Silicon nanowire array (SiNWs)-based photoelectrochemical (PEC) cells are regarded as a new and prospective candidate for optoelectronic applications due to their excellent optical absorption, large specific surface, and low-cost preparation. However, they suffer from the surface recombination of photocarriers and from photo-corrosion/photo-oxidation. In this work, the PEC response characteristics of SiNWs before and after covering with a thin carbon film were investigated. An enhancement factor of 35.87% in the PEC responsivity was observed after coating with the carbon shell. The degradations of the photocurrent with increasing illumination time and of the photocurrent versus potential with increasing measurement number were suppressed by the carbon shell.To obtain high performance from conventional photovoltaic devices arranged in a bulk formation, two fundamental requirements must be fulfilled, i.e., the photoactive layers must be thick enough to adequately absorb incident photons (especially for indirect-band materials like silicon (Si) and germanium (Ge)), and the minority-carrier diffusion length must be compatible with the large absorption depth (i.e., 125 μm thick Si is needed to absorb 90% of the above-bandgap photons), which means that the materials should be highly purified. 1,2 The simultaneous demands of high-quality crystalline materials and thick absorption layers inevitably give rise to a high production cost. However, one-dimensional (1D) nanostructures provide a promising and prospective approach to fabricate low-cost and high-performance optoelectronic devices owning to their large length-to-diameter and surface-to-volume ratios. 3-6 First, excellent light absorption can be realized from 1D nanostructure arrays with a small volume due to their moth-eye-like morphology perfect for antireflection effect 7,8 and light confinement under various optical mechanisms. 9-11 Second, the promising orthogonal spatial relation between carrier separation and photon absorption (via radial junction) guarantees a short diffusion distance and an effective carrier collection, allowing the lowgrade materials to be available for high-performance optoelectronic devices. 1,2,12 To fabricate solid-state and uniform radial junctions, complex instruments and harsh conditions are usually needed for in situ growth of the coaxial multishell 1D nanostructures. 13 The situation becomes even more severe if a radial junction with a specific doping requirement is involved. 14 In contrast, liquid-state radial junctions, which can be easily prepared via photoelectrochemical (PEC) cells, 15-17 emerge as a prototypical configuration for 1D nanostructure arrays in order to explore new concepts for solar energy applications. Nevertheless, two challenges still exist in achieving high-performance nanostructured devices based on liquid-state junctions. First, the nanostructure photoelectrodes in an electrolyte are generally degenerated significantly by photo-oxidation and/or photo-corrosion due to the large surface-to-volume ratio and ...