Abstract
Perovskite solar cells are gaining popularity day by day due to the continuous effort of solar
scientists. However, there are several barriers to the commercialization of this solar cell. Various
materials can be used to achieve higher efficiency of perovskite solar cell design. Some of these
materials may also contain lead (Pb), which harms human life and the environment. Another
crucial hindrance for perovskite solar cells is the cost regarding hole transport material (HTM),
electron transport material (ETM), and back contact; most of the common HTM, ETM, and back
contact materials are expensive. In this study, we have chosen inexpensive HTM, ETM, and back
contact to determine highly efficient and less expensive cell structures. Eleven non-toxic and three
Pb-based absorber materials have been simulated using SCAPS-1D simulator where ETM (ZnO)
and HTM (PEDOT: PSS+WO3) are constant to determine the best absorber material. Later the
effect of thickness, temperature, back and front contact, electron affinity, defect density, and series
resistance are also considered. After simulation and optimization, it is found that Ni is the least
expensive back contact material for providing optimal efficiency, MAPbI3 is the best Pb-based
absorber material with open circuit voltage (Voc) =1.10V, short circuit current (Jsc) =28.47
mA/cm2, fill factor (FF) =86.42%, power conversion efficiency (eta(%)) =27.10%. In contrast, the
best non-toxic material is MASnI3 with Voc =0.97V, Jsc =34.89mA/cm2, FF =82.51% and eta (%)
=27.98%.