No data available.
Please log in to see this content.
You have no subscription access to this content.
No metrics data to plot.
The attempt to load metrics for this article has failed.
The attempt to plot a graph for these metrics has failed.
Pump absorption and saturation in the CH3F 496‐μm laser
1.T. Y. Chang and T. J. Bridges, Opt. Commun. 1, 423 (1970).
2.T. Y. Chang, IEEE Trans. Microwave Theory Tech. MTT‐22, 983 (1974).
3.D. E. Evans, L. E. Sharp, B. W. James, and W. A. Peebles, Appl. Phys. Lett. 26, 630 (1975).
4.F. Brown, S. R. Horman, and A. Palevsky, Opt. Commun. 9, 28 (1973).
5.T. Y. Chang and J. D. McGee, Appl. Phys. Lett. 19, 103 (1971).
6.H. C. Allen, Jr. and P. C. Cross, Molecular Vib‐Rotors (Wiley, New York, 1963), p. 103.
7.S. M. Freund, G. Duxbury, M. Romheld, J. T. Tiedje, and T. Oka, J. Mol. Spectrosc. 52, 38 (1974).
8.J. R. Tucker, Conference Digest, International Conference on Submillimeter Waves and Their Applications, Atlanta, Ga., 1974 (IEEE, New York, 1974), Cat. No. 74. CHO 856‐5MTT, p. 17. The complete expression for the absorption coefficient contains the additional term in the denominator of Eq. (1), where is the Doppler line shape. Estimating the diffusion rate as the numerical value of this term under conditions of the present experiment is expected to be which is negligible at the intensities and pressures in Fig. 2. The reverse situation, in which the above diffusion term dominates and the absorption becomes proportional to Г; and pressure independent, has been observed in larger‐diameter beams and reported in Ref. 9.
9.D. T. Hodges, J. R. Tucker, and T. S. Hartwick, Proceedings of the International Conference on Infrared Physics, Zurich, 1975 [Infrared Phys. (to be published)].
10.G. Birnbaum, E. R. Cohen, and J. R. Rusk, J. Chem. Phys. 44, 5150 (1968).
11.R. G. Brewer and R. L. Schoemaker, Phys. Rev. Lett. 27, 631 (1971).
Article metrics loading...
Full text loading...
Most read this month
Most cited this month