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Effect of Various Electron and Hole Transport Layers on the Performance of CsPbI(3)-Based Perovskite Solar Cells: A Numerical Investigation in DFT, SCAPS-1D, and wxAMPS Frameworks
[Image: see text] CsPbI(3) has recently received tremendous attention as a possible absorber of perovskite solar cells (PSCs). However, CsPbI(3)-based PSCs have yet to achieve the high performance of the hybrid PSCs. In this work, we performed a density functional theory (DFT) study using the Cambri...
Autores principales: | , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
American Chemical Society
2022
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Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9713884/ https://www.ncbi.nlm.nih.gov/pubmed/36467947 http://dx.doi.org/10.1021/acsomega.2c05912 |
Sumario: | [Image: see text] CsPbI(3) has recently received tremendous attention as a possible absorber of perovskite solar cells (PSCs). However, CsPbI(3)-based PSCs have yet to achieve the high performance of the hybrid PSCs. In this work, we performed a density functional theory (DFT) study using the Cambridge Serial Total Energy Package (CASTEP) code for the cubic CsPbI(3) absorber to compare and evaluate its structural, electronic, and optical properties. The calculated electronic band gap (E(g)) using the GGA-PBE approach of CASTEP was 1.483 eV for this CsPbI(3) absorber. Moreover, the computed density of states (DOS) exhibited the dominant contribution from the Pb-5d orbital, and most charges also accumulated for the Pb atom as seen from the electronic charge density map. Fermi surface calculation showed multiband character, and optical properties were computed to investigate the optical response of CsPbI(3). Furthermore, we used IGZO, SnO(2), WS(2), CeO(2), PCBM, TiO(2), ZnO, and C(60) as the electron transport layers (ETLs) and Cu(2)O, CuSCN, CuSbS(2), Spiro-MeOTAD, V(2)O(5), CBTS, CFTS, P3HT, PEDOT:PSS, NiO, CuO, and CuI as the hole transport layers (HTLs) to identify the best HTL/CsPbI(3)/ETL combinations using the SCAPS-1D solar cell simulation software. Among 96 device structures, the best-optimized device structure, ITO/TiO(2)/CsPbI(3)/CBTS/Au, was identified, which exhibited an efficiency of 17.9%. The effect of the absorber and ETL thickness, series resistance, shunt resistance, and operating temperature was also evaluated for the six best devices along with their corresponding generation rate, recombination rate, capacitance–voltage, current density–voltage, and quantum efficiency characteristics. The obtained results from SCAPS-1D were also compared with wxAMPS simulation results. |
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