“…For a semiconductor to serve as an X-ray detector with characteristics approaching ideal performance, several requirements must be fulfilled: high resistivity (≤10 10 Ω cm) and hence sufficiently low noise levels for resolving charges generated by a single photon, high carrier mobility-lifetime (µτ) product for the efficient collection of photon-generated carriers, and absorption of (nearly) all X-ray photons-the latter scales with the thickness and the average atomic number (Z) of constituting elements. Very few high-Z semiconductors were proposed to fulfill these requirements at room temperature 6,14,15,16,17 and thus far, only costly, ultrapure CdTe and CdZnTe single crystals, usually grown from a melt by high-pressure Bridgman or by Czochralski methods, have been commercially deployed 18,19 . Lead halide perovskite semiconductors (general formula APbX3, where A is a cation, either organic methylammonium (MA + ) or formamidinium, or inorganic Cs + ; and X is an anion of I, Br or Cl halogen) are the most intensely studied class of contender high-Z materials for high-energy photon detection 3,4,5,6,7,12,13,20,21,22,23,24,25,26,27,28 .…”