Department of Chemistry , University of Otago , P.O. Box 56 , Dunedin , New Zealand.
Institute for Physical Chemistry , Friedrich Schiller University Jena , Helmholtzweg 4 , 07743 Jena , Germany.
J Am Chem Soc. 2018 Apr 4;140(13):4534-4542. doi: 10.1021/jacs.7b12868. Epub 2018 Mar 22.
The ground and excited state photophysical properties of a series of fac-[Re(L)(CO)(α-diimine)] complexes, where L = Br, Cl, 4-dimethylaminopyridine (dmap) and pyridine (py) have been extensively studied utilizing numerous electronic and vibrational spectroscopic techniques in conjunction with a suite of quantum chemical methods. The α-diimine ligand consists of 1,10-phenanthroline with the highly electron donating triphenylamine (TPA) appended in the 5 position. This gives rise to intraligand charge transfer (ILCT) states lying lower in energy than the conventional metal-to-ligand charge transfer (MLCT) state, the energies of which are red and blue-shifted, respectively, as the ancillary ligand, L becomes more electron withdrawing. The emitting state is ILCT in nature for all complexes studied, characterized through transient absorption and emission, transient resonance Raman (TR), time-resolved infrared (TRIR) spectroscopy and TDDFT calculations. Systematic modulation of the ancillary ligand causes unanticipated variation in the ILCT lifetime by 2 orders of magnitude, ranging from 6.0 μs for L = Br to 27 ns for L = py, without altering the nature of the excited state formed or the relative order of the other CT states present. Temperature dependent lifetime measurements and quantum chemical calculations provide no clear indication of close lying deactivating states, MO switching, contributions from a halide-to-ligand charge transfer (XLCT) state or dramatic changes in spin-orbit coupling. It appears that the influence of the ancillary ligand on the excited state lifetime could be explained in terms of energy gap law, in which there is a correlation between ln( k) and E with a slope of -21.4 eV for the ILCT emission.
一系列 fac-[Re(L)(CO)(α-二亚胺)] 配合物的基态和激发态光物理性质已通过多种电子和振动光谱技术与一系列量子化学方法相结合进行了广泛研究。α-二亚胺配体由 1,10-菲咯啉组成,在 5 位上附加了高度供电子的三苯胺(TPA)。这导致了内配体电荷转移(ILCT)态位于比传统的金属-配体电荷转移(MLCT)态更低的能量,随着辅助配体 L 变得更具吸电子性,这些态的能量分别红移和蓝移。所有研究的配合物的发射态都是 ILCT,通过瞬态吸收和发射、瞬态共振拉曼(TR)、时间分辨红外(TRIR)光谱和 TDDFT 计算来表征。辅助配体的系统调制导致 ILCT 寿命发生意想不到的 2 个数量级的变化,范围从 L = Br 时的 6.0 μs 到 L = py 时的 27 ns,而不改变形成的激发态的性质或存在的其他 CT 态的相对顺序。温度依赖性寿命测量和量子化学计算没有提供明显的靠近失活态、MO 开关、卤化物-配体电荷转移(XLCT)态贡献或自旋轨道耦合剧烈变化的迹象。似乎辅助配体对激发态寿命的影响可以用能隙定律来解释,其中 ILCT 发射的 ln(k)和 E 之间存在相关性,斜率为-21.4 eV。