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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Published inPlasma physics reports Vol. 41; no. 12; pp. 1002 - 1015
Main Authors 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.
Format Journal Article
LanguageEnglish
Published Moscow Pleiades Publishing 01.12.2015
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Summary: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