dc conductivity as a geometric phase

dc.citation.epage235123-6en_US
dc.citation.issueNumber23en_US
dc.citation.spage235123-1en_US
dc.citation.volumeNumber87en_US
dc.contributor.authorHetényi, B.en_US
dc.date.accessioned2016-02-08T09:38:09Z
dc.date.available2016-02-08T09:38:09Z
dc.date.issued2013en_US
dc.departmentDepartment of Physicsen_US
dc.description.abstractThe zero-frequency conductivity (Dc), the criterion to distinguish between conductors and insulators, is expressed in terms of a geometric phase. Dc is also expressed using the formalism of the modern theory of polarization. The tenet of Kohn, namely that insulation is due to localization in the many-body space, is refined as follows. Wave functions, which are eigenfunctions of the total current operator, give rise to a finite Dc and are therefore metallic. They are also delocalized. Based on the value of Dc it is also possible to distinguish purely metallic states from states in which the metallic and insulating phases coexist. Several examples which corroborate the results are presented, as well as a numerical implementation. The formalism is also applied to the Hall conductance, and the quantization condition for zero Hall conductance is derived to be eΦBNhc=QM, with Q and M as integers.en_US
dc.identifier.doi10.1103/PhysRevB.87.235123en_US
dc.identifier.issn1098-0121
dc.identifier.urihttp://hdl.handle.net/11693/20928
dc.language.isoEnglishen_US
dc.publisherAmerican Physical Societyen_US
dc.relation.isversionofhttp://dx.doi.org/10.1103/PhysRevB.87.235123en_US
dc.source.titlePhysical Review B - Condensed Matter and Materials Physicsen_US
dc.titledc conductivity as a geometric phaseen_US
dc.typeArticleen_US

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