The molecule is nearly T-shaped with the NaN bond slightly
shorter than the NaC bond. Therefore, the molecule should be
considered more as sodium isocyanide rather than as
sodium cyanide.
The first entry from Apr. 2007 has been revised based on
an analysis from
(1) H. S. P. Müller, D. T. Halfen, and
L. M. Ziurys,
2012, J. Mol. Spectrosc. 272, 23.
The experimental measurements were taken
from
(2) J. J. van Vaals, W. L. Meerts, and A. Dymanus,
1984, Chem. Phys. 86, 147.
As described in (1), the reported uncertainties in (2) were
assumed to be 3 σ values.
The experimental data set is rather small. Nevertheless, the
predictions should be fairly reliable as long as the predicted
uncertainties do not exceed 0.5 MHz.
While in the laboratory b-type transitions have been
observed, their intensities are likely very small because
the b dipole moment component is about 1.5 orders
of magnitude smaller than the a component; hence,
transitions will be about three orders of magnitude weaker.
Hyperfine structure splitting caused by the 14N nucleus
or the 23Na nucleus are not of relevance for
astronomical observations.
The dipole moment was assumed to be the same as for the
main isotopic species, see e049510.cat.
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