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Investigation of Combinatorial WO(3)-MoO(3) Mixed Layers by Spectroscopic Ellipsometry Using Different Optical Models
Reactive (Ar-O(2) plasma) magnetron sputtered WO(3)-MoO(3) (nanometer scaled) mixed layers were investigated and mapped by Spectroscopic Ellipsometry (SE). The W- and Mo-targets were placed separately, and 30 × 30 cm glass substrates were slowly moved under the two (W and Mo) separated targets. We u...
Autores principales: | , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
MDPI
2022
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9317069/ https://www.ncbi.nlm.nih.gov/pubmed/35889645 http://dx.doi.org/10.3390/nano12142421 |
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author | Fried, Miklos Bogar, Renato Takacs, Daniel Labadi, Zoltan Horvath, Zsolt Endre Zolnai, Zsolt |
author_facet | Fried, Miklos Bogar, Renato Takacs, Daniel Labadi, Zoltan Horvath, Zsolt Endre Zolnai, Zsolt |
author_sort | Fried, Miklos |
collection | PubMed |
description | Reactive (Ar-O(2) plasma) magnetron sputtered WO(3)-MoO(3) (nanometer scaled) mixed layers were investigated and mapped by Spectroscopic Ellipsometry (SE). The W- and Mo-targets were placed separately, and 30 × 30 cm glass substrates were slowly moved under the two (W and Mo) separated targets. We used different (oscillator- and Effective Medium Approximation, EMA-based) optical models to obtain the thickness and composition maps of the sample layer relatively quickly and in a cost-effective and contactless way. In addition, we used Rutherford Backscattering Spectrometry to check the SE results. Herein, we compare the “goodness” of different optical models depending upon the sample preparation conditions, for instance, the speed and cycle number of the substrate motion. Finally, we can choose between appropriate optical models (2-Tauc-Lorentz oscillator model vs. the Bruggeman Effective Medium Approximation, BEMA) depending on the process parameters. If one has more than one “molecular layer” in the “sublayers”, BEMA can be used. If one has an atomic mixture, the multiple oscillator model is better (more precise) for this type of layer structure. |
format | Online Article Text |
id | pubmed-9317069 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2022 |
publisher | MDPI |
record_format | MEDLINE/PubMed |
spelling | pubmed-93170692022-07-27 Investigation of Combinatorial WO(3)-MoO(3) Mixed Layers by Spectroscopic Ellipsometry Using Different Optical Models Fried, Miklos Bogar, Renato Takacs, Daniel Labadi, Zoltan Horvath, Zsolt Endre Zolnai, Zsolt Nanomaterials (Basel) Article Reactive (Ar-O(2) plasma) magnetron sputtered WO(3)-MoO(3) (nanometer scaled) mixed layers were investigated and mapped by Spectroscopic Ellipsometry (SE). The W- and Mo-targets were placed separately, and 30 × 30 cm glass substrates were slowly moved under the two (W and Mo) separated targets. We used different (oscillator- and Effective Medium Approximation, EMA-based) optical models to obtain the thickness and composition maps of the sample layer relatively quickly and in a cost-effective and contactless way. In addition, we used Rutherford Backscattering Spectrometry to check the SE results. Herein, we compare the “goodness” of different optical models depending upon the sample preparation conditions, for instance, the speed and cycle number of the substrate motion. Finally, we can choose between appropriate optical models (2-Tauc-Lorentz oscillator model vs. the Bruggeman Effective Medium Approximation, BEMA) depending on the process parameters. If one has more than one “molecular layer” in the “sublayers”, BEMA can be used. If one has an atomic mixture, the multiple oscillator model is better (more precise) for this type of layer structure. MDPI 2022-07-14 /pmc/articles/PMC9317069/ /pubmed/35889645 http://dx.doi.org/10.3390/nano12142421 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 Fried, Miklos Bogar, Renato Takacs, Daniel Labadi, Zoltan Horvath, Zsolt Endre Zolnai, Zsolt Investigation of Combinatorial WO(3)-MoO(3) Mixed Layers by Spectroscopic Ellipsometry Using Different Optical Models |
title | Investigation of Combinatorial WO(3)-MoO(3) Mixed Layers by Spectroscopic Ellipsometry Using Different Optical Models |
title_full | Investigation of Combinatorial WO(3)-MoO(3) Mixed Layers by Spectroscopic Ellipsometry Using Different Optical Models |
title_fullStr | Investigation of Combinatorial WO(3)-MoO(3) Mixed Layers by Spectroscopic Ellipsometry Using Different Optical Models |
title_full_unstemmed | Investigation of Combinatorial WO(3)-MoO(3) Mixed Layers by Spectroscopic Ellipsometry Using Different Optical Models |
title_short | Investigation of Combinatorial WO(3)-MoO(3) Mixed Layers by Spectroscopic Ellipsometry Using Different Optical Models |
title_sort | investigation of combinatorial wo(3)-moo(3) mixed layers by spectroscopic ellipsometry using different optical models |
topic | Article |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9317069/ https://www.ncbi.nlm.nih.gov/pubmed/35889645 http://dx.doi.org/10.3390/nano12142421 |
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