Gary Gibbons

Last updated

Gary Gibbons
FRS
GaryGibbons.JPG
Gary Gibbons at Harvard University, c.2005
Born
Gary William Gibbons

(1946-07-01) 1 July 1946 (age 78) [1]
Coulsdon, London, England
Education Purley County Grammar School
Alma mater University of Cambridge (BA, PhD)
Known for
Awards
Scientific career
Fields
Institutions
Thesis Some aspects of gravitational radiation and gravitational collapse  (1973)
Doctoral advisor
Doctoral students Chris Hull [4] [5]
Website damtp.cam.ac.uk/people/g.w.gibbons

Gary William Gibbons (born 1 July 1946) [1] is a British theoretical physicist. [6] [7]

Contents

Education

Gibbons was born in Coulsdon, Surrey. He was educated at Purley County Grammar School [1] and the University of Cambridge, where in 1969 he became a research student under the supervision of Dennis Sciama. When Sciama moved to the University of Oxford, he became a student of Stephen Hawking, obtaining his PhD from Cambridge in 1973. [2]

Career and research

Apart from a stay at the Max Planck Institute in Munich in the 1970s he has remained in Cambridge throughout his career, becoming a full professor in 1997, a Fellow of the Royal Society in 1999, [3] and a Fellow of Trinity College, Cambridge in 2002.

Having worked on classical general relativity for his PhD thesis, Gibbons focused on the quantum theory of black holes afterwards. Together with Malcolm Perry, he used thermal Green's functions to prove the universality of thermodynamic properties of horizons, including cosmological event horizons. [8] He developed the Euclidean approach to quantum gravity with Stephen Hawking, which allows a derivation of the thermodynamics of black holes from a functional integral approach. [9] As the Euclidean action for gravity is not positive definite, the integral only converges when a particular contour is used for conformal factors. [10]

His work in more recent years includes contributions to research on supergravity, p-branes [11] and M-theory, mainly motivated by string theory. Gibbons remains interested in geometrical problems of all sorts which have applications to physics.

Awards and honours

Gibbons was elected a Fellow of the Royal Society (FRS) in 1999. His nomination reads

Distinguished for his contributions to General Relativity and the Quantum Theory of Gravity. He played a leading role in the development of the Euclidean approach to quantum gravity and showed how it could be used to understand the thermal character of black holes and inflating universes. This revealed a deep and unexpected relationship between gravitation and thermodynamics. As part of the Euclidean quantum gravity programme, he discovered many of the known gravitational instantons and classified their properties. In the more conventional Lorentzian approach to gravity, he has studied the behaviour of solitons in gauge theories and General Relativity and has shown how supersymmetry leads to Bogomolny inequalities on the masses and charges. More recently he has been investigating the role of topology in gravity and has obtained important restrictions on how the topology of spacetime can change. He is recognised world wide as a leader in the field. [3]

Related Research Articles

<span class="mw-page-title-main">General relativity</span> Theory of gravitation as curved spacetime

General relativity, also known as the general theory of relativity, and as Einstein's theory of gravity, is the geometric theory of gravitation published by Albert Einstein in 1915 and is the current description of gravitation in modern physics. General relativity generalizes special relativity and refines Newton's law of universal gravitation, providing a unified description of gravity as a geometric property of space and time, or four-dimensional spacetime. In particular, the curvature of spacetime is directly related to the energy and momentum of whatever present matter and radiation. The relation is specified by the Einstein field equations, a system of second-order partial differential equations.

The holographic principle is a property of string theories and a supposed property of quantum gravity that states that the description of a volume of space can be thought of as encoded on a lower-dimensional boundary to the region – such as a light-like boundary like a gravitational horizon. First proposed by Gerard 't Hooft, it was given a precise string theoretic interpretation by Leonard Susskind, who combined his ideas with previous ones of 't Hooft and Charles Thorn. Susskind said, "The three-dimensional world of ordinary experience—the universe filled with galaxies, stars, planets, houses, boulders, and people—is a hologram, an image of reality coded on a distant two-dimensional surface." As pointed out by Raphael Bousso, Thorn observed in 1978, that string theory admits a lower-dimensional description in which gravity emerges from it in what would now be called a holographic way. The prime example of holography is the AdS/CFT correspondence.

<span class="mw-page-title-main">Quantum gravity</span> Description of gravity using discrete values

Quantum gravity (QG) is a field of theoretical physics that seeks to describe gravity according to the principles of quantum mechanics. It deals with environments in which neither gravitational nor quantum effects can be ignored, such as in the vicinity of black holes or similar compact astrophysical objects, as well as in the early stages of the universe moments after the Big Bang.

<span class="mw-page-title-main">Gravitational singularity</span> Condition in which spacetime itself breaks down

A gravitational singularity, spacetime singularity, or simply singularity, is a theoretical condition in which gravity is predicted to be so intense that spacetime itself would break down catastrophically. As such, a singularity is by definition no longer part of the regular spacetime and cannot be determined by "where" or "when". Gravitational singularities exist at a junction between general relativity and quantum mechanics; therefore, the properties of the singularity cannot be described without an established theory of quantum gravity. Trying to find a complete and precise definition of singularities in the theory of general relativity, the current best theory of gravity, remains a difficult problem. A singularity in general relativity can be defined by the scalar invariant curvature becoming infinite or, better, by a geodesic being incomplete.

<span class="mw-page-title-main">Black hole thermodynamics</span> Area of study

In physics, black hole thermodynamics is the area of study that seeks to reconcile the laws of thermodynamics with the existence of black hole event horizons. As the study of the statistical mechanics of black-body radiation led to the development of the theory of quantum mechanics, the effort to understand the statistical mechanics of black holes has had a deep impact upon the understanding of quantum gravity, leading to the formulation of the holographic principle.

The chronology protection conjecture is a hypothesis first proposed by Stephen Hawking that laws of physics beyond those of standard general relativity prevent time travel—even when the latter theory states that it should be possible. The permissibility of time travel is represented mathematically by the existence of closed timelike curves in some solutions to the field equations of general relativity. The chronology protection conjecture should be distinguished from chronological censorship under which every closed timelike curve passes through an event horizon, which might prevent an observer from detecting the causal violation.

Micro black holes, also called mini black holes or quantum mechanical black holes, are hypothetical tiny black holes, for which quantum mechanical effects play an important role. The concept that black holes may exist that are smaller than stellar mass was introduced in 1971 by Stephen Hawking.

In theoretical physics, Euclidean quantum gravity is a version of quantum gravity. It seeks to use the Wick rotation to describe the force of gravity according to the principles of quantum mechanics.

<span class="mw-page-title-main">Quantum field theory in curved spacetime</span> Extension of quantum field theory to curved spacetime

In theoretical physics, quantum field theory in curved spacetime (QFTCS) is an extension of quantum field theory from Minkowski spacetime to a general curved spacetime. This theory uses a semi-classical approach; it treats spacetime as a fixed, classical background, while giving a quantum-mechanical description of the matter and energy propagating through that spacetime. A general prediction of this theory is that particles can be created by time-dependent gravitational fields (multigraviton pair production), or by time-independent gravitational fields that contain horizons. The most famous example of the latter is the phenomenon of Hawking radiation emitted by black holes.

In theoretical physics and quantum physics, a graviphoton or gravivector is a hypothetical particle which emerges as an excitation of the metric tensor in spacetime dimensions higher than four, as described in Kaluza–Klein theory. However, its crucial physical properties are analogous to a (massive) photon: it induces a "vector force", sometimes dubbed a "fifth force". The electromagnetic potential emerges from an extra component of the metric tensor , where the figure 5 labels an additional, fifth dimension.

<span class="mw-page-title-main">Gravitational anomaly</span> Breakdown of general covariance at the quantum level

In theoretical physics, a gravitational anomaly is an example of a gauge anomaly: it is an effect of quantum mechanics — usually a one-loop diagram—that invalidates the general covariance of a theory of general relativity combined with some other fields. The adjective "gravitational" is derived from the symmetry of a gravitational theory, namely from general covariance. A gravitational anomaly is generally synonymous with diffeomorphism anomaly, since general covariance is symmetry under coordinate reparametrization; i.e. diffeomorphism.

In physics, there is a speculative hypothesis that if there were a black hole with the same mass, charge and angular momentum as an electron, it would share other properties of the electron. Most notably, Brandon Carter showed in 1968 that the magnetic moment of such an object would match that of an electron. This is interesting because calculations ignoring special relativity and treating the electron as a small rotating sphere of charge give a magnetic moment roughly half the experimental value.

Werner Israel, was a theoretical physicist known for his contributions to gravitational theory, and especially to the understanding of black holes.

<span class="mw-page-title-main">Dennis W. Sciama</span> British physicist (1926–1999)

Dennis William Siahou Sciama, was an English physicist who, through his own work and that of his students, played a major role in developing British physics after the Second World War. He was the PhD supervisor to many famous physicists and astrophysicists, including John D. Barrow, David Deutsch, George F. R. Ellis, Stephen Hawking, Adrian Melott and Martin Rees, among others; he is considered one of the fathers of modern cosmology.

Malcolm John Perry is a British theoretical physicist and emeritus professor of theoretical physics at University of Cambridge and professor of theoretical physics at Queen Mary University of London. His research mainly concerns quantum gravity, black holes, general relativity, and supergravity.

In theoretical physics, thermal quantum field theory or finite temperature field theory is a set of methods to calculate expectation values of physical observables of a quantum field theory at finite temperature.

In the theory of general relativity, the Gibbons–Hawking effect is the statement that a temperature can be associated to each solution of the Einstein field equations that contains a causal horizon. It is named after Gary Gibbons and Stephen Hawking.

Sergio Ferrara is an Italian physicist working on theoretical physics of elementary particles and mathematical physics. He is renowned for the discovery of theories introducing supersymmetry as a symmetry of elementary particles and of supergravity, the first significant extension of Einstein's general relativity, based on the principle of "local supersymmetry". He is an emeritus staff member at CERN and a professor emeritus at the University of California, Los Angeles.

The following outline is provided as an overview of and topical guide to black holes:

Hermann Nicolai is a German theoretical physicist and director emeritus at the Max Planck Institute for Gravitational Physics in Potsdam-Golm.

References

  1. 1 2 3 Anon (2014). "Gibbons, Prof. Gary William" . Who's Who (online Oxford University Press  ed.). Oxford: A & C Black. doi:10.1093/ww/9780199540884.013.17017.(Subscription or UK public library membership required.)
  2. 1 2 3 Gibbons, Gary William (1973). Some aspects of gravitational radiation and gravitational collapse. lib.cam.ac.uk (PhD thesis). University of Cambridge. EThOS   uk.bl.ethos.599378.
  3. 1 2 3 "Library and Archive Catalogue: EC/1999/16 Gibbons, Gary William". London: The Royal Society. Archived from the original on 7 February 2014.
  4. 1 2 Gary Gibbons at the Mathematics Genealogy Project
  5. Hull, Christopher Michael (1983). The structure and stability of the vacua of supergravity. lib.cam.ac.uk (PhD thesis). University of Cambridge. OCLC   499826125. EThOS   uk.bl.ethos.350108.
  6. Gary Gibbons's publications indexed by the Scopus bibliographic database. (subscription required)
  7. Euclidean Quantum Gravity, World Scientific (Singapore, 1993) Archived 19 May 2012 at the Wayback Machine ; Paperback ISBN   981-02-0516-3
  8. Gibbons, G. W., Hawking, S. W. (1977). "Cosmological Event Horizons, Thermodynamics, and Particle Creation". Physical Review D . 15 (10): 2738–2751. Bibcode:1977PhRvD..15.2738G. doi: 10.1103/PhysRevD.15.2738 .{{cite journal}}: CS1 maint: multiple names: authors list (link)
  9. Gibbons, G. W., Hawking, S. W. (1977). "Action Integrals and Partition Functions in Quantum Gravity". Physical Review D . 15 (10): 2752–2756. Bibcode:1977PhRvD..15.2752G. doi:10.1103/PhysRevD.15.2752.{{cite journal}}: CS1 maint: multiple names: authors list (link)
  10. Gibbons, G. W., Hawking, S. W., Perry, M. J. (1978). "Path Integrals and the Indefiniteness of the Gravitational Action". Nucl. Phys. B. 138 (1): 141–150. Bibcode:1978NuPhB.138..141G. doi:10.1016/0550-3213(78)90161-X.{{cite journal}}: CS1 maint: multiple names: authors list (link)
  11. Gibbons, G. W. (1998). "Born–Infeld particles and Dirichlet p-branes". Nucl. Phys. B. 514 (3): 603–639. arXiv: hep-th/9709027 . Bibcode:1998NuPhB.514..603G. doi:10.1016/S0550-3213(97)00795-5. S2CID   119331128.