stability, [3,4] insensitivity to moisture and ultralow self-doping effect. [5][6][7][8] Unlike the more roundly expanded 3D perovskites, LDRP perovskites with chemical formula of (A) 2 MA n−1 Pb n I 3n+1 (where A is alkylammonium cation and n is the number of inorganic slabs) are considered as infinite nanoplatelets with atomic or molecular size obtained by quantizing the number of [PbI 6 ] 4− octahedra layers between organic ligands which causes quantum and dielectric confinement along one axis. [9][10][11][12] These ultrathin perovskite nanoplatelets are assembled together by intercalating organic cations (Van der Waals force), which protects the degradation of lattice by water and oxygen, resists ion migration and maintains the structural integrity of the 2D and quasi-2D (q-2D) perovskites. [13][14][15] As a result, perovskite solar cells (PSCs) prepared by LDRP perovskite exhibit good stability. [16][17][18][19][20] Although hydrophobic slabs of LDRP perovskites prevent corrosion form water and oxygen, the power conversion efficiency (PCE) of the PSCs are much lower than that of 3D perovskite devices. As the high dielectric constant and exciton binding energy of LDRP perovskite not only narrow the optical absorption windows, but also confine electron-hole pairs to form tight bound excitons. [21][22][23] Low-dimensional Ruddlesden-Popper (LDRP) perovskites are a current theme in solar energy research as researchers attempt to fabricate stable photovoltaic devices from them. However, poor exciton dissociation and insufficiently fast charge transfer slows the charge extraction in these devices, resulting in inferior performance. 1,4-Butanediamine (BEA)-based low-dimensional perovskites are designed to improve the carrier extraction efficiency in such devices. Structural characterization using single-crystal X-ray diffraction reveals that these layered perovskites are formed by the alternating ordering of diammonium (BEA 2+ ) and monoammonium (MA + ) cations in the interlayer space (B-ACI) with the formula (BEA) 0.5 MA n Pb n I 3n+1 . Compared to the typical LDRP counterparts, these B-ACI perovskites deliver a wider light absorption window and lower exciton binding energies with a more stable layered perovskite structure. Additionally, ultrafast transient absorption indicates that B-ACI perovskites exhibit a narrow distribution of quantum well widths, leading to a barrier-free and balanced carrier transport pathway with enhanced carrier diffusion (electron and hole) length over 350 nm. A perovskite solar cell incorporating BEA ligands achieves record efficiencies of 14.86% for (BEA) 0.5 MA 3 Pb 3 I 10 and 17.39% for (BEA) 0.5 Cs 0.15 (FA 0.83 MA 0.17 ) 2.85 Pb 3 (I 0.83 Br 0.17 ) 10 without hysteresis. Furthermore, the triple cations B-ACI devices can retain over 90% of their initial power conversion efficiency when stored under ambient atmospheric conditions for 2400 h and show no significant degradation under constant illumination for over 500 h.