increased over the past decade. This is attributed to the intrinsically excellent photoelectric properties of photoactive perovskite materials, including tunable bandgap, high absorption coefficient, long carrier diffusion length, high photoluminescence quantum yield, and high color purity. [3][4][5] However, the long-term instability of PSCs [6] and PeLEDs [7] limits future commercialization. Device performance gradually degrades under external stimuli, such as moisture, oxygen, light, heat, and electric fields, [8] causing photocarrier recombination and ion migration [9] which are intimately linked to the device microstructure. [10,11] Perovskites are typically fabricated through techniques such as solution process [12][13][14] or thermal evaporation, [15] which can lead to local fluctuations in the microstructural features, such as the presence of grain boundaries, [16,17] intragrain defects, [18,19] surfaces, [20,21] and inhomogeneous domain structures. [22,23] These microstructures have a significant effect on recombination, carrier transport, band alignment, and electrical instability. [24] Transmission electron microscopy (TEM), combined with energy-dispersive X-ray spectroscopy (EDS), [25,26] electron energy loss spectroscopy (EELS), [16] cathodoluminescence (CL), [27] and photoluminescence [28] can provide direct and indispensable insights into the structure, composition, andThe ORCID identification number(s) for the author(s) of this article can be found under