Position-dependent exact-exchange energy for slabs and semi-infinite jellium
arXiv:0911.1338 · doi:10.1103/PhysRevB.80.235101
Abstract
The position-dependent exact-exchange energy per particle (defined as the interaction between a given electron at and its exact-exchange hole) at metal surfaces is investigated, by using either jellium slabs or the semi-infinite (SI) jellium model. For jellium slabs, we prove analytically and numerically that in the vacuum region far away from the surface , {\it independent} of the bulk electron density, which is exactly half the corresponding exact-exchange potential [Phys. Rev. Lett. {\bf 97}, 026802 (2006)] of density-functional theory, as occurs in the case of finite systems. The fitting of to a physically motivated image-like expression is feasible, but the resulting location of the image plane shows strong finite-size oscillations every time a slab discrete energy level becomes occupied. For a semi-infinite jellium, the asymptotic behavior of is somehow different. As in the case of jellium slabs has an image-like behavior of the form , but now with a density-dependent coefficient that in general differs from the slab universal coefficient 1/2. Our numerical estimates for this coefficient agree with two previous analytical estimates for the same. For an arbitrary finite thickness of a jellium slab, we find that the asymptotic limits of and only coincide in the low-density limit (), where the density-dependent coefficient of the semi-infinite jellium approaches the slab {\it universal} coefficient 1/2.
26 pages, 7 figures, to appear in Phys. Rev. B
References in corpus (4)
Cited by in corpus (8)
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