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Transport properties of MoS(2)/V(7)(Bz)(8) and graphene/V(7)(Bz)(8) vdW junctions tuned by bias and gate voltages
The MoS(2)/V(7)(Bz)(8) and graphene/V(7)(Bz)(8) vdW junctions are designed and the transport properties of their four-terminal devices are comparatively investigated based on density functional theory (DFT) and the nonequilibrium Green's function (NEGF) technique. The MoS(2) and graphene nanori...
Autores principales: | , , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
The Royal Society of Chemistry
2022
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9189623/ https://www.ncbi.nlm.nih.gov/pubmed/35765433 http://dx.doi.org/10.1039/d2ra02196j |
Sumario: | The MoS(2)/V(7)(Bz)(8) and graphene/V(7)(Bz)(8) vdW junctions are designed and the transport properties of their four-terminal devices are comparatively investigated based on density functional theory (DFT) and the nonequilibrium Green's function (NEGF) technique. The MoS(2) and graphene nanoribbons act as the source-to-drain channel and the spin-polarized one-dimensional (1D) benzene–V multidecker complex nanowire (V(7)(Bz)(8)) serves as the gate channel. Gate voltages applied on V(7)(Bz)(8) exert different influences of electron transport on MoS(2)/V(7)(Bz)(8) and graphene/V(7)(Bz)(8). In MoS(2)/V(7)(Bz)(8), the interplay of source and gate bias potentials could induce promising properties such as negative differential resistance (NDR) behavior, output/input current switching, and spin-polarized currents. In contrast, the gate bias plays an insignificant effect on the transport along graphene in graphene/V(7)(Bz)(8). This dissimilarity is attributed to the fact that the conductivity follows the sequence of MoS(2) < V(7)(Bz)(8) < graphene. These transport characteristics are examined by analyzing the conductivity, the currents, the local density of states (LDOS), and the transmission spectra. These results are valuable in designing multi-terminal nanoelectronic devices. |
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