Hyperbolic manifold

Space where every point locally resembles a hyperbolic space
In mathematics, a hyperbolic manifold is a space where every point looks locally like hyperbolic space of some dimension. They are especially studied in dimensions 2 and 3, where they are called hyperbolic surfaces and hyperbolic 3 manifolds, respectively. In these dimensions, they are important because most manifolds can be made into a hyperbolic manifold by a homeomorphism. This is a consequence of the uniformization theorem for surfaces and the geometrization theorem for 3 manifolds proved by Perelman.

A hyperbolic manifold is a complete Riemannian manifold of constant sectional curvature
Every complete, connected, simply connected manifold of constant negative curvature is isometric to the real hyperbolic space As a result, the universal cover of any closed manifold of constant negative curvature is Thus, every such can be written as where is a torsion free discrete group of isometries on That is, is a discrete subgroup of The manifold has finite volume if and only if is a lattice. Its thick–thin decomposition has a thin part consisting of tubular neighborhoods of closed geodesics and ends which are the product of a Euclidean manifold and the closed half ray. The manifold is of finite volume if and only if its thick part is compact.

The simplest example of a hyperbolic manifold is hyperbolic space, as each point in hyperbolic space has a neighborhood isometric to hyperbolic space. A simple non trivial example, however, is the once punctured torus. This is an example of an (Isom , ) manifold. This can be formed by taking an ideal rectangle in – that is, a rectangle where the vertices are on the boundary at infinity, and thus don't exist in the resulting manifold – and identifying opposite images. In a similar fashion, we can construct the thrice punctured sphere, shown below, by gluing two ideal triangles together. This also shows how to draw curves on the surface – the black line in the diagram becomes the closed curve when the green edges are glued together. As we are working with a punctured sphere, the colored circles in the surface – including their boundaries – are not part of the surface, and hence are represented in the diagram as ideal vertices. Many knots and links, including some of the simpler knots such as the figure eight knot and the Borromean rings, are hyperbolic, and so the complement of the knot or link in is a hyperbolic 3 manifold of finite volume.

For the hyperbolic structure on a finite volume hyperbolic manifold is unique by Mostow rigidity and so geometric invariants are in fact topological invariants. One of these geometric invariants used as a topological invariant is the hyperbolic volume of a knot or link complement, which can allow us to distinguish two knots from each other by studying the geometry of their respective manifolds.