Abstract
An explicit expression for the quadratic density-response function of a many-electron system is obtained in the framework of the time-dependent density-functional theory, in terms of the linear and quadratic density-response functions of noninteracting Kohn-Sham electrons and functional derivatives of the time-dependent exchange-correlation potential. This is used to evaluate the quadratic stopping power of a homogeneous electron gas for slow ions, which is demonstrated to be equivalent to that obtained up to second order in the ion charge in the framework of a fully nonlinear scattering approach. Numerical calculations are reported, thereby exploring the range of validity of quadratic-response theory.
| Original language | English |
|---|---|
| Pages (from-to) | 8621-8631 |
| Number of pages | 11 |
| Journal | Journal of Physics Condensed Matter |
| Volume | 16 |
| Issue number | 47 |
| DOIs | |
| State | Published - 1 Dec 2004 |
| Externally published | Yes |
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