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dc.contributor.authorWitek, Henryk A.en_US
dc.contributor.authorKoehler, Christofen_US
dc.contributor.authorFrauenheim, Thomasen_US
dc.contributor.authorMorokuma, Keijien_US
dc.contributor.authorElstner, Marcusen_US
dc.date.accessioned2014-12-08T15:05:51Z-
dc.date.available2014-12-08T15:05:51Z-
dc.date.issued2007-07-05en_US
dc.identifier.issn1089-5639en_US
dc.identifier.urihttp://dx.doi.org/10.1021/jp070786oen_US
dc.identifier.urihttp://hdl.handle.net/11536/4374-
dc.description.abstractA detailed treatment of a confined relativistic atom, needed as an initial step for the parametrization of the self-consistent-charge density-functional tight-binding method, is presented and discussed. The required one-component quantities, i.e., orbital energies, orbital wave functions, and Hubbard parameters, are obtained by weighted averaging of the corresponding numbers determined for the atomic spinors. The wave function and density confinement is achieved by introducing the Woods-Saxon potential in the atomic four-component Dirac-Kohn-Sham problem. The effect of the additional confining potential on energy eigenvalues and the shape of atomic wave functions and densities is discussed and numerical examples are presented for the valence spinors of carbon, germanium, and lead.en_US
dc.language.isoen_USen_US
dc.titleRelativistic parametrization of the self-consistent-charge density-functional tight-binding method. 1. Atomic wave functions and energiesen_US
dc.typeArticle; Proceedings Paperen_US
dc.identifier.doi10.1021/jp070786oen_US
dc.identifier.journalJOURNAL OF PHYSICAL CHEMISTRY Aen_US
dc.citation.volume111en_US
dc.citation.issue26en_US
dc.citation.spage5712en_US
dc.citation.epage5719en_US
dc.contributor.department應用化學系分子科學碩博班zh_TW
dc.contributor.departmentInstitute of Molecular scienceen_US
dc.identifier.wosnumberWOS:000247573600016-
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