Photoelectrochemical water splitting (PEC) is a compelling approach to convert solar energy to chemical energy by liberating hydrogen, making it a possible solution to the worldwide energy crisis by eliminating all carbon dioxide emissions. In practice, no single electrode material can meet all PEC water splitting requirements. The major challenges for PEC are electron-hole pair recombination, stability and reduced absorption of visible light. Transition Metal dichalcogenides (TMD) based heterostructures are being envisioned as novel electrode materials because of their exceptional electrical, chemical, mechanical and thermal stability which include high electron mobility, highly exposed active sites, layer dependent band gap, and higher ionic conductivity etc. TMDs have higher electro conductivity resulting in significant enhancement of the electrochemical performance in PEC. Further, it also exhibits desirable electrochemical behaviour through its oxygen evolution reaction (OER) and hydrogen evolution reaction (HER) as a photoelectrode for water splitting. However, due to poor absorbance and significant reflection at the grain boundaries, the light harvesting ability of bulk or nanosized TMD materials is often limited. The charge carriers produced by light illumination will also reach the surface faster than bulk materials in the semiconductor, because of the lesser transport distance.In the present work, heterostructures consisting of Tungsten disulfide (WS2) and cadmium sulphide (CdS) were synthesized using a hydrothermal method and Successive Ionic Layer Adsorption Reaction (SILAR) deposition method. The presence of these nanostructures was confirmed by XRD, Raman, UV-Visible spectroscopy, SEM, TEM and PL spectroscopy. The morphological study clearly indicates a homogeneous distribution of CdS nanospheres on WS2 nanostructures, indicating close contact between them which helps in efficient charge separation and migration. Further, the continuous nature of the heterostructures of the two materials is not limited to any visible discrete entities. The porosity of the pristine WS2 nanostructures allows CdS nanospheres to deposit inside the pores along the entire thickness of the nanosphere, and hence, the highly homogeneous nature of the heterostructures is obtained as indicated by the physical characterization.Due to this unique structure, the obtained heterostructures showed excellent performance as photoanode. The CdS@WS2 photoanode demonstrated a photocurrent density of 0.15 mA cm−2 at 1.23 V vs. RHE, which is over 20 times higher than that of the pure pristine materials. Further, CdS@WS2 heterostructures, as compared to pure materials, have demonstrated longer emission-decay-life times and dramatically quenched the emission of fluorescence compared to pristine materials. In CdS@WS2 heterostructures, the absorption edge of the WS2 nanostructures also exhibit a considerable increase in light absorption in the total visible spectrum. This results in enhanced charge separation with proper band alignment leading to improvements in electrochemical performance of CdS@WS2 photoelectrodes. Further, the low onset potential further eliminates the need for voltage bias in practical applications.
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