Au and Ag nanoshells are investigated as substrates for surfaceenhanced Raman scattering (SERS). We find that SERS enhancements on nanoshell films are dramatically different from those observed on colloidal aggregates, specifically that the Raman enhancement follows the plasmon resonance of the individual nanoparticles. Comparative finite difference time domain calculations of fields at the surface of smooth and roughened nanoshells reveal that surface roughness contributes only slightly to the total enhancement. SERS enhancements as large as 2.5 ؋ 10 10 on Ag nanoshell films for the nonresonant molecule p-mercaptoaniline are measured.nanoparticles ͉ nanoshells ͉ plasmons ͉ spectroscopy S ince the initial discovery of surface-enhanced Raman scattering (SERS) (1-4), understanding how the local electromagnetic environment enhances the substrate-adsorbate complex's spectral response has been of central importance. It has become increasingly evident that plasmon resonances of the metallic substrate provide intense, local optical-frequency fields responsible for the electromagnetic contribution to SERS (5-7).The lack of reliable techniques for controlling the properties of the local field at the metal surface has been a major experimental limitation in the quantification and understanding of SERS. A striking example of this is the series of experiments reporting enormous SERS enhancements of 10 12 to 10 15 for dye molecules adsorbed on surfaces of aggregated Au and Ag colloid films (6,8,9). The SERS enhancements reported in these experiments have been attributed to localized plasmons, or ''hot spots,'' occurring randomly across this film that fortuitously provide the appropriate electromagnetic nanoenvironment for large SERS enhancements (10). More recent studies have shown that localized plasmons giving rise to very large field enhancements can be formed at the junctions between adjacent nanoparticles (11,12). These plasmons can be described within the plasmon hybridization picture as dimer resonances (13-15). Likewise, self-similar geometries also provide a means for developing large field enhancements (10, 16).Several experimentally realizable geometries, such as triangles (17), nanorings (18), and nanoshells (19), support well defined plasmon resonances whose frequencies can be controlled by judicious modification of the geometry of the nanoparticle. Each of these nanostructured geometries offers its own unique nearfield properties: plasmon resonant frequency, spatial distribution of the near-field amplitude across the surface of the nanostructure, orientation dependence on polarization of the incident light wave, and spatial extent of the near field. The near-field properties of metallic nanoparticles can be calculated very precisely by a variety of methods, such as analytic Mie scattering theory for high-symmetry geometries, and numerical methods such as the discrete dipole approximation (DDA) (20) and the finite difference time domain (21) methods for nanoscale objects of reduced symmetry. Thus, we can approac...