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This research proposes "many-body caging" as a disorder-free mechanism for glassy behavior in quantum systems, utilizing flat bands generated by quantum interference rather than structural randomness. The study demonstrates these phenomena through many-body Rabi oscillations and long-time memory effects within 2D lattice gauge theories applicable to Rydberg atom experiments. By defining new order parameters based on band overlaps over the many-body state graph, this work offers a theoretical pathway to realizing novel nonequilibrium quantum states without external disorder.
Many-body cages: disorder-free glassiness from flat bands in Fock space, and many-body Rabi oscillations
arXiv:2504.13086v2 Announce Type: replace-cross Abstract: We introduce many-body caging as a novel mechanism for nonthermal behaviour in quantum matter. We define many-body cages as eigenstates that, through quantum interference, become localised on a subgraph of the many-body state graph. These many-body cages can lead to the formation of flat bands in the many-body spectrum at characteristic, system-independent energies. These flat bands can realize a novel type of glassy eigenspectrum order in the absence of disorder, which we quantify by a band-overlap order parameter with an intricate, possibly fractal, distribution over the many-body state graph. We further show that these many-body cages exhibit distinctive signatures in experimentally accessible quantities, such as through a nonvanishing long-time memory of the initial condition, and many-body Rabi oscillations set by the characteristic flat band energies. While our predictions in principle apply to any constrained quantum system, we demonstrate them here for 2D lattice gauge theories and models relevant for current experiments in Rydberg atoms. We expect that these many-body cages offer a promising route to realize nonequilibrium quantum states with novel properties.
Abstract:We introduce many-body caging as a novel mechanism for nonthermal behaviour in quantum matter. We define many-body cages as eigenstates that, through quantum interference, become localised on a subgraph of the many-body state graph. These many-body cages can lead to the formation of flat bands in the many-body spectrum at characteristic, system-independent energies. These flat bands can realize a novel type of glassy eigenspectrum order in the absence of disorder, which we quantify by a band-overlap order parameter with an intricate, possibly fractal, distribution over the many-body state graph. We further show that these many-body cages exhibit distinctive signatures in experimentally accessible quantities, such as through a nonvanishing long-time memory of the initial condition, and many-body Rabi oscillations set by the characteristic flat band energies. While our predictions in principle apply to any constrained quantum system, we demonstrate them here for 2D lattice gauge theories and models relevant for current experiments in Rydberg atoms. We expect that these many-body cages offer a promising route to realize nonequilibrium quantum states with novel properties.
Quantum Gases (cond-mat.quant-gas); Disordered Systems and Neural Networks (cond-mat.dis-nn); Quantum Physics (quant-ph)
arXiv:2504.13086 [cond-mat.quant-gas]
(or arXiv:2504.13086v2 [cond-mat.quant-gas] for this version)
https://doi.org/10.48550/arXiv.2504.13086 Focus to learn more arXiv-issued DOI via DataCite
https://doi.org/10.1103/gmw6-x94c Focus to learn more DOI(s) linking to related resources
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Full text under the publisher's open licence · 283 words
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