Quantum spin Hall insulators with arbitrary spin J support J+1/2 pairs of helical edge modes protected by mirror Chern numbers, described by a generalized Dirac fermion with higher-order dispersion and nonlinear transport.
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In the 3D Hofstadter-Hubbard model, superconductivity occurs for arbitrarily weak attraction below the critical flux for Weyl points with BCS-like gap scaling, but requires finite interaction strength above it.
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Quantum higher-spin Hall insulators
Quantum spin Hall insulators with arbitrary spin J support J+1/2 pairs of helical edge modes protected by mirror Chern numbers, described by a generalized Dirac fermion with higher-order dispersion and nonlinear transport.
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Superconducting properties of the three-dimensional Hofstadter-Hubbard model below the critical flux for Weyl points
In the 3D Hofstadter-Hubbard model, superconductivity occurs for arbitrarily weak attraction below the critical flux for Weyl points with BCS-like gap scaling, but requires finite interaction strength above it.