The calculational method is described in
(1) T. Amano and E. Hirota,
1974, J. Mol. Spectrosc. 53, 346.
The lines are taken from
(2) E. Tiemann, 1982, J. Mol. Spectrosc. 91, 60,
(3) M. Bogey, C. Demuynck, J. L. Destombes,
1982, Chem. Phys. 66, 99,
(4) Th. Klaus, A. H. Saleck, S. P. Belov, G. Winnewisser, Y. Hirahara,
M. Hayashi, E. Kagi, and K. Kawaguchi,
1996, J. Mol. Spectrosc. 180, 197,
(5) M. Bogey, S. Civis, B. Delcroix, C. Demuynck, A. F. Krupnov,
J. Quiguer, M. Yu. Tretyakov, and A. Walters,
1997, J. Mol. Spectrosc. 182, 85,
(6) N. Hansen, U. Andresen, H. Dreizler, J.-U. Grabow,
H. Mäder, and F. Temps,
1998, Chem. Phys. Lett. 289, 311.
Both electric and magnetic dipole transitions are listed in the catalog.
The dipole moments were assumed to be the same as for the ground
vibrational state, see e048501.cat. This state is
1111.5 cm1 above v = 0
((7) G. Herzberg,
1950, Spectra of Diatomic Molecules, Van Nostrands, New York).
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