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Tweaking the Electronic and Optical Properties of α-MoO(3) by Sulphur and Selenium Doping – a Density Functional Theory Study
First-principles calculations were carried out to understand how anionic isovalent-atom doping affects the electronic structures and optical properties of α-MoO(3). The effects of the sulphur and selenium doping at the three unique oxygen sites (O(t), O(a), and O(t)) of α-MoO(3) were examined. We fo...
Autores principales: | , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
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Nature Publishing Group UK
2018
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6031609/ https://www.ncbi.nlm.nih.gov/pubmed/29973657 http://dx.doi.org/10.1038/s41598-018-28522-7 |
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author | Bandaru, Sateesh Saranya, Govindarajan English, Niall J. Yam, Chiyung Chen, Mingyang |
author_facet | Bandaru, Sateesh Saranya, Govindarajan English, Niall J. Yam, Chiyung Chen, Mingyang |
author_sort | Bandaru, Sateesh |
collection | PubMed |
description | First-principles calculations were carried out to understand how anionic isovalent-atom doping affects the electronic structures and optical properties of α-MoO(3). The effects of the sulphur and selenium doping at the three unique oxygen sites (O(t), O(a), and O(t)) of α-MoO(3) were examined. We found that the valence p orbitals of Sulphur/Selenium dopant atoms give rise to impurity bands above the valence band maximum in the band structure of α-MoO(3). The number of impurity bands in the doped material depends on the specific doping sites and the local chemical environment of the dopants in MoO(3). The impurity bands give rise to the enhanced optical absorptions of the S- and Se-doped MoO(3) in the visible and infrared regions. At low local doping concentration, the effects of the dopant sites on the electronic structure of the material are additive, so increasing the doping concentration will enhance the optical absorption properties of the material in the visible and infrared regions. Further increasing the doping concentration will result in a larger gap between the maximum edge of impurity bands and the conduction band minimum, and will undermine the optical absorption in the visible and infrared region. Such effects are caused by the local geometry change at the high local doping concentration with the dopants displaced from the original O sites, so the resulting impurity bands are no long the superpositions of the impurity bands of each individual on-site dopant atom. Switching from S-doping to Se-doping decreases the gap between the maximum edge of the impurity bands and conduction band minimum, and leads to the optical absorption edge red-shifting further into the visible and infrared regions. |
format | Online Article Text |
id | pubmed-6031609 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2018 |
publisher | Nature Publishing Group UK |
record_format | MEDLINE/PubMed |
spelling | pubmed-60316092018-07-11 Tweaking the Electronic and Optical Properties of α-MoO(3) by Sulphur and Selenium Doping – a Density Functional Theory Study Bandaru, Sateesh Saranya, Govindarajan English, Niall J. Yam, Chiyung Chen, Mingyang Sci Rep Article First-principles calculations were carried out to understand how anionic isovalent-atom doping affects the electronic structures and optical properties of α-MoO(3). The effects of the sulphur and selenium doping at the three unique oxygen sites (O(t), O(a), and O(t)) of α-MoO(3) were examined. We found that the valence p orbitals of Sulphur/Selenium dopant atoms give rise to impurity bands above the valence band maximum in the band structure of α-MoO(3). The number of impurity bands in the doped material depends on the specific doping sites and the local chemical environment of the dopants in MoO(3). The impurity bands give rise to the enhanced optical absorptions of the S- and Se-doped MoO(3) in the visible and infrared regions. At low local doping concentration, the effects of the dopant sites on the electronic structure of the material are additive, so increasing the doping concentration will enhance the optical absorption properties of the material in the visible and infrared regions. Further increasing the doping concentration will result in a larger gap between the maximum edge of impurity bands and the conduction band minimum, and will undermine the optical absorption in the visible and infrared region. Such effects are caused by the local geometry change at the high local doping concentration with the dopants displaced from the original O sites, so the resulting impurity bands are no long the superpositions of the impurity bands of each individual on-site dopant atom. Switching from S-doping to Se-doping decreases the gap between the maximum edge of the impurity bands and conduction band minimum, and leads to the optical absorption edge red-shifting further into the visible and infrared regions. Nature Publishing Group UK 2018-07-04 /pmc/articles/PMC6031609/ /pubmed/29973657 http://dx.doi.org/10.1038/s41598-018-28522-7 Text en © The Author(s) 2018 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 Bandaru, Sateesh Saranya, Govindarajan English, Niall J. Yam, Chiyung Chen, Mingyang Tweaking the Electronic and Optical Properties of α-MoO(3) by Sulphur and Selenium Doping – a Density Functional Theory Study |
title | Tweaking the Electronic and Optical Properties of α-MoO(3) by Sulphur and Selenium Doping – a Density Functional Theory Study |
title_full | Tweaking the Electronic and Optical Properties of α-MoO(3) by Sulphur and Selenium Doping – a Density Functional Theory Study |
title_fullStr | Tweaking the Electronic and Optical Properties of α-MoO(3) by Sulphur and Selenium Doping – a Density Functional Theory Study |
title_full_unstemmed | Tweaking the Electronic and Optical Properties of α-MoO(3) by Sulphur and Selenium Doping – a Density Functional Theory Study |
title_short | Tweaking the Electronic and Optical Properties of α-MoO(3) by Sulphur and Selenium Doping – a Density Functional Theory Study |
title_sort | tweaking the electronic and optical properties of α-moo(3) by sulphur and selenium doping – a density functional theory study |
topic | Article |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6031609/ https://www.ncbi.nlm.nih.gov/pubmed/29973657 http://dx.doi.org/10.1038/s41598-018-28522-7 |
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