Complete manifold

{{Short description|Riemannian manifold in which geodesics extend infinitely in all directions}}

In mathematics, a complete manifold (or geodesically complete manifold) {{Mvar|M}} is a (pseudo-) Riemannian manifold for which, starting at any point {{Math|p}}, there are straight paths extending infinitely in all directions.

Formally, a manifold M is (geodesically) complete if for any maximal geodesic \ell : I \to M, it holds that I=(-\infty,\infty).{{sfn|Lee|2018|p=131}} A geodesic is maximal if its domain cannot be extended.

Equivalently, M is (geodesically) complete if for all points p \in M, the exponential map at p is defined on T_pM, the entire tangent space at p.{{sfn|Lee|2018|p=131}}

Hopf–Rinow theorem

{{Main|Hopf–Rinow theorem}}

The Hopf–Rinow theorem gives alternative characterizations of completeness. Let (M,g) be a connected Riemannian manifold and let d_g : M \times M \to [0,\infty) be its Riemannian distance function.

The Hopf–Rinow theorem states that (M,g) is (geodesically) complete if and only if it satisfies one of the following equivalent conditions:{{sfn|do Carmo|1992|p=146-147}}

  • The metric space (M,d_g) is complete (every d_g-Cauchy sequence converges),
  • All closed and bounded subsets of M are compact.

Examples and non-examples

Euclidean space \mathbb{R}^n, the sphere \mathbb{S}^n, and the tori \mathbb{T}^n (with their natural Riemannian metrics) are all complete manifolds.

All compact Riemannian manifolds and all homogeneous manifolds are geodesically complete. All symmetric spaces are geodesically complete.

= Non-examples =

File:Punctured plane is not geodesically complete.svg

A simple example of a non-complete manifold is given by the punctured plane \mathbb{R}^2 \smallsetminus \lbrace 0 \rbrace (with its induced metric). Geodesics going to the origin cannot be defined on the entire real line. By the Hopf–Rinow theorem, we can alternatively observe that 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.

There exist non-geodesically complete compact pseudo-Riemannian (but not Riemannian) manifolds. An example of this is the Clifton–Pohl torus.

In the theory of general relativity, which describes gravity in terms of a pseudo-Riemannian geometry, many important examples of geodesically incomplete spaces arise, e.g. non-rotating uncharged black-holes or cosmologies with a Big Bang. The fact that such incompleteness is fairly generic in general relativity is shown in the Penrose–Hawking singularity theorems.

Extendibility

If M is geodesically complete, then it is not isometric to an open proper submanifold of any other Riemannian manifold. The converse does not hold.{{sfn|do Carmo|1992|p=145}}

References

= Notes =

{{reflist}}

= Sources =

  • {{citation

| last = do Carmo |first=Manfredo Perdigão|authorlink=Manfredo do Carmo

| title = Riemannian geometry

| series = Mathematics: theory and applications

| publisher = Birkhäuser

| location = Boston

| year = 1992

| pages = xvi+300

| isbn = 0-8176-3490-8

}}

  • {{Cite book|last=Lee|first=John|title=Introduction to Riemannian Manifolds|series=Graduate Texts in Mathematics|publisher=Springer International Publishing AG|year=2018}}
  • {{Cite book|title=Semi-Riemannian Geometry|last=O'Neill|first=Barrett|publisher=Academic Press|year=1983|isbn=0-12-526740-1|at=Chapter 3}}

{{Manifolds}}

{{Riemannian geometry}}

{{DEFAULTSORT:Complete Manifold}}

Category:Differential geometry

Category:Geodesic (mathematics)

Category:Manifolds

Category:Riemannian geometry