ONE-DIMENSIONAL DYNAMICS
ONE-DIMENSIONAL DYNAMICS
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DOI:
10.1007/3-540-26844-8_2
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发表时间:
2013
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影响因子:
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通讯作者:
Michał Misiurewicz
中科院分区:
文献类型:
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作者:
Michał Misiurewicz
The study of one-dimensional transformations is a classical subject going back to Poincare. Here these systems interest us primarily as models for dynamical behavior in higher dimensions. We focus on continuous smooth maps with finitely many critical (multimodal maps) exhibiting complicated behavior. This area of Dynamics has been experiencing remarkable progress since the late seventies. Recent surveys have been written by Graczyk, Swiatek [199] and Lyubich [275], and the book of de Melo, van Strien [147] remains the fundamental expository text on the subject. Hyperbolicity is the simplest form of behavior for one-dimensional maps. We recall the definition and characterization in Section 2.1. A special feature of these maps is that the dynamics is always very much hyperbolic far from critical points, as we comment upon in Section 2.2. It had been conjectured for a long time, and was only recently established, that hyperbolic dynamics is Cr-dense among these maps. This remarkable fact, which has no counterpart in higher dimensions, is discussed in Section 2.3. On the other hand, the presence of critical points may also give rise to non-uniform hyperbolicity persistently in parameter space. This is the theme of Section 2.4. Most of the recent progress in this area has been driven by the effort to understand the renormalization operator, and explain the universality phenomena discovered by Coullet, Tresser [138] and Feigenbaum [181] in cascades of bifurcations. See Section 2.5. Among the main recent achievements, let us mention the proof that almost all maps inside typical families of unimodal maps are either hyperbolic (regular) or chaotic (stochastic) and, in either case, stochastically stable. This is discussed in Section 2.6.