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・ Hypercompe ochreator
・ Hypercompe ockendeni
・ Hypercompe ocularia
・ Hypercompe orbiculata
・ Hypercompe orsa
・ Hypercompe oslari
・ Hypercompe permaculata
・ Hypercompe perplexa
・ Hypercompe persephone
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・ Hypercompe pertestacea
・ Hypercompe peruvensis
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・ Hyperbolic law of cosines
・ Hyperbolic link
Hyperbolic manifold
・ Hyperbolic motion
・ Hyperbolic motion (relativity)
・ Hyperbolic navigation
・ Hyperbolic orthogonality
・ Hyperbolic partial differential equation
・ Hyperbolic plane (disambiguation)
・ Hyperbolic point
・ Hyperbolic quaternion
・ Hyperbolic secant distribution
・ Hyperbolic sector
・ Hyperbolic set
・ Hyperbolic space
・ Hyperbolic spiral
・ Hyperbolic structure


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Hyperbolic manifold : ウィキペディア英語版
Hyperbolic manifold
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.

==Rigorous Definition==
A hyperbolic n-manifold is a complete Riemannian n-manifold of constant sectional curvature -1.
Every complete, connected, simply-connected manifold of constant negative curvature −1 is isometric to the real hyperbolic space \mathbb^n. As a result, the universal cover of any closed manifold M of constant negative curvature −1 is \mathbb^n. Thus, every such M can be written as \mathbb^n/\Gamma where Γ is a torsion-free discrete group of isometries on \mathbb^n. That is, Γ is a discrete subgroup of SO^+_\mathbb. The manifold has finite volume if and only if Γ 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 ''n-1''-manifold and the closed half-ray. The manifold is of finite volume if and only if its thick part is compact.
For n>2 the hyperbolic structure on a ''finite volume'' hyperbolic ''n''-manifold is unique by Mostow rigidity and so geometric invariants are in fact topological invariants.

抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)
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