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Electron Transport of the Nanojunctions of (BN)(n) (n = 1–4) Linear Chains: A First-Principles Study
[Image: see text] We applied the density functional theory and nonequilibrium Green’s function method (DFT + NEGF) to investigate the relationship between the conductance and chain length in the stretching process, the asymmetric coupling of contact points, and the influence of positive and negative...
Autores principales: | , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
American Chemical Society
2021
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Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8223222/ https://www.ncbi.nlm.nih.gov/pubmed/34179616 http://dx.doi.org/10.1021/acsomega.1c00999 |
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author | Zhao, Ying-Qin Lan, Jun-Qing Hu, Cui-E Mu, Yi Chen, Xiang-Rong |
author_facet | Zhao, Ying-Qin Lan, Jun-Qing Hu, Cui-E Mu, Yi Chen, Xiang-Rong |
author_sort | Zhao, Ying-Qin |
collection | PubMed |
description | [Image: see text] We applied the density functional theory and nonequilibrium Green’s function method (DFT + NEGF) to investigate the relationship between the conductance and chain length in the stretching process, the asymmetric coupling of contact points, and the influence of positive and negative biases on the electron transport properties of the nanojunctions formed by the coupling of (BN)(n) (n = 1–4) linear chains and Au(100)-3 × 3 semi-infinite electrodes. We find that the BN junction has the lowest stability and the (BN)(2) junction has the highest stability. Under zero bias, the equilibrium conductance decreases as the chain length increases; p(x) and p(y) orbitals play a leading role in electron transport. In the bias range of −1.6 to 1.6 V, the current of the (BN)(n) (n = 1–4) linear chains increases linearly with increasing voltage. Under the same bias voltage, (BN)(1) has the largest current, so its electron transport property is the best. The rectification effect reflects the asymmetry of the structure of BN linear chains themselves and the asymmetry of coupling with the Au electrode surfaces at both ends. With the chain length increasing, the transmission spectrum near E(f) is suppressed, the tunneling current decreases, and the rectification ratio increases. (BN)(4) molecular junctions have the largest rectification ratio, reaching 13.32 when the bias voltage is 1.6 V. Additionally, the Au–N strong coupling is more conducive to the electron transport of the molecular chain than the Au–B weak coupling. Our calculations provide an important theoretical reference for the design and development of BN linear-chain nanodevices. |
format | Online Article Text |
id | pubmed-8223222 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2021 |
publisher | American Chemical Society |
record_format | MEDLINE/PubMed |
spelling | pubmed-82232222021-06-25 Electron Transport of the Nanojunctions of (BN)(n) (n = 1–4) Linear Chains: A First-Principles Study Zhao, Ying-Qin Lan, Jun-Qing Hu, Cui-E Mu, Yi Chen, Xiang-Rong ACS Omega [Image: see text] We applied the density functional theory and nonequilibrium Green’s function method (DFT + NEGF) to investigate the relationship between the conductance and chain length in the stretching process, the asymmetric coupling of contact points, and the influence of positive and negative biases on the electron transport properties of the nanojunctions formed by the coupling of (BN)(n) (n = 1–4) linear chains and Au(100)-3 × 3 semi-infinite electrodes. We find that the BN junction has the lowest stability and the (BN)(2) junction has the highest stability. Under zero bias, the equilibrium conductance decreases as the chain length increases; p(x) and p(y) orbitals play a leading role in electron transport. In the bias range of −1.6 to 1.6 V, the current of the (BN)(n) (n = 1–4) linear chains increases linearly with increasing voltage. Under the same bias voltage, (BN)(1) has the largest current, so its electron transport property is the best. The rectification effect reflects the asymmetry of the structure of BN linear chains themselves and the asymmetry of coupling with the Au electrode surfaces at both ends. With the chain length increasing, the transmission spectrum near E(f) is suppressed, the tunneling current decreases, and the rectification ratio increases. (BN)(4) molecular junctions have the largest rectification ratio, reaching 13.32 when the bias voltage is 1.6 V. Additionally, the Au–N strong coupling is more conducive to the electron transport of the molecular chain than the Au–B weak coupling. Our calculations provide an important theoretical reference for the design and development of BN linear-chain nanodevices. American Chemical Society 2021-06-08 /pmc/articles/PMC8223222/ /pubmed/34179616 http://dx.doi.org/10.1021/acsomega.1c00999 Text en © 2021 The Authors. Published by American Chemical Society Permits non-commercial access and re-use, provided that author attribution and integrity are maintained; but does not permit creation of adaptations or other derivative works (https://creativecommons.org/licenses/by-nc-nd/4.0/). |
spellingShingle | Zhao, Ying-Qin Lan, Jun-Qing Hu, Cui-E Mu, Yi Chen, Xiang-Rong Electron Transport of the Nanojunctions of (BN)(n) (n = 1–4) Linear Chains: A First-Principles Study |
title | Electron Transport of the Nanojunctions of (BN)(n) (n = 1–4) Linear Chains:
A First-Principles Study |
title_full | Electron Transport of the Nanojunctions of (BN)(n) (n = 1–4) Linear Chains:
A First-Principles Study |
title_fullStr | Electron Transport of the Nanojunctions of (BN)(n) (n = 1–4) Linear Chains:
A First-Principles Study |
title_full_unstemmed | Electron Transport of the Nanojunctions of (BN)(n) (n = 1–4) Linear Chains:
A First-Principles Study |
title_short | Electron Transport of the Nanojunctions of (BN)(n) (n = 1–4) Linear Chains:
A First-Principles Study |
title_sort | electron transport of the nanojunctions of (bn)(n) (n = 1–4) linear chains:
a first-principles study |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8223222/ https://www.ncbi.nlm.nih.gov/pubmed/34179616 http://dx.doi.org/10.1021/acsomega.1c00999 |
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