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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U(3) infrared parton theory unifies a ν=1/3 FCI with topological superconductors (SC* preserving U(1)_3, chiral TSC with c_-=3/2, strong-pairing with c_-=3) and a σ_xy=0 CDW.
Higher-order k corrections to Dirac dispersion enable Kohn-Luttinger superconductivity, producing topological p-ip pairing in broken-TR systems and anisotropic or warped pairings on TI surfaces.
Disorder effects on anyon composite fermion bands drive plateau transitions that explain observed superconductivity and RIQAH phases near doped nu_e=2/3 FQAH states in twisted MoTe2.
citing papers explorer
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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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Topological superconductivity from Abelian fractional Chern insulators
U(3) infrared parton theory unifies a ν=1/3 FCI with topological superconductors (SC* preserving U(1)_3, chiral TSC with c_-=3/2, strong-pairing with c_-=3) and a σ_xy=0 CDW.
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Anyon superconductivity and plateau transitions in doped fractional quantum anomalous Hall insulators
Disorder effects on anyon composite fermion bands drive plateau transitions that explain observed superconductivity and RIQAH phases near doped nu_e=2/3 FQAH states in twisted MoTe2.