Out-of-time correlation functions in single-body systems

• URL: http://arxiv.org/abs/2512.00471v1
• Date: Sat, 29 Nov 2025 12:46:57 GMT
• Title: Out-of-time correlation functions in single-body systems
• Authors: Andrew C. Hunt,
• Abstract summary: Out of time ordered correlators' (OTOCs) are commonly used to quantify the rate at which quantum information is scrambled.<n>Recent studies have shown that instantons, delocalised structures that dominate tunnelling statistics over barriers, reduce the growth rate of OTOCs.
• Score: 0.0
• License: http://creativecommons.org/licenses/by/4.0/
• Abstract: In the study of quantum chaos, `out of time ordered correlators' (OTOCs) are commonly used to quantify the rate at which quantum information is scrambled. This rate has been conjectured by Maldecena et al. to obey a universal, temperature dependent bound. Recent studies have shown that instantons, delocalised structures that dominate tunnelling statistics over barriers, reduce the growth rate of OTOCs. For the case of the symmetric double well, this reduction ensures the bound is maintained for OTOCs generated using ring polymer molecular dynamics (RPMD), a method with approximate dynamics but exact quantum statistics. In this report we set out to further understand the role of the instanton in the enforcement of the Maldacena bound and test whether RPMD is sufficient to satisfy the bound. We also investigate the impact of coherence on the flattening of of OTOCs by contrasting bounded with scattering systems. For the scattering system we observe a significantly smaller OTOC growth rate than that of the analogous bounded system, and a flattening in growth rate as time progresses. We attribute the first effect to influence of the Boltzmann operator, and the second to interference caused by anharmonicity of the potential. In our studies of RPMD, we find counterexamples showing that it is not sufficient to satisfy the bound. We develop a theory for OTOCs using (analytically-continued) Matsubara dynamics, revealing significantly different dynamical behaviour around the instanton compared to the predictions of RPMD. The instanton is found to be stationary in all coordinates but its collective angle $Φ_0$, and fluctuations about it no longer resemble that of classical dynamics on a first order saddle as in RPMD.

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