Confinement-deconfinement transition due to spontaneous symmetry breaking in quantum Hall bilayers
arXiv:1504.05154 · doi:10.1038/ncomms10462
Abstract
Band-inverted electron-hole bilayers support quantum spin Hall insulator and exciton condensate phases. We investigate such a bilayer in an external magnetic field. We show that the interlayer correlations lead to formation of a helical quantum Hall exciton condensate state. In contrast to the chiral edge states of the quantum Hall exciton condensate in electron-electron bilayers, existence of the counterpropagating edge modes results in formation of a ground state spin-texture not supporting gapless single-particle excitations. This feature has deep consequences for the low energy behavior of the system. Namely, the charged edge excitations in a sufficiently narrow Hall bar are confined, i.e.~a charge on one of the edges always gives rise to an opposite charge on the other edge. Moreover, we show that magnetic field and gate voltages allow to control confinement-deconfinement transition of charged edge excitations, which can be probed with nonlocal conductance. Confinement-deconfinement transitions are of great interest, not least because of their possible significance in shedding light on the confinement problem of quarks.
19 pages, 8 figures; v3: added Landau level diagrams and discussion of quantization breakdown
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- Designing three-dimensional flat bands in nodal-line semimetals
- Interplay of topology and interactions in quantum Hall topological insulators: U(1) symmetry, tunable Luttinger liquid, and interaction-induced phase transitions
- Transition between canted antiferromagnetic and spin-polarized ferromagnetic quantum Hall states in graphene on a ferrimagnetic insulator
- Topological Charge/spin density Wave in InAs/GaSb Quantum Wells under an In-plane Magnetic Field
- Exciton Condensation in Landau Levels of Quantum Spin Hall Insulators
- Conservation of Quantum Correlations in Multimode Systems with Symmetry