D13CN
Deuterium Cyanide, 13C isotopic species
Species tag 029510
Version1*
Date of EntryApr. 2006
ContributorsH. S. P. Müller
S. Brünken

The observed transitions have been summarized in
(1) S. Brünken, U. Fuchs, F. Lewen, S. Urban, T. Giesen, and G. Winnewisser, 2004, J. Mol. Spectrosc., 225, 152.
The v = 0 and v2 = 1 state data have been fit together along with ν2 infrared data from
(2) E. Möllmann, A. G. Maki, M. Winnewisser, B. P. Winnewisser, and W. Quapp, 2002, J. Mol. Spectrosc. 212, 22.
The dipole moment was assumed to agree with that of DCN, see e028509.cat.
The 14N hyperfine splitting can be resolved for low values of J. Therefore, a separate hyperfine calculation is provided for J" ≤ 6. The spin multiplicity gI of 3 for the 14N nucleus is included in the partition function.
The partition function takes into account both vibrational states. Contributions of vibrational states to the partition function are given in parentheses.

Lines Listed64
Frequency / GHz< 4498
Max. J64
log STR0-10.0
log STR1-10.0
Isotope Corr.-5.915
Egy / (cm–1)0.0
 µa / D2.9908
 µb / D 
 µc / D 
 A 
 B35587.646
 C 
 Q(500.0)1227.6777 (880.0554, 347.6223)
 Q(300.0)599.1599 (528.2407, 70.9191)
 Q(225.0)418.0283 (396.3769, 21.6514)
 Q(150.0)266.9418 (264.5497, 2.3921)
 Q(75.00)132.7656 (132.7602, 0.0054)
 Q(37.50)66.8825 (66.8825)
 Q(18.75)33.9541 (33.9541)
 Q(9.375)17.5052 (17.5052)
detected in ISM/CSMno


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