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Interface contact and modulated electronic properties by in-plain strains in a graphene–MoS(2) heterostructure
Designing a specific heterojunction by assembling suitable two-dimensional (2D) semiconductors has shown significant potential in next-generation micro-nano electronic devices. In this paper, we study the structural and electronic properties of graphene–MoS(2) (Gr–MoS(2)) heterostructures with in-pl...
Autores principales: | , , , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
The Royal Society of Chemistry
2023
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9850458/ https://www.ncbi.nlm.nih.gov/pubmed/36756432 http://dx.doi.org/10.1039/d2ra07949f |
Sumario: | Designing a specific heterojunction by assembling suitable two-dimensional (2D) semiconductors has shown significant potential in next-generation micro-nano electronic devices. In this paper, we study the structural and electronic properties of graphene–MoS(2) (Gr–MoS(2)) heterostructures with in-plain biaxial strain using density functional theory. It is found that the interaction between graphene and monolayer MoS(2) is characterized by a weak van der Waals interlayer coupling with the stable layer spacing of 3.39 Å and binding energy of 0.35 J m(−2). In the presence of MoS(2), the linear bands on the Dirac cone of graphene are slightly split. A tiny band gap about 1.2 meV opens in the Gr–MoS(2) heterojunction due to the breaking of sublattice symmetry, and it could be effectively modulated by strain. Furthermore, an n-type Schottky contact is formed at the Gr–MoS(2) interface with a Schottky barrier height of 0.33 eV, which can be effectively modulated by in-plane strain. Especially, an n-type ohmic contact is obtained when 6% tensile strain is imposed. The appearance of the non-zero band gap in graphene has opened up new possibilities for its application and the ohmic contact predicts the Gr–MoS(2) van der Waals heterojunction nanocomposite as a competitive candidate in next-generation optoelectronics and Schottky devices. |
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