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Hadamard manifold

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In mathematics, a Hadamard manifold, named after Jacques Hadamard — more often called a Cartan–Hadamard manifold, after Élie Cartan — is a Riemannian manifold ( M , g ) {\displaystyle (M,g)} that is complete and simply connected and has everywhere non-positive sectional curvature. By Cartan–Hadamard theorem all Cartan–Hadamard manifolds are diffeomorphic to the Euclidean space R n . {\displaystyle \mathbb {R} ^{n}.} Furthermore it follows from the Hopf–Rinow theorem that every pairs of points in a Cartan–Hadamard manifold may be connected by a unique geodesic segment. Thus Cartan–Hadamard manifolds are some of the closest relatives of R n . {\displaystyle \mathbb {R} ^{n}.}

Examples

The Euclidean space R n {\displaystyle \mathbb {R} ^{n}} with its usual metric is a Cartan–Hadamard manifold with constant sectional curvature equal to 0. {\displaystyle 0.}

Standard n {\displaystyle n} -dimensional hyperbolic space H n {\displaystyle \mathbb {H} ^{n}} is a Cartan–Hadamard manifold with constant sectional curvature equal to 1. {\displaystyle -1.}

Properties

In Cartan-Hadamard manifolds, the map exp p : T M p M {\displaystyle \exp _{p}:\operatorname {T} M_{p}\to M} is a diffeomorphism for all p M . {\displaystyle p\in M.}

See also

References

  1. Li, Peter (2012). Geometric Analysis. Cambridge University Press. p. 381. doi:10.1017/CBO9781139105798. ISBN 9781107020641.
  2. Lang, Serge (1989). Fundamentals of Differential Geometry, Volume 160. Springer. pp. 252–253. ISBN 9780387985930.
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