The experimental lines were taken from
(1) M. C. McCarthy, E. S. Levine, A. J. Apponi, and P. Thaddeus,
2000, J. Mol. Spectrosc. 203, 75.
The number of transition frequencies is too small to determine
D reliably. Therefore, it was estimated from the main
isotopolog. The calculated frequencies should be viewed with
caution above 25 GHz.
Values for eQq and C were evaluated upon
comparison with experimental and quantum chemically derived
values of other HCxN molecules presented
in
(2) T. F. Giesen, M. E. Harding, J. Gauss, J.-U. Grabow,
and H. S. P. Müller,
2020, J. Mol. Spectrosc. 371, Art. No. 111303.
The 14N hyperfine splitting may be resolved in the ISM
at low values of J. Therefore, separate calculations with
14N hyperfine splitting are available for
J" < 10. The partition function takes into
account the hyperfine splitting, but no vibrational contributions !
The dipole moment was assumed to agree with that of the main
isotopic species calculated by
(3) P. Botschwina and M. Horn,
1997, J. Mol. Spectrosc. 185, 191.
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