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Effect of noise on quantum circuit realization of non-Hermitian time crystals

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arxiv 2409.06113 v3 pith:KEETZP6J submitted 2024-09-09 cond-mat.str-el cond-mat.stat-mechquant-ph

classification cond-mat.str-elcond-mat.stat-mechquant-ph
keywords dynamicsquantumnoisenon-hermitianoscillationslong-livedconsiderfloquet
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Non-Hermitian quantum dynamics lie in an intermediate regime between unitary Hamiltonian dynamics and trace-preserving non-unitary open quantum system dynamics. Given differences in the noise tolerance of unitary and non-unitary dynamics, it is interesting to consider implementing non-Hermitian dynamics on a noisy quantum computer. In this paper, we do so for a non-Hermitian Ising Floquet model whose many-body dynamics gives rise to persistent temporal oscillations, a form of time crystallinity. In the simplest two qubit case that we consider, there is an infinitely long-lived periodic steady state at certain fine-tuned points. These oscillations remain reasonably long-lived over a range of parameters in the ideal non-Hermitean dynamics and for the levels of noise and imperfection expected of modern day quantum devices. Using a generalized Floquet analysis, we show that infinitely long-lived oscillations are generically lost for arbitrarily weak values of common types of noise and compute corresponding damping rate. We perform simulations using IBM's Qiskit platform to confirm our findings; however, experiments on a real device (ibmq-lima) do not show remnants of these oscillations.

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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. Unpolarized prethermal discrete time crystal

    cond-mat.quant-gas 2025-01 conditional novelty 7.0 of 10

    Period-doubled, prethermal time-crystalline signatures can appear in the autocorrelation of staggered magnetization for an unpolarized ground state, even though the magnetization expectation value is zero.

  2. Effects of non-integrability in a non-Hermitian time crystal

    cond-mat.str-el 2024-12 conditional novelty 6.0 of 10

    Adding XX interactions to a non-Hermitian Floquet Ising chain shifts its time-crystal phase boundaries and, above K_c ≈ 0.085, stabilizes a new x-ferromagnetic phase at R=1.

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