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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
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author Su, Jie
He, Jian
Zhang, Junjing
Lin, Zhenhua
Chang, Jingjing
Zhang, Jincheng
Hao, Yue
author_facet Su, Jie
He, Jian
Zhang, Junjing
Lin, Zhenhua
Chang, Jingjing
Zhang, Jincheng
Hao, Yue
author_sort Su, Jie
collection PubMed
description 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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spelling pubmed-64011282019-03-07 Unusual properties and potential applications of strain BN-MS(2) (M = Mo, W) heterostructures Su, Jie He, Jian Zhang, Junjing Lin, Zhenhua Chang, Jingjing Zhang, Jincheng Hao, Yue Sci Rep Article 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). Nature Publishing Group UK 2019-03-05 /pmc/articles/PMC6401128/ /pubmed/30837562 http://dx.doi.org/10.1038/s41598-019-39970-0 Text en © The Author(s) 2019 Open Access This article is licensed under a Creative Commons Attribution 4.0 International License, which permits use, sharing, adaptation, distribution and reproduction in any medium or format, as long as you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons license, and indicate if changes were made. The images or other third party material in this article are included in the article’s Creative Commons license, unless indicated otherwise in a credit line to the material. If material is not included in the article’s Creative Commons license and your intended use is not permitted by statutory regulation or exceeds the permitted use, you will need to obtain permission directly from the copyright holder. To view a copy of this license, visit http://creativecommons.org/licenses/by/4.0/.
spellingShingle Article
Su, Jie
He, Jian
Zhang, Junjing
Lin, Zhenhua
Chang, Jingjing
Zhang, Jincheng
Hao, Yue
Unusual properties and potential applications of strain BN-MS(2) (M = Mo, W) heterostructures
title Unusual properties and potential applications of strain BN-MS(2) (M = Mo, W) heterostructures
title_full Unusual properties and potential applications of strain BN-MS(2) (M = Mo, W) heterostructures
title_fullStr Unusual properties and potential applications of strain BN-MS(2) (M = Mo, W) heterostructures
title_full_unstemmed Unusual properties and potential applications of strain BN-MS(2) (M = Mo, W) heterostructures
title_short Unusual properties and potential applications of strain BN-MS(2) (M = Mo, W) heterostructures
title_sort unusual properties and potential applications of strain bn-ms(2) (m = mo, w) heterostructures
topic Article
url 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
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