Abstract
The temporal evolutions of the electron distribution function and the electric field in a dense, hot, multiply charged plasma due to the presence of a sharp temperature gradient from one side (plasma–cold matter contact) and a sharp density gradient from the other side (plasma-vacuum boundary) are studied. The prospects for x-ray lasing in such a plasma are discussed. The analogy with a p-n junction semiconductor laser is emphasized.
- Received 8 February 1994
DOI:https://doi.org/10.1103/PhysRevA.50.2691
©1994 American Physical Society