Experimental and theoretical studies of IR, VCD, and Raman spectra have been performed on synthesized peptides (iPrCO-Aib-L-Ala-Aib-L-Ala-L-Ala-Aib-NHiPr) having a 310-helical conformation. These sequences vary only due to isotopic labeling (13C=O) of the L-Ala on the relative (i , i +1), (i, i + 2), and(i, i + 3) positions. Di-alkyl substitution on the α-carbon of Aib restricts the rotational freedom of the backbone torsional angles (f, ψ) and favors the formation of 310-helices [1]. Theoretical IR, VCD and Raman simulations were performed on sequences identical to the synthesized ones but constrained (in terms of f, ψ torsional angles) to an ideal 310-helical geometry (−60, −30) and fully optimizing all the other coordinates. All calculations were performed for peptides in vacuum using the DFT BPW91/6-31G∗ level of theory. The simulations predicated the relative separations of 13C=O and 12C=O features and their dependence on conformation as seen experimentally, with the exception that end effects caused a change in diagonal force field not well represented in the theoretical modeling. Experimental spectra for longer sequences and singly labeled variants confirmed the source of deviation for the i,i+1 and i,i+3 models. Comparison of IR and VCD intensity patters helped sort out the vibrational coupling constants sensed in the 13C=O modes. The isotopic labeled group vibrations are coupled to each other most strongly when degenerate and are effectively uncoupled from those of the unlabeled groups.[1] Wang et al., Peptide Science, 2009, 92, 452-456.