Effect of selective lateral chromium doping by rf magnetron sputtering on the structural, and opto-electrical properties of nickel oxide
In this study, chromium (Cr)-doped nickel oxide (NiO) thin films were deposited by employing selective lateral doping of Cr in NiO by radio-frequency magnetron sputtering at different doping times ranging from 0 s (undoped) to 80 s. The structural, optical, and electrical properties of the resulting...
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my.uniten.dspace-258652023-05-29T17:05:21Z Effect of selective lateral chromium doping by rf magnetron sputtering on the structural, and opto-electrical properties of nickel oxide Jamal M.S. Sobayel K. Misran H. Nasrin T. Althubeiti K. Alkhammash H.I. Shahiduzzaman M. Sopian K. Amin N. Akhtaruzzaman M. 55887499100 57194049079 6506899840 57218826777 57209509894 56711980800 55640096500 7003375391 7102424614 57195441001 In this study, chromium (Cr)-doped nickel oxide (NiO) thin films were deposited by employing selective lateral doping of Cr in NiO by radio-frequency magnetron sputtering at different doping times ranging from 0 s (undoped) to 80 s. The structural, optical, and electrical properties of the resulting Cr-doped NiO thin films were investigated. Structural investigation from XRD patterns indicated that the grown Cr-doped NiO layer crystallized in a cubic phase. Broadening of the diffraction peak with increasing doping time from 0 s to 80 s led to a reduction in the crystallite size that varied from 23.52 nm to 14.65 nm. Compared with the undoped NiO, the diffraction peak along the (200) plane shifted from left to right as a function of doping time. This result indicated that Cr+3 could easily enter the NiO lattice. Results from the Hall-effect study disclosed that electrical properties of Cr-doped NiO was highly dependent on doping time. The conductivity of NiO was increased with doping time, and the highest conductivity (8.73 � 10?2 Scm?1) was achieved at a doping time of 80 s. Finally, optical investigations revealed that as doping time increased, the optical bandgap of Cr-doped NiO films dropped from 3.43 eV to 3.28 eV. The highest Urbach energy at higher doping time indicated that crystallinity became poorer, and the degree of defects increased with increasing doping time. � 2021 by the authors. 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/). Final 2023-05-29T09:05:21Z 2023-05-29T09:05:21Z 2021 Article 10.3390/app112311546 2-s2.0-85120782049 https://www.scopus.com/inward/record.uri?eid=2-s2.0-85120782049&doi=10.3390%2fapp112311546&partnerID=40&md5=c6782bfecef3b5d1a7bb6c0950e3e87e https://irepository.uniten.edu.my/handle/123456789/25865 11 23 11546 All Open Access, Gold MDPI Scopus |
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In this study, chromium (Cr)-doped nickel oxide (NiO) thin films were deposited by employing selective lateral doping of Cr in NiO by radio-frequency magnetron sputtering at different doping times ranging from 0 s (undoped) to 80 s. The structural, optical, and electrical properties of the resulting Cr-doped NiO thin films were investigated. Structural investigation from XRD patterns indicated that the grown Cr-doped NiO layer crystallized in a cubic phase. Broadening of the diffraction peak with increasing doping time from 0 s to 80 s led to a reduction in the crystallite size that varied from 23.52 nm to 14.65 nm. Compared with the undoped NiO, the diffraction peak along the (200) plane shifted from left to right as a function of doping time. This result indicated that Cr+3 could easily enter the NiO lattice. Results from the Hall-effect study disclosed that electrical properties of Cr-doped NiO was highly dependent on doping time. The conductivity of NiO was increased with doping time, and the highest conductivity (8.73 � 10?2 Scm?1) was achieved at a doping time of 80 s. Finally, optical investigations revealed that as doping time increased, the optical bandgap of Cr-doped NiO films dropped from 3.43 eV to 3.28 eV. The highest Urbach energy at higher doping time indicated that crystallinity became poorer, and the degree of defects increased with increasing doping time. � 2021 by the authors. 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/). |
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55887499100 |
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55887499100 Jamal M.S. Sobayel K. Misran H. Nasrin T. Althubeiti K. Alkhammash H.I. Shahiduzzaman M. Sopian K. Amin N. Akhtaruzzaman M. |
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Jamal M.S. Sobayel K. Misran H. Nasrin T. Althubeiti K. Alkhammash H.I. Shahiduzzaman M. Sopian K. Amin N. Akhtaruzzaman M. |
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Jamal M.S. Sobayel K. Misran H. Nasrin T. Althubeiti K. Alkhammash H.I. Shahiduzzaman M. Sopian K. Amin N. Akhtaruzzaman M. Effect of selective lateral chromium doping by rf magnetron sputtering on the structural, and opto-electrical properties of nickel oxide |
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Jamal M.S. |
title |
Effect of selective lateral chromium doping by rf magnetron sputtering on the structural, and opto-electrical properties of nickel oxide |
title_short |
Effect of selective lateral chromium doping by rf magnetron sputtering on the structural, and opto-electrical properties of nickel oxide |
title_full |
Effect of selective lateral chromium doping by rf magnetron sputtering on the structural, and opto-electrical properties of nickel oxide |
title_fullStr |
Effect of selective lateral chromium doping by rf magnetron sputtering on the structural, and opto-electrical properties of nickel oxide |
title_full_unstemmed |
Effect of selective lateral chromium doping by rf magnetron sputtering on the structural, and opto-electrical properties of nickel oxide |
title_sort |
effect of selective lateral chromium doping by rf magnetron sputtering on the structural, and opto-electrical properties of nickel oxide |
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MDPI |
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2023 |
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1806428078567587840 |
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13.214268 |