Anderson impurity in a semiconductor

dc.creatorGalpin, Martin R.
dc.creatorLogan, David E.
dc.date2009-02-25
dc.date.accessioned2026-07-07T12:46:42Z
dc.date.available2026-07-07T12:46:42Z
dc.descriptionWe consider an Anderson impurity model in which the locally correlated orbital is coupled to a host with a gapped density of states. Single-particle dynamics are studied, within a perturbative framework that includes both explicit second-order perturbation theory and self-consistent perturbation theory to all orders in the interaction. Away from particle-hole symmetry the system is shown to be a generalized Fermi liquid (GFL) in the sense of being perturbatively connectable to the non-interacting limit; and the exact Friedel sum rule for the GFL phase is obtained. We show by contrast that the particle-hole symmetric point of the model is not perturbatively connected to the non-interacting limit, and as such is a non-Fermi liquid for all non-zero gaps. Our conclusions are in agreement with NRG studies of the problem.
dc.description7 pages, 4 figures
dc.identifierhttps://arxiv.org/abs/0902.4334
dc.identifierhttp://arxiv.org/abs/0902.4334
dc.identifierPhys. Rev. B 77, 195108 (2008)
dc.identifierdoi:10.1103/PhysRevB.77.195108
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/221473
dc.subjectStrongly Correlated Electrons
dc.titleAnderson impurity in a semiconductor
dc.typetext

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