By S. M. George (auth.), Professor Dr. Michael Grunze, Dr. Jeffrey J. Weimer, Professor Dr. Hans Jürgen Kreuzer (eds.)

Diffusion in solids and at interfaces is a really lively region of analysis, because the contributions to this quantity attest.

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Additional resources for Diffusion at Interfaces: Microscopic Concepts: Proceedings of a Workshop, Campobello Island, Canada, August 18–22, 1987

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The weighting function is the electrostatic potential ~a of the adatom. This theory was applied successfully to rare gas atomsinsulator systems [11,28]. o in [6] has been est~ated to be about 42 ev - A3 [11,29]. Our charge density per) is obtained by adding contributions from individual ions: ... p (r) = ... E Pi (r - r i) (7) i where P i (~ - ~ i) is t~ken to be the crystal charge density of the ith ion at position ri' [30]. i\r) = Pioe-Bir. 70A- 1 foro 2 and Mg2+, respectively. The third term in Eq.

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