Giant magnetoelastic coupling in Love acoustic waveguide based on uniaxial multilayered TbCo2/FeCo nanostructured thin film on Quartz ST-cut

TL;DR

This study investigates the giant magnetoelastic coupling in a uniaxial multilayered TbCo2/FeCo thin film on Quartz ST-cut, demonstrating significant phase velocity shifts and attenuation in shear horizontal acoustic waves for magnetic sensing applications.

Contribution

The paper presents a combined theoretical and experimental analysis of shear horizontal wave interaction with uniaxial multilayered TbCo2/FeCo films, revealing large magnetoelastic effects and high sensitivity for magnetic field sensing.

Findings

Maximum phase velocity shift of 2.5% at 1.2 GHz

Attenuation reaching 500 dB/cm at 1.2 GHz

High sensitivity of 250 ppm/Oe

Abstract

Coupling between dynamic strain and magnetization in ferromagnetic thin films has attracted special consideration as it presents both intriguing fundamental physics problems and technological importance for potential multi-functional devices and information handling. The dynamic strain can be generated by acoustic waves including bulk, surface or guided waves. In this work, we propose the theoretical and experimental investigation of the interaction of pure shear horizontal (SH) wave with a uniaxial multilayered TbCo2/FeCo thin film in a delay line configuration fabricated on Quartz ST-90X cut. We evaluate theoretically the evolution of phase velocity as a function of magnetic field and experimentally the variation of the transmission coefficient. A piezomagnetic model was developed allowing us to calculate the elastic stiffness constants of the multilayer as a function of the applied magnetic field. The model was also implemented for acoustic waves dispersion curves calculation. We show that the evolution of phase velocity is dominated by the C66 elastic stiffness constant variation as expected for the case of shear horizontal surface wave. The fabricated device let us exciting both fundamental and third harmonic shear mode at 410 MHz and 1.2 GHz, respectively. For both modes, the theoretical results corroborate very well the experimental ones. At 1.2 GHz the mode exhibits a maximum phase velocity shift close to 2.5% and an attenuation reaching 500 dB/cm, for a sensitivity as high as 250 ppm/Oe. The reported theoretical model and experimental results are of tremendous interest for the development of advanced devices for magnetic field sensing applications as well as investigating magnon-phonon interaction at a fundamental level.