Subsystem information capacity distinguishes critical phases in the generalized Aubry-André-Harper model by exposing spatial heterogeneity, stepwise subsystem-size dependence, and subregion echoes linked to incommensurately distributed zeros in hopping terms.
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9 Pith papers cite this work. Polarity classification is still indexing.
representative citing papers
Periodic driving of the generalized Aubry-André model produces controllable delocalized-localized and multifractal-localized Floquet mobility edges with corresponding superdiffusive to subdiffusive transport.
Tilt-induced quasiperiodic potential on a square lattice produces a mobility-edge-embedded Hofstadter butterfly with fractal dimension 0.8-1.0.
Uncorrelated hopping disorder in the generalized Aubry-André model enhances localization and turns the transition into a crossover, while spatially correlated disorder causes partial delocalization near strong bonds, as shown in momentum-space lattice experiments with 87Rb atoms.
Quasiperiodic modulation of Peierls phases in a disorder-free two-leg ladder drives Anderson localization transitions, yielding delocalized, localized, and mixed phases.
Adding a constant offset to the quasiperiodic potential in the diamond chain transforms anomalous mobility edges into conventional ones and demonstrates Avila's global theory fails to predict mobility edge locations.
Stealthy disorder in the 1D Anderson model makes the localization length scale as a higher inverse power of disorder strength W, allowing it to exceed system size for sufficient stealthiness parameter χ.
Kerr nonlinearity enables state-selective access to a critical window of coexisting localized, critical, and extended states in a quasiperiodic photonic lattice.
Unbound states survive and narrow in energy in near-infinitely deep quasiperiodic potentials; in non-Hermitian versions they form mixed bound-unbound phases with exact Lyapunov-exponent boundaries.
citing papers explorer
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Probing critical phases in quasiperiodic systems via subsystem information capacity
Subsystem information capacity distinguishes critical phases in the generalized Aubry-André-Harper model by exposing spatial heterogeneity, stepwise subsystem-size dependence, and subregion echoes linked to incommensurately distributed zeros in hopping terms.
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Floquet mobility edges and transport in a periodically driven generalized Aubry-Andr\'e model
Periodic driving of the generalized Aubry-André model produces controllable delocalized-localized and multifractal-localized Floquet mobility edges with corresponding superdiffusive to subdiffusive transport.
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Mobility-edge-embedded Hofstadter butterfly from a tilt-induced quasiperiodic potential
Tilt-induced quasiperiodic potential on a square lattice produces a mobility-edge-embedded Hofstadter butterfly with fractal dimension 0.8-1.0.
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Localization with Hopping Disorder in Quasi-periodic Synthetic Momentum Lattice
Uncorrelated hopping disorder in the generalized Aubry-André model enhances localization and turns the transition into a crossover, while spatially correlated disorder causes partial delocalization near strong bonds, as shown in momentum-space lattice experiments with 87Rb atoms.
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Anderson localization via Peierls phase modulation
Quasiperiodic modulation of Peierls phases in a disorder-free two-leg ladder drives Anderson localization transitions, yielding delocalized, localized, and mixed phases.
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Inapplicability of Avila's theory in the diamond chain with quasiperiodic disorder
Adding a constant offset to the quasiperiodic potential in the diamond chain transforms anomalous mobility edges into conventional ones and demonstrates Avila's global theory fails to predict mobility edge locations.
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Effective delocalization in the one-dimensional Anderson model with stealthy disorder
Stealthy disorder in the 1D Anderson model makes the localization length scale as a higher inverse power of disorder strength W, allowing it to exceed system size for sufficient stealthiness parameter χ.
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Nonlinear Photonic Tripartite Phase
Kerr nonlinearity enables state-selective access to a critical window of coexisting localized, critical, and extended states in a quasiperiodic photonic lattice.
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Unbound States and Mixed Bound--Unbound Phases in Near-Infinitely Deep Potentials
Unbound states survive and narrow in energy in near-infinitely deep quasiperiodic potentials; in non-Hermitian versions they form mixed bound-unbound phases with exact Lyapunov-exponent boundaries.