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Dielectric polarization measurements on the antiferromagnetic triangular lattice system CuFeO2 in pulsed high magnetic fields

机译:脉冲强磁场中反铁磁三角晶格系统CuFeO2的介电极化测量

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摘要

Dielectric polarization parallel to the [110] direction of a single crystal of the triangular lattice antiferromagnet CuFeO2 has been measured by a pyroelectric method in pulsed high magnetic fields up to 43 T applied along the [00 1] direction. No distinct spontaneous dielectric polarization P is detected in the fourth field-induced phase with a noncollinear spin structure and 4-, 5-, and 3-sublattice phases with commensurate collinear spin structures. Among five magnetic phases that appear in magnetic fields, a finite P is observed only in the first field-induced phase with the incommensurate noncollinear spin structure. We also confirmed that P in the first field-induced phase is predominantly oriented within the (001) plane. A strong history dependence has been observed in P, and is interpreted in terms of the alignment and repopulation of magnetic Q-domains. The experimental technique for measuring P in pulsed high magnetic fields is described in detail.
机译:已经通过热电法在沿[00 1]方向施加的高达43 T的脉冲高磁场中,通过热电法测量了与三角形晶格反铁磁体CuFeO2的单晶的[110]方向平行的介电极化。在具有非共线自旋结构的第四场感应相和具有相应共线自旋结构的4、5和3亚晶格相中,没有检测到明显的自发电介质极化P。在磁场中出现的五个磁相中,仅在具有不相称的非共线自旋结构的第一场感应相中观察到有限的P。我们还证实,在第一场感应相中的P主要位于(001)平面内。在P中观察到了很强的历史依赖性,并根据磁性Q域的排列和重新组装来解释。详细介绍了在脉冲强磁场中测量P的实验技术。

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