Electron-magnon coupling at the interface between a normal metal and a magnetically ordered insulator modifies the electrical conductivity of the normal metal, an effect known as spin-Hall magnetoresistance. It can also facilitate magnon-mediated current drag, the nonlocal electric current response of two normal metal layers separated by a magnetic insulator. In this article, we present a theory of these two spintronic effects and their nonlinear counterparts for time-dependent applied electric fields E(ω), with driving frequencies ω up to the THz regime. We compare various mechanisms leading to a quadratic-in-E response $-$ Joule heating, spin-torque diode effect, and magnonic unidirectional spin-Hall magnetoresistance $-$ and show how these can be disentangled by their characteristic dependences on ω and the magnetization direction.
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Franke et al. (2024) studied this question.
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