Abstract
Steady-state electron currents were driven by fast waves with ${\ensuremath{\omega}}_{\mathrm{ci}}$\ensuremath{\ll}\ensuremath{\omega}\ensuremath{\ll}${\ensuremath{\omega}}_{\mathrm{ce}}$ in an initially current-free plasma in the Irvine Torus. Current direction was controlled by the fast-wave phased-array antenna. Low power experiments (l25 W) generated up to 1.3 A of electron current with a peak effeciency of \ensuremath{\eta}=InR/P\ensuremath{\simeq}(6\ifmmode\times\else\texttimes\fi{}${10}^{\mathrm{\ensuremath{-}}2}$ A/W)(${10}^{13}$ ${\mathrm{cm}}^{\mathrm{\ensuremath{-}}3}$)m. Up to 14% of the wave energy was converted to poloidal magnetic field energy.
Highlights
Steady-state electron currents were driven by fast waves with ~„&&ru
Current direction was controlled by the fast-wave phased
A of electron current with a 14% of the wave energy was converted to poloidal magnetic field energy
Summary
Steady-state electron currents were driven by fast waves with ~„&&ru && co„ in an initially current-free plasma in the Irvine Torus. S. In this Letter we report observations of steady-state electron currents driven in a plasma by a phased-array fast-wave antenna. The experiment was performed at a density above the "density limit" encountered by lower-hybrid current drive. — Recently, experimental results of fast-wave current rampup via toroidal eigenmode excitation (tu 10tu„) For both the slow and the fast waves there is an accessibility criterion which places an upper limit on the density to which the waves will propagate and a cutoff condition which places a lo~er limit on the density. Fast-wave coupling efficiency may be estimated by theory and compared with experiment by calculation of the impedance mismatch from the antenna to the plasma.
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