非扭曲系统中偶数孪生岛诱导的无剪切力有效混乱传输障碍

M. Mugnaine, J. D. Szezech Jr., R. L. Viana, I. L. Caldas, P. J. Morrison
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摘要

几十年来,人们已经知道,具有无剪切不变环的非扭转哈密顿系统具有混沌传输障碍。在扰动作用下,这些障碍具有很强的抗破坏性,因此出现这些障碍的区域是寻找传输障碍的天然场所。我们描述了一种新型的有效障碍,它在无剪切环被打破后仍然存在。由于这种现象是通用的,为了方便起见,我们研究了标准非扭曲图(SNM),这是一种面积保留图,在相空间局部违反了扭曲条件。当存在双偶数周期岛时,新障碍就会出现在非扭曲系统中,这在 SNM 的国外参数值范围内都会发生。在由不规则和不规则轨道组成的相空间中,无剪切曲线、总障碍以及由双曲点的稳定流形和不稳定流形组成的部分障碍网络的存在阻碍了混沌轨迹的运动。作为一个退化系统,SNM 有孪生岛,因此也有孪生双曲点。我们证明,流形形成的结构本质上取决于孪生岛的周期奇偶性。在这种偶发情况下,由于不同双曲点的流形在偶极配置顶端形成了一个错综复杂的链条,通过链条的混沌轨迹传输成为罕见事件,因此出现了名为 "环形自由屏障 "的新结构。这种结构影响了传输的出现、混沌轨迹的逃逸盆地、传输机制和混沌鞍。奇周期轨道的情况则不同:我们发现在这种情况下,最后一条不变量曲线断裂后立即出现了传输,这导致了更高传输的情况,具有错综复杂的逃逸盆地边界和非均匀分布点的混沌鞍。
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Shearless effective barriers to chaotic transport induced by even twin islands in nontwist systems
For several decades now it has been known that systems with shearless invariant tori, nontwist Hamiltonian systems, possess barriers to chaotic transport. These barriers are resilient to breakage under perturbation and therefore regions where they occur are natural places to look for barriers to transport. We describe a novel kind of effective barrier that persists after the shearless torus is broken. Because phenomena are generic, for convenience we study the Standard Nontwist Map (SNM), an area-preserving map that violates the twist condition locally in the phase space. The novel barrier occurs in nontwist systems when twin even period islands are present, which happens for a broad range of parameter values in the SNM. With a phase space composed of regular and irregular orbits, the movement of chaotic trajectories is hampered by the existence of both shearless curves, total barriers, and a network of partial barriers formed by the stable and unstable manifolds of the hyperbolic points. Being a degenerate system, the SNM has twin islands and, consequently, twin hyperbolic points. We show that the structures formed by the manifolds intrinsically depend on period parity of the twin islands. For this even scenario the novel structure, named a torus free barrier, occurs because the manifolds of different hyperbolic points form an intricate chain atop a dipole configuration and the transport of chaotic trajectories through the chain becomes a rare event. This structure impacts the emergence of transport, the escape basin for chaotic trajectories, the transport mechanism and the chaotic saddle. The case of odd periodic orbits is different: we find for this case the emergence of transport immediately after the breakup of the last invariant curve, and this leads to a scenario of higher transport, with intricate escape basin boundary and a chaotic saddle with non-uniformly distributed points.
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