Characteristics of the three-half-turn-antenna-driven RF discharge in the Uragan-3M torsatron

In the ℓ = 3 Uragan-3M torsatron hydrogen plasma is produced by RF fields in the Alfvén range of frequencies (ω ≤ ω ci ). The initial (target) plasma with the line-averaged density of units 10 12 cm −3 is produced by a frame antenna with a broad spectrum of generated parallel wavenumbers. After this...

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Veröffentlicht in:Plasma physics reports 2015-12, Vol.41 (12), p.1002-1015
Hauptverfasser: Grigor’eva, L. I., Chechkin, V. V., Moiseenko, V. E., Grekov, D. L., Pavlichenko, R. O., Lozin, A. V., Tarasov, I. K., Kulaga, A. Ye, Zamanov, N. V., Tretiak, K. K., Kozulya, M. M., Beletskii, A. A., Kasilov, A. A., Mironov, Yu. K., Romanov, V. S., Voitsenya, V. S.
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Sprache:eng
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Zusammenfassung:In the ℓ = 3 Uragan-3M torsatron hydrogen plasma is produced by RF fields in the Alfvén range of frequencies (ω ≤ ω ci ). The initial (target) plasma with the line-averaged density of units 10 12 cm −3 is produced by a frame antenna with a broad spectrum of generated parallel wavenumbers. After this, to heat the plasma and bring its density to ~10 13 cm –3 , another, shorter wavelength three-half-turn antenna with large transverse currents is used. The behavior of the density, electron temperature, and loss of the plasma supported by the three-half-turn antenna is studied depending on the RF power fed to the antenna and initial values of the density and electron temperature supplied by the frame antenna.
ISSN:1063-780X
1562-6938
DOI:10.1134/S1063780X1512003X