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 in | Plasma physics reports Vol. 41; no. 12; pp. 1002 - 1015 |
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Main Authors | , , , , , , , , , , , , , , , |
Format | Journal Article |
Language | English |
Published |
Moscow
Pleiades Publishing
01.12.2015
|
Subjects | |
Online Access | Get full text |
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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. |
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ISSN: | 1063-780X 1562-6938 |
DOI: | 10.1134/S1063780X1512003X |