Abstract

In ordinary semiconductor bilayers, exciton condensates appear at total Landau level filling factor νT=1ν_{T}=1. We predict that similar states will occur in Bernal stacked graphene bilayers at many non-zero integer filling factors. For νT=−3,1ν_{T} = -3,1 we find that the superfluid density of the exciton condensate vanishes and that a finite-temperature fluctuation induced first order isotropic-smectic phase transition occurs when the layer densities are not balanced. These anomalous properties of bilayer graphene exciton condensates are due to the degeneracy of Landau levels with n=0n=0 and n=1n=1 orbital character.

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