Department of Chemistry, Imperial College London, Imperial College Road, London SW7 2AZ, United Kingdom.
Institute of Organic Chemistry and Biochemistry, Academy of Sciences, Flemingovo náměstí 2, 16610 Prague, Czech Republic.
J Chem Theory Comput. 2020 Apr 14;16(4):2627-2634. doi: 10.1021/acs.jctc.0c00081. Epub 2020 Mar 17.
Transition-metal complexes provide rich features in vibrational circular dichroism (VCD) spectra, including significant intensity enhancements, and become thus useful in structural and functional studies of molecules. Quite often, however, the vibrational spectral bands are mixed with the electronic ones, and interpretation of such experiments is difficult. In the present study, we elaborate on the theory needed to calculate the VCD intensities beyond the Born-Oppenheimer (BO) approximation. Within a perturbation approach, the coupling between the electronic and vibrational states is estimated using the harmonic approximation and simplified wave functions obtainable from common density functional theory (DFT) computations. Explicit expressions, including Slater determinants and derivatives of molecular orbitals, are given. On a model diamine complex, the implementation is tested and factors affecting spectral intensities and frequencies are investigated. For two larger molecules, the results are in a qualitative agreement with previous experimental data. Typically, the electronic-vibrational interaction Hamiltonian coupling elements are rather small (∼0 to 10 cm), which provides negligible contributions to vibrational frequencies and absorption intensities. However, significant changes in VCD spectra are induced due to the large transition magnetic dipole moment associated with the d-d metal transitions. The possibility to model the spectra beyond the BO limit opens the way to further applications of chiral spectroscopy and transition-metal complexes.
过渡金属配合物在振动圆二色性(VCD)光谱中提供了丰富的特征,包括显著的强度增强,因此在分子的结构和功能研究中很有用。然而,振动光谱带经常与电子谱带混合,因此很难解释这样的实验。在本研究中,我们详细阐述了超越 Born-Oppenheimer(BO)近似计算 VCD 强度所需的理论。在微扰方法中,使用谐波近似和常见密度泛函理论(DFT)计算中可获得的简化波函数来估计电子态和振动态之间的耦合。给出了包括 Slater 行列式和分子轨道导数在内的显式表达式。在一个模型二胺配合物上进行了实现测试,并研究了影响光谱强度和频率的因素。对于两个较大的分子,结果与以前的实验数据定性一致。通常,电子-振动相互作用哈密顿耦合元素相当小(∼0 到 10 cm),这对振动频率和吸收强度的贡献可以忽略不计。然而,由于与 d-d 金属跃迁相关的大跃迁磁偶极矩,VCD 光谱会发生显著变化。超越 BO 极限模拟光谱的可能性为手性光谱和过渡金属配合物的进一步应用开辟了道路。