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Hyperfine splitting and nuclear spin polarization in NdPd$$_5$$Al$$_2$$ and Nd$$_3$$Pd$$_{20}$$Ge$$_6$$

目時 直人; 柴田 薫; 松浦 直人*; 北澤 英明*; 鈴木 博之*; 山内 宏樹; 萩原 雅人; Frontzek, M. D.*; 松田 雅昌*

Journal of the Physical Society of Japan, 91(5), p.054710_1 - 054710_6, 2022/05

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

NdPd$$_5$$Al$$_2$$におけるNdの超微細相互作用分裂を高分解能の中性子非弾性散乱によって研究した。Nd核の核スピン($$I$$=7/2)と、$$|pm9/2rangle$$の軌道が主成分の$$Gamma_6$$基底状態を示す4$$f$$電子との間の超微細相互作用によって、磁気秩序相において生じた超微細相互作用分裂に起因する中性子非弾性散乱ピークを、$$hbaromega$$ = $$pm$$3$$mu$$eVのエネルギーに観察した。低温では、Nd核スピンの低エネルギー状態の占拠確率が増加することによりNd核スピンが偏極し、反強磁性散乱ピーク強度に寄与するが、その際、中性子の非スピン反転過程の寄与が最も大きい。この現象の応用として反強磁性散乱ピーク強度の温度変化から、Nd$$_3$$Pd$$_{20}$$Ge$$_6$$のNd磁気モーメント及び超微細相互作用分裂の大きさを見積もることに成功した。


$$q$$=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

 被引用回数:18 パーセンタイル:85.16(Materials Science, Multidisciplinary)

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。


The $$f$$-electron state of the heavy fermion superconductor NpPd$$_5$$Al$$_2$$ and the isostructural family

目時 直人; Aczel, A. A.*; 青木 大*; Chi, S.*; Fernandez-Baca, J. A.*; Griveau, J.-C.*; 萩原 雅人*; Hong, T.*; 芳賀 芳範; 池内 和彦*; et al.

JPS Conference Proceedings (Internet), 30, p.011123_1 - 011123_6, 2020/03



Nature of structural instabilities in superconducting Sr$$_3$$Ir$$_4$$Sn$$_{13}$$

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

JPS Conference Proceedings (Internet), 30, p.011032_1 - 011032_6, 2020/03

A quantum critical point appears as a second-order phase transition which takes place at zero temperature. In contrast to heavy-fermion systems in which magnetism often plays a vital role, recent studies revealed that structural instabilities can drive a system to a quantum critical point as well. In quasi-skutterudite (Ca,Sr)$$_3T_4$$Sn$$_{13}$$ ($$T$$=Rh, Ir), Sr$$_3$$Ir$$_4$$Sn$$_{13}$$ exhibits superconductivity around $$T_{rm sc}$$$${sim}$$5 K and a structural transition at $$T^*{simeq}$$147 K. Applying physical or chemical pressure on Sr$$_3$$Ir$$_4$$Sn$$_{13}$$ suppresses $$T^*$$ rapidly, and a quasi-linear $$T$$ dependence of electrical resistivity, signature of non-Fermi liquid behavior, was observed where $$T^*$$ extrapolates to 0 K. The isomorphs (Ca$$_x$$Sr$$_{1-x}$$)$$_3$$Rh$$_4$$Sn$$_{13}$$ exhibits similar behavior, where the criticality can be reached by $$x{sim}$$0.9 without external pressure. Neutron scattering experiments in Sr$$_3$$Ir$$_4$$Sn$$_{13}$$ evidences the second order nature of the structural transition at $$T^*$$ by the observation of a continuous evolution of superlattice peak below $$T^*$$ and a gradual increase of critical scattering upon approaching to $$T^*$$ by cooling. Increase of $$x$$ in (Ca$$_x$$Sr$$_{1-x}$$)$$_3$$Rh$$_4$$Sn$$_{13}$$ toward the quantum critical point leads to the systematic variation of the critical exponents of the order parameter. In addition, this substitution induces the phonon softening around the M point towards zero energy revealed by inelastic X-ray scattering experiment. We will present systematic variations in both elastic and inelastic channels upon approaching to the quantum critical point.


Coexistence of ferromagnetic and stripe-type antiferromagnetic spin fluctuations in YFe$$_{2}$$Ge$$_{2}$$

Wo, H.*; Wang, Q.*; Shen, Y.*; Zhang, X.*; Hao, Y.*; Feng, Y.*; Shen, S.*; He, Z.*; Pan, B.*; Wang, W.*; et al.

Physical Review Letters, 122(21), p.217003_1 - 217003_5, 2019/05

 被引用回数:3 パーセンタイル:34.77(Physics, Multidisciplinary)

We report neutron scattering measurements of single-crystalline YFe$$_{2}$$Ge$$_{2}$$ in the normal state, which has the same crystal structure as the 122 family of iron pnictide superconductors. YFe$$_{2}$$Ge$$_{2}$$ does not exhibit long-range magnetic order but exhibits strong spin fluctuations. Like the iron pnictides, YFe$$_{2}$$Ge$$_{2}$$ displays anisotropic stripe-type antiferromagnetic spin fluctuations at ($$pi, 0, pi$$). More interesting, however, is the observation of strong spin fluctuations at the in-plane ferromagnetic wave vector ($$0, 0, pi$$). These ferromagnetic spin fluctuations are isotropic in the ($$H, K$$) plane, whose intensity exceeds that of stripe spin fluctuations. Both the ferromagnetic and stripe spin fluctuations remain gapless down to the lowest measured energies. Our results naturally explain the absence of magnetic order in YFe$$_{2}$$Ge$$_{2}$$ and also imply that the ferromagnetic correlations may be a key ingredient for iron-based materials.


New precise measurements of muonium hyperfine structure at J-PARC MUSE

Strasser, P.*; 阿部 充志*; 青木 正治*; Choi, S.*; 深尾 祥紀*; 東 芳隆*; 樋口 嵩*; 飯沼 裕美*; 池戸 豊*; 石田 勝彦*; et al.

EPJ Web of Conferences, 198, p.00003_1 - 00003_8, 2019/01

 被引用回数:12 パーセンタイル:99.51

High precision measurements of the ground state hyperfine structure (HFS) of muonium is a stringent tool for testing bound-state quantum electrodynamics (QED) theory, determining fundamental constants of the muon magnetic moment and mass, and searches for new physics. Muonium is the most suitable system to test QED because both theoretical and experimental values can be precisely determined. Previous measurements were performed decades ago at LAMPF with uncertainties mostly dominated by statistical errors. At the J-PARC Muon Science Facility (MUSE), the MuSEUM collaboration is planning complementary measurements of muonium HFS both at zero and high magnetic field. The new high-intensity muon beam that will soon be available at 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 for high-field measurements, and the latest results at zero field are presented.


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:50 パーセンタイル:95.2(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.


Localized 5$$f^2$$ states in UPd$$_5$$Al$$_2$$ and valence crossover in the Vicinity of Heavy-Fermion superconductivity

目時 直人; 芳賀 芳範; 山本 悦嗣; 松田 雅昌*

Journal of the Physical Society of Japan, 87(11), p.114712_1 - 114712_9, 2018/11

 被引用回数:3 パーセンタイル:32.79(Physics, Multidisciplinary)



$$f$$-electron states in PrPd$$_5$$Al$$_2$$

目時 直人; 山内 宏樹; 鈴木 博之*; 北澤 英明*; 萩原 雅人*; 益田 隆嗣*; Aczel, A. A.*; Chi, S.*; Hong, T.*; 松田 雅昌*; et al.

Journal of the Physical Society of Japan, 87(9), p.094704_1 - 094704_8, 2018/09

 被引用回数:6 パーセンタイル:51.04(Physics, Multidisciplinary)



Polarized neutron scattering study of the multiple order parameter system NdB$$_4$$

目時 直人; 山内 宏樹; 松田 雅昌*; Fernandez-Baca, J. A.*; 綿貫 竜太*; 萩原 雅人*

Physical Review B, 97(17), p.174416_1 - 174416_10, 2018/05

 被引用回数:3 パーセンタイル:18.48(Materials Science, Multidisciplinary)



Measurements and analyses of the distribution of the radioactivity induced by the secondary neutrons produced by 17-MeV protons in compact cyclotron facility

松田 規宏; 泉 雄一*; 山中 吉之*; 丸藤 俊之*; 山田 正明*; 大石 晃嗣*

EPJ Web of Conferences, 153, p.07001_1 - 07001_6, 2017/09

 被引用回数:0 パーセンタイル:0.03

Measurements of reaction rate distributions of secondary neutrons produced by 17-MeV protons were conducted at a compact cyclotron facility with the foil activation method. The experimentally obtained distribution suggests that the target and the deflector as components of the cyclotron are principal beam loss points. The experimental data are compared with the results by the Monte Carlo simulation. The calculated results from the deflector based on the assumption of the beam loss rates were about 3 times higher than the experimental ones. This result implies that the overestimation may results from indeterminate beam loss rates at the deflector.


Measurement of aluminum activation cross section and gas production cross section for 0.4 and 3-GeV protons

明午 伸一郎; 西川 雅章; 岩元 大樹; 松田 洋樹

EPJ Web of Conferences, 146, p.11039_1 - 11039_4, 2017/09


 被引用回数:2 パーセンタイル:80.99



Magnetic structure and dispersion relation of the $$S$$=1/2 quasi-one-dimensional Ising-like antiferromagnet BaCo$$_{2}$$V$$_{2}$$O$$_{8}$$ in a transverse magnetic field

松田 雅昌*; 大西 弘明; 奥谷 顕*; Ma, J.*; Agrawal, H.*; Hong, T.*; Pajerowski, D. M.*; Copley, J. R. D.*; 奥西 巧一*; 森 道康; et al.

Physical Review B, 96(2), p.024439_1 - 024439_8, 2017/07

 被引用回数:11 パーセンタイル:53.05(Materials Science, Multidisciplinary)

BaCo$$_{2}$$V$$_{2}$$O$$_{8}$$ consists of Co chains, in which Co$$^{2+}$$ ion carries a fictitious spin $$frac{1}{2}$$ with Ising anisotropy. We performed elastic and inelastic neutron scattering experiments in BaCo$$_{2}$$V$$_{2}$$O$$_{8}$$ in magnetic field perpendicular to the $$c$$ axis which is the chain direction. With applying magnetic field along the $$a$$ axis at 3.5 K, the antiferromagnetic order with the easy axis along the $$c$$ axis, observed in zero magnetic field, is completely suppressed at 8 T, while the magnetic field gradually induces an antiferromagnetic order with the spin component along the $$b$$ axis. We also studied magnetic excitations as a function of transverse magnetic field. The lower boundary of the spinon excitations splits gradually with increasing magnetic field. The overall feature of the magnetic excitation spectra in magnetic field is reproduced by the theoretical calculation based on the spin $$frac{1}{2}$$ $$XXZ$$ antiferromagnetic chain model, which predicts that the dynamic magnetic structure factor of the spin component along the chain direction is enhanced and that along the field direction has clear incommensurate correlations.


Neutron powder diffraction study on the magnetic structure of NdPd$$_5$$Al$$_2$$

目時 直人; 山内 宏樹; 北澤 英明*; 鈴木 博之*; 萩原 雅人*; Frontzek, M. D.*; 松田 雅昌*; Fernandez-Baca, J. A.*

Journal of the Physical Society of Japan, 86(3), p.034710_1 - 034710_5, 2017/03

 被引用回数:9 パーセンタイル:60.32(Physics, Multidisciplinary)

中性子回折実験によりNdPd$$_5$$Al$$_2$$の磁気構造を研究した。$$q$$=(1/2 0 0)の変調ベクトルで説明できる顕著な反強磁性ピークを磁気転移温度$$T_textrm{N}$$=1.2K以下で観察した。c軸に平行なNdの磁気モーメントは0.3Kで2.9(1)$${mu}_{rm B}$$の大きさであり、a面内で強磁性的に整列した層がa軸方向に++--と4枚周期で配列する。各Nd層の面間隔はa/2である。この構造は$$q$$=(0.23 0.23 0)であるCePd$$_5$$Al$$_2$$によく似ていて、面内成分$$q_{|}$$のみの変調構造は、これらの物質の2次元的なフェルミ面によって生じていると理解できる。その2次元性は、これらの物質の縦長のとてもユニークな形のユニットセルと、2枚PdとAl層によって隔てられたNdの原子間距離がc軸方向に7${AA}$以上ととても大きいことに起因している。


Melting of Pb charge glass and simultaneous Pb-Cr charge transfer in PbCrO$$_{3}$$ as the origin of volume collapse

Yu, R.*; 北條 元*; 綿貫 徹; 水牧 仁一朗*; 溝川 貴司*; 岡 研吾*; Kim, H.*; 町田 晃彦; 榊 浩司*; 中村 優美子*; et al.

Journal of the American Chemical Society, 137(39), p.12719 - 12728, 2015/10

 被引用回数:32 パーセンタイル:70.25(Chemistry, Multidisciplinary)



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:16 パーセンタイル:70.13(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.


Neutron scattering studies of the spin-5/2 antiferromagnetic linear trimer substance SrMn$$_3$$P$$_4$$O$$_{14}$$

長谷 正司*; D$"o$nni, A.*; 小澤 清*; 北澤 英明*; 酒井 治*; Pomjakushin, V. Y.*; Keller, L.*; 金子 耕士; 目時 直人; 加倉井 和久; et al.

Journal of Physics; Conference Series, 340, p.012066_1 - 012066_7, 2012/00

 被引用回数:1 パーセンタイル:45.99

スピン5/2反強磁性Mn量子トリマーの[0, $$k_y$$, 0]インコメンシュレート構造($$k_y$$=0.316-0.331)を中性子粉末回折により明らかにし、$$T_{rm N2}=1.75(5)$$Kにおいて波数が急激に替わることから磁気秩序層が二つ存在することを明らかにした。非弾性散乱実験によって観察された分散を示さない励起(0.46, 0.68, and 1.02meV)が、この系の磁気励起が反強磁性量子トリマーモデルで説明できることを明らかにした。解析によって、量子トリマー形成に重要な最近接相互作用$$J$$$$_1$$=0.29meVが半強磁性的であることを明らかにした。


Magnetic excitations in the spin-5/2 antiferromagnetic trimer substance SrMn$$_3$$P$$_4$$O$$_{14}$$

長谷 正司*; 松田 雅昌*; 金子 耕士; 目時 直人; 加倉井 和久; Yang, T.*; Cong, R.*; Lin, J.*; 小澤 清*; 北澤 英明*

Physical Review B, 84(21), p.214402_1 - 214402_6, 2011/12

 被引用回数:10 パーセンタイル:43.32(Materials Science, Multidisciplinary)

A quantum-mechanical 1/3 magnetization plateau and magnetic long-range order appear in the large-spin (5/2) substance SrMn$$_{3}$$P$$_{4}$$O$$_{14}$$. Previous magnetization results suggest that the spin system consists of antiferromagnetic trimers that are weakly coupled with one another. We inferred that the magnetization plateau originated from discrete energy levels of the trimer. In order to confirm the discrete energy levels, we performed inelastic neutron scattering experiments on SrMn$$_{3}$$P$$_4$$O$$_{14}$$ powders. Observed magnetic excitations are consistent with excitations expected in the trimer model.


Effect of spin dilution on the magnetic state of delafossite CuCrO$$_{2}$$ with an $$S$$ = 3/2 antiferromagnetic triangular sublattice

奥田 哲治*; 宇都 数馬*; 関 真一郎*; 小野瀬 佳文*; 十倉 好紀*; 梶本 亮一; 松田 雅昌*

Journal of the Physical Society of Japan, 80(1), p.014711_1 - 014711_7, 2011/04

 被引用回数:25 パーセンタイル:76.47(Physics, Multidisciplinary)

We investigated an effect of spin dilution on the magnetic and thermal properties of delafossite CuCrO$$_{2}$$ having an $$S$$ = 3/2 antiferromagnetic triangular lattice (ATL) by the substitution of Al$$^{3+}$$ for Cr$$^{3+}$$ by measurements of magnetization, specific heat, and neutron scattering. Spin defects introduced into Cr ATL layers blur the antiferromagnetic transition and induce a dimensional crossover of low-energy magnetic excitation in the residual Cr ATL region due to the reduction of inter-layer magnetic interaction, while accompanying an enhancement of a spin-glass component. The observed $$T^{2}$$ contribution to the low-$$T$$ $$C_mathrm{mag}$$ above $$y$$ = 0.15, as well as in Cu$$_{0.85}$$Ag$$_{0.15}$$CrO$$_{2}$$, comes mainly from a short-range 2D AF excitation originating in a nontrivial magnetic state such as spin-nematic or spin-liquid states.


Anomalous low-field diamagnetic response in ultraclean URu$$_2$$Si$$_2$$ superconductor

岡崎 竜二*; 下澤 雅明*; 宍戸 寛明*; Konczykowski, M.*; 芳賀 芳範; 松田 達磨; 山本 悦嗣; 大貫 惇睦; 柳瀬 陽一*; 芝内 孝禎*; et al.

Journal of Physics; Conference Series, 273, p.012081_1 - 012081_4, 2011/02

 被引用回数:3 パーセンタイル:64.26

The low critical field $$H_{rm c1}$$ in ultraclean URu$$_2$$Si$$_2$$ single crystals with residual resistivity ration exceeding 700 is precisely determined. The whole $$H_{rm c1}$$ for $$H parallel a$$ can be explained by the two-gap with line and point nodes. In contrast, for $$H parallel c$$ a distinct kink in the slope of $$H_{rm c1}$$ was found at 1.2 K, which cannot be accounted for by the two-gap. This outstanding anomaly demonstrates a highly unusual superconducting state embedded in the hidden order state possibly related to the time reversal symmetry breaking.

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