Hostname: page-component-848d4c4894-x24gv Total loading time: 0 Render date: 2024-05-09T08:38:00.327Z Has data issue: false hasContentIssue false

Kinetic theory of the high-frequency part of the slow electromagnetic mode in weakly ionized gas-discharge argon plasma with inelastic collisions

Published online by Cambridge University Press:  13 March 2009

V. J. Žigman
Affiliation:
Institute of Physics, Faculty of Natural and Mathematical Sciences, Belgrade, Yugoslavia
B. S. Milić
Affiliation:
Institute of Physics, Faculty of Natural and Mathematical Sciences, Belgrade, Yugoslavia

Abstract

The spectral characteristics of the high-frequency part of the slow electromagnetic mode, specific for plasmas placed in an external d.c. electric field, as well as the features of the corresponding instability, are analysed for weakly ionized argon gas-discharge plasmas with E/n ranging from 25 to 150 Td, and with electron temperatures between 60000 and 70000 K. The analysis is based on the linear theory of perturbation, and the dynamics of the electrons is described by appropriately modified kinetic equations for the one-particle distribution function. Attention is focused on the collisional processes between electrons and neutrals, and both elastic and excitational collisions are taken into account. Apart from the ‘indirect’ collision effects (modifications of the form of the electron steady-state distribution function, evaluated here analytically, with the thermal motion of the neutrals included), their ‘direct’ influence (arising from perturbations of the collision integrals) is also significant in the electron temperature range considered. As a consequence of the ‘direct’ influence of inelastic collisions, in particular, the mode studied was found to exist in two distinctly separate wavelength ranges. The instability was found to develop only in the one corresponding to shorter wavelengths (below some 30 cm).

Type
Research Article
Copyright
Copyright © Cambridge University Press 1987

Access options

Get access to the full version of this content by using one of the access options below. (Log in options will check for institutional or personal access. Content may require purchase if you do not have access.)

References

REFERENCES

Braglia, L., Wilhelm, J. & Winkler, R. 1985 Lett. Nuovo Cimento, 44, 365.CrossRefGoogle Scholar
Chutjian, A. & Cartwright, D. C. 1981 Phys. Rev. A, 23, 2178.CrossRefGoogle Scholar
Dias, T. H. V. T., Stauffer, A. D. & Conde, C. A. N. 1986 J. Phys. D, 19, 527.CrossRefGoogle Scholar
Golant, V. E. 1957 Zhurn. Tekhn. Fiz. (USSR), 27, 756.Google Scholar
Huxley, L. G. H. & Crompton, R. W. 1974 The Diffusion and Drift of Electrons in Gases. Wiley - Interscience.Google Scholar
Makabe, T. & Mori, T. 1980 J. Phys. D, 13, 387.CrossRefGoogle Scholar
Makabe, T. & Mori, T. 1982 J. Phys. D, 15, 1395.CrossRefGoogle Scholar
McDaniel, E. W. 1964 Collision Phenomena in Ionized Gases. Wiley.Google Scholar
McEachran, R. P. & Stauffer, A. D. 1983 J. Phys. B, 16, 4023.CrossRefGoogle Scholar
Milić, B. S. 1968 Fizika, 1, 59.Google Scholar
Milić, B. S. & Rukhadze, A. A. 1968 Zhurn. Tekhn. Fiz. (USSR), 38, 229.Google Scholar
Milloy, H. B., Crompton, R. W., Rees, J. A. & Robertson, A. G. 1977 Aust. J. Phys. 30, 61.CrossRefGoogle Scholar
Padial, N. T., Meneses, G. D., Da Paixão, F. J., Csanak, Gy. & Cartwright, D. C. 1981 Phys. Rev. A, 23, 2194.CrossRefGoogle Scholar
Silin, V. P. & Rukhadze, A. A. 1961 Electromagnetic Properties of Plasmas and Plasma-Like Media. Gosatomizdat (in Russian).Google Scholar
Smits, R. M. M. 1977 Ph.D. Thesis, Eindhoven.Google Scholar
Srivastava, S. K., Tanaka, H., Chutjian, A. & Trajmar, S. 1981 Phys. Rev. A, 23, 2156.CrossRefGoogle Scholar
Williams, J. F. 1979 J. Phys. B, 12, 265.Google Scholar
Žigman, V. J. & Milić, B. S. 1980 J. Plasma Phys. 24, 503.CrossRefGoogle Scholar
Žigman, V. J. & Milić, B. S. 1982 J. Plasma Phys. 28, 177.CrossRefGoogle Scholar
Žigman, V. J. & Milić, B. S. 1984 J. Plasma Phys. 34, 359.CrossRefGoogle Scholar