- Autor(in)
- Referenz
-
10 Shkarofsky, I. P., Proc. IRE 49 (1961) 1857.
11 Borgnis, F. E., u. C. H. Papas, Randwertprobleme der Mikrowellenphysik, Berlin/Göttingen/Heidelberg 1955.
12 Müller, C., Grundprobleme der mathematischen Theorie elektromagnetischer Schwingungen. Berlin/Göttingen/Heidelberg 1957.
13 Müller, C., u. H. Niemeyer, Arch. Rat. Mech. Analys. 7 (1961) 305.
14 Goubau, G., Elektromagnetische Wellenleiter und Hohlr äume. Stuttgart 1955. Der Abschnitt über Hohlraumresonatoren stammt von R. MÜLLER.
15 Stratton, J. A., u. L. J. Chu, Phys. Rev. 56 (1939) 99.
16 Bracewell, R. N., Hbd. d. Phys. Bd. 54, p. 42. Berlin/Göttingen/Heidelberg 1962.
17 Fields, H., G. Bekefi, u. S. C. Brown, Phys. Rev. 129 (1963) 506.
18 Jelley, J. V., Proc. IEEE 51 (1963) 30.
19 Hamilton, D. R., J. K. Knipp, u. J. B. H. Kuper, Klystrons and Microwave Triodes. New York/Toronto/London 1948.
1 Allis, W. P., Hdb. d. Phys. Bd. 21, p. 383, Berlin/Göttingen/Heidelberg 1956.
2 Allis, W. P., S. J. Buchsbaum u. A. BERS, Waves in Anisotropic Plasma, Cambridge, Mass. 1963.
3 Ginzburg, V. L., u. A. V. Gurevic, Fortschr. d. Phys. 8 (1960) 97.
4 Ginzburg, V. L., Propagation of Elektromagnetic Waves in plasma, New York/Amsterdam o. J.
5 Stewart, G. E., u. Z. A. Kapriellan, Proc. V. Int. Conf. on Ioniz. Phen. in Gases 1961, Bd. 1, p. 395.
6 Gerstenkorn, H., Z. Physik 162 (1961) 363.
7 Thompson, W. B., An Introduction to Plasma Physics, Oxford/London/New York/Paris 1962.
8 v. Ardenne, M., Tabellen zur angewandten Physik, Bd. 2, Berlin 1964.
9 Crawford, F. W., u. G. S. Kino, Proc. IRE 49 (1961) 1767.
- Seitenbereich
-
0007 - 0032
- Zusammenfsg.
-
If a microwave cavity containing an anisotropic, inhomogeneous plasma is excited with a nonresonant frequency ω, the electron density distribution inside the plasma can be obtained from a knowledge of the tangential electrical field on a surface enclosing the plasma. The main step is the derivation of an integralequation relating the tangential field to the highfrequency plasma current. An experimental setup is discussed. The obtainable precision is limited by the noise like density fluctuations in the plasma itself and is about 1% for \documentclass{article}\pagestyle{empty}\begin{document}$\frac{{\delta N}}{{\bar N}}$\end{document} for a spatial resolution in the same order of magnitude.
- Artikel-Typen
- Forschungsartikel