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Effect of noise on quantum circuit realization of non-Hermitian time crystals
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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.
Forward citations
Cited by 2 Pith papers
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Unpolarized prethermal discrete time crystal
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.
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Effects of non-integrability in a non-Hermitian time crystal
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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