- Space form
In
mathematics , a space form is a completeRiemannian manifold "M" of constantsectional curvature "K".Reduction to generalized crystallography
It is a theorem of Riemannian geometry that the
universal cover of an n dimensional space form M^n with curvature K = -1 is isometric to H^n,hyperbolic space , with curvature K = 0 is isometric to R^n, Euclidean n-space, and with curvature K = +1 is isometric to S^n, the n-dimensional sphere of points distance 1 from the origin in R^{n+1}.By rescaling the
Riemannian metric on H^n, we may create a space M_K of constant curvature K for any K < 0. Similarly, by rescaling the Riemannian metric on S^n, we may create a space M_K of constant curvature K for any K > 0. Thus the universal cover of a space form M with constant curvature K is isometric to M_K.This reduces the problem of studying space form to studying discrete groups of isometries Gamma of M_K which act properly discontinuously. Note that the
fundamental group of M, pi_1(M), will be isomorphic to Gamma. Groups acting in this manner on R^n are calledcrystallographic group s. Groups acting in this manner on H^2 and H^3 are calledFuchsian group s andKleinian group s, respectively.pace form problem
The space form problem is a conjecture stating that any two compact aspherical Riemannian manifolds with isomorphic
fundamental group s are homeomorphic.The possible extensions are limited. One might wish to conjecture that the manifolds are isometric, but rescaling the
Riemannian metric on a compact aspherical Riemannian manifold preserves the fundamental group and shows this to be false. One might also wish to conjecture that the manifolds are diffeomorphic, butJohn Milnor 'sexotic sphere s are all homeomorphic and hence have isomorphic fundamental group, showing this to be false.ee also
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Borel conjecture
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