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Genuine quantum scars in many-body spin systems

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arxiv 2408.10301 v2 pith:YXYIN5NA submitted 2024-08-19 quant-ph cond-mat.quant-gascond-mat.stat-mechcond-mat.str-el

classification quant-phcond-mat.quant-gascond-mat.stat-mechcond-mat.str-el
keywords quantumsystemsmany-bodychaosmakesmanypastscarring
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Chaos makes isolated systems of many interacting particles quickly thermalize and forget about their past. Here, we show that quantum mechanics hinders chaos in many-body systems: although the quantum eigenstates are thermal and strongly entangled, exponentially many of them are scarred, that is, have an enlarged weight along underlying classical unstable periodic orbits. Scarring makes the system more likely to be found on an orbit it was initialized on, retaining a memory of its past and thus weakly breaking ergodicity, even at long times and despite the system being fully thermal and the eigenstate thermalization hypothesis fulfilled. We demonstrate the ubiquity of quantum scarring in many-body systems by considering a large family of spin models, including some of the most popular ones from condensed matter physics. Our findings, at hand for modern quantum simulators, prove structure in spite of chaos in many-body quantum systems.

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Cited by 2 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score. Full citation record

  1. Asymmetric decay of quantum many-body scars in XYZ quantum spin chains

    quant-ph 2025-05 accept novelty 7.0 of 10

    Universal Granovskii-Zhedanov product-state scars in XYZ spin chains decay asymmetrically under perturbations, with slow linear decay on one side and exponential decay on the other, as predicted by semiclassical spin-...

  2. Quantum trails and memory effects in the phase space of chaotic quantum systems

    quant-ph 2024-12 conditional novelty 6.0 of 10

    Eigenstate phase-space projections in chaotic systems are correlated along short-time classical trajectories, producing quantum trails that cause a wavepacket to remember its initial trajectory and weakly break ergodicity.

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