Finite density of anyonic excitons in bilayer Laughlin states at total filling 2/3 yields an exciton superfluid with specific bulk topological order, edge spectrum, and stiffness scaling as |δν|^{1/2} near Halperin (112) transitions.
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Composite 2Ne superconducting and 2NkF density-wave susceptibilities are shown to dominate over conventional instabilities at strong forward-scattering coupling in a D-dimensional Fermi liquid.
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Anyon superfluidity of excitons in quantum Hall bilayers
Finite density of anyonic excitons in bilayer Laughlin states at total filling 2/3 yields an exciton superfluid with specific bulk topological order, edge spectrum, and stiffness scaling as |δν|^{1/2} near Halperin (112) transitions.
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Instabilities of Fermi Liquids with Arbitrary Forward Scattering: Exact Approach
Composite 2Ne superconducting and 2NkF density-wave susceptibilities are shown to dominate over conventional instabilities at strong forward-scattering coupling in a D-dimensional Fermi liquid.