Polarity‐Reversal of Exchange Bias in van der Waals FePS<sub>3</sub>/Fe<sub>3</sub>GaTe<sub>2</sub> Heterostructures
Article 2024 en
Authors
HX
Han Xiao
BL
Bingbing Lyu
MM
Mengjuan Mi
Abstract
1 min read
Exchange bias (EB) in antiferromagnetic (AFM)/ferromagnetic heterostructures is crucial for the advancement of spintronic devices and has attracted significant attention. The common EB effect in van der Waals heterostructures features a low blocking temperature (T<sub>b</sub>) and a single polarity. In this work, a significant EB effect with a T<sub>b</sub> up to 150 K is observed in FePS<sub>3</sub>/Fe<sub>3</sub>GaTe<sub>2</sub> heterostructures, and in particular, the EB exhibits an unusual temperature-dependent polarity-reversal behavior. Under a high positive field-cooling condition (e.g., μ<sub>0</sub>H ≥ 0.5 T), a negative EB field (H<sub>EB</sub>) is observed at low temperatures, and with increasing temperature, the H<sub>EB</sub> crosses zero at ≈20 K, subsequently becomes positive and later approaches zero again at T<sub>b</sub>. A model composed of a top FePS<sub>3</sub>/interfacial FePS<sub>3</sub>/Fe<sub>3</sub>GaTe<sub>2</sub> sandwich structure is proposed. The charge transfer from Fe<sub>3</sub>GaTe<sub>2</sub> to FePS<sub>3</sub> at the interface induces net magnetic moments (∆M) in FePS<sub>3</sub>. The interface favors AFM coupling, and thus the reversal of ∆M of the interfacial FePS<sub>3</sub> leads to the polarity-reversal of EB. Moreover, the EB can be extended to the bare Fe<sub>3</sub>GaTe<sub>2</sub> region of the Fe<sub>3</sub>GaTe<sub>2</sub> flake partially covered by FePS<sub>3</sub>. This work provides opportunities for a deeper understanding of the EB effect and opens a new route toward constructing novel spintronic devices.
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