Please use this identifier to cite or link to this item: http://hdl.handle.net/2289/1211
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dc.contributor.authorDhar, Abhishek-
dc.contributor.authorSen, Diptiman-
dc.date.accessioned2006-05-12T10:50:56Z-
dc.date.available2006-05-12T10:50:56Z-
dc.date.issued2006-02-28-
dc.identifier.citationPhysical Review B, 2006, Vol.73, 085119en
dc.identifier.issn1098-0121-
dc.identifier.issn1550-235X (online)-
dc.identifier.urihttp://hdl.handle.net/2289/1211-
dc.description.abstractThe nonequilibrium Green's function formalism for infinitely extended reservoirs coupled to a finite system can be derived by solving the equations of motion for a tight-binding Hamiltonian. While this approach gives the correct density for the continuum states, we find that it does not lead, in the absence of any additional mechanisms for equilibration, to a unique expression for the density matrix of any bound states which may be present. Introducing some auxiliary reservoirs which are very weakly coupled to the system leads to a density matrix which is unique in the equilibrium situation, but which depends on the details of the auxiliary reservoirs in the nonequilibrium case.en
dc.format.extent440644 bytes-
dc.format.mimetypeapplication/pdf-
dc.language.isoenen
dc.publisherThe American Physical Societyen
dc.relation.urihttp://link.aps.org/abstract/PRB/v73/e085119en
dc.relation.urihttp://arxiv.org/abs/cond-mat/0510303-
dc.rights(2006) by the American Physical Societyen
dc.titleNonequilibrium Green's function formalism and the problem of bound statesen
dc.typeArticleen
Appears in Collections:Research Papers (TP)

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