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Study on use of superconducting magnet and first inelastic neutron scattering experiment under magnetic field at 4SEASONS spectrometer

梶本 亮一; 石角 元志*; 吉良 弘*; 金子 耕士; 中村 充孝; 蒲沢 和也*; 稲村 泰弘; 池内 和彦*; 飯田 一樹*; 村井 直樹; et al.

Physica B; Condensed Matter, 556, p.26 - 30, 2019/03

 被引用回数:2 パーセンタイル:17.06(Physics, Condensed Matter)

Magnets are important for studying magnetism and are commonly used as sample environment devices of neutron scattering instruments. However, the use of magnets was prevented at the time-of-flight direct-geometry neutron spectrometer 4SEASONS in Materials and Life Science Experimental Facility (MLF) at J-PARC, because the instrument is surrounded by iron components, and it is equipped with a piece of equipment operated with magnetic bearings. In the present work, we investigate the influence of stray magnetic fields from a superconducting magnet which is shared among neutron scattering instruments in MLF. Based on the investigation, we modified 4SEASONS such that it can be used with the magnet. Finally, we successfully performed the first inelastic neutron scattering experiments with applied magnetic fields using this sample environment.


Unique helical magnetic order and field-induced phase in trillium lattice antiferromagnet EuPtSi

金子 耕士; Frontzek, M. D.*; 松田 雅昌*; 中尾 朗子*; 宗像 孝司*; 大原 高志; 垣花 将司*; 芳賀 芳範; 辺土 正人*; 仲間 隆男*; et al.

Journal of the Physical Society of Japan, 88, p.013702_1 - 013702_5, 2019/01

 被引用回数:1 パーセンタイル:14.05(Physics, Multidisciplinary)

Magnetic transitions in chiral antiferromagnet EuPtSi were investigated by means of single crystal neutron diffraction. In the ground state, magnetic peaks emerge at positions represented by $$q_{1}$$=$$(0.2, 0.3, 0)$$. Upon heating, an additional magnetic peak splitting around 2.5 K was uncovered, indicating a presence of a first-order transition with $$q^*_{1}$$=$$(0.2, 0.3, {delta})$$. An half-polarized neutron scattering for polarization parallel to Q reveled that polarization antiparallel to Q has stronger intensity in both magnetic phases. This feature clarifies single chiral character of helical structure with moments normal to the ordering vector in both ordered states. Under vertical magnetic field along [1,1,1] in the $$A$$ phase, magnetic peaks form hexagonal patterns in the equatorial scattering plane around nuclear. An ordering vector $$q_{A}$$ of the $$A$$-phase has the similar size in the periodicity to $$q_{1}$$, and could be a hallmark of a formation of skyrmion lattice in EuPtSi.


Evidence of a structural quantum critical point in (Ca$$_x$$Sr$$_{1-x}$$)$$_3$$Rh$$_4$$Sn$$_{13}$$ from a lattice dynamics study

Cheung, Y. W.*; Hu, Y. J.*; 今井 正樹*; 谷奥 泰明*; 金川 響*; 村川 譲一*; 森山 広大*; Zhang, W.*; Lai, K. T.*; 吉村 一良*; et al.

Physical Review B, 98(16), p.161103_1 - 161103_5, 2018/10

 パーセンタイル:100(Materials Science, Multidisciplinary)

Approaching a quantum critical point has been an effective route to stabilize superconductivity. While the role of magnetic QCPs has been extensively discussed, similar exploration of a structural QCP is scarce. Using inelastic X-ray scattering, we examine the phonon spectrum of the nonmagnetic quasi-skutterudite (Ca$$_x$$Sr$$_{1-x}$$)$$_3$$Rh$$_4$$Sn$$_{13}$$, which represents a precious system to explore the interplay between structural instabilities and superconductivity by tuning the Ca concentration x. We unambiguously detect the softening of phonon modes around the M point on cooling towards the structural transition. Intriguingly, at x = 0:85, the soft mode energy squared at the M point extrapolates to zero at -5.7 K, providing the first compelling microscopic evidence of a structural QCP in (Ca$$_x$$Sr$$_{1-x}$$)$$_3$$Rh$$_4$$Sn$$_{13}$$. The enhanced phonon density-of-states at low energy provides the essential ingredient for realizing strong-coupling superconductivity near the structural QCP.


Inelastic X-ray scattering of $$RT$$Al$$_3$$ ($$R$$ = La, Ce, $$T$$ = Cu, Au)

筒井 智嗣*; 金子 耕士; Pospisil, J.; 芳賀 芳範

Physica B; Condensed Matter, 536, p.24 - 27, 2018/05

 パーセンタイル:100(Physics, Condensed Matter)

Inelastic X-ray scattering (IXS) experiments of RTAl$$_3$$ ($$R$$ = La Ce, $$T$$ = Cu, Au) were carried out at 300 and 5.5 K. The spectra between LaCuAl$$_3$$ and CeCuAl$$_3$$ (LaAuAl$$_3$$ and CeAuAl$$_3$$) are nearly identical at both temperatures except for temperature factors such as temperature dependence of Bose factor in IXS spectra and effect on thermal expansion. This means that no evident temperature dependence of IXS spectra was observed in CeTAl$$_3$$ ($$T$$ = Cu, Au).


Retreat from stress; Rattling in a planar coordination

末國 晃一郎*; Lee, C. H.*; 田中 博己*; 西堀 英治*; 中村 篤*; 笠井 秀隆*; 森 仁志*; 臼井 秀知*; 越智 正之*; 長谷川 巧*; et al.

Advanced Materials, 30(13), p.1706230_1 - 1706230_6, 2018/03

 被引用回数:6 パーセンタイル:13.58(Chemistry, Multidisciplinary)



Materials and Life Science Experimental Facility (MLF) at the Japan Proton Accelerator Research Complex, 2; Neutron scattering instruments

中島 健次; 川北 至信; 伊藤 晋一*; 阿部 淳*; 相澤 一也; 青木 裕之; 遠藤 仁*; 藤田 全基*; 舟越 賢一*; Gong, W.*; et al.

Quantum Beam Science (Internet), 1(3), p.9_1 - 9_59, 2017/12



Second-order structural transition in (Ca$$_{0.5}$$Sr$$_{0.5}$$)$$_3$$Rh$$_4$$Sn$$_{13}$$

Cheung, Y. W.*; Hu, Y. J.*; Goh, S. K.*; 金子 耕士; 筒井 智嗣; Logg, P. W.*; Grosche, F. M.*; 金川 響*; 谷奥 泰明*; 今井 正樹*; et al.

Journal of Physics; Conference Series, 807(3), p.032002_1 - 032002_4, 2017/04


(Ca$$_{0.5}$$Sr$$_{0.5}$$)$$_3$$Rh$$_4$$Sn$$_{13}$$ is a member of the substitution series (Ca$$_{x}$$Sr$$_{1-x}$$)$$_3$$Rh$$_4$$Sn$$_{13}$$ which has recently been argued to feature a structural quantum critical point at $$x_c$$ = 0.9. In the stoichiometric compound Sr$$_{3}$$Rh$$_{4}$$Sn$$_{13}$$, the structural transition at $$T^*$$ $$approx$$ 138 K has been shown to be a second-order phase transition. Moving towards xc, we examine the character of the structural transition in (Ca$$_{0.5}$$Sr$$_{0.5}$$)$$_3$$Rh$$_4$$Sn$$_{13}$$ (i.e. $$x$$ = 0.5, $$T^*$$ $$approx$$ 55 K) using electrical resistivity, heat capacity and X-ray scattering. The absence of the thermal hysteresis in specific heat around $$T^*$$, and the continuous evolution of the superlattice reflection detected by X-ray diffraction are consistent with the scenario that the structural transition associated with a modulation vector $$q$$ = (0.5, 0.5, 0) in (Ca$$_{0.5}$$Sr$$_{0.5}$$)$$_3$$Rh$$_4$$Sn$$_{13}$$ remains second-order on approaching the quantum critical point.


Magnetic structure of divalent europium compound EuGa$$_{4}$$ studied by single-crystal time-of-flight neutron diffraction

川崎 卓郎; 金子 耕士; 仲村 愛*; 阿曽 尚文*; 辺土 正人*; 仲間 隆男*; 大原 高志; 鬼柳 亮嗣; 及川 健一; 田村 格良; et al.

Journal of the Physical Society of Japan, 85(11), p.114711_1 - 114711_5, 2016/11

 パーセンタイル:100(Physics, Multidisciplinary)

The magnetic structure of the intermetallic compound EuGa$$_{4}$$ was investigated using single-crystal neutron diffraction with TOF Laue technique on the new diffractometer SENJU at MLF of J-PARC. Despite of the high neutron absorption of Eu, a vast number of diffraction spots were observed without isotope enrichment. The magnetic reflections appeared at $$h + k + l$$ $$neq$$ 2$$n$$ below 16 K, indicating that the ordering vector is $$q$$ = (0, 0, 0). The continuous evolution of the magnetic reflection intensity below T$$_{N}$$ follows a squared Brillouin function for $$S$$ = 7/2. By adopting a wavelength-dependent absorption collection, the magnetic structure of EuGa$$_{4}$$ revealed that a nearly full magnetic moment of 6.4 $$mu$$B of Eu lies within the basal plane of the lattice.


Unique magnetic structure of YbCo$$_2$$Si$$_2$$

Mufti, N.*; 金子 耕士; Hoser, A.*; Gutmann, M.*; Geibel, C.*; Krellner, C.*; Stockert, O.*

Physical Review B, 94(4), p.045116_1 - 045116_8, 2016/07


 パーセンタイル:100(Materials Science, Multidisciplinary)

We report on the results of powder and single crystal neutron diffraction to investigate the magnetic order in YbCo$$_2$$Si$$_2$$ below the N$'e$el temperature $$T_{rm N} = 1.7$$,K in detail. Two different magnetically ordered phases can clearly be distinguished. At lowest temperatures a commensurate magnetic structure with a propagation vector $${bf k}_1 = (0.25 0.25 1)$$ is found, while the intermediate phase ($$T > 0.9$$,K) is characterized by an incommensurate magnetic structure with $${bf k}_2 = (0.25 0.086 1)$$. The magnetic structure in YbCo$$_2$$Si$$_2$$ is in marked contrast to all other known $$R$$Co$$_2$$Si$$_2$$ compounds ($$R$$ = rare earth element) likely due to some itineracy of the Yb 4f states being responsible for the magnetism.


Second-order structural transition in the superconductor La$$_3$$Co$$_4$$Sn$$_{13}$$

Cheung, Y. W.*; Zhang, J. Z.*; Zhu, J. Y.*; Yu, W. C.*; Hu, Y. J.*; Wang, D. G.*; 大友 優香*; 岩佐 和晃*; 金子 耕士; 今井 正樹*; et al.

Physical Review B, 93(24), p.241112_1 - 241112_5, 2016/06


 被引用回数:10 パーセンタイル:27.32(Materials Science, Multidisciplinary)

The quasi-skutterudite superconductor La$$_3$$Co$$_4$$Sn$$_{13}$$ undergoes a phase transition at $$T^{*}$$ = 152 K. By measuring the temperature dependence of heat capacity, electrical resistivity, and the superlattice reflection intensity using X-ray, we explore the character of the phase transition at $$T^{*}$$. Our lattice dynamic calculations found imaginary phonon frequencies around the $$M$$ point, when the high temperature structure is used in the calculations, indicating that the structure is unstable at the zero temperature limit. The combined experimental and computational results establish that $$T^{*}$$ is associated with a second-order structural transition with $$q$$ = (0.5, 0.5, 0) (or the $$M$$ point). Further electronic band structure calculations reveal Fermi surface sheets with low-curvature segments, which allow us to draw qualitative comparison with both Sr$$_3$$Ir$$_4$$Sn$$_{13}$$ and Sr$$_3$$Rh$$_4$$Sn$$_{13}$$ in which similar physics has been discussed recently.


SENJU; A New time-of-flight single-crystal neutron diffractometer at J-PARC

大原 高志; 鬼柳 亮嗣; 及川 健一; 金子 耕士; 川崎 卓郎; 田村 格良; 中尾 朗子*; 花島 隆泰*; 宗像 孝司*; 茂吉 武人*; et al.

Journal of Applied Crystallography, 49(1), p.120 - 127, 2016/02

 被引用回数:13 パーセンタイル:11.41(Chemistry, Multidisciplinary)

SENJU, a time-of-flight Laue-type single-crystal neutron diffractometer, was developed at the Materials and Life Science Experimental Facility (MLF) of the Japan Accelerator Research Complex (J-PARC). Molecular structure analysis of a sub-millimeter taurine crystal and magnetic structure analysis of a MnF$$_{2}$$ crystal were performed to evaluate its performance.



三田村 裕之*; 綿貫 竜太*; 金子 耕士; 榊原 俊郎*

固体物理, 50(12), p.821 - 832, 2015/12



Science from the initial operation of HRC

伊藤 晋一*; 横尾 哲也*; 益田 隆嗣*; 吉澤 英樹*; 左右田 稔*; 池田 陽一*; 井深 壮史*; 川名 大地*; 佐藤 卓*; 南部 雄亮*; et al.

JPS Conference Proceedings (Internet), 8, p.034001_1 - 034001_6, 2015/09

Since the installation of the High Resolution Chopper Spectrometer, HRC, experiments using the HRC are being conducted to observe the dynamics in wide range of physics. Scientific results during the period since the initial construction are summarized.


Influence of electron doping on magnetic order in CeRu$$_2$$Al$$_{10}$$

小林 理気*; 金子 耕士; 斉藤 耕太郎*; Mignot, J.-M.*; Andr$'e$, G.*; Robert, J.*; 脇本 秀一; 松田 雅昌*; Chi, S.*; 芳賀 芳範; et al.

Journal of the Physical Society of Japan, 83(10), p.104707_1 - 104707_5, 2014/10

 被引用回数:12 パーセンタイル:26.29(Physics, Multidisciplinary)

The effect of electron doping by the substitution of Rh for Ru on unconventional magnetic order in CeRu$$_2$$Al$$_{10}$$ was investigated via neutron powder diffraction. In Ce(Ru$$_{1-x}$$Rh$$_x$$)$$_2$$Al$$_{10}$$ with $$x$$ = 0.05, 0.12, 0.2, reorientation of the ordered moment from the $$c$$- to the $$a$$-axis takes place in all samples, while the ordering vector $$q$$ = (0 1 0) remains unchanged within this concentration range. The moment reorientation is accompanied by an enhancement in its size by a factor of 2.4, from $${mu}$$=0.43 $${mu}_B$$ at $$x$$ = 0 to $${mu}$$=1.06, 1.04, and 1.02 $${mu}_B$$ for $$x$$ = 0.05, 0.12 and 0.2, respectively. The continuous decrease in N$'e$el temperature $$T_0$$($$T_N$$), despite an abrupt increase in $${mu}$$, underlines the strong anisotropy in the exchange interaction in CeRu$$_2$$Al$$_{10}$$, and the fact that this anisotropy is easily suppressed by electron doping.


Spin-chirality-driven ferroelectricity on a perfect triangular lattice antiferromagnet

三田村 裕之*; 綿貫 竜太*; 金子 耕士; 小野崎 紀道*; 天羽 祐太*; 橘高 俊一郎*; 小林 理気*; 志村 恭通*; 山本 勲*; 鈴木 和也*; et al.

Physical Review Letters, 113(14), p.147202_1 - 147202_5, 2014/10

 被引用回数:10 パーセンタイル:30.15(Physics, Multidisciplinary)

Magnetic field ($$B$$) variation of the electrical polarization $$P$$$$_{c}$$ ($${parallel}$$c) of the perfect triangular lattice antiferromagnet RbFe (MoO$$_4$$)$$_2$$ is examined up to the saturation point of the magnetization for B$${perp}c$$. $$P$$$$_{c}$$ is observed only in phases for which chirality is predicted in the in-plane magnetic structures. No strong anomaly is observed in $$P$$$$_{c}$$ at the field at which the spin modulation along the c axis exhibits a discontinuity to the commensurate state. These results indicate that ferroelectricity in this compound originates predominantly from triangular-spin chirality. The obtained field-temperature phase diagrams of ferroelectricity well agree with those theoretically predicted for the spin chirality of a Heisenberg spin triangular lattice antiferromagnet.


Field-induced order in heavy-fermion compound YbCo$$_2$$Zn$$_{20}$$

金子 耕士; Raymond, S.*; Ressouche, E.*; Lapertot, G.*; 竹内 徹也*; 広瀬 雄介*; 本多 史憲*; 大貫 惇睦

JPS Conference Proceedings (Internet), 3, p.011061_1 - 011061_5, 2014/06

YbCo$$_2$$Zn$$_{20}$$ has a heavy-fermion ground state with an enormously large Sommerfeld coefficient of 8 J/molK$$^2$$, and that is sensitive to external fields. Whereas pressure induces antiferromagnetic order, magnetic field induces metamagnetic transitions around 0.5 T, and new ordered state appears above 6 T for $$B{parallel}{langle}111{rangle}$$. In order to get insights into electronic states and its magnetic field response, neutron scattering experiments on single crystalline samples were carried. In a field-induced phase, magnetic reflections were successfully observed, which has a different propagation vector to that of pressure induced phase. Inelastic neutron scattering probes a crystal-field excitation at a low excitation energy which overlaps to quasielastic response. The results suggest degenerated energy scale, and that leads to variety of external response in YbCo$$_2$$Zn$$_{20}$$.


Anharmonic Pr guest modes in Pr(Os$$_{1-x}$$Ru$$_x$$)$$_4$$Sb$$_{12}$$ investigated by inelastic X-ray scattering

筒井 智嗣; 金子 耕士; 宮崎 亮一*; 東中 隆二*; 青木 勇二*; 小林 理気*; 脇本 秀一; Baron, A. Q. R.*; 菅原 仁*; 佐藤 英行*

JPS Conference Proceedings (Internet), 3, p.011060_1 - 011060_5, 2014/06

We have investigated the Ru/Os concentration dependence of the Pr guest mode in Pr(Os$$_{1-x}$$Ru$$_x$$)$$_4$$Sb$$_{12}$$ and its variation with temperature. The Pr guest mode at 3.2 meV in PrOs$$_4$$Sb$$_{12}$$ at the N point linearly shifts to a higher energy with the substitution of Ru into the Os site. The energy of the Pr guest mode decreases with decreasing temperature for all compositions, indicating the presence of an anharmonic potential at the Pr site. The slope of the temperature dependence of the guest mode energy is steeper for pure PrOs$$_4$$Sb$$_{12}$$ than for the other Pr(Os$$_{1-x}$$Ru$$_x$$)$$_4$$Sb$$_{12}$$ compounds we measured. The present results imply the importance of the transition metal in determining anharmonicity in Pr(Os$$_{1-x}$$Ru$$_x$$)$$_4$$Sb$$_{12}$$.


Magnetic-field-enhanced aniferromagnetism in the noncentrosymmetric heavy-fermion superconductor CePt$$_3$$Si

金子 耕士; Stockert, O.*; F${aa}$k, B.*; Raymond, S.*; Skoulatos, M.*; 竹内 徹也*; 大貫 惇睦*

Physical Review B, 89(24), p.241105_1 - 241105_5, 2014/06


 被引用回数:1 パーセンタイル:92.3(Materials Science, Multidisciplinary)

The effect of magnetic field on the static and dynamic spin correlations in the non-centrosymmetric heavy-fermion superconductor CePt$$_3$$Si was investigated by neutron scattering. The application of a magnetic field B increases the antiferromagnetic (AFM) peak intensity. This increase depends strongly on the field direction: for $$B{parallel}c$$ the intensity increases by a factor of 4.6 at a field of 6.6T, which corresponds to more than a doubling of the AFM moment, while the moment increases by only 10% for $$B{parallel}a$$ at 5T. This is in strong contrast to the inelastic response near the antiferromagnetic ordering vector, where no marked field variations are observed for $$B{parallel}c$$ up to 3.8T. The results reveal that the AFM state in CePt$$_3$$Si, which coexists with superconductivity, is distinctly different from other unconventional superconductors.


Instrument design and performance evaluation of a new single crystal neutron diffractometer SENJU at J-PARC

及川 健一; 川崎 卓郎; 大原 高志; 鬼柳 亮嗣; 金子 耕士; 田村 格良; 中村 龍也; 原田 正英; 中尾 朗子*; 花島 隆泰*; et al.

JPS Conference Proceedings (Internet), 1, p.014013_1 - 014013_5, 2014/03

新しいTOF型単結晶中性子回折装置がJ-PARC/MLFのBL18に設置された。本装置「SENJU」は、低温高磁場のような多重極限環境下において1.0mm$$^3$$未満の小さな単結晶を使用して精密な結晶構造や磁気構造解析を実現するために設計された。2012年3月5日に、本装置へ初中性子が導かれ、その後SENJUのハードウェア及びソフトウェアが設計通り機能していることが確認された。また、幾つかの有機及び無機の標準的な単結晶を用いて回折実験が行われた。これらの測定では、高いQ領域(d$$<$$ 0.5 $AA)$のブラッグ反射が明確に測定され、精度よく解析された。発表では、SENJUの装置設計及びその性能評価を詳細に報告する。


Single crystal neutron diffraction study of high neutron absorbing compound EuGa$$_{4}$$

川崎 卓郎; 金子 耕士; 阿曽 尚文*; 仲村 愛*; 辺土 正人*; 仲間 隆男*; 大貫 惇睦*; 大原 高志; 鬼柳 亮嗣; 及川 健一; et al.

JPS Conference Proceedings (Internet), 1, p.014009_1 - 014009_4, 2014/03

Single crystal neutron diffraction measurement of EuGa$$_{4}$$ has been carried out using time-of-flight single crystal neutron diffractometer SENJU at BL18 in MLF/J-PARC. In spite of extremely high neutron absorption of natural Eu, significant numbers of Bragg reflection were observed. Lattice parameters and Bravais lattice at above $$T_mathrm{N}$$ (=15 K) obtained from the positions and systematic extinction of the reflections were well agreed with the result of single crystal X-ray diffraction. Further, magnetic reflections were clearly observed at below $$T_mathrm{N}$$ at the positions of forbidden reflections of body-centered lattice of EuGa$$_{4}$$. An antiferromagnetic structure with the propagation vector $$q$$ = 0 was clarified.

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