Abstract

A temporal wave packet of frequency ω0(ωci, ωpi≪ω0≪ωce, ωpe) applied to a finite antenna in a magnetically confined plasma, is shown to excite an electrostatic field consisting of (1) a short-duration resonance cone and (2) a wave-like disturbance which follows afterward. This latter disturbance, which is related to the lower frequency mode of the delta-function induced transients discussed by Simonutti, persists long after the resonance cone. The phase factor associated with the disturbance is independent of ω0, and its constant-phase surfaces are lines which emanate from the antenna and make a small angle ϑ with respect to the confining magnetic field B. ϑ decreases with increasing time so that ’’wavelengths’’ perpendicular to B also decrease with increasing time. The correspondence of the fields obtained by wave-packet excitation to those obtained by both cw and delta-function excitations is discussed and experimental results are reported.

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