Ĭhatterjee S, Pal AJ (2018) Tin (IV) substitution in (CH 3NH 3) 3Sb 2I 9: toward low-band-gap defect-ordered hybrid perovskite solar cells. Ĭhakraborty K, Choudhury MG, Paul S (2021) Study of physical, optical, and electrical properties of cesium titanium (IV)-based single halide perovskite solar cell. Ĭameron J, Skabara PJ (2020) The damaging effects of the acidity in PEDOT:PSS on semiconductor device performance and solutions based on non-acidic alternatives. īoopathi KM et al (2017) Solution-processable antimony-based light absorbing materials beyond lead halide perovskites. īishnoi S, Pandey SK (2018) Device performance analysis for lead-free perovskite solar cell optimisation. īernal LC et al (2019) Impedance analysis of perovskite solar cells: a case study. īeedri NI, Inamuddin N et al (2018b) Bilayered ZnO/Nb 2O 5 photoanode for dye sensitized solar cell. īeedri NI, Inamuddin NS et al (2018a) N3-sensitized TiO 2/Nb 2O 5: a novel bilayer structure for dye-sensitized solar-cell application. Īlanne K, Saari A (2006) Distributed energy generation and sustainable development. Īhmed MI, Habib A, Javaid SS (2015) Perovskite solar cells: potentials, challenges, and opportunities. This study also suggests a low-cost perovskite solar cell, which is free from carcinogenic agents that can be used for solar energy harvesting in a larger scale.Īfzaal M, Yates HM, Walter A, Nicolay S (2019) Improved FTO/NiO x interfaces for inverted planar triple-cation perovskite solar cells. Also, the optical and electrical properties of the device such as absorption coefficient, indirect and direct bandgap transition, capacitance–voltage and conductance–voltage characteristics have been obtained and analysed with the help of Tauc and Bode plots. The device has been successfully compared with the previous works to showcase its performance enhancement. The final optimized solar cell has reached a Fill factor (FF) of 85.44%, a short-circuit current density ( J sc) of 31.12 mA/cm 2, a power conversion efficiency (PCE) of 32.36%, and an open-circuit voltage ( V oc) of 1.22 V. The optimal thickness of the perovskite layer has been found to be 400 nm that leads to a performance improvement of ~ 8%. The designed solar cell has been optimized by varying parameters such as active layer thickness, absorber defect density and work function of the bottom electrode. The design and performance of inorganic tin-based perovskite known as cesium tin iodide (CsSnI 3), which serves to be an alternative for conventional toxic lead-based solar cells have been reported.
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