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arXiv 2403.01488math.DS
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鞍结点展开中的解析弱稳定流形

Analytic weak-stable manifolds in unfoldings of saddle-nodes

Kristian Uldall Kristiansen, Peter Szmolyan

AI总结:

本文研究二维解析向量场趋近鞍结点时解析弱稳定流形的变化,揭示参数穿过无穷多共振时弱稳定流形位置剧烈变化的拍动机制,并将其与鞍结点中心流形缺乏解析性联系起来。

摘要:

二维解析向量场的任何吸引、双曲且真结点都具有唯一的强稳定流形,该流形是解析的。另一方面,相应的弱稳定流形并不唯一,但在非共振情形下存在唯一的解析弱稳定流形。当系统在参数变化下趋近鞍结点时,会出现一系列(阶数递增的)共振。本文详细描述了这一过程中解析弱稳定流形的行为。特别地,我们将一种“拍动机制”与鞍结点处中心流形缺乏解析性联系起来;该机制对应于当参数穿过无穷多个共振时解析弱稳定流形位置发生剧烈变化。我们的工作受到 Merle、Raphaël、Rodnianski 和 Szeftel 工作的启发,在他们的工作中,这种拍动机制是构造可压缩 Euler 方程的 $C^\infty$ 光滑自相似解的关键要素。

英文摘要:

Any attracting, hyperbolic and proper node of a two-dimensional analytic vector-field has a unique strong-stable manifold. This manifold is analytic. The corresponding weak-stable manifolds are, on the other hand, not unique, but in the nonresonant case there is a unique weak-stable manifold that is analytic. As the system approaches a saddle-node (under parameter variation), a sequence of resonances (of increasing order) occur. In this paper, we give a detailed description of the analytic weak-stable manifolds during this process. In particular, we relate a ``flapping-mechanism'', corresponding to a dramatic change of the position of the analytic weak-stable manifold as the parameter passes through the infinitely many resonances, to the lack of analyticity of the center manifold at the saddle-node. Our work is motivated and inspired by the work of Merle, Raphaël, Rodnianski, and Szeftel, where this flapping mechanism is the crucial ingredient in the construction of $C^\infty$-smooth self-similar solutions of the compressible Euler equations.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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