Hard ferromagnetism down to the thinnest limit of iron-intercalated tantalum disulfide

TL;DR

This study demonstrates that Fe-intercalated TaS2 maintains ferromagnetic order down to the bilayer limit with giant coercivities, highlighting chemical intercalation as a versatile method to tailor magnetic properties in 2D materials.

Contribution

It reveals that chemical intercalation enables the stabilization of hard ferromagnetism in atomically thin Fe-intercalated TaS2, with tunable magnetic properties based on intercalation parameters.

Findings

Ferromagnetic order persists in bilayer Fe$_x$TaS$_2$ with coercivity up to 3 Tesla.

Chemical intercalation allows tuning of magnetic properties in 2D van der Waals crystals.

Dimensionality, intercalation degree, and order influence the magnetic behavior of Fe$_x$TaS$_2$.

Abstract

Two-dimensional (2D) magnetic crystals hold promise for miniaturized and ultralow power electronic devices that exploit spin manipulation. In these materials, large, controllable magnetocrystalline anisotropy is a prerequisite for the stabilization and manipulation of long-range magnetic order. In known 2D magnetic crystals, relatively weak magnetocrystalline anisotropy results in typically soft ferromagnetism. Here, we demonstrate that ferromagnetic order persists down to the thinnest limit of Fe$_x$TaS$_2$ (Fe-intercalated bilayer 2H-TaS$_2$) with giant coercivities up to 3 tesla. We prepare Fe-intercalated TaS$_2$ by chemical intercalation of van der Waals layered 2H-TaS$_2$ crystals and perform variable-temperature quantum transport, transmission electron microscopy, and confocal Raman spectroscopy measurements to shed new light on the coupled effects of dimensionality, degree of intercalation, and intercalant order/disorder on the hard ferromagnetic behavior of Fe$_x$TaS$_2$. More generally, we show that chemical intercalation gives access to a rich synthetic parameter space for low-dimensional magnets, in which magnetic properties can be tailored by the choice of the host material and intercalant identity/amount, in addition to the manifold distinctive degrees of freedom available in atomically thin, van der Waals crystals.