To realize room-temperature ferromagnetic semiconductors is still a challenge in spintronics. Recent experiments have obtained two-dimensional (2D) room-temperature ferromagnetic metals, such as monolayer MnSe₂. In this paper, we proposed a way to obtain room-temperature ferromagnetic semiconductors through metal-semiconductor transition. By the density-functional theory calculations, a room-temperature ferromagnetic semiconductor is obtained in monolayer MnSe₂ with a few-percent tensile strain, where a metal-semiconductor transition occurs with 2.2% tensile strain. The tensile strains raise the energy of d orbitals of Mn atoms and p orbitals of Se atoms near the Fermi level, making the Fermi-level sets in the energy gap of bonding and antibonding states of these p and d orbitals, and opening a small band gap. The room-temperature ferromagnetic semiconductors are also obtained in the heterostructures MnSe₂/X (X = Al₂Se₃, GaSe, SiH, and GaP), where metal-semiconductor transition happens due to the tensile strains by interface of heterostructures. In addition, a large magneto-optical Kerr effect (MOKE) is obtained in monolayer MnSe₂ with tensile strain and MnSe₂-based heterostructures. Our theoretical results pave a way to obtain room-temperature magnetic semiconductors from experimentally obtained 2D room-temperature ferromagnetic metals through metal-semiconductor transitions.
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Li et al. (2024) studied this question.
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