Abstract
The theory and first nonlinear simulations of the Rayleigh-Taylor instability in the limit of large ion Larmor radius are presented. It is shown that in the limit of large Larmor radius, the Rayleigh-Taylor instability evolves much faster and in a dramatically different manner than in the limit of small Larmor radius.
- Received 15 June 1987
DOI:https://doi.org/10.1103/PhysRevLett.59.2971
©1987 American Physical Society