Abstract
Three-dimensional ion acoustic turbulence is excited by injecting a cold ion beam into a nonmagnetized plasma with . A rapid, approximately exponential heating of the ion beam is observed along the beam path. The heating rates level off when the ion temperature approaches . The turbulent ion acoustic wave energy density does not exceed . Wave saturation, which occurs before significant dissipation of ion beam energy, is consistent with orbit-diffusion strong-turbulence theory.
- Received 28 January 1972
DOI:https://doi.org/10.1103/PhysRevLett.29.34
©1972 American Physical Society