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Position-dependent exact-exchange energy for slabs and semi-infinite jellium | C. M. Horowitz
; L. A. Constantin
; C. R. Proetto
; J. M. Pitarke
; | Date: |
6 Nov 2009 | Abstract: | The position-dependent exact-exchange energy per particle $varepsilon_x(z)$
(defined as the interaction between a given electron at $z$ 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 $varepsilon_{x}^{ ext{Slab}}(z o infty) o - e^{2}/2z$, {it
independent} of the bulk electron density, which is exactly half the
corresponding exact-exchange potential $V_{x}(z o infty) o - e^2/z$ [Phys.
Rev. Lett. {f 97}, 026802 (2006)] of density-functional theory, as occurs in
the case of finite systems. The fitting of $varepsilon_{x}^{ ext{Slab}}(z)$
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 $varepsilon_{x}^{ ext{SI}}(z)$ is somehow different.
As in the case of jellium slabs $varepsilon_{x}^{ ext{SI}}(z o infty)$ has
an image-like behavior of the form $propto - e^2/z$, 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
$varepsilon_{x}^{ ext{Slab}}(z)$ and $varepsilon_{x}^{ ext{SI}}(z)$ only
coincide in the low-density limit ($r_s o infty$), where the
density-dependent coefficient of the semi-infinite jellium approaches the slab
{it universal} coefficient 1/2. | Source: | arXiv, 0911.1338 | Services: | Forum | Review | PDF | Favorites |
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