dc.contributor.author | Horowitz, Claudio M. | |
dc.contributor.author | Constantin, Lucian A. | |
dc.contributor.author | Proetto, C. R. | |
dc.contributor.author | Pitarke de la Torre, José María | |
dc.date.accessioned | 2011-05-27T16:39:14Z | |
dc.date.available | 2011-05-27T16:39:14Z | |
dc.date.issued | 2009-12 | |
dc.identifier.citation | Physical Review B 80(23) : (2009) // Article 235101 | es |
dc.identifier.issn | 1098-0121 | |
dc.identifier.uri | http://hdl.handle.net/10810/2648 | |
dc.description | 26 p., 7 figuras | es |
dc.description.abstract | The position-dependent exact-exchange energy per particle epsilon(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 epsilon(Slab)(x)(z ->infinity)->-e(2)/2z, independent of the bulk electron density, which is exactly half the corresponding exact-exchange potential V-x(z ->infinity)->-e(2)/z [Horowitz , Phys. Rev. Lett. 97, 026802 (2006)] of density-functional theory, as occurs in the case of finite systems. The fitting of epsilon(Slab)(x)(z) to a physically motivated imagelike 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 epsilon(SI)(x)(z) is somehow different. As in the case of jellium slabs epsilon(SI)(x)(z ->infinity) has an imagelike behavior of the form proportional to-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 epsilon(Slab)(x)(z) and epsilon(SI)(x)(z) only coincide in the low-density limit (r(s)->infinity), where the density-dependent coefficient of the semi-infinite jellium approaches the slab-universal coefficient 1/2. | es |
dc.description.sponsorship | Support received from CONICET of Argentina. C. R. P. was supported by the European Community through a Marie Curie IIF (Grant No. MIF1-CT-2006-040222) and CONICET of Argentina under Grant No. PIP 5254. J.M.P. acknowledges partial support by the University of the Basque Country, the Basque Unibertsitate eta Ikerketa Saila, and the Spanish Ministerio de Educacion y Ciencia (Grants No. FIS200601343 and No. CSD2006-53). | es |
dc.language.iso | eng | es |
dc.publisher | American Physical Society | es |
dc.relation | info:eu-repo/grantAgreement/MICINN/FIS2006-01343 | |
dc.relation | info:eu-repo/grantAgreement/MICINN/CSD2006-53 | |
dc.rights | info:eu-repo/semantics/openAccess | es |
dc.subject | density functional theory | es |
dc.subject | electron density | es |
dc.subject | jellium | es |
dc.subject | slabs | es |
dc.subject | surface states | es |
dc.title | Position-dependent exact-exchange energy for slabs and semi-infinite jellium | es |
dc.type | info:eu-repo/semantics/preprint | es |
dc.rights.holder | © 2009 The American Physical Society | es |
dc.relation.publisherversion | http://link.aps.org/doi/10.1103/PhysRevB.80.235101 | es |
dc.identifier.doi | 10.1103/PhysRevB.80.235101 | |
dc.departamentoes | Física de la materia condensada | es_ES |
dc.departamentoeu | Materia kondentsatuaren fisika | es_ES |
dc.subject.categoria | ELECTRONIC, OPTICAL AND MAGNETIC MATERIALS | |
dc.subject.categoria | PHYSICS, CONDENSED MATTER | |