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具有3-6-8元环和宽带隙半导体特性的二维氮化硼同素异形体铱硼氮(Irida-BN)

Two-dimensional boron nitride allotrope Irida-BN with 3-6-8 membered rings and wide-bandgap semiconducting properties.

作者信息

Pereira Marcelo L, da S Gomes Djardiel, Lima Kleuton A L, Nze Georges D A, Mendonça Fábio L L, Ribeiro Luiz A

机构信息

University of Brasília, College of Technology, Department of Electrical Engineering, Brasília, Brazil.

University of Brasília, Faculty UnB Planaltina, Materials Science Postgraduate Program, Brasília, Brazil.

出版信息

Sci Rep. 2024 Nov 21;14(1):28892. doi: 10.1038/s41598-024-79823-z.

DOI:10.1038/s41598-024-79823-z
PMID:39572707
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC11582624/
Abstract

We present a novel two-dimensional (2D) boron nitride allotrope, Irida- (Ir-BN), analogous to the all-carbon Irida-Graphene (Ir-G). The predicted structure of Ir-BN consists of alternating boron and nitrogen atoms, forming three distinct lattices with 3-, 6-, and 8-membered ring patterns. First-principles calculations based on density functional theory (DFT) formalism and ab initio molecular dynamics (AIMD) simulations were performed to investigate its structural, mechanical, electronic, and optical properties. The Ir-BN lattices exhibit good dynamical and thermal stability, supporting their viability as new 2D materials. Substantial anisotropy is observed in the mechanical properties, with in-plane stiffness ranging from 16 to 142 N/m, depending on the direction, and bulk moduli between 78 and 95 N/m. The electronic structure analysis reveals that Ir-BN is a wide-bandgap semiconductor, with band gaps ranging from 2.4 to 3.2 eV. The material shows optical activity particularly in the visible and ultraviolet regions.

摘要

我们展示了一种新型二维(2D)氮化硼同素异形体,铱型氮化硼(Ir-BN),类似于全碳的铱型石墨烯(Ir-G)。预测的Ir-BN结构由交替的硼和氮原子组成,形成具有3元、6元和8元环图案的三种不同晶格。基于密度泛函理论(DFT)形式主义和从头算分子动力学(AIMD)模拟进行了第一性原理计算,以研究其结构、力学、电子和光学性质。Ir-BN晶格表现出良好的动力学和热稳定性,证明了它们作为新型二维材料的可行性。在力学性能方面观察到显著的各向异性,面内刚度根据方向不同在16至142 N/m之间,体模量在78至95 N/m之间。电子结构分析表明,Ir-BN是一种宽带隙半导体,带隙范围为2.4至3.2 eV。该材料尤其在可见光和紫外区域表现出光学活性。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/fa34/11582624/b715d2689ee7/41598_2024_79823_Fig8_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/fa34/11582624/1899038b60a1/41598_2024_79823_Fig1_HTML.jpg
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https://cdn.ncbi.nlm.nih.gov/pmc/blobs/fa34/11582624/16b96c95fca5/41598_2024_79823_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/fa34/11582624/76f2a54f0a93/41598_2024_79823_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/fa34/11582624/addd531b7b71/41598_2024_79823_Fig6_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/fa34/11582624/c4be0705b87d/41598_2024_79823_Fig7_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/fa34/11582624/b715d2689ee7/41598_2024_79823_Fig8_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/fa34/11582624/1899038b60a1/41598_2024_79823_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/fa34/11582624/546fa97900be/41598_2024_79823_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/fa34/11582624/f70871cca327/41598_2024_79823_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/fa34/11582624/16b96c95fca5/41598_2024_79823_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/fa34/11582624/76f2a54f0a93/41598_2024_79823_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/fa34/11582624/addd531b7b71/41598_2024_79823_Fig6_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/fa34/11582624/c4be0705b87d/41598_2024_79823_Fig7_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/fa34/11582624/b715d2689ee7/41598_2024_79823_Fig8_HTML.jpg

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