LHPs are emerging as highly efficient light emitters with a narrow full width at half-maximum (FWHM) and tunable emission throughout the visible region (400-700 nm). [3] In particular, all inorganic cesium lead halide (CsPbX 3 , X = Cl, Br, I) perovskite quantum dots (QDs) with near-unity photoluminescence quantum yields (PLQYs) in the blue, green, and red regions and high color purity have been regarded as highly efficient narrow-band phosphors for lighting and next-generation displays devices. [4] Despite their excellent optical properties together with their impressive performance in various lighting fields, LHPs have received criticism because of the toxicity of lead and the lack of long-term stability. [5] Concerning the environmental issues, tin-, bismuth-, and antimony-based analogs such as CsSnX 3 , [6] Cs 3 Bi 2 X 9 , [7] and Cs 3 Sb 2 X 9 , [8] were developed to replace the toxic lead complexes, but both the PLQYs and the stability failed to meet the requirements of practical applications. For example, CsSnX 3 suffers from a low PLQY (0.14% for CsSnBr 3 QDs); simultaneously, it is highly sensitive to oxygen, which subsequently results in severe photoluminescence (PL) quenching. [6] Recently, silverbismuth-based Cs 2 AgBiX 6 double perovskites have attracted wide attention owing to their relatively higher stability. [5a,9] Nevertheless, the PLQY (6.7% for Cs 2 AgBiCl 6 QDs) is still limited. [9a] Similarly, tin(IV)-based Cs 2 SnX 6 double perovskites Lead halide perovskites (LHPs) have received increased attention owing to their intriguing optoelectronic and photonic properties. However, the toxicity of lead and the lack of long-term stability are potential obstacles for the application of LHPs. Herein, the epitaxial synthesis of CsPbX 3 (X = Cl, Br, I) perovskite quantum dots (QDs) by surface chemical conversion of Cs 2 GeF 6 double perovskites with PbX 2 (X = Cl, Br, I) is reported. The experimental results show that the surface of the Cs