Pb 2+ ; X = Cl − , Br − , I − ) have demonstrated impressive performance. Capitalizing on their tunable dimensionality, layered perovskites such as 2D and 2D/3D (or quasi-2D) structures have also emerged significantly expanding semiconducting material candidates due to the wide diversity of potential A-site cation and/or X-site anion spacer selections. [9,10] The unique advantages of layered lead halide perovskites are high stability, quantum confinement effect, and tunable photophysical properties. They are increasingly sought after for optoelectronic research in recent years. [11][12][13] The most popular layered lead halide perovskites are based on the Ruddlesden-Popper (RP) structure with the general formula of A n+1 B n X 3n+1 (n = 1, 2, …), where A-site-substituted layered RP-type perovskites are generally hybrid organic-inorganic compounds containing long organic chains. These long organic chains however are insulating. Added to this, the spatial confinements of charge carrier and dielectric contrast between perovskite stack and spacer [11,12] result in a large exciton binding energy, typically ten times larger than the those of 3D perovskites. [14] Most of the reported 2D Ruddlesden-Popper (RP) lead halide perovskites with the general formula of A n+1 B n X 3n+1 (n = 1, 2, …) comprise layered perovskites separated by A-site-substituted organic spacers. To date, only a small number of X-site-substituted RP perovskites have been reported. Herein, the first inorganic-cation pseudohalide 2D phase perovskite single crystal, Cs 2 Pb(SCN) 2 Br 2 , is reported. It is synthesized by the antisolvent vapor-assisted crystallization (AVC) method at room temperature. It exhibits a standard single-layer (n = 1) Ruddlesden-Popper structure described in space group of Pmmn (#59) and has a small separation (d = 1.69 Å) between the perovskite layers. The SCN − anions are found to bend the 2D Pb(SCN) 2 Br 2 framework slightly into a kite-shaped octahedron, limiting the formation of a quasi-2D perovskite structure (n > 1). This 2D single crystal exhibits a reversible first-order phase transformation to 3D CsPbBr 3 (Pm3m #221) at 450 K. It has a low exciton binding energy of 160 meV-one of the lowest for 2D perovskites (n = 1). A Cs 2 Pb(SCN) 2 Br 2 -single-crystal photodetector is demonstrated with respectable responsivity of 8.46 mA W −1 and detectivity of ≈1.2 × 10 10 Jones at a low bias voltage of 0.5 V.