Twisted 1T-ZrS₂ and 1T-SnSe₂ host isolated topological moiré valence bands with quantum spin Hall and high spin Chern states that arise from inter-branch and inter-orbital coupling under approximate spin-U(1) symmetry.
Balents , author C
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A universal magnetic energy scale J* emerges at finite doping in the Fermi-Hubbard model, controlling magnetic correlations, bimagnon spectra, pseudogap onset, and the transition to incommensurate spin-density waves.
A self-consistent continuum Hartree+U model with long-range Coulomb interactions maps the magnetic phase diagram of magic-angle twisted bilayer and trilayer graphene versus doping and twist angle.
citing papers explorer
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Engineering topological flat bands in $\Gamma$-valley moir\'e systems with Ising-type SOC: twisted 1T-ZrS$_2$ and 1T-SnSe$_2$
Twisted 1T-ZrS₂ and 1T-SnSe₂ host isolated topological moiré valence bands with quantum spin Hall and high spin Chern states that arise from inter-branch and inter-orbital coupling under approximate spin-U(1) symmetry.
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Universal magnetic energy scale in the doped Fermi-Hubbard model
A universal magnetic energy scale J* emerges at finite doping in the Fermi-Hubbard model, controlling magnetic correlations, bimagnon spectra, pseudogap onset, and the transition to incommensurate spin-density waves.
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Magnetic Ordering in Moir\'e Graphene Multilayers from a Continuum Hartree+U Approach
A self-consistent continuum Hartree+U model with long-range Coulomb interactions maps the magnetic phase diagram of magic-angle twisted bilayer and trilayer graphene versus doping and twist angle.