Maple-leaf lattice realizes U(1) Dirac spin liquid with N_f=12, where five symmetry-trivial charge-one monopoles may be dynamically irrelevant, providing a large-flavor platform to test compact QED3 stability.
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Numerical simulations of the dynamical dimer structure factor on the triangular Heisenberg model provide support for a gapless U(1) Dirac quantum spin liquid with gapless singlet monopole excitations at X = K/2 momenta.
Lattice DQMC simulations of mixed QED3 with flavor chemical potential identify a chiral flux phase featuring spontaneous emergent gauge flux, broken U(1)m symmetry, and relativistic Landau levels for Dirac fermions.
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Large-flavor route to a stable U(1) Dirac spin liquid on the maple-leaf lattice
Maple-leaf lattice realizes U(1) Dirac spin liquid with N_f=12, where five symmetry-trivial charge-one monopoles may be dynamically irrelevant, providing a large-flavor platform to test compact QED3 stability.
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Dynamical dimer structure factor of the triangular $S=1/2$ Heisenberg antiferromagnet
Numerical simulations of the dynamical dimer structure factor on the triangular Heisenberg model provide support for a gapless U(1) Dirac quantum spin liquid with gapless singlet monopole excitations at X = K/2 momenta.
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Emergent gauge flux in mixed QED$_3$ with flavor chemical potential: application to magnetized U(1) Dirac spin liquids
Lattice DQMC simulations of mixed QED3 with flavor chemical potential identify a chiral flux phase featuring spontaneous emergent gauge flux, broken U(1)m symmetry, and relativistic Landau levels for Dirac fermions.