represent a class of materials described by the general formula S 2 Y n−1 M n X 3n+1 , where S (typically C m H 2m+1 NH 3 + ) and Y (typically methylammonium (MA), formamidinium (FA), or their mixtures) are organic cations, M is a divalent metal cation (Pb 2+ , Sn 2+ ), and X is a halide ion (Br − , I − ). RPPs form layered structures of perovskite-like slabs separated by the organic ammonium cation spacers (S), where the value of n represents the number of layers of [MX 6 ] 4− octahedra in the stack (Figure 1a; n = 1-3). These structural features render the RPPs natural quantum wells where the number of layers in conjunction with the nature of the spacer group determines the optoelectronic properties. [1][2][3] While MA-based layered perovskite compositions have been extensively explored, [3,5,6] reports of FA-based layered perovskites remain scarce despite the better stability of the FA cation. [7][8][9] In addition, unlike their 3D analogues, layered 2D perovskites generally suffer from poor solarto-electric power conversion efficiencies, [1][2][3] particularly for the FA-based layered perovskites reported to date. Despite the ongoing effort, some of the best performing MA-based layered 2D perovskites have exceeded efficiencies of 12% with hotcasting techniques, [3] whereas the present FA-based analogues gave efficiencies around 1% for various compositions, reaching over 6% after extensive treatments. [7][8][9] This relatively poor performance of RPPs can be predominantly attributed to the inhibition of charge transport by the organic cations that act as insulating layers, since it is the inorganic domains that mainly contribute to the conductivity of the system. [1] Moreover, RPPs possess higher exciton binding energies, which result in decreased performance owing to inefficient exciton dissociation, and in turn to short-circuit photocurrent losses. [3,5] This has been counterbalanced by using additives, such as thiourea, [7][8][9] or employing hot-casting fabrication techniques, [1] with limited reproducibility as well as lack of operational stability reports.Here, we consider that these limitations on the performance of RPPs might be overcome by exploiting the potential tunability of the inherent structural properties through the design Perovskite solar cells are one of the most promising photovoltaic technologies, although their molecular level design and stability toward environmental factors remain a challenge. Layered 2D Ruddlesden-Popper perovskite phases feature an organic spacer bilayer that enhances their environmental stability. Here, the concept of supramolecular engineering of 2D perovskite materials is demonstrated in the case of formamidinium (FA) containing A 2 FA n−1 Pb n I 3n+1 formulations by employing (adamantan-1-yl)methanammonium (A) spacers exhibiting propensity for strong Van der Waals interactions complemented by structural adaptability. The molecular design translates into desirable structural features and phases with different compositions and dimensionalities, identified uniquely ...