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arXiv 1404.7679nlin.CDastro-ph.EPmath.DS
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不稳定点附近的解析不变流形与混沌结构

Analytical invariant manifolds near unstable points and the structure of chaos

C. Efthymiopoulos, G. Contopoulos, M. Katsanikas

摘要:

已知保守系统中围绕不稳定周期轨道的渐近不变流形可以用收敛级数表示(Cherry 1926,Moser 1956,1958,Giorgilli 2001)。不稳定流形和稳定流形相交于无穷多个同宿点,产生复杂的同宿缠结。在简单映射的情况下,人们发现(Da Silva Ritter et al. 1987)形式级数的收敛域沿着不变流形延伸到无穷远。这使得在实践中研究同宿缠结只使用系列。然而,在哈密尔顿系统的情况下,或映射与一个有限的解析域,收敛的级数沿渐近流形也是有限的。在这里,我们提供的数值表明,收敛不会达到任何同宿点。我们详细讨论了在各种情况下的收敛问题,我们发现的解析不变流形的真实(数值)流形的逼近程度,因为i)截断的级数增加的顺序,和ii)我们使用更高的数值精度计算系数的系列。然后,我们介绍了一种新的方法系列组成,通过使用作用角变量,允许计算的渐近流形到一个任意大的程度。这是第一种情况下的分析发展,允许计算的不变流形和它们的交叉点在一个哈密顿系统的程度足够长,以允许研究同宿混沌的分析手段。

英文摘要:

It is known that the asymptotic invariant manifolds around an unstable periodic orbit in conservative systems can be represented by convergent series (Cherry 1926, Moser 1956, 1958, Giorgilli 2001). The unstable and stable manifolds intersect at an infinity of homoclinic points, generating a complicated homoclinic tangle. In the case of simple mappings it was found (Da Silva Ritter et al. 1987) that the domain of convergence of the formal series extends to infinity along the invariant manifolds. This allows in practice to study the homoclinic tangle using only series. However in the case of Hamiltonian systems, or mappings with a finite analyticity domain,the convergence of the series along the asymptotic manifolds is also finite. Here, we provide numerical indications that the convergence does not reach any homoclinic points. We discuss in detail the convergence problem in various cases and we find the degree of approximation of the analytical invariant manifolds to the real (numerical) manifolds as i) the order of truncation of the series increases, and ii) we use higher numerical precision in computing the coefficients of the series. Then we introduce a new method of series composition, by using action-angle variables, that allows the calculation of the asymptotic manifolds up to an a arbitrarily large extent. This is the first case of an analytic development that allows the computation of the invariant manifolds and their intersections in a Hamiltonian system for an extent long enough to allow the study of homoclinic chaos by analytical means.

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