Phases of Mott-Hubbard bilayers

dc.creatorHan, Jung Hoon
dc.creatorJia, Chenglong
dc.date2006-05-17
dc.date.accessioned2026-07-07T07:09:00Z
dc.date.available2026-07-07T07:09:00Z
dc.descriptionA phase diagram of two Mott-Hubbard planes interacting with a short-range Coulomb repulsion is presented. Considering the case of equal amount of doping by holes in one layer as electrons in the other, a holon-doublon inter-layer exciton formation is shown to be a natural consequence of Coulomb attraction. Quasiparticle spectrum is gapped and incoherent below a critical doping $δ_c$ due to the formation of excitons. A spin liquid insulator (SLI) phase is thus realized without the lattice frustration. The critical value $δ_{c}$ sensitively depends on the inter-layer interaction strength. In the $tJ$ model description of each layer with the d-wave pairing, $δ_{c}$ marks the crossover between SLI and d-wave superconductor. The SLI phase, despite being non-superconducting and charge-gapped, still shows electromagnetic response similar to that of a superfluid due to the exciton transport. Including antiferromagnetic order in the $tJ$ model introduces magnetically ordered phases at low doping and pushes the spin liquid phase to a larger inter-layer interaction strength and higher doping concentrations.
dc.identifierhttps://arxiv.org/abs/cond-mat/0605426
dc.identifierhttp://arxiv.org/abs/cond-mat/0605426
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/110910
dc.subjectSuperconductivity
dc.subjectStrongly Correlated Electrons
dc.titlePhases of Mott-Hubbard bilayers
dc.typetext

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