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Analytic relation between coupling phases and locking bandwidth in large oscillator networks

Derive an analytic relation that characterizes how the coupling phase parameters β_{k,j} determine the size of the frequency-locking (synchronization) bandwidth in networks with an arbitrary number K of nonlinear oscillators governed by the Slavin–Tiberkevich universal auto‑oscillator model, where pairwise coupling strengths Ω_{k,j} are random. The relation should generalize beyond special two‑oscillator cases and provide explicit dependence of the locking bandwidth on β_{k,j} for large, randomly coupled arrays.

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Background

In the universal nonlinear oscillator model, the effective phase dynamics includes coupling phases β_{k,j}, which are known to influence synchronization bandwidth in two-oscillator settings. For two nearly identical oscillators, appropriate β choices can compensate nonlinear frequency shifts and maximize synchronization, but these insights do not straightforwardly extend to large networks.

The paper notes the absence of a known analytic relation linking β{k,j} to the locking bandwidth in networks with an arbitrary number of oscillators and random couplings Ω{k,j}. Establishing such a relation would guide the design of coupling phases to optimize synchronization in practical large‑scale oscillator arrays, impacting hardware implementations and training stability under Equilibrium Propagation.

References

To our knowledge, there is no analytic relation between the coupling phases and the size of the locking bandwidth in the case of an arbitrary number of such oscillators with random pairwise couplings \Omega_{k,j}.

Training and synchronizing oscillator networks with Equilibrium Propagation (2504.11884 - Rageau et al., 16 Apr 2025) in Appendix, Subsection “Nonlinear frequency shift N and coupling phase β_{k,j}” (Section s:nonlinear_frequency_shift)