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Origins of Negative Differential Resistance in N-doped ZnO Nano-ribbons: Ab-initio Investigation

The electronic transport in low-dimensional materials is controlled by quantum coherence and non-equilibrium statistics. The scope of the present investigation is to search for the origins of negative-differential resistance (NDR) behavior in N-doped ultra-narrow zigzag-edge ZnO nano-ribbons (ZnO-NR...

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Autores principales: Shaheen, Alaa, Ali, Muhammad, Othman, Wael, Tit, Nacir
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Nature Publishing Group UK 2019
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6617463/
https://www.ncbi.nlm.nih.gov/pubmed/31289305
http://dx.doi.org/10.1038/s41598-019-46335-0
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author Shaheen, Alaa
Ali, Muhammad
Othman, Wael
Tit, Nacir
author_facet Shaheen, Alaa
Ali, Muhammad
Othman, Wael
Tit, Nacir
author_sort Shaheen, Alaa
collection PubMed
description The electronic transport in low-dimensional materials is controlled by quantum coherence and non-equilibrium statistics. The scope of the present investigation is to search for the origins of negative-differential resistance (NDR) behavior in N-doped ultra-narrow zigzag-edge ZnO nano-ribbons (ZnO-NRs). A state-of-the-art technique, based on a combination of density-functional theory (DFT) and non-equilibrium Green’s function (NEGF) formalism, is employed to probe the electronic and transport properties. The effect of location of N dopant, with respect to the NR edges, on IV-curve and NDR is tested and three different positions for N-atom are considered: (i) at the oxygen-rich edge; (ii) at the center; and (iii) at the Zn-rich edge. The results show that both resistance and top-to-valley current ratio (TVCR) reduce when N-atom is displaced from O-rich edge to center to Zn-rich edge, respectively. After an analysis based on the calculations of transmission coefficient versus bias, band structures, and charge-density plots of HOMO/LUMO states, one is able to draw a conclusion about the origins of NDR. The unpaired electron of N dopant is causing the curdling/localization of wave-function, which in turn causes strong back-scattering and suppression of conductive channels. These effects manifest themselves in the drawback of electric current (or so called NDR). The relevance of NDR for applications in nano-electronic devices (e.g., switches, rectifiers, amplifiers, gas sensing) is further discussed.
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spelling pubmed-66174632019-07-18 Origins of Negative Differential Resistance in N-doped ZnO Nano-ribbons: Ab-initio Investigation Shaheen, Alaa Ali, Muhammad Othman, Wael Tit, Nacir Sci Rep Article The electronic transport in low-dimensional materials is controlled by quantum coherence and non-equilibrium statistics. The scope of the present investigation is to search for the origins of negative-differential resistance (NDR) behavior in N-doped ultra-narrow zigzag-edge ZnO nano-ribbons (ZnO-NRs). A state-of-the-art technique, based on a combination of density-functional theory (DFT) and non-equilibrium Green’s function (NEGF) formalism, is employed to probe the electronic and transport properties. The effect of location of N dopant, with respect to the NR edges, on IV-curve and NDR is tested and three different positions for N-atom are considered: (i) at the oxygen-rich edge; (ii) at the center; and (iii) at the Zn-rich edge. The results show that both resistance and top-to-valley current ratio (TVCR) reduce when N-atom is displaced from O-rich edge to center to Zn-rich edge, respectively. After an analysis based on the calculations of transmission coefficient versus bias, band structures, and charge-density plots of HOMO/LUMO states, one is able to draw a conclusion about the origins of NDR. The unpaired electron of N dopant is causing the curdling/localization of wave-function, which in turn causes strong back-scattering and suppression of conductive channels. These effects manifest themselves in the drawback of electric current (or so called NDR). The relevance of NDR for applications in nano-electronic devices (e.g., switches, rectifiers, amplifiers, gas sensing) is further discussed. Nature Publishing Group UK 2019-07-09 /pmc/articles/PMC6617463/ /pubmed/31289305 http://dx.doi.org/10.1038/s41598-019-46335-0 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
Shaheen, Alaa
Ali, Muhammad
Othman, Wael
Tit, Nacir
Origins of Negative Differential Resistance in N-doped ZnO Nano-ribbons: Ab-initio Investigation
title Origins of Negative Differential Resistance in N-doped ZnO Nano-ribbons: Ab-initio Investigation
title_full Origins of Negative Differential Resistance in N-doped ZnO Nano-ribbons: Ab-initio Investigation
title_fullStr Origins of Negative Differential Resistance in N-doped ZnO Nano-ribbons: Ab-initio Investigation
title_full_unstemmed Origins of Negative Differential Resistance in N-doped ZnO Nano-ribbons: Ab-initio Investigation
title_short Origins of Negative Differential Resistance in N-doped ZnO Nano-ribbons: Ab-initio Investigation
title_sort origins of negative differential resistance in n-doped zno nano-ribbons: ab-initio investigation
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6617463/
https://www.ncbi.nlm.nih.gov/pubmed/31289305
http://dx.doi.org/10.1038/s41598-019-46335-0
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