Tunable magnetic anisotropy and phase transitions in 2D Janus transition-metal chalcogenide halides
Two-dimensional (2D) magnetic semiconductors have received increasing interest for spintronic applications due to their tunable magnetic properties. Using first-principles calculations, we design a series of 2D novel ferromagnetic semiconductors, including VSBr and Janus M<sub>2</sub>S<sub>2</sub>BrX (M = Cr/V, X = F, Cl, I), which exhibit various exotic properties. We realize an indirect-to-direct bandgap transition in Cr<sub>2</sub>S<sub>2</sub>BrF, a giant perpendicular magnetic anisotropy in V<sub>2</sub>S<sub>2</sub>BrI, and a significant <i>T</i><sub>C</sub> enhancement in both V<sub>2</sub>S<sub>2</sub>BrF and V<sub>2</sub>S<sub>2</sub>BrI. Notably, we reveal that biaxial tensile strain can induce a phase transition from ferromagnetic to antiferromagnetic states in the VSBr, V<sub>2</sub>S<sub>2</sub>BrCl and V<sub>2</sub>S<sub>2</sub>BrI, which is driven by the sign reversal of the third nearest-neighbor spin interaction <i>J</i><sub>3</sub>. Meanwhile, under tensile strain, the <i>T</i><sub>C</sub> of VSBr and V<sub>2</sub>S<sub>2</sub>BrCl reach 264 K and 297 K, respectively. These findings highlight our designed materials for great potential applications in advanced electronic and spintronic devices, showcasing their unique capabilities and promising performance.
Authors
- Siyu Han (ORCID: https://orcid.org/0000-0001-8709-5564)
- Jiaqi Wang (ORCID: https://orcid.org/0000-0002-5045-1497)
- Naihua Miao (ORCID: https://orcid.org/0000-0002-5383-9008)
- Jian Zhou (ORCID: https://orcid.org/0000-0003-0531-8918)
- Zhimei Sun (ORCID: https://orcid.org/0000-0002-4438-5032)
- Tong Zhao (ORCID: https://orcid.org/0009-0007-4482-0077)
Institutions
- Beihang University (CN)
Publication Details
- Journal
- Physical Chemistry Chemical Physics
- Published
- 2025-01-01
- DOI
- https://doi.org/10.1039/d5cp01626f
- Citations
- 1
- Primary Topic
- 2D Materials and Applications
- Type
- article
- Field-Weighted Citation Impact
- 0.52