Department of Chemistry, University of Calgary, University Drive 2500, Calgary AB T2N-1N4, Canada.
J Phys Chem A. 2012 Feb 23;116(7):1864-76. doi: 10.1021/jp212292j. Epub 2012 Feb 9.
We have applied time dependent density functional theory to study excited state structures of the tetroxo d(0) transition metal complexes MnO(4)(-), TcO(4)(-), RuO(4), and OsO(4). The excited state geometry optimization was based on a newly implemented scheme [Seth et al. Theor. Chem. Acc. 2011, 129, 331]. The first excited state has a C(3v) geometry for all investigated complexes and is due to a "charge transfer" transition from the oxygen based HOMO to the metal based LUMO. The second excited state can uniformly be characterized by "charge transfer" from the oxygen HOMO-1 to the metal LUMO with a D(2d) geometry for TcO(4)(-), RuO(4), and OsO(4) and two C(2v) geometries for MnO(4)(-). It is finally found that the third excited state of MnO(4)(-) representing the HOMO to metal based LUMO+1 orbital transition has a D(2d) geometry. On the basis of the calculated excited state structures and vibrational modes, the Franck-Condon method was used to simulate the vibronic structure of the absorption spectra for the tetroxo d(0) transition metal complexes. The Franck-Condon scheme seems to reproduce the salient features of the experimental spectra as well as the simulated vibronic structure for MnO(4)(-) generated from an alternative scheme [Neugebauer J. J. Phys. Chem. A 2005, 109, 1168] that does not apply the Franck-Condon approximation.
我们应用含时密度泛函理论研究了四氧基 d(0)过渡金属配合物 MnO(4)(-), TcO(4)(-), RuO(4) 和 OsO(4) 的激发态结构。激发态几何优化是基于新实现的方案 [Seth 等人,Theor. Chem. Acc. 2011, 129, 331]。所有研究的配合物的第一激发态具有 C(3v) 几何形状,这是由于氧基 HOMO 到金属基 LUMO 的“电荷转移”跃迁。第二激发态可以统一地用 D(2d) 几何形状来描述 TcO(4)(-), RuO(4) 和 OsO(4) 中从氧 HOMO-1 到金属 LUMO 的“电荷转移”,以及 MnO(4)(-) 中的两个 C(2v) 几何形状。最后发现,MnO(4)(-) 的第三激发态代表 HOMO 到金属基 LUMO+1 轨道跃迁,具有 D(2d) 几何形状。基于计算的激发态结构和振动模式,Franck-Condon 方法被用于模拟四氧基 d(0)过渡金属配合物吸收光谱的振子结构。Franck-Condon 方案似乎再现了实验光谱的显著特征,以及来自替代方案 [Neugebauer J. J. Phys. Chem. A 2005, 109, 1168] 的 MnO(4)(-) 的模拟振子结构,该方案不应用 Franck-Condon 近似。