This paper describes how metal-organic frameworks (MOFs) conformally coated on plasmonic nanoparticle arrays can support excitonplasmon modes with features resembling strong coupling but that are better understood by a weak coupling model. Thin films of Znporphyrin MOFs were assembled by dip coating on arrays of silver nanoparticles (NP@MOF) that sustain surface lattice resonances (SLRs). Coupling of excitons with these lattice plasmons led to an SLR-like mixed mode in both transmission and transient absorption spectra. The spectral position of the mixed mode could be tailored by detuning the SLR in different refractive index environments and by changing the periodicity of the nanoparticle array. Photoluminescence showed mode splitting that can be interpreted as modulation of the exciton line shape by the Fano profile of the surface lattice mode, without requiring Rabi splitting. Compared with pristine Znporphyrin, hybrid NP@MOF structures achieved a 16-fold enhancement in emission intensity. Our results establish MOFs as a crystalline molecular emitter material that can couple with plasmonic structures for energy exchange and transfer. metal-organic framework | plasmonic nanoparticle arrays | conformal coating | surface lattice resonance | photoluminescence P lasmonic nanoparticles (NPs) are driving advances in nanophotonics (1, 2) and photochemistry (3, 4) because of their ability to concentrate and convert optical excitations into heat production, hot-electron generation, and light localization (5). Interactions between the localized surface plasmons (LSPs) (6) of isolated metallic NPs and excitons from molecular emitters can both enhance light absorption and emission (7) and engineer radiative and nonradiative decay pathways (8). Compared with LSPs, surface lattice resonances (SLRs), also referred to as lattice plasmons, are collective modes supported in arrays of NPs that exhibit stronger near-electric field enhancements and higher quality factors Q (9, 10). Because SLRs result from hybridization of LSPs on individual NPs with Bragg diffraction modes from the array (11, 12), their resonance wavelength can be tuned by changing local dielectric environment and lattice periodicity (13,14). Strong coupling between excitons and surface plasmons has been demonstrated by integrating emitters such as single-walled carbon nanotubes (15), monolayer MoS 2 (16), organic dyes (17)(18)(19), and light-harvesting complexes (20, 21) with plasmonic NP arrays.Plasmon-exciton coupling is sensitive to the location of emitters (22): those very close to the NPs are quenched (8), whereas the ones beyond the near-field region show little effect (23). Reports of coupling between organic dyes and plasmonic NP arrays have limited control over emitter locations, and hence, exciton contributions to the mixed SLR-exciton states cannot be tuned (17)(18)(19). Although strong exciton-SLR coupling can be obtained at high dye concentrations (24), such densities typically result in aggregation-induced photoluminescence quenching (25). Thus, the...