NCHCCO
Cyanoethenone, cyanoketene
Species tag 067502
Version2*
Date of EntryJune 2020
ContributorH. S. P. Müller

Extensive experimental laboratory frequencies up to 40 GHz, hyperfine parameters, and the dipole moment were reported in
(1) M. Hahn, H.-K. Bodenseh, and M. Ferner, 2004, J. Mol. Spectrosc. 223, 138.
With respect to the first entry from June 2006, additional data, largely in the millimeter region, were included from
(2) L. Margulès, B. A. McGuire, R. A. Motiyenko, C. Brogan, T. Hunter, A. Remijan, and J.-C. Guillemin, 2020, Astron. Astrophys. 637, Art. No. A81.
The calculations should be sufficient for all observational purposes. Caution is advised for transitions having calculated uncertainties in excess of 0.2 MHz. The 14N hyperfine splitting may be resolvable at lower frequencies or at lower quantum numbers. Therefore, a separate calculation with hyperfine structure is available up to 188 GHz and with J up to 5. The spin-multiplicity of the 14N nucleus was considered in the calculation of the partition function.

Lines Listed14690
Frequency / GHz< 720
Max. J136
log STR0-9.0
log STR1-5.3
Isotope Corr.-0.0
Egy / cm–10.0
 µa / D2.844
 µb / D2.110
 µc / D 
 A / MHz29601.18
 B / MHz2812.149
 C / MHz2563.722
 Q(300.0)181926.2899
 Q(225.0)117882.8472
 Q(150.0)64000.8171
 Q(75.00)22568.1438
 Q(37.50)7971.2583
 Q(18.75)2819.1640
 Q(9.375)998.5223
 Q(5.000)390.3433
 Q(2.725)158.1246
detected in ISM/CSMno


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