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    Obstruction to ergodicity in nonlinear Schrödinger equations with resonant potentials

    Anxo Biasi1, Oleg Evnin2,3, and Boris A. Malomed4,5

    • 1Laboratoire de Physique de l'Ecole Normale Supérieure ENS Université PSL, CNRS, Sorbonne Université, Université de Paris, F-75005 Paris, France
    • 2Department of Physics, Faculty of Science, Chulalongkorn University, Bangkok 10330, Thailand
    • 3Theoretische Natuurkunde, Vrije Universiteit Brussel and International Solvay Institutes, Brussels 1050, Belgium
    • 4Department of Physical Electronics, School of Electrical Engineering, Tel Aviv University, Tel Aviv 69978, Israel
    • 5Instituto de Alta Investigación, Universidad de Tarapacá, Casilla 7D, Arica, Chile

    Phys. Rev. E 108, 034204 – Published 8 September, 2023

    DOI: https://doi.org/10.1103/PhysRevE.108.034204

    Abstract

    We identify a class of trapping potentials in cubic nonlinear Schrödinger equations (NLSEs) that make them nonintegrable, but prevent the emergence of power spectra associated with ergodicity. The potentials are characterized by equidistant energy spectra (e.g., the harmonic-oscillator trap), which give rise to a large number of resonances enhancing the nonlinearity. In a broad range of dynamical solutions, spanning the regimes in which the nonlinearity may be either weak or strong in comparison with the linear part of the NLSE, the power spectra are shaped as narrow (quasidiscrete), evenly spaced spikes, unlike generic truly continuous (ergodic) spectra. We develop an analytical explanation for the emergence of these spectral features in the case of weak nonlinearity. In the strongly nonlinear regime, the presence of such structures is tracked numerically by performing simulations with random initial conditions. Some potentials that prevent ergodicity in this manner are of direct relevance to Bose-Einstein condensates: they naturally appear in 1D, 2D, and 3D Gross-Pitaevskii equations (GPEs), the quintic version of these equations, and a two-component GPE system.

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