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Anyon Superconductivity from Topological Criticality in a Hofstadter-Hubbard Model
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We argue that the combination of strong repulsive interactions and high magnetic fields can generate electron pairing and superconductivity. Inspired by the large lattice constants of moir\'e materials, which make large flux per unit cell accessible at laboratory fields, we study the triangular lattice Hofstadter-Hubbard model at one-quarter flux quantum per plaquette, where previous literature has argued that a chiral spin liquid separates a weak-coupling integer quantum Hall phase and a strong-coupling topologically-trivial antiferromagnetic insulator at a density of one electron per site. We argue that topological superconductivity emerges upon doping in the vicinity of the integer quantum Hall to chiral spin liquid transition. We employ exact diagonalization and density matrix renormalization group methods to examine this theoretical scenario and find that electronic pairing indeed occurs on both sides of criticality over a remarkably broad range of interaction strengths. On the chiral spin liquid side, our results provide a concrete model realization of the long-hypothesized mechanism of anyon superconductivity. Our study thus establishes a beyond-BCS mechanism for electron pairing in a well-controlled limit, relying crucially on the interplay between electron correlations and band topology.
Forward citations
Cited by 10 Pith papers
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Chern-Simons-matter conformal field theory on fuzzy sphere: Confinement transition of Kalmeyer-Laughlin chiral spin liquid
A fuzzy-sphere exact diagonalization study shows the fIQH to bFQH transition is continuous, with emergent conformal symmetry and a single relevant singlet of scaling dimension Delta_S = 1.52(18).
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Anyon Dispersion in Aharonov-Casher Bands and Implications for Twisted MoTe${}_2$
Laughlin quasiholes in an Aharonov-Casher band acquire a finite dispersion, of order 1 meV in twisted MoTe2, produced by non-uniform quantum geometry and the anyon Berry phase.
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Anyon dispersion from non-uniform magnetic field on the sphere
For a specifically chosen non-uniform magnetic field on the sphere, Laughlin quasiholes acquire an analytically computed, interaction-generated energy dispersion whose functional form is exact up to a fitted overall scale.
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Fractionalized metals from doped anyons: Application to tMoTe2
Lightly doped 2/3 FQAH anyons form U(3)-symmetric Z3 Orthogonal Metals of charge-1/3 fermions that explain large resistivity and pair into ordinary 2e superconductors.
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Superconducting and charge-ordered phases from Dirac quantum spin liquids on the triangular lattice
Chargon condensation in a triangular-lattice Dirac spin liquid produces a catalog of pair-density-wave, charge-density-wave, bond-density-wave, and current-loop orders, with uniform d+id superconductivity allowed but ...
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Coloring in anyon superconductivity
Doping the ν=2/3 FQAH state produces a unifying 'quark metal' of charge-e/3 fermions whose superconducting and ferromagnetic instabilities reproduce and extend the known zoo of anyon-driven superconductors.
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Color superconductors and holon metals from doping a Fractional Chern insulator
Doping a C=1/3 fractional Chern insulator can produce charge-2e superconductors and holon metals described by a nine-pocket SU(3) parton theory.
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Non-Abelian topological superconductivity from melting Abelian fractional Chern insulators
Bandwidth tuning can melt a single ν=2/3 Jain fractional Chern insulator into five distinct superconductors, two with non-Abelian order, with higher-charge variants predicted at general Jain fillings.
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Topological Chiral Superconductivity in the Triangular-Lattice Hofstadter-Hubbard Model
DMRG and quantum Monte Carlo show that the lightly doped triangular Hofstadter-Hubbard model supports chiral superconductivity with power-law pairing and spin Chern number 2.
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Anyon delocalization transitions out of a disordered FQAH insulator
A theory predicts that doping a ν=2/3 fractional quantum anomalous Hall insulator with charge-2/3 anyons can drive a direct transition to a chiral topological superconductor, with a universal resistance peak, while ch...
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