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Sur les relations entre la topologie de contact et la dynamique de champs de Reeb

机译:接触拓扑与Reeb场动力学之间的关系

摘要

In this thesis we study the relations between the contact topological properties of contact manifolds and the dynamics of Reeb flows. On the first part of the thesis, we establish a relation between the growth of the cylindrical contact homology of a contact manifold and the topological entropy of Reeb flows on this manifold. We build on this to show in Chapter 6 that if a contact manifold M admits a hypertight contact form A for which the cylindrical contact homology has exponential homotopical growth rate, then the Reeb flow of every contact form on M has positive topological entropy. Using this result, we exhibit in Chapter 8 and 9 numerous new examples of contact 3-manifolds on which every Reeb flow has positive topological entropy. On Chapter 10 we present a joint result with Chris Wendl that gives a dynamical obstruction for contact 3-manifold to be planar. We then use the obstruction to show that a contact 3-manifold that possesses a Reeb flow that is a transversely orientable Anosov flow, cannot be planar. On Chapter 11 we study the topological entropy for Reeb flows on spherizations. The result we obtain is a refinement of a result of Macarini and Schlenk, that states that every Reeb flow on the unit tangent bundle U of a high genus surface S has positive topological entropy. We show that for any Reeb flow on U, the omega-limit of almost every Legendrian fiber is a compact invariant set on which the dynamics has positive topological entropy.
机译:本文研究了接触流形的接触拓扑特性与Reeb流动动力学之间的关系。在论文的第一部分,我们建立了接触歧管的圆柱接触同源性的增长与该歧管上Reeb流的拓扑熵之间的关系。我们以此为基础在第6章中证明,如果接触流形M接受超紧密接触形式A,对于该接触形式A,圆柱形接触同源性具有指数同位增长速度,则M上每个接触形式的Reeb流都具有正拓扑熵。使用这个结果,我们在第8章和第9章中展示了接触3流形的许多新示例,其中每个Reeb流都具有正拓扑熵。在第10章中,我们提出了与克里斯·温德尔(Chris Wendl)的联合结果,该结果为接触3流形为平面提供了动力障碍。然后,我们使用障碍物来显示具有Reeb流(即横向可定向Anosov流)的接触3流形不能为平面。在第11章,我们研究了球化过程中Reeb流的拓扑熵。我们获得的结果是Macarini和Schlenk结果的改进,该结果表明,高属曲面S的单位切线束U上的每个Reeb流都具有正拓扑熵。我们表明,对于U上的任何Reeb流,几乎每个Legendrian纤维的Ω极限都是一个紧凑的不变集,其动力学具有正拓扑熵。

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