This is a combined CDMS/JPL catalog entry.
The data have been summarized in
(1) B. J. Drouin, S. Yu, C. E. Miller, H. S. P.
Müller, F. Lewen, S. Brünken, and H. Habara,
2010, J. Quant. Spectrosc. Radiat. Transfer
111, 1167.
This work provides new data between 0.42 and
1.88 THz. Additional submmW data were
taken from
(2) L. R. Zink and M. Mizushima,
1987, J. Mol. Spectrosc. 125, 154;
from
(3) K. Park, I. G. Nolt, T. C. Steele, L. R. Zink,
K. M. Evenson, K. V. Chance, and A. G. Murray,
1996, J. Quant. Spectrosc. Radiat. Transfer
56, 315;
and from
(4) G. Y. Golbyatnikov and A. F. Krupnov,
2003, J. Mol. Spectrosc. 217, 282.
The mmW data were taken from
(5) J. S. Knight and W. Gordy,
1968, Phys. Rev. Lett. 21, 1787;
from
(6) Y. Endo and M. Mizushima,
1982, Jpn. J. Appl. Phys. 21, L379;
and from
(7) M. Y. Tretyakov, M. A. Koshelev, V. V. Dorovskikh,
D. S. Makarov, and P. W. Rosenkranz,
2005, J. Mol. Spectrosc. 231, 1.
For multiply measured transitions differing in
uncertainties by less than a factor of 2
weighted averaged have been derived.
Predictions should be viewed with caution above 4 THz.
Intensities were calculated based on g values
obtained by magnetic resonance in
(8) K. D. Bowers, R. A. Kamper, and C. D. Lustig,
1959, Proc. Roy. Soc. London, A251, 565.
