Chiral metal halide perovskites (MHPs) are emerging as one of the most appealing classes of chiral materials due to their potential use for chiroptoelectronics, spintronics, and ferroelectrics. One of the most common strategies used to induce chirality-dependent properties in MHPs, such as circular dichroism (CD), circular polarized luminescence (CPL), chiro-induced spin selectivity (CISS) effect and ferroelectricity, is based on the introduction of a chiral ligand in low-dimensional MHPs. This approach, coupled with their rich structural tunability, made the preparation of 2D, 1D, and 0D chiral MHPs possible.