We report strong photoluminescence from a top-emitting organic light-emitting structure where emission takes place through a thin ͑55 nm͒ silver film. We show that this emission is mediated via coupled surface plasmon-polariton modes. Our results show that the addition of a dielectric grating to otherwise planar structures, such as surface-emitting organic light-emitting diodes, may offer a way to increase the external efficiency of top-emitting organic light-emitting diodes. have two advantages over substrate-emitting structures. First, the drive electronics may be integrated into an opaque silicon substrate and second, losses associated with guided modes in the substrate are eliminated. However, a top-emitting OLED does present other problems, notably losses to the surface plasmon-polariton (SPP) modes associated with the metallic cathode. Calculations show that up to 40% of the power that would otherwise be emitted may be lost via this decay channel, 4,5 thus limiting the external quantum efficiency. If some way could be found to recover some of the power lost to these SPPs to light, device efficiency could be improved. One method of coupling SPP modes to light has been the introduction of a periodic microstructure into the metal film, allowing the SPPs to Bragg scatter, 6-8 however, such an approach is demanding in terms of fabrication. Here, we present an alternative in which a microstructured dielectric overlayer is superimposed onto the completed device.A metallic cathode supports two SPP modes, one associated with each metal surface. For a given frequency, these two modes have different in-plane wave vectors (momenta) and so do not interact. An emitter in the organic layer couples more strongly to the SPP associated with the metal/ organic interface than with the SPP associated with the metal/air interface. 9 The energy coupled into the metal/ organic SPP thus needs to be transported across the metal if it is to emerge as light. One way is to use grating-mediated SPP cross coupling; an appropriate microstructure enables the momentum mismatch between the SPP modes to be overcome, allowing them to interact providing a route to transport energy across the film.9,10 However, emission mediated via SPP cross-coupling occurs only over a narrow range of emission angles and wavelengths. 9 An alternative method of coupling the SPPs is to ensure that the materials on either side of the metal have the same refractive index, the SPP wave vectors are then degenerate and may couple.11 It is this coupled geometry that we employ here, a dielectric overlayer added to the metal acts to match the effective refractive index sampled by SPP fields. The coupled SPPs are then scattered to light by a microstructure imposed on the top surface of the dielectric layer.Our experimental structure consisted of a silica substrate spin coated with a 160 nm film of a polymer poly(methylmethacrylate) (PMMA) doped with tris(8-hydroxyquinoline)aluminium ͑Alq 3 ͒ (3% Alq 3 by weight). A 55 nm thick silver film was added by thermal evaporation...