Please use this identifier to cite or link to this item: http://hdl.handle.net/2248/5768
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dc.contributor.authorDhar, A-
dc.contributor.authorMaji, M-
dc.contributor.authorMishra, T-
dc.contributor.authorPai, R. V-
dc.contributor.authorMukerjee, S-
dc.contributor.authorParamekanti, A-
dc.date.accessioned2012-05-07T14:18:04Z-
dc.date.available2012-05-07T14:18:04Z-
dc.date.issued2012-04-
dc.identifier.citationPhysical Review A, Vol. 85, No. 4, 041602en
dc.identifier.urihttp://hdl.handle.net/2248/5768-
dc.description.abstractMotivated by experiments on Josephson junction arrays, and cold atoms in an optical lattice in a synthetic magnetic field, we study the “fully frustrated” Bose-Hubbard model with half a magnetic flux quantum per plaquette. We obtain the phase diagram of this model on a two-leg ladder at integer filling via the density matrix renormalization group approach, complemented by Monte Carlo simulations on an effective classical XY model. The ground state at intermediate correlations is consistently shown to be a chiral Mott insulator (CMI) with a gap to all excitations and staggered loop currents which spontaneously break time-reversal symmetry. We characterize the CMI state as a vortex supersolid or an indirect exciton condensate, and discuss various experimental implications.en
dc.language.isoenen
dc.publisherAmerican Physical Societyen
dc.relation.urihttp://link.aps.org/doi/10.1103/PhysRevA.85.041602en
dc.rights© American Physical Societyen
dc.titleBose-Hubbard model in a strong effective magnetic field: Emergence of a chiral Mott insulator ground stateen
dc.typeArticleen
Appears in Collections:IIAP Publications

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