Tuning THz magnons in a mixed van-der-Waals antiferromagnet

TL;DR

This paper demonstrates the ability to tune the magnon gap across the THz range in a van-der-Waals antiferromagnetic alloy, enabling potential applications in THz technologies and spintronics.

Contribution

It introduces a method to control the magnon gap in a mixed van-der-Waals antiferromagnet by alloying FePS3 and NiPS3, showing wide tunability of magnetic excitations.

Findings

Magnon gap can be tuned across the THz range.

Alloying FePS3 with NiPS3 adjusts magnetic anisotropy.

Wide magnon gap tunability achieved in Fe$_{1-x}$Ni$_x$PS$_3$.

Abstract

Alloying stands out as a pivotal technological method employed across various compounds, be they metallic, magnetic, or semiconducting, serving to fine-tune their properties to meet specific requirements. Ternary semiconductors represent a prominent example of such alloys. They offer fine-tuning of electronic bands, the band gap in particular, thus granting the technology of semiconductor heterostructures devices, key elements in current electronics and optoelectronics. In the realm of magnetically ordered systems, akin to electronic bands in solids, spin waves exhibit characteristic dispersion relations, featuring sizeable magnon gaps in many antiferromagnets. The engineering of the magnon gap constitutes a relevant direction in current research on antiferromagnets, aiming to leverage their distinct properties for THz technologies, spintronics, or magnonics. In this study, we showcase the tunability of the magnon gap across the THz spectral range within an alloy comprising representative semiconducting van-der-Waals antiferromagnets FePS$_3$ and NiPS$_3$. These constituents share identical in-plane crystal structures, magnetic unit cells and the direction of the magnetic anisotropy, but differ in the amplitude and sign of the latter. Altogether these attributes result in the wide tunability of the magnon gap in the Fe$_{1-x}$Ni$_x$PS$_3$ alloy in which the magnetic order is imposed by stronger, perpendicular anisotropy of iron.