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2502.20614

SYNCHRONIZATION IN THE COMPLEXIFIED KURAMOTO MODEL

Ting-Yang Hsiao, Yun-Feng Lo, Winnie Wang

correcthigh confidence
Category
math.DS
Journal tier
Strong Field
Processed
Sep 28, 2025, 12:56 AM

Audit review

The paper’s Theorem 3.5 proves, under the strong-coupling/initial-separation hypotheses (λ > λ_c/sin δ and x(0) ∈ [0, π−δ]^N with ∑ω_n = 0), that phase synchronization occurs if and only if all natural frequencies are identical; the proof leverages Lemma 3.1 (real-part full phase-locking), Lemma 3.2 (imaginary-part contraction), Theorem 3.3 (full phase-locking), and Theorem 3.4 (frequency synchronization), then passes to the limit in the real-part equation to conclude phase synchronization and necessity of identical ω’s . The model gives a different direct proof: for ω_1=…=ω_N (hence λ_c=0), it shows diameter contraction of the real parts and exponential decay of the imaginary-part variance (after the real-part diameter enters a cone), and for necessity it uses a Cesàro-average argument on the pairwise difference equation. The two arguments are logically consistent with the same statement; the model’s route via a gradient-flow potential and a clean Ḋ_x-inequality is distinct from the paper’s energy-function and lemma chain. Minor technical gaps in the model (handling non-unique maximizers of x_i(t) when differentiating D_x) are easily fixed with Dini-derivatives; overall, both are correct.

Referee report (LaTeX)

\textbf{Recommendation:} minor revisions

\textbf{Journal Tier:} strong field

\textbf{Justification:}

The theorem proved in the strong-coupling regime—phase synchronization if and only if natural frequencies are identical—is correct and appropriately scoped. The paper’s proof structure is well organized and sound; explicit mention of certain routine steps (e.g., uniqueness of equilibria within the cone and continuity arguments in the limit) would enhance clarity. The alternative gradient-flow proof independently corroborates the result and could be usefully acknowledged.