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In general relativity, the cosmic censorship hypothesis (CCH) is a conjecture about the nature of singularities in spacetime. An illustration of a rotating black hole at the center of a galaxy General relativity (GR) (aka general theory of relativity (GTR)) is the geometrical theory of gravitation published by Albert Einstein in 1915/16. ...
A gravitational singularity (sometimes spacetime singularity) is, approximately, a place where quantities which are used to measure the gravitational field become infinite. ...
In physics, spacetime is any mathematical model that combines space and time into a single construct called the space-time continuum. ...
Singularities that arise in the solutions of Einstein's equations are typically hidden within event horizons, and therefore cannot be seen from the rest of spacetime. Singularities which are not so hidden are called naked. The weak cosmic censorship hypothesis conjectures that no naked singularities other than the Big Bang singularity exist in the universe. This article or section is in need of attention from an expert on the subject. ...
In physics, the Einstein field equation or Einstein equation is a differential equation in Einsteins theory of general relativity. ...
For the science fiction film, see Event Horizon (film). ...
blah blah blah, some people believe God made the universe and that is all there is. ...
According to the Big Bang model, the universe emerged from an extremely dense and hot state. ...
The Universe is defined as the summation of all particles and energy that exist and the space-time in which all events occur. ...
Basics
The fundamental concern is that since the physical behavior of singularities is unknown, if singularities can be seen from the rest of spacetime, causality may break down, and physics may lose its predictive power. The issue cannot be avoided, since according to the Penrose-Hawking singularity theorems, singularities are inevitable in physically reasonable situations. Still, in the absence of naked singularities, the universe is deterministic — it's possible to predict the entire evolution of the universe (possibly excluding some finite regions of space hidden inside event horizons of singularities), knowing only its condition at a certain moment of time (more precisely, everywhere on a spacelike 3-dimensional hypersurface, called the Cauchy surface). Failure of the cosmic censorship hypothesis leads to the failure of determinism, because it is impossible to predict the behavior of space-time in the causal future of a singularity. Cosmic censorship is not merely a problem of formal interest, some form of it is assumed whenever black hole event horizons are mentioned. It has been suggested that this article be split into multiple articles accessible from a disambiguation page. ...
A magnet levitating above a high-temperature superconductor demonstrates the Meissner effect. ...
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Determinism is the philosophical proposition that every event, including human cognition and behavior, decision and action, is causally determined by an unbroken chain of prior occurrences. ...
In the context of special relativity, space-like separated points (or events) in spacetime have a spacetime interval less than 0 (see sign convention). ...
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Simulated view of a black hole in front of the Milky Way. ...
The hypothesis was first formulated by Roger Penrose in 1969, and it is not stated in a completely formal way. In a sense it is more of a research program proposal: part of the research is to find a proper formal statement that is physically reasonable and that can be proved to be true or false (and that is sufficiently general to be interesting). Sir Roger Penrose, OM, FRS (born 8 August 1931) is an English mathematical physicist and Emeritus Rouse Ball Professor of Mathematics at the Mathematical Institute, University of Oxford and Emeritus Fellow of Wadham College. ...
Weak and strong cosmic censorship hypothesis There are currently two versions of this hypothesis, known as "weak" and "strong". - Weak cosmic censorship hypothesis asserts that causal future of any singularity can not extend to future null infinity. In essence, it says that singularities may be observable, but any observer who has observed a singularity is destined to fall into it eventually. As such, for classical general relativity to be a complete theory, an observer of a naked singularity should still have a theory to explain what is observed.
- A stronger version of the hypothesis (known as the strong cosmic censorship hypothesis) asserts that no singularity is ever visible to any observer.
Problems with the concept There are a number of difficulties in formalizing the hypothesis: - There are technical difficulties with properly formalizing the notion of a singularity.
- It is not difficult to construct spacetimes which have naked singularities, but which are not "physically reasonable;" the canonical example of such a spacetime is perhaps the "superextremal" M < | Q | Reissner-Nordstrom solution, which contains a singularity at r = 0 that is not surrounded by a horizon. A formal statement needs some set of hypotheses which exclude these situations.
- Caustics may occur in simple models of gravitational collapse, and can appear to lead to singularities. These have more to do with the simplified models of bulk matter used, and in any case have nothing to do with general relativity, and need to be excluded.
- Computer models of gravitational collapse have shown that naked singularities can arise, but these models rely on very special circumstances (such as spherical symmetry). These special circumstances need to be excluded by some hypothesis.
In 1991, John Preskill and Kip Thorne bet against Stephen Hawking that the hypothesis was false (Thorne-Hawking-Preskill bet). They won the bet (for an encyclopedia of the winner's choice) due to the discovery of the special situations just mentioned. Hawking later reformulated the bet to exclude those technicalities.[citation needed] The revised bet is still open. In physics and astronomy, a Reissner-Nordstrøm black hole is a black hole that carries electric charge , no angular momentum, and mass . ...
This article may be too technical for most readers to understand. ...
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Kip S. Thorne Professor Kip Stephen Thorne, Ph. ...
Stephen William Hawking, CH, CBE, FRS, FRSA, (born 8 January 1942) is a British theoretical physicist. ...
In 1997, the physics theorists Kip Thorne, Stephen Hawking and John Preskill made a public bet on the outcome of the black hole information paradox: Thorne and Hawking argued that since general relativity made it impossible for black holes to radiate, and lose information, the mass-energy and information carried...
Counter-example An exact solution to the scalar-Einstein equations Rab = 2φaφb which forms a counter example to many formulations of the cosmic censorship hypothesis was found by Mark D. Roberts in 1985  where σ is a constant.
References - Earman, John: Bangs, Crunches, Whimpers, and Shrieks: Singularities and Acausalities in Relativistic Spacetimes (1995), see especially chapter 2 (ISBN 0-19-509591-X)
- Roberts, Mark D. : Scalar Field Counter-Examples to the Cosmic Censorship Hypothesis. Gen.Rel.Grav.21(1989)907-939.
- Penrose, Roger: "The Question of Cosmic Censorship", Chapter 5 in Black Holes and Relativistic Stars, Robert Wald (editor), (1994) (ISBN 0-226-87034-0)
- Penrose, Roger: "Singularities and time-asymmetry", Chapter 12 in General Relativity: An Einstein Centenary Survey (Hawking and Israel, editors), (1979), see especially section 12.3.2, pp. 617-629 (ISBN 0-521-22285-0)
- Shapiro, S. L., and Teukolsky, S. A.: "Formation of Naked Singularities: The Violation of Cosmic Censorship", Physical Review Letters 66, 994-997 (1991)
- Wald, Robert, General Relativity, 299-308 (1984) (ISBN 0-226-87033-2)
See also This article or section cites very few or no references or sources. ...
The chronology protection conjecture is a conjecture by the physicist Professor Stephen Hawking that the laws of physics are such as to prevent time travel (closed timelike curves) on all but sub-microscopic scales. ...
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