the interaction between light and matter, has attracted intensive research interest, due to its potential applications in water electrolysis, [1a] biosensors, [2] photochemical catalysis, [3] and optical heating. [4] LSPR modes are the collective oscillations of conduction band electrons at the interface between materials with negative and positive permittivity, [5] such as Au, [6] Ag, [5c] and Cu, [7] upon illumination with light of specific wavelengths. The electromagnetic field at the surface of the metals is amplified by the electron oscillations. [8] Such near field enhancement affords higher energy electrons, and therefore significantly promote the catalytic performance of the plasmonic metals. [9] The LSPR effect is highly dependent upon the physiochemical properties of the catalysts, such as morphology of the plasmonic metals and the localized electronic landscape. [7,10] Effective utilization of the LSPR effect for high-performance catalysis is require fine tuning of dielectric relaxation routes between the excited plasmonic metals and the surrounding substances. [11] For instance, when the plasmonic metals are nanosized (<30 nm), the LSPR decay would favor chemical transformation, as a result of nonthermalized charge-carriers distributing according to the Landau damping model. [12] So far, enormous efforts have been devoted to controlling the plasmon decay by designing distinctive plasmonic metal-containing nanostructures. [11a,13] Au nanoparticles (NPs) have been frequently studied as typical plasmonic metal catalysts. [5b,14] The deposition of Au NPs onto Ni(OH) 2 nanosheets promoted electrochemical water oxidation under illumination, compared to bare Ni(OH) 2 and bare Au NPs. [1a] Additionally, yolkshell nanostructures (YSs) and core-shell nanostructures (CSs) possess the advantage of collection of radiative, energetic carriers at the shells from the high concentration of electron-hole pairs at the cores, and thus facilitate the charge transfer of the nanomaterials to the adsorbates. [8a,9a,b,e,15] Energy losses within the CSs can be minimized by weakening the scattering, and thus, the confinement of the illumination energy by LSPR can be maximized. The controllable dielectric relaxation of LSPR decay of YSs has been observed in Ag@Pt CSs nanostructures under wavelength-specific illumination. [15b] However, the energy transfer mechanism between the core/yolk and the shell in YSs is still unclear.In this work, hybrid YSs with Au yolk (ca. 8 nm) and Ni 3 S 2 shell (ca. 8 nm in thickness) were fabricated to promote the visible-light-assisted OER. The efficient harvesting of solar energy Hybrid nanostructures with a plasmonic core and catalytic shell often show significantly enhanced catalytic efficiency under illumination of specific frequency. Excitation of localized surface plasmonic resonance on plasmonic metals under illumination can generate hot electrons that assist in the catalytic reaction. However, the correlation between the microstructural geometry, dielectric environment, internal e...