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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>.
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| ==Examples==
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| All [[compact space|compact]] manifolds and all [[homogeneous space|homogeneous]] manifolds are geodesically complete.
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| [[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.
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| 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.
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| ==Path-connectedness, completeness and geodesic completeness==
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| 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.
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| ==References==
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| * {{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''.
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| {{DEFAULTSORT:Complete Manifold}}
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| [[Category:Riemannian geometry]]
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| [[Category:Manifolds]]
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Latest revision as of 12:41, 10 April 2014
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