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The resulting LFL quasiparticle residue will be given byZ∼ |⟨Φ⟩| 2

This is particularly clear in the parton picture, as⟨Φ⟩ ̸= 0 allows us to identifyfandc, as the dynamical gauge fieldais Higgsed

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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 49

    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.