Abstract

We consider a toy model for emergence of chaos in a quantum many-body short-range-interacting system: two one-dimensional hard-core particles in a box, with a small mass defect as a perturbation over an integrable system, the latter represented by two equal mass particles. To that system, we apply a quantum generalization of Chirikov's criterion for the onset of chaos, i.e. the criterion of overlapping resonances. There, classical nonlinear resonances translate almost automatically to the quantum language. Quantum mechanics intervenes at a later stage: the resonances occupying less than one Hamiltonian eigenstate are excluded from the chaos criterion. Resonances appear as contiguous patches of low purity unperturbed eigenstates, separated by the groups of undestroyed states-the quantum analogues of the classical KAM tori.

Highlights

  • The celebrated Chirikov resonance-overlap criterion [1, 2] constitutes a simple analytic estimate for the onset of chaos in an integrable, deterministic Hamiltonian system weakly perturbed from integrability

  • What we found was that not all the resonances identified in the classical system are eligible to being included in the resonance overlap consideration

  • The quantum analogues of the classical resonances appear as contiguous patches of low purity unperturbed eigenstates

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Summary

Introduction

The celebrated Chirikov resonance-overlap criterion [1, 2] constitutes a simple analytic estimate for the onset of chaos in an integrable, deterministic Hamiltonian system weakly perturbed from integrability. This criterion can be considered as a heuristic and intuitive precursor to the rigorous Kolmogorov-Arnold-Moser (KAM) theorem [3,4,5] that serves the same purpose for classical systems. In [10,11,12,13], the authors study a quantum system with exactly two nonlinear resonances, while in [14, 15], the studied quantum system is truncated to two resonances Both systems consist of a single particle driven by an external field. In the quantum model the threshold for the emergence of chaos is restored even for a system with short-range interactions

Chirikov condition
Quantum two-particle model
Conclusions and outlook
Set-up
Nonlinear resonances
Chirikov criterion
B Special case of the 1:0 resonance

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