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- W4327720956 abstract "A prototype of the monoaxial chiral magnet ${mathrm{CrNb}}_{3}{mathrm{S}}_{6}$ exhibited two magnetostriction (MS) effects: (1) spontaneous MS due to the exchange interaction and spin-orbit coupling (SOC) at zero dc magnetic field ($H$) [Phys. Rev. B 102, 014446 (2020)] and (2) paramagnetic MS due to SOC and Zeeman energy at room temperature [Phys. Rev. B 105, 104412 (2022)]. ${mathrm{CrNb}}_{3}{mathrm{S}}_{6}$ has various magnetic structures, such as helimagnetic, first chiral soliton lattice (CSL-1), second CSL (CSL-2), CSL-2 with irreversibility, and forced ferromagnetic phases, resulting from the Dzyaloshinskii--Moriya interaction as a function of $H$ below the magnetic ordering temperature (${T}_{mathrm{c}}$). In this study, we conducted powder x-ray diffraction analyses to investigate the effects of $H$ and temperature ($T$) on the MS at the atomic level. The $T$ dependence of the lattice constants reveals that below ${T}_{mathrm{c}}$, the MS depends on the magnetic structure. The MS below ${T}_{mathrm{c}}$ is discussed in this study in terms of both the hybridization between the ${z}^{2}$ orbital of $mathrm{Nb}(4f)$ and delocalized ${a}_{1}$ orbital of Cr and the structural symmetry of the ${mathrm{CrS}}_{6}$ octahedron." @default.
- W4327720956 created "2023-03-18" @default.
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- W4327720956 date "2023-02-21" @default.
- W4327720956 modified "2023-10-18" @default.
- W4327720956 title "Magnetic ground state dependent magnetostriction effects on the chiral magnet <mml:math xmlns:mml=http://www.w3.org/1998/Math/MathML><mml:msub><mml:mi mathvariant=normal>CrNb</mml:mi><mml:mn>3</mml:mn></mml:msub><mml:msub><mml:mi mathvariant=normal>S</mml:mi><mml:mn>6</mml:mn></mml:msub></mml:math>" @default.
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- W4327720956 doi "https://doi.org/10.1103/physrevb.107.054427" @default.
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