Ag nanoparticles (NPs) are deposited on BiVO 4 photoanodes to study their effect on the photoelectrochemical (PEC) water splitting performance of the semiconductor. 15 nm light-absorbing NPs and 65 nm light scattering NPs were studied separately to compare their light trapping ability for enhancing the semiconductor's absorption through light concentration and light scattering, respectively. The 15 nm NPs enhanced the BiVO 4 external quantum efficiency throughout the semiconductor's absorption range (e.g., % 2.5 fold at l = 400 nm). However, when a hole scavenger was added to the electrolyte, no enhancement was observed upon NP deposition, indicating that the NPs only facilitate the injection of holes from the semiconductor surface to the electrolyte but do not enhance its absorption. On the other hand, the 65 nm scattering NPs not only facilitated hole injection to the electrolyte, but also enhanced the absorption of the semiconductor (by % 6 %) through light scattering. Such a dual effect, i.e., of enhancing both the surface properties and the absorption of the semiconductor, makes light scattering Ag NPs an ideal decoration for PEC water splitting photoelectrodes.The collective oscillation of valence electrons in metal nanoparticles (NPs) resulting from their electromagnetic interaction with light is known as surface plasmon resonance (SPR). As a result of this phenomenon, metal NPs can either absorb or scatter the irradiating light.[1] The photon frequencies in which the SPR takes place (i.e., the resonant frequencies) depend on the material, shape and size of the NPs.[1] Noble metal NPs (e.g., Ag and Au) exhibit resonance frequencies within the visible spectrum and are great candidate materials in solar energy conversion devices (e.g., photovoltaic and photocatalytic). [2][3][4][5][6] It has been shown that the incident energy absorbed by plasmonic NPs can be transferred to a nearby semiconducting photoelectrode, thereby enhancing its performance. [3][4][5][7][8][9] As a result, many noble metal NP/semiconductor systems have been studied to date, in particular to improve the rate of solar photoelectrochemical reactions (e.g., water splitting for hydrogen generation and phenol degradation for water purification). [4,8,[10][11][12][13][14][15][16][17] In many of these studies, the improvement of the semiconductor's performance, upon plasmonic NP functionalization, has been explained by a light trapping mechanism called local electromagnetic field enhancement or light concentration. In this mechanism, the SPR significantly enhances the intensity of the incoming electromagnetic field (e.g., solar radiation) in the vicinity of the NP, which locally increases the absorption in a nearby semiconductor. [3][4][5]7] Increasing the absorption in the vicinity of the NPs is advantageous when the NPs are placed at the semiconductor-electrolyte interface since, in this case, the absorption increase takes place in the semiconductor space-charge layer where the electron-hole pairs are more efficiently separated. In...