自旋电子学
反铁磁性
居里温度
铁磁性
磁性
单层
密度泛函理论
材料科学
凝聚态物理
带隙
半导体
磁性半导体
光电子学
纳米技术
物理
化学
计算化学
作者
Yujie Liu,Shu Wang,Yanbiao Wang,Zijin Wang,Xue Rui,Jinlian Lu,Yongjun Liu,Xiuyun Zhang,Xueke Yu
标识
DOI:10.1021/acsanm.4c03825
摘要
Currently, two-dimensional (2D) ferromagnetic (FM) materials have become one type of promising spintronic devices. However, the practical applications of 2D FM materials are severely hampered by low Curie temperature ( T C ), which emphasizes the urgent need to design high-temperature 2D ferromagnets. Herein, we predict two stable Kagome-latticed Ti 3 X 4 (X = S or Se) monolayers using first-principles calculations and investigate their stability, electronic structures, and magnetism. The Ti 3 S 4 monolayer is a robust FM bipolar magnetic semiconductor with a band gap of 0.41 eV, and the Ti 3 Se 4 monolayer is a FM half metal (HM) with a band gap in the spin-down channel of 0.44 eV. Monte Carlo simulations indicate that both Ti 3 S 4 and Ti 3 Se 4 monolayers exhibit above-room-temperature T C s of 382 and 436 K, respectively. Interestingly, the FM–antiferromagnetic transition and HM-to-semiconductor transition are found under tensile strains. Our findings propose an effective platform to design promising FM candidates for potential spintronic devices.
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