S. Belov et al., ELECTRIC RESONANCE OPTOTHERMAL SPECTRUM OF THE 920-CM(-1) NU(14)+NU(15) TORSIONAL COMBINATION BAND OF ACETALDEHYDE, Molecular physics, 81(2), 1994, pp. 359-368
The 920 cm(-1) vibrational band of acetaldehyde (CH3CHO) has been stud
ied at about 2 MHz (FWHM) resolution using an electric resonance optot
hermal spectrometer and a tunable microwave-sideband CO2 laser. Microw
ave and radiofrequency infrared double resonance and precise combinati
on differences are used to assign the spectrum and verify that it orig
inates from the vibrational ground state of the molecule. The band is
observed to have a large A-E torsional tunnelling splitting of 145 cm(
-1), with the A state higher in energy than the E state. The K' = 1 an
d 2 levels for the E state have large K splittings of 28.8 GHz and 54.
5 GHz, respectively, which are similar to the 37.3 GHz and 58.4 GHz sp
littings found for the first excited torsional vibration of the ground
vibrational state. The above observations demonstrate that the 920 cm
(-1) vibrational state has one quantum of torsional excitation, confir
ming previous low-resolution assignments of the band to the A' nu(14)
+ nu(15) combination vibration, consisting of the CH out-of-plane bend
(nu(14) approximate to 764 cm(-1)) and the CH3 torsion (nu(15) M 143
cm(-1)). An effect of the previously proposed Fermi-resonance interact
ion between nu(14) + nu(15) and nu(9) is seen in the much smaller tors
ional splitting in the nu(14) + nu(15) state compared with the nu(15)
fundamental. The observation of a large number of forbidden transition
s for the E state suggests that caution should be used when invoking i
ntramolecular vibrational redistribution as the source of spectral con
gestion in molecules with internal rotors.