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論文

Giant Hall effect in a highly conductive frustrated magnet GdCu$$_{2}$$

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$$_{2}$$, 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.

論文

Spin-orbit-entangled state of Ba$$_2$$CaOsO$$_6$$ studied by O $$K$$-edge resonant inelastic X-ray scattering and Raman spectroscopy

岡本 淳*; 芝田 悟朗; 藤森 淳; 他9名*

npj Quantum Materials (Internet), 10, p.44_1 - 44_8, 2025/04

 被引用回数:0 パーセンタイル:64.27(Materials Science, Multidisciplinary)

Transition-metal ions with 5$$d^2$$ electronic configuration in a cubic crystal field are prone to have a vanishing dipolar magnetic moment but finite higher-order multipolar moments, and they are expected to exhibit exotic physical properties. Through an investigation using resonant inelastic X-ray spectroscopy (RIXS), Raman spectroscopy, and theoretical ligand-field multiplet and ab initio calculations, we fully characterized the electronic structure of Ba$$_2$$CaOsO$$_6$$, particularly, the crystal field symmetry of the 5$$d^2$$ electrons in this anomalous material. The low-energy multiplet excitations from RIXS at the oxygen $$K$$ edge and Raman-active phonons both show no splitting, confirming the absence of Jahn-Teller distortion. These findings are consistent with the ground state with the "hidden order" of magnetic octupoles.

論文

Strong local moment antiferromagnetic spin fluctuations in V-doped LiFeAs

Xu, Z.*; Dai, G.*; Li, Y.*; Yin, Z.*; Rong, Y.*; Tian, L.*; Liu, P.*; Wang, H.*; Xing, L.*; Wei, Y.*; et al.

npj Quantum Materials (Internet), 5(1), p.11_1 - 11_7, 2020/02

 被引用回数:5 パーセンタイル:42.20(Materials Science, Multidisciplinary)

We use neutron scattering to study Vanadium (hole)-doped LiFe$$_{1-x}$$V$$_{x}$$As. In the undoped state, LiFeAs exhibits superconductivity at $$T_mathrm{c} = 18$$ K and transverse incommensurate spin excitations similar to electron overdoped iron pnictides. Upon Vanadium doping to form LiFe$$_{0.955}$$V$$_{0.045}$$, the transverse incommensurate spin excitations in LiFeAs transform into longitudinally elongated ones in a similar fashion to that of potassium (hole)-doped Ba$$_{0.7}$$K$$_{0.3}$$Fe$$_{2}$$As$$_{2}$$ but with dramatically enhanced magnetic scattering and elimination of superconductivity. This is different from the suppression of the overall magnetic excitations in hole-doped BaFe$$_{2}$$As$$_{2}$$ and the enhancement of superconductivity near optimal hole doping. These results are consistent with density function theory plus dynamic mean field theory calculations, suggesting that Vanadium doping in LiFeAs may induce an enlarged effective magnetic moment $$S_mathrm{eff}$$ with a spin crossover ground state arising from the inter-orbital scattering of itinerant electrons.

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