Abstract :
Summary form only given. Observations of growth and nonlinear saturation of highly oblique ion-acoustic waves near the lower hybrid frequency are reported. The waves are driven unstable by the electron diamagnetic drift in a linear, pulsed discharge plasma column (1-m diam., 2-m length, ne≃1012 cm-3 , kTe≃2 eV) immersed in a weak axial DC magnetic field (Bo=10 G). The ions (Ar) are essentially unmagnetized. while the electrons undergo a diamagnetic drift due to radial pressure gradients. When the diamagnetic drift exceeds the sound speed, low-frequency fluctuations grow in the region of steep density gradients. The frequency is below but near the lower hybrid frequency, the waves propagate at νphase≃kTe/mi 12≃2×105 cm/s<νdia initially along the azimuthal diamagnetic drift. As they grow to large amplitudes, the wave fronts steepen into electrostatic shocks, and the direction of wave propagation bends toward the radial direction. While steepening is understood as a nonlinear feature of sound waves, the new self-refraction effect is thought to arise from the diamagnetic drift, which is modified by the large amplitude wave itself. The wave refracts so as to reduce the local drift velocity whereby it saturates
Keywords :
discharges (electric); fluctuations; plasma shock waves; plasma turbulence; plasma waves; 1 m; 10 G; 2 m; Ar; DC magnetic field; azimuthal diamagnetic drift; density gradients; diamagnetic drift; electron diamagnetic drift; electrostatic shocks; growth; highly oblique ion-acoustic waves; local drift velocity; low-frequency fluctuations; lower hybrid frequency; nonlinear saturation; pressure-driven low frequency turbulence; pulsed discharge plasma column; radial direction; radial pressure gradients; self-refraction effect; sound speed; steepening; wave fronts; wave propagation;