A 1D Mott insulator exhibits persistent, strengthening interference peaks and oscillatory exponentially decaying coherence across lattice sites, matching QMC simulations.
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The frame potential of a disordered Tomonaga-Luttinger liquid decays as a power law at early times and saturates to a late-time plateau controlled by a single coupling parameter.
In 1D Anderson and Kondo lattices, reservoir-mediated extended interactions produce near-long-range superconducting and magnetic correlations at intermediate scales before the insulating state dominates.
The second plateau at about 3/5 the first in 3D QHE arises from spin-density-wave order induced by nesting between spin-up and spin-down Landau bands after a Lifshitz transition.
citing papers explorer
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The wave nature of a Mott insulator
A 1D Mott insulator exhibits persistent, strengthening interference peaks and oscillatory exponentially decaying coherence across lattice sites, matching QMC simulations.
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Solvable Random Unitary Dynamics in a Disordered Tomonaga-Luttinger Liquid
The frame potential of a disordered Tomonaga-Luttinger liquid decays as a power law at early times and saturates to a late-time plateau controlled by a single coupling parameter.
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Mapping reservoir-enhanced superconductivity to near-long-range magnetic order in the undoped one-dimensional Anderson and Kondo lattices
In 1D Anderson and Kondo lattices, reservoir-mediated extended interactions produce near-long-range superconducting and magnetic correlations at intermediate scales before the insulating state dominates.
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3D Quantum Hall Effect with Two Distinct Plateaus
The second plateau at about 3/5 the first in 3D QHE arises from spin-density-wave order induced by nesting between spin-up and spin-down Landau bands after a Lifshitz transition.