A lead-free, completely inorganic, and nontoxic Cs 2 TiBr 6 -based double perovskite solar cell (PSC) was simulated via SCAPS 1-D. La-doped BaSnO 3 (LBSO) was applied as the electron transport layer (ETL) unprecedentedly in the simulation study of PSCs, while CuSbS 2 was utilized as the hole transport layer (HTL). wxAMPS was used to validate the results of SCAPS simulations. Moreover, the first-principle density function theory (DFT) calculations were performed for validating the 1.6 eV bandgap of the Cs 2 TiBr 6 absorber. To enhance the device performance, we analyzed and optimized various parameters of the PSC using SCAPS. The optimum thickness, defect density, and bandgap of the absorber were 1000 nm, 10 13 cm À3 , and 1.4 eV, respectively. Furthermore, the optimum thickness, hole mobility, and electron affinity of the HTL were 400 nm, 10 2 cm 2 V À1 s À1 , and 4.1 eV, respectively. However, the ETL thickness had a negligible effect on the device's efficiency. The optimized values of doping density for the absorber layer, HTL, and ETL were 10 15 , 10 20 , and 10 21 cm À3 , respectively. Herein, the effect of different HTLs was analyzed by matching up the built-in voltage (V bi ) in respect of the open-circuit voltage (V OC ). It was found that the V bi was directly proportional to the V OC , and CuSbS 2 was the champion in terms of efficiency for the PSC. The optimum work function of metal contact and temperature of the PSC were 5.9 eV and 300 K, respectively. After the final optimization, the device achieved an exhilarating PCE of 29.13%.
Novelty Statement• LBSO was used as the ETL for the very first time in the simulation study of PSCs, while CuSbS 2 was utilized as the HTL.