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Operator Entanglement in Local Quantum Circuits I: Chaotic Dual-Unitary Circuits

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arxiv 1909.07407 v2 pith:3RBMAOUJ submitted 2019-09-16 cond-mat.stat-mech hep-thnlin.CDquant-ph

classification cond-mat.stat-mechhep-thnlin.CDquant-ph
keywords circuitsentanglementquantumchaoticlocal-operatordual-unitaryclassconjecture
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The entanglement in operator space is a well established measure for the complexity of the quantum many-body dynamics. In particular, that of local operators has recently been proposed as dynamical chaos indicator, i.e. as a quantity able to discriminate between quantum systems with integrable and chaotic dynamics. For chaotic systems the local-operator entanglement is expected to grow linearly in time, while it is expected to grow at most logarithmically in the integrable case. Here we study local-operator entanglement in dual-unitary quantum circuits, a class of "statistically solvable" quantum circuits that we recently introduced. We identify a class of "completely chaotic" dual-unitary circuits where the local-operator entanglement grows linearly and we provide a conjecture for its asymptotic behaviour which is in excellent agreement with the numerical results. Interestingly, our conjecture also predicts a "phase transition" in the slope of the local-operator entanglement when varying the parameters of the circuits.

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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. $p$-Body $\simeq$ Range $p-1$: Exact Order-Range Mapping and Dual-Unitarity

    quant-ph 2026-07 conditional novelty 7.0 of 10

    A kicked p-body Ising chain at interaction strength pi/4 is exactly equivalent, up to a global phase, to a two-body Ising chain with range p-1 couplings, giving new p-body dual-unitary Floquet models.

  2. Thermalization with partial information

    quant-ph 2025-08 unverdicted novelty 6.0 of 10

    A maximum channel entropy principle, backed by a microcanonical-style derivation, identifies the canonical noisy channel that models thermalization under partial information.

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