Metal island films, especially silver island films, have attracted considerable interest in the past few years in view of their unusual optical properties and potential applications." -91 In this Communication we report on the correlation between the island size and shape distribution and the resulting optical properties. The three-dimensional surface topography of silver island films on glass substrates was investigated by atomic force microscopy (AFM) both before and after thermal annealing and after laser irradiation. Drastic changes due to the annealing process became apparent.In as-prepared films, the islands have diameters of typically 80 nm and are strongly coalesced, forming a rather homogeneous film with a height corrugation of about 2 nm. In contrast, films annealed at 410 K show clearly separated spheroidal silver particles of significantly smaller diameter (typically 25 nm) and a corrugation height of 3-4 nm. Due to the annealing, the peak in the optical absorption spectrum shifts from 493 nm to 431 nm and becomes narrower, a phenomenon which can be explained qualitatively by the observed changes in particle shape and size distribution. Similar effects are observed due to laser irradiation of the as-prepared island films. Calculations of the absorption spectrum based on the experimentally determined size distribution of the islands are in good agreement with the position and shape of the experimentally determined absorption peak.Metal island films,"' i.e., thin layers of certain metals deposited on solid substrates, consist of small droplet-like submicroscopic particles with typical dimensions between 10 and 100 nm. The films are formed during the early stages of slow thermal evaporation and have a typical thickness of several nanometers. Due to the interaction with the substrate, the particle symmetry is broken such that second harmonic generation (SHG) can be excited in the film^.[^-^' Apart from surface-enhanced nonlinear optics and surface enhanced photochemistry, the films also represent suitable substrates for surface-enhanced Raman scattering (SERS),[2.3. ' .' , 9 -1 'I yielding enhancement factors of up to 10'.The physical explanation of the different surface-enhanced optical properties is based on the excitation of localized surface plasmons. The electromagnetic field impinging on the metal islands resonantly drives plasma oscillations, thus producing a secondary field near the surface which may exceed the primary field by one or two orders of magnitude. Mole-[*] Dr. T. Schimmel Experimentalphysik V1, Universitat Bayreuth D-95440 Bayreuth (FRG) H.-G. Bingler, Dr. D. Franrke)" Prof. A. Wokaun Physikalische Chemie 11, Universitat Bayreuth D-95440 Bayreuth (FRG) CH-8092 Zurich (Switzerland) [' I Present address: Laboratorium fur Physikalische Chemie, ETH Zentrum.cules adsorbed on the surface may be excited by this amplified local field. The enhancement factor of the field near the surface is determined by the plasma resonance frequency of the individual metal islands, which, in turn, depends on ...