26AlF v = 0 – 2
Aluminum monofluoride, X 1Σ+, 26Al isotopolog
Species tag 045523
Version1*
Date of EntryJan. 2019
ContributorH. S. P. Müller

Experimental data refer to the 27AlF isotopic species. A Born-Oppenheimer breakdown value was estimated for Y01, even though its effect is very small.
Rotational transition frequencies were reported by
(1) F. C. Wyse, W. Gordy, and E. F. Pearson, 1970, J. Chem. Phys. 52, 3887;
and by
(2) J. Hoeft, F. J. Lovas, E. Tiemann, and T. Törring, 1970, Z. Naturforsch. 25a, 1029.
Also used in the model were rovibrational transition frequencies from
(3) A. G. Maki and F. J. Lovas, 1982, J. Mol. Spectrosc. 95, 80;
and from
(4) H. G. Hedderich and P. F. Bernath, 1992, J. Mol. Spectrosc. 153, 73.
The highest-J ground state transition of (1) was omitted because of a large deviation between measured frequency and that calculted from the final spectroscopic parameters.
The calculated transitions should be accurate enough for all observational purposes. Some caution may be advised for those at high J or high v. Al hyperfine splitting may be resolvable at very low J, but these transitions are likely too weak to be observable.
Only the first 5 vibrational states were included in the calculation of partition function values. The values at 1000 K and higher have been estimated.
The dipole moment from a quantum-chemical calculation was assumed to agree with that of the main isotoplog, see e046528.cat.

Lines Listed270
Frequency / GHz< 3000
Max. J93
log STR0-11.0
log STR1-12.0
Isotope Corr.-0.0
Egy / cm–10.0, 798.856, 1588.037
 µa / D1.440, 1.506, 1.573
 µb / D 
 µc / D 
 A / MHz 
 B / MHz16748.506, ...
 C / MHz 
 Q(3000.)12034.9
 Q(2500.)8703.1
 Q(2000.)5862.0
 Q(1500.)3565.3
 Q(1000.)1844.2
 Q(500.0)694.4543
 Q(300.0)382.4785
 Q(225.0)282.2800
 Q(150.0)187.1703
 Q(75.00)93.6742
 Q(37.50)46.9964
 Q(18.75)23.6649
 Q(9.375)12.0030
detected in ISM/CSMyes (v = 0)


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