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Optimizing Geometry and ETL Materials for High-Performance Inverted Perovskite Solar Cells by TCAD Simulation

Irodakhon GulomovaRenewable Energy Sources Laboratory, Andijan State University, Andijan 170100, UzbekistanOussama AccoucheCollege of Engineering and Technology, American University of the Middle East, Egaila 54200, KuwaitRayimjon AlievRenewable Energy Sources Laboratory, Andijan State University, Andijan 170100, UzbekistanZaher Al BarakehCollege of Engineering and Technology, American University of the Middle East, Egaila 54200, KuwaitValikhon AbduazimovRenewable Energy Sources Laboratory, Andijan State University, Andijan 170100, Uzbekistan
Nanomaterialsjournal2024en
ABI

Annotatsiya

Due to the optical properties of the electron transport layer (ETL) and hole transport layer (HTL), inverted perovskite solar cells can perform better than traditional perovskite solar cells. It is essential to compare both types to understand their efficiencies. In this article, we studied inverted perovskite solar cells with NiOx/CH3NH3Pb3/ETL (ETL = MoO3, TiO2, ZnO) structures. Our results showed that the optimal thickness of NiOx is 80 nm for all structures. The optimal perovskite thickness is 600 nm for solar cells with ZnO and MoO3, and 800 nm for those with TiO2. For the ETLs, the best thicknesses are 100 nm for ZnO, 80 nm for MoO3, and 60 nm for TiO2. We found that the efficiencies of inverted perovskite solar cells with ZnO, MoO3, and TiO2 as ETLs, and with optimal layer thicknesses, are 30.16%, 18.69%, and 35.21%, respectively. These efficiencies are 1.5%, 5.7%, and 1.5% higher than those of traditional perovskite solar cells. Our study highlights the potential of optimizing layer thicknesses in inverted perovskite solar cells to achieve higher efficiencies than traditional structures.

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