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dc.contributor.authorTanatar, Bilalen_US
dc.date.accessioned2016-02-08T10:55:36Z
dc.date.available2016-02-08T10:55:36Z
dc.date.issued1992en_US
dc.identifier.issn1631829
dc.identifier.urihttp://hdl.handle.net/11693/26138
dc.description.abstractThe exchange-correlation potentials, fxc(q=0,), to be used in the local-density approximation to the density-functional theory for two-dimensional homogeneous electron liquids in the normal and fully spin-polarized phases are calculated. We make use of accurate Monte Carlo energies and sum rules in the local-field correction, G(q,), to construct fxc(q,) which is valid in the long-wavelength limit. Our results are qualitatively similar to the three-dimensional case. © 1992 The American Physical Society.en_US
dc.language.isoEnglishen_US
dc.source.titlePhysical Review Ben_US
dc.relation.isversionofhttp://dx.doi.org/10.1103/PhysRevB.46.1347en_US
dc.titleDynamic response of two-dimensional electron liquids in the local-density-functional theoryen_US
dc.typeArticleen_US
dc.departmentDepartment of Physicsen_US
dc.citation.spage1347en_US
dc.citation.epage1350en_US
dc.citation.volumeNumber46en_US
dc.citation.issueNumber3en_US
dc.identifier.doi10.1103/PhysRevB.46.1347en_US
dc.contributor.bilkentauthorTanatar, Bilal


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