Department of Chemistry, University of California, Berkeley , Berkeley, California 94720, United States.
J Am Chem Soc. 2017 Feb 8;139(5):1830-1841. doi: 10.1021/jacs.6b09550. Epub 2016 Dec 20.
The initial step of photocatalytic water oxidation reaction at the metal oxide/aqueous interface involves intermediates formed by trapping photogenerated, valence band holes on different reactive sites of the oxide surface. In SrTiO these one-electron intermediates are radicals located in Ti-O (oxyl) and Ti-O-Ti (bridge) groups arranged perpendicular and parallel to the surface respectively, and form electronic states in the band gap of SrTiO. Using an ultrafast sub band gap probe of 400 nm and white light, we excited transitions between these radical states and the conduction band. By measuring the time evolution of surface reflectivity following the pump pulse of 266 nm light, we determined an initial radical formation time of 1.3 ± 0.2 ps, which is identical to the time to populate the surface with titanium oxyl (Ti-O) radicals. The oxyl was separately observed by a subsurface vibration near 800 cm from Ti-O located in the plane right below Ti-O. Second, a polarized transition optical dipole allows us to assign the 1.3 ps time constant to the production of both O-site radicals. After a 4.5 ps delay, another distinct surface species forms with a time constant of 36 ± 10 ps with a yet undetermined structure. As would be expected, the radicals' decay, specifically probed by the oxyl's subsurface vibration, parallels that of the photocurrent. Our results led us to propose a nonadiabatic kinetic mechanism for generating radicals of the type Ti-O and Ti-O-Ti from valence band holes based on their solvation at aqueous interfaces.
在金属氧化物/水界面上进行光催化水氧化反应的初始步骤涉及通过将光生价带空穴捕获在氧化物表面的不同反应性位点上形成的中间体。在 SrTiO 中,这些单电子中间体是位于 Ti-O(氧)和 Ti-O-Ti(桥)基团中的自由基,它们分别垂直和平行于表面排列,并在 SrTiO 的带隙中形成电子态。使用 400nm 的超快亚带隙探针和白光,我们激发了这些自由基态与导带之间的跃迁。通过测量 266nm 光泵浦脉冲后的表面反射率随时间的演化,我们确定了自由基形成的初始时间为 1.3 ± 0.2ps,这与用钛氧(Ti-O)自由基填充表面的时间相同。通过在钛氧下方平面中位于 Ti-O 附近的近 800cm 的亚表面振动,单独观察到了氧。其次,偏振跃迁光偶极允许我们将 1.3ps 的时间常数分配给 O 位自由基的产生。4.5ps 延迟后,另一个具有 36 ± 10ps 的时间常数的独特表面物种形成,其结构尚未确定。正如预期的那样,自由基的衰减,特别是通过氧的亚表面振动来探测,与光电流的衰减平行。我们的结果促使我们提出了一种非绝热动力学机制,用于基于在水界面处的溶剂化作用从价带空穴生成 Ti-O 和 Ti-O-Ti 类型的自由基。