INFRARED-SPECTRA OF THE 10-MU-M BANDS OF 1,2-DIFLUOROETHANE AND 1,1,2-TRIFLUOROETHANE - VIBRATIONALLY MEDIATED TORSIONAL TUNNELING IN 1,1,2-TRIFLUOROETHANE
Sc. Stone et al., INFRARED-SPECTRA OF THE 10-MU-M BANDS OF 1,2-DIFLUOROETHANE AND 1,1,2-TRIFLUOROETHANE - VIBRATIONALLY MEDIATED TORSIONAL TUNNELING IN 1,1,2-TRIFLUOROETHANE, Journal of molecular spectroscopy, 174(2), 1995, pp. 297-318
Citations number
31
Categorie Soggetti
Spectroscopy,"Physics, Atomic, Molecular & Chemical
The 3-MHz-resolution infrared spectra of the 10-mu m bands of the gauc
he conformer of 1,2-difluoroethane (HFC152) and the C-1-symmetry confo
rmer of 1,1,2-trifluoroethane (HFC143) have been measured using a mole
cular-beam electric-resonance optothermal spectrometer with a tunable
microwave-sideband CO2 laser source. For 1,2-difluoroethane, two bands
have been studied, the upsilon(17) B-symmetry C-F stretch at 1077.3 c
m(-1) and the upsilon(13) B-symmetry CH2 rock at 896.6 cm(-1). Both ba
nds are well fit to a asymmetric-rotor Hamiltonian to better than 0.5
MHz. The upsilon(13) band is effectively unperturbed, while the upsilo
n(17) band is weakly perturbed, as shown by the large change in centri
fugal distortion constants from the ground state values. Two bands hav
e also been studied for 1,1,2-trifluoroethane, the upsilon(11) symmetr
ic CF2 stretch at 1077.2 cm(-1) and the upsilon(13) C-C stretch at 905
.1 cm(-1). One of the two bands, upsilon(11), is unperturbed and fit t
o near the experimental precision. The upsilon(13) vibration, on the o
ther hand, is weakly perturbed by an interaction with a nearby state.
This perturbation leads to a doubling or splitting of the lines, due t
o a perturbation-induced lifting of the degeneracy of the symmetric an
d antisymmetric tunneling states associated with tunneling between the
two equivalent C-1 forms. For the J, K-a states studied, the splittin
gs are as large as 37 MHz. Combining this observation with published l
ow-resolution far-infrared measurements of torsional sequence-band and
hot-band frequencies and calculations from an empirical torsional pot
ential allows us to identify the perturbing state as upsilon(17) + 6 u
psilon(18). Here, upsilon(17) is the CF2 twist and upsilon(18) is the
torsion, The matrix element responsible for this interaction exchanges
eight vibrational quanta! (C) 1995 Academic Press, Inc.