Bose condensation is responsible for many of the most spectacular effects in physics because it can promote quantum behavior from the microscopic to the macroscopic world. Bose condensates can be distinguished by the condensing object; electron-electron Cooper-pairs are responsible for superconductivity, Helium atoms for superfluidity, and ultracold alkali atoms in vapors for coherent matter waves. Electron-hole pair (exciton) condensation has maintained special interest because it has been difficult to realize experimentally, and because exciton phase coherence is never[1] perfectly spontaneous. Although ideal condensates can support[2] an exciton supercurrent, it has not been clear [3] how such a current could be induced or detected, or how its experimental manifestation would be altered by the phase-fixing exciton creation and annihilation processes which are inevitably present. In this article we explain how to induce an exciton supercurrent in separately contacted bilayer condensates, and predict electrical effects which enable unambiguous detection.
PACS numbers:The order parameter of an exciton condensate iswhereψ † andψ are electron creation and annihilation operators, φ( r) is the condensate phase, the labels e (electron) and h (hole) refer to the states between which phase coherence is established (nearly!) spontaneously, and ρ(h, r, e, r) is the anomalous density matrix. Microscopic considerations suggest[4] that spontaneous coherence is likely between a conduction band with occupied states inside a Fermi surface and a valence band with occupied states outside a nearly [5] identical Fermi surface. Part of the reason that exciton condensation has not been easy to realize is that sufficiently perfect nesting between conduction and valence bands is unlikely to occur naturally. The systems of interest here are artificially fabricated bilayers in which the electrons and holes are in well separated two-dimensional electron systems(2DESs), either semiconductor quantum wells [6,7] or graphene layers [8] separated by a dielectric barrier. The dielectric barrier reduces the strength of exciton creation and annihilation processes, and gate control of the density in each layer allows electron and hole band Fermi surfaces to be tuned to the same area. Although simple to describe, this quantum engineering is difficult [6,7,9] to execute successfully. Exciton condensation has so far been realized [10] only in the quantum Hall regime in which band dispersion is irrelevant allowing spontaneous coherence to occur between spatially separated conduction bands, or spatially separated valence bands, under circumstances that are achieved routinely. The considerations explained in this article apply to quantum Hall exciton condensates in the Corbino geometry [11,12], in which current flows across the 2DES bulk, but not directly to the Hall bar geometry [13] in which currents flows along the 2DES edge.In their pioneering work on exciton Bose condensation Blatt et al. [3] argued that because an exciton is neutral, condensation...