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    Topologically protected edge oscillations in nonlinear dynamical units

    Sayantan Nag Chowdhury1,* and Hildegard Meyer-Ortmanns1,2,†

    • *Contact author: snagchowdh@constructor.university
    • †Contact author: hmeyerortm@constructor.university

    Phys. Rev. E 112, 044204 – Published 6 October, 2025

    DOI: https://doi.org/10.1103/lskh-hp3x

    Abstract

    Many examples from quantum and classical physics are known where topological protection is responsible for the robustness of the dynamics. Less explored is the role of topological protection in the context of classical oscillatory systems. As on-site dynamics, we consider prototypical oscillator models with possible applications in biochemical systems. However, our choice of coupling geometry is inspired by models from condensed matter physics which—in isolation—guarantee nontrivial topology in momentum space. We choose directed couplings between units on a two-dimensional grid, alternating between weak and strong values, such that oscillations become localized at the edges of the grid while bulk units transition to oscillation-death states, resulting in a frequency-chimera-like state. These patterns are resilient to parameter mismatches, additive noise, and structural defects. To explain the robustness of these edge oscillations we use topological characteristics and calculate Zak phases. As it turns out, the edge-localized oscillations result from a bulk-boundary correspondence that applies to our system even though our derived effective Hamiltonian is non-Hermitian. By appropriately tuning the system parameters, it is possible to control which regions of the two-dimensional grid are in an oscillatory state and which settle to oscillation-death states.

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