Myers's theorem

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Short description: Bounds the length of geodetic segments in Riemannian manifolds based in Ricci curvature

Myers's theorem, also known as the Bonnet–Myers theorem, is a celebrated, fundamental theorem in the mathematical field of Riemannian geometry. It was discovered by Sumner Byron Myers in 1941. It asserts the following:

Let (M,g) be a complete Riemannian manifold of dimension n whose Ricci curvature satisfies Ric(g)(n1)k for some positive real number k. Then any two points of M can be joined by a geodesic segment of length at most πk.

In the special case of surfaces, this result was proved by Ossian Bonnet in 1855. For a surface, the Gauss, sectional, and Ricci curvatures are all the same, but Bonnet's proof easily generalizes to higher dimensions if one assumes a positive lower bound on the sectional curvature. Myers' key contribution was therefore to show that a Ricci lower bound is all that is needed to reach the same conclusion.

Corollaries

The conclusion of the theorem says, in particular, that the diameter of (M,g) is finite. The Hopf-Rinow theorem therefore implies that M must be compact, as a closed (and hence compact) ball of radius π/k in any tangent space is carried onto all of M by the exponential map.

As a very particular case, this shows that any complete and noncompact smooth Riemannian manifold which is Einstein must have nonpositive Einstein constant.

Consider the smooth universal covering map π:NM. One may consider the Riemannian metric π*g on N. Since π is a local diffeomorphism, Myers' theorem applies to the Riemannian manifold (N*g) and hence N is compact. This implies that the fundamental group of Mis finite.

Cheng's diameter rigidity theorem

The conclusion of Myers' theorem says that for any p,qM, one has dg(p,q) ≤ π/k. In 1975, Shiu-Yuen Cheng proved:

Let (M,g) be a complete and smooth Riemannian manifold of dimension n. If k is a positive number with Ricg ≥ (n-1)k, and if there exists p and q in M with dg(p,q) = π/k, then (M,g) is simply-connected and has constant sectional curvature k.

See also

References