C3N, v5 = 1
Cyanoethynyl, v5 = 1, 2Πi
Species tag 050512
Version1
Date of EntryDec. 2003
ContributorH. S. P. Müller

The experimental lines have been taken from
(1) H. Mikami, S. Yamamoto, S. Saito, and M. Guélin, 1989, Astron. Astrophys. 217, L5.
14N hyperfine splitting was not resolved in these measurements. However, it may be resolvable at lower values of N both in the laboratory and in the ISM. The spin-multiplicity 3 of 14N was considered in the calculation of the partition function in order to be consistent with calculations for the ground vibrational state,
According to ab initio calculation in
(2) M. C. McCarthy, C. A. Gottlieb, P. Thaddeus, M. Horn, and P. Botschwina, 1995, J. Chem. Phys. 103, 7820,
the v5 = 1 lowest vibrational state is located at about 150 cm–1.
Individual contributions of v = 0 and v5 = 1 to the partition function are given in parentheses. Since the vibrational energy of v5 = 1 is only an estimate, these contributions should be viewed with some caution !
The dipole moment was assumed to be identical to that of the ground vibrational state, see e050511.cat.

Lines Listed558
Frequency / GHz< 982
Max. J99
log STR0-12.0
log STR1-5.5
Isotope Corr.-0.0
Egy / (cm-1)ca. 150
 µa / D2.85
 µb / D 
 µc / D 
 A / MHz 
 B / MHz4967.56
 C / MHz 
 Q(300.0)14945.4583 (7585.4957; 7359.9626)
 Q(225.0)10032.1148 (5689.0749; 4343.0399)
 Q(150.0)5585.5305 (3793.0189; 1792.5116)
 Q(75.00)2110.0444 (1897.3279; 212.7165)
 Q(37.50)955.6120 (949.6199; 5.9921)
 Q(18.75)475.8115 (475.8020; 0.0095)
 Q(9.375)238.9055 (238.9055; 0.0)
detected in ISM/CSMno


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