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NiN-Passivated NiO Hole-Transport Layer Improves Halide Perovskite-Based Solar Cell
[Image: see text] The interfaces between inorganic selective contacts and halide perovskites (HaPs) are possibly the greatest challenge for making stable and reproducible solar cells with these materials. NiO(x), an attractive hole-transport layer as it fits the electronic structure of HaPs, is high...
Autores principales: | , , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
American Chemical Society
2022
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Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9614719/ https://www.ncbi.nlm.nih.gov/pubmed/36226899 http://dx.doi.org/10.1021/acsami.2c11701 |
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author | Itzhak, Anat He, Xu Kama, Adi Kumar, Sujit Ejgenberg, Michal Kahn, Antoine Cahen, David |
author_facet | Itzhak, Anat He, Xu Kama, Adi Kumar, Sujit Ejgenberg, Michal Kahn, Antoine Cahen, David |
author_sort | Itzhak, Anat |
collection | PubMed |
description | [Image: see text] The interfaces between inorganic selective contacts and halide perovskites (HaPs) are possibly the greatest challenge for making stable and reproducible solar cells with these materials. NiO(x), an attractive hole-transport layer as it fits the electronic structure of HaPs, is highly stable and can be produced at a low cost. Furthermore, NiO(x) can be fabricated via scalable and controlled physical deposition methods such as RF sputtering to facilitate the quest for scalable, solvent-free, vacuum-deposited HaP-based solar cells (PSCs). However, the interface between NiO(x) and HaPs is still not well-controlled, which leads at times to a lack of stability and V(oc) losses. Here, we use RF sputtering to fabricate NiO(x) and then cover it with a Ni(y)N layer without breaking vacuum. The Ni(y)N layer protects NiO(x) doubly during PSC production. Firstly, the Ni(y)N layer protects NiO(x) from Ni(3+) species being reduced to Ni(2+) by Ar plasma, thus maintaining NiO(x) conductivity. Secondly, it passivates the interface between NiO(x) and the HaPs, retaining PSC stability over time. This double effect improves PSC efficiency from an average of 16.5% with a 17.4% record cell to a 19% average with a 19.8% record cell and increases the device stability. |
format | Online Article Text |
id | pubmed-9614719 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2022 |
publisher | American Chemical Society |
record_format | MEDLINE/PubMed |
spelling | pubmed-96147192022-10-29 NiN-Passivated NiO Hole-Transport Layer Improves Halide Perovskite-Based Solar Cell Itzhak, Anat He, Xu Kama, Adi Kumar, Sujit Ejgenberg, Michal Kahn, Antoine Cahen, David ACS Appl Mater Interfaces [Image: see text] The interfaces between inorganic selective contacts and halide perovskites (HaPs) are possibly the greatest challenge for making stable and reproducible solar cells with these materials. NiO(x), an attractive hole-transport layer as it fits the electronic structure of HaPs, is highly stable and can be produced at a low cost. Furthermore, NiO(x) can be fabricated via scalable and controlled physical deposition methods such as RF sputtering to facilitate the quest for scalable, solvent-free, vacuum-deposited HaP-based solar cells (PSCs). However, the interface between NiO(x) and HaPs is still not well-controlled, which leads at times to a lack of stability and V(oc) losses. Here, we use RF sputtering to fabricate NiO(x) and then cover it with a Ni(y)N layer without breaking vacuum. The Ni(y)N layer protects NiO(x) doubly during PSC production. Firstly, the Ni(y)N layer protects NiO(x) from Ni(3+) species being reduced to Ni(2+) by Ar plasma, thus maintaining NiO(x) conductivity. Secondly, it passivates the interface between NiO(x) and the HaPs, retaining PSC stability over time. This double effect improves PSC efficiency from an average of 16.5% with a 17.4% record cell to a 19% average with a 19.8% record cell and increases the device stability. American Chemical Society 2022-10-13 2022-10-26 /pmc/articles/PMC9614719/ /pubmed/36226899 http://dx.doi.org/10.1021/acsami.2c11701 Text en © 2022 The Authors. Published by American Chemical Society https://creativecommons.org/licenses/by/4.0/Permits the broadest form of re-use including for commercial purposes, provided that author attribution and integrity are maintained (https://creativecommons.org/licenses/by/4.0/). |
spellingShingle | Itzhak, Anat He, Xu Kama, Adi Kumar, Sujit Ejgenberg, Michal Kahn, Antoine Cahen, David NiN-Passivated NiO Hole-Transport Layer Improves Halide Perovskite-Based Solar Cell |
title | NiN-Passivated NiO
Hole-Transport Layer Improves Halide
Perovskite-Based Solar Cell |
title_full | NiN-Passivated NiO
Hole-Transport Layer Improves Halide
Perovskite-Based Solar Cell |
title_fullStr | NiN-Passivated NiO
Hole-Transport Layer Improves Halide
Perovskite-Based Solar Cell |
title_full_unstemmed | NiN-Passivated NiO
Hole-Transport Layer Improves Halide
Perovskite-Based Solar Cell |
title_short | NiN-Passivated NiO
Hole-Transport Layer Improves Halide
Perovskite-Based Solar Cell |
title_sort | nin-passivated nio
hole-transport layer improves halide
perovskite-based solar cell |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9614719/ https://www.ncbi.nlm.nih.gov/pubmed/36226899 http://dx.doi.org/10.1021/acsami.2c11701 |
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