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arXiv 2602.21149nlin.CD
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几何与惯性限制下的经典多体系统混沌增长

Geometry- and inertia-limited chaotic growth in classical many-body systems

SRM University–AP(SRM大学安得拉邦分校)

Swetamber Das

AI总结:

本文研究了经典多体系统中混沌增长的几何与惯性限制,通过建立显式上界揭示了惯性和相互作用几何对持续混沌增长的约束作用。

摘要:

许多体系统中的混沌不稳定性通常通过最大的李雅普诺夫指数来量化,但对经典相互作用系统中其大小的普遍约束仍缺乏深入理解。本文建立了经典多体系统中局部相互作用系统的最大李雅普诺夫指数的显式上界,这些上界源于哈密顿流的瞬时稳定性约束,并以惯性尺度和相互作用势能的曲率来表达。我们证明这些上界自然分为两种质上不同的类别:不可违反的上界,由最坏的局部曲率尺度、惯性和对空间结构不敏感的控制;以及ergodic上限,保留谱信息并编码集体模式和有限尺寸效应,在一般动态演化下。对于一个典型的二维耦合转子链(约瑟夫森结阵列),ergodic上限允许闭合的解析形式,并在李雅普诺夫指数-能量平面中产生一个动态不可达的区域,用于持续的混沌增长,我们通过数值方法确认了这一点。与不可违反的估计相比,ergodic上限通过捕捉集体抑制机制,提供了更严格的混沌增长约束,这些机制在局部曲率单独考虑时是不存在的。令人惊讶的是,在热力学极限下,ergodic上限渐近接近一个惯性上限,限制了持续的李雅普诺夫增长,变得与温度和相互作用强度无关。虽然经典系统不承认普遍的混沌上限,但我们的结果识别出一个广泛的自然哈密顿系统类别,在其中混沌增长被惯性和相互作用几何限制,从而设定了一个最小的微观时间尺度,用于长时间失去初始条件的记忆。

英文摘要:

Chaotic instability in many-body systems is commonly quantified by the largest Lyapunov exponent, yet general constraints on its magnitude in classical interacting systems remain poorly understood. Here we establish explicit, Hamiltonian-specific upper bounds on the largest Lyapunov exponent for classical many-body systems with local interactions. These bounds arise from instantaneous stability constraints on the Hamiltonian flow and are expressed in terms of inertial scales and the curvature of the interaction potential. We show that they naturally separate into two qualitatively distinct classes: non-violable bounds, controlled by worst-case local curvature scales and inertia and insensitive to spatial structure, and ergodic ceilings, which retain spectral information and encode collective modes and finite-size effects under generic dynamical evolution. For a paradigmatic one-dimensional coupled-rotor chain (Josephson junction array), the ergodic ceiling admits a closed analytic form and produces a dynamically inaccessible region for sustained chaotic growth in the Lyapunov exponent-energy plane, which we confirm numerically. In contrast to non-violable estimates, the ergodic ceiling yields a sharper constraint on chaotic growth by capturing collective suppression mechanisms absent at the level of local curvature alone. Remarkably, in the thermodynamic limit the ergodic ceiling asymptotically approaches an inertial ceiling that limits sustained Lyapunov growth, becoming independent of temperature and interaction strength. While classical systems do not admit universal chaos bounds, our results identify a broad class of natural Hamiltonian systems in which chaotic growth is inherently limited by inertia and interaction geometry, thereby setting a minimal microscopic timescale for long-time loss of memory of initial conditions.

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