Solvation-dependent intracluster proton transfer (ICPT) within bare and Ar-tagged protonated naphthalene− (water) n clusters, H + (Np−W n ) with n ≤ 3, is characterized by infrared photodissociation (IRPD) spectroscopy in a supersonic plasma expansion. IRPD spectra of size-selected clusters recorded in the CH and OH stretch range (2750−3800 cm −1 ) are analyzed with dispersion-corrected density functional theory (DFT) calculations (B3LYP-D3/aug-cc-pVTZ) to determine both the protonation site and the structure of the hydration network. Ar tagging of H + (Np−W n ) leads to colder spectra with higher spectral resolution. The position of the excess proton is controlled by a subtle balance between the difference in proton affinity (PA) of Np and W n and the involved solvation energies. For n = 1, the excess proton is localized on the Np ring, leading to a H + Np−W structure with a bifurcated CH•••O ionic H-bond, because of the large difference in PA of Np and W. For n = 2, ICPT occurs, and the cluster has a structure in which a symmetric Zundel ion is connected to Np via two strong OH•••π ionic H-bonds. Because of the similar PA values of W 2 and Np, the energetics of the ICPT is largely decided by the higher solvation energy in favor of Np−H + W 2 as compared to H + Np−W 2 . For n ≥ 3, the PA of W n substantially exceeds the one of Np, leading to ICPT. Attachment of the bulky planar Np ring to H + W n causes an increasing perturbation of the bare H + W n cluster with size by symmetry reduction and the strong OH•••π H-bonds. Comparison of H + (Np−W n ) with the related H + (Bz−W n ) clusters (Bz = benzene) indicates the implications of extending the aromatic π-electron system on both the critical threshold size for ICPT (n c = 1 for Bz and n c = 2 for Np) and the structure of the hydration network.