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arXiv 2409.09241cond-mat.mes-hall
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交错磁体中由量子几何诱导的内禀非线性电导及面内Néel矢量的测量

Intrinsic nonlinear conductivity induced by quantum geometry in altermagnets and measurement of the in-plane Néel vector

Motohiko Ezawa

AI总结:

本文研究含Rashba相互作用的d波交错磁体二阶非线性电导,证明量子度规与非线性Drude响应可用于测量面内Néel矢量,并给出纵向、横向解析公式。

摘要:

在交错磁体中,由于时间反演对称性破缺,Néel矢量的z分量可通过反常霍尔电导测量。另一方面,如何测量Néel矢量的面内分量则是一个非平凡问题。我们研究了由具有Rashba相互作用的d波交错磁体构成系统的二阶非线性电导。结果表明,量子度规诱导的非线性电导和非线性Drude电导均正比于Néel矢量的面内分量,因此Néel矢量的面内分量是可测量的。我们得到了纵向和横向电导情形下量子度规诱导非线性电导与非线性Drude电导的解析公式。量子度规诱导的非线性电导在Dirac点发散,而非线性Drude电导始终有限。因此,无论弛豫时间如何,量子度规诱导的非线性电导在Dirac点都占主导地位。

英文摘要:

The $z$-component of the Néel vector is measurable by the anomalous Hall conductivity in altermagnets because time reversal symmetry is broken. On the other hand, it is a nontrivial problem how to measure the in-plane component of the Néel vector. We study the second-order nonlinear conductivity of a system made of the $d$-wave altermagnet with the Rashba interaction. It is shown that the quantum-metric induced nonlinear conductivity and the nonlinear Drude conductivity are proportional to the in-plane component of the Néel vector, and hence, the in-plane component of the Néel vector is measurable. We obtain analytic formulas of the quantum-metric induced nonlinear conductivity and the nonlinear Drude conductivity both for the longitudinal and transverse conductivities. The quantum-metric induced nonlinear conductivity diverges at the Dirac point, while the nonlinear Drude conductivity is always finite. Hence, the quantum-metric induced nonlinear conductivity is dominant at the Dirac point irrespective of the relaxation time.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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