Computation of High Frequency Magnetoelastic Waves in Layered Materials

TL;DR

This paper presents an efficient computational method to analyze high-frequency magnetoelastic wave dispersion in layered magnetic materials, providing detailed insights into energy transfer mechanisms relevant for spintronic devices.

Contribution

It introduces a spectral collocation method to accurately compute magnetoelastic wave dispersion in layered media, including high-frequency regimes relevant for ultrafast magnetism.

Findings

Dispersion maps reveal energy transfer between elastic and magnetic waves.

Analytical approximation explains nonresonant interactions.

Method applicable to various layered configurations.

Abstract

The direct calculation of magnetoelastic wave dispersion in layered media is presented using an efficient, accurate computational technique. The governing, coupled equations for elasticity and magnetism, the Navier and Landau-Lifshitz equations, respectively, are linearized to form a quadratic eigenvalue problem that determines a complex web of wavenumber-frequency dispersion branches and their corresponding mode profiles. Numerical discretization of the eigenvalue problem via a spectral collocation method (SCM) is employed to determine the complete dispersion maps for both a single, finite-thickness magnetic layer and a finite magnetic-nonmagnetic double-layer. The SCM, previously used to study elastic waves in non-magnetic media, is fast, accurate, and adaptable to a variety of sample configurations and geometries. Emphasis is placed on the extremely high frequency regimes being accessed in ultrafast magnetism experiments. The dispersion maps and modes provide insight into how energy propagates through the coupled system, including how energy can be transferred between elastic- and magnetic-dominated waves as well as between different layers. The numerical computations for a single layer are further understood by a simplified analytical calculation in the high-frequency, exchange-dominated regime where the resonance condition required for energy exchange (an anticrossing) between quasi-elastic and quasi-magnetic dispersion branches is determined. Nonresonant interactions are shown to be well approximated by the dispersion of uncoupled elastic and magnetic waves. The methods and results provide fundamental theoretical tools to model and understand current and future magnetic devices powering spintronic innovation.