The remarkable high PCE of hybrid PSCs relies on the unique advantages of perovskite materials (high light-absorption coefficient, [7] broad lightabsorption range, [8] fast charge-carrier mobility, [9] long diffusion length, [10] tunable bandgap, [11] small exciton binding energy, [12] etc.) and effective structural and surface modifications (compositional engineering, interfacial passivation, additive engineering, etc.). [13][14][15][16] Perovskites based on FA x MA 1−x PbI 3 (FA, formamidinium; MA, methylammonium) have been widely applied in hybrid PSCs due to their lower bandgap and higher solar light-harvesting efficiency in contrast to MAPbI 3 . [17][18][19][20][21] Compared with FAPbI 3 , partial substitution of FA (ionic radius = 2.79 Å) with MA (ionic radius = 2.17 Å) could improve the stability of hybrid PSCs due to the reduced tolerance factor to the appropriate range (0.8-1). [22,23] However, the low-boilingpoint MA cations easily escape from the perovskite lattice during the device fabrication process, and the large FA cations are impeded from embedding into the MA vacancies due to their weak interaction with the established lattice, both of which lead to many defects (MA/FA vacancies, undercoordinated Pb 2+ , and Pb I antisites) at the surface and interface of the perovskite. [24][25][26] Those defects always act as non-radiative recombination Formamidinium methylammonium lead iodide (FAMAPbI 3 ) perovskite has been intensively investigated as a potential photovoltaic material because it has higher phase stability than its pure FAPbI 3 perovskite counterpart. However, its power conversion efficiency (PCE) is significantly inferior due to its high density of surface detects and mismatched energy level with electrodes. Herein, a bifunctional passivator, methyl haloacetate (methyl chloroacetate, (MClA), methyl bromoacetate (MBrA)), is designed to reduce defect density, to tune the energy levels and to improve interfacial charge extraction in the FAMAPbI 3 perovskite cell by synergistic passivation of both CO groups and halogen anions. As predicted by modeling undercoordinated Pb 2+ , the MBrA shows a very strong interaction with Pb 2+ by forming a dimer complex ([C 6 H 10 Br 2 O 4 Pb] 2+ ), which effectively reduces the defect density of the perovskite and suppresses non-radiative recombination. Meanwhile, the Br − in MBrA passivates iodine-deficient defects. Consequently, the MBrA-modified device presents an excellent PCE of 24.29%, an open-circuit voltage (V oc ) of 1.18 V (V oc loss ≈ 0.38 V), which is one of the highest PCEs among all FAMAPbI 3 -based perovskite solar cells reported to date. Furthermore, the MBrA-modified devices without any encapsulation exhibit remarkable long-term stability with only 9% of PCE loss after exposure to ambient air for 1440 h.