The Hubbard model on the triangular lattice: Spiral order and spin liquid

dc.creatorSahebsara, Peyman
dc.creatorSénéchal, David
dc.date2007-11-02
dc.date2008-04-15
dc.date.accessioned2026-07-07T09:32:25Z
dc.date.available2026-07-07T09:32:25Z
dc.descriptionWe investigate the half-filled Hubbard model on an isotropic triangular lattice with the variational cluster approximation. By decreasing the on-site repulsion $U$ (or equivalently increasing pressure) we go from a phase with long range, three-sublattice, spiral magnetic order, to a non-magnetic Mott insulating phase -- a spin liquid -- and then, for $U\lesssim6.7t$, to a metallic phase. Clusters of sizes 3, 6 and 15 with open boundary conditions are used in these calculations, and an extrapolation to infinite size is argued to lead to a disordered phase at $U=8t$, but to a spiral order at $U\gtrsim 12$.
dc.description4 pages, 5 figures (published version)
dc.identifierhttps://arxiv.org/abs/0711.0244
dc.identifierhttp://arxiv.org/abs/0711.0244
dc.identifierPhys. Rev. Lett. 100, 136402 (2008)
dc.identifierdoi:10.1103/PhysRevLett.100.136402
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/158773
dc.subjectStrongly Correlated Electrons
dc.titleThe Hubbard model on the triangular lattice: Spiral order and spin liquid
dc.typetext

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