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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)...

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Detalles Bibliográficos
Autores principales: Su, Jie, He, Jian, Zhang, Junjing, Lin, Zhenhua, Chang, Jingjing, Zhang, Jincheng, Hao, Yue
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Nature Publishing Group UK 2019
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
Descripción
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).