Red-Shifting versus Blue-Shifting Hydrogen Bonds: Perspective from Ab Initio Valence Bond Theory

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• 作者：Xin Chang ; Yang Zhang ; Xinzhen Weng ; Peifeng Su ; Wei Wu ; Yirong Mo
• 刊名：Journal of Physical Chemistry A
• 出版年：2016
• 出版时间：May 5, 2016
• 年：2016
• 卷：120
• 期：17
• 页码：2749-2756
• 全文大小：348K
• 年卷期：0
• ISSN：1520-5215

文摘

Both proper, red-shifting and improper, blue-shifting hydrogen bonds have been well-recognized with enormous experimental and computational studies. The current consensus is that there is no difference in nature between these two kinds of hydrogen bonds, where the electrostatic interaction dominates. Since most if not all the computational studies are based on molecular orbital theory, it would be interesting to gain insight into the hydrogen bonds with modern valence bond (VB) theory. In this work, we performed ab initio VBSCF computations on a series of hydrogen-bonding systems, where the sole hydrogen bond donor CF<sub>3sub>H interacts with ten hydrogen bond acceptors Y (═NH<sub>2sub>CH<sub>3sub>, NH<sub>3sub>, NH<sub>2sub>Cl, OH<sup>–sup>, H<sub>2sub>O, CH<sub>3sub>OH, (CH<sub>3sub>)<sub>2sub>O, F<sup>–sup>, HF, or CH<sub>3sub>F). This series includes four red-shifting and six blue-shifting hydrogen bonds. Consistent with existing findings in literature, VB-based energy decomposition analyses show that electrostatic interaction plays the dominating role and polarization plays the secondary role in all these hydrogen-bonding systems, and the charge transfer interaction, which denotes the hyperconjugation effect, contributes only slightly to the total interaction energy. As VB theory describes any real chemical bond in terms of pure covalent and ionic structures, our fragment interaction analysis reveals that with the approaching of a hydrogen bond acceptor Y, the covalent state of the F<sub>3sub>C–H bond tends to blue-shift, due to the strong repulsion between the hydrogen atom and Y. In contrast, the ionic state F<sub>3sub>C<sup>–sup> H<sup>+sup> leads to the red-shifting of the C–H vibrational frequency, owing to the attraction between the proton and Y. Thus, the relative weights of the covalent and ionic structures essentially determine the direction of frequency change. Indeed, we find the correlation between the structural weights and vibrational frequency changes.