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{{Otheruses}}

[[Image:BH_LMC.png|thumb|right|Simulated view of a black hole in front of the [[Large Magellanic Cloud]]. The ratio between the black hole Schwarzschild radius and the observer distance to it is 1:9. Of note is the gravitational lensing effect known as an [[Einstein ring]], which produces a set of two fairly bright and large but highly distorted images of the Cloud as compared to its actual angular size.]]
{{General relativity|cTopic=Phenomena}}
In [[general relativity]], a '''black hole''' is a region of space in which the [[gravitational field]] is so powerful that nothing, not even [[light]], can escape. The black hole has a one-way surface, called an [[event horizon]], into which objects can fall, but out of which nothing can come. It is called "black" because it absorbs all the light that hits it, reflecting nothing, just like a perfect [[black-body]] in [[thermodynamics]].<ref>[http://cosmos.asu.edu/publications/papers/ThermodynamicTheoryofBlackHoles%2034.pdf Thermodynamics of Black Holes],P.C.W Davies, ''Rep. Prog. Phys'' '''Vol. 41'''(1978), pp.1313-1355.</ref> Quantum analysis of black holes shows them to possess a [[temperature]] and [[Hawking radiation]].

Despite its invisible interior, a black hole can reveal its presence through interaction with other matter. A black hole can be inferred by tracking the movement of a group of stars that orbit a region in space which looks empty. Alternatively, one can see gas falling into a relatively small black hole, from a companion star. This gas spirals inward, heating up to very high temperatures and emitting large amounts of radiation that can be detected from earthbound and earth-orbiting telescopes. Such observations have resulted in the scientific consensus that, barring a breakdown in our understanding of nature, black holes do exist in our galaxy. <cite>
==Introduction and terminology==
A black hole is often defined as an object whose [[escape velocity]] exceeds the [[speed of light]]. This picture is qualitatively wrong, but provides a way of understanding the order of magnitude for the black hole radius.

The escape velocity is the minimum speed at which an object needs to travel so as to escape a source of gravity without falling back into orbit before stopping. On the Earth, the escape velocity is equal to 11.2&nbsp;km/s, so no matter what the object is, whether a bullet or a baseball, it must go at least 11.2&nbsp;km/s to avoid falling back to the Earth's surface. To calculate the escape velocity in Newtonian mechanics, consider a heavy object of mass <math>M</math> centered at the origin. A second object with mass <math>m</math> starting at distance <math>r</math> from the origin with speed <math>v</math>, trying to escape to infinity, needs to have just enough kinetic energy to make up for the negative gravitational potential energy, with nothing left over:

::<math> {mv^2\over 2} - {GMm\over r} = 0 </math>

(where <math>G</math> is the [[gravitational constant]]). That way, as it gets closer to <math>r=\infty</math> it has less and less kinetic energy, finally ending up at infinity with zero speed.

This relation gives the critical escape velocity <math>v</math> in terms of <math>M</math> and <math>r</math>. But it also says that for each value of <math>v</math> and <math>M</math>, there is a critical value of <math>r</math> so that a particle with speed <math>v</math> is just able to escape:

::<math> r = {2GM\over v^2}</math>

When the velocity is equal to the speed of light, this gives the radius of a hypothetical Newtonian '''dark star''', a Newtonian body from which a particle moving at the speed of light cannot escape. In the most commonly used convention for the value of the radius of a black hole, the radius of the event horizon is equal to this Newtonian value.

::<math> r_{\rm Schwarzschild} = {2GM\over c^2}</math>

In [[general relativity]], the coordinate r is not completely straightforward to define due to the curved nature of space-time and the choice of different coordinates. For this result to be true, the value of r should be defined so that the surface area A of a sphere of radius r in the curved space time is still given by the formula <math>A=4\pi r^2</math>. This definition of r only makes sense when the gravitational field is spherically symmetric, so that there are concentric spheres on which the gravitational field is constant.

The velocity necessary to escape from an object's gravitational field (called the object's [[escape velocity]]) depends on how [[dense]] the object is; that is, the [[ratio]] of its [[mass]] to its [[volume]]. A black hole forms when an object is so dense that, within a certain distance of it, even [[light]] is not fast enough to escape, since the [[speed of light]] is slower than the black hole's escape velocity. Unlike in Newtonian gravity, in [[general relativity]], light going away from a black hole doesn't slow down and turn around. The Schwarzschild radius is still the last distance from which light can escape to infinity, but outgoing light which starts at the Schwarzschild radius doesn't go out and come back, it just stays there. Inside the Schwarzschild radius, everything must move inward, getting crushed somehow at the center.

In general relativity, the black hole's mass can be thought of as concentrated at a [[Gravitational singularity|singularity]], which can be a point, a ring, a light-ray, or a sphere; the exact details are not currently well understood in all circumstances. Surrounding the singularity is a spherical boundary called the [[event horizon]]. The event horizon marks the '[[point of no return]],' a boundary beyond which matter and radiation inevitably fall inwards, towards the singularity. The distance from the singularity at the center to the event horizon is the size of the black hole, and is equal to twice the mass in [[natural units|units where G and c equal 1]].

The radius of a black hole of mass equal to that of the [[Sun]] is about 3&nbsp;km. At distances much larger than this, the black hole has the exact same total gravitational attraction as any other body of the same mass, just like the sun. So if the sun were replaced by a black hole of the same mass, the orbits of the [[planets]] would remain unchanged.

There are several types of black holes, characterized by their typical size. When they form as a result of the [[gravitational collapse]] of a [[star]], they are called [[stellar black hole]]s. Black holes found at the center of galaxies have a mass up to several billion [[solar masses]] and are called [[supermassive black hole|supermassive black holes]]. Between these two scales, there are believed to be ''intermediate black holes'' with a mass of several thousand solar masses. Black holes with very small masses, believed to have formed early in the history of the [[Universe]], during the [[Big Bang]], might also exist, and are referred to as [[primordial black holes]]. Their existence is, at present, not confirmed.

It is impossible to directly observe a black hole. However, it is possible to infer its presence by its gravitational action on the surrounding [[Environment (systems)|environment]], particularly with [[microquasars]] and [[Active galactic nucleus|active galactic nuclei]], where material falling into a nearby black hole is significantly heated and emits a large amount of [[X-ray]] radiation. This observation method allows [[astronomers]] to detect their existence. The only objects that agree with these observations and are consistent within the framework of [[general relativity]] are black holes.

==History==
[[Image:Black hole lensing web.gif|right|frame|alt=Schwarzschild black hole|Simulation of [[Gravitational lensing]] by a black hole which distorts the image of a [[galaxy]] in the background. ([[:Image:BlackHole Lensing.gif|Click for larger animation.]])]]
The idea of a body so massive that even light could not escape was put forward by [[geologist]] [[John Michell]] in a letter written to [[Henry Cavendish]] in 1783 to the [[Royal Society]]:

{{quote|If the semi-diameter of a sphere of the same density as the Sun were to exceed that of the Sun in the proportion of 500 to 1, a body falling from an infinite height towards it would have acquired at its surface greater velocity than that of light, and consequently supposing light to be attracted by the same force in proportion to its vis inertiae, with other bodies, all light emitted from such a body would be made to return towards it by its own proper gravity.|[[John Michell]]<ref name="Michell1784">{{citation |last=Michell |first=J. |year=1784 |title=On the Means of Discovering the Distance, Magnitude, &c. of the Fixed Stars, in Consequence of the Diminution of the Velocity of Their Light, in Case Such a Diminution Should be Found to Take Place in any of Them, and Such Other Data Should be Procured from Observations, as Would be Farther Necessary for That Purpose |journal=Phil. Trans. R. Soc. (London) |volume=74 |pages=35–57|url=http://www.jstor.org/pss/106576}}.</ref>}}

In 1796, mathematician [[Pierre-Simon Laplace]] promoted the same idea in the first and second editions of his book ''Exposition du système du Monde'' (it was removed from later editions).<ref>{{cite web |url=http://library.thinkquest.org/25715/discovery/conceiving.htm#darkstars |title=Dark Stars (1783) |accessdate=2008-05-28 |quote= |publisher=[[Thinkquest]] }}</ref><ref>Laplace; see Israel, Werner (1987), "Dark stars: the evolution of an idea", in Hawking, Stephen W. & Israel, Werner, 300 Years of Gravitation, Cambridge University Press, Sec. 7.4</ref> Such "[[dark star]]s" were largely ignored in the nineteenth century, since light was then thought to be a massless wave and therefore not influenced by gravity. Unlike the modern black hole concept, the object behind the horizon is assumed to be stable against collapse.

In 1915, [[Albert Einstein]] developed his general theory of relativity, having earlier shown that gravity does in fact influence light's motion. A few months later, [[Karl Schwarzschild]] gave the [[Schwarzschild metric|solution]] for the gravitational field of a point mass and a spherical mass,<ref name ="Schwarzschild1916"/> showing that a black hole could theoretically exist. The [[Schwarzschild radius]] is now known to be the radius of the [[event horizon]] of a non-rotating black hole, but this was not well understood at that time, for example Schwarzschild himself thought it was not physical. Johannes Droste, a student of [[Hendrik Lorentz]], independently gave the same solution for the point mass a few months after Schwarzschild and wrote more extensively about its properties.

In 1930, [[astrophysicist]] [[Subrahmanyan Chandrasekhar]] calculated, using general relativity, that a non-rotating body of [[electron-degenerate matter]] above 1.44 solar masses (the [[Chandrasekhar limit]]) would collapse. His arguments were opposed by [[Arthur Eddington]], who believed that something would inevitably stop the collapse. Eddington was partly correct: a [[white dwarf]] slightly more massive than the Chandrasekhar limit will collapse into a [[neutron star]]. But in 1939, [[Robert Oppenheimer]] and others predicted that stars above approximately three solar masses (the [[Tolman-Oppenheimer-Volkoff limit]]) would collapse into black holes for the reasons presented by Chandrasekhar.<ref>[http://prola.aps.org/abstract/PR/v55/i4/p374_1 On Massive Neutron Cores], J. R. Oppenheimer and G. M. Volkoff, ''Physical Review'' '''55''', #374 (15 February 1939), pp. 374&ndash;381.</ref>

Oppenheimer and his co-authors used [[Schwarzschild metric|Schwarzschild's system of coordinates]] (the only coordinates available in 1939), which produced [[mathematical singularity|mathematical singularities]] at the [[Schwarzschild radius]], in other words some of the terms in the equations became [[infinity|infinite]] at the Schwarzschild radius. This was interpreted as indicating that the Schwarzschild radius was the boundary of a bubble in which time stopped. This is a valid point of view for external observers, but not for infalling observers.

Because of this property, the collapsed stars were briefly known as "frozen stars,"{{Fact|date=March 2009}} because an outside observer would see the surface of the star frozen in time at the instant where its collapse takes it inside the Schwarzschild radius. This is a known property of modern black holes, but it must be emphasized that the light from the surface of the frozen star becomes redshifted very fast, turning the black hole black very quickly. Many physicists could not accept the idea of time standing still at the Schwarzschild radius, and there was little interest in the subject for over 20 years.

In 1958, [[David Finkelstein]] introduced the concept of the [[event horizon]] by presenting [[Eddington-Finkelstein coordinates]], which enabled him to show that "The Schwarzschild surface r = 2&nbsp;m is not a singularity, but that it acts as a perfect unidirectional membrane: causal influences can cross it in only one direction".<ref>D. Finkelstein (1958). "Past-Future Asymmetry of the Gravitational Field of a Point Particle". Phys. Rev. 110: 965–967. </ref> This did not strictly contradict Oppenheimer's results, but extended them to include the point of view of infalling observers. All theories up to this point, including Finkelstein's, covered only non-rotating black holes.

In 1963, [[Roy Kerr]] found the exact solution for a rotating black hole. The rotating singularity of this solution was a ring, and not a point. A short while later, [[Roger Penrose]] was able to prove that singularities occur inside any black hole.

In 1967, astronomers discovered [[pulsars]],<ref>{{cite journal
| last=Hewish | first=Antony | coauthors=S J Bell, J D H Pilkington, P F Scott, R A Collins
| title=Observation of a Rapidly Pulsating Radio Source
| journal=Nature | year=1968
| volume=217 | issue= | pages=709–713
| url=http://www.nature.com/nature/journal/v235/n5332/abs/235037a0.html
| accessdate=2007-07-06 | doi=10.1038/217709a0 }}</ref><ref>{{cite journal
| last=Pilkington | first=J D H | coauthors=A Hewish, S J Bell, T W Cole
| title=Observations of some further Pulsed Radio Sources
| journal=Nature | year=1968
| volume=218 | issue= | pages=126–129
| url=http://www.nature.com/nature/journal/v218/n5137/pdf/218126a0.pdf
| accessdate=2007-07-06 | doi=10.1038/218126a0 }}</ref> and within a few years could show that the known pulsars were rapidly rotating [[neutron star]]s. Until that time, neutron stars were also regarded as just theoretical curiosities. So the discovery of pulsars awakened interest in all types of ultra-dense objects that might be formed by gravitational collapse.

Physicist [[John Archibald Wheeler|John Wheeler]] is widely credited with coining the term ''black hole'' in his 1967 public lecture ''Our Universe: the Known and Unknown'', as an alternative to the more cumbersome "gravitationally completely collapsed star." However, Wheeler insisted that someone else at the conference had coined the term and he had merely adopted it as useful shorthand. The term was also cited in a 1964 letter by Anne Ewing to the [[AAAS]]:

{{quote|According to Einstein’s general theory of relativity, as mass is added to a degenerate star a sudden collapse will take place and the intense gravitational field of the star will close in on itself. Such a star then forms a "black hole" in the universe.|Ann Ewing|letter to ''AAAS''<ref>{{cite web|title=Black Hole|work=World Wide Words|author=Michael Quinion|url=http://www.worldwidewords.org/topicalwords/tw-bla1.htm|accessdate=2008-06-17}}</ref>}}

==Properties and features==
The [[No hair theorem]] states that, once it settles down, a black hole has only three independent physical properties: mass, charge, and angular momentum.<ref>{{citation|last=Heusler |first=M. |year=1998 |title=Stationary Black Holes: Uniqueness and Beyond |journal=Living Rev. Relativity |volume=1 |number=6 |url=http://www.livingreviews.org/Articles/Volume1/1998-6heusler/}}</ref> Any two black holes that share the same values for these properties, or parameters, are classically indistinguishable.

These properties are special because they are visible from outside the black hole. For example, a charged black hole repels other like charges just like any other charged object, despite the fact that photons, the particles responsible for electric and magnetic forces, cannot escape from the interior region. The reason is [[Gauss's law]], the total electric flux going out of a big sphere always stays the same, and measures the total charge inside the sphere. When charge falls into a black hole, electric field lines still remain, poking out of the horizon, and these field lines conserve the total charge of all the infalling matter. The electric field lines eventually spread out evenly over the surface of the black hole, settling down to a uniform field-line density on the surface. The black hole acts in this regard like a classical conducting sphere with a definite resistivity.<ref> Thorne, "Black Holes, The Membrane Paradigm"</ref>

Similarly, the total mass inside a sphere containing a black hole can be found by using the gravitational analog of Gauss's law, far away from the black hole. Likewise, the angular momentum can be measured from far away using [[frame dragging]] by the gravitomagnetic field.

When a black hole swallows any form of matter, its horizon oscillates like a stretchy membrane with friction, a [[dissipative system]], until it settles down to a simple final state. This is different from other field theories like electromagnetism or gauge theory, which never have any friction or resistivity, because they are time reversible. Because the black hole eventually settles down into a final state with only three parameters, there is no way to avoid losing information about the initial conditions: The gravitational and electric fields of the black hole give very little information about what went in. The information that is lost includes every quantity that cannot be measured far away from the black hole horizon, including the total [[baryon number]], [[lepton number]], and all the other nearly conserved pseudo-charges of particle physics. This behavior is so puzzling, that it has been called the [[black hole information loss paradox]].<ref>{{citeweb|url=http://math.ucr.edu/home/baez/physics/Relativity/BlackHoles/info_loss.html|title=The Black Hole Information Loss Problem|last=Anderson|first=Warren G.|date=1996|accessdate=2009-03-24}}</ref><ref>John Preskill(1994)"[http://www.theory.caltech.edu/~preskill/talks/blackholes.pdf Black holes and information: A crisis in quantum physics]"</ref><ref>Daniel Carmody(2008)"[http://www.carmodyfamily.com/bnb/QCI_Paper.pdf The Fate of Quantum Information in a Black Hole]"</ref>

The loss of information in black holes is puzzling even classically, because general relativity is a [[Lagrangian]] theory, which superficially appears to be time reversible and [[Hamiltonian system|Hamiltonian]]. But because of the horizon, a black hole is not time reversible: matter can enter but it cannot escape. The time reverse of a classical black hole has been called a [[white hole]], although entropy considerations and quantum mechanics suggest that white holes are just the same as black holes.

The no-hair theorem makes some assumptions about the nature of our universe and the matter it contains, and other assumptions lead to different conclusions. For example, if [[Magnetic monopole]]s exist, as predicted by some theories,<ref>{{cite web|url=http://arxiv.org/PS_cache/hep-ph/pdf/9811/9811320v1.pdf|title=Black holes with magnetic charge and quantized mass|coauthors=A.Yu.Ignatiev, G.C.Joshi and Kameshwar C.Wali|publisher=Research Centre for High Energy Physics, School of Physics, University of Melbourne, Parkville 3052, Victoria, Australia|accessdate=2009-03-24}}</ref> the magnetic charge would be a fourth parameter for a classical black hole.

Counterexamples to the no-hair theorem are known for the following cases:
# In spacetime dimensions higher than four
# In the presence of [[non-abelian]] [[Yang-Mills field]]s
# For discrete gauge symmetries.
# Some non-minimally coupled [[scalar fields]]<ref>{{cite web|url=http://people.na.infn.it/~scud/PLA201-95.pdf|title=Nonminimal coupling, no-hair theorem and matter cosmologies|accessdate=2009-03-24}}</ref>
# When scalars can be topologically twisted, as in the case of [[skyrmion]]s
# In modified theories of gravity, different from [[Einstein]]’s [[general relativity]].

These exceptions are sometimes unstable, and sometimes do not lead to new conserved quantum numbers far away from the black hole.<ref>{{cite web|url=file:///C:/Users/Ben/AppData/Local/Temp/569.pdf|title=The No Hair Theorem?|last=Hsu|first=Rue-Ron|date=1992-01-09|publisher=CHINESE JOURNAL OF PHYSICS|accessdate=2009-03-24}}</ref> For large black holes in our apparently four-dimensional, very nearly flat universe,<ref>{{citation| author=Hinshaw, G. et al. |title=Five-Year Wilkinson Microwave Anisotropy Probe (WMAP) Observations: Data Processing, Sky Maps, and Basic Results |year=2008 |url=http://arxiv.org/abs/0803.0732}}.</ref> the theorem should hold.
===Classification===
====By physical properties====
The simplest black hole has mass but neither charge nor angular momentum. These black holes are often referred to as [[Schwarzschild metric|Schwarzschild black hole]]s after the physicist [[Karl Schwarzschild]] who discovered this [[Solutions of the Einstein field equations|solution]] in 1915.<ref name="Schwarzschild1916">{{Citation
| last=Schwarzschild
| first=Karl
| author-link=Karl Schwarzschild
| title=Über das Gravitationsfeld eines Massenpunktes nach der Einsteinschen Theorie
| journal=Sitzungsber. Preuss. Akad. D. Wiss.
| year=1916
|pages=189–196
}} and {{Citation
| last=Schwarzschild
| first=Karl
| author-link=Karl Schwarzschild
| title=Über das Gravitationsfeld eines Kugel aus inkompressibler Flüssigkeit nach der Einsteinschen Theorie
| journal=Sitzungsber. Preuss. Akad. D. Wiss.
| pages=424–434
| year=1916
}}.</ref> It was the first non-trivial [[Exact solutions in general relativity|exact solution]] to the [[Einstein field equations]] to be discovered, and according to [[Birkhoff's theorem (relativity)|Birkhoff's theorem]], the only [[Vacuum solution (general relativity)|vacuum solution]] that is [[Spherically symmetric spacetime|spherically symmetric]].<ref>{{cite web|url=http://myweb.lsbu.ac.uk/~whittyr/MathSci/TheoremOfTheDay/CombinatorialTheory/Birkhoff/TotDBirkhoff.pdf|title=Garrett Birkhoff’s Theorem|accessdate=2009-03-25}}</ref> This means that there is no observable difference between the gravitational field of such a black hole and that of any other spherical object of the same mass. The popular notion of a black hole "sucking in everything" in its surroundings is therefore only correct near the black hole horizon; far away, the external gravitational field is essentially like that of ordinary massive bodies.<ref>{{cite web|url=http://astro.airynothing.com/2006/02/black_holes_do_not_suck.html|title=Black Holes do not suck!|date=2006-02-17|accessdate=2009-03-25}}</ref>

More general black hole solutions were discovered later in the 20th century. The [[Reissner-Nordström metric]] describes a black hole with electric charge, while the [[Kerr metric]] yields a rotating black hole. The more generally known [[Stationary spacetime|stationary]] black hole solution, the [[Kerr-Newman metric]], describes both charge and angular momentum.

While the mass of a black hole can take any positive value, the charge and angular momentum are constrained by the mass. In [[natural units]] , the total charge <math>Q\, </math> and the total angular momentum <math>J\, </math> are expected to satisfy
:<math>Q^2+\left ( \tfrac{J}{M} \right )^2\le M^2\, </math>
for a black hole of mass ''M''.

Black holes saturating this inequality are called [[extremal black hole|extremal]]. Solutions of Einstein's equations violating the inequality do exist, but do not have a horizon. These solutions have [[Naked singularity|naked singularities]] and are deemed ''unphysical'', as the [[cosmic censorship hypothesis]] rules out such singularities due to the generic gravitational collapse of [[Energy conditions|realistic matter]].<ref>For a review see {{citation |last=Wald |first=Robert. M. |author-link=Robert Wald |title=Gravitational Collapse and Cosmic Censorship |year=1997 |url=http://arxiv.org/abs/gr-qc/9710068}}.</ref> This is supported by numerical simulations.<ref>For a discussion of these numerical simulations see {{Citation| last=Berger | first=Beverly K. | year=2002 | url=http://www.livingreviews.org/lrr-2002-1 | title=Numerical Approaches to Spacetime Singularities | journal=Living Rev. Relativity | volume=5 |access-date=2007-08-04}}.</ref>

Due to the relatively large strength of the [[electromagnetism|electromagnetic force]], black holes forming from the collapse of stars are expected to retain the nearly neutral charge of the star. Rotation, however, is expected to be a common feature of compact objects, and the black-hole candidate binary X-ray source [[GRS 1915+105]]<ref>{{citation |first1=Jeffrey E. |last1=McClintock |first2=Rebecca |last2=Shafee |first3=Ramesh |last3=Narayan |first4=Ronald A. |last4=Remillard |first5=Shane W. |last5=Davis |first6=Li-Xin |last6=Li |title=The Spin of the Near-Extreme Kerr Black Hole GRS 1915+105 |journal=Astrophys.J. |volume=652 |year=2006 |pages=518–539 |url=http://arxiv.org/abs/astro-ph/0606076}}.</ref> appears to have an angular momentum near the maximum allowed value.
====By mass====
{| align="right" class="wikitable" style="margin: 1ex"
|-
! Class !! Mass !! Size
|-
| [[Supermassive black hole ]] || style="text-align: center;"| ~10<sup>5</sup>&ndash;10<sup>9</sup> M<sub>[[Sun]]</sub> || style="text-align: center;"| ~0.001&ndash;10 [[Astronomical unit|AU]]
|-
| [[Intermediate-mass black hole]] || style="text-align: center;"| ~10<sup>3</sup> M<sub>[[Sun]]</sub> || style="text-align: center;"| ~10<sup>3</sup> km = R<sub>[[Earth]]</sub>
|-
| [[Stellar black hole|Stellar-mass]] || style="text-align: center;"| ~10 M<sub>[[Sun]]</sub> || style="text-align: center;"| ~30&nbsp;km
|-
| [[Micro black hole]] || style="text-align: center;"| up to ~M<sub>[[Moon]]</sub> || style="text-align: center;"|up to ~0.1&nbsp;mm
|}
Black holes are commonly classified according to their mass, independent of angular momentum <math>J\,</math>. The size of a black hole, as determined by the radius of the event horizon, or [[Schwarzschild radius]], is proportional to the mass <math>M\,</math> through
:<math>r_{sh} \approx 2.95\, M/M_\bigodot \;\mathrm{km,}</math>
where <math>r_{sh}\,</math> is the Schwarzschild radius and <math>M_\bigodot</math> is the [[solar mass|mass of the Sun]]. A black hole's size and mass are thus simply related [[Rotating black hole|independent of rotation]]. According to this criterion, black holes are classed as:

*[[Supermassive black hole|Supermassive]] &ndash; contain hundreds of thousands to billions of solar masses, and are thought to exist in the center of most galaxies,<ref>{{Cite journal
| volume=31
| issue=1
| pages=473–521
| last=Antonucci
| first=R.
| title=Unified Models for Active Galactic Nuclei and Quasars
| journal=Annual Reviews in Astronomy and Astrophysics
| date=1993
| doi=10.1146/annurev.aa.31.090193.002353
}}</ref><ref>{{Cite journal
| volume=107
| pages=803–845
| last=Urry
| first=C.
| coauthors=Paolo Padovani
| title=Unified Schemes for Radio-Loud Active Galactic Nuclei
| journal=Publications of the Astronomical Society of the Pacific
| date=1995
| doi=10.1086/133630
}}</ref> including the [[Milky Way]].<ref>{{cite journal |last=Schödel |first=R. |authorlink= |coauthors=''et al.'' |year=2002 |month= |title=A star in a 15.2-year orbit around the supermassive black hole at the centre of the Milky Way |journal=Nature |volume=419 |issue=6908 |pages=694–696 |doi=10.1038/nature01121 |url= |accessdate= |quote= }}</ref> They are believed to be responsible for [[Active galactic nucleus|active galactic nuclei]], and presumably form either from the coalescence of smaller black holes, or by the accretion of stars and gas onto them. The largest known supermassive black hole is located in [[OJ 287]] weighing in at 18 billion solar masses.<ref>{{Citation |last1=Valtonen |first1=M.J. |last2=et al.. |title=A massive binary black-hole system in OJ 287 and a
test of general relativity |journal=[[Nature (journal)|Nature]] |year=2008 |volume=452 |doi=10.1038/nature06896 |pages=851}}</ref>

*[[Intermediate-mass black hole|Intermediate]] &ndash; contain thousands of solar masses. They have been proposed as a possible power source for [[ultraluminous X-ray source]]s.<ref>{{Citation |last1=Maccarone |first1=T.J. |last2=et al.. |title=A black hole in a globular cluster |journal=[[Nature (journal)|Nature]] |year=2007 |volume=455 |doi=10.1038/nature05434 |pages=183-185}}</ref> There is no known mechanism for them to form directly, so they likely form via collisions of lower mass black holes, either in the dense stellar cores of [[globular cluster]]s or galaxies.{{Fact|date=March 2009}} Such creation events should produce intense bursts of [[gravitational wave]]s, which [[LIGO|may be observed]] soon. The boundary between super- and intermediate-mass black holes is a matter of convention. Their lower mass limit, the maximum mass for direct formation of a single black hole from collapse of a massive star, is poorly known at present, but is thought to be somewhere well below 200&nbsp;solar masses.

*[[Stellar black hole|Stellar-mass]] &ndash; have masses ranging from a lower limit of about 1.4&ndash;3&nbsp;solar masses (1.4 is the [[Chandrasekhar limit]] and 3 is the [[Tolman-Oppenheimer-Volkoff limit]] for the maximum mass of neutron stars) up to perhaps 15–20 solar masses. They are created by the collapse of individual stars, or by the coalescence (inevitable, due to [[gravitational radiation]]) of [[Neutron star#Binary neutron stars|binary neutron stars]]. Stars may form with [[Initial mass function|initial masses]] up to about 100&nbsp;solar masses, or in the distant past, possibly even higher, but these shed most of their outer massive layers during earlier phases of their evolution, either blown away in stellar winds during the [[red giant]], [[Asymptotic giant branch|AGB]], and [[Wolf-Rayet star|Wolf-Rayet]] stages, or expelled in [[supernova]] explosions for stars that turn into neutron stars or black holes. Being known mostly by theoretical models for late-stage stellar evolution, the upper limit for the mass of stellar-mass black holes is somewhat uncertain at present. The cores of still lighter stars form [[white dwarf]]s.

*[[Micro black hole|Micro]] &ndash; (also ''mini black holes'') have masses much less than that of a star. At these sizes, [[quantum mechanics]] is expected to take effect. There is no known mechanism for them to form via normal processes of stellar evolution, but certain [[cosmic inflation|inflationary]] scenarios predict their production during the early stages of the evolution of the universe.{{Fact|date=March 2009}} According to some theories of [[quantum gravity]] they may also be produced in the highly energetic reaction produced by [[cosmic rays]] hitting the [[atmosphere]] or even in [[particle accelerators]] such as the [[Large Hadron Collider]].{{Fact|date=March 2009}} The theory of [[Hawking radiation]] predicts that such black holes will evaporate in bright flashes of [[gamma radiation]]. [[NASA]]'s [[Fermi Gamma-ray Space Telescope]] satellite (formerly GLAST) launched in 2008 is searching for such flashes.<ref>{{cite web |url=http://www.nasa.gov/mission_pages/GLAST/news/glast_gbm.html |title=NASA's GLAST Burst Monitor Team Hard at Work Fine-Tuning Instrument and Operations |publisher=NASA |date=2008-07-28}}</ref>

===Event horizon===
{{main|Event horizon}}
{| align="right" class="wikitable" style="margin:1ex 1ex 1ex 1ex" width="400"
|- width
| [[File:BH-no-escape-1.svg|Image:BH-no-escape-1.svg]]<br/>Far away from the black hole a particle can move in any direction. It is only restricted by the speed of light.
|-
| [[File:BH-no-escape-2.svg|Image:BH-no-escape-2.svg]]<br/>Closer to the black hole spacetime starts to deform. There are more paths going towards the black hole than paths moving away.
|-
| [[File:BH-no-escape-3.svg|Image:BH-no-escape-3.svg]]<br/>Inside of the event horizon all paths bring the particle closer to the center of the black hole. It is no longer possible for the particle to escape.
|}
The defining feature of a black hole is the appearance of an event horizon; a boundary in [[spacetime]] beyond which events cannot affect an outside observer. As predicted by general relativity, the presence of a mass deforms spacetime in such a way that the paths particles take tend towards the mass. At the event horizon of a black hole this deformation becomes so strong that there are no more paths that lead away from the black hole.<ref>{{cite web|url=http://archive.ncsa.uiuc.edu/Cyberia/NumRel/BlackHoleAnat.html|title=Anatomy of a Black Hole|accessdate=2009-03-25}}</ref> Once a particle is inside the horizon, moving into the hole is as inevitable as moving forward in time (and can actually be thought of as equivalent to doing so).

To a distant observer clocks near a black hole appear to tick more slowly than those further away from the black hole.<ref>{{harvnb|Carroll|2004|p=217}}</ref> Due to this effect (known as [[gravitational time dilation]]) the distant observer will see an object falling into a black hole slow down as it approaches the event horizon, taking an infinite time to reach it.<ref>{{cite web|url=http://www.vectorsite.net/tprelp.html|title=[8] GENERAL RELATIVITY IN PRACTICE / BLACK HOLES|accessdate=2009-03-26}}</ref> At the same time all processes on this object slow down causing emitted light to appear redder and dimmer, an effect known as [[gravitational redshift|gravitational red shift]].<ref>{{cite web|url=http://nrumiano.free.fr/Estars/int_bh.html|title=Inside a black hole|accessdate=2009-03-26}}</ref> Eventually, the falling object becomes so dim that it can no longer be seen, at a point just before it reaches the event horizon.

For a non rotating (static) black hole, the [[Schwarzschild radius]] delimits a spherical event horizon. The Schwarzschild radius of an object is proportional to the mass.<ref>{{cite web|url=http://www.physics.eku.edu/Yoder/l16_BH.htm|title=Black Holes|accessdate=2009-03-25}}</ref> Rotating black holes have distorted, nonspherical event horizons. Since the event horizon is not a material surface but rather merely a mathematically defined demarcation boundary, nothing prevents matter or radiation from entering a black hole, only from exiting one. The description of black holes given by general relativity is known to be an approximation, and it is expected that [[quantum gravity]] effects become significant near the vicinity of the event horizon.<ref>{{cite web|url=http://www.ias.ac.in/jarch/pramana/51/693-698.pdf|title=Physical nature of the event horizon|accessdate=2009-03-25}}</ref> This allows observations of matter in the vicinity of a black hole's event horizon to be used to indirectly study [[general relativity]] and proposed extensions to it.

Though black holes themselves may not radiate energy, electromagnetic radiation and matter particles may be radiated from just outside the event horizon via Hawking radiation.<ref>{{cite web|url=http://casa.colorado.edu/~ajsh/hawk.html|title=Hawking Radiation|accessdate=2009-03-25}}</ref>

===Singularity===
{{main|Gravitational singularity}}
At the center of a black hole lies the ''singularity'', where matter is crushed to [[infinite]] density, the pull of gravity is infinitely strong, and spacetime has infinite curvature.<ref>{{cite web|url=http://archive.ncsa.uiuc.edu/Cyberia/NumRel/BlackHoleAnat.html|title=The Singularity|accessdate=2009-03-26}}</ref> This means that a black hole's mass becomes entirely compressed into a region with zero volume.<ref>{{cite web|url=http://casa.colorado.edu/~ajsh/singularity.html|title=Falling to the Singularity of the Black Hole|accessdate=2009-03-26}}</ref> This zero-volume, infinitely dense region at the center of a black hole is called a [[gravitational singularity]].

The singularity of a non-rotating black hole has zero length, width, and height; a [[rotating black hole]] is smeared out to form a [[ring singularity|ring shape]] lying in the plane of rotation.<ref>{{cite web|url=http://www.unc.edu/~mgood/research/Singularity.pdf|title=The Black Hole Singularity|last=Good|first=Michael|publisher=reEvolutionary Physics|pages=1-4|accessdate=2009-03-26}}</ref> The ring still has no thickness and hence no volume.

The appearance of singularities in general relativity is commonly perceived as signaling the breakdown of the theory.<ref>{{cite web|url=http://www.mat.unb.br/~matcont/28_8.pdf|title=THE GEOMETRY OF GRAVITATIONAL COLLAPSE|last=Giamb�o|first=Roberto|accessdate=2009-03-26}}</ref> This breakdown, however, is expected; it occurs in a situation where [[quantum mechanics|quantum mechanical]] effects should describe these actions due to the extremely high density and therefore particle interactions. To date it has not been possible to combine quantum and gravitational effects into a single theory. It is generally expected that a theory of [[quantum gravity]] will feature black holes without singularities.<ref>{{cite web|url=http://www.damtp.cam.ac.uk/user/gr/public/bh_hawk.html|title=Black Holes and Quantum Gravity|accessdate=2009-03-26}}</ref><ref>{{cite web|url=http://imagine.gsfc.nasa.gov/docs/ask_astro/answers/980420b.html|title=Ask an Astrophysicist : Quantum Gravity and Black Holes |accessdate=2009-03-26}}</ref>

===Photon sphere===
{{main|Photon sphere}}
The photon sphere is a spherical boundary of zero thickness such that photons moving along [[Tangent#Geometry|tangents]] to the sphere will be trapped in a circular orbit. For non-rotating black holes, the photon sphere has a radius 1.5 times the [[Schwarzschild radius]]. The orbits are [[instability|dynamically unstable]], hence any small perturbation (such as a particle of infalling matter) will grow over time, either setting it on an outward trajectory escaping the black hole or on an inward spiral eventually crossing the event horizon.

While light can still escape from inside the photon sphere, any light that crosses the photon sphere on an inbound trajectory will be captured by the black hole. Hence any light reaching an outside observer from inside the photon sphere must have been emitted by objects inside the photon sphere but still outside of the event horizon.

Other [[compact object]]s, such as [[neutron stars]], can also have photon spheres.<ref>

{{citation |first=Robert J. |last=Nemiroff |title=Visual distortions near a neutron star and black hole |journal= American Journal of Physics |volume=61 |pages=619 |year=1993 |doi=10.1119/1.17224}}</ref> This follows from the fact that the gravitational field of an object does not depend on its actual size, hence any object that is smaller than 1.5 times the Schwarzschild radius corresponding to its mass will indeed have a photon sphere.
===Ergosphere===
{{main|Ergosphere}}
[[Image:Ergosphere.svg|thumb|right|ergosphere of a rotating black hole|The ergosphere is an oblate spheroid region outside of the event horizon, where objects cannot remain stationary.]]
Rotating black holes are surrounded by a region of spacetime in which it is impossible to stand still, called the ergosphere. This is the result of a process known as [[frame-dragging]]; general relativity predicts that any rotating mass will tend to slightly "drag" along the spacetime immediately surrounding it. Any object near the rotating mass will tend to start moving in the direction of rotation. For a rotating black hole this effect becomes so strong near the event horizon that an object would have to move faster than the speed of light in the opposite direction to just stand still.

The ergosphere of a black hole is bounded by:

*On the outside, an [[oblate]] spheroid, which coincides with the event horizon at the poles and is noticeably wider around the "equator." This boundary is sometimes called the "ergosurface," but it is just a boundary and has no more solidity than the event horizon. At points exactly on the ergosurface, spacetime is "dragged around at the speed of light."
*On the inside, the (outer) event horizon.

Within the ergosphere, space-time is dragged around faster than light—general relativity forbids material objects to travel faster than light (so does [[special relativity]]), but allows regions of space-time to move faster than light relative to other regions of space-time.

Objects and radiation (including light) can stay in ''orbit'' within the ergosphere without falling to the center. But they cannot hover (remain stationary, as seen by an external observer), because that would require them to move backwards faster than light relative to their own regions of space-time, which are moving faster than light relative to an external observer.

Objects and radiation can also ''escape'' from the ergosphere. In fact the [[Penrose process]] predicts that objects will sometimes fly out of the ergosphere, obtaining the energy for this by "stealing" some of the black hole's rotational energy. If a large total mass of objects escapes in this way, the black hole will spin more slowly and may even stop spinning eventually.

==Formation and evolution==
From the exotic nature of black holes, it is natural to question if such bizarre objects could actually exist in nature or that they are merely pathological solutions to Einstein's equations. Einstein himself wrongly believed that black holes would not form, because he believed that the angular momentum of collapsing particles would stabilize their motion at some radius.<ref>{{cite journal|author= Einstein, A. |title= On A Stationary System With Spherical Symmetry Consisting of Many Gravitating Masses|journal= Annals of Mathematics| volume=40 No. 4 |pages=922-936|year=1939}}</ref> This led the general relativity community to dismiss all results to the contrary for many years. However, a minority of relativists continued to believe that black holes were physical objects,<ref>{{cite web | title=Discovering the Kerr and Kerr-Schild metrics | publisher=Roy P. Kerr | work=To appear in "The Kerr Spacetime", Eds D.L. Wiltshire, M. Visser and S.M. Scott, Cambridge Univ. Press| url=http://www.arxiv.org/abs/0706.1109 | dateformat=mdy | accessdate=June 19 2007 }}</ref> and by the end of the 1960s, they had persuaded the majority of researchers in the field that there is no obstacle to forming an event horizon.

Once an event horizon forms, [[Roger Penrose]] proved that a singularity will form somewhere inside it. Shortly afterwards, [[Stephen Hawking]] showed that many cosmological solutions describing the [[big bang]] have singularities, in the absence of scalar fields or other exotic matter (see [[Penrose-Hawking singularity theorems]]). The [[Kerr solution]], the [[no-hair theorem]] and the laws of [[black hole thermodynamics]] showed that the physical properties of black holes were simple and comprehensible, making them respectable subjects for research.<ref name=HawkingPenrose1970>{{cite journal |doi=10.1098/rspa.1970.0021 |url=http://rspa.royalsocietypublishing.org/content/314/1519/529.abstract |first=Stephen |last=Hawking |authorlink=Stephen Hawking |coauthors=[[Roger Penrose]] |month=January |year=1970 |title=The Singularities of Gravitational Collapse and Cosmology |journal=[[Proceedings of the Royal Society#Proceedings of the Royal Society A|Proceedings of the Royal Society A]] |volume=314 |issue=1519 |pages=529–548}}</ref> The primary formation process for black holes is expected to be the [[gravitational collapse]] of heavy objects such as stars, but there are also more exotic processes that can lead to the production of black holes.
===Gravitational collapse===
{{main|Gravitational collapse}}
Gravitational collapse occurs when an object's internal pressure is insufficient to resist the object's own gravity. For stars this usually occurs either because a star has too little [[Stellar nucleosynthesis|"fuel"]] left to maintain its temperature, or because a star which would have been stable receives a lot of extra matter in a way which does not raise its core temperature. In either case the star's temperature is no longer high enough to prevent it from collapsing under its own weight (the [[ideal gas law]] explains the connection between pressure, temperature, and volume).

The collapse may be stopped by the [[degeneracy pressure]] of the star's constituents, condensing the matter in an exotic [[Degenerate matter|denser state]]. The result is one of the various types of [[compact star]]. Which type of compact star is formed depends on the mass of the remnant - the matter left over after changes triggered by the collapse (such as [[supernova]] or pulsations leading to a [[planetary nebula]]) have blown away the outer layers. Note that this can be substantially less than the original star - remnants exceeding 5 solar masses are produced by stars which were over 20 solar masses before the collapse.

If the mass of the remnant exceeds ~3-4 solar masses (the [[Tolman-Oppenheimer-Volkoff limit]])—either because the original star was very heavy or because the remnant collected additional mass through accretion of matter—even the degeneracy pressure of [[neutrons]] is insufficient to stop the collapse. After this no known mechanism (except possibly quark degeneracy pressure, see [[quark star]]) is powerful enough to stop the collapse and the object will inevitably collapse to a black hole.

This gravitational collapse of heavy stars is assumed to be responsible for the formation of most (if not all) [[stellar mass black hole]]s.
=====Primordial black holes in The Big Bang=====
Gravitational collapse requires great densities. In the current epoch of the universe these high densities are only found in stars, but in the early universe shortly after the [[big bang]] densities were much greater, possibly allowing for the creation of black holes. The high density alone is not enough to allow the formation of black holes since a uniform mass distribution will not allow the mass to bunch up. In order for [[primordial black holes]] to form in such a dense medium, there must be initial density perturbations which can then grow under their own gravity. Different models for the early universe vary widely in their predictions of the size of these perturbations. Various models predict the creation of black holes, ranging from a [[Planck mass]] to hundreds of thousands of solar masses.<ref>{{cite arXiv |eprint=astro-ph/0511743v1 |last1=Carr | first1=B. J. |title=Primordial Black Holes: Do They Exist and Are They Useful? |class=astro-ph |year=2005}}</ref> Primordial black holes could thus account for the creation of any type of black hole.

===High energy collisions===
[[Image:CMS Higgs-event.jpg|thumb|right|A simulated event in the CMS detector, a collision in which a micro black hole may be created.]]
Gravitational collapse is not the only process that could create black holes. In principle, black holes could also be created in high energy collisions that create sufficient density. However, to date, no such events have ever been detected either directly or indirectly as a deficiency of the mass balance in [[particle accelerator]] experiments.<ref>{{cite journal |doi=10.1103/PhysRevD.65.056010 |id={{arXiv|archive=hep-ph|id=0106219v4}} |title=High energy colliders as black hole factories: The end of short distance physics |year=2002 |author=Giddings, Steven B. |journal=Physical Review D |volume=65 |pages=056010}}</ref> This suggests that there must be a lower limit for the mass of black holes. Theoretically this boundary is expected to lie around the [[Planck mass]] (~10<sup>19</sup> [[GeV]]/c<sup>2</sup> = ~2 × 10<sup>-8</sup> kg), where quantum effects are expected to make the theory of general relativity break down completely.{{Fact|date=June 2008}} This would put the creation of black holes firmly out of reach of any high energy process occurring on or near the Earth. Certain developments in quantum gravity however suggest that this bound could be much lower. Some [[braneworld]] scenarios for example put the Planck mass much lower, may be even as low as 1 TeV/c<sup>2</sup>.<ref>{{cite journal |id={{arXiv|arxhive=hep-ph|id=9803315v1}} |doi=10.1016/S0370-2693(98)00466-3 |title=The hierarchy problem and new dimensions at a millimeter |year=1998 |author=Arkani–Hamed, N |journal=Physics Letters B |volume=429 |pages=263}}</ref> This would make it possible for [[micro black hole]]s to be created in the high energy collisions occurring when cosmic rays hit the Earth's atmosphere, or possibly in the new [[Large Hadron Collider]] at [[CERN]]. These theories are however very speculative, and the creation of black holes in these processes is deemed unlikely by many specialists.
===Growth===
Once a black hole has formed, it can continue to grow by absorbing additional matter. Any black hole will continually absorb [[interstellar dust]] from its direct surroundings and omnipresent [[cosmic background radiation]], but neither of these processes should significantly affect the mass of a stellar black hole. More significant contributions can occur when the black hole formed in a [[binary star]] system. After formation the black hole can then leech significant amounts of matter from its companion.

Much larger contributions can be obtained when a black hole merges with other stars or compact objects. The [[supermassive black hole]]s suspected in the center of most galaxies are expected to have formed from the coagulation of many smaller objects. The process has also been proposed as the origin of some [[intermediate-mass black hole]]s.

As an object approaches the event horizon, the horizon near the object bulges up and swallows the object. Shortly thereafter the increase in radius (due to the extra mass) is distributed evenly around the hole.
===Evaporation===
{{main|Hawking radiation}}
In 1974, [[Stephen Hawking]] showed that black holes are not entirely black but emit small amounts of thermal radiation.<ref name=Hawking1974>{{Citation|last=Hawking |first=S.W. |title=Black hole explosions? |journal=Nature |year=1974 |volume=248 |pages=30–31 |url=http://www.nature.com/nature/journal/v248/n5443/abs/248030a0.html |doi=10.1038/248030a0}}</ref> He got this result by applying [[quantum field theory]] in a static black hole background. The result of his calculations is that a black hole should emit particles in a perfect [[black body spectrum]]. This effect has become known as [[Hawking radiation]]. Since Hawking's result, many others have verified the effect through various methods.<ref>{{cite journal |id={{arXiv|archive=hep-th|id=0409024v3}} |doi=10.1088/1367-2630/7/1/203 |title=Hawking radiation and black hole thermodynamics |year=2005 |author=Page, Don N |journal=New Journal of Physics |volume=7 |pages=203}}</ref> If his theory of black hole radiation is correct then black holes are expected to emit a thermal spectrum of radiation, and thereby lose mass, because according to the theory of relativity mass is just highly condensed energy (''E''&nbsp;= ''mc''<sup>2</sup>).<ref name=Hawking1974/> Black holes will shrink and evaporate over time. The temperature of this spectrum ([[Hawking temperature]]) is proportional to the [[surface gravity]] of the black hole, which in turn is inversely proportional to the mass. Large black holes, therefore, emit less radiation than small black holes.

A stellar black hole of 5 solar masses has a Hawking temperature of about 12 nanokelvins. This is far less than the 2.7 K produced by the [[cosmic microwave background]]. Stellar mass (and larger) black holes receive more mass from the cosmic microwave background than they emit through Hawking radiation and will thus grow instead of shrink. In order to have a Hawking temperature larger than 2.7 K (and be able to evaporate) a black hole needs to be lighter than the [[Moon]] (and therefore a diameter of less than a tenth of a millimeter).

On the other hand if a black hole is very small, the radiation effects are expected to become very strong. Even a black hole that is heavy compared to a human would evaporate in an instant. A black hole the weight of a car (~10<sup>-24</sup> m) would only take a nanosecond to evaporate, during which time it would briefly have a luminosity more than 200 times that of the sun. Lighter black holes are expected to evaporate even faster, for example a black hole of mass 1 TeV/''c''<sup>2</sup> would take less than 10<sup>-88</sup> seconds to evaporate completely. Of course, for such a small black hole [[quantum gravity|quantum gravitation]] effects are expected to play an important role and could even{{ndash}} although current developments in quantum gravity do not indicate so{{ndash}} hypothetically make such a small black hole stable.

==Observation==
===Accretion disks and gas jets===
[[Image:Black hole jet diagram.jpg|thumb|left|Formation of extragalactic jets from a black hole's [[Accretion disc|accretion disk]]]]
Most [[Accretion disc|accretion disks]] and [[Relativistic jet|gas jets]] are not clear proof that a [[stellar-mass black hole]] is present, because other massive, ultra-dense objects such as [[neutron star]]s and [[white dwarf]]s cause accretion disks and gas jets to form and to behave in the same ways as those around black holes. But they can often help by telling astronomers where it might be worth looking for a black hole.

On the other hand, extremely large accretion disks and gas jets may be good evidence for the presence of [[supermassive black hole]]s, because as far as we know any mass large enough to power these phenomena must be a black hole.
===Strong radiation emissions===
Steady [[X-ray]] and [[gamma ray]] emissions also do not prove that a black hole is present, but can tell astronomers where it might be worth looking for one - and they have the advantage that they pass fairly easily through [[nebula]]e and gas clouds.

But strong, irregular emissions of [[X-ray]]s, [[gamma ray]]s and other [[electromagnetic radiation]] can help to prove that a massive, ultra-dense object is ''not'' a black hole, so that "black hole hunters" can move on to some other object. Neutron stars and other very dense stars have surfaces, and matter colliding with the surface at a high percentage of the speed of light will produce intense flares of radiation at irregular intervals. Black holes have no material surface, so the absence of irregular flares around a massive, ultra-dense object suggests that there is a good chance of finding a black hole there.

Intense but one-time [[gamma ray burst]]s (GRBs) may signal the birth of "new" black holes, because astrophysicists think that GRBs are caused either by the [[gravitational collapse]] of giant stars<ref>{{cite journal |id={{arXiv|arxhive=astro-ph|id=0010176}} |doi=10.1086/338893 |title=The Observed Offset Distribution of Gamma-Ray Bursts from Their Host Galaxies: A Robust Clue to the Nature of the Progenitors |year=2002 |author=Bloom, J. S. |journal=The Astronomical Journal |volume=123 |pages=1111}}</ref> or by collisions between neutron stars,<ref name = "Harvard.edu-NeutronStars">{{
cite journal
|id={{bibcode|1984SvAL...10..177B}}
|author=Blinnikov, S., ''et al.''
|year=1984
|title=Exploding Neutron Stars in Close Binaries
|journal=Soviet Astronomy Letters
|volume=10
|pages=177
}}</ref> and both types of event involve sufficient mass and pressure to produce black holes. But it appears that a collision between a neutron star and a black hole can also cause a GRB,<ref>{{cite journal |doi=10.1086/154860 |title=The tidal disruption of neutron stars by black holes in close binaries |year=1976 |author=Lattimer, J. M. |journal=The Astrophysical Journal |volume=210 |pages=549}}</ref> so a GRB is not proof that a "new" black hole has been formed.
All known GRBs come from outside our own galaxy, and most come from billions of [[light year]]s away<ref>{{cite journal |id={{arXiv|archive=astro-ph|id=9505096}} |doi=10.1086/133674 |journal=[[Publications of the Astronomical Society of the Pacific]] |title=How Far Away Are Gamma-Ray Bursters? |first=Bohdan |last=Paczynski |authorlink=Bohdan Paczyński |volume=107 |year=1995 |pages=1167}}</ref> so the black holes associated with them are actually billions of years old.

Some astrophysicists believe that some [[ultraluminous X-ray source]]s may be the [[Accretion disc|accretion disks]] of [[intermediate-mass black hole]]s.<ref>{{cite journal |id={{arXiv|archive=astro-ph|id=0512480v2}} |doi=10.1086/506579 |title=''XMM‐Newton'' Archival Study of the Ultraluminous X‐Ray Population in Nearby Galaxies |year=2006 |author=Winter, Lisa M. |journal=The Astrophysical Journal |volume=649 |pages=730}}</ref>

[[Quasars]] are thought to be the accretion disks of [[supermassive black hole]]s, since no other known object is powerful enough to produce such strong emissions. Quasars produce strong emission across the [[electromagnetic spectrum]], including [[UV]], [[X-rays]] and [[gamma-rays]] and are visible at tremendous distances due to their high [[luminosity]]. Between 5 and 25% of quasars are "radio loud," so called because of their powerful [[radio]] emission.<ref>{{cite journal |id={{arXiv|archive=astro-ph|id=0611453}} |doi=10.1086/510831 |title=The Radio‐Loud Fraction of Quasars is a Strong Function of Redshift and Optical Luminosity |year=2007 |author=Jiang, Linhua |journal=The Astrophysical Journal |volume=656 |pages=680}}</ref>
===Gravitational lensing===
{{further|[[Gravitational lens]]}}
A [[gravitational lens]] is formed when the light from a very distant, bright source (such as a [[quasar]]) is bent around a massive object (such as a black hole) between the source object and the observer. The process is known as '''gravitational lensing''', and is one of the [[tests of general relativity|predictions]] of the general theory of relativity. According to this theory, [[mass]] warps [[space-time]] to create [[gravitational field]]s and therefore bend [[light]] as a result.

A source image behind the lens may appear as multiple images to the observer. In cases where the source, massive lensing object, and the observer lie in a straight line, the source will appear as a ring behind the massive object.

Gravitational lensing can be caused by objects other than black holes, because any very strong gravitational field will bend light rays. Some of these multiple-image effects are probably produced by distant galaxies.

===Orbiting objects===
{{See also|Kepler problem in general relativity}}
Objects orbiting black holes probe the gravitational field around the central object. An early example, discovered in the 1970s, is the accretion disk orbiting the putative black hole responsible for [[Cygnus X-1]], a famous X-ray source. While the material itself cannot be seen directly, the X rays flicker on a millisecond time scale, as expected for hot clumpy material orbiting a ~10 solar-mass black hole just prior to accretion. The X-ray spectrum exhibits the characteristic shape expected for a disk of orbiting relativistic material, with an iron line, emitted at ~6.4 keV, broadened to the red (on the receding side of the disk) and to the blue (on the approaching side).

Another example is the [[S2 (star)|star S2]], seen orbiting the [[Galactic center]]. Here the star is several light hours from the ~3.5×10<sup>6</sup> solar mass black hole, so its orbital motion can be plotted. Nothing is observed at the center of the observed orbit, the position of the black hole itself—as expected for a black object.
===Determining the mass of black holes===
[[Quasi-periodic oscillations]] can be used to determine the mass of black holes.<ref>{{cite press release |title=NASA scientists identify smallest known black hole |publisher=[[Goddard Space Flight Center]] |date=2008-04-01 |url=http://www.eurekalert.org/pub_releases/2008-04/nsfc-nsi040108.php |accessdate=2009-03-14}}</ref> The technique uses a relationship between black holes and the inner part of their surrounding disks, where gas spirals inward before reaching the event horizon. As the gas collapses inwards, it radiates X-rays with an intensity that varies in a pattern that repeats itself over a nearly regular interval. This signal is the Quasi-Periodic Oscillation, or QPO. A QPO’s frequency depends on the black hole’s mass; the event horizon lies close in for small black holes, so the QPO has a higher frequency. For black holes with a larger mass, the event horizon is farther out, so the QPO frequency is lower.
==Black hole candidates==
===Supermassive===
{{main| Supermassive black hole}}
[[Image:M87 jet.jpg|right|thumb|The jet originating from the center of [[Messier 87|M87]] in this image comes from an [[active galactic nucleus]] that may contain a [[supermassive black hole]]. Credit: [[Hubble Space Telescope]]/[[NASA]]/[[ESA]].]]

It is now widely accepted that the center of every or at least nearly every galaxy contains a supermassive black hole.<ref name="King">{{cite journal|url=http://www.iop.org/EJ/article/1538-4357/596/1/L27/17559.text.html|last=King|first=Andrew|date=2003-09-15|title=Black Holes, Galaxy Formation, and the MBH-σ Relation|journal=The Astrophysical Journal|publisher=The American Astronomical Society.|pages=596:L27-L29}}</ref><ref name="Richstone">{{cite web|url=http://hubblesite.org/newscenter/archive/releases/1997/01/text/|title=Massive Black Holes Dwell in Most Galaxies, According to Hubble Census|last= Richstone|first=Douglas|coauthors=Karl Gebhardt (University of Michigan), Scott Tremaine and John Magorrian (University of Toronto, Canadian Institute for Advanced Research), John Kormendy (University of Hawaii), Tod Lauer (National Optical Astronomy Observatories), Alan Dressler (Carnegie Observatories), Sandra Faber (University of California), Ralf Bender (Ludwig Maximilian University, Munich), Ed Ajhar (National Optical Astronomy Observatories), and Carl Grillmair (Jet Propulsion Laboratory).|date=January 13, 1997 |publisher=189th Meeting of the American Astronomical Society|accessdate=2009-05-17}}</ref> The close observational correlation between the mass of this hole and the velocity dispersion of the host galaxy's bulge, known as the [[M-sigma relation]], strongly suggests a connection between the formation of the black hole and the galaxy itself.<ref name="King" />

For decades, astronomers have used the term "[[active galaxy]]" to describe galaxies with unusual characteristics, such as unusual [[spectral line]] emission and very strong [[radio]] emission.<ref name="krolik1999">{{cite book
| author=J. H. Krolik
| year=1999
| title=Active Galactic Nuclei
| publisher=Princeton University Press
| location=Princeton, New Jersey
| isbn=0-691-01151-6}}{{pn}}</ref><ref name="sparkegallagher2000">{{cite book
| author=L. S. Sparke, J. S. Gallagher III
| year=2000
| title=Galaxies in the Universe: An Introduction
| publisher=Cambridge University Press
| location=Cambridge
| isbn=0-521-59704-4}}{{pn}}</ref> However, theoretical and observational studies have shown that the [[Active galactic nucleus|active galactic nuclei]] (AGN) in these galaxies may contain [[supermassive black holes]].<ref name="krolik1999"/><ref name="sparkegallagher2000"/> The models of these AGN consist of a central black hole that may be millions or billions of times more massive than the [[Sun]]; a disk of [[interstellar gas|gas]] and [[interstellar dust|dust]] called an [[Accretion disc|accretion disk]]; and two [[relativistic jet|jets]] that are perpendicular to the accretion disk.<ref name="sparkegallagher2000"/>

Although supermassive black holes are expected to be found in most AGN, only some galaxies' nuclei have been more carefully studied in attempts to both identify and measure the actual masses of the central supermassive black hole candidates. Some of the most notable galaxies with supermassive black hole candidates include the [[Andromeda Galaxy]], [[Messier 32|M32]], [[Messier 87|M87]], [[NGC 3115]], [[NGC 3377]], [[NGC 4258]], and the [[Sombrero Galaxy]].<ref name="kormendyrichstone1995">{{cite journal
| author=J. Kormendy, D. Richstone
| title=Inward Bound---The Search For Supermassive Black Holes In Galactic Nuclei
| journal=Annual Reviews of Astronomy and Astrophysics
| year=1995
| volume=33
| pages=581–624
| id={{bibcode|1995ARA&A..33..581K}}
| doi=10.1146/annurev.aa.33.090195.003053}}</ref>

Astronomers are confident that our own [[Milky Way]] galaxy has a supermassive black hole at its center, in a region called [[Sagittarius A*]]<ref name="Henderson">{{cite news|url=http://www.timesonline.co.uk/tol/news/uk/science/article5316001.ece|title=Astronomers confirm black hole at the heart of the Milky Way|last=Henderson|first=Mark|date=December 9, 2008 |publisher= Times Online|accessdate=2009-05-17}}</ref> since:
:* A star called [[S2 (star)|S2]] follows an [[elliptical]] orbit with a [[orbital period|period]] of 15.2 years and a [[pericenter]] (closest) distance of 17 [[light hour]]s from the central object.<ref>{{cite journal|last=Schödel|first=R.|coauthors=et al.|date=17 October 2002|title=A star in a 15.2-year orbit around the supermassive black hole at the centre of the Milky Way|journal=Nature |issue=419|pages=694-696|url=http://www.nature.com/nature/journal/v419/n6908/abs/nature01121.html|accessdate=Schodel}}</ref>
:* The first estimates indicated that the central object contains 2.6 million solar masses and has a radius of less than 17 light hours. Only a black hole can contain such a vast mass in such a small volume.
:* Further observations<ref>{{cite journal |last=Ghez |first=A. M. |authorlink=Andrea Ghez |coauthors=Salim, S.; Hornstein, S. D.; Tanner, A.; Lu, J. R.; Morris, M.; Becklin, E. E.; Duchêne, G. |title=Stellar Orbits around the Galactic Center Black Hole |journal=The Astrophysical Journal |volume=620 |issue=2 |pages=744–757 |year=2005 |month=May |url=http://www.journals.uchicago.edu/doi/abs/10.1086/427175 |accessdate=2008-05-10 |doi=10.1086/427175 |id={{arXiv|archive=astro-ph|id=0306130v2}}}}</ref> strengthened the case for a black hole, by showing that the central object's mass is about 3.7 million solar masses and its radius no more than 6.25 light-hours.

===Intermediate-mass===
{{main|Intermediate-mass black hole}}
In 2002, the Hubble Space Telescope produced observations indicating that [[globular clusters]] named [[Messier 15|M15]] and [[Mayall II|G1]] may contain [[intermediate-mass black hole]]s.<ref>{{cite arXiv |eprint=astro-ph/0209315v2 |author1=Joris Gerssen |last2=van der Marel | first2=Roeland P. |author3=Karl Gebhardt |author4=Puragra Guhathakurta |author5=Ruth Peterson |author6=Carlton Pryor |title=Hubble Space Telescope Evidence for an Intermediate-Mass Black Hole in the Globular Cluster M15: II. Kinematical Analysis and Dynamical Modeling |class=astro-ph |year=2002}}</ref><ref>{{cite press release |title=Hubble Discovers Black Holes in Unexpected Places |url=http://hubblesite.org/newscenter/archive/releases/cosmology/2002/18/text/ |publisher=[[Space Telescope Science Institute]] |date=2002-09-17 |accessdate=2009-03-14}}</ref> This interpretation is based on the sizes and periods of the orbits of the stars in the globular clusters. But the Hubble evidence is not conclusive, since a group of [[neutron star]]s could cause similar observations. Until recent discoveries, many astronomers thought that the complex gravitational interactions in globular clusters would eject newly-formed black holes.

In November 2004 a team of astronomers reported the discovery of the first well-confirmed [[intermediate-mass black hole]] in our Galaxy, orbiting three light-years from Sagittarius A*. This black hole of 1,300 solar masses is within a cluster of seven stars, possibly the remnant of a massive star cluster that has been stripped down by the Galactic Centre.<ref name = "Nature.com-20060325">{{cite web |url=http://www.nature.com/news/2004/041108/full/news041108-2.html |title=Second black hole found at the centre of our Galaxy |work=NatureNews |accessdate=2006-03-25 |doi=10.1038/news041108-2 |year=2004 |last=Peplow |first=Mark}}</ref><ref name = "edpsciences-usa.org-2004">{{cite arXiv |eprint=astro-ph/0404450v1 |last1=Maillard | first1=J. P. |last2=Paumard | first2=T. |last3=Stolovy | first3=S. R. |last4=Rigaut | first4=F. |title=The nature of the Galactic Center source IRS 13 revealed by high spatial resolution in the infrared |class=astro-ph |year=2004}}</ref> This observation may add support to the idea that supermassive black holes grow by absorbing nearby smaller black holes and stars.

In January 2007, researchers at the University of Southampton in the United Kingdom reported finding a black hole, possibly of about 10 solar masses, in a globular cluster associated with a galaxy named NGC 4472, some 55 million light-years away.<ref>{{cite arXiv |eprint=0805.2952v2 |last1=Zepf | first1=Stephen E. |author2=Daniel Stern |last3=Maccarone | first3=Thomas J. |author4=Arunav Kundu |author5=Marc Kamionkowski |last6=Rhode | first6=Katherine L. |last7=Salzer | first7=John J. |author8=Robin Ciardullo |author9=Caryl Gronwall |title=Very Broad [O III]4959,5007 Emission from the NGC 4472 Globular Cluster
RZ2109 and Implications for the Mass of Its Black Hole X-ray Source |class=astro-ph |year=2008}}</ref><ref>{{cite arXiv |eprint=astro-ph/0701310v1 |last1=Maccarone | first1=Thomas J. |author2=Arunav Kundu |last3=Zepf | first3=Stephen E. |last4=Rhode | first4=Katherine L. |title=A black hole in a globular cluster |class=astro-ph |year=2007}}</ref>
===Stellar-mass===
{{main|Stellar black hole}}
[[Image:Accretion disk.jpg|right|thumb|Artist's impression of a binary system consisting of a black hole and a [[main sequence]] star. The black hole is drawing matter from the main sequence star via an [[Accretion disc|accretion disk]] around it, and some of this matter forms a [[Relativistic jet|gas jet]].]]

Our Milky Way galaxy contains several probable [[stellar-mass black hole]]s which are closer to us than the supermassive black hole in the [[Sagittarius A*]] region. These candidates are all members of [[X-ray binary]] systems in which the denser object draws matter from its partner via an accretion disk. The probable black holes in these pairs range from three to more than a dozen [[solar mass]]es.<ref name = "Casares-Holes">{{cite arXiv |eprint=astro-ph/0612312v1 |author1=Jorge Casares |title=Observational evidence for stellar-mass black holes |class=astro-ph |year=2006}}</ref><ref name = "Garcia-Jets">{{cite arXiv |eprint=astro-ph/0302230v2 |last1=Garcia | first1=M. R. |last2=Miller | first2=J. M. |last3=McClintock | first3=J. E. |last4=King | first4=A. R. |last5=Orosz | first5=J. |title=Resolved Jets and Long-Period Black Hole X-ray Novae |class=astro-ph |year=2003}}</ref> The most distant stellar-mass black hole ever observed is a member of a binary system located in the [[Messier 33]] galaxy.<ref>{{cite arXiv |eprint=0710.3165v1 |last1=Orosz | first1=Jerome A. |last2=McClintock | first2=Jeffrey E. |author3=Ramesh Narayan |last4=Bailyn | first4=Charles D. |last5=Hartman | first5=Joel D. |author6=Lucas Mracri |author7=Jiefeng Liu |author8=Wolfgang Pietsch |last9=Remillard | first9=Ronald A. |author10=Avi Shporer |author11=Tsevi Mazeh |title=A 15.65 solar mass black hole in an eclipsing binary in the nearby spiral galaxy Messier 33 |class=astro-ph |year=2007}}</ref>
===Micro===
{{main|Micro black hole}}
There is theoretically no smallest size for a black hole. Once created, it has the properties of a black hole. [[Stephen Hawking]] theorized that [[primordial black hole]]s could evaporate and become even tinier, i.e. [[micro black hole]]s. Searches for evaporating primordial black holes are proposed for the [[Fermi Gamma-ray Space Telescope]], which was launched on June 11, 2008. However, if micro black holes can be created by other means, such as by cosmic ray impacts or in colliders, that does not imply that they must evaporate.

The formation of black hole analogs on Earth in [[particle accelerators]] has been reported. These black hole analogs are not the same as gravitational black holes, but they are vital testing grounds for quantum theories of gravity.<ref>{{cite arXiv |eprint=hep-th/0501068v3 |first=Horatiu |last=Nastase |authorlink=Horaţiu Năstase |title=The RHIC fireball as a dual black hole |class=hep-th |year=2005 |author1=Horatiu Nastase}}</ref>

They act like black holes because of the [[AdS/CFT correspondence|correspondence]] between the theory of the strong nuclear force, which has nothing to do with gravity, and the quantum theory of gravity. They are similar because both are described by [[string theory]]. So the formation and disintegration of a [[quark-gluon plasma|fireball]] in quark gluon plasma can be interpreted in black hole language. The fireball at the [[Relativistic Heavy Ion Collider]] [RHIC] is a phenomenon which is closely analogous to a black hole, and many of its physical properties can be correctly predicted using this analogy. The fireball, however, is not a gravitational object. It is presently unknown whether the much more energetic [[Large Hadron Collider]] [LHC] would be capable of producing the speculative large extra dimension micro black hole, as many theorists have suggested. See [[Safety of particle collisions at the Large Hadron Collider]] for a more in depth discussion.
==Advanced topics==
===Worm holes===
{{main|Wormhole}}
[[Image:LorentzianWormhole.jpg|thumb|Diagram of a Schwarzschild wormhole.]]
General relativity describes the possibility of configurations in which two black holes are connected to each other. Such a configuration is usually called a [[wormhole]]. Wormholes have inspired [[science fiction]] authors because they offer a means to travel quickly over long distances and even time travel. In practice, such configurations seem completely unfeasible in astrophysics, because no known process seems to allow the formation of such objects.
===Entropy and Hawking radiation===
{{further|[[Hawking radiation]]|[[Black hole thermodynamics]]}}
In 1971, [[Stephen Hawking]] showed that the total area of the event horizons of any collection of classical black holes can never decrease, even if they collide and swallow each other; that is merge.<ref>{{cite book |first=Stephen |last=Hawking |authorlink=Stephen Hawking |title=[[A Brief History of Time]] |publisher=Bantam Books |location=New York |year=1998 |pages= |isbn=0-553-38016-8}}{{pn}}</ref> This is remarkably similar to the Second Law of [[Thermodynamics]], with area playing the role of [[entropy]]. As a classical object with zero temperature it was assumed that black holes had zero entropy. If this were the case, the second law of thermodynamics would be violated by entropy-laden matter entering the black hole, resulting in a decrease of the total entropy of the universe. Therefore, [[Jacob Bekenstein]] proposed that a black hole should have an entropy, and that it should be proportional to its horizon area. Since black holes do not classically emit radiation, the thermodynamic viewpoint seemed simply an analogy, since zero temperature implies infinite changes in entropy with any addition of heat, which implies infinite entropy. However, in 1974, Hawking applied [[quantum field theory]] to the curved spacetime around the event horizon and discovered that black holes emit [[Hawking radiation]], a form of [[thermal radiation]], allied to the [[Unruh effect]], which implied they had a positive temperature. This strengthened the analogy being drawn between black hole dynamics and thermodynamics: using the [[Laws of black hole mechanics#The First Law|first law of black hole mechanics]], it follows that the entropy of a non-rotating black hole is one quarter of the area of the horizon. This is a universal result and can be extended to apply to cosmological horizons such as in [[de Sitter space]]. It was later suggested that black holes are maximum-entropy objects, meaning that the maximum possible entropy of a region of space is the entropy of the largest black hole that can fit into it. This led to the [[holographic principle]].

The Hawking radiation reflects a characteristic [[temperature]] of the black hole, which can be calculated from its entropy. The more its temperature falls, the more massive a black hole becomes: the more energy a black hole absorbs, the colder it gets. A black hole with roughly the [[Orders of magnitude (mass)#23|mass of the planet Mercury]] would have a temperature in equilibrium with the cosmic microwave background radiation (about 2.73 K). More massive than this, a black hole will be colder than the background radiation, and it will gain energy from the background faster than it gives energy up through Hawking radiation, becoming even colder still. However, for a less massive black hole the effect implies that the mass of the black hole will slowly evaporate with time, with the black hole becoming hotter and hotter as it does so. Although these effects are negligible for black holes massive enough to have been formed astronomically, they would rapidly become significant for hypothetical [[micro black hole|smaller black holes]], where quantum-mechanical effects dominate. Indeed, small black holes are predicted to undergo runaway evaporation and eventually vanish in a burst of radiation.
[[Image:First Gold Beam-Beam Collision Events at RHIC at 100 100 GeV c per beam recorded by STAR.jpg|thumb|left|If ultra-high-energy collisions of particles in a [[particle accelerator]] can create microscopic black holes, it is expected that all types of particles will be emitted by black hole evaporation, providing key evidence for any [[grand unified theory]]. Above are the high energy particles produced in a gold ion collision on the [[Relativistic Heavy Ion Collider|RHIC]].]]
Although general relativity can be used to perform a semi-classical calculation of black hole entropy, this situation is theoretically unsatisfying. In [[statistical mechanics]], entropy is understood as counting the number of microscopic configurations of a system which have the same macroscopic qualities (such as [[mass]], [[Charge (physics)|charge]], [[pressure]], etc.). But without a satisfactory theory of [[quantum gravity]], one cannot perform such a computation for black holes. Some promise has been shown by [[string theory]], however, which posits that the microscopic degrees of freedom of the black hole are [[D-brane]]s. By counting the states of D-branes with given charges and energy, the entropy for certain [[supersymmetric]] black holes has been reproduced. Extending the region of validity of these calculations is an ongoing area of research.

===Black hole unitarity===
{{main|Black hole information paradox}}
An open question in fundamental physics is the so-called information loss paradox, or [[black hole information paradox|black hole unitarity]] paradox. Classically, the laws of physics are the same run forward or in reverse ([[T-symmetry]]). [[Liouville's Theorem]] dictates conservation of phase space volume, which can be thought of as 'conservation of information', so there is some problem even in classical (non-quantum general relativity) physics. In quantum mechanics, this corresponds to a vital property called [[unitarity (physics)|unitarity]], which has to do with the conservation of probability (It can also be thought of as a conservation of quantum phase space volume as expressed by the [[density matrix]]).<ref name="PlayDice000">{{cite web
| title=Does God Play Dice?
| first=Stephen
| last=Hawking
| authorlink=Stephen Hawking
| url=http://www.hawking.org.uk/index.php/lectures/publiclectures/64
| accessdate=2009-03-14
}}</ref>

Black holes, however, might violate this rule. The position under classical general relativity is subtle but straightforward: because of the classical [[no hair theorem]], it can never be determined what went into the black hole. However, as seen from the outside, information is never actually destroyed, as matter falling into the black hole takes an infinite time to reach the event horizon.

It should be pointed out that the equations of [[general relativity]] in fact obey [[T-symmetry]], and given that the logic above comes from application of (classical) general relativity, one should be suspicious. This is due to the fact that it should not be possible to derive time-reversal-asymmetric conclusions from a time-symmetric theory ([[Loschmidt's paradox]]), which is general relativity in this case. [[Rindler coordinates]], which apply near the event horizon for an observer "held" just outside the black hole, are T-symmetric and therefore there should not exist any such thing as an 'irreversible' process. It is possible that the 'paradox' is a result of applying time-asymmetric boundary conditions to the time-symmetric theory, making it a form of Loschmidt's paradox.

[[Bekenstein bound|Ideas about quantum gravity]], on the other hand, suggest that there can only be a limited finite entropy (i.e. a maximum finite amount of information) associated with the space near the horizon; but the change in the entropy of the horizon plus the entropy of the Hawking radiation is always sufficient to take up all of the entropy of matter and energy falling into the black hole.

Many physicists are concerned, however, that this is still not sufficiently well understood. In particular, at a quantum level, is the quantum state of the Hawking radiation uniquely determined by the history of what has fallen into the black hole; and is the history of what has fallen into the black hole uniquely determined by the quantum state of the black hole and the radiation? This is what determinism, and unitarity, would require.

For a long time [[Stephen Hawking]] had opposed such ideas, holding to his original 1975 position that the Hawking radiation is entirely thermal and therefore entirely random, containing none of the information held in material the hole has swallowed in the past; this information he reasoned had been lost. However, on 21 July 2004 he presented a new argument, reversing his previous position.<ref name = "Nature-20040407">{{cite web |url=http://www.nature.com/news/2004/040715/full/news040712-12.html |title=Hawking changes his mind about black holes |work=Nature News |accessdate=2006-03-25 |doi=10.1038/news040712-12}}</ref> On this new calculation, the entropy (and hence information) associated with the black hole escapes in the Hawking radiation itself. However, making sense of it, even in principle, is difficult until the black hole completes its evaporation. Until then it is impossible to relate in a 1:1 way the information in the Hawking radiation (embodied in its detailed internal correlations) to the initial state of the system. Once the black hole evaporates completely, such identification can be made, and unitarity is preserved.

By the time Hawking completed his calculation, it was already very clear from the AdS/CFT correspondence that black holes decay in a unitary way. This is because the fireballs in gauge theories, which are analogous to Hawking radiation, are unquestionably unitary. Hawking's new calculation has not been evaluated by the specialist scientific community, because the methods he uses are unfamiliar and of dubious consistency; but Hawking himself found it sufficiently convincing to pay out on a [[Thorne-Hawking-Preskill bet|bet]] he had made in 1997 with Caltech physicist [[John Preskill]], to considerable media interest.

===Holographic world===
{{main|Holographic principle}}
[[Leonard Susskind]] and Nobel prizewinner [[Gerard 't Hooft]] have suggested that the three dimensional space surrounding a black hole can be completely described by a two dimensional behavior of the horizon.<ref>{{cite news |url=http://www.newscientist.com/article/mg20126911.300-our-world-may-be-a-giant-hologram.html |title=Our world may be a giant hologram |work=[[New Scientist]] |date=2009-01-15 |issue=2691 |first=Marcus |last=Chown |authorlink=Marcus Chown}}</ref> They believe this because this can resolve the [[black hole information paradox|black hole information-loss paradox]]. This idea has been made precise within string theory, and it is known as the [[holographic principle]].<!--

==Mathematical theory of non-rotating, uncharged black holes==
{{see|Schwarzschild metric |Deriving the Schwarzschild solution}}
===Black holes in 3 dimensions===
A black hole solution is also known for 3 dimensional spacetimes. This so called [[BTZ black hole]] exists however only for a negative cosmological constant.

In general relativity, there are many known solutions of the [[Einstein field equations]] which describe [[Black hole#Types of black holes|different types of black holes]]. The [[Schwarzschild metric]] is one of the earliest and simplest solutions. This solution describes the [[curvature]] of [[spacetime]] in the vicinity of a static and [[sphere|spherically]] [[symmetry|symmetric]] uncharged object, where the [[Metric space|metric]] is,

:<math> \mathrm{d}s^2 = - c^2 \left( 1 - {2Gm \over c^2 r} \right) \mathrm{d}t^2 + \left( 1 - {2Gm \over c^2 r} \right)^{-1} \mathrm{d}r^2 + r^2 \mathrm{d}\Omega^2 </math>,

where <math>\mathrm{d}\Omega^2 = \mathrm{d}\theta^2 + \sin^2\theta\; \mathrm{d}\phi^2</math> is a standard element of solid angle.

According to general relativity, a gravitating object will collapse into a black hole if its radius is smaller than a characteristic distance, known as the [[Schwarzschild radius]]. (Indeed, [[Buchdahl's theorem]] in general relativity shows that in the case of a [[fluid solution|perfect fluid model]] of a compact object, the true lower limit is somewhat larger than the Schwarzschild radius.) Below this radius, spacetime is so strongly curved that any light ray emitted in this region, regardless of the direction in which it is emitted, will travel towards the centre of the system. Because [[special relativity|relativity]] forbids anything from traveling [[faster-than-light|faster than light]], anything below the Schwarzschild radius &ndash; including the constituent particles of the gravitating object &ndash; will collapse into the centre. A [[gravitational singularity]], a region of theoretically infinite density, forms at this point. Because not even light can escape from within the Schwarzschild radius, a classical black hole would truly appear [[black]].

The Schwarzschild radius is given by

:<math>r_{\rm S} = {2\,Gm \over c^2} </math>

where ''G'' is the [[gravitational constant]], ''m'' is the [[mass]] of the object, and ''c'' is the [[speed of light]]. For an object with the mass of the [[Earth]], the Schwarzschild radius is a mere 9 millimeters&mdash;about the size of a [[marble (toy)|marble]].

The mean density inside the Schwarzschild radius decreases as the mass of the black hole increases, so while an earth-mass black hole would have a density of 2&nbsp;×&nbsp;10<sup>30</sup>&nbsp;kg/m³, a supermassive black hole of 10<sup>9</sup> [[solar mass]]es has a density of around 20&nbsp;kg/m³, less than water! The mean density is given by

:<math>\rho=\frac{3\,c^6}{32\pi m^2G^3}.</math>

Since the Earth has a mean radius of 6371&nbsp;km, its volume would have to be reduced 4 × 10<sup>26</sup> times to collapse into a black hole. For an object with the mass of the [[Sun]], the Schwarzschild radius is approximately 3&nbsp;km, much smaller than the Sun's current radius of about 696,000&nbsp;km. It is also significantly smaller than the radius to which the Sun will ultimately shrink after exhausting its nuclear fuel, which is several thousand kilometers. More massive stars can collapse into black holes at the end of their lifetimes.

The formula also implies that any object with a given mean density is a black hole if its radius is large enough. The same formula applies for [[white holes]] as well. For example, if the [[observable universe]] has a mean density equal to the [[critical density]], then it is a [[white hole]], since its [[Gravitational singularity|singularity]] is in the past and not in the future as should be for a black hole.

There is also the Black Hole Entropy formula:

:<math>S = \frac{Akc^3}{4\hbar G}.</math>

Where '''A''' is the area of the event horizon of the black hole, '''<math>\hbar</math>''' is [[Dirac's constant]] (the "reduced [[Planck constant]]"), '''k''' is the [[Boltzmann constant]], '''G''' is the [[gravitational constant]], '''c''' is the [[speed of light]] and '''S''' is the [[entropy]].

A convenient length scale to measure black hole processes is the "gravitational radius", which is equal to
:<math>r_{\rm G} = {Gm \over c^2} .</math>
When expressed in terms of this length scale, many phenomena appear at integer radii.
For example, the radius of a Schwarzschild black hole is two gravitational radii and the radius of a maximally rotating Kerr black hole is one gravitational radius. The location of the light circularization radius around a Schwarzschild black hole (where light may orbit the hole in an unstable circular orbit) is <math>3r_{\rm G}</math>. The location of the marginally stable orbit, thought to be close to the inner edge of an accretion disk, is at <math>6r_{\rm G}</math> for a Schwarzschild black hole. -->

===Fuzzballs===
{{main|Fuzzball (string theory)}}
Fuzzballs are theorized by some [[superstring theory]] scientists to be the true [[Quantum mechanics|quantum]] description of black holes. The theory resolves two intractable problems that classic black holes pose for modern physics:

# The [[Black hole information paradox|information paradox]] wherein the quantum information bound in in{{nbhyph}}falling matter and energy entirely disappears into a singularity; that is, the black hole would undergo zero physical change in its composition regardless of the nature of what fell into&nbsp;it.
# The singularity at the heart of the black hole, where conventional black hole theory says there is infinite spacetime curvature due to an infinitely intense gravitational field from a region of zero volume. Modern physics breaks down when such parameters are infinite and zero.<!--

--><ref>The smallest linear dimension in physics that has any meaning in the measurement of spacetime is the [[Planck length]], which is {{val|1.616252|(81)|e=-35|u=m}} ([http://physics.nist.gov/cgi-bin/cuu/Value?plkl CODATA value]). Below the Planck length, the effects of quantum foam dominate and it is meaningless to conjecture about length at a finer scale—much like how meaningless it would be to measure ocean tides at a precision of one centimeter in storm-tossed seas. A singularity is thought to have a diameter that doesn’t amount to even one Planck length; which is to say, zero.</ref>

Fuzzball theory replaces the singularity at the heart of a black hole by positing that the entire region within the black hole’s event horizon is actually a ball of [[String (physics)|strings]], which are advanced as the ultimate building blocks of matter and energy. Strings are thought to be bundles of energy vibrating in complex ways in both the three physical dimensions of space as well as in ''compact directions''—extra dimensions interwoven in the [[quantum foam]] (also known as ''spacetime foam)''.

==See also==
{{col-begin}}
{{col-break}}
*[[Schwarzschild metric]]
*[[Black hole information paradox]]
*[[Black string]]
*[[Fuzzball (string theory)]]
*[[Gravitational singularity]]
*[[Kugelblitz (astrophysics)]]
*[[Wormhole]]
{{col-break}}
*[[Neutron star]]
*[[Spacetime]]
*[[Supermassive black hole]]
*[[Susskind-Hawking battle]]
*[[Timeline of black hole physics]]
*[[White hole]]
*[[List of black holes]]
{{col-end}}

==References==
{{reflist|2}}
==Further reading==
===Popular reading===
*{{Citation | author=Ferguson, Kitty | title=Black Holes in Space-Time | publisher=Watts Franklin | year=1991 | id=ISBN 0-531-12524-6}}.
*{{Citation |first1=Stephen |last1=Hawking |author1-link=Stephen Hawking | title=[[A Brief History of Time]] | publisher=Bantam Books, Inc | year=1988 | id=ISBN 0-553-38016-8}}.
*{{Citation |first1=Stephen |last1=Hawking |author1-link=Stephen Hawking |first2=Roger |last2=Penrose |author2-link=Roger Penrose |title=The Nature of Space and Time |year=1996 |publisher=Princeton University Press |isbn=0-691-03791-2 |url=http://books.google.nl/books?id=LstaQTXP65cC}}.
*{{Citation | author=[[Fulvio Melia|Melia, Fulvio]] | title=The Black Hole at the Center of Our Galaxy | publisher=Princeton U Press | year=2003 | id=ISBN 978-0-691-09505-9}}.
*{{Citation | author=[[Fulvio Melia|Melia, Fulvio]] | title=The Edge of Infinity. Supermassive Black Holes in the Universe | publisher=Cambridge U Press | year=2003 | id=ISBN 978-0-521-81405-8}}.
*{{Citation | author=Pickover, Clifford | title=Black Holes: A Traveler's Guide | publisher=Wiley, John & Sons, Inc | year=1998 | id=ISBN 0-471-19704-1}}.
*{{Citation | author=Thorne, Kip S. |author-link=Kip Thorne | title=[[Black Holes and Time Warps]] | publisher=Norton, W. W. & Company, Inc | year=1994 | id=ISBN 0-393-31276-3}}.
*{{Citation |last=Stern |first=B. |title=Blackhole |url= http://www.wikilivres.info/wiki/Blackhole_%28Stern%29
|year=2008}}, poem.

===University textbooks and monographs===
*{{Citation |last=Carroll |first=Sean M. |title=Spacetime and Geometry |year=2004 |publisher=Addison Wesley |isbn=0-8053-8732-3}}, the lecture notes on which the book was based are available for free from Sean Carroll's [http://pancake.uchicago.edu/~carroll/notes/ website].
*{{Citation |last=Carter |first=B. |year=1973 |chapter=Black hole equilibrium states |title=Black Holes |editor-last=DeWitt |editor-first=B.S. |editor1-link=Bryce De Witt |editor2-last=DeWitt |editor2-first=C.}}.
*{{Citation | author=Chandrasekhar, Subrahmanyan | title=Mathematical Theory of Black Holes | publisher=Oxford University Press | year=1999 | id=ISBN 0-19-850370-9}}.
*{{Citation |last1=Frolov |first1=V.P. |last2=Novikov |first2=I.D. |year=1998 |title=Black hole physics}}.
*{{Citation| last1=Hawking |first1=S.W. |author-link=Stephen Hawking |last2=Ellis |first2=G.F.R. |title=Large Scale Structure of space time |publisher=Cambridge University Press |year=1973 |url=http://books.google.nl/books?id=QagG_KI7Ll8C |isbn=0521099064}}.
*{{Citation | author=[[Fulvio Melia|Melia, Fulvio]] | title=The Galactic Supermassive Black Hole | publisher=Princeton U Press | year=2007 | id=ISBN 978-0-691-13129-0}}.
*{{Citation | author1=Taylor, Edwin F. |author2=Wheeler, John Archibald |author2-link=John Wheeler|
title=Exploring Black Holes | publisher=Addison Wesley Longman |
year=2000 | id=ISBN 0-201-38423-X}}.
*{{Citation |author1=Thorne, Kip S. |author2=Misner, Charles |author3=Wheeler, John |author1-link=Kip Thorne |author2-link=Charles W. Misner|author3-link=John Wheeler | title=Gravitation | publisher=W. H. Freeman and Company | year=1973 | id=ISBN 0-7167-0344-0}}.
*{{Citation | author=Wald, Robert M. |author-link=Robert Wald | title=Space, Time, and Gravity: The Theory of the Big Bang and Black Holes | publisher= University of Chicago Press| year=1992 | id=ISBN 0-226-87029-4}}.

===Research papers===
*{{cite journal |id={{arXiv|archive=hep-th|id=0507171v2}} |doi=10.1103/PhysRevD.72.084013 |title=Information loss in black holes |year=2005 |author=Hawking, S. |journal=Physical Review D |volume=72 |pages=084013}} Stephen Hawking's purported solution to the black hole [[unitarity]] paradox, first reported at a conference in July 2004.
*{{cite journal |id={{arXiv|archive=astro-ph|id=0306130v2}} |doi=10.1086/427175 |title=Stellar Orbits around the Galactic Center Black Hole |year=2005 |author=Ghez, A. M. |journal=The Astrophysical Journal |volume=620 |pages=744}} More accurate mass and position for the black hole at the centre of the Milky Way.
*{{cite arXiv |eprint=hep-ph/0511217v2 |last1=Hughes | first1=Scott A. |title=Trust but verify: The case for astrophysical black holes |class=hep-ph |year=2005}} Lecture notes from 2005 [[SLAC]] Summer Institute.
==External links==
* [[Stanford Encyclopedia of Philosophy]]: "[http://plato.stanford.edu/entries/spacetime-singularities/ Singularities and Black Holes]" by Erik Curiel and Peter Bokulich.
*''[[Scientific American]]'':
**"[http://www.sciam.com/article.cfm?chanID=sa006&articleID=0004567B-11FB-1EDD-8E1C809EC588EF21 The Galactic Odd Couple: giant black holes and stellar baby booms,]" July 2003;
**"[http://www.sciam.com/article.cfm?chanID=sa006&articleID=000CCC72-2AED-1264-980683414B7F0000 Quantum Black Holes,]" May 2005.
*"[http://www.scholarpedia.org/article/Black_hole Black hole]" on Scholarpedia.
*"[http://news.bbc.co.uk/2/hi/science/nature/7774287.stm Black Hole confirmed in Milky Way.]" Retrieved December 10, 2008
*[http://video.google.com/videoplay?docid=-6215434494081736769&hl=en Yale University Video Lecture: Introduction to Black Holes] at Google Video.
*[http://hubblesite.org/explore_astronomy/black_holes/ Black Holes: Gravity's Relentless Pull] - Award-winning interactive multimedia Web site about the physics and astronomy of black holes from the Space Telescope Science Institute
*[http://antwrp.gsfc.nasa.gov/htmltest/gifcity/bh_pub_faq.html FAQ on black holes]
*"[http://casa.colorado.edu/~ajsh/schwp.html Schwarzschild Geometry]" on [http://casa.colorado.edu/~ajsh/ Andrew Hamilton’s website]
*Tufts University: [http://hepguru.com/blackholes/ Student Project (Great Kid's Section)]
*[http://www.mpe.mpg.de/ir/GC/index.php Movie of Black Hole Candidate from Max Planck Institute]
*[https://blue.utb.edu/newsandinfo/2006%AD%AD_04_13BreakthroughBlackHoles.htm UT Brownsville Group Simulates Spinning Black-Hole Binaries]
*[http://www.sciencedaily.com/news/space_time/black_holes/ Black Hole Research News] on [http://www.sciencedaily.com/ ScienceDaily]
*[http://www.space.com/blackholes/ SPACE.com All About Black Holes] - News, Features and Interesting Original Videos
*[http://www.damtp.cam.ac.uk/user/gr/public/bh_intro.html Black Holes Intro] - Introduction to Black Holes
*[http://library.thinkquest.org/C007571/english/advance/core8.htm Advanced Mathematics of Black Hole Evaporation]
*[http://science.howstuffworks.com/black-hole.htm HowStuffWorks: How Black Holes Work] - Easy to consume guide to Black Holes
*[http://www.richmond.edu/~ebunn/ Ted Bunn's] [http://cosmology.berkeley.edu/Education/BHfaq.html Black Holes FAQ] explains in simple language some other consequences of the way in which black holes bend space-time.
*[http://thefutureofthings.com/news/1313/is-the-mass-of-black-holes-limited.html Is the Mass of Black Holes Limited?] - [[The Future of Things]] article

{{Black holes|state=uncollapsed}}
[[Category:Black holes|Black holes]]
[[Category:Dark matter]]
[[Category:Relativity]]
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[[bg:Черна дупка]]
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[[de:Schwarzes Loch]]
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[[ka:შავი ხვრელი]]
[[sw:Shimo nyeusi]]
[[ku:Çala Reş]]
[[la:Gurges ater]]
[[lv:Melnais caurums]]
[[lt:Juodoji skylė]]
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[[hu:Fekete lyuk]]
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[[zh-yue:黑洞]]
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[[zh:黑洞]]

Revision as of 19:59, 2 October 2009

Its 5 inches from the earth.

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