Non-interacting charge-e/3 anyons with θ=-π/3 statistics superconduct via a hidden weak-pairing state of three-pocket composite fermions that realizes a chiral f-if superconductor with edge central charge c_-=-1/2.
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Anyon Bloch bands in ideal FCIs have m-fold degeneracy in the magnetic BZ and bandwidth controlled by quantum geometry non-uniformity, with higher harmonics strongly suppressing dispersion through emergent symmetries.
Doping a fractional Chern insulator yields an anyon fluid that can form an SC* superconductor with residual Z2 order or a non-Fermi liquid Z3 orthogonal metal.
citing papers explorer
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Hidden weak-pairing superconductivity of non-interacting anyons obeying $\frac{1}{3}$ statistics
Non-interacting charge-e/3 anyons with θ=-π/3 statistics superconduct via a hidden weak-pairing state of three-pocket composite fermions that realizes a chiral f-if superconductor with edge central charge c_-=-1/2.
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Dispersion of Anyon Bloch Bands
Anyon Bloch bands in ideal FCIs have m-fold degeneracy in the magnetic BZ and bandwidth controlled by quantum geometry non-uniformity, with higher harmonics strongly suppressing dispersion through emergent symmetries.
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Superconductivity and non-Fermi liquid metals in a charge-1/3 anyon fluid
Doping a fractional Chern insulator yields an anyon fluid that can form an SC* superconductor with residual Z2 order or a non-Fermi liquid Z3 orthogonal metal.