Exploiting plasmonic Au nanoparticles to sensitize TiO 2 to visible light is aw idely employed route to produce efficient photocatalysts.H owever,adescription of the atomic and electronic structure of the semiconductor sites in which charges are injected is still not available.S uch ad escription is of great importance in understanding the underlying physical mechanisms and to improve the design of catalysts with enhanced photoactivity.W ei nvestigated changes in the local electronic structure of Ti in pure and N-doped nanostructured TiO 2 loaded with Au nanoparticles during continuous selective excitation of the Au localized surface plasmon resonance with X-ray absorption spectroscopy( XAS) and resonant inelastic X-ray scattering (RIXS). Spectral variations strongly support the presence of long-lived charges localized on Ti states at the semiconductor surface,g iving rise to new laser-induced lowcoordinated Ti sites. Thesearchforinnovativeandefficientschemesfortheuseof solar energy is motivated by the increasing demand for clean energy.M aterials used in artificial photosynthesis,f or example,inwater splitting/CO 2 reduction, [1,2] also find application in important chemical processes,s uch as wastewater treatment, pollutant removal, and production of fine chemicals. [3, 4] Wide band gap semiconductors,t hat is,T iO 2 ,h ave al ow conversion efficiency owing to their poor absorption of solar light. Among the new concepts introduced to increase light harvesting,t he use of plasmonics is particularly promising. [3] Plasmonic nanoparticles (NPs) have extremely high absorption cross-sections as ar esult of localized surface plasmon resonance (LSPR), which is easily tailored across the solar spectrum by the NPs shape and size.U pon illumination, plasmonic NPs can sensitize semiconductors to below bandgap light and create charge-separated states with prolonged lifetime.[4] Them ain sensitization mechanism is the generation of hot electrons (e À )w hich have sufficient energy to overcome the Schottky barrier at the metal/TiO 2 interface and be injected into the TiO 2 conduction band (CB). In parallel, the unique ability of plasmonic NPs to concentrate electromagnetic fields in nanoscale volumes can induce as econdary process where plasmon oscillation resonates with the semiconductor band gap,that is,plasmonic resonantenergy transfer (PRET).[4] Recently,p lasmonic driven processes (whether charge or energy transfer) have been the focus of intense research. [3, 4] Fore xample,M ubeen et al. reported aw ater-splitting device based on Au/TiO 2 in which all the charge carriers involved in the reaction were Au hot e À .[2] Tailored composite materials and bimetallic plasmonic NPs have also shown high efficiencyi nd riving extensive number of selective chemical reactions. [3, 4] In metal oxides that are used to convert solar light into chemical energy,t he catalytic process is driven by transient changes in the metal oxide'sp roperties,s uch as the metal oxidation state and/or the local reconstruction of cata...