“…Halide perovskites in the form of bulk thin films have attracted significant interest owing to rapid rises in photovoltaic efficiencies. − Nanocrystals (NCs) of the same material have been garnering strong interest since 2014 for light emission applications due to high photoluminescence quantum yields (PLQYs) approaching unity and an emission wavelength that is tunable throughout the visible range by changing the halide ion. − Two of the important limitations currently hindering the widespread use of this material are (i) a very low efficiency of chloride-containing perovskite NCs, and thus only poor performance in the blue spectral range, and (ii) a tendency of mixed-halide perovskite to phase segregate into domains with different halide ion contents and resulting bandgaps, consequently shifting the emission wavelength strongly during operation of LEDs. − While most of these NCs are either bulklike or only weakly confined, several studies have shown strong quantum confinement in perovskite NCs as a further viable method to tune the emission wavelength especially toward the blue spectral range. − In particular, two-dimensional (2D) nanoplatelets (NPls) have been demonstrated with an atomic-precision control over their thickness down to a single monolayer (ML) and large exciton binding energies, an appealing characteristic for light-emitting applications. ,− These NPls are unfortunately strongly susceptible to surface defects due to a large surface-to-volume ratio, rendering their QYs typically quite low. ,,,, It was often observed that the PLQY of both hybrid and inorganic perovskite NCs drastically decreases with the change in morphology from cubic to platelet form. ,,, For instance, the PLQY of CsPbBr 3 NCs drops from 78% to 31% with a change of morphology from cubic to thick NPls. , Additionally, it is difficult to produce NPls of only a single thickness using current synthesis routes, and the resulting NPls tend to have problems with long-term stability. ,,− …”