Aa. Elazhary et Hu. Suter, COMPARISON BETWEEN OPTIMIZED GEOMETRIES AND VIBRATIONAL FREQUENCIES CALCULATED BY THE DFT METHODS, Journal of physical chemistry, 100(37), 1996, pp. 15056-15063
Optimized geometries, vibrational frequencies, and scale factors were
calculated for furan and thiophene with the HF, MP2, LDA, BVWN, BLYP,
and B3LYP methods of theory using the 6-31G*, cc-pVDZ, and cc-pVTZ ba
sis sets. The agreement between the optimized and experimental geometr
ies was in the order B3LYP, MP2, LDA, BVWN, BLYP, then HF. The calcula
ted frequencies by the unscaled BVWN force field had the smallest aver
age error in the mid-IR region, but using one-scale-factor scaling, th
ose calculated by the scaled B3LYP force field had the lowest average
error. Using one-scale-factor scaling, scale factors of 0.82, 0.89, 0.
98, 0.93, 0.96, and 0.96 were obtained by the KF, MP2, BLYP, B3LYP, LD
A, and BVWN force fields, respectively, using the 6-31G* basis set. T
he effect of the basis set on the calculated bond angles, frequencies,
and scale factors by the DFT methods was minor, but except with the L
DA method, the agreement between the calculated and experimental bond
lengths can be arranged in the order cc-pVDZ, 6-31G*, then cc-pVTZ ba
sis set.