Unusual blue to red shifting of C–H stretching frequency of CHCl3 in co-operatively P⋯Cl phosphorus bonded POCl3–CHCl3 heterodimers at low temperature inert matrixes

化学 氢键 费米共振 密度泛函理论 红外光谱学 从头算 伦敦分散部队 红外线的 结晶学 计算化学 分子 范德瓦尔斯力 有机化学 物理 光学
作者
P.K. Sruthi,Swaroop Chandra,N. Ramanathan,K. Sundararajan
出处
期刊:Journal of Chemical Physics [American Institute of Physics]
卷期号:153 (17) 被引量:15
标识
DOI:10.1063/5.0031162
摘要

Heterodimers of POCl3—CHCl3 were generated in Ne, Ar, and Kr matrixes at low temperatures and were studied using infrared spectroscopy. The remarkable role of co-operative pentavalent phosphorus bonding in the stabilization of the structure dictated by hydrogen bonding is deciphered. The complete potential energy surface of the heterodimer was scanned by ab initio and density functional theory computational methodologies. The hydrogen bond between the phosphoryl oxygen of POCl3 and C—H group of CHCl3 in heterodimers induces a blue-shift in the C—H stretching frequency within the Ne matrix. However, in Ar and Kr matrixes, the C—H stretching frequency is exceptionally red-shifted in stark contrast with Ne. The plausibility of the Fermi resonance by the C—H stretching vibrational mode with higher order modes in the heterodimers has been eliminated as a possible cause within Ar and Kr matrixes by isotopic substitution (CDCl3) experiments. To evaluate the influence of matrixes as a possible cause of red-shift, self-consistent Iso-density polarized continuum reaction field model was applied. This conveyed the important role of the dielectric matrixes in inducing the fascinating vibrational shift from blue (Ne) to red (Ar and Kr) due to the matrix specific transmutation of the POCl3—CHCl3 structure. The heterodimer produced in the Ne matrix possesses a cyclic structure stabilized by hydrogen bonding with co-operative phosphorus bonding, while in Ar and Kr the generation of an acyclic open structure stabilized solely by hydrogen bonding is promoted. Compelling justification regarding the dispersion force based influence of matrix environments in addition to the well-known dielectric influence is presented.
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