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Unusual properties and potential applications of strain BN-MS(2) (M = Mo, W) heterostructures
Heterostructures receive intensive attentions due to their excellent intrinsic properties and wide applications. Here, we investigate the natural physical properties and performances of strain BN-MS(2) (M = Mo, W) heterostructure by density functional theory. Different to compressive monolayer MS(2)...
Autores principales: | , , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
Nature Publishing Group UK
2019
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6401128/ https://www.ncbi.nlm.nih.gov/pubmed/30837562 http://dx.doi.org/10.1038/s41598-019-39970-0 |
Sumario: | Heterostructures receive intensive attentions due to their excellent intrinsic properties and wide applications. Here, we investigate the natural physical properties and performances of strain BN-MS(2) (M = Mo, W) heterostructure by density functional theory. Different to compressive monolayer MS(2), corresponding BN-MS(2) heterostructures keep direct band-gap characters because effects of charge transfer on anti-bonding dz(2) orbitals are stronger than those of Poisson effect. Mexican-hat-like bands without magnetic moments are observed at strain BN-MS(2) heterostructures when the compression is enough. Consequently, electron mobilities of strain BN-MS(2) heterostructures are slightly reduced at first and then enlarged with increasing compressive strain. Note that, strain BN-MS(2) heterostructures reduce the band edges of MS(2) layers and extend their application in photocatalytic water splitting. But just the n-type and p-type Schottky barriers of devices with strain BN-MS(2) heterostructures are reduced and even vanished with the increasing tensile and compressive, respectively. Besides, electron mobilities of strain BN-MoS(2) and BN-WS(2) heterostructures can be enhanced to 1290 and 1926 cm(2) V (−1) s(−1), respectively, with increasing tensile strain. Interestingly, the exciton binding energies of strain BN-MS(2) heterostructures exhibit oscillation variations, different to those of strain monolayer MS(2). |
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