Propagating spin waves in nanometer-thick yttrium iron garnet films: Dependence on wave vector, magnetic field strength and angle

TL;DR

This study investigates how propagating spin waves in nanometer-thick yttrium iron garnet films depend on wave vector, magnetic field strength, and angle, providing detailed measurements of their dispersion, damping, and decay length.

Contribution

It offers a comprehensive experimental analysis of spin-wave propagation in thin YIG films, including how key parameters vary with magnetic bias and wave vector, using broadband spectroscopy techniques.

Findings

Damping constant of 3.5 x 10^{-4} in 40-nm YIG film

Maximum decay length of 1.2 mm observed

Strong dependence of spin-wave properties on magnetic field and angle

Abstract

We present a comprehensive investigation of propagating spin waves in nanometer-thick yttrium iron garnet (YIG) films. We use broadband spin-wave spectroscopy with integrated coplanar waveguides (CPWs) and microstrip antennas on top of continuous and patterned YIG films to characterize spin waves with wave vectors up to 10 rad/$\mu$m. All films are grown by pulsed laser deposition. From spin-wave transmission spectra, parameters such as the Gilbert damping constant, spin-wave dispersion relation, group velocity, relaxation time, and decay length are derived and their dependence on magnetic bias field strength and angle is systematically gauged. For a 40-nm-thick YIG film, we obtain a damping constant of $3.5 \times 10^{-4}$ and a maximum decay length of 1.2 mm. Our experiments reveal a strong variation of spin-wave parameters with magnetic bias field and wave vector. Spin-wave properties change considerably up to a magnetic bias field of about 30 mT and above a field angle of $\theta_{H} = 20^{\circ}$, where $\theta_{H} = 0^{\circ}$ corresponds to the Damon-Eshbach configuration.