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'''Higher-dimensional Einstein gravity''' is any of various physical theories that attempt to generalize to higher dimensions various results of the standard (four-dimensional) [[Albert Einstein]]'s gravitational theory, that is, [[general relativity]]. This attempt at generalization has been strongly influenced in recent decades by [[string theory]]. These extensions of general relativity are central to many modern theories of fundamental physics, including string theory, [[M-theory]], and [[Brane cosmology|brane world]] scenarios. These models are used to explore theoretical aspects of gravity and spacetime in contexts beyond four-dimensional physics, and provide novel solutions to Einstein's equations, such as higher-dimensional [[Black hole|black holes]] and black rings.


'''Higher-dimensional Einstein gravity''' is any of various physical theories that attempt to generalise to higher dimensions various results of the well established theory of standard (four-dimensional) [[Albert Einstein]]'s gravitational theory, that is, [[general relativity]]. This attempt at generalisation has been strongly influenced in recent decades by [[string theory]].
At present, these theories remain largely theoretical and lack direct observational or experimental support. Currently, it has no ''direct'' observational and experimental support, in contrast to four-dimensional general relativity. However, this theoretical work has led to the possibility of proving the existence of extra dimensions.<ref>{{cite arXiv | eprint=hep-th/0211290 | last1=Reall | first1=Harvey S. | title=Higher dimensional black holes and supersymmetry | date=2002 }}</ref> This is demonstrated by the proof of Harvey Reall and Roberto Emparan that there is a 'black ring' solution in 5 dimensions.<ref>{{Cite journal |last1=Emparan |first1=Roberto |last2=Reall |first2=Harvey S. |date=2002-02-21 |title=A Rotating Black Ring Solution in Five Dimensions |url=https://link.aps.org/doi/10.1103/PhysRevLett.88.101101 |journal=Physical Review Letters |volume=88 |issue=10 |pages=101101 |doi=10.1103/PhysRevLett.88.101101|pmid=11909335 |bibcode=2002PhRvL..88j1101E |arxiv=hep-th/0110260 }}</ref> If such a 'black ring' could be produced in a particle accelerator such as the [[Large Hadron Collider]], this could potentially provide evidence supporting the existence of extra dimensions.<ref>{{Cite journal |last1=Emparan |first1=Roberto |last2=Reall |first2=Harvey S. |date=2002-02-21 |title=A Rotating Black Ring Solution in Five Dimensions |url=https://link.aps.org/doi/10.1103/PhysRevLett.88.101101 |journal=Physical Review Letters |volume=88 |issue=10 |pages=101101 |doi=10.1103/PhysRevLett.88.101101|pmid=11909335 |bibcode=2002PhRvL..88j1101E |arxiv=hep-th/0110260 }}</ref>


At present, this work can probably be most fairly described as extended theoretical speculation. Currently, it has no ''direct'' observational and experimental support, in contrast to four-dimensional general relativity. However, this theoretical work has led to the possibility of proving the existence of extra dimensions. This is best demonstrated by the proof of [[Harvey Reall]] and [[Roberto Emparan]] that there is a 'black ring' solution in 5 dimensions. If such a 'black ring' could be produced in a particle accelerator such as the [[Large Hadron Collider]], this would provide the evidence that higher dimensions exist.
== Historical background ==
The first attempts to introduce extra dimensions date back to the 1920s with the work of [[Theodor Kaluza]] and [[Oskar Klein]], who developed a five-dimensional theory to unify gravity and electromagnetism, now known as [[Kaluza–Klein theory]]. This approach introduced the idea that extra dimensions could be compactified, or curled up to unobservable sizes.
 
Interest in higher-dimensional theories re-emerged in the 1970s and 1980s with the development of [[supergravity]]<ref>{{cite arXiv | eprint=hep-th/9802138 | last1=Tanii | first1=Y. | title=Introduction to Supergravities in Diverse Dimensions | date=1998 }}</ref> and string theory. [[Superstring theory]] requires ten spacetime dimensions for mathematical consistency, while M-theory, a proposed unification of all string theories, is formulated in eleven dimensions.<ref>{{cite arXiv | eprint=1104.2051 | last1=Taylor | first1=Washington | title=TASI Lectures on Supergravity and String Vacua in Various Dimensions | date=2011 | class=hep-th }}</ref>
 
== Theoretical framework ==
In higher-dimensional gravity, the [[Einstein field equations]] are extended to account for additional spacetime dimensions. These generalizations allow for the analysis of more varied geometric structures and physical scenarios.<ref>{{cite journal | arxiv=2405.03698 | doi=10.1140/epjc/s10052-017-5452-y | title=Generalization of Einstein's gravitational field equations | date=2017 | last1=Moulin | first1=Frédéric | journal=The European Physical Journal C | volume=77 | issue=12 | page=878 | bibcode=2017EPJC...77..878M }}</ref> While the core ideas remain rooted in the curvature of spacetime and its relation to matter and energy, higher dimensions allow for a broader variety of solutions and physical implications.
 
Theoretical models in higher-dimensional gravity often incorporate compactified or warped extra dimensions, and can include corrections to the classical [[Einstein–Hilbert action]]. A notable extension is [[Lovelock theory of gravity|Lovelock gravity]], which modifies the action by introducing higher-order curvature terms while still yielding second-order field equations.<ref>{{cite journal | arxiv=1302.2151 | doi=10.1016/j.physrep.2013.05.007 | title=Lanczos–Lovelock models of gravity | date=2013 | last1=Padmanabhan | first1=T. | last2=Kothawala | first2=D. | journal=Physics Reports | volume=531 | issue=3 | pages=115–171 | bibcode=2013PhR...531..115P }}</ref> These modifications are introduced because in dimensions greater than four, the Einstein–Hilbert action is not the most general theory that leads to second-order equations of motion, which are important for physical consistency and stability.
 
One especially significant case is [[Gauss–Bonnet gravity]], which includes quadratic curvature corrections and becomes dynamically non-trivial in dimensions five and higher.<ref>{{Cite journal |last1=Brassel |first1=Byron P. |last2=Maharaj |first2=Sunil D. |last3=Goswami |first3=Rituparno |date=2019-07-01 |title=Higher-dimensional radiating black holes in Einstein-Gauss-Bonnet gravity |url=https://link.aps.org/doi/10.1103/PhysRevD.100.024001 |journal=Physical Review D |volume=100 |issue=2 |pages=024001 |doi=10.1103/PhysRevD.100.024001|bibcode=2019PhRvD.100b4001B |url-access=subscription }}</ref> These theories are studied in the context of problems in  [[Particle physics|high-energy physics]], such as the nature of singularities, the behavior of black holes in higher dimensions, and the unification of gravity with quantum field theory.


==Exact solutions==
==Exact solutions==
{{jargon|date=February 2024}}
The higher-dimensional generalization of the [[Kerr metric]] was discovered by [[Robert Myers (physicist)|Robert Myers]] and [[Malcolm Perry (physicist)|Malcolm Perry]].<ref>{{cite journal |author=Robert C. Myers, M.J. Perry |year=1986 |title=Black Holes in Higher Dimensional Space-Times |journal=Annals of Physics |volume=172 |issue=2 |pages=304–347 |bibcode=1986AnPhy.172..304M |doi=10.1016/0003-4916(86)90186-7}}</ref> Like the Kerr metric, the Myers–Perry metric has spherical horizon topology. The construction involves making a [[Kerr–Schild spacetime|Kerr–Schild]] [[ansatz]]; by a similar method, the solution has been generalized to include a [[cosmological constant]]. The '''black ring''' is a solution of five-dimensional general relativity. It inherits its name from the fact that its event horizon is topologically S<sup>1</sup> × S<sup>2</sup>. This is unlike other known black hole solutions in five dimensions, which typically have horizon topology S<sup>3</sup>.
The higher-dimensional generalization of the [[Kerr metric]] was discovered by [[Robert Myers (physicist)|Robert Myers]] and [[Malcolm Perry (physicist)|Malcolm Perry]].<ref>
{{cite journal
| title = Black Holes in Higher Dimensional Space-Times
| author = Robert C. Myers, M.J. Perry
| journal = Annals of Physics  
| volume = 172
| pages = 304–347
| year = 1986
| issue = 2
| doi = 10.1016/0003-4916(86)90186-7
|bibcode = 1986AnPhy.172..304M }}</ref> Like the Kerr metric, the Myers–Perry metric has spherical horizon topology. The construction involves making a [[Kerr–Schild spacetime|Kerr–Schild]] [[ansatz]]; by a similar method, the solution has been generalized to include a [[cosmological constant]]. The '''black ring''' is a solution of five-dimensional general relativity. It inherits its name from the fact that its event horizon is topologically S<sup>1</sup> × S<sup>2</sup>. This is in contrast to other known black hole solutions in five dimensions which have horizon topology S<sup>3</sup>.


In 2014, Hari Kunduri and James Lucietti proved the existence of a black hole with [[Lens space]] topology of the ''L''(2, 1) type in five dimensions,<ref>{{Cite journal |last1=Kunduri |first1=Hari K. |last2=Lucietti |first2=James |date=2014-11-17 |title=Supersymmetric Black Holes with Lens-Space Topology |journal=Physical Review Letters |volume=113 |issue=21 |pages=211101 |arxiv=1408.6083 |doi=10.1103/PhysRevLett.113.211101|pmid=25479484 |bibcode=2014PhRvL.113u1101K |s2cid=119060757 }}</ref> this was next extended to all ''L''(p, 1) with positive integers p by Shinya Tomizawa and Masato Nozawa in 2016<ref>{{Cite journal |last1=Tomizawa |first1=Shinya |last2=Nozawa |first2=Masato |date=2016-08-22 |title=Supersymmetric black lenses in five dimensions |journal=Physical Review D |volume=94 |issue=4 |pages=044037 |arxiv=1606.06643 |doi=10.1103/PhysRevD.94.044037|bibcode=2016PhRvD..94d4037T |s2cid=118524018 }}</ref> and finally in a preprint to all ''L''(p, q) and any dimension by Marcus Khuri and Jordan Rainone in 2022,<ref>{{Cite journal|last1=Khuri |first1=Marcus A. |last2=Rainone |first2=Jordan F. |date=2023 |title=Black Lenses in Kaluza-Klein Matter |journal=Physical Review Letters |volume=131 |issue=4 |page=041402 |doi=10.1103/PhysRevLett.131.041402 |pmid=37566867 |arxiv=2212.06762|bibcode=2023PhRvL.131d1402K |s2cid=254591339 }}</ref><ref>{{Cite web |last=Nadis |first=Steve |date=2023-01-24 |title=Mathematicians Find an Infinity of Possible Black Hole Shapes |url=https://www.quantamagazine.org/mathematicians-find-an-infinity-of-possible-black-hole-shapes-20230124/ |access-date=2023-01-24 |website=Quanta Magazine |language=en}}</ref> a '''black lens''' doesn't necessarily need to rotate as a black ring but all examples so far need a matter field coming from the extra dimensions to remain stable.
In 2014, Hari Kunduri and James Lucietti proved the existence of a black hole with [[Lens space]] topology of the ''L''(2, 1) type in five dimensions,<ref>{{Cite journal |last1=Kunduri |first1=Hari K. |last2=Lucietti |first2=James |date=2014-11-17 |title=Supersymmetric Black Holes with Lens-Space Topology |journal=Physical Review Letters |volume=113 |issue=21 |pages=211101 |arxiv=1408.6083 |bibcode=2014PhRvL.113u1101K |doi=10.1103/PhysRevLett.113.211101 |pmid=25479484 |s2cid=119060757}}</ref> this was next extended to all ''L''(p, 1) with positive integers p by Shinya Tomizawa and Masato Nozawa in 2016<ref>{{Cite journal |last1=Tomizawa |first1=Shinya |last2=Nozawa |first2=Masato |date=2016-08-22 |title=Supersymmetric black lenses in five dimensions |journal=Physical Review D |volume=94 |issue=4 |pages=044037 |arxiv=1606.06643 |bibcode=2016PhRvD..94d4037T |doi=10.1103/PhysRevD.94.044037 |s2cid=118524018}}</ref> and finally in a preprint to all ''L''(p, q) and any dimension by Marcus Khuri and Jordan Rainone in 2022,<ref>{{Cite journal |last1=Khuri |first1=Marcus A. |last2=Rainone |first2=Jordan F. |date=2023 |title=Black Lenses in Kaluza-Klein Matter |journal=Physical Review Letters |volume=131 |issue=4 |page=041402 |arxiv=2212.06762 |bibcode=2023PhRvL.131d1402K |doi=10.1103/PhysRevLett.131.041402 |pmid=37566867 |s2cid=254591339}}</ref><ref>{{Cite web |last=Nadis |first=Steve |date=2023-01-24 |title=Mathematicians Find an Infinity of Possible Black Hole Shapes |url=https://www.quantamagazine.org/mathematicians-find-an-infinity-of-possible-black-hole-shapes-20230124/ |access-date=2023-01-24 |website=Quanta Magazine |language=en}}</ref> a '''black lens''' doesn't necessarily need to rotate as a black ring, although known examples require a matter field sourced from the extra dimensions for stability.


==Black hole uniqueness==
==Black hole uniqueness==
In four dimensions, [[Stephen Hawking|Hawking]] proved that the topology of the [[event horizon]] of a non-rotating [[black hole]] must be spherical.<ref>{{Cite journal |last=Hawking |first=S. W. |date=1972 |title=Black holes in general relativity |url=https://projecteuclid.org/journals/communications-in-mathematical-physics/volume-25/issue-2/Black-holes-in-general-relativity/cmp/1103857884.full |journal=Communications in Mathematical Physics |volume=25 |issue=2 |pages=152–166 |doi=10.1007/BF01877517 |bibcode=1972CMaPh..25..152H |s2cid=121527613 |issn=0010-3616}}</ref> Because the proof uses the [[Gauss–Bonnet theorem]], it does not generalize to higher dimensions. The discovery of black ring solutions in five dimensions<ref>{{cite journal
In four dimensions, [[Stephen Hawking|Hawking]] proved that the topology of the [[event horizon]] of a non-rotating [[black hole]] must be spherical.<ref>{{Cite journal |last=Hawking |first=S. W. |date=1972 |title=Black holes in general relativity |url=https://projecteuclid.org/journals/communications-in-mathematical-physics/volume-25/issue-2/Black-holes-in-general-relativity/cmp/1103857884.full |journal=Communications in Mathematical Physics |volume=25 |issue=2 |pages=152–166 |bibcode=1972CMaPh..25..152H |doi=10.1007/BF01877517 |issn=0010-3616 |s2cid=121527613}}</ref> Because the proof uses the [[Gauss–Bonnet theorem]], it does not generalize to higher dimensions. The discovery of black ring solutions in five dimensions<ref>{{cite journal |last1=Emparan |first1=Roberto |last2=Reall |first2=Harvey S. |date=21 February 2002 |title=A Rotating Black Ring Solution in Five Dimensions |journal=Phys. Rev. Lett. |volume=88 |issue=10 |pages=101101–101104 |arxiv=hep-th/0110260 |bibcode=2002PhRvL..88j1101E |doi=10.1103/PhysRevLett.88.101101 |pmid=11909335 |s2cid=6923777 |hdl-access=free |hdl=2445/13248}}</ref> shows that other topologies are allowed in higher dimensions, but it is unclear precisely which topologies are allowed. It has been shown that the horizon must be of positive Yamabe type, meaning that it must admit a metric of positive [[scalar curvature]].<ref>{{Cite journal |last1=Galloway |first1=Gregory J. |last2=Schoen |first2=Richard |date=2006-09-01 |title=A Generalization of Hawking's Black Hole Topology Theorem to Higher Dimensions |journal=Communications in Mathematical Physics |language=en |volume=266 |issue=2 |pages=571–576 |arxiv=gr-qc/0509107 |bibcode=2006CMaPh.266..571G |doi=10.1007/s00220-006-0019-z |issn=1432-0916 |s2cid=5439828}}</ref>
| last1=Emparan | first1=Roberto  
 
| last2=Reall | first2=Harvey S.
== Applications in string theory and quantum gravity ==
| title = A Rotating Black Ring Solution in Five Dimensions
Higher-dimensional gravity appears in string theory and M-theory as a central element for mathematical consistency, where extra dimensions are essential for mathematical consistency. In these frameworks, gravity is inherently higher-dimensional, while standard model forces are often confined to lower-dimensional [[Hypersurface|hypersurfaces]] known as [[Brane|branes]].
| journal = Phys. Rev. Lett.
 
| volume = 88 | issue= 10
Compactification mechanisms, such as [[Calabi–Yau manifold|Calabi–Yau manifolds]] in string theory, reduce the apparent number of dimensions to four at observable scales.<ref>{{Cite journal |last1=Lin |first1=Jieming |last2=Skrzypek |first2=Torben |last3=Stelle |first3=K. S. |date=2025-03-27 |title=Compactification on Calabi-Yau threefolds: consistent truncation to pure supergravity |url=https://doi.org/10.1007/JHEP03(2025)200 |journal=Journal of High Energy Physics |language=en |volume=2025 |issue=3 |pages=200 |doi=10.1007/JHEP03(2025)200 |arxiv=2412.00186 |bibcode=2025JHEP...03..200L |issn=1029-8479}}</ref> The geometry and topology of the compactified dimensions may influence the properties of particles and interactions in the effective four-dimensional theory.
| pages = 101101–101104
 
| date = 21 February 2002
Higher-dimensional solutions are also important in the context of the [[AdS/CFT correspondence]], a conjectured duality between gravity in [[anti-de Sitter space]] and a [[conformal field theory]] on its boundary.<ref>{{Cite journal |last1=Cano |first1=Pablo A. |last2=David |first2=Marina |date=2024-03-06 |title=Near-horizon geometries and black hole thermodynamics in higher-derivative AdS5 supergravity |url=https://doi.org/10.1007/JHEP03(2024)036 |journal=Journal of High Energy Physics |language=en |volume=2024 |issue=3 |pages=36 |doi=10.1007/JHEP03(2024)036 |issn=1029-8479|doi-access=free }}</ref> In this context, black hole solutions in higher dimensions correspond to thermal states<ref>{{Cite journal |last1=Ezroura |first1=Nizar |last2=Larsen |first2=Finn |date=2024-12-03 |title=Supergravity spectrum of AdS5 black holes |url=https://doi.org/10.1007/JHEP12(2024)020 |journal=Journal of High Energy Physics |language=en |volume=2024 |issue=12 |pages=20 |doi=10.1007/JHEP12(2024)020 |issn=1029-8479|doi-access=free }}</ref> in the dual [[quantum field theory]] and have been applied to study strongly coupled systems in [[Condensed matter physics|condensed matter]] and [[nuclear physics]].
| doi = 10.1103/PhysRevLett.88.101101| pmid=11909335  
| arxiv=hep-th/0110260
| bibcode=2002PhRvL..88j1101E
| hdl=2445/13248  
| s2cid=6923777
| hdl-access=free}}</ref> shows that other topologies are allowed in higher dimensions, but it is unclear precisely which topologies are allowed. It has been shown that the horizon must be of positive Yamabe type, meaning that it must admit a metric of positive [[scalar curvature]].<ref>{{Cite journal |last1=Galloway |first1=Gregory J. |last2=Schoen |first2=Richard |date=2006-09-01 |title=A Generalization of Hawking's Black Hole Topology Theorem to Higher Dimensions |journal=Communications in Mathematical Physics |language=en |volume=266 |issue=2 |pages=571–576 |arxiv=gr-qc/0509107 |doi=10.1007/s00220-006-0019-z |bibcode=2006CMaPh.266..571G |s2cid=5439828 |issn=1432-0916}}</ref>


==See also==
==See also==

Latest revision as of 03:37, 30 June 2025

Higher-dimensional Einstein gravity is any of various physical theories that attempt to generalize to higher dimensions various results of the standard (four-dimensional) Albert Einstein's gravitational theory, that is, general relativity. This attempt at generalization has been strongly influenced in recent decades by string theory. These extensions of general relativity are central to many modern theories of fundamental physics, including string theory, M-theory, and brane world scenarios. These models are used to explore theoretical aspects of gravity and spacetime in contexts beyond four-dimensional physics, and provide novel solutions to Einstein's equations, such as higher-dimensional black holes and black rings.

At present, these theories remain largely theoretical and lack direct observational or experimental support. Currently, it has no direct observational and experimental support, in contrast to four-dimensional general relativity. However, this theoretical work has led to the possibility of proving the existence of extra dimensions.[1] This is demonstrated by the proof of Harvey Reall and Roberto Emparan that there is a 'black ring' solution in 5 dimensions.[2] If such a 'black ring' could be produced in a particle accelerator such as the Large Hadron Collider, this could potentially provide evidence supporting the existence of extra dimensions.[3]

Historical background

The first attempts to introduce extra dimensions date back to the 1920s with the work of Theodor Kaluza and Oskar Klein, who developed a five-dimensional theory to unify gravity and electromagnetism, now known as Kaluza–Klein theory. This approach introduced the idea that extra dimensions could be compactified, or curled up to unobservable sizes.

Interest in higher-dimensional theories re-emerged in the 1970s and 1980s with the development of supergravity[4] and string theory. Superstring theory requires ten spacetime dimensions for mathematical consistency, while M-theory, a proposed unification of all string theories, is formulated in eleven dimensions.[5]

Theoretical framework

In higher-dimensional gravity, the Einstein field equations are extended to account for additional spacetime dimensions. These generalizations allow for the analysis of more varied geometric structures and physical scenarios.[6] While the core ideas remain rooted in the curvature of spacetime and its relation to matter and energy, higher dimensions allow for a broader variety of solutions and physical implications.

Theoretical models in higher-dimensional gravity often incorporate compactified or warped extra dimensions, and can include corrections to the classical Einstein–Hilbert action. A notable extension is Lovelock gravity, which modifies the action by introducing higher-order curvature terms while still yielding second-order field equations.[7] These modifications are introduced because in dimensions greater than four, the Einstein–Hilbert action is not the most general theory that leads to second-order equations of motion, which are important for physical consistency and stability.

One especially significant case is Gauss–Bonnet gravity, which includes quadratic curvature corrections and becomes dynamically non-trivial in dimensions five and higher.[8] These theories are studied in the context of problems in high-energy physics, such as the nature of singularities, the behavior of black holes in higher dimensions, and the unification of gravity with quantum field theory.

Exact solutions

The higher-dimensional generalization of the Kerr metric was discovered by Robert Myers and Malcolm Perry.[9] Like the Kerr metric, the Myers–Perry metric has spherical horizon topology. The construction involves making a Kerr–Schild ansatz; by a similar method, the solution has been generalized to include a cosmological constant. The black ring is a solution of five-dimensional general relativity. It inherits its name from the fact that its event horizon is topologically S1 × S2. This is unlike other known black hole solutions in five dimensions, which typically have horizon topology S3.

In 2014, Hari Kunduri and James Lucietti proved the existence of a black hole with Lens space topology of the L(2, 1) type in five dimensions,[10] this was next extended to all L(p, 1) with positive integers p by Shinya Tomizawa and Masato Nozawa in 2016[11] and finally in a preprint to all L(p, q) and any dimension by Marcus Khuri and Jordan Rainone in 2022,[12][13] a black lens doesn't necessarily need to rotate as a black ring, although known examples require a matter field sourced from the extra dimensions for stability.

Black hole uniqueness

In four dimensions, Hawking proved that the topology of the event horizon of a non-rotating black hole must be spherical.[14] Because the proof uses the Gauss–Bonnet theorem, it does not generalize to higher dimensions. The discovery of black ring solutions in five dimensions[15] shows that other topologies are allowed in higher dimensions, but it is unclear precisely which topologies are allowed. It has been shown that the horizon must be of positive Yamabe type, meaning that it must admit a metric of positive scalar curvature.[16]

Applications in string theory and quantum gravity

Higher-dimensional gravity appears in string theory and M-theory as a central element for mathematical consistency, where extra dimensions are essential for mathematical consistency. In these frameworks, gravity is inherently higher-dimensional, while standard model forces are often confined to lower-dimensional hypersurfaces known as branes.

Compactification mechanisms, such as Calabi–Yau manifolds in string theory, reduce the apparent number of dimensions to four at observable scales.[17] The geometry and topology of the compactified dimensions may influence the properties of particles and interactions in the effective four-dimensional theory.

Higher-dimensional solutions are also important in the context of the AdS/CFT correspondence, a conjectured duality between gravity in anti-de Sitter space and a conformal field theory on its boundary.[18] In this context, black hole solutions in higher dimensions correspond to thermal states[19] in the dual quantum field theory and have been applied to study strongly coupled systems in condensed matter and nuclear physics.

See also

References

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