Abstract
The coefficient of the von Weizsäcker term in the Thomas–Fermi–von Weizsäcker energy functional is determined within a perturbation framework for high-temperature plasmas. A notable deviation in comparison to the corresponding zero-temperature result is found.
- Received 25 February 1991
DOI:https://doi.org/10.1103/PhysRevA.43.7077
©1991 American Physical Society
