Rawool Sushma A, Pai Mrinal R, Banerjee A M, Nath S, Bapat R D, Sharma R K, Dutta B, Hassan P A, Tripathi A K
Chemistry Division, Bhabha Atomic Research Centre, Mumbai 400085, Maharashtra India.
Homi Bhabha National Institute, Training School Complex, Anushaktinagar, Mumbai 400094, Maharashtra India.
ACS Appl Mater Interfaces. 2023 Aug 23;15(33):39926-39945. doi: 10.1021/acsami.3c05833. Epub 2023 Aug 9.
Various literature studies (Table 6) have reported that dispersion of metal nanoparticles (NPs) on graphitic carbon nitride g-CN (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@ 2.7 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-CN as compared to other metals. The maximum Schottky barrier height (Φ) of 0.66 V was observed at Pt/CN followed by Φ (0.46 V) and Φ (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 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, ,, of 2.5 × 10 s was observed for Pt/CN, while 0.087 × 10 s 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 potential and hence behave like deep trap states. Thus, in Pd/CN (τ = 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.
各种文献研究(表6)报道,金属纳米颗粒(NPs)在石墨相氮化碳g-CN(M/CN)上的分散显著提高了光催化产氢量。据了解,金属NPs在CN表面产生活性位点并作为助催化剂。然而,不同金属NPs在CN表面引起的精确变化仍不清楚。在此,我们报告了对不同M/CN(M = Pt、Pd、Au、Ag、Cu)的形态、金属-载体相互作用、界面电荷转移动力学和能带特征与光催化活性之间的全面理解和比较。在所有金属中,发现Pt/CN在阳光和紫外-可见光照射下都是最佳的。在阳光下,Pt/CN上观察到最大H@ 2.7 mmol/h/g,其次是Pd/CN > Au/CN > Ag/CN > Cu/CN ≈ CN。本研究表明,在所有金属中,与其他金属相比,Pt与g-CN形成了更好的界面接触。在Pt/CN处观察到最大肖特基势垒高度(Φ)为0.66 V,其次是Φ(0.46 V)和Φ(0.05 V)。Pt-XPS中缺电子Pt的存在、VB-XPS中费米能级附近Pt的d-DOS强度降低、CB尾态增加以及MS图中的阴极位移充分证实了Pt/CN中强烈的金属-载体相互作用。由于表面等离子体共振(SPR)效应,Au和Ag NPs在光沉积过程中发生团聚且分散性差。通过飞秒瞬态吸收光谱研究发现,精细分散的Pt NPs(2-4 nm,53%分散度)成功地与浅/深陷阱态竞争,并在极短的时间内将光生电子驱动到活性金属位点。通常,Pt/CN的界面电子转移速率,,为2.5×10 s,而Au/CN中为0.087×10 s。推导了M/CN肖特基结处的能带排列/电势,最有利于Pt/CN,其CB尾态远高于水还原电势;然而,对于Pd,这些延伸到远低于H/H电势,因此表现为深陷阱态。因此,在Pd/CN(τ = 4200 ps,49%)和Ag/CN(3870 ps,53%)中,电子深陷阱主导了向活性位点的电荷转移。本研究将有助于设计未来的新型助催化剂-光催化剂系统。