A spin-polarized scheme for obtaining quasi-particle energies within the density functional theory

dc.creatorBarbiellini, B.
dc.creatorBansil, A.
dc.date2005-05-18
dc.date.accessioned2026-07-07T08:35:34Z
dc.date.available2026-07-07T08:35:34Z
dc.descriptionWe discuss an efficient scheme for obtaining spin-polarized quasi-particle excitation energies within the general framework of the density functional theory (DFT). Our approach is to correct the DFT eigenvalues via the electrostatic energy of a majority or minority spin electron resulting from its interaction with the associated exchange and correlation holes by using appropriate spin-resolved pair correlation functions. A version of the method for treating systems with localized orbitals, including the case of partially filled metallic bands, is considered. Illustrative results on Cu are presented.
dc.description6 pages, 3 figures, to appear in J. Phys. Chem. Solids
dc.identifierhttps://arxiv.org/abs/cond-mat/0505433
dc.identifierhttp://arxiv.org/abs/cond-mat/0505433
dc.identifierJ. Phys. Chem. Solids 66, 2192 (2005)
dc.identifierdoi:10.1016/j.jpcs.2005.09.014
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/139787
dc.subjectStrongly Correlated Electrons
dc.subjectMaterials Science
dc.titleA spin-polarized scheme for obtaining quasi-particle energies within the density functional theory
dc.typetext

Files

Collections