DQMC simulations of the doped Hubbard model find that Hall conductivity, unlike robust T-linear resistivity, is sensitive to asymmetry and Fermi surface details and reveals a crossover to quantum-coherent transport.
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SU(2) gauge theory plus DMFT with long-wavelength magnetic fluctuations produces damping asymmetry in chargon hole pockets that forms Fermi arcs in the underdoped regime.
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Hall conductivity reveals the nature of quantum coherence in strongly correlated metals
DQMC simulations of the doped Hubbard model find that Hall conductivity, unlike robust T-linear resistivity, is sensitive to asymmetry and Fermi surface details and reveals a crossover to quantum-coherent transport.
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The pseudogap in high-$T_c$ superconductors from SU(2) gauge symmetry and dynamic correlation effects
SU(2) gauge theory plus DMFT with long-wavelength magnetic fluctuations produces damping asymmetry in chargon hole pockets that forms Fermi arcs in the underdoped regime.