Future generations of photoelectrodes for solar fuel generation must employ inexpensive, earth-abundant absorber materials in order to provide a large-scale source of clean energy. These materials tend to have poor electrical transport properties and exhibit carrier diffusion lengths which are significantly shorter than the absorption depth of light. As a result, many photo-excited carriers are generated too far from a reactive surface, and recombine instead of participating in solar-tofuel-conversion. We demonstrate that plasmonic resonances in metallic nanostructures and multi-layer interference effects can be engineered to strongly concentrate sunlight close to the electrode/liquid interface, precisely where the relevant reactions take place. By comparing spectral features in the enhanced photocurrent spectra to full-field electromagnetic simulations, the contribution of surface plasmon excitations is verified. These results open the door to the optimization of a wide variety of photochemical processes by leveraging the rapid advances in the field of plasmonics.Solar fuel generation based on inexpensive, earth-abundant materials constitutes one potentially viable option to satisfy the demand for a terawatt scale renewable source of energy that can be stored and used on demand 1 . The efficiency of solar water splitting 2, 3 based on earth-abundant materials made using scalable processing techniques has remained low despite intensive research efforts since the 1970s. One of the underlying reasons for the observed inefficiency is that many of these materials exhibit a large mismatch between the length scales over which photon absorption takes place (up to micrometers), and the relatively short distances over which electronic carriers can be extracted (often limited to a few 10's of nanometers). One possible approach to circumvent this challenge is to synthesize nanostructured electrodes in which the photon propagation and charge transport directions are orthogonalized. This type of geometry can be accomplished in wire arrays [4][5][6] or other nanostructures with large surface-tovolume ratios 7 . We pursue a new approach that is aimed at the use of metallic