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This study establishes a rigorous benchmark for out-of-time-order correlator (OTOC) dynamics within non-Hermitian oscillator models, specifically analyzing how integrability, nonlinearity, and parity-time symmetry breaking influence correlation growth. By characterizing critical scaling near exceptional points across zero and finite temperatures, the work provides a theoretical framework for observing these effects in photonic, circuit-QED, and trapped-ion platforms. The findings offer a clear reference point for understanding chaos and thermalization in weakly anharmonic quantum systems.
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Out-of-time-order correlators for Swanson Hamiltonian with interaction terms

arXiv2 min read

arXiv:2606.04062v1 Announce Type: new Abstract: In this work, we compute the out-of-time-ordered correlator (OTOC) for canonical position and momentum operators across a hierarchy of non-Hermitian oscillator models: the exactly solvable Swanson Hamiltonian, its Kerr-nonlinear extension, and parametrically driven variants. By employing the biorthogonal formalism required for parity-time symmetric quantum mechanics, we evaluate OTOCs both at zero and finite temperature, distinguishing behavior in the unbroken (real-spectrum) and broken (complex-spectrum) phases. Our analysis reveals how integrability, nonlinearity, driving, and parity-time symmetry breaking shape the temporal growth of operator correlations -- providing a clear benchmark for OTOC dynamics in non-Hermitian quadratic and weakly anharmonic systems. We further characterize critical scaling of the OTOC near the exceptional point and discuss experimental perspectives for observing these effects in photonic, circuit-QED, and trapped-ion platforms.

Abstract:In this work, we compute the out-of-time-ordered correlator (OTOC) for canonical position and momentum operators across a hierarchy of non-Hermitian oscillator models: the exactly solvable Swanson Hamiltonian, its Kerr-nonlinear extension, and parametrically driven variants. By employing the biorthogonal formalism required for parity-time symmetric quantum mechanics, we evaluate OTOCs both at zero and finite temperature, distinguishing behavior in the unbroken (real-spectrum) and broken (complex-spectrum) phases. Our analysis reveals how integrability, nonlinearity, driving, and parity-time symmetry breaking shape the temporal growth of operator correlations -- providing a clear benchmark for OTOC dynamics in non-Hermitian quadratic and weakly anharmonic systems. We further characterize critical scaling of the OTOC near the exceptional point and discuss experimental perspectives for observing these effects in photonic, circuit-QED, and trapped-ion platforms.

arXiv:2606.04062 [quant-ph]

(or arXiv:2606.04062v1 [quant-ph] for this version)

https://doi.org/10.48550/arXiv.2606.04062 Focus to learn more arXiv-issued DOI via DataCite (pending registration)

Phys. Rev. A 113, 062205 (2026)

https://doi.org/10.1103/tbjm-b9hq Focus to learn more DOI(s) linking to related resources

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