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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...

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Autores principales: Itzhak, Anat, He, Xu, Kama, Adi, Kumar, Sujit, Ejgenberg, Michal, Kahn, Antoine, Cahen, David
Formato: Online Artículo Texto
Lenguaje:English
Publicado: American Chemical Society 2022
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.
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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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