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Inorganic Lead-Free B-γ-CsSnI(3) Perovskite Solar Cells Using Diverse Electron-Transporting Materials: A Simulation Study

[Image: see text] B-γ-CsSnI(3) perovskite solar cells (PSCs) are simulated employing diverse electron-transporting layers (ETLs, including TiO(2), ZnO, SnO(2), GaN, C(60), and PCBM), and a comparative study has been made. Both regular and inverted planar structures are simulated. Effects of the thic...

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Detalles Bibliográficos
Autores principales: Lin, Shuo, Zhang, Baoping, Lü, Tie-Yu, Zheng, Jin-Cheng, Pan, Huaqing, Chen, Huanting, Lin, Chuanjin, Li, Xirong, Zhou, Jinrong
Formato: Online Artículo Texto
Lenguaje:English
Publicado: American Chemical Society 2021
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8515834/
https://www.ncbi.nlm.nih.gov/pubmed/34661022
http://dx.doi.org/10.1021/acsomega.1c04096
Descripción
Sumario:[Image: see text] B-γ-CsSnI(3) perovskite solar cells (PSCs) are simulated employing diverse electron-transporting layers (ETLs, including TiO(2), ZnO, SnO(2), GaN, C(60), and PCBM), and a comparative study has been made. Both regular and inverted planar structures are simulated. Effects of the thickness of absorbers and ETLs, doping of ETLs, and interface trap states on the photovoltaic performance are studied to optimize the device structures. The regular structures have larger short-circuit current density (J(sc)) than the inverted structures, but the inverted structures have larger fill factor (FF). All of the simulated optimal PSCs have similar open-circuit voltages (V(oc)) of ∼0.96 V. The PSCs with TiO(2) ETLs have the best photovoltaic performance, and the optimum structure exhibits the highest efficiency of 20.2% with a V(oc) of 0.97 V, J(sc) of 29.67 mA/cm(2), and FF of 0.70. The optimal PSCs with ZnO, GaN, C(60), and PCBM ETLs exhibit efficiencies of 17.88, 18.09, 16.71, and 16.59%, respectively. The optimal PSC with SnO(2) ETL exhibits the lowest efficiency of 15.5% in all of the simulated PSCs due to its cliff-like band offset at the SnO(2)/CsSnI(3) interface. Furthermore, the increase of interface trap density and capture cross section is found to reduce the photovoltaic performance of PSCs. This work contributes to designing and fabricating CsSnI(3) PSCs.