The interacting Anderson Quantum Sun model exhibits unconventional regimes featuring volume-law entanglement with intermediate spectral statistics and Poisson statistics with sub-volume entanglement growth.
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Charge transport capacity grows with system size in numerically accessible interacting Anderson chains because many-body resonances become more probable, indicating that short-ranged resonances have not yet converged and may contribute to apparent thermalization.
Superconducting qubit experiments reveal a non-ergodic glassy regime in a 2D disordered spin model, with power-law Hilbert-space dynamics, frozen degrees of freedom, and vanishing spin diffusion above a disorder threshold.
Local loops on Husimi trees reduce the critical disorder for Anderson localization and increase the spatial extent of localized eigenstates, providing a better single-particle analogy for many-body localization.
citing papers explorer
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Unconventional Thermalization of a Localized Chain Interacting with an Ergodic Bath
The interacting Anderson Quantum Sun model exhibits unconventional regimes featuring volume-law entanglement with intermediate spectral statistics and Poisson statistics with sub-volume entanglement growth.
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Charge Transport Capacity as a Probe of Resonances in Models of Many-Body Localization
Charge transport capacity grows with system size in numerically accessible interacting Anderson chains because many-body resonances become more probable, indicating that short-ranged resonances have not yet converged and may contribute to apparent thermalization.
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Hilbert space signatures of non-ergodic glassy dynamics
Superconducting qubit experiments reveal a non-ergodic glassy regime in a 2D disordered spin model, with power-law Hilbert-space dynamics, frozen degrees of freedom, and vanishing spin diffusion above a disorder threshold.
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Anderson Localization on Husimi Trees and its implications for Many-Body localization
Local loops on Husimi trees reduce the critical disorder for Anderson localization and increase the spatial extent of localized eigenstates, providing a better single-particle analogy for many-body localization.