Department of Molecular Engineering, Graduate School of Engineering, Kyoto University, Nishikyo-ku, Kyoto 615-8510, Japan.
Inorg Chem. 2012 Mar 5;51(5):2785-92. doi: 10.1021/ic2017402. Epub 2012 Feb 22.
The theoretical evaluation of the oscillator strength of a symmetry-forbidden d-d transition is not easy even nowadays. A new approximate method is proposed here and applied to octahedral complexes Co(NH(3))(6) and Rh(NH(3))(6) as an example. Our method incorporates the effects of geometry distortion induced by molecular vibration and the thermal distribution of such distorted geometries but does not need the Herzberg-Teller approximation. The calculated oscillator strengths of Co(NH(3))(6) agree well with the experimental values in both (1)A(1g) → (1)T(1g) and (1)A(1g) → (1)T(2g) transitions. In the Rh analogue, though the calculated oscillator strengths are somewhat smaller than the experimental values, computational results reproduce well the experimental trends that the oscillator strengths of Rh(NH(3))(6) are much larger than those of the Co analogue and the oscillator strength of the (1)A(1g) → (1)T(1g) transition is larger than that of the (1)A(1g) → (1)T(2g) transition. It is clearly shown that the oscillator strength is not negligibly small even at 0 K because the distorted geometry (or the uncertainty in geometry) by zero-point vibration contributes to the oscillator strength at 0 K. These results are discussed in terms of frequency of molecular vibration, extent of distortion induced by molecular vibration, and charge-transfer character involved in the d-d transition. The computational results clearly show that our method is useful in evaluating and discussing the oscillator strength of symmetry-forbidden d-d absorption of transition metal complex.
即使在今天,对对称性禁阻的 d-d 跃迁的振子强度进行理论评估也不容易。本文提出了一种新的近似方法,并将其应用于八面体配合物Co(NH(3))(6)和Rh(NH(3))(6)为例。我们的方法结合了分子振动引起的几何变形效应和这种变形几何的热分布效应,但不需要 Herzberg-Teller 近似。计算得到的Co(NH(3))(6)的振子强度在(1)A(1g)→(1)T(1g)和(1)A(1g)→(1)T(2g)跃迁中与实验值吻合良好。在 Rh 类似物中,尽管计算得到的振子强度略小于实验值,但计算结果很好地再现了实验趋势,即Rh(NH(3))(6)的振子强度远大于 Co 类似物的振子强度,且(1)A(1g)→(1)T(1g)跃迁的振子强度大于(1)A(1g)→(1)T(2g)跃迁的振子强度。很明显,即使在 0 K 时,振子强度也不是微不足道的,因为零点振动引起的变形几何(或几何不确定性)对 0 K 时的振子强度有贡献。这些结果从分子振动的频率、分子振动引起的变形程度以及 d-d 跃迁涉及的电荷转移特性等方面进行了讨论。计算结果清楚地表明,我们的方法在评估和讨论过渡金属配合物对称性禁阻的 d-d 吸收的振子强度方面是有用的。