Superconductivity emerges from a state with anomalous Hall effects in the flat Chern band of twisted bilayer MoTe2, providing the first reported coexistence with fractional quantum anomalous Hall effects.
Doping a fractional quantum anomalous hall insulator
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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.
Tunneling probes can measure anyon dispersion via quasiparticle interference patterns and continuum thresholds in fractional Chern 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.
citing papers explorer
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Signatures of unconventional superconductivity near reentrant and fractional quantum anomalous Hall insulators
Superconductivity emerges from a state with anomalous Hall effects in the flat Chern band of twisted bilayer MoTe2, providing the first reported coexistence with fractional quantum anomalous Hall effects.
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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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Measuring anyon dispersion with tunneling probes
Tunneling probes can measure anyon dispersion via quasiparticle interference patterns and continuum thresholds in fractional Chern insulators.
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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.
- Superconductivity and non-Fermi liquid metals in a charge-1/3 anyon fluid
- Topological superconductivity from Abelian fractional Chern insulators