Monotone homotopies and contracting discs on Riemannian surfaces

Monotone homotopies and contracting discs on Riemannian surfaces
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黎曼曲面上的单调同伦和收缩圆

DOI:
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发表时间:
2013
期刊:
Journal of Topology and Analysis (JTA)
影响因子:
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通讯作者:
R. Rotman
R. Rotman
中科院分区:
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文献类型:
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作者:
Gregory R. Chambers;R. Rotman

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单调同伦是由两两不相交的简单闭曲线组成的同伦。在本文中,我们证明了单调同伦的一个“胶合”定理,我们表明,两个单调同伦,有适当的重叠可以替换为一个单一的单调同伦。用于证明这个定理的思想在[G. R. Chambers和Y. Liokumovich,Existence of minimal hypersurfaces in complete manifolds of finite volume,arXiv:1609.04058]证明了一个类似的结果循环,这形成了一个关键的一步,他们的证明存在极小曲面在完整的非紧流形的有限体积。我们还表明,如果单调同伦存在,那么通过短曲线的不动点收缩存在。特别地,假设[公式:见正文]是黎曼曲面的一条简单闭曲线,并且存在覆盖一个圆盘的单调收缩,该圆盘由长度为[公式:见正文]的曲线构成[公式:见正文]的边界。如果[公式:见正文]和[公式:见正文],则存在一个同伦,它将[Formula:see text]收缩到[Formula:see text]上的循环,这些循环基于[Formula:see text],长度由[Formula:see text]限定,其中[Formula:see text]是曲面的直径。如果曲面是一个圆盘,并且[Formula:see text]是这个圆盘的边界,那么这个边界可以改进为[Formula:see text]。
A monotone homotopy is a homotopy composed of simple closed curves which are also pairwise disjoint. In this paper, we prove a “gluing” theorem for monotone homotopies; we show that two monotone homotopies which have appropriate overlap can be replaced by a single monotone homotopy. The ideas used to prove this theorem are used in [G. R. Chambers and Y. Liokumovich, Existence of minimal hypersurfaces in complete manifolds of finite volume, arXiv:1609.04058] to prove an analogous result for cycles, which forms a critical step in their proof of the existence of minimal surfaces in complete non-compact manifolds of finite volume. We also show that, if monotone homotopies exist, then fixed point contractions through short curves exist. In particular, suppose that [Formula: see text] is a simple closed curve of a Riemannian surface, and that there exists a monotone contraction which covers a disc which [Formula: see text] bounds consisting of curves of length [Formula: see text]. If [Formula: see text] and [Formula: see text], then there exists a homotopy that contracts [Formula: see text] to [Formula: see text] over loops that are based at [Formula: see text] and have length bounded by [Formula: see text], where [Formula: see text] is the diameter of the surface. If the surface is a disc, and if [Formula: see text] is the boundary of this disc, then this bound can be improved to [Formula: see text].