A Cauchy hypersurface is an achronal hypersurface met exactly once by every inextendible timelike curve. Its topology records the global spatial topology of a globally hyperbolic spacetime.
The set of events for which every past-inextendible causal curve meets . This causal characterization permits an initial sign condition on a null geodesic congruence to propagate throughout the regular region by integrating a focusing inequality from .
The future or past Cauchy horizon of a partial Cauchy hypersurface is the boundary of the region whose physical evolution is determined by data on that hypersurface. Crossing it can destroy uniqueness of the maximal globally hyperbolic development.
A complete Cauchy hypersurface in Minkowski spacetime, such as , has full domain of dependence and empty Cauchy horizons. This does not forbid horizons for a non-Cauchy initial surface in the same spacetime. The smooth edgeless spacelike hyperboloid , , has domain of dependence and a past Cauchy horizon on the future light cone of the origin. Every causal curve starting inside that cone crosses the hyperboloid in the direction needed for dependence: passes through , while a null generator of the cone never meets it. The time-reversed hyperboloid gives the analogous future horizon.
Near a nondegenerate outgoing inner Cauchy horizon, a regular null coordinate behaves as , where is the magnitude of the inner-horizon surface gravity. Transforming stress components gives . Even a small power-law tail can therefore cause an unbounded locally measured flux, motivating mass inflation.
Mass inflation is the growth of the interior effective mass and curvature near an inner Cauchy horizon under suitably perturbed black-hole data. It can obstruct regular spacetime extensions that exist for an exact Reissner-Nordstrom spacetime. The extension regularity matters: curvature blowup alone does not rule out every continuous-metric extension.
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A **Cauchy surface** is a concept used in the context of general relativity and differential geometry, particularly in the study of spacetime. It is a type of hypersurface that has important implications for the determination of the evolution of physical fields and signals in spacetime.