Cn. Tam et al., VIBRATIONAL OPTICAL-ACTIVITY OF (3S,6S)-3,6-DIMETHYL-1,4-DIOXANE-2,5-DIONE, Journal of the American Chemical Society, 118(42), 1996, pp. 10285-10293
Vibrational circular dichroism (VCD), absorption, Raman, and Raman opt
ical activity (ROA) spectra for the title compound, a cyclic dimer, we
re measured in non-aqueous solution. The vibrational normal modes are
assigned based on the result from ab initio force field calculation. H
armonic frequencies and atomic polar tensors for simulation of IR abso
rption were calculated both on the (Hartree-Fock SCF) HF/6-31G* level
and using density functional theory (DFT) methods with the Becke3/LYP
hybrid functional. Magnetic transition dipole derivatives were calcul
ated on the HF/6-31G level, and the ROA polarizability tensors were ca
lculated on the HF/4-31G level. Excellent agreement between the DFT ca
lculated and experimental frequencies was obtained without a need for
scaling. Furthermore, using the DFT force field, the correct VCD sign
and intensity patterns were reproduced as compared to the experimental
mid-IR spectra. Reasonable near-IR VCD and mid-IR ROA sign patterns f
or the intense peaks were also calculated. The excellent agreement for
the mid-IR VCD results shows that medium-sized, biologically relevant
molecules can have their spectra simulated using quantum mechanical t
echniques to a high level, certainly one suitable for conformational a
nalyses by direct comparison of theory to experimental results. Compar
ison of DFT and HF level calculations suggests that the improvement fo
und using DFT methods is primarily due to the force field and not to t
he intensity parameters. DFT atomic polar tensors were systematically
weaker than the HF generated ones. Weak coupling between the subunits
of this dimer implies dominance by local interactions which suggests t
hat useful extension of these calculational techniques to larger oligo
mers might be accomplished by transfer of parameters.