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Optical Characterization of As(x)Te(100−x) Films Grown by Plasma Deposition Based on the Advanced Optimizing Envelope Method

Three As(x)Te(100)(−)(x) films with different x and dissimilar average thickness [Formula: see text] are characterized mainly from one interference transmittance spectrum T(λ = 300 to 3000 nm) of such film on a substrate based on the advanced optimizing envelope method (AOEM). A simple dual transfor...

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Autores principales: Minkov, Dorian, Angelov, George, Nestorov, Radi, Nezhdanov, Aleksey, Usanov, Dmitry, Kudryashov, Mikhail, Mashin, Aleksandr
Formato: Online Artículo Texto
Lenguaje:English
Publicado: MDPI 2020
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7372394/
https://www.ncbi.nlm.nih.gov/pubmed/32635359
http://dx.doi.org/10.3390/ma13132981
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author Minkov, Dorian
Angelov, George
Nestorov, Radi
Nezhdanov, Aleksey
Usanov, Dmitry
Kudryashov, Mikhail
Mashin, Aleksandr
author_facet Minkov, Dorian
Angelov, George
Nestorov, Radi
Nezhdanov, Aleksey
Usanov, Dmitry
Kudryashov, Mikhail
Mashin, Aleksandr
author_sort Minkov, Dorian
collection PubMed
description Three As(x)Te(100)(−)(x) films with different x and dissimilar average thickness [Formula: see text] are characterized mainly from one interference transmittance spectrum T(λ = 300 to 3000 nm) of such film on a substrate based on the advanced optimizing envelope method (AOEM). A simple dual transformation of T(λ) is proposed and used for increasing the accuracy of computation of its envelopes T(+)(λ) and T(−)(λ) accounting for the significant glass substrate absorption especially for λ > 2500 nm. The refractive index n(λ) of As(40)Te(60) and As(98)Te(2) films is determined with a relative error <0.30%. As far as we know, the As(80)Te(20) film is the only one with anomalous dispersion and the thickest, with estimated [Formula: see text] = 1.1446 nm, ever characterized by an envelope method. It is also shown and explained why the extinction coefficient k(λ) of any of the three As(x)Te(100)(−)(x) films is computed more accurately from the quantity T(i)(λ) = [T(+)(λ)T(−)(λ)](0.5) compared to its commonly employed computation from T(+)(λ). The obtained results strengthen our conviction that the AOEM has a capacity for providing most accurate optical characterization of almost every dielectric or semiconductor film with [Formula: see text] > 300 nm on a substrate, compared to all the other methods for characterization of such films only from T(λ).
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spelling pubmed-73723942020-08-05 Optical Characterization of As(x)Te(100−x) Films Grown by Plasma Deposition Based on the Advanced Optimizing Envelope Method Minkov, Dorian Angelov, George Nestorov, Radi Nezhdanov, Aleksey Usanov, Dmitry Kudryashov, Mikhail Mashin, Aleksandr Materials (Basel) Article Three As(x)Te(100)(−)(x) films with different x and dissimilar average thickness [Formula: see text] are characterized mainly from one interference transmittance spectrum T(λ = 300 to 3000 nm) of such film on a substrate based on the advanced optimizing envelope method (AOEM). A simple dual transformation of T(λ) is proposed and used for increasing the accuracy of computation of its envelopes T(+)(λ) and T(−)(λ) accounting for the significant glass substrate absorption especially for λ > 2500 nm. The refractive index n(λ) of As(40)Te(60) and As(98)Te(2) films is determined with a relative error <0.30%. As far as we know, the As(80)Te(20) film is the only one with anomalous dispersion and the thickest, with estimated [Formula: see text] = 1.1446 nm, ever characterized by an envelope method. It is also shown and explained why the extinction coefficient k(λ) of any of the three As(x)Te(100)(−)(x) films is computed more accurately from the quantity T(i)(λ) = [T(+)(λ)T(−)(λ)](0.5) compared to its commonly employed computation from T(+)(λ). The obtained results strengthen our conviction that the AOEM has a capacity for providing most accurate optical characterization of almost every dielectric or semiconductor film with [Formula: see text] > 300 nm on a substrate, compared to all the other methods for characterization of such films only from T(λ). MDPI 2020-07-03 /pmc/articles/PMC7372394/ /pubmed/32635359 http://dx.doi.org/10.3390/ma13132981 Text en © 2020 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 (http://creativecommons.org/licenses/by/4.0/).
spellingShingle Article
Minkov, Dorian
Angelov, George
Nestorov, Radi
Nezhdanov, Aleksey
Usanov, Dmitry
Kudryashov, Mikhail
Mashin, Aleksandr
Optical Characterization of As(x)Te(100−x) Films Grown by Plasma Deposition Based on the Advanced Optimizing Envelope Method
title Optical Characterization of As(x)Te(100−x) Films Grown by Plasma Deposition Based on the Advanced Optimizing Envelope Method
title_full Optical Characterization of As(x)Te(100−x) Films Grown by Plasma Deposition Based on the Advanced Optimizing Envelope Method
title_fullStr Optical Characterization of As(x)Te(100−x) Films Grown by Plasma Deposition Based on the Advanced Optimizing Envelope Method
title_full_unstemmed Optical Characterization of As(x)Te(100−x) Films Grown by Plasma Deposition Based on the Advanced Optimizing Envelope Method
title_short Optical Characterization of As(x)Te(100−x) Films Grown by Plasma Deposition Based on the Advanced Optimizing Envelope Method
title_sort optical characterization of as(x)te(100−x) films grown by plasma deposition based on the advanced optimizing envelope method
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7372394/
https://www.ncbi.nlm.nih.gov/pubmed/32635359
http://dx.doi.org/10.3390/ma13132981
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