Quasi-integrable systems are slow to thermalize but may be good scramblers
arXiv:1909.02145 · doi:10.1103/PhysRevE.102.022201
Abstract
Classical quasi-integrable systems are known to have Lyapunov times much shorter than their ergodicity time -- the most clear example being the Solar System -- but the situation for their quantum counterparts is less well understood. As a first example, we examine the quantum Lyapunov exponent, defined by the evolution of the 4-point out-of-time-order correlator (OTOC), of integrable systems which are weakly perturbed by an external noise, a setting that has proven to be illuminating in the classical case. In analogy to the tangent space in classical systems, we derive a linear superoperator equation which dictates the OTOC dynamics. We find that i) in the semi-classical limit the quantum Lyapunov exponent is given by the classical one: it scales as , with being the variance of the random drive, leading to short Lyapunov times compared to the diffusion time (which is ). ii) in the highly quantal regime the Lyapunov instability is suppressed by quantum fluctuations, and iii) for sufficiently small perturbations the dependence is also suppressed -- another purely quantum effect which we explain. These essential features of the problem are already present in a rotor that is kicked weakly but randomly. Concerning quantum limits on chaos, we find that quasi-integrable systems are relatively good scramblers in the sense that the ratio between the Lyapunov exponent and may stay finite at a low temperature .
This version includes a replacement and an extension of arXiv:1911.04011
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- Semiclassical Limit of Measurement-Induced Transition in Many-Body Chaos in Integrable and Nonintegrable Oscillator Chains
- Quantum Kolmogorov-Sinai entropy and Pesin relation
- Quantum speed limit for the OTOC from an open systems perspective
- Deconfinement of classical Yang-Mills color fields in a disorder potential