52CrN
Chromium mononitride, X 4Σ
Species tag 066511
Version1*
Date of EntryMar. 2019
ContributorH. S. P. Müller

Transition frequencies without hyperfine structure splitting were taken from
(1) P. M. Sheridan, M. A. Brewster, L. M. Ziurys, 2002, Astrophys. J. 576, 1108.
Transition frequencies with hyperfine structure splitting were taken from
(2) K. C. Namiki and T. C. Steimle, 1999, J. Chem. Phys. 111, 6385.
The partition function does not take into account vibrational corrections but takes into accout the HFS splitting. The predictions should be sufficiently accurate for observational purposes. Some caution is advised for frequencies with calculated uncertainties exceeding 0.2 MHz.
14N hyperfine splitting may be resolved for low values of J. Therefore, a separate hyperfine calculation is provided for frequencies below 215 GHz.
The dipole moment was determined by
(3) T. C. Steimle, J. S. Robinson, D. Goodridge, 1999, J. Chem. Phys. 110, 881.

Lines Listed150
Frequency / GHz< 1000
Max. J28
log STR0-5.7
log STR1-4.0
Isotope Corr.-0.0778
Egy / cm–10.0
 µa / D2.31
 µb / D 
 µc / D 
 A / MHz 
 B / MHz18702.90
 C / MHz 
 Q(300.0)3944.2956
 Q(225.0)2940.2507
 Q(150.0)1937.3795
 Q(75.00)937.3600
 Q(37.50)442.1794
 Q(18.75)202.0658
 Q(9.375)91.7261
detected in ISM/CSMno


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