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{{Short description|Alternative model for black holes}}
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{{fringe|date=July 2021}}
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The '''magnetospheric eternally collapsing object''' ('''MECO''') is an alternative model for [[black hole]]s initially proposed by Indian scientist Abhas Mitra in 1998<ref name="Mitra1998">{{cite arXiv |first=Abhas |last=Mitra |date=1998 |title=Final state of spherical gravitational collapse and likely sources of Gamma Ray bursts |eprint=astro-ph/9803014 }}</ref><ref name="Mitra 2000 543">{{cite journal |first=Abhas |last=Mitra |date=2000 |title=Non-occurrence of trapped surfaces and black holes in spherical gravitational collapse: An abridged version |journal=[[Foundations of Physics Letters]] |volume=13 |issue=6 |page=543 |doi=10.1023/A:1007810414531 |arxiv=astro-ph/9910408 |s2cid=13945362 }}</ref><ref name="link.springer.com">{{cite journal |title=On the final state of spherical gravitational collapse |journal=Foundations of Physics Letters |volume=15 |issue=5 |pages=439–471 |doi=10.1023/A:1023968113757 |year=2002 |last1=Mitra |first1=Abhas |arxiv=astro-ph/0207056 |bibcode=2002FoPhL..15..439M |s2cid=119363978 }}</ref> and later generalized by American researchers Darryl J. Leiter and Stanley L. Robertson.<ref>{{cite journal |first1=Darryl J. |last1=Leiter |first2=Stanley L. |last2=Robertson |date=2003 |title=Does the principle of equivalence prevent trapped surfaces from being formed in the general relativistic collapse process? |journal=Foundations of Physics Letters |volume=16 |issue=2 |page=143 |doi=10.1023/A:1024170711427 |arxiv=astro-ph/0111421 |s2cid=123650253 }}</ref> A proposed observable difference between MECOs and black holes is that a MECO can produce its own intrinsic [[magnetic field]]. An uncharged black hole cannot produce its own magnetic field, though its [[accretion disc]] can.<ref name="Mitra1998" />
The '''magnetospheric eternally collapsing object''' ('''MECO''') is an alternative model for [[black hole]]s initially proposed by Indian scientist Abhas Mitra in 1998<ref name="Mitra1998">{{cite arXiv |first=Abhas |last=Mitra |date=1998 |title=Final state of spherical gravitational collapse and likely sources of Gamma Ray bursts |eprint=astro-ph/9803014 }}</ref><ref name="Mitra 2000 543">{{cite journal |first=Abhas |last=Mitra |date=2000 |title=Non-occurrence of trapped surfaces and black holes in spherical gravitational collapse: An abridged version |journal=[[Foundations of Physics Letters]] |volume=13 |issue=6 |page=543 |doi=10.1023/A:1007810414531 |arxiv=astro-ph/9910408 |s2cid=13945362 }}</ref><ref name="link.springer.com">{{cite journal |title=On the final state of spherical gravitational collapse |journal=Foundations of Physics Letters |volume=15 |issue=5 |pages=439–471 |doi=10.1023/A:1023968113757 |year=2002 |last1=Mitra |first1=Abhas |arxiv=astro-ph/0207056 |bibcode=2002FoPhL..15..439M |s2cid=119363978 }}</ref> and later generalized by American researchers Darryl J. Leiter and Stanley L. Robertson.<ref>{{cite journal |first1=Darryl J. |last1=Leiter |first2=Stanley L. |last2=Robertson |date=2003 |title=Does the principle of equivalence prevent trapped surfaces from being formed in the general relativistic collapse process? |journal=Foundations of Physics Letters |volume=16 |issue=2 |page=143 |doi=10.1023/A:1024170711427 |arxiv=astro-ph/0111421 |s2cid=123650253 }}</ref> A proposed observable difference between MECOs and black holes is that a MECO can produce its own intrinsic [[magnetic field]]. An uncharged black hole cannot produce its own magnetic field, though its [[accretion disk]] can.<ref name="Mitra1998" />


==Theoretical model==
==Theoretical model==
In the theoretical model a MECO begins to form in much the same way as a [[black hole]], with a large amount of matter collapsing inward toward a single point. However, as it becomes smaller and denser, a MECO does not form an [[event horizon]].<ref name="prd.aps.org">{{cite journal |title=Why gravitational contraction must be accompanied by emission of radiation in both Newtonian and Einstein gravity |journal=Physical Review D |volume=74 |issue=2 |doi=10.1103/PhysRevD.74.024010 |year=2006 |last1=Mitra |first1=Abhas |page=024010 |arxiv=gr-qc/0605066 |bibcode=2006PhRvD..74b4010M |s2cid=119364634 }}</ref><ref name="mnrasl.oxfordjournals.org">{{cite journal |title=A generic relation between baryonic and radiative energy densities of stars |journal=Monthly Notices of the Royal Astronomical Society: Letters |volume=367 |pages=L66–L68 |doi=10.1111/j.1745-3933.2006.00141.x |year=2006 |last1=Mitra |first1=Abhas |issue=1 |arxiv=gr-qc/0601025 |bibcode=2006MNRAS.367L..66M |s2cid=8776989 }}</ref><ref name="mnras.oxfordjournals.org">{{cite journal |title=Radiation pressure supported stars in Einstein gravity: eternally collapsing objects |journal=Monthly Notices of the Royal Astronomical Society |volume=369 |pages=492–496 |doi=10.1111/j.1365-2966.2006.10332.x |year=2006 |last1=Mitra |first1=Abhas |issue=1 |arxiv=gr-qc/0603055 |bibcode=2006MNRAS.369..492M |s2cid=16271230 }}</ref><ref name="sciencedirect.com">{{cite journal |title=Sources of stellar energy, Einstein Eddington timescale of gravitational contraction and eternally collapsing objects |doi=10.1016/j.newast.2006.08.001 |volume=12 |issue=2 |journal=New Astronomy |pages=146–160 |arxiv=astro-ph/0608178 |bibcode=2006NewA...12..146M |date=November 2006 |last1=Mitra |first1=Abhas |last2=Robertson |first2=Stanley L. |citeseerx=10.1.1.256.3740 |s2cid=15066591 }}</ref><ref name="A. Mitra 2010">{{cite journal |title=Likely formation of general relativistic radiation pressure supported stars or 'eternally collapsing objects' |journal=Monthly Notices of the Royal Astronomical Society: Letters |volume=404 |pages=L50–L54 |doi=10.1111/j.1745-3933.2010.00833.x |year=2010 |last1=Mitra |first1=Abhas |last2=Glendenning |first2=Norman K. |issue=1 |arxiv=1003.3518 |bibcode=2010MNRAS.404L..50M |s2cid=119164101 }}</ref>
In the theoretical model a MECO begins to form in much the same way as a [[black hole]], with a large amount of matter collapsing inward toward a single point. However, as it becomes smaller and denser, a MECO does not form an [[event horizon]].<ref name="prd.aps.org">{{cite journal |title=Why gravitational contraction must be accompanied by emission of radiation in both Newtonian and Einstein gravity |journal=Physical Review D |volume=74 |issue=2 |doi=10.1103/PhysRevD.74.024010 |year=2006 |last1=Mitra |first1=Abhas |page=024010 |arxiv=gr-qc/0605066 |bibcode=2006PhRvD..74b4010M |s2cid=119364634 }}</ref><ref name="mnrasl.oxfordjournals.org">{{cite journal |title=A generic relation between baryonic and radiative energy densities of stars |journal=Monthly Notices of the Royal Astronomical Society: Letters |volume=367 |pages=L66–L68 |doi=10.1111/j.1745-3933.2006.00141.x |year=2006 |last1=Mitra |first1=Abhas |issue=1 |doi-access=free |arxiv=gr-qc/0601025 |bibcode=2006MNRAS.367L..66M |s2cid=8776989 }}</ref><ref name="mnras.oxfordjournals.org">{{cite journal |title=Radiation pressure supported stars in Einstein gravity: eternally collapsing objects |journal=Monthly Notices of the Royal Astronomical Society |volume=369 |pages=492–496 |doi=10.1111/j.1365-2966.2006.10332.x |year=2006 |last1=Mitra |first1=Abhas |issue=1 |doi-access=free |arxiv=gr-qc/0603055 |bibcode=2006MNRAS.369..492M |s2cid=16271230 }}</ref><ref name="sciencedirect.com">{{cite journal |title=Sources of stellar energy, Einstein Eddington timescale of gravitational contraction and eternally collapsing objects |doi=10.1016/j.newast.2006.08.001 |volume=12 |issue=2 |journal=New Astronomy |pages=146–160 |arxiv=astro-ph/0608178 |bibcode=2006NewA...12..146M |date=November 2006 |last1=Mitra |first1=Abhas |last2=Robertson |first2=Stanley L. |citeseerx=10.1.1.256.3740 |s2cid=15066591 }}</ref><ref name="A. Mitra 2010">{{cite journal |title=Likely formation of general relativistic radiation pressure supported stars or 'eternally collapsing objects' |journal=Monthly Notices of the Royal Astronomical Society: Letters |volume=404 |pages=L50–L54 |doi=10.1111/j.1745-3933.2010.00833.x |year=2010 |last1=Mitra |first1=Abhas |last2=Glendenning |first2=Norman K. |issue=1 |doi-access=free |arxiv=1003.3518 |bibcode=2010MNRAS.404L..50M |s2cid=119164101 }}</ref>


As the matter becomes denser and hotter, it glows more brightly. Eventually its interior approaches the [[Eddington luminosity|Eddington limit]]. At this point the internal [[radiation pressure]] is sufficient to slow the inward collapse almost to a standstill.<ref name="prd.aps.org" /><ref name="mnrasl.oxfordjournals.org" /><ref name="mnras.oxfordjournals.org" /><ref name="sciencedirect.com" /><ref name="A. Mitra 2010" />
As the matter becomes denser and hotter, it glows more brightly. Eventually its interior approaches the [[Eddington luminosity|Eddington limit]]. At this point the internal [[radiation pressure]] is sufficient to slow the inward collapse almost to a standstill.<ref name="prd.aps.org" /><ref name="mnrasl.oxfordjournals.org" /><ref name="mnras.oxfordjournals.org" /><ref name="sciencedirect.com" /><ref name="A. Mitra 2010" />
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===Eternal collapse===
===Eternal collapse===
Mitra's paper claiming non-occurrence of event horizons and exact black holes later appeared in the Pramana-Journal of Physics. In this paper, Mitra proposes that so-called black holes are eternally collapsing while Schwarzschild black holes have a [[gravitational mass]] M = 0.<ref name="springer.com/journal/12043">{{cite journal |title=Quantum information paradox: Real or fictitious? |journal=Pramana-Journal of Physics|volume=73|issue=3 |pages= 615–622|doi= 10.1007/s12043-009-0113-9 |year=2009 |last1=Mitra |first1=Abhas |arxiv=0911.3518|bibcode=2009Prama..73..615M|s2cid=119117345 }}</ref> He argued that all proposed black holes are instead quasi-black holes rather than exact black holes and that during the gravitational collapse to a black hole, the entire mass energy and angular momentum of the collapsing objects is radiated away before formation of exact mathematical black holes. Mitra proposes that in his formulation since a mathematical zero-mass black hole requires infinite proper time to form, continued gravitational collapse becomes eternal, and the observed black hole candidates must instead be eternally collapsing objects (ECOs). For physical realization of this, he argued that in an extremely relativistic regime, continued collapse must be slowed to a near halt by [[radiation pressure]] at the [[Eddington luminosity|Eddington limit]].<ref name="prd.aps.org" /><ref name="mnrasl.oxfordjournals.org" /><ref name="mnras.oxfordjournals.org" /><ref name="sciencedirect.com" /><ref name="A. Mitra 2010" />
Mitra's paper claiming non-occurrence of event horizons and exact black holes later appeared in ''Pramana - Journal of Physics''. In this paper, Mitra proposes that so-called black holes are eternally collapsing while Schwarzschild black holes have a [[gravitational mass]] M = 0.<ref name="springer.com/journal/12043">{{cite journal |title=Quantum information paradox: Real or fictitious? |journal=Pramana - Journal of Physics|volume=73|issue=3 |pages= 615–622|doi= 10.1007/s12043-009-0113-9 |year=2009 |last1=Mitra |first1=Abhas |arxiv=0911.3518|bibcode=2009Prama..73..615M|s2cid=119117345 }}</ref> He argued that all proposed black holes are instead quasi-black holes rather than exact black holes and that during the gravitational collapse to a black hole, the entire mass energy and angular momentum of the collapsing objects is radiated away before formation of exact mathematical black holes. Mitra proposes that in his formulation since a mathematical zero-mass black hole requires infinite proper time to form, continued gravitational collapse becomes eternal, and the observed black hole candidates must instead be eternally collapsing objects (ECOs). For physical realization of this, he argued that in an extremely relativistic regime, continued collapse must be slowed to a near halt by [[radiation pressure]] at the [[Eddington luminosity|Eddington limit]].<ref name="prd.aps.org" /><ref name="mnrasl.oxfordjournals.org" /><ref name="mnras.oxfordjournals.org" /><ref name="sciencedirect.com" /><ref name="A. Mitra 2010" />


===Magnetic field===
===Magnetic field===
Line 22: Line 25:


==Reception of the MECO model==
==Reception of the MECO model==
Mitra's hypothesis that black holes cannot form is based in part on the argument that in order for a black hole to form, the collapsing matter must travel faster than the speed of light with respect to a fixed observer.<ref name="Mitra 2000 543" /> In 2002; Paulo Crawford and Ismael Tereno cited this as an example of a "wrong and widespread view", and explain that in order for a [[frame of reference]] to be valid, the observer must be moving along a [[timelike]] [[worldline]]. At or inside the [[event horizon]] of a black hole, it is not possible for such an observer to remain fixed; all observers are drawn toward the black hole.<ref name="CrawfordTereno">{{cite journal |first1=Paulo |last1=Crawford |first2=Ismael |last2=Tereno |date=2002 |title=Generalized observers and velocity measurements in General Relativity |journal=[[General Relativity and Gravitation]] |volume=34 |issue=12 |pages=2075–88 |doi=10.1023/A:1021131401034 |arxiv=gr-qc/0111073 |bibcode=2002GReGr..34.2075C |s2cid=2556392 }}</ref> Mitra argues that he has proven that the world-line of an in-falling test particle would tend to be [[lightlike]] at the event horizon, independent of the definition of "velocity".<ref name="link.springer.com" /><ref>{{cite journal |title=The Mass of the Oppenheimer-Snyder Hole: Only Finite Mass Quasi-Black Holes |journal=International Journal of Modern Physics D |volume=22 |issue=9 |pages=1350054 |doi=10.1142/S0218271813500545 |year=2013 |last1=Mitra |first1=Abhas |last2=Singh |first2=K. K. |bibcode=2013IJMPD..2250054M |s2cid=118493061 }}</ref>
Mitra's hypothesis that black holes cannot form is based in part on the argument that in order for a black hole to form, the collapsing matter must travel faster than the speed of light with respect to a fixed observer.<ref name="Mitra 2000 543" /> In 2002, Paulo Crawford and Ismael Tereno cited this as an example of a "wrong and widespread view", and explain that in order for a [[frame of reference]] to be valid, the observer must be moving along a [[timelike]] [[worldline]]. At or inside the [[event horizon]] of a black hole, it is not possible for such an observer to remain fixed; all observers are drawn toward the black hole.<ref name="CrawfordTereno">{{cite journal |first1=Paulo |last1=Crawford |first2=Ismael |last2=Tereno |date=2002 |title=Generalized observers and velocity measurements in General Relativity |journal=[[General Relativity and Gravitation]] |volume=34 |issue=12 |pages=2075–88 |doi=10.1023/A:1021131401034 |arxiv=gr-qc/0111073 |bibcode=2002GReGr..34.2075C |s2cid=2556392 }}</ref> Mitra argues that he has proven that the world-line of an in-falling test particle would tend to be [[lightlike]] at the event horizon, independent of the definition of "velocity".<ref name="link.springer.com" /><ref>{{cite journal |title=The Mass of the Oppenheimer-Snyder Hole: Only Finite Mass Quasi-Black Holes |journal=International Journal of Modern Physics D |volume=22 |issue=9 |pages=1350054 |doi=10.1142/S0218271813500545 |year=2013 |last1=Mitra |first1=Abhas |last2=Singh |first2=K. K. |bibcode=2013IJMPD..2250054M |s2cid=118493061 }}</ref>


==See also==
==See also==
*[[Apparent horizon]]
*[[Apparent horizon]]
*[[Firewall paradox]]
*[[Firewall (physics)|Firewall paradox]]
*[[Planck star]]
*[[Planck star]]
*[[No-hair theorem]]


==References==
==References==

Latest revision as of 09:34, 29 July 2024

The magnetospheric eternally collapsing object (MECO) is an alternative model for black holes initially proposed by Indian scientist Abhas Mitra in 1998[1][2][3] and later generalized by American researchers Darryl J. Leiter and Stanley L. Robertson.[4] A proposed observable difference between MECOs and black holes is that a MECO can produce its own intrinsic magnetic field. An uncharged black hole cannot produce its own magnetic field, though its accretion disk can.[1]

Theoretical model

[edit]

In the theoretical model a MECO begins to form in much the same way as a black hole, with a large amount of matter collapsing inward toward a single point. However, as it becomes smaller and denser, a MECO does not form an event horizon.[5][6][7][8][9]

As the matter becomes denser and hotter, it glows more brightly. Eventually its interior approaches the Eddington limit. At this point the internal radiation pressure is sufficient to slow the inward collapse almost to a standstill.[5][6][7][8][9]

In fact, the collapse gets slower and slower, so a singularity could only form in an infinite future. Unlike a black hole, the MECO never fully collapses. Rather, according to the model it slows down and enters an eternal collapse.[5][6][7][8][9]

Mitra provides a review of the evolution of black hole alternatives including his model of eternal collapse and MECOs.[10]

Eternal collapse

[edit]

Mitra's paper claiming non-occurrence of event horizons and exact black holes later appeared in Pramana - Journal of Physics. In this paper, Mitra proposes that so-called black holes are eternally collapsing while Schwarzschild black holes have a gravitational mass M = 0.[11] He argued that all proposed black holes are instead quasi-black holes rather than exact black holes and that during the gravitational collapse to a black hole, the entire mass energy and angular momentum of the collapsing objects is radiated away before formation of exact mathematical black holes. Mitra proposes that in his formulation since a mathematical zero-mass black hole requires infinite proper time to form, continued gravitational collapse becomes eternal, and the observed black hole candidates must instead be eternally collapsing objects (ECOs). For physical realization of this, he argued that in an extremely relativistic regime, continued collapse must be slowed to a near halt by radiation pressure at the Eddington limit.[5][6][7][8][9]

Magnetic field

[edit]

A MECO can carry electric and magnetic properties, has a finite size, can carry angular momentum and rotate.[citation needed]

Observational evidence

[edit]

Astronomer Rudolph Schild of the HarvardSmithsonian Center for Astrophysics claimed in 2006 to have found evidence consistent with an intrinsic magnetic field from the black hole candidate in the quasar Q0957+561.[12][13] Chris Reynolds of the University of Maryland has criticised the MECO interpretation, suggesting instead that the apparent hole in the disc could be filled with very hot, tenuous gas, which would not radiate much and would be hard to see; however, Leiter in turn questions the viability of Reynolds's interpretation.[12]

Reception of the MECO model

[edit]

Mitra's hypothesis that black holes cannot form is based in part on the argument that in order for a black hole to form, the collapsing matter must travel faster than the speed of light with respect to a fixed observer.[2] In 2002, Paulo Crawford and Ismael Tereno cited this as an example of a "wrong and widespread view", and explain that in order for a frame of reference to be valid, the observer must be moving along a timelike worldline. At or inside the event horizon of a black hole, it is not possible for such an observer to remain fixed; all observers are drawn toward the black hole.[14] Mitra argues that he has proven that the world-line of an in-falling test particle would tend to be lightlike at the event horizon, independent of the definition of "velocity".[3][15]

See also

[edit]

References

[edit]
  1. ^ a b Mitra, Abhas (1998). "Final state of spherical gravitational collapse and likely sources of Gamma Ray bursts". arXiv:astro-ph/9803014.
  2. ^ a b Mitra, Abhas (2000). "Non-occurrence of trapped surfaces and black holes in spherical gravitational collapse: An abridged version". Foundations of Physics Letters. 13 (6): 543. arXiv:astro-ph/9910408. doi:10.1023/A:1007810414531. S2CID 13945362.
  3. ^ a b Mitra, Abhas (2002). "On the final state of spherical gravitational collapse". Foundations of Physics Letters. 15 (5): 439–471. arXiv:astro-ph/0207056. Bibcode:2002FoPhL..15..439M. doi:10.1023/A:1023968113757. S2CID 119363978.
  4. ^ Leiter, Darryl J.; Robertson, Stanley L. (2003). "Does the principle of equivalence prevent trapped surfaces from being formed in the general relativistic collapse process?". Foundations of Physics Letters. 16 (2): 143. arXiv:astro-ph/0111421. doi:10.1023/A:1024170711427. S2CID 123650253.
  5. ^ a b c d Mitra, Abhas (2006). "Why gravitational contraction must be accompanied by emission of radiation in both Newtonian and Einstein gravity". Physical Review D. 74 (2): 024010. arXiv:gr-qc/0605066. Bibcode:2006PhRvD..74b4010M. doi:10.1103/PhysRevD.74.024010. S2CID 119364634.
  6. ^ a b c d Mitra, Abhas (2006). "A generic relation between baryonic and radiative energy densities of stars". Monthly Notices of the Royal Astronomical Society: Letters. 367 (1): L66–L68. arXiv:gr-qc/0601025. Bibcode:2006MNRAS.367L..66M. doi:10.1111/j.1745-3933.2006.00141.x. S2CID 8776989.
  7. ^ a b c d Mitra, Abhas (2006). "Radiation pressure supported stars in Einstein gravity: eternally collapsing objects". Monthly Notices of the Royal Astronomical Society. 369 (1): 492–496. arXiv:gr-qc/0603055. Bibcode:2006MNRAS.369..492M. doi:10.1111/j.1365-2966.2006.10332.x. S2CID 16271230.
  8. ^ a b c d Mitra, Abhas; Robertson, Stanley L. (November 2006). "Sources of stellar energy, Einstein Eddington timescale of gravitational contraction and eternally collapsing objects". New Astronomy. 12 (2): 146–160. arXiv:astro-ph/0608178. Bibcode:2006NewA...12..146M. CiteSeerX 10.1.1.256.3740. doi:10.1016/j.newast.2006.08.001. S2CID 15066591.
  9. ^ a b c d Mitra, Abhas; Glendenning, Norman K. (2010). "Likely formation of general relativistic radiation pressure supported stars or 'eternally collapsing objects'". Monthly Notices of the Royal Astronomical Society: Letters. 404 (1): L50–L54. arXiv:1003.3518. Bibcode:2010MNRAS.404L..50M. doi:10.1111/j.1745-3933.2010.00833.x. S2CID 119164101.
  10. ^ Mitra, Abhas (2021). The Rise and Fall of the Black Hole Paradigm. Pan Macmillan Publishing India Pvt. Ltd. ISBN 978-9389104141.
  11. ^ Mitra, Abhas (2009). "Quantum information paradox: Real or fictitious?". Pramana - Journal of Physics. 73 (3): 615–622. arXiv:0911.3518. Bibcode:2009Prama..73..615M. doi:10.1007/s12043-009-0113-9. S2CID 119117345.
  12. ^ a b Shiga, David (2006). "Mysterious quasar casts doubt on black holes". New Scientist. Retrieved 2 December 2014.
  13. ^ Schild, Rudolph E.; Leiter, Darryl J.; Robertson, Stanley L. (2006). "Observations supporting the existence of an intrinsic magnetic moment inside the central compact object within the Quasar Q0957+561". Astronomical Journal. 132 (1): 420–32. arXiv:astro-ph/0505518. Bibcode:2006AJ....132..420S. doi:10.1086/504898. S2CID 119355221.
  14. ^ Crawford, Paulo; Tereno, Ismael (2002). "Generalized observers and velocity measurements in General Relativity". General Relativity and Gravitation. 34 (12): 2075–88. arXiv:gr-qc/0111073. Bibcode:2002GReGr..34.2075C. doi:10.1023/A:1021131401034. S2CID 2556392.
  15. ^ Mitra, Abhas; Singh, K. K. (2013). "The Mass of the Oppenheimer-Snyder Hole: Only Finite Mass Quasi-Black Holes". International Journal of Modern Physics D. 22 (9): 1350054. Bibcode:2013IJMPD..2250054M. doi:10.1142/S0218271813500545. S2CID 118493061.