Department of Chemistry and Biochemistry , Auburn University , Auburn , Alabama 36849 , United States.
J Phys Chem A. 2019 Oct 10;123(40):8607-8618. doi: 10.1021/acs.jpca.9b06028. Epub 2019 Sep 30.
We elucidate the subtle energetic effects that give rise to chiral recognition in the propylene oxide dimer. Specifically, we investigate six homochiral () and six heterochiral () structures of this complex, with the - pair sharing the same pattern of weak O···H-C hydrogen bonds but subtly differing in energy due to chiral effects. The interaction energies for the 12 structures are computed at various levels of electronic structure theory and basis set up to the complete basis set limit of the coupled-cluster approach with single, double, and perturbative triple excitations (CCSD(T)). These benchmark interaction energies are compared to the results of various approximate approaches, both density functional theory-based and wave function-based. We find that while the - diastereomeric energy differences exhibit a great deal of error cancellation between the individual interaction energies, most approximate methods have a hard time even reproducing the correct signs of these differences consistently. The origins of the - differences are elucidated by several symmetry-adapted perturbation theory (SAPT) analyses ranging from ordinary intermolecular SAPT to a functional-group SAPT (F-SAPT) decomposition of direct and indirect H → CH substitution effects leading from achiral ethylene oxide complexes to chiral propylene oxide ones. It is shown that the largest diastereomeric energy differences are correlated to the variations in the electrostatic and dispersion SAPT contributions. Finally, the effect of chiral interactions on the vibrational frequencies of a propylene oxide molecule is investigated, showing that the interaction results in largest frequency shifts, splittings, and chiral discrimination effects in the lowest, torsional vibrational mode of the noninteracting monomer.
我们阐明了在环氧丙烷二聚体中产生手性识别的微妙能量效应。具体来说,我们研究了这个复合物的六个同手性()和六个异手性()结构,其中 - 对共享相同的弱 O···H-C 氢键模式,但由于手性效应而在能量上略有不同。我们在电子结构理论的各个层次上计算了这 12 个结构的相互作用能,并在耦合簇方法的完全基组极限下使用单、双和微扰三重激发(CCSD(T))扩展到完全基组。将这些基准相互作用能与各种近似方法的结果进行了比较,包括基于密度泛函理论和波函数的方法。我们发现,尽管 - 非对映异构体的能量差异在各个相互作用能之间表现出很大的误差抵消,但大多数近似方法甚至很难一致地重现这些差异的正确符号。通过几种对称适应微扰理论(SAPT)分析,阐明了 - 差异的起源,这些分析从普通的分子间 SAPT 到直接和间接 H → CH 取代效应的功能组 SAPT(F-SAPT)分解,从非手性环氧乙烷复合物到手性环氧丙烷复合物。结果表明,最大的非对映异构体能量差异与静电和色散 SAPT 贡献的变化相关。最后,研究了手性相互作用对环氧丙烷分子振动频率的影响,结果表明,相互作用导致非相互作用单体的最低扭转振动模式中最大的频率位移、分裂和手性分辨效应。