A gravitational singularity, spacetime singularity or simply singularity is a location in spacetime where the mass and gravitational field of a celestial body is predicted to become infinite by general relativity in a way that does not depend on the coordinate system. The quantities used to measure gravitational field strength are the scalar invariant curvatures of spacetime, which includes a measure of the density of matter. Since such quantities become infinite at the singularity, the laws of normal spacetime break down.[1][2]

Gravitational singularities are mainly considered in the context of general relativity, where density apparently becomes infinite at the center of a black hole, and within astrophysics and cosmology as the earliest state of the universe during the Big Bang. Physicists are undecided whether the prediction of singularities means that they actually exist (or existed at the start of the Big Bang), or that current knowledge is insufficient to describe what happens at such extreme densities.

General relativity predicts that any object collapsing beyond a certain point (for stars this is the Schwarzschild radius) would form a black hole, inside which a singularity (covered by an event horizon) would be formed.[3] The Penrose–Hawking singularity theorems define a singularity to have geodesics that cannot be extended in a smooth manner.[4] The termination of such a geodesic is considered to be the singularity.

The initial state of the universe, at the beginning of the Big Bang, is also predicted by modern theories to have been a singularity.[5] In this case, the universe did not collapse into a black hole, because currently-known calculations and density limits for gravitational collapse are usually based upon objects of relatively constant size, such as stars, and do not necessarily apply in the same way to rapidly expanding space such as the Big Bang. Neither general relativity nor quantum mechanics can currently describe the earliest moments of the Big Bang,[6] but in general, quantum mechanics does not permit particles to inhabit a space smaller than their wavelengths.[7]


Many theories in physics have mathematical singularities of one kind or another. Equations for these physical theories predict that the ball of mass of some quantity becomes infinite or increases without limit. This is generally a sign for a missing piece in the theory, as in the ultraviolet catastrophe, re-normalization, and instability of a hydrogen atom predicted by the Larmor formula.

Some theories, such as the theory of loop quantum gravity, suggest that singularities may not exist.[8] This is also true for such classical unified field theories as the Einstein–Maxwell–Dirac equations. The idea can be stated in the form that due to quantum gravity effects, there is a minimum distance beyond which the force of gravity no longer continues to increase as the distance between the masses becomes shorter, or alternatively that interpenetrating particle waves mask gravitational effects that would be felt at a distance.

There are different types of singularities, each with different physical features which have characteristics relevant to the theories from which they originally emerged, such as the different shape of the singularities, conical and curved. They have also been hypothesized to occur without Event Horizons, structures which delineate one spacetime section from another in which events cannot affect past the horizon; these are called naked.

A conical singularity occurs when there is a point where the limit of every diffeomorphism invariant quantity is finite, in which case spacetime is not smooth at the point of the limit itself. Thus, spacetime looks like a cone around this point, where the singularity is located at the tip of the cone. The metric can be finite everywhere coordinate system is used.

An example of such a conical singularity is a cosmic string and a Schwarzschild black hole.[9]
A simple illustration of a non-spinning black hole and its singularity

Solutions to the equations of general relativity or another theory of gravity (such as supergravity) often result in encountering points where the metric blows up to infinity. However, many of these points are completely regular, and the infinities are merely a result of using an inappropriate coordinate system at this point. In order to test whether there is a singularity at a certain point, one must check whether at this point diffeomorphism invariant quantities (i.e. scalars) become infinite. Such quantities are the same in every coordinate system, so these infinities will not "go away" by a change of coordinates.

An example is the Schwarzschild solution that describes a non-rotating, uncharged black hole. In coordinate systems convenient for working in regions far away from the black hole, a part of the metric becomes infinite at the event horizon. However, spacetime at the event horizon is regular. The regularity becomes evident when changing to another coordinate system (such as the Kruskal coordinates), where the metric is perfectly smooth. On the other hand, in the center of the black hole, where the metric becomes infinite as well, the solutions suggest a singularity exists. The existence of the singularity can be verified by noting that the Kretschmann scalar, being the square of the Riemann tensor i.e. \( R_{\mu\nu\rho\sigma}R^{\mu\nu\rho\sigma} \), which is diffeomorphism invariant, is infinite.

While in a non-rotating black hole the singularity occurs at a single point in the model coordinates, called a "point singularity", in a rotating black hole, also known as a Kerr black hole, the singularity occurs on a ring (a circular line), known as a "ring singularity". Such a singularity may also theoretically become a wormhole.[10]

More generally, a spacetime is considered singular if it is geodesically incomplete, meaning that there are freely-falling particles whose motion cannot be determined beyond a finite time, being after the point of reaching the singularity. For example, any observer inside the event horizon of a non-rotating black hole would fall into its center within a finite period of time. The classical version of the Big Bang cosmological model of the universe contains a causal singularity at the start of time (t=0), where all time-like geodesics have no extensions into the past. Extrapolating backward to this hypothetical time 0 results in a universe with all spatial dimensions of size zero, infinite density, infinite temperature, and infinite spacetime curvature.
Naked singularity

Until the early 1990s, it was widely believed that general relativity hides every singularity behind an event horizon, making naked singularities impossible. This is referred to as the cosmic censorship hypothesis. However, in 1991, physicists Stuart Shapiro and Saul Teukolsky performed computer simulations of a rotating plane of dust that indicated that general relativity might allow for "naked" singularities. What these objects would actually look like in such a model is unknown. Nor is it known whether singularities would still arise if the simplifying assumptions used to make the simulation were removed. However, it is hypothesized that light entering a singularity would similarly have its geodesics terminated, thus making the naked singularity look like a black hole.[11][12][13]

Disappearing event horizons exist in the Kerr metric, which is a spinning black hole in a vacuum, if the angular momentum ( J {\displaystyle J} J) is high enough. Transforming the Kerr metric to Boyer–Lindquist coordinates, it can be shown[14] that the coordinate (which is not the radius) of the event horizon is, \( r_{\pm }=\mu \pm (\mu ^{2}-a^{2})^{1/2} \), where \( \mu =GM/c^{2} \), and a=J/Mc. In this case, "event horizons disappear" means when the solutions are complex for \( r_{\pm } \), or \( \mu ^{2}<a^{2} \). However, this corresponds to a case where J exceeds \( {\displaystyle GM^{2}/c} \) (or in Planck units, \( {\displaystyle J>M^{2}}), \) i.e. the spin exceeds what is normally viewed as the upper limit of its physically possible values.

Similarly, disappearing event horizons can also be seen with the Reissner–Nordström geometry of a charged black hole if the charge ( Q) is high enough. In this metric, it can be shown[15] that the singularities occur at \( r_{\pm }=\mu \pm (\mu ^{2}-q^{2})^{1/2} \), where μ\( \mu =GM/c^{2} \), and \( {\displaystyle q^{2}=GQ^{2}/(4\pi \epsilon _{0}c^{4})} \). Of the three possible cases for the relative values of \( \mu \) and q, the case where \( \mu ^{2}<q^{2} \) causes both r ± {\displaystyle r_{\pm }} r_{\pm } to be complex. This means the metric is regular for all positive values of r, or in other words, the singularity has no event horizon. However, this corresponds to a case where \( {\displaystyle Q/{\sqrt {4\pi \epsilon _{0}}}} \) exceeds \( {\displaystyle M{\sqrt {G}}} \) (or in Planck units, \( {\displaystyle Q>M}) \), i.e. the charge exceeds what is normally viewed as the upper limit of its physically possible values. Also, actual astrophysical black holes are not expected to possess any appreciable charge.

A black hole possessing the lowest M value consistent with its J and Q values and the limits noted above, i.e., one just at the point of losing its event horizon, is termed extremal.
Further information: Black hole, Hawking radiation, and Entropy

Before Stephen Hawking came up with the concept of Hawking radiation, the question of black holes having entropy had been avoided. However, this concept demonstrates that black holes radiate energy, which conserves entropy and solves the incompatibility problems with the second law of thermodynamics. Entropy, however, implies heat and therefore temperature. The loss of energy also implies that black holes do not last forever, but rather evaporate or decay slowly. Black hole temperature is inversely related to mass.[16] All known black hole candidates are so large that their temperature is far below that of the cosmic background radiation, which means they will gain energy on net by absorbing this radiation. They cannot begin to lose energy on net until the background temperature falls below their own temperature. This will occur at a cosmological redshift of more than one million, rather than the thousand or so since the background radiation formed.
See also

0-dimensional singularity: magnetic monopole
1-dimensional singularity: cosmic string
2-dimensional singularity: domain wall
Fuzzball (string theory)
Penrose-Hawking singularity theorems
White hole
BKL singularity


"Blackholes and Wormholes".
Claes Uggla (2006). "Spacetime Singularities". Einstein Online. 2 (1002). Archived from the original on 2017-01-24. Retrieved 2015-10-20.
Curiel, Erik & Peter Bokulich. "Singularities and Black Holes". Stanford Encyclopedia of Philosophy. Center for the Study of Language and Information, Stanford University. Retrieved 26 December 2012.
Moulay, Emmanuel. "The universe and photons" (PDF). FQXi Foundational Questions Institute. Retrieved 26 December 2012.
Wald, p. 99
Hawking, Stephen. "The Beginning of Time". Stephen Hawking: The Official Website. Cambridge University. Retrieved 26 December 2012.
Zebrowski, Ernest (2000). A History of the Circle: Mathematical Reasoning and the Physical Universe. Piscataway NJ: Rutgers University Press. p. 180. ISBN 978-0813528984.
Rodolfo Gambini; Javier Olmedo; Jorge Pullin (2014). "Quantum black holes in Loop Quantum Gravity". Classical and Quantum Gravity. 31 (9): 095009.arXiv:1310.5996. Bibcode:2014CQGra..31i5009G. doi:10.1088/0264-9381/31/9/095009. S2CID 119247455.
Copeland, Edmund J; Myers, Robert C; Polchinski, Joseph (2004). "Cosmic F- and D-strings". Journal of High Energy Physics. 2004 (6): 013.arXiv:hep-th/0312067. Bibcode:2004JHEP...06..013C. doi:10.1088/1126-6708/2004/06/013. S2CID 140465.
If a rotating singularity is given a uniform electrical charge, a repellent force results, causing a ring singularity to form. The effect may be a stable wormhole, a non-point-like puncture in spacetime that may be connected to a second ring singularity on the other end. Although such wormholes are often suggested as routes for faster-than-light travel, such suggestions ignore the problem of escaping the black hole at the other end, or even of surviving the immense tidal forces in the tightly curved interior of the wormhole.
M. Bojowald (2008). "Loop Quantum Cosmology". Living Reviews in Relativity. 11 (4): 4. Bibcode:2008LRR....11....4B. doi:10.12942/lrr-2008-4. PMC 5253914. PMID 28163651. Archived from the original on 2015-12-21.
R. Goswami; P. Joshi (2008). "Spherical gravitational collapse in N-dimensions". Physical Review D. 76 (8): 084026.arXiv:gr-qc/0608136. Bibcode:2007PhRvD..76h4026G. doi:10.1103/PhysRevD.76.084026. S2CID 119441682.
R. Goswami; P. Joshi; P. Singh (2006). "Quantum evaporation of a naked singularity". Physical Review Letters. 96 (3): 031302.arXiv:gr-qc/0506129. Bibcode:2006PhRvL..96c1302G. doi:10.1103/PhysRevLett.96.031302. PMID 16486681. S2CID 19851285.
Hobson, et al., General Relativity an Introduction for Physicists, Cambridge University Press 2007, p. 300-305
Hobson, et al., General Relativity an Introduction for Physicists, Cambridge University Press 2007, p. 320-325

LoPresto, M. C. (2003). "Some Simple Black Hole Thermodynamics". The Physics Teacher. 41 (5): 299–301. Bibcode:2003PhTea..41..299L. doi:10.1119/1.1571268. S2CID 122758428.


Hawking, S. W.; Penrose, R. (1970), "The Singularities of Gravitational Collapse and Cosmology", Proc. R. Soc. A, 314 (1519): 529–548, Bibcode:1970RSPSA.314..529H, doi:10.1098/rspa.1970.0021 (Free access.)
Shapiro, Stuart L.; Teukolsky, Saul A. (1991). "Formation of naked singularities: The violation of cosmic censorship" (PDF). Physical Review Letters. 66 (8): 994–997. Bibcode:1991PhRvL..66..994S. doi:10.1103/PhysRevLett.66.994. PMID 10043968.
Robert M. Wald (1984). General Relativity. University of Chicago Press. ISBN 0-226-87033-2.
Misner, Charles W.; Thorne, Kip; Wheeler, John Archibald (1973). Gravitation. W. H. Freeman. ISBN 0-7167-0344-0. §31.2 The nonsingularity of the gravitational radius, and following sections; §34 Global Techniques, Horizons, and Singularity Theorems

Roger Penrose(1996). "Chandrasekhar, Black Holes, and Singularities".
Roger Penrose (1999). "The Question of Cosmic Censorship".
Τ. P. Singh. "Gravitational Collapse, Black Holes and Naked Singularities".

Further reading

The Elegant Universe by Brian Greene. This book provides a layman's introduction to string theory, although some of the views expressed are already becoming outdated. His use of common terms and his providing of examples throughout the text help the layperson understand the basics of string theory.



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