孝; 依田 芳卓*; 松田 達磨*; 青木 勇二*; 佐藤 英行*
Interactions (Internet), 245(1), p.9_1 - 9_10, 2024/12
Sm synchrotron-radiation-based Mssbauer spectroscopy has been applied to Sm-based heavy fermion intermetallics, Sm
Al
(
= Ti, V and Cr) and SmOs
Sb
. The isomer shifts obtained demonstrate that the Sm valence states in these compounds are intermediate. Since the difference of the isomer shifts in 22.502 keV Sm Mssbauer effect between Sm
and Sm
state is comparable to the 2nd order Doppler shift, consideration of the 2nd order Doppler shift is required to precisely discuss Sm valence state through the shifts of the Mssbauer spectra. In addition, the plots of the isomer shifts obtained by the Mssbauer spectroscopy against the Sm valence states estimated from Sm L-edge X-ray absorption spectroscopy exhibit a linear correlation except for that in SmOs
Sb. This implies that the origin of the intermediate valence state in SmOsSb differs from that in SmAl ( = Ti, V and Cr).
Sm synchrotron-radiation-based Mssbauer and 
SR studies of Sm
RuGe
筒井 智嗣; 伊藤 孝; 中村 仁*; 吉田 実生*; 小林 義男*; 依田 芳卓*; 中村 惇平*; 幸田 章宏*; 東中 隆二*; 青木 大*; et al.
Interactions (Internet), 245(1), p.55_1 - 55_9, 2024/12
Sm SR-based Mssbauer and muon spin relaxation (SR) spectroscopies have been applied to SmRuGe. The temperature dependence of the Sm SR-based Mssbauer spectra in the paramagnetic state implies the presence of dynamical nuclear Zeeman and/or quadrupole interactions. The time differential SR spectra also exhibit a marked temperature dependence in the paramagnetic state, indicating the presence of magnetic fluctuation in SmRuGe at least. These results in the present work infer that the dynamical hyperfine interactions observed using the mutually complementary spectroscopic methods are connected with the mechanism of the heavy fermion behavior in SmRuGe.
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：3 パーセンタイル：72.20(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.
伊與田 宗慶*; 松田 朋己*; 佐野 智一*; 茂田 正哉*; 菖蒲 敬久; 湯本 博勝*; 小山 貴久*; 山崎 裕史*; 仙波 泰徳*; 大橋 治彦*; et al.
Journal of Manufacturing Processes, 94, p.424 - 434, 2023/05
被引用回数：7 パーセンタイル：72.06(Engineering, Manufacturing)Aluminum alloys are increasingly being applied to automobile bodies to reduce the weight of automobiles. In joining steel materials and aluminum alloys using resistance spot welding (RSW), it is important to control the state of intermetallic compounds due to the temperature at the joining interface. In other words, in RSW of Fe/Al dissimilar materials, it is necessary to clarify the heating and cooling phenomena of the interface temperature during joining. Although the convection behavior of the molten aluminum alloy is thought to influence the temperature distribution at the joining interface, there are no studies that have directly observed this phenomenon. In this study, convection in molten zone of aluminum alloy during RSW of steel and aluminum alloy is discussed. Direct observations were attempted in order to clarify the convection behavior of the molten aluminum alloy in RSW of steel and aluminum alloy. The main feature of this experiment is that a real-scale test piece and an RSW apparatus used in actual production were used to observe convection during actual production. The observation experiments were conducted using synchrotron radiation X-ray at SPring-8. During welding, the specimens were irradiated with synchrotron radiation X-ray, and convection was observed from the behavior of tracer particles placed on the specimens. As a results, three types of convection were observed: radial outward convection from the center of the molten zone at the joining interface, convection from the edge of the molten zone toward its center, and weak circulating convection at the edge of the molten zone. And, small convection velocities were generated at the edge of the molten zone. Furthermore, the convection velocity inside the molten zone was calculated to be approximately 1.75 m/s. In addition, it was shown that there is a correlation between convection behavior and the shape of the molten zone.
-based superconductor LaBiSO
F玉造 博夢; 長谷川 巧*; 佐賀山 基*; 水牧 仁一朗*; 村上 洋一*; 梶谷 丈*; 東中 隆二*; 松田 達磨*; 青木 勇二*; 筒井 智嗣*
Physical Review B, 107(2), p.024303_1 - 024303_8, 2023/01
被引用回数：1 パーセンタイル：15.88(Materials Science, Multidisciplinary)The phonon dispersion of a BiS-based superconductor LaBiSOF is investigated by first-principles calculations and inelastic X-ray scattering experiments. The origin of superlattice (SL) reflections arising from transverse-type lattice modulation, which were recently reported in [J. Kajitani 
., J. Phys. Soc. Jpn. 
, 103601 (2021)], is discussed in terms of lattice dynamics. Our first-principles calculations of phonon dispersion and the Fermi surfaces (FSs) demonstrate that the phonon mode corresponding to the transverse-type lattice modulation is unstable, and the propagation vector corresponding to the SL reflections is close to the FS nesting vector, which suggests that the phonon softening originates from the FS nesting. Against these calculated expectations, measured phonon dispersion in LaBiSOF along the Z-A direction, where the SL point is located, shows no remarkable temperature dependence, and there are no steeply declining branches accompanied with a softening around the SL point. Based on these results, we discuss the two possibilities for the transverse lattice modulation in LaBiSOF: the order-disorder type structural transition and the displacive structural transition with an overdamped mode, for both of which the local structure distortion or the short range correlation within the BiS plane would be essential.
RhSn岩佐 和晃*; Suyama, Kazuya*; 河村 聖子; 中島 健次; Raymond, S.*; Steffens, P.*; Yamada, Akira*; 松田 達磨*; 青木 勇二*; 川崎 郁斗; et al.
Physical Review Materials (Internet), 7(1), p.014201_1 - 014201_11, 2023/01
被引用回数：3 パーセンタイル：37.12(Materials Science, Multidisciplinary)The spin dynamics, crystalline-electric-field (CEF) level scheme, specific heat, and X-ray photoemission spectra (XPS) of CeRhSn were investigated, which exhibits anomalous semimetal transport in the chiral crystallographic phase. CEF excitations observed at approximately 7 and 39 meV are consistent with the two inequivalent Ce-ion cites in the chiral structure. Because of broader CEF excitations and a strong 4
peak at the Fermi level in the Ce 4
on-resonance spectrum, the hybridized Ce 4 electrons contribute to the semimetal carriers. In addition, the spin fluctuation associated with the Kramers doublet ground state is characterized by the peak located at 0.15 meV. The electronic state involving the spin fluctuation causes the 
behavior of specific heat below 0.6 K, which is attributed to linear dispersion relations of electrons of the Weyl Kondo semimetal in the chiral-lattice symmetry.
Sm Mssbauer and Sm L
-edge X-ray absorption spectroscopies筒井 智嗣; 東中 隆二*; 中村 頼人*; 藤原 孝将*; 中村 仁*; 小林 義男*; 伊藤 孝; 依田 芳卓*; 加藤 和男*; 新田 清文*; et al.
Hyperfine Interactions, 242(1), p.32_1 - 32_10, 2021/12
被引用回数：1 パーセンタイル：75.97(Physics, Atomic, Molecular & Chemical)Sm synchrotron-radiation-based Mssbauer spectroscopy was performed in Sm-based intermetallics having a cubic crystal structure, Sm
Ge, SmB
, SmBe, and Sm
Al ( = transition metals). In spite of the difference of the local structure around the Sm sites, the observed Mssbauer spectra consist of a single line at 300 K. On the other hand, Sm L-edge X-ray absorption spectra consist of two components, suggesting Sm and Sm states. Difference of the number of the spectral components between the Mssbauer spectroscopy and X-ray absorption spectroscopy is caused by the difference of the time window in the scattering process of these measurements. Correlation between the isomer shifts in the Mssbauer spectroscopy and average Sm valence states estimated from the X-ray absorption spectroscopy exhibits a linear correlation.
宮原 信哉*; 大平 直也*; 有田 裕二*; 前川 藤夫; 松田 洋樹; 佐々 敏信; 明午 伸一郎
Nuclear Engineering and Design, 352, p.110192_1 - 110192_8, 2019/10
被引用回数：5 パーセンタイル：42.35(Nuclear Science & Technology)鉛ビスマス共晶(LBE)合金は加速器駆動システム(ADS)の核破砕中性子ターゲットや冷却材として用いられ、核破砕生成物として多くの元素が生成するため、その放出および輸送挙動を評価することが重要である。そこで、J-PARCのADSターゲット試験施設(TEF-T)のLBEループについて、LBE中に生成する核破砕生成物のインベントリおよび物理化学的組成について検討した。LBE内の核破砕生成物インベントリは、PHITSコードを使用して評価した。LBE中の核破砕生成物の物理化学的組成は、350
C
500CのLBE運転温度及びLBE中の酸素濃度10ppb1ppmの条件下、Thermo-Calcコードを用いて計算した。計算の結果、Rb, Tl, Tc, Os, Ir, Pt, Au, Hgの8元素がすべての条件下でLBEに可溶であり、化合物は形成されなかった。Ce, Sr, Zr及びYの酸化物はLBE中でCeO, SrO, ZrOおよびYOとして安定であることが示唆された。
中根 僚宏*; 米山 翔太*; 兒玉 健*; 菊地 耕一*; 中尾 朗子*; 大原 高志; 東中 隆二*; 松田 達磨*; 青木 勇二*; 藤田 渉*
Dalton Transactions (Internet), 48(1), p.333 - 338, 2019/01
被引用回数：3 パーセンタイル：15.56(Chemistry, Inorganic & Nuclear)The two-dimensional quadratic lattice magnet, bis(glycolato)cobalt(II) ([Co(HOCHCO)]), showed anti-ferromagnetic ordering at 15.0 K and an abrupt increase in magnetisation at H = 22 600 Oe and 2 K, thereby acting as a metamagnet. Neutron diffraction studies suggested that the magnetic moment vectors of the Co(II) ions had an amplitude of 3.59 mB and were not aligned in a fully antiparallel fashion to those of their neighbours, which caused canting between the magnetic moment vectors in the sheet. The canting angle was determined to be 7.1deg. Canting induced net magnetisation in the sheet, but this magnetisation was cancelled between sheets. The magnetisations in the sheets were oriented parallel to the magnetic field at the critical magnetic field.
竹田 幸治; 斎藤 祐児; 岡根 哲夫; 山上 浩志; 松田 達磨*; 山本 悦嗣; 芳賀 芳範; 大貫 惇睦*
Physical Review B, 97(18), p.184414_1 - 184414_7, 2018/05
被引用回数：3 パーセンタイル：13.76(Materials Science, Multidisciplinary)We have performed soft X-ray magnetic circular dichroism (XMCD) experiments on the itinerant-electron metamagnet UCoAl at the U 4
-5 (
) and Co 2
-3 (
) absorption edges in order to investigate the magnetic properties of the U 5 and Co 3 electrons separately. From the line shape of the XMCD spectrum, it is deduced that the orbital magnetic moment of the Co 3 electrons is unusually large. Through the systematic temperature (
)- and magnetic field (
)-dependent XMCD measurements, we have obtained two types of the magnetization curve as a function of and (M-H curve and M-T curve, respectively). The metamagnetic transition from a paramagnetic state to a field-induced ferromagnetic state was observed clearly under 15 K at 
. The value of the and its -dependence agree well between the U and Co sites, and the bulk magnetization. Whereas, we have discovered the remarkable differences in the M-H and M-T curves between the U and Co sites. The present findings show clearly that the role of the Co 3 electrons should be considered more carefully in order to understand the origin of the magnetic ordering in UCoAl.
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 勝彦*; 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：4 パーセンタイル：84.40(Physics, Atomic, Molecular & Chemical)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.
by tuning nematicity and magnetism in FeSe
S
superconductors松浦 康平*; 水上 雄太*; 新井 佑基*; 杉村 優一*; 前島 尚行*; 町田 晃彦*; 綿貫 徹*; 福田 竜生; 矢島 健*; 廣井 善二*; et al.
Nature Communications (Internet), 8, p.1143_1 - 1143_6, 2017/10
被引用回数：95 パーセンタイル：91.90(Multidisciplinary Sciences)A fundamental issue concerning iron-based superconductivity is the roles of electronic nematicity and magnetism in realising high transition temperature (). To address this issue, FeSe is a key material, as it exhibits a unique pressure phase diagram involving nonmagnetic nematic and pressure-induced antiferromagnetic ordered phases. However, as these two phases in FeSe have considerable overlap, how each order affects superconductivity remains perplexing. Here we construct the three-dimensional electronic phase diagram, temperature () against pressure (
) and iso-valent S-substitution (
), for FeSeS. By simultaneously tuning chemical and physical pressures, against which the chalcogen height shows a contrasting variation, we achieve a complete separation of nematic and antiferromagnetic phases. In between, an extended nonmagnetic tetragonal phase emerges, where shows a striking enhancement. The completed phase diagram uncovers that high- superconductivity lies near both ends of the dome-shaped antiferromagnetic phase, whereas remainslow near the nematic critical point.
岩元 洋介; 佐藤 達彦; 橋本 慎太郎; 小川 達彦; 古田 琢哉; 安部 晋一郎; 甲斐 健師; 松田 規宏; 細山田 龍二*; 仁井田 浩二*
Journal of Nuclear Science and Technology, 54(5), p.617 - 635, 2017/05
被引用回数：112 パーセンタイル：99.72(Nuclear Science & Technology)粒子・重イオン輸送計算コードPHITSは、加速器遮蔽設計、医学物理計算など様々な目的で利用されている。本研究では、最新のPHITSバージョン2.88を用いて、核反応による粒子生成断面積、中性子輸送計算、電磁カスケード等に対する58ケースのベンチマーク計算を実施した。本稿では、このうち特徴的な結果を示した22のケースについて詳細に報告する。ベンチマーク計算の結果、100MeV以上の陽子、中性子、重イオン等の入射反応や電磁カスケードについては、PHITSによる計算結果は実験値を概ね再現した。一方、100MeV未満の粒子入射反応は、PHITSが設定を推奨している核内カスケードモデルINCL4の適用範囲外のエネルギー領域であるため、再現性が悪いことが確認された。また、100MeV以上の陽子入射反応のうち、核分裂成分の収率に対して、蒸発モデルGEMの高エネルギー核分裂過程の取り扱いの問題から実験値を再現しない場合があった。これらの課題は、評価済み核データJENDL4.0/HEをPHITSに組み込むこと等で改善していく予定である。以上のように、本研究でPHITSの様々な適用分野における計算精度を検証するとともに、今後の効率的な改善に重要な指針を得ることができた。
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 勝彦*; 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：7 パーセンタイル：89.72(Physics, Atomic, Molecular & Chemical)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.
Si as a reference to the strongly correlated isostructural metals investigated by quantum oscillations松本 裕司*; 芳賀 芳範; 立岩 尚之; 青木 晴善*; 木村 憲彰*; 山村 朝雄*; 山本 悦嗣; 松田 達磨*; Fisk, Z.*; 山上 浩志*
Journal of the Physical Society of Japan, 85(10), p.104709_1 - 104709_7, 2016/10
被引用回数：3 パーセンタイル：26.07(Physics, Multidisciplinary)dHvA oscillations were detected on an actinide compound ThRu
Si which is regarded as a reference to strongly correlated electron systems URuSi and CeRuSi. Observed Fermi surfaces well coincides with the band structure calculations, as well as experimentally obtained ones for a heavy fermion compound CeRuSi. On the other hand, Fermi surfaces of URuSi have significantly different characteristics, suggesting an itinerant ground state of 5f electrons.
Si山下 卓也*; 下山 祐介*; 芳賀 芳範; 松田 達磨*; 山本 悦嗣; 大貫 惇睦; 住吉 浩明*; 藤本 聡*; Levchenko, A.*; 芝内 孝禎*; et al.
Nature Physics, 11(1), p.17 - 20, 2015/01
被引用回数：59 パーセンタイル：90.32(Physics, Multidisciplinary)Observation of a colossal Nernst signal is reported. URuSi is known as a heavy fermion superconductor. The superconductivity coexists with the so-called hidden-order phase. The Nernst coefficient is enhanced by as large as million times over the theoretically expected value within the standard framework of superconducting fluctuations. Moreover, contrary to the conventional wisdom, the enhancement is more significant with the reduction of the impurity scattering rate. This anomalous Nernst effect intimately reflects the highly unusual superconducting state in URuSi.
Si松本 裕司*; 芳賀 芳範; 立岩 尚之; 青木 晴善*; 木村 憲彰*; 松田 達磨*; 山本 悦嗣; Fisk, Z.; 山上 浩志*
JPS Conference Proceedings (Internet), 3, p.011096_1 - 011096_5, 2014/06
Electronic differences between heavy Fermion CeRuSi and isoelectronic nonmagnetic ThRuSi have been investigated. We succeeded in observing the de Haas-van Alphen oscillation in a high quality single crystal of ThRuSi. The mean free path of conduction carriers has been estimated as 6400 
, indicating the high quality of the present sample.
Si利根川 翔*; 笠原 成*; 福田 竜生; 杉本 邦久*; 安田 伸広*; 鶴原 悠悟*; 渡邊 大樹*; 水上 雄太*; 芳賀 芳範; 松田 達磨*; et al.
Nature Communications (Internet), 5, p.4188_1 - 4188_7, 2014/06
被引用回数：52 パーセンタイル：88.02(Multidisciplinary Sciences)We report on the observation of lattice symmetry breaking from the fourfold to twofold structure by high-resolution synchrotron X-ray diffraction measurements at zero field. Small orthorhombic symmetry-breaking distortion sets in at the transition temperature with a jump, uncovering the weakly first-order nature of the hidden-order transition. This distortion is observed only in ultra pure samples, implying a highly unusual coupling nature between the electronic pneumaticity and underlying lattice.
P; Evidence from resonant and nonresonant X-ray diffraction松村 武*; 道村 真司*; 稲見 俊哉; 林 佑弥*; 伏屋 健吾*; 松田 達磨*; 東中 隆二*; 青木 勇二*; 菅原 仁*
Physical Review B, 89(16), p.161116_1 - 161116_5, 2014/04
被引用回数：15 パーセンタイル：52.32(Materials Science, Multidisciplinary)SmRuPの
K以下の反強磁性相と
と
(=14K)間の中間相を共鳴と非共鳴のX線回折法で研究した。中間相では非共鳴の
=(1,0,0)のThomson散乱が磁場によって誘起される。この現象は理論的に予言されているバンドの電荷秩序を反映した原子変位によって引き起こされている。同時にSmの磁場方向の反強磁性モーメントが強調され、これは
結晶場状態の交互配列を反映していると考えられる。この結果は、軌道に依存した-混成とpバンドのネスティング不安定性がPrRuPやPrFePと同様な非従来型電荷秩序を引き起こしていることを示している。
Si利根川 翔*; 橋本 顕一郎*; 井加田 洸輔*; 鶴原 悠悟*; Lin, Y.-H.*; 宍戸 寛明*; 芳賀 芳範; 松田 達磨; 山本 悦嗣; 大貫 惇睦; et al.
Physical Review B, 88(24), p.245131_1 - 245131_13, 2013/12
被引用回数：12 パーセンタイル：47.08(Materials Science, Multidisciplinary)Detailed analyses of the cyclotron resonance lines in a uranium compound URuSi are reported. The analyses of the resonance profiles reveals that the heavier branch of the split line has a larger scattering rate, providing evidence for the existence of hot-spot along the [110] direction. The result is consistent with the broken fourfold symmetry in the hidden-order phase.
