them, CsPbI 2 Br possesses a high stability for preparing in air [3,4] and a suitable bandgap for solar-spectrum absorption, [5,6] so it is considered to be an excellent candidate for fabricating efficient all-inorganic perovskite solar cells (PSCs). However, the black-phase CsPbI 2 Br (cubic α-phase) is unstable under ambient conditions and tends to convert into the most stable nonperovskite δ-CsPbI 2 Br phase, which poses a major hurdle in the path toward commercial viability. Furthermore, despite the rapid development of the CsPbI 2 Br PSCs, their efficiencies achieved to date are still unsatisfactory, leaving much room for further improvement. [7] Recent research shows that the interface state in a PSC is the main factor affecting the stability and performance of the device. [8-11] Therefore, in order to enhance the efficiency and stability of inorganic PSCs, engineering of the different interfaces (such as the electron transport layer (ETL)/CsPbX 3 interface, hole transport layer (HTL)/CsPbX 3 interface) is essential and has been developed in separate works. [12-16] Inorganic perovskite nanocrystals (NCs) consisting of abundant elements and possessing tunable energy levels, excellent crystallinity, and high stability are very attractive for both elemental doping and interface engineering in the inorganic CsPbX 3 PSCs. [17] For example, inorganic CsPbI 3 NCs have been used