Arw. Mckellar et al., Isotopic probing of very weak intermolecular forces: Microwave and infrared spectra of CO-He isotopomers, J CHEM PHYS, 110(22), 1999, pp. 10766-10773
The pure rotational transition (J, j, l) = (101)<--(000) of the weakly boun
d CO-He complex has been observed in the 17 GHz region for five isotopomers
, namely (CO)-C-12-O-16-He-4, (CO)-C-13-O-16-He-4, (CO)-C-12-O-18-He-4, (CO
)-C-13-O-18-He-4, and (CO)-C-13-O-17-He-4, using a pulsed-jet cavity Fourie
r-transform microwave spectrometer. Hyperfine structure due to the quadrupo
lar O-17 (I = 5/2) nucleus has been observed and analyzed to yield the quad
rupole coupling parameters. A new microwave-terahertz double resonance spec
trometer has been used to carry out an experiment on (CO)-C-13-O-16-He-4 in
which a submillimeter-wave pump transition (J, j, l) = (110)<--(000) and a
microwave signal transition (211) <--(110) were detected. Infrared spectra
of (CO)-C-13-O-16-He-4 and (CO)-C-12-O-18-He-4, have been obtained in the
2100 cm(-1) region of the C-O stretch using a tunable diode laser spectrome
ter and a long-path (200 m), low-temperature (46 K) equilibrium gas cell. T
he combined data are sufficient to construct essentially complete experimen
tal energy level schemes for the bound states of the (CO)-C-12-O-16-He-4, (
CO)-C-13-O-16-He-4, and (CO)-C-12-O-18-He-4 forms of the complex. These ene
rgies are compared with calculated levels derived from two intermolecular p
otential models, V-(3,V-3,V-3) and XC (fit). It is shown that the new spect
ra, in particular those of (CO)-C-13-O-16-He-4, discriminate between the tw
o models and indicate that V-(3,V-3,V-3) provides a better representation o
f the potential in the region of the attractive well probed by the bound st
ates. A quasibound state of CO-He was observed for the first time, and its
width due to predissociation was approximately determined, providing a sens
itive measure of the depth of the potential. (C) 1999 American Institute of
Physics. [S0021-9606(99)00622-4].