Self-doped Wigner crystals arise from preempted band-inversion transitions between commensurate crystals, as established by non-perturbative arguments and Hartree-Fock calculations in jellium and rhombohedral graphene models.
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Chirality reorganizes the sign structure of finite-q photon-drag photocurrents in 2D Dirac fermions, yielding sign reversals for J≥2 but not for J=1, with transverse symmetry and vanishing at q=0 in centrosymmetric cases.
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.
citing papers explorer
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Self-doped Crystal from Preempted Band-inversion Transitions
Self-doped Wigner crystals arise from preempted band-inversion transitions between commensurate crystals, as established by non-perturbative arguments and Hartree-Fock calculations in jellium and rhombohedral graphene models.
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Finite-q photon-drag shift current in two-dimensional massive chiral Dirac fermions
Chirality reorganizes the sign structure of finite-q photon-drag photocurrents in 2D Dirac fermions, yielding sign reversals for J≥2 but not for J=1, with transverse symmetry and vanishing at q=0 in centrosymmetric cases.
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Pathways from a chiral superconductor to a composite Fermi liquid
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.