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Vapor-Deposited n = 2 Ruddlesden–Popper Interface Layers Aid Charge Carrier Extraction in Perovskite Solar Cells AITranslate

Georgia Institute of Technology; Georgia Institute of Technology; Lawrence Berkeley National Laboratory; Georgia Institute of Technology; Georgia Institute of Technology; Georgia Institute of Technology; Brookhaven National Laboratory; University of Washington; University of Washington; University of Washington; Lawrence Berkeley National Laboratory; University of Washington; Georgia Institute of Technology
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Publisher: ACS
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Abstract AITranslate

Interfacial passivation with bulky organic cations such as phenetylammonium iodide has enabled high performance for metal halide perovskite optoelectronic devices. However, the homogeneity of these interfaces and their formation dynamics are poorly understood. We study how Ruddlesden–Popper 2D phases form at a 3D perovskite interface when the 2D precursors are introduced via solution or via vapor. When using vapor deposition, we observe uniform coverage of the capping layer and the formation of a predominantly n = 2 Ruddlesden–Popper phase. In contrast, when using solution deposition, we observe the presence of a mixture of n = 2 and n = 1 in the film and the formation of aggregates of the organic cations. As a result of the better phase purity and uniformity, vapor deposition enables higher median solar cell performance with narrower distribution compared to solution-treated films. This study provides fundamental information that the perovskite community can use to better design capping layers to achieve higher charge extraction efficiencies.

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DOI:https://doi.org/10.1021/acsenergylett.2c02419

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Citation Information:

Interfacial passivation with bulky organic cations such as phenetylammonium iodide has enabled high performance for metal halide perovskite optoelectronic devices. However, the homogeneity of these interfaces and their formation dynamics are poorly understood. We study how Ruddlesden–Popper 2D phases form at a 3D perovskite interface when the 2D precursors are introduced via solution or via vapor. When using vapor deposition, we observe uniform coverage of the capping layer and the formation of a predominantly n = 2 Ruddlesden–Popper phase. In contrast, when using solution deposition, we observe the presence of a mixture of n = 2 and n = 1 in the film and the formation of aggregates of the organic cations. As a result of the better phase purity and uniformity, vapor deposition enables higher median solar cell performance with narrower distribution compared to solution-treated films. This study provides fundamental information that the perovskite community can use to better design capping layers to achieve higher charge extraction efficiencies.

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GB/T 7714-2015 [1] Carlo A. R. Perini, AndresFelipe CastroMendez, Tim Kodalle, et al. ACS Energy Letters, 2023(8). DOI:10.1021/acsenergylett.2c02419.
MLA [1] Carlo A. R. Perini, et al., ACS Energy Letters, no. 8, 2023, https://doi.org/10.1021/acsenergylett.2c02419.
APA [1] Carlo A. R. Perini, AndresFelipe CastroMendez, Tim Kodalle, Magdalena Ravello, Juanita Hidalgo, Martin GomezDominguez, Ruipeng Li, Margherita Taddei, Rajiv Giridharagopal, Justin Pothoof, Carolin M. SutterFella, David S. Ginger, & JuanPablo CorreaBaena. (2023). ACS Energy Letters(8). https://doi.org/10.1021/acsenergylett.2c02419
IEEE [1] Carlo A. R. Perini, AndresFelipe CastroMendez, Tim Kodalle, Magdalena Ravello, Juanita Hidalgo, Martin GomezDominguez, Ruipeng Li, Margherita Taddei, Rajiv Giridharagopal, Justin Pothoof, Carolin M. SutterFella, David S. Ginger, and JuanPablo CorreaBaena, ACS Energy Letters, no. 8, 2023, doi: 10.1021/acsenergylett.2c02419.