c-C3H6O
Oxetane, trimethylene oxide
Species tag 058515
Version1*
Date of EntryOct. 2016
ContributorH. S. P. Müller

The heavy atoms of oxetane are effectively planar, i.e., the molecule has a double minimum potential, but the ground vibrational state is slightly above the barrier. This leads to a very low-lying, very anharmonic ring puckering vibration. The experimental data were taken from
(1) R. A. Creswell, I. M. Mills, 1974, J. Mol. Spectrosc. 52, 392;
and from
(2) A. Lessari, S. Blanco, and J. C. López, 1995, J. Mol. Struct. 354, 237.
Two lines from (1) with residuals much larger than the uncertainties were omitted from the fit.
The predictions are deemed to be sufficient for all needs of astronomers. Predictions with uncertainties larger than 0.3 MHz should be viewed with caution.
Spin-statistics matter for the intensities. The nuclear spin-weight ratio is 9 : 7 for ortho-c-C5H5N : para-c-C5H5N. The ortho states are described by Ka odd, the para states by Ka even.
The dipole moment was taken from (2).

Lines Listed9444
Frequency / GHz< 1000
Max. J75
log STR0-9.0
log STR1-6.3
Isotope Corr.0.0
Egy / (cm–1)0.0
 µa / D1.944
 µb / D 
 µc / D 
 A / MHz12045.46
 B / MHz11734.05
 C / MHz6730.66
 Q(300.0)227549.1389
 Q(225.0)147772.8077
 Q(150.0)80433.0933
 Q(75.00)28449.3307
 Q(37.50)10071.1692
 Q(18.75)3570.5531
 Q(9.375)1269.5286
 Q(5.000)499.4176
 Q(2.725)204.5682
detected in ISM/CSMno


Database maintained by Holger S. P. Müller and Sven Thorwirth, programming by D. Roth and F. Schlöder