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Electronic and Magnetic Properties of Defected Monolayer WSe(2) with Vacancies

By adopting the first-principle methods based on the density functional theory, we studied the structural, electronic, and magnetic properties of defected monolayer WSe(2) with vacancies and the influences of external strain on the defected configurations. Our calculations show that the two W atom v...

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Detalles Bibliográficos
Autores principales: Yang, Danxi, Fan, Xiaoli, Zhang, Fengxia, Hu, Yan, Luo, Zhifen
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Springer US 2019
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6548794/
https://www.ncbi.nlm.nih.gov/pubmed/31165263
http://dx.doi.org/10.1186/s11671-019-3002-2
Descripción
Sumario:By adopting the first-principle methods based on the density functional theory, we studied the structural, electronic, and magnetic properties of defected monolayer WSe(2) with vacancies and the influences of external strain on the defected configurations. Our calculations show that the two W atom vacancies (V(W2)) and one W atom and its nearby three pairs of Se atom vacancies (V(WSe6)) both induce magnetism into monolayer WSe(2) with magnetic moments of 2 and 6 μ(B), respectively. The magnetic moments are mainly contributed by the atoms around the vacancies. Particularly, monolayer WSe(2) with V(W2) is half-metallic. Additionally, one Se and one W atom vacancies (V(Se), V(W)), two Se atom vacancies (V(Se-Se)), and one W atom and the nearby three Se atoms on the same layer vacancy (V(WSe3))-doped monolayer WSe(2) remain as non-magnetic semiconducting. But the impure electronic states attributed from the W d and Se p orbitals around the vacancies locate around the Fermi level and narrow down the energy gaps. Meanwhile, our calculations indicate that the tensile strain of 0~7% not only manipulates the electronic properties of defected monolayer WSe(2) with vacancies by narrowing down their energy gaps, but also controls the magnetic moments of V(W)-, V(W2)-, and V(WSe6)-doped monolayer WSe(2).