Zahorski theorem: Difference between revisions

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In [[mathematics]], a '''complete manifold''' (or '''geodesically complete manifold''') is a ([[Pseudo-Riemannian manifold|pseudo]]-) [[Riemannian manifold]] for which every maximal (inextendible) [[geodesic]] is defined on <math>\mathbb{R}</math>.
 
==Examples==
All [[compact space|compact]] manifolds and all [[homogeneous space|homogeneous]] manifolds are geodesically complete.
 
[[Euclidean space]] <math>\mathbb{R}^{n}</math>, the [[sphere]]s <math>\mathbb{S}^{n}</math> and the [[torus|tori]] <math>\mathbb{T}^{n}</math> (with their natural [[Riemannian metric]]s) are all complete manifolds.
 
A simple example of a non-complete manifold is given by the punctured plane <math>M := \mathbb{R}^{2} \setminus \{ 0 \}</math> (with its induced metric). Geodesics going to the origin cannot be defined on the entire real line.
 
==Path-connectedness, completeness and geodesic completeness==
It can be shown that a finite dimensional [[Connected space#Path connectedness|path-connected]] Riemannian manifold is a [[complete metric space]] (with respect to the [[Riemannian_manifold#Riemannian_manifolds_as_metric_spaces_2|Riemannian distance]]) if and only if it is geodesically complete. This is the [[Hopf–Rinow theorem]]. This theorem does not hold for infinite dimensional manifolds. The example of a non-complete manifold (the punctured plane) given above fails to be geodesically complete because, although it is path-connected, it is not a complete metric space: any sequence in the plane converging to the origin is a non-converging Cauchy sequence in the punctured plane.
 
==References==
* {{Citation | last1=O'Neill | first1=Barrett | title=Semi-Riemannian Geometry | publisher=[[Academic Press]] | isbn=0-12-526740-1 | year=1983}}. ''See chapter 3, pp. 68''.
 
{{DEFAULTSORT:Complete Manifold}}
[[Category:Riemannian geometry]]
[[Category:Manifolds]]

Latest revision as of 12:41, 10 April 2014

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