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Two-Dimensional Octuple-Atomic-Layer M(2)Si(2)N(4) (M = Al, Ga and In) with Long Carrier Lifetime

Bulk III-nitride materials MN (M = Al, Ga and In) and their alloys have been widely used in high-power electronic and optoelectronic devices, but stable two-dimensional (2D) III-nitride materials, except h-BN, have not been realized yet. A new kind of 2D III-nitride material M [Formula: see text] Si...

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Autores principales: Ding, Yimin, Xue, Kui, Zhang, Jing, Yan, Luo, Li, Qiaoqiao, Yao, Yisen, Zhou, Liujiang
Formato: Online Artículo Texto
Lenguaje:English
Publicado: MDPI 2023
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9966885/
https://www.ncbi.nlm.nih.gov/pubmed/36838105
http://dx.doi.org/10.3390/mi14020405
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author Ding, Yimin
Xue, Kui
Zhang, Jing
Yan, Luo
Li, Qiaoqiao
Yao, Yisen
Zhou, Liujiang
author_facet Ding, Yimin
Xue, Kui
Zhang, Jing
Yan, Luo
Li, Qiaoqiao
Yao, Yisen
Zhou, Liujiang
author_sort Ding, Yimin
collection PubMed
description Bulk III-nitride materials MN (M = Al, Ga and In) and their alloys have been widely used in high-power electronic and optoelectronic devices, but stable two-dimensional (2D) III-nitride materials, except h-BN, have not been realized yet. A new kind of 2D III-nitride material M [Formula: see text] Si [Formula: see text] N [Formula: see text] (M = Al, Ga and In) is predicted by choosing Si as the appropriate passivation element. The stability, electronic and optical properties of 2D M [Formula: see text] Si [Formula: see text] N [Formula: see text] materials are studied systematically based on first-principles calculations. The results show that Al [Formula: see text] Si [Formula: see text] N [Formula: see text] and Ga [Formula: see text] Si [Formula: see text] N [Formula: see text] are found to be indirect bandgap semiconductors, while In [Formula: see text] Si [Formula: see text] N [Formula: see text] is a direct bandgap semiconductor. Moreover, Al [Formula: see text] Si [Formula: see text] N [Formula: see text] and In [Formula: see text] Si [Formula: see text] N [Formula: see text] have good absorption ability in the visible light region, while Ga [Formula: see text] Si [Formula: see text] N [Formula: see text] is an ultraviolet-light-absorbing material. Furthermore, the carrier lifetimes of Ga [Formula: see text] Si [Formula: see text] N [Formula: see text] and In [Formula: see text] Si [Formula: see text] N [Formula: see text] are as large as 157.89 and 103.99 ns, respectively. All these desirable properties of M [Formula: see text] Si [Formula: see text] N [Formula: see text] materials make them attractive for applications in electronics and photoelectronics.
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spelling pubmed-99668852023-02-26 Two-Dimensional Octuple-Atomic-Layer M(2)Si(2)N(4) (M = Al, Ga and In) with Long Carrier Lifetime Ding, Yimin Xue, Kui Zhang, Jing Yan, Luo Li, Qiaoqiao Yao, Yisen Zhou, Liujiang Micromachines (Basel) Article Bulk III-nitride materials MN (M = Al, Ga and In) and their alloys have been widely used in high-power electronic and optoelectronic devices, but stable two-dimensional (2D) III-nitride materials, except h-BN, have not been realized yet. A new kind of 2D III-nitride material M [Formula: see text] Si [Formula: see text] N [Formula: see text] (M = Al, Ga and In) is predicted by choosing Si as the appropriate passivation element. The stability, electronic and optical properties of 2D M [Formula: see text] Si [Formula: see text] N [Formula: see text] materials are studied systematically based on first-principles calculations. The results show that Al [Formula: see text] Si [Formula: see text] N [Formula: see text] and Ga [Formula: see text] Si [Formula: see text] N [Formula: see text] are found to be indirect bandgap semiconductors, while In [Formula: see text] Si [Formula: see text] N [Formula: see text] is a direct bandgap semiconductor. Moreover, Al [Formula: see text] Si [Formula: see text] N [Formula: see text] and In [Formula: see text] Si [Formula: see text] N [Formula: see text] have good absorption ability in the visible light region, while Ga [Formula: see text] Si [Formula: see text] N [Formula: see text] is an ultraviolet-light-absorbing material. Furthermore, the carrier lifetimes of Ga [Formula: see text] Si [Formula: see text] N [Formula: see text] and In [Formula: see text] Si [Formula: see text] N [Formula: see text] are as large as 157.89 and 103.99 ns, respectively. All these desirable properties of M [Formula: see text] Si [Formula: see text] N [Formula: see text] materials make them attractive for applications in electronics and photoelectronics. MDPI 2023-02-08 /pmc/articles/PMC9966885/ /pubmed/36838105 http://dx.doi.org/10.3390/mi14020405 Text en © 2023 by the authors. https://creativecommons.org/licenses/by/4.0/Licensee MDPI, Basel, Switzerland. This article is an open access article distributed under the terms and conditions of the Creative Commons Attribution (CC BY) license (https://creativecommons.org/licenses/by/4.0/).
spellingShingle Article
Ding, Yimin
Xue, Kui
Zhang, Jing
Yan, Luo
Li, Qiaoqiao
Yao, Yisen
Zhou, Liujiang
Two-Dimensional Octuple-Atomic-Layer M(2)Si(2)N(4) (M = Al, Ga and In) with Long Carrier Lifetime
title Two-Dimensional Octuple-Atomic-Layer M(2)Si(2)N(4) (M = Al, Ga and In) with Long Carrier Lifetime
title_full Two-Dimensional Octuple-Atomic-Layer M(2)Si(2)N(4) (M = Al, Ga and In) with Long Carrier Lifetime
title_fullStr Two-Dimensional Octuple-Atomic-Layer M(2)Si(2)N(4) (M = Al, Ga and In) with Long Carrier Lifetime
title_full_unstemmed Two-Dimensional Octuple-Atomic-Layer M(2)Si(2)N(4) (M = Al, Ga and In) with Long Carrier Lifetime
title_short Two-Dimensional Octuple-Atomic-Layer M(2)Si(2)N(4) (M = Al, Ga and In) with Long Carrier Lifetime
title_sort two-dimensional octuple-atomic-layer m(2)si(2)n(4) (m = al, ga and in) with long carrier lifetime
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9966885/
https://www.ncbi.nlm.nih.gov/pubmed/36838105
http://dx.doi.org/10.3390/mi14020405
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