Charge carrier dynamics controlling performance of lead-based halide perovskite solar cells

Abstract We review our studies to assess charge carrier dynamics inside a perovskite film and interfacial charge transfer dynamics for a perovskite layer sandwiched by an electron transporting layer (ETL) such as TiO 2 compact or mesoporous layer and a hole transporting layer (HTL) such as spiro-OMeTAD. Both electron and hole injection occur faster than electron-hole recombination inside a perovskite film, however, both change injection yields decrease with an increase in excitation intensity. Since the electron mobility inside methylammonium lead iodide (MAPbI 3 ) perovskite is lower than the hole mobility, employing a mesoporous ETL structure is suitable to maximise the electron injection yield. Interfacial charge recombination lifetime increases with an increase in perovskite film thickness. We therefore conclude that for p-type MAPbI 3 solar cells, the perovskite film thickness should be increased to the hole diffusion length, while the mesoporous ETL structure should be employed to maximise the electron injection yield.

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Publication Details

Journal
Japanese Journal of Applied Physics
Published
2025-04-21
DOI
https://doi.org/10.35848/1347-4065/adcef3
Primary Topic
Perovskite Materials and Applications
Type
article
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article

Charge carrier dynamics controlling performance of lead-based halide perovskite solar cells

Maning Liu, Yasuhiro Tachibana, Chathurika Maduwanthi
Japanese Journal of Applied Physics
Perovskite Materials and Applications
article

Charge carrier dynamics controlling performance of lead-based halide perovskite solar cells

Maning Liu, Yasuhiro Tachibana, Chathurika Maduwanthi
article en

Abstract

Abstract We review our studies to assess charge carrier dynamics inside a perovskite film and interfacial charge transfer dynamics for a perovskite layer sandwiched by an electron transporting layer (ETL) such as TiO 2 compact or mesoporous layer and a hole transporting layer (HTL) such as spiro-OMeTAD. Both electron and hole injection occur faster than electron-hole recombination inside a perovskite film, however, both change injection yields decrease with an increase in excitation intensity. Since the electron mobility inside methylammonium lead iodide (MAPbI 3 ) perovskite is lower than the hole mobility, employing a mesoporous ETL structure is suitable to maximise the electron injection yield. Interfacial charge recombination lifetime increases with an increase in perovskite film thickness. We therefore conclude that for p-type MAPbI 3 solar cells, the perovskite film thickness should be increased to the hole diffusion length, while the mesoporous ETL structure should be employed to maximise the electron injection yield.

Japanese Journal of Applied PhysicsVol. 64(5)
Lund University (SE), Toneyama National Hospital (JP), RMIT University (AU)
Openalex Percentile: Top 94%
Perovskite Materials and Applications
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