A partially ionized helium plasma (nₑ=5×10¹³ cm^-3) was heated by an intense (νγ1) relativistic electron beam (600 keV, 25-60 kA). Observations of the emitted line radiation and Thomson-scattered light indicate noncollisional electron heating rates consistent with electron-ion instability predictions, and total energy deposition consistent with electron-electron- instability saturation levels.
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Goldenbaum et al. (1974) studied this question.
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