Layered Kitaev-Ising spin-orbital models map to N-flavor Hubbard models with emergent SU(N) symmetry; mean-field for N=3 yields intertwined orders and spin fragmentation with liquid orbitals.
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Quadratic-band-touching Hamiltonians in 2D possess USp(2N) symmetry; respecting interactions are limited to two terms that either preserve the symmetry or break it to USp(N) x USp(N), while lattice versions reduce to U(N) symmetry.
Time evolution in the time-dependent SU(2) Gross-Neveu model with RG-matched coupling is equivalent to renormalization group flow, generating an exponentially decaying dynamical mass gap in the adiabatic regime.
Charm and bottom quark masses are extracted as 1275.8 ± 0.4 MeV and 4177.0 ± 7.2 MeV using PMC-improved conformal series from quarkonium sum-rule moments, agreeing with PDG averages within 1σ.
citing papers explorer
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Fractionalization, emergent SU($N$) symmetries, and fragmentation in layered quantum spin-orbital models
Layered Kitaev-Ising spin-orbital models map to N-flavor Hubbard models with emergent SU(N) symmetry; mean-field for N=3 yields intertwined orders and spin fragmentation with liquid orbitals.
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Symplectic symmetry of quadratic-band-touching Hamiltonians in two dimensions
Quadratic-band-touching Hamiltonians in 2D possess USp(2N) symmetry; respecting interactions are limited to two terms that either preserve the symmetry or break it to USp(N) x USp(N), while lattice versions reduce to U(N) symmetry.
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Time-Dependent Dynamical Dimensional Transmutation in the $SU(2)$ Gross-Neveu Model with Time-Dependent Interaction Strength
Time evolution in the time-dependent SU(2) Gross-Neveu model with RG-matched coupling is equivalent to renormalization group flow, generating an exponentially decaying dynamical mass gap in the adiabatic regime.
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New Determinations of the Charm and Bottom Quark Masses Using QCD Quarkonium Sum Rules
Charm and bottom quark masses are extracted as 1275.8 ± 0.4 MeV and 4177.0 ± 7.2 MeV using PMC-improved conformal series from quarkonium sum-rule moments, agreeing with PDG averages within 1σ.