Exact asymptotic wavefunction for arbitrary spin s in the time-dependent Richardson-Gaudin model is derived independently per spin size, yielding a non-thermal steady state outside the natural GGE with mean-field exact for finite products of distinct-site spin operators.
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Experimental signatures of ferrimagnetism with antiferromagnetic correlations and finite polarization observed in ultracold fermions on a Lieb lattice at half filling.
ARPES on tMoTe2 reveals non-monotonic hole effective mass versus twist angle peaking near 2 degrees, consistent with predicted magic-angle band flattening, plus doping-dependent band evolution confirming a direct gap.
Pressure tunes band flatness and geometry in tMoTe2 to control FCI and GWC phases and their topological transitions at fractional fillings.
citing papers explorer
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Higher spin Richardson-Gaudin model with time-dependent coupling: Exact dynamics
Exact asymptotic wavefunction for arbitrary spin s in the time-dependent Richardson-Gaudin model is derived independently per spin size, yielding a non-thermal steady state outside the natural GGE with mean-field exact for finite products of distinct-site spin operators.
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Ferrimagnetism of ultracold fermions in a multi-band Hubbard system
Experimental signatures of ferrimagnetism with antiferromagnetic correlations and finite polarization observed in ultracold fermions on a Lieb lattice at half filling.
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Non-monotonic band flattening near the magic angle of twisted bilayer MoTe$_2$
ARPES on tMoTe2 reveals non-monotonic hole effective mass versus twist angle peaking near 2 degrees, consistent with predicted magic-angle band flattening, plus doping-dependent band evolution confirming a direct gap.
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Pressure-Tunable Generalized Wigner Crystal and Fractional Chern Insulator in twisted MoTe$_2$
Pressure tunes band flatness and geometry in tMoTe2 to control FCI and GWC phases and their topological transitions at fractional fillings.