First-principles calculations reveal strong intrinsic magnetic anisotropy and DMI in H-FeTe2, suggesting potential for spintronic applications.
In the ongoing research on two-dimensional (2D) ferromagnetic materials with strong intrinsic Dzyaloshinskii--Moriya interaction (DMI), most efforts have focused on doping, Janus engineering, or heterostructure formation to break inversion symmetry and enhance spin--orbit coupling (SOC). Here, we demonstrate that a pristine 2D material, monolayer H-FeTe₂, can naturally host robust DMI and magnetic anisotropy due to its intrinsic broken inversion symmetry and the strong SOC of Te atoms. We explore the effect of biaxial strain and electron correlation on H-FeTe₂ using first-principles DFT+U calculations. We systematically investigate the Heisenberg exchange interaction, magnetic anisotropy, and DMI in the space spanned by strain and correlation. Our results reveal a distinct, non-monotonic strain dependence of both magnetic anisotropy energy (MAE) and DMI, including a strain-tunable crossover between in-plane and out-of-plane magnetic easy axes. A remarkable enhancement of the in-plane DMI is observed under the combined influence of strain and strong correlations, which is unusual for pristine 2D materials and suggests a favorable regime for spintronic applications.Notably, even in the absence of strain, H-FeTe₂ exhibits finite DMI and considerable anisotropy, which is rare for a pure 2D material. Through these findings, we present H-FeTe₂ as a unique pristine 2D system with robust and tunable spin interactions for exploring fundamental spin--orbit-driven magnetic phenomena.
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Rani et al. (2025) studied this question.
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