Topological censorship, the Glossary
The topological censorship theorem (if valid) states that general relativity does not allow an observer to probe the topology of spacetime: any topological structure collapses too quickly to allow light to traverse it.[1]
Table of Contents
7 relations: Asymptotically flat spacetime, Causal structure, Energy condition, General relativity, Globally hyperbolic manifold, Null infinity, Sergey Krasnikov.
- Lorentzian manifolds
Asymptotically flat spacetime
An asymptotically flat spacetime is a Lorentzian manifold in which, roughly speaking, the curvature vanishes at large distances from some region, so that at large distances, the geometry becomes indistinguishable from that of Minkowski spacetime. Topological censorship and asymptotically flat spacetime are Lorentzian manifolds.
See Topological censorship and Asymptotically flat spacetime
Causal structure
In mathematical physics, the causal structure of a Lorentzian manifold describes the causal relationships between points in the manifold. Topological censorship and causal structure are Lorentzian manifolds.
See Topological censorship and Causal structure
Energy condition
In relativistic classical field theories of gravitation, particularly general relativity, an energy condition is a generalization of the statement "the energy density of a region of space cannot be negative" in a relativistically phrased mathematical formulation.
See Topological censorship and Energy condition
General relativity
General relativity, also known as the general theory of relativity and Einstein's theory of gravity, is the geometric theory of gravitation published by Albert Einstein in 1915 and is the current description of gravitation in modern physics.
See Topological censorship and General relativity
Globally hyperbolic manifold
In mathematical physics, global hyperbolicity is a certain condition on the causal structure of a spacetime manifold (that is, a Lorentzian manifold). Topological censorship and Globally hyperbolic manifold are relativity stubs.
See Topological censorship and Globally hyperbolic manifold
Null infinity
In theoretical physics, null infinity is a region at the boundary of asymptotically flat spacetimes. Topological censorship and null infinity are Lorentzian manifolds.
See Topological censorship and Null infinity
Sergey Krasnikov
Serguei Vladilenovich Krasnikov (Серге́й Владиле́нович Кра́сников; 1961) is a Russian physicist.
See Topological censorship and Sergey Krasnikov
See also
Lorentzian manifolds
- Alcubierre drive
- Asymptotically flat spacetime
- Bel decomposition
- Bondi–Metzner–Sachs group
- Cauchy surface
- Causal structure
- Causality conditions
- Christoffel symbols
- Classification of electromagnetic fields
- Clifton–Pohl torus
- Closed timelike curve
- Congruence (general relativity)
- Gaussian polar coordinates
- Geroch's splitting theorem
- Gravitational singularity
- Gullstrand–Painlevé coordinates
- Isotropic coordinates
- Kretschmann scalar
- Kruskal–Szekeres coordinates
- Kundt spacetime
- Light cone
- McVittie metric
- Minkowski space
- Null hypersurface
- Null infinity
- Penrose diagram
- Pseudo-Euclidean space
- Pseudo-Riemannian manifold
- Schwarzschild coordinates
- Spacetime symmetries
- Spacetime topology
- Spherically symmetric spacetime
- Static spacetime
- Stationary spacetime
- Timelike homotopy
- Timelike simply connected
- Topological censorship
- Vanishing scalar invariant spacetime
- Wormhole