bivalent cation (Pb 2+ , Sn 2+ or Ge 2+ ) enveloped by an octahedron comprising six halide ions (XCl − , Br − or I − ) with A being a monovalent cation (e.g., CH 3 NH 3 + , NH 2 CHNH 2 + , or Cs + ) residing in between these corner sharing octahedra. [13,14] These components not only dictate the crystal structure, but also control their optical and electronic properties. [2,15] Exemplary is the optical bandgap, which can be tuned throughout the visible range by controlling the halide content. Halide perovskites can form two-dimensional (2D) or quasi-2D layered structures with thickness of one or a few octahedral layers. [16] The reduced thickness of these layers leads to quantum confinement effects, which changes their optical properties significantly in comparison with their three-dimensional (3D) counterparts, as studied since the 80's on thin film perovskites. [17] Recent studies have shown that nanocrystalline perovskites exhibit enhanced PLQYs and offer tunable optical properties not only through their constituent ions but also through their size. [3,[8][9][10][11]15,18,19] Quantum size effects, as illustrated in Figure 1a, have been extensively investigated in conventional semiconductor nanocrystals such as metal chalcogenides and utilized for a wide range of applications during the last two decades. [20] As the size of the nanocrystals approaches the exciton Bohr radius of the material, quantum confinement effects start to influence the excitonic wave function and the energetic states of the exciton, leading to blueshifted photoluminescence (Figure 1a). Precise control of colloidal semiconductor nanocrystal size has enabled the tuning of the PL emission over wide wavelength ranges. Similarly, perovskite nanocrystals of reduced dimensionality exhibit quantum confinement effects, as shown for the case of nanoplatelets in 2015. [8][9][10]21,22] Despite recent advances, an accurate understanding of thickness-and dimensionality-dependent optical properties of perovskite nanocrystals still proves elusive due to difficulties in the controlled syntheses and characterization of their dimensions. Additionally, while many recent publications present perovskite nanocrystals, most of these show negligible or no quantum confinement. [23,24] Here we will provide a concise overview of quantum confinement effects in perovskite nanocrystals, highlighting synthetic methods and resulting properties, characterization methods and finally applications for these enticing nanostructures.Metal halide perovskites have emerged as a promising new class of layered semiconductor material for light-emitting and photovoltaic applications owing to their outstanding optical and optoelectronic properties. In nanocrystalline form, these layered perovskites exhibit extremely high photoluminescence quantum yields (PLQYs) and show quantum confinement effects analogous to conventional semiconductors when their dimensions are reduced to sizes comparable to their respective exciton Bohr radii. The reduction in size leads to strongly blueshifted ...