改变磁体中量子几何诱导的内在非线性传导性以及平面内奈尔矢量的测量

Motohiko Ezawa
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引用次数: 0

摘要

由于时间反转对称性被打破,N\'{e}el矢量的$z$分量可以通过反常霍尔电导率在反向磁体中测量。另一方面,如何测量 N\'{e}el 向量的面内分量是一个非难解决的问题。我们研究了由具有拉什巴相互作用的 $d$ 波反向磁体构成的系统的二阶非线性传导性。研究表明,量子计量诱导非线性电导率和非线性德鲁德电导率与N\'{e}el矢量的面内分量成正比,因此,N\'{e}el矢量的面内分量是可测量的。我们得到了量子计量诱导非线性电导率和非线性德鲁德电导率的纵向和横向电导率的解析公式。量子计量诱导非线性电导率在狄拉克点处发散,而非线性德鲁德电导率始终是无限的。因此,无论弛豫时间长短,量子计量诱导的非线性电导率在狄拉克点都占主导地位。
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Intrinsic nonlinear conductivity induced by quantum geometry in altermagnets and measurement of the in-plane Néel vector
The $z$-component of the N\'{e}el 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 N\'{e}el 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 N\'{e}el vector, and hence, the in-plane component of the N\'{e}el 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.
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