g-i-C3H7OH
Isopropanol, gauche conformer
Species tag 060518
Version1*
Date of EntryApr. 2018
ContributorH. S. P. Müller

Isopropanol is the branched isomer of normal propanol. There are two conformers, the doubly degenerate gauche and the singly degenerate anti, also known as trans, which is about 120 K (or 83.4 cm–1) higher in energy. Tunneling between the equivalent gauche conformations lifts the degeneracy, creating a symmetric (state number 0) and an antisymmetric (state number 1) tunneling substate. The latter is about 46.8 GHz above the former.
A very extensive list of transition frequencies was taken from
(1) A. Maeda, I. R. Medvedev, F. C. De Lucia, E. Herbst, 2006 Astrophys. J. Suppl. Ser. 166, 650.
A modest number of transition frequencies were taken from
(2) E. Hirota, 1979 J. Phys. Chem. 83, 1457;
from
(3) O. N. Ulenikov, A. B. Malikova, Ch. O. Qager, S. A. Musaev, A. A. Adilov, and M. I. Mehtiev, 1991 J. Mol. Spectrosc. 145, 262;
and from
(4) H. S. P. Müller, 2018, unpublished.
Very widespread rotation-tunneling interaction takes place between the two gauche substates. There is no clear evidence for rotation-tunneling interaction between anti and either gauche substate. The Hamiltonian consists only of even order parameters, in contrast to (1). It is largely set up as proposed in
(5) D. Christen and H. S. P. Müller, 2003 Phys. Chem. Chem. Phys. 5, 3600.
The differences in the Hamiltonian afforded a small number of transitions from (1) to be reassigned. In addition, a very small number of transition frequencies with large residuals were omitted from the fit. The signs of the lowest order interaction parameters Fab and Fac were chosen to be negative and positive, respectively, as in (1), (2), and (3). Careful inspection of relative intensities in (4) required the b-dipole component to be negative if the a- and c-components are positive. Data from (4) were not merged. Predicted transition frequencies with uncertainties around 0.1 MHz should be viewed with some caution because of the severe rotation-tunneling interaction, those with uncertainties greater than 0.2 MHz should be viewed with considerable caution. Nevertheless, predictions should be sufficient for all observational purposes.
The partition functions takes into consideration only the ground vibrational states of both conformers. Individual contributions are available. Vibrational correction factors should be available in the near future.
The dipole moment components were reported in (2).

Lines Listed60716
Frequency / GHz< 720
Max. J83
log STR0-9.0
log STR1-7.0
Isotope Corr.-0.0
Egy / cm–10.0 / 1.561
 µa / D1.114
 µb / D-0.737
 µc / D0.813
 A / MHz8639.542
 B / MHz8063.218
 C / MHz4768.249
 Q(300.0)128589.1576
 Q(225.0)80775.5612
 Q(150.0)41510.5232
 Q(75.00)13084.1903
 Q(37.50)4221.9020
 Q(18.75)1424.3947
 Q(9.375)478.3373
 Q(5.000)171.9917
 Q(2.725)61.5401
detected in ISM/CSMno


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