Perturbed random Floquet-Clifford circuits exhibit operator-space fragmentation into wall-separated sectors for p < 1, yielding exact local integrals of motion, tunable operator spreading length, an entanglement bottleneck, and a pre-RMT fragmentation timescale at p = 1.
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Quasiperiodic Fibonacci edges in zigzag graphene nanoribbons combined with moderate electron interactions induce a conductive regime with transmission oscillations, while non-interacting and strongly interacting cases remain localized.
The generalized Aubry-André model exhibits an ergodic-MBL transition whose critical disorder strength is characterized via the Frobenius norm of the adiabatic gauge potential, with finite-size scaling and Thouless time analysis.
Evanescent modes can dominate cooperative spontaneous decay and radiation transfer in waveguide atomic ensembles by modifying dipole-dipole interatomic interactions.
Numerical simulations of two incommensurate tight-binding chains reveal a mobility edge with abrupt localization onset in higher-energy states, enhanced by weak magnetic fields but reversed by strong fields.
The spectrum E = R²(e^p + e^{-p}) + (e^x + e^{-x}) from local P¹ × P¹ is identified with the almost Mathieu operator, yielding three spectral phases separated by transitions at R² = 1 and R² = e^β.
In an off-diagonal Aubry-André-Harper chain, transport signatures distinguish edge states, in-band bulk states, and band-edge bulk states by their system-size dependence, resonance broadening, and dephasing sensitivity.
citing papers explorer
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Operator space fragmentation in perturbed Floquet-Clifford circuits
Perturbed random Floquet-Clifford circuits exhibit operator-space fragmentation into wall-separated sectors for p < 1, yielding exact local integrals of motion, tunable operator spreading length, an entanglement bottleneck, and a pre-RMT fragmentation timescale at p = 1.
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Engineering Delocalization in Graphene Nanoribbons via Quasiperiodic Edges and Electronic Interactions
Quasiperiodic Fibonacci edges in zigzag graphene nanoribbons combined with moderate electron interactions induce a conductive regime with transmission oscillations, while non-interacting and strongly interacting cases remain localized.
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Characterization of Thermalization Behaviour in a Generalized Aubry-Andr\'e Model
The generalized Aubry-André model exhibits an ergodic-MBL transition whose critical disorder strength is characterized via the Frobenius norm of the adiabatic gauge potential, with finite-size scaling and Thouless time analysis.
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The influence of evanescent waves on the nature of optical cooperative effects in atomic ensembles in a waveguide
Evanescent modes can dominate cooperative spontaneous decay and radiation transfer in waveguide atomic ensembles by modifying dipole-dipole interatomic interactions.
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Quantum localization in incommensurate tight-binding chains
Numerical simulations of two incommensurate tight-binding chains reveal a mobility edge with abrupt localization onset in higher-energy states, enhanced by weak magnetic fields but reversed by strong fields.
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Geometric Engineering and Almost Mathieu Operator
The spectrum E = R²(e^p + e^{-p}) + (e^x + e^{-x}) from local P¹ × P¹ is identified with the almost Mathieu operator, yielding three spectral phases separated by transitions at R² = 1 and R² = e^β.
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Transport characteristics of bulk and edge states in an off-diagonal Aubry--Andr\'e--Harper chain
In an off-diagonal Aubry-André-Harper chain, transport signatures distinguish edge states, in-band bulk states, and band-edge bulk states by their system-size dependence, resonance broadening, and dephasing sensitivity.