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Kinetic processes in the electrically excited mercuric‐bromide dissociation laser
1.E. J. Schimitschek and J. E. Celto, Opt. Lett. 2, 64 (1978);
1.Appl. Phys. Lett. 36, (1980) (to be published).
2.R. Burnham, Appl. Phys. Lett. 33, 156 (1978).
3.R. S. F. Chang and R. Burnham (unpublished).
4.J. Allison and R. N. Zare, Chem. Phys. 35, 263 (1978).
5.K. Wieland, Z. Phys. 77, 157 (1932);
5.W. R. Wadt, J. Chem. Phys. (to be published).
6.H. H. Michels (private communication).
7.For the purpose of the present analysis, the ionization cross section for has been assumed to increase from threshold at 10.6 eV to a peak value of in the 50‐100‐eV range. The rate coefficient for dissociative attachment of was taken as The results presented in Figs. 2 and 3 were found to be relatively insensitive to variations in the ionization and attachment rate coefficients.
8.R. T. Brown and W. L. Nighan, Appl. Phys. Lett. 32, 730 (1978).
9.In this analysis an effective electron‐ion recombination coefficient of was used for along with a value of for the reaction as recently computed by M. R. Flannery (private communication).
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