Lockard Jenny V, Valverde Guadalupe, Neuhauser Daniel, Zink Jeffrey I, Luo Yun, Weaver Michael N, Nelsen Stephen F
Department of Chemistry and Biochemistry, University of California, Los Angeles, California 90095, USA.
J Phys Chem A. 2006 Jan 12;110(1):57-66. doi: 10.1021/jp055880o.
Excited state mixed valence (ESMV) occurs in molecules in which the ground state has a symmetrical charge distribution but the excited state possesses two or more interchangeably equivalent sites that have different formal oxidation states. Although mixed valence excited states are relatively common in both organic and inorganic molecules, their properties have only recently been explored, primarily because their spectroscopic features are usually overlapped or obscured by other transitions in the molecule. The mixed valence excited state absorption bands of 2,3-di-p-anisyl-2,3-diazabicyclo[2.2.2]octane radical cation are well-separated from others in the absorption spectrum and are particularly well-suited for detailed analysis using the ESMV model. Excited state coupling splits the absorption band into two components. The lower energy component is broader and more intense than the higher energy component. The absorption bandwidths are caused by progressions in totally symmetric modes, and the difference in bandwidths is caused by the coordinate dependence of the excited state coupling. The Raman intensities obtained in resonance with the high and low energy components differ significantly from those expected based on the oscillator strengths of the bands. This unexpected observation is a result of the excited state coupling and is explained by both the averaging of the transition dipole moment orientation over all angles for the two types of spectroscopies and the coordinate-dependent coupling. The absorption spectrum is fit using a coupled two-state model in which both symmetric and asymmetric coordinates are included. The physical meaning of the observed resonance Raman intensity trends is discussed along with the origin of the coordinate-dependent coupling. The well-separated mixed valence excited state spectroscopic components enable detailed electronic and resonance Raman data to be obtained from which the model can be more fully developed and tested.
激发态混合价(ESMV)出现在基态具有对称电荷分布但激发态拥有两个或更多形式氧化态不同的可互换等价位点的分子中。尽管混合价激发态在有机和无机分子中都相对常见,但它们的性质直到最近才被探索,主要是因为它们的光谱特征通常与分子中的其他跃迁重叠或被掩盖。2,3-二对甲氧基苯基-2,3-二氮杂双环[2.2.2]辛烷自由基阳离子的混合价激发态吸收带在吸收光谱中与其他吸收带很好地分离,特别适合使用ESMV模型进行详细分析。激发态耦合将吸收带分裂为两个组分。能量较低的组分比能量较高的组分更宽且更强。吸收带宽是由全对称模式的进展引起的,带宽差异是由激发态耦合的坐标依赖性引起的。与高、低能量组分共振获得的拉曼强度与基于能带振子强度预期的强度有显著差异。这一意外观察结果是激发态耦合的结果,并且通过两种光谱学中跃迁偶极矩取向在所有角度上的平均以及坐标依赖性耦合来解释。使用包含对称和不对称坐标的耦合双态模型对吸收光谱进行拟合。讨论了观察到的共振拉曼强度趋势的物理意义以及坐标依赖性耦合的起源。分离良好的混合价激发态光谱组分使得能够获得详细的电子和共振拉曼数据,从而可以更全面地开发和测试该模型。