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However, no such insulator of bosons is possible atν= 1/2 unless translation symmetry is broken, leading us to conclude the flavor adjoint masses must break translation

As argued in [22], adding a flavor mass to the critical point leads to a trivial insulator

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Pathways from a chiral superconductor to a composite Fermi liquid

cond-mat.str-el · 2025-09-25 · unverdicted · novelty 5.0

For weak attractive interactions the evolution from chiral superconductor to composite Fermi liquid passes through an intermediate stable Landau Fermi liquid, while stronger interactions may route through a non-Abelian paired quantum Hall state.

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  • Pathways from a chiral superconductor to a composite Fermi liquid cond-mat.str-el · 2025-09-25 · unverdicted · none · ref 54

    For weak attractive interactions the evolution from chiral superconductor to composite Fermi liquid passes through an intermediate stable Landau Fermi liquid, while stronger interactions may route through a non-Abelian paired quantum Hall state.