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Tuning the Metal–Insulator Transition Properties of VO(2) Thin Films with the Synergetic Combination of Oxygen Vacancies, Strain Engineering, and Tungsten Doping

Vanadium oxide (VO(2)) is considered a Peierls–Mott insulator with a metal–insulator transition (MIT) at T(c) = 68° C. The tuning of MIT parameters is a crucial point to use VO(2) within thermoelectric, electrochromic, or thermochromic applications. In this study, the effect of oxygen deficiencies,...

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Autores principales: Basyooni, Mohamed A., Al-Dossari, Mawaheb, Zaki, Shrouk E., Eker, Yasin Ramazan, Yilmaz, Mucahit, Shaban, Mohamed
Formato: Online Artículo Texto
Lenguaje:English
Publicado: MDPI 2022
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9099983/
https://www.ncbi.nlm.nih.gov/pubmed/35564181
http://dx.doi.org/10.3390/nano12091470
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author Basyooni, Mohamed A.
Al-Dossari, Mawaheb
Zaki, Shrouk E.
Eker, Yasin Ramazan
Yilmaz, Mucahit
Shaban, Mohamed
author_facet Basyooni, Mohamed A.
Al-Dossari, Mawaheb
Zaki, Shrouk E.
Eker, Yasin Ramazan
Yilmaz, Mucahit
Shaban, Mohamed
author_sort Basyooni, Mohamed A.
collection PubMed
description Vanadium oxide (VO(2)) is considered a Peierls–Mott insulator with a metal–insulator transition (MIT) at T(c) = 68° C. The tuning of MIT parameters is a crucial point to use VO(2) within thermoelectric, electrochromic, or thermochromic applications. In this study, the effect of oxygen deficiencies, strain engineering, and metal tungsten doping are combined to tune the MIT with a low phase transition of 20 °C in the air without capsulation. Narrow hysteresis phase transition devices based on multilayer VO(2), WO(3), Mo(0.2)W(0.8)O(3,) and/or MoO(3) oxide thin films deposited through a high vacuum sputtering are investigated. The deposited films are structurally, chemically, electrically, and optically characterized. Different conductivity behaviour was observed, with the highest value towards VO(1.75)/WO(2.94) and the lowest VO(1.75) on FTO glass. VO(1.75)/WO(2.94) showed a narrow hysteresis curve with a single-phase transition. Thanks to the role of oxygen vacancies, the MIT temperature decreased to 35 °C, while the lowest value (T(c) = 20 °C) was reached with Mo(0.2)W(0.8)O(3)/VO(2)/MoO(3) structure. In this former sample, Mo(0.2)W(0.8)O(3) was used for the first time as an anti-reflective and anti-oxidative layer. The results showed that the MoO(3) bottom layer is more suitable than WO(3) to enhance the electrical properties of VO(2) thin films. This work is applied to fast phase transition devices.
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spelling pubmed-90999832022-05-14 Tuning the Metal–Insulator Transition Properties of VO(2) Thin Films with the Synergetic Combination of Oxygen Vacancies, Strain Engineering, and Tungsten Doping Basyooni, Mohamed A. Al-Dossari, Mawaheb Zaki, Shrouk E. Eker, Yasin Ramazan Yilmaz, Mucahit Shaban, Mohamed Nanomaterials (Basel) Article Vanadium oxide (VO(2)) is considered a Peierls–Mott insulator with a metal–insulator transition (MIT) at T(c) = 68° C. The tuning of MIT parameters is a crucial point to use VO(2) within thermoelectric, electrochromic, or thermochromic applications. In this study, the effect of oxygen deficiencies, strain engineering, and metal tungsten doping are combined to tune the MIT with a low phase transition of 20 °C in the air without capsulation. Narrow hysteresis phase transition devices based on multilayer VO(2), WO(3), Mo(0.2)W(0.8)O(3,) and/or MoO(3) oxide thin films deposited through a high vacuum sputtering are investigated. The deposited films are structurally, chemically, electrically, and optically characterized. Different conductivity behaviour was observed, with the highest value towards VO(1.75)/WO(2.94) and the lowest VO(1.75) on FTO glass. VO(1.75)/WO(2.94) showed a narrow hysteresis curve with a single-phase transition. Thanks to the role of oxygen vacancies, the MIT temperature decreased to 35 °C, while the lowest value (T(c) = 20 °C) was reached with Mo(0.2)W(0.8)O(3)/VO(2)/MoO(3) structure. In this former sample, Mo(0.2)W(0.8)O(3) was used for the first time as an anti-reflective and anti-oxidative layer. The results showed that the MoO(3) bottom layer is more suitable than WO(3) to enhance the electrical properties of VO(2) thin films. This work is applied to fast phase transition devices. MDPI 2022-04-26 /pmc/articles/PMC9099983/ /pubmed/35564181 http://dx.doi.org/10.3390/nano12091470 Text en © 2022 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
Basyooni, Mohamed A.
Al-Dossari, Mawaheb
Zaki, Shrouk E.
Eker, Yasin Ramazan
Yilmaz, Mucahit
Shaban, Mohamed
Tuning the Metal–Insulator Transition Properties of VO(2) Thin Films with the Synergetic Combination of Oxygen Vacancies, Strain Engineering, and Tungsten Doping
title Tuning the Metal–Insulator Transition Properties of VO(2) Thin Films with the Synergetic Combination of Oxygen Vacancies, Strain Engineering, and Tungsten Doping
title_full Tuning the Metal–Insulator Transition Properties of VO(2) Thin Films with the Synergetic Combination of Oxygen Vacancies, Strain Engineering, and Tungsten Doping
title_fullStr Tuning the Metal–Insulator Transition Properties of VO(2) Thin Films with the Synergetic Combination of Oxygen Vacancies, Strain Engineering, and Tungsten Doping
title_full_unstemmed Tuning the Metal–Insulator Transition Properties of VO(2) Thin Films with the Synergetic Combination of Oxygen Vacancies, Strain Engineering, and Tungsten Doping
title_short Tuning the Metal–Insulator Transition Properties of VO(2) Thin Films with the Synergetic Combination of Oxygen Vacancies, Strain Engineering, and Tungsten Doping
title_sort tuning the metal–insulator transition properties of vo(2) thin films with the synergetic combination of oxygen vacancies, strain engineering, and tungsten doping
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9099983/
https://www.ncbi.nlm.nih.gov/pubmed/35564181
http://dx.doi.org/10.3390/nano12091470
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