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Nonsingular black hole models

From Wikipedia, the free encyclopedia
Models of black holes without gravitational singularities

Anonsingular black hole model is a mathematical theory ofblack holes that avoids certain theoretical problems with the standard black hole model, includinginformation loss and the unobservable nature of the black holeevent horizon.

Avoiding paradoxes in the standard black hole model

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For a black hole to physically exist as a solution toEinstein's equation, it must form an event horizon in finite time relative to outside observers. This requires an accurate theory of black hole formation, of which several have been proposed. In 2007,Shuan Nan Zhang ofTsinghua University proposed a model in which the event horizon of a potential black hole only forms (or expands) after an object falls into the existing horizon, or after the horizon has exceeded the critical density. In other words, an infalling object causes the horizon of a black hole to expand, which only occurs after the object has fallen into the hole, allowing an observable horizon in finite time.[1][2]

Alternative black hole models

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Nonsingular black hole models have been proposed since theoretical problems with black holes were first realized.[3] Today some of the most viable candidates for the result of the collapse of a star with mass well above theChandrasekhar limit include thegravastar and thedark energy star.

While black holes were a well-established part of mainstream physics for most of the end of the 20th century, alternative models received new attention when models proposed byGeorge Chapline and later byLawrence Krauss,Dejan Stojkovic, andTanmay Vachaspati ofCase Western Reserve University showed in several separate models that black hole horizons could not form.[4][5]

Such research has attracted much media attention,[6] as black holes have long captured the imagination of both scientists and the public for both their innate simplicity and mysteriousness. The recent theoretical results have therefore undergone much scrutiny and most of them are now ruled out by theoretical studies. For example, several alternative black hole models were shown to be unstable in extremely fast rotation,[7] which, by conservation ofangular momentum, would be a not unusual physical scenario for a collapsed star (seepulsar). Nevertheless, the existence of a stable model of a nonsingular black hole is still an open question.

Hayward metric

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TheHayward metric is the simplest description of ablack hole that isnon-singular. The metric was written down by Sean Hayward as the minimal model that is regular, static,spherically symmetric andasymptotically flat.[8]

Ayón-Beato–García metric

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The Ayón-Beato–García model is the first exact charged regular black hole with a source.[9] The model was proposed by Eloy Ayón Beato and Alberto García in 1998 based on the minimal coupling between anonlinear electrodynamics model andgeneral relativity, considering a static andspherically symmetric spacetime. Later the same authors reinterpreted the first non-singular black hole geometry, the Bardeen toy Model,[10] as a nonlinear-electrodynamics-based regular black hole.[11] Nowadays, it is known that the Ayón-Beato–García model may mimic the absorption properties of theReissner–Nordström metric, from the perspective of the absorption of massless testscalar fields.[12]

Nonsingular black holes as dark matter

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In 2024, Paul C.W. Davies, Damien A. Easson, and Phillip B. Levin proposed that nonsingular black holes are a viable candidate for dark matter.[13] They showed that the nonsingular Schwarzschild-de Sitter black hole slowly evaporates, reaching a maximum but finite temperature, then forms a black hole remnant that does not have a singularity and whose mass is on the order of the Planck mass. This nonsingular black hole can comprise all of the dark matter in the observable universe because the fraction of primordial black holes that is dark matter is inversely proportional to the smallest mass primordial black hole that could have survived since the primordial era. It was previously thought that Hawking evaporation set the lower bound of primordial black holes to be 1012 kg, but nonsingular black holes, which form remnants and do not evaporate completely, lower this bound to the Planck mass, which is 10−8 kg. Thus Planck mass nonsingular black holes formed primordially can comprise all of the dark matter in the observable universe today.

See also

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References

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  1. ^Zhang, Shuang Nan; Tang, Sumin (2007-07-06)."Witnessing matter falling into a black hole by a distant observer". Tsinghua University. Retrieved2007-11-03.[permanent dead link]
  2. ^Zhang, Shuang Nan; Liu, Yuan (2008). "Observe matter falling into a black hole".AIP Conf. Proc.968:384–391.arXiv:0710.2443.Bibcode:2008AIPC..968..384Z.doi:10.1063/1.2840436.S2CID 15169576.
  3. ^Bardeen, JM (1968). "Non-singular general relativistic gravitational collapse".In Proceedings of the International Conference GR5, Tbilisi, USSR.174: 87.Bibcode:1968qtr..conf...87B.
  4. ^Chapline, George (July 1998). "The Black Hole Information Puzzle and Evidence for a Cosmological Constant".arXiv:hep-th/9807175.
  5. ^Vachaspati, Tanmay;Dejan Stojkovic;Lawrence M. Krauss (June 2007). "Observation of Incipient Black Holes and the Information Loss Problem".Phys. Rev. D.76 (2) 024005.arXiv:gr-qc/0609024.Bibcode:2007PhRvD..76b4005V.doi:10.1103/PhysRevD.76.024005.S2CID 119333620.
  6. ^Rockets, Rusty (2007-06-22)."Rethinking Black Holes". Science A Gogo.Archived from the original on 2007-10-10. Retrieved2007-11-03.
  7. ^Cardoso, Vitor; Paolo Pani; Mariano Cadoni; Marco Cavaglia (2008). "Ergoregion instability rules out black hole doubles".Phys. Rev. D.77 (12) 124044.arXiv:0709.0532.Bibcode:2008PhRvD..77l4044C.doi:10.1103/PhysRevD.77.124044.S2CID 119119838.
  8. ^Hayward, Sean A. (26 January 2006). "Formation and evaporation of non-singular black holes".Physical Review Letters.96 (3) 031103.arXiv:gr-qc/0506126.Bibcode:2006PhRvL..96c1103H.doi:10.1103/PhysRevLett.96.031103.PMID 16486679.S2CID 15851759.
  9. ^Ayón-Beato, Eloy; García, Alberto (8 June 1998). "Regular Black Hole in General Relativity Coupled to Nonlinear Electrodynamics".Physical Review Letters.80 (23):5056–5059.arXiv:gr-qc/9911046.Bibcode:1998PhRvL..80.5056A.doi:10.1103/PhysRevLett.80.5056.PMID 16486679.S2CID 39766986.
  10. ^Bardeen, JM (1968). "Non-singular general relativistic gravitational collapse".In Proceedings of the International Conference GR5, Tbilisi, USSR.174: 87.Bibcode:1968qtr..conf...87B.
  11. ^Ayón-Beato, Eloy; García, Alberto (9 November 2000). "The Bardeen model as a nonlinear magnetic monopole".Physical Review B.493 (1–2):149–152.arXiv:gr-qc/0009077.Bibcode:2000PhLB..493..149A.doi:10.1016/S0370-2693(00)01125-4.S2CID 55773188.
  12. ^Paula, Marco; Leite, Luiz; Crispino, Luís (12 November 2020). "Electrically charged black holes in linear and nonlinear electrodynamics: Geodesic analysis and scalar absorption".Physical Review D.102 (10) 104033.arXiv:2011.08633.Bibcode:2020PhRvD.102j4033P.doi:10.1103/PhysRevD.102.104033.PMID 16486679.S2CID 226975771.
  13. ^Davies, Paul C.W.; Easson, Damien A.; Levin, Phillip B. (2025). "Nonsingular black holes as dark matter".Physical Review D.111 (10) 103512.arXiv:2410.21577.Bibcode:2025PhRvD.111j3512D.doi:10.1103/PhysRevD.111.103512.

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