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Plasmonic and Conductive Structures of TCO Films with Embedded Cu Nanoparticles

Cu nanoparticles were produced by using solid-state dewetting (dry) of a 1.3 nm Cu layer or laser ablation of a Cu solid target (wet) in acetone and methanol. The morphology and chemical composition of the nanoparticles were investigated as a function of the synthesis methods and their key parameter...

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Autores principales: Boscarino, Stefano, Iacono, Valentina, Lo Mastro, Andrea, Tringali, Fiorella, Terrasi, Antonio, Grimaldi, Maria Grazia, Ruffino, Francesco
Formato: Online Artículo Texto
Lenguaje:English
Publicado: MDPI 2022
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9569451/
https://www.ncbi.nlm.nih.gov/pubmed/36233188
http://dx.doi.org/10.3390/ijms231911886
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author Boscarino, Stefano
Iacono, Valentina
Lo Mastro, Andrea
Tringali, Fiorella
Terrasi, Antonio
Grimaldi, Maria Grazia
Ruffino, Francesco
author_facet Boscarino, Stefano
Iacono, Valentina
Lo Mastro, Andrea
Tringali, Fiorella
Terrasi, Antonio
Grimaldi, Maria Grazia
Ruffino, Francesco
author_sort Boscarino, Stefano
collection PubMed
description Cu nanoparticles were produced by using solid-state dewetting (dry) of a 1.3 nm Cu layer or laser ablation of a Cu solid target (wet) in acetone and methanol. The morphology and chemical composition of the nanoparticles were investigated as a function of the synthesis methods and their key parameters of the annealing temperature (200–500 °C) and the liquid environment during the ablation. Cu nanoparticles were then embedded in transparent conductive oxide (TCO) films as aluminum-doped zinc oxide (AZO) or zirconium-doped indium oxide (IZrO); the TCO(bott)/Cu nanoparticle/TCO(top) structures were synthesized with all combinations of AZO and IZrO as the top and bottom layers. The goal was to achieve a plasmonic and conductive structure for photovoltaic applications via a comparison of the involved methods and all fabricated structures. In particular, solid-state dewetting produced faceted or spherical (depending on the annealing temperature) nanoparticles with an average size below 150 nm while laser ablation produced spherical nanoparticles below 250 nm. Dry and wet plasmonic conductive structures as a function of the TCOs employed and the temperature of annealing could reach a sheet resistance of 86 Ω/sq. The energy band-gap E(gap), absorbance, transmittance, and reflectance of the plasmonic conductive structures were investigated in the UV–vis–NIR range. They showed a dependence on the sequence of the top and bottom TCO, with best transmittances of 89.4% for the dry plasmonic conductive structure and 84.7% for the wet plasmonic conductive structure. The latter showed a higher diffused transmittance of between 10–20% in the visible range.
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spelling pubmed-95694512022-10-17 Plasmonic and Conductive Structures of TCO Films with Embedded Cu Nanoparticles Boscarino, Stefano Iacono, Valentina Lo Mastro, Andrea Tringali, Fiorella Terrasi, Antonio Grimaldi, Maria Grazia Ruffino, Francesco Int J Mol Sci Article Cu nanoparticles were produced by using solid-state dewetting (dry) of a 1.3 nm Cu layer or laser ablation of a Cu solid target (wet) in acetone and methanol. The morphology and chemical composition of the nanoparticles were investigated as a function of the synthesis methods and their key parameters of the annealing temperature (200–500 °C) and the liquid environment during the ablation. Cu nanoparticles were then embedded in transparent conductive oxide (TCO) films as aluminum-doped zinc oxide (AZO) or zirconium-doped indium oxide (IZrO); the TCO(bott)/Cu nanoparticle/TCO(top) structures were synthesized with all combinations of AZO and IZrO as the top and bottom layers. The goal was to achieve a plasmonic and conductive structure for photovoltaic applications via a comparison of the involved methods and all fabricated structures. In particular, solid-state dewetting produced faceted or spherical (depending on the annealing temperature) nanoparticles with an average size below 150 nm while laser ablation produced spherical nanoparticles below 250 nm. Dry and wet plasmonic conductive structures as a function of the TCOs employed and the temperature of annealing could reach a sheet resistance of 86 Ω/sq. The energy band-gap E(gap), absorbance, transmittance, and reflectance of the plasmonic conductive structures were investigated in the UV–vis–NIR range. They showed a dependence on the sequence of the top and bottom TCO, with best transmittances of 89.4% for the dry plasmonic conductive structure and 84.7% for the wet plasmonic conductive structure. The latter showed a higher diffused transmittance of between 10–20% in the visible range. MDPI 2022-10-06 /pmc/articles/PMC9569451/ /pubmed/36233188 http://dx.doi.org/10.3390/ijms231911886 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
Boscarino, Stefano
Iacono, Valentina
Lo Mastro, Andrea
Tringali, Fiorella
Terrasi, Antonio
Grimaldi, Maria Grazia
Ruffino, Francesco
Plasmonic and Conductive Structures of TCO Films with Embedded Cu Nanoparticles
title Plasmonic and Conductive Structures of TCO Films with Embedded Cu Nanoparticles
title_full Plasmonic and Conductive Structures of TCO Films with Embedded Cu Nanoparticles
title_fullStr Plasmonic and Conductive Structures of TCO Films with Embedded Cu Nanoparticles
title_full_unstemmed Plasmonic and Conductive Structures of TCO Films with Embedded Cu Nanoparticles
title_short Plasmonic and Conductive Structures of TCO Films with Embedded Cu Nanoparticles
title_sort plasmonic and conductive structures of tco films with embedded cu nanoparticles
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9569451/
https://www.ncbi.nlm.nih.gov/pubmed/36233188
http://dx.doi.org/10.3390/ijms231911886
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