Electric control of emergent magnonic spin current and dynamic multiferroicity in magnetic insulators at finite temperatures

TL;DR

This paper proposes a method to generate and control magnonic spin currents and multiferroicity in magnetic insulators at finite temperatures using spatially inhomogeneous electric fields, enabling heat-to-spin conversion without large thermal gradients.

Contribution

It introduces a novel approach for electric control of magnonic spin currents and multiferroicity through inhomogeneous electric fields, supported by analytical and numerical methods.

Findings

Electric fields modify magnon dispersion locally.

Gradient in magnon density induces spin current.

Predicted spin currents comparable to thermally driven currents.

Abstract

Conversion of thermal energy into magnonic spin currents and/or effective electric polarization promises new device functionalities. A versatile approach is presented here for generating and controlling open circuit magnonic spin currents and an effective multiferroicity at a uniform temperature with the aid of spatially inhomogeneous, external, static electric fields. This field applied to a ferromagnetic insulator with a Dzyaloshinskii-Moriya type coupling changes locally the magnon dispersion and modifies the density of thermally excited magnons in a region of the scale of the field inhomogeneity. The resulting gradient in the magnon density can be viewed as a gradient in the effective magnon temperature. This effective thermal gradient together with local magnon dispersion result in an open-circuit, electric field controlled magnonic spin current. In fact, for a moderate variation in the external electric field the predicted magnonic spin current is on the scale of the spin (Seebeck) current generated by a comparable external temperature gradient. Analytical methods supported by full-fledge numerics confirm that both, a finite temperature and an inhomogeneous electric field are necessary for this emergent non-equilibrium phenomena. The proposal can be integrated in magnonic and multiferroic circuits, for instance to convert heat into electrically controlled pure spin current using for example nanopatterning, without the need to generate large thermal gradients on the nanoscale.