A convex-geometric framework for fully phase-locked states in the finite Kuramoto model

TL;DR

This paper introduces a convex-geometric framework to analyze the stability and existence of fully phase-locked states in the finite Kuramoto model, providing explicit bounds and geometric insights.

Contribution

It develops a convex-geometric approach to characterize the stability region and critical coupling in the finite Kuramoto model, including explicit bounds and geometric interpretations.

Findings

The stability region maps to a convex set in frequency space.

The critical coupling corresponds to the first intersection of a ray with the convex boundary.

An explicit polytope provides a computable upper bound for the critical coupling.

Abstract

We study the finite-size Kuramoto model of all-to-all coupled phase oscillators with heterogeneous natural frequencies and characterize the minimal coupling strength required for the existence of a fully phase-locked equilibrium (in a co-rotating frame). To remove the degeneracy due to uniform phase shifts, we move to a reduced co-rotating frame and assess stability through the Jacobian of the reduced system: a fully phase-locked state is stable when this Jacobian is negative definite. This defines a stability region in the phase space. The Kuramoto vector field maps this region to a convex set in frequency space, so a fully-locked state at coupling $K$ exists exactly when the rescaled frequency vector $\hat{\mathbf{\omega}}/K$ lies inside that convex image. The critical coupling $K_{\ell}$ is defined as the smallest coupling strength for which a fully phase-locked equilibrium exists; geometrically, it corresponds to the first intersection of the ray $t\hat{\mathbf{\omega}}$ with the boundary of this convex set. Building on this convex-geometric structure, we construct an explicit polytope from analytically computable boundary points of the stability region, providing a closed-form upper bound $K_b \ge K_{\ell}$. The bound is exact for frequencies aligned with polytope vertices and offers a fully explicit outer approximation for general frequency vectors. While not uniformly sharp in a quantitative sense, this construction exposes the underlying geometry of stable fully phase-locking solutions. These results provide a practical use the convex-geometric structure underlying stable fully-locked states in the Kuramoto model.