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脉冲耦合振荡器同步盆的算术性质

Arithmetic of the sync basin for pulse-coupled oscillators

K. P. O'Keeffe

arXiv 2609.01668首次发表:更新:

发表机构

Starling Research Institute(星形研究所)

机构由 AI 辅助整理,请以论文原文为准。

AI 中文总结

该研究揭示N个脉冲耦合振荡器的同步结果由N的素因子分解控制,同步概率有算术结构,为奇异盆几何新增算术盆类型。

AI 中文摘要

N个相同的脉冲耦合振荡器群体最终会收敛到两种结果之一:完全同步或共存的同步簇状态。我们证明,出现哪种结果由N的素因子分解控制。在临界充电曲线(线性,同步与聚类区域的边界)处,同步盆呈现精确的算术结构。对所有N,同步概率为$\u03a8_{sync}=A_{N,1}/N^N$,其中$A_{N,1}$满足精确递推关系。对于素数N,$A_{N,1}=N^N-1$,给出闭式$\u03a8_{sync}=1-1/N^N$;对于合数N,观测到的渐近标度为$1-\u03a8_{sync}\u223c C_m N^{-(m-1)}$,其中m是最小素因子。该结果为奇异盆几何图集增添了新成员:除了分形、 riddled和触手状盆,现在还有一个算术盆。

英文摘要

A population of $N$ identical pulse-coupled oscillators ultimately settles into one of two outcomes: full synchrony or a state of co-existing synchronized clusters. We show that which outcome occurs is controlled by the prime factorization of $N$. At the critical charging curve --- linear, the boundary between the synchronizing and clustering regimes --- the synchronization basin acquires exact arithmetic structure. The synchronization probability is $\Psync=A_{N,1}/N^N$ for all $N$, where $A_{N,1}$ satisfies an exact recurrence relation. For prime $N$, $A_{N,1}=N^N-1$ giving the closed form $\Psync=1-1/N^N$; for composite $N$, the observed asymptotic scaling is $1-\Psync\sim C_m N^{-(m-1)}$, where $m$ is the smallest prime divisor. The result adds a new member to the atlas of exotic basin geometries: alongside fractal, riddled, and tentacled basins, we now have a basin that is arithmetic.

CommentsAdded explicit K=1 recurrence after eq. (3) per referee optional remark; Supplementary Material updated; fixed truncated title

论文原文

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