Gatty M Gilbert, Pullen S, Sheibani E, Tian H, Ott S, Hammarström L
Physical Chemistry , Department of Chemistry , Ångström Laboratory , Uppsala University , Box 523 , 75120 Uppsala , Sweden . Email:
Organic Chemistry , Department of Chemistry , Chemical Science and Engineering , KTH , Royal Institute of Technology , Teknikringen 30 , 100 44 Stockholm , Sweden.
Chem Sci. 2018 May 8;9(22):4983-4991. doi: 10.1039/c8sc00990b. eCollection 2018 Jun 14.
Co-sensitization of molecular dyes and catalysts on semiconductor surfaces is a promising strategy to build photoelectrodes for solar fuel production. In such a photoelectrode, understanding the charge transfer reactions between the molecular dye, catalyst and semiconductor material is key to guide further improvement of their photocatalytic performance. Herein, femtosecond mid-infrared transient absorption spectroscopy is used, for the first time, to probe charge transfer reactions leading to catalyst reduction on co-sensitized nickel oxide (NiO) photocathodes. The NiO films were co-sensitized with a molecular dye and a proton reducing catalyst from the family of FeFe(CO) (bdt = benzene-1,2-dithiolate) complexes. Two dyes were used: an organic push-pull dye denoted E2 with a triarylamine-oligothiophene-dicyanovinyl structure and a coumarin 343 dye. Upon photo-excitation of the dye, a clear spectroscopic signature of the reduced catalyst is observed a few picoseconds after excitation in all co-sensitized NiO films. However, kinetic analysis of the transient absorption signals of the dye and reduced catalyst reveal important mechanistic differences in the first reduction of the catalyst depending on the co-sensitized molecular dye (E2 or C343). While catalyst reduction is preceded by hole injection in NiO in C343-sensitized NiO films, the singly reduced catalyst is formed by direct electron transfer from the excited dye E2* to the catalyst in E2-sensitized NiO films. This change in mechanism also impacts the lifetime of the reduced catalyst, which is only 50 ps in E2-sensitized NiO films but is >5 ns in C343-sensitized NiO films. Finally, the implication of this mechanistic study for the development of better co-sensitized photocathodes is discussed.
分子染料与催化剂在半导体表面的共敏化是构建用于太阳能燃料生产的光电极的一种有前景的策略。在这样的光电极中,理解分子染料、催化剂与半导体材料之间的电荷转移反应是指导进一步提高其光催化性能的关键。在此,首次使用飞秒中红外瞬态吸收光谱来探测导致共敏化氧化镍(NiO)光阴极上催化剂还原的电荷转移反应。NiO薄膜用一种分子染料和来自FeFe(CO)(bdt = 苯 - 1,2 - 二硫醇盐)配合物家族的质子还原催化剂进行共敏化。使用了两种染料:一种具有三芳基胺 - 低聚噻吩 - 二氰基乙烯结构的有机推拉染料E2和香豆素343染料。在染料光激发后,在所有共敏化的NiO薄膜中,激发后几皮秒就观察到了还原催化剂的清晰光谱特征。然而,对染料和还原催化剂的瞬态吸收信号的动力学分析揭示了取决于共敏化分子染料(E2或C343),催化剂首次还原过程中重要的机理差异。在C343敏化的NiO薄膜中,催化剂还原之前是NiO中的空穴注入,而在E2敏化的NiO薄膜中,单还原催化剂是由激发态染料E2*直接向催化剂的电子转移形成的。这种机理变化也影响了还原催化剂的寿命,其在E2敏化的NiO薄膜中仅为50皮秒,但在C343敏化的NiO薄膜中大于5纳秒。最后,讨论了这种机理研究对开发更好的共敏化光阴极的意义。