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Influence of Quenching on the Opto-Electronic Properties of F:SnO(2) Layers

[Image: see text] For many opto-electronic applications, F:SnO(2) materials must benefit from high transparency, high conductivity, and high mechanical strength even after quenching. The purpose of this study was to investigate the influence of quenching on the opto-electronic properties of the F:Sn...

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Autores principales: Manceriu, Laura Maria, Maho, Anthony, Labrugere, Christine, Tixhon, Eric, Schrijnemakers, Audrey, Rougier, Aline, Colson, Pierre, Cloots, Rudi
Formato: Online Artículo Texto
Lenguaje:English
Publicado: American Chemical Society 2020
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7330897/
https://www.ncbi.nlm.nih.gov/pubmed/32637773
http://dx.doi.org/10.1021/acsomega.0c00589
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author Manceriu, Laura Maria
Maho, Anthony
Labrugere, Christine
Tixhon, Eric
Schrijnemakers, Audrey
Rougier, Aline
Colson, Pierre
Cloots, Rudi
author_facet Manceriu, Laura Maria
Maho, Anthony
Labrugere, Christine
Tixhon, Eric
Schrijnemakers, Audrey
Rougier, Aline
Colson, Pierre
Cloots, Rudi
author_sort Manceriu, Laura Maria
collection PubMed
description [Image: see text] For many opto-electronic applications, F:SnO(2) materials must benefit from high transparency, high conductivity, and high mechanical strength even after quenching. The purpose of this study was to investigate the influence of quenching on the opto-electronic properties of the F:SnO(2) layers synthesized at high temperature on Si(x)C(y)O-coated soda-lime glass by atmospheric chemical vapor deposition. The morphology, structure, and composition of the layers were studied before and after quenching in air- and oxygen-rich atmospheres at 670 °C. The free carrier concentration was reduced by oxygen vacancy (V(O)) passivation, as well as by F and Na diffusion, with all effects scaling up with quenching time in air. The transmittance also decreased with quenching time as Na impurities acted as absorption and electron recombination centers. In an oxygen-rich atmosphere, the V(O) passivation was even more emphasized, with however a moderate contribution to conductivity loss. The F:SnO(2) layer microstructure and composition were rather fringed through high-temperature deposition. The almost invariable free carrier concentration and transmittance of the F:SnO(2) samples quenched in O(2) versus air were related to a moderation in Na diffusion. For long quenching times (>20 min) in air, Na and F diffusion prevailed explaining the conductivity drop.
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spelling pubmed-73308972020-07-06 Influence of Quenching on the Opto-Electronic Properties of F:SnO(2) Layers Manceriu, Laura Maria Maho, Anthony Labrugere, Christine Tixhon, Eric Schrijnemakers, Audrey Rougier, Aline Colson, Pierre Cloots, Rudi ACS Omega [Image: see text] For many opto-electronic applications, F:SnO(2) materials must benefit from high transparency, high conductivity, and high mechanical strength even after quenching. The purpose of this study was to investigate the influence of quenching on the opto-electronic properties of the F:SnO(2) layers synthesized at high temperature on Si(x)C(y)O-coated soda-lime glass by atmospheric chemical vapor deposition. The morphology, structure, and composition of the layers were studied before and after quenching in air- and oxygen-rich atmospheres at 670 °C. The free carrier concentration was reduced by oxygen vacancy (V(O)) passivation, as well as by F and Na diffusion, with all effects scaling up with quenching time in air. The transmittance also decreased with quenching time as Na impurities acted as absorption and electron recombination centers. In an oxygen-rich atmosphere, the V(O) passivation was even more emphasized, with however a moderate contribution to conductivity loss. The F:SnO(2) layer microstructure and composition were rather fringed through high-temperature deposition. The almost invariable free carrier concentration and transmittance of the F:SnO(2) samples quenched in O(2) versus air were related to a moderation in Na diffusion. For long quenching times (>20 min) in air, Na and F diffusion prevailed explaining the conductivity drop. American Chemical Society 2020-06-19 /pmc/articles/PMC7330897/ /pubmed/32637773 http://dx.doi.org/10.1021/acsomega.0c00589 Text en Copyright © 2020 American Chemical Society This is an open access article published under an ACS AuthorChoice License (http://pubs.acs.org/page/policy/authorchoice_termsofuse.html) , which permits copying and redistribution of the article or any adaptations for non-commercial purposes.
spellingShingle Manceriu, Laura Maria
Maho, Anthony
Labrugere, Christine
Tixhon, Eric
Schrijnemakers, Audrey
Rougier, Aline
Colson, Pierre
Cloots, Rudi
Influence of Quenching on the Opto-Electronic Properties of F:SnO(2) Layers
title Influence of Quenching on the Opto-Electronic Properties of F:SnO(2) Layers
title_full Influence of Quenching on the Opto-Electronic Properties of F:SnO(2) Layers
title_fullStr Influence of Quenching on the Opto-Electronic Properties of F:SnO(2) Layers
title_full_unstemmed Influence of Quenching on the Opto-Electronic Properties of F:SnO(2) Layers
title_short Influence of Quenching on the Opto-Electronic Properties of F:SnO(2) Layers
title_sort influence of quenching on the opto-electronic properties of f:sno(2) layers
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7330897/
https://www.ncbi.nlm.nih.gov/pubmed/32637773
http://dx.doi.org/10.1021/acsomega.0c00589
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