Abstract
The velocity dependence of the stopping power of a two-dimensional noninteracting electron gas for heavy in-plane ions is calculated. The transport cross section required in the kinetic treatment is determined for a bare Coulomb potential. Detailed analytical and illustrative numerical results are derived. The problem of screening is also discussed.
- Received 28 April 1994
DOI:https://doi.org/10.1103/PhysRevB.51.77
©1995 American Physical Society
