“…As a result, perovskites have surpassed other third-generation photovoltaic technologies. [28][29][30] Perovskite materials are represented by the generalized formula ABX 3 : the cubo-octahedral A site is occupied by an organic or inorganic cation such as methylammonium + (MA + ), formamidinium + (FA + ), Cs + , and Rb + ; the octahedral B site is occupied by a divalent cation such as Pb 2 + , Sn 2 + , and Ge 2 + ; and the octahedral X sites are filled by halogens such as Cl À , Br À , and I À (Figure 1c). [10,31] This class of materials exhibits remarkable optoelectronic properties, including tunable bandgaps aided via compositional engineering, high absorption coefficients, low exciton binding energies, high charge-carrier mobilities, and long carrier diffusion lengths, affording their suitability as excellent photo-absorbers for artificial light harvesting.…”