Metal halide perovskites (henceforth referred to as just "perovskites" for brevity), since their first appearance as an absorber layer in solar cells in 2009, [1] have led to an explosion of academic [2] and industrial [3] interest. The power conversion efficiency (PCE) of lab-scale perovskite solar cells has surpassed that of polycrystalline silicon and is now comparable with monocrystalline silicon. [4,5] For these reasons, perovskite solar cells are hoped to play a decisive role in improving the commercial attractiveness of utility-scale solar energy production and, ultimately, in mitigating the worst effects of climate change.Perovskite is the designated name for materials isostructural to ABX 3 where A and B are cations, and X is an anion, which is commonly a halide in the perovskite solar cell community. Research into perovskites started with compounds based on a single cation such as MAPbI 3 or FAPbI 3 , [1,6,7] where MA is methylammonium and FA is formamidinium. Nowadays, compounds formed from mixed X-site halides and mixed A-site cations are known to generally yield greater PCE [8,9] and stability [10,11] than single-cation, single-halide systems. While extensive efforts are devoted to find the optimal composition by tuning A-site and X-site constituents, [2,12] lead (Pb) is now believed to be essential for the defecttolerant nature of perovskites with a bandgap close to 1.5 eV. [13] For this reason, studies into B-site composition are less common for single-junction solar cells.Modifying the composition provides a means to tune the properties of perovskite-based devices. Changing the composition of the X-site is known to strongly effect optoelectronic properties [2] and in particular the bandgap. [14] The A-site cation contributes more to structure stability, with a mixed A-site believed to frustrate the known decomposition routes for MAPbI 3 and FAPbI 3 . [15] Cs doping in an FA structure showed the reduced formation of nonperovskite phases, [16,17] and triple-cation systems have shown better PCE in solar cell devices also. [8] However, most systematic studies into perovskite composition are carried out on finished solar cell devices, with the majority of conclusions drawn on perovskite properties being based on electrical parameters, such as PCE. [18] In this work, we investigate how the electronic properties of perovskites themselves, rather than of finished devices, depend on composition. Proxies for carrier mobility and lifetime are evaluated for perovskite thin films using time-resolved microwave conductivity (TRMC). We study single-, double-, and triple-cation lead iodide perovskites and how composition effects optoelectronic properties. In order to keep this a targeted study, we here restrict our attention to the A-site cation rather than the X-site halide. Analogous studies into the role played by X-site composition have previously been carried out. [19] 2. Evaluation of Electronic Properties Via Time-Resolved Microwave Conductivity