McKean Donald C, Craig Norman C, Law Mark M
School of Chemistry, University of Edinburgh, Edinburgh , UK.
J Phys Chem A. 2008 Jul 24;112(29):6760-71. doi: 10.1021/jp800628x. Epub 2008 Jun 27.
Potential functions and harmonic (omega(i)) and anharmonic (nu(i)) fundamental frequencies have been calculated for 1,1-difluorocyclopropane (DFCP) and its d4 and d2 isotopomers using the program Gaussian 03. B3LYP and MP2 models were employed, each with the bases 6-311++G** and cc-pVTZ. Anharmonicity corrections Delta(i) = omega(i) - nu(i) are listed and shown to be different for symmetric and antisymmetric CH stretching modes in situations where Fermi resonance appears to be absent. The same effect is missing in C2H4, for which similar calculations were made. The quadratic force fields for DFCP have been scaled in symmetry coordinate space with 15 scale factors both to observed frequencies nu(obsd)and also to omega (obsd), where omega(obsd) = nu(obsd) + Delta. With nu(obsd) especially, different scale factors are needed for the symmetric and antisymmetric CH stretching force constants due to their differing anharmonicities. The source of the latter in the quartic and cubic force field is explored. MP2 calculations of valence interaction force constants involving the stretching of bonds on a common carbon atom are preferred to those from a B3LYP model. In either model, scaling to omega(obsd) rather than to nu(obsd) does not remove the necessity of varying scale factors for differing types of motion in the same group. Theoretical values of the five quartic centrifugal distortion constants are listed for the normal species and compared with new experimental data. The predictions are sufficiently good to be useful in fitting pure rotational transitions. A weakness is identified in the current Gaussian 03 code for the calculation of vibration-rotation quantities, and limitations are noted in the manner in which Fermi resonance is handled.
使用高斯03程序计算了1,1 - 二氟环丙烷(DFCP)及其d4和d2同位素异构体的势能函数、谐波(ω(i))和非谐波(ν(i))基频。采用了B3LYP和MP2模型,每个模型都使用了6 - 311++G**和cc - pVTZ基组。列出了非谐性校正量Δ(i)=ω(i) - ν(i),并表明在似乎不存在费米共振的情况下,对称和反对称CH伸缩模式的校正量是不同的。在进行了类似计算的C2H4中没有这种相同的效应。DFCP的二次力场已在对称坐标空间中用15个比例因子进行了缩放,以使其与观测频率ν(obsd)以及ω(obsd)相匹配,其中ω(obsd)=ν(obsd)+Δ。特别是对于ν(obsd),由于对称和反对称CH伸缩力常数的非谐性不同,需要不同的比例因子。探讨了四次和三次力场中后者的来源。涉及在同一碳原子上键的伸缩的价相互作用力常数的MP2计算比B3LYP模型的计算更可取。在任何一个模型中,按ω(obsd)而不是按ν(obsd)进行缩放并不能消除对同一组中不同类型运动使用不同比例因子的必要性。列出了正常物种的五个四次离心畸变常数的理论值,并与新的实验数据进行了比较。这些预测足够准确,可用于拟合纯转动跃迁。在当前用于计算振动 - 转动量的高斯03代码中发现了一个弱点,并指出了处理费米共振方式的局限性。