Source abstract
Abstract
Various literature studies (Table 6) have reported that dispersion of metal nanoparticles (NPs) on graphitic carbon nitride g-C 3 N 4 (M/CN) has considerably improved the photocatalytic hydrogen yield. It is understood that metal NPs create active sites on the surface of CN and act as a cocatalyst. However, the precise changes induced by different metal NPs on the surface of CN still elude us. Here, we report a thorough understanding and comparison of the morphology, metal–support interactions, interfacial charge transfer kinetics, and band characteristics in different M/CN (M = Pt, Pd, Au, Ag, Cu) correlated with photocatalytic activity. Among all metals, Pt/CN was found to be the best performer both under sunlight and UV–visible irradiation. Under sunlight, maximum H 2 @ 2.7 mmol/h/g was observed over Pt/CN followed by Pd/CN > Au/CN > Ag/CN > Cu/CN ≈ CN. The present study revealed that among all metals, Pt formed superior interfacial contact with g-C 3 N 4 as compared to other metals. The maximum Schottky barrier height (Φ b,Pt ) of 0.66 V was observed at Pt/CN followed by Φ b,Au/CN (0.46 V) and Φ b,Pd/CN (0.05 V). The presence of electron-deficient Pt in Pt-XPS, decrease in the intensity of d-DOS of Pt near the Fermi level in VB-XPS, increase in CB tail states, and cathodic shift in V fb in MS plots sufficiently confirmed strong metal–support interactions in Pt/CN. Due to the SPR effect, Au and Ag NPs suffered from agglomeration and poor dispersion during photodeposition. Finely dispersed Pt NPs (2–4 nm, 53% dispersion) successfully competed with shallow/deep trap states and drove the photogenerated electrons to active metallic sites in a drastically reduced time period as investigated by femtosecond transient absorption spectroscopy. Typically, an interfacial electron transfer rate, K IET, avg, of 2.5 × 10 10 s –1 was observed for Pt/CN, while 0.087 × 10 10 s –1 was observed in Au/CN. Band alignment/potentials at M/CN Schottky junctions were derived and most favorable in Pt/CN with CB tail states much above the water reduction potential; however, in the case of Pd, these extend much below the H + /H 2 potential and hence behave like deep trap states. Thus, in Pd/CN (τ 0 = 4200 ps, 49%) and Ag/CN (3870 ps, 53%), electron deep trapping dominates over charge transfer to active sites. The present study will help in designing futuristic new cocatalyst–photocatalyst systems.
Source: openalex_inverted_index · Quality: baseline
Affiliations
Chemistry Division, Bhabha Atomic Research Centre, Mumbai 400085, Maharashtra India
Homi Bhabha National Institute, Training School Complex, Anushaktinagar, Mumbai 400094, Maharashtra India
Radiation & Photochemistry Division, Bhabha Atomic Research Centre, Mumbai 400085, Maharashtra India
Department of Condensed Matter Physics and Materials Science, Tata Institute of Fundamental Research, Homi Bhabha Road, Mumbai 400005, Maharashtra India
Technical Physics Division, Bhabha Atomic Research Centre, Mumbai 400085, Maharashtra, India
Funding
Department of Science and Technology, Ministry of Science and Technology, India