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  "body": "\n## Definition\n\nA *hyperbolic plane* is a model of the axioms of [[absolute geometry|VKFPCSRNDH]], including Dedekind's axiom of continuity, in which the hyperbolic parallel axiom holds.\nThat axiom says: for each line $\\ell$ and each point $P$ not on $\\ell$, at least two distinct lines through $P$ do not meet $\\ell$.\n*Hyperbolic geometry* is the study of the hyperbolic plane and of its higher-dimensional analogues.\n\n## Remarks\n\nAny two hyperbolic planes in this sense are isomorphic, so hyperbolic geometry is a [[non-Euclidean geometry|SPCYMFN5V2]] with a single model up to isomorphism.\nIn differential geometry, the hyperbolic $n$-space $\\mathbb{H}^n$ is the complete simply connected [[Riemannian manifold|7CBT4SM83Y]] of dimension $n$ with constant sectional curvature $-1$.\nFor $n = 2$ this is a surface of [[Gaussian curvature|SQVQ5DQT6W]] $-1$, and it is a hyperbolic plane in the axiomatic sense.\nIn it, a triangle with angles $\\alpha, \\beta, \\gamma$ has area $\\pi - \\alpha - \\beta - \\gamma$.\n\nExample: the [[Poincaré half-plane model|RHKSMPBSQ1]] $\\set{(x, y) : y \u003e 0}$ with the metric $(dx^2 + dy^2)/y^2$ satisfies the axioms.\nIts lines are the vertical half-lines and the semicircles centred on the $x$-axis.\n\nNon-example: the Euclidean plane satisfies the axioms of absolute geometry.\nIt fails the hyperbolic parallel axiom, because each point off a line lies on exactly one parallel.\n",
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