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Room-Temperature-Processed Amorphous Sn-In-O Electron Transport Layer for Perovskite Solar Cells

We report amorphous tin-indium-oxide (TIO, Sn fraction: >50 atomic percentage (at%)) thin films as a new electron transport layer (ETL) of perovskite solar cells (PSCs). TIO thin films with Sn fraction of 52, 77, 83, 92, and 100 at% were grown on crystalline indium-tin-oxide (ITO, Sn fraction: ~1...

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Autores principales: Baek, Seungtae, Han, Jeong Woo, Vidyasagar, Devthade, Cho, Hanbyeol, HA, Hwi-Heon, Kim, Dong Hoe, Heo, Young-Woo, Lee, Sangwook
Formato: Online Artículo Texto
Lenguaje:English
Publicado: MDPI 2019
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6981739/
https://www.ncbi.nlm.nih.gov/pubmed/31861710
http://dx.doi.org/10.3390/ma13010032
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author Baek, Seungtae
Han, Jeong Woo
Vidyasagar, Devthade
Cho, Hanbyeol
HA, Hwi-Heon
Kim, Dong Hoe
Heo, Young-Woo
Lee, Sangwook
author_facet Baek, Seungtae
Han, Jeong Woo
Vidyasagar, Devthade
Cho, Hanbyeol
HA, Hwi-Heon
Kim, Dong Hoe
Heo, Young-Woo
Lee, Sangwook
author_sort Baek, Seungtae
collection PubMed
description We report amorphous tin-indium-oxide (TIO, Sn fraction: >50 atomic percentage (at%)) thin films as a new electron transport layer (ETL) of perovskite solar cells (PSCs). TIO thin films with Sn fraction of 52, 77, 83, 92, and 100 at% were grown on crystalline indium-tin-oxide (ITO, Sn fraction: ~10 at%) thin films, a common transparent conducting oxide, by co-sputtering In(2)O(3) and SnO(2) at room temperature. The energy band structures of the amorphous TIO thin films were determined from the optical absorbance and the ultraviolet photoelectron spectra. All the examined compositions are characterized by a conduction band edge lying between that of ITO and that of perovskite (here, methylammonium lead triiodide), indicating that TIO is a potentially viable ETL of PSCs. The photovoltaic characteristics of the TIO-based PSCs were evaluated. Owing mainly to the highest fill factor and open circuit voltage, the optimal power conversion efficiency was obtained for the 77 at%-Sn TIO ETL with TiCl(4) treatment. The fill factor and the open circuit voltage changes with varying the Sn fraction, despite similar conduction band edges. We attribute these differences to the considerable changes in the electrical resistivity of the TIO ETL. This would have a significant effect on the shunt and/or the series resistances. The TIO ETL can be continuously grown on an ITO TCO in a chamber, as ITO and TIO are composed of identical elements, which would help to reduce production time and costs.
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spelling pubmed-69817392020-02-07 Room-Temperature-Processed Amorphous Sn-In-O Electron Transport Layer for Perovskite Solar Cells Baek, Seungtae Han, Jeong Woo Vidyasagar, Devthade Cho, Hanbyeol HA, Hwi-Heon Kim, Dong Hoe Heo, Young-Woo Lee, Sangwook Materials (Basel) Article We report amorphous tin-indium-oxide (TIO, Sn fraction: >50 atomic percentage (at%)) thin films as a new electron transport layer (ETL) of perovskite solar cells (PSCs). TIO thin films with Sn fraction of 52, 77, 83, 92, and 100 at% were grown on crystalline indium-tin-oxide (ITO, Sn fraction: ~10 at%) thin films, a common transparent conducting oxide, by co-sputtering In(2)O(3) and SnO(2) at room temperature. The energy band structures of the amorphous TIO thin films were determined from the optical absorbance and the ultraviolet photoelectron spectra. All the examined compositions are characterized by a conduction band edge lying between that of ITO and that of perovskite (here, methylammonium lead triiodide), indicating that TIO is a potentially viable ETL of PSCs. The photovoltaic characteristics of the TIO-based PSCs were evaluated. Owing mainly to the highest fill factor and open circuit voltage, the optimal power conversion efficiency was obtained for the 77 at%-Sn TIO ETL with TiCl(4) treatment. The fill factor and the open circuit voltage changes with varying the Sn fraction, despite similar conduction band edges. We attribute these differences to the considerable changes in the electrical resistivity of the TIO ETL. This would have a significant effect on the shunt and/or the series resistances. The TIO ETL can be continuously grown on an ITO TCO in a chamber, as ITO and TIO are composed of identical elements, which would help to reduce production time and costs. MDPI 2019-12-19 /pmc/articles/PMC6981739/ /pubmed/31861710 http://dx.doi.org/10.3390/ma13010032 Text en © 2019 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
Baek, Seungtae
Han, Jeong Woo
Vidyasagar, Devthade
Cho, Hanbyeol
HA, Hwi-Heon
Kim, Dong Hoe
Heo, Young-Woo
Lee, Sangwook
Room-Temperature-Processed Amorphous Sn-In-O Electron Transport Layer for Perovskite Solar Cells
title Room-Temperature-Processed Amorphous Sn-In-O Electron Transport Layer for Perovskite Solar Cells
title_full Room-Temperature-Processed Amorphous Sn-In-O Electron Transport Layer for Perovskite Solar Cells
title_fullStr Room-Temperature-Processed Amorphous Sn-In-O Electron Transport Layer for Perovskite Solar Cells
title_full_unstemmed Room-Temperature-Processed Amorphous Sn-In-O Electron Transport Layer for Perovskite Solar Cells
title_short Room-Temperature-Processed Amorphous Sn-In-O Electron Transport Layer for Perovskite Solar Cells
title_sort room-temperature-processed amorphous sn-in-o electron transport layer for perovskite solar cells
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6981739/
https://www.ncbi.nlm.nih.gov/pubmed/31861710
http://dx.doi.org/10.3390/ma13010032
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