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Unified field theory

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In physics, a unified field theory (UFT) is a type of field theory that allows all that is usually thought of as fundamental forces and elementary particles to be written in terms of a pair of physical and virtual fields. According to modern discoveries in physics, forces are not transmitted directly between interacting objects but instead are described and interpreted by intermediary entities called fields.[1]

However, a duality of the fields is combined into a single physical field.[2] For over a century, unified field theory has remained an open line of research. The term was coined by Albert Einstein,[3] who attempted to unify his general theory of relativity with electromagnetism. The "Theory of Everything" [4] and Grand Unified Theory[5] are closely related to unified field theory, but differ by not requiring the basis of nature to be fields, and often by attempting to explain physical constants of nature. Earlier attempts based on classical physics are described in the article on classical unified field theories.

The goal of a unified field theory has led to a great deal of progress for future theoretical physics, and progress continues.[6]

Introduction

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Forces

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The Standard Model of elementary particles + hypothetical Graviton

All four of the known fundamental forces are mediated by fields, which in the Standard Model of particle physics result from the exchange of gauge bosons. Specifically, the four fundamental interactions to be unified are:

Modern unified field theory attempts to bring these four forces and matter together into a single framework.

History

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Classic theory

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The first successful classical unified field theory was developed by James Clerk Maxwell. In 1820, Hans Christian Ørsted discovered that electric currents exerted forces on magnets, while in 1831, Michael Faraday made the observation that time-varying magnetic fields could induce electric currents. Until then, electricity and magnetism had been thought of as unrelated phenomena. In 1864, Maxwell published his famous paper on a dynamical theory of the electromagnetic field. This was the first example of a theory that was able to encompass previously separate field theories (namely electricity and magnetism) to provide a unifying theory of electromagnetism. By 1905, Albert Einstein had used the constancy of the speed-of-light in Maxwell's theory to unify our notions of space and time into an entity we now call spacetime. In 1915, he expanded this theory of special relativity to a description of gravity, general relativity, using a field to describe the curving geometry of four-dimensional (4D) spacetime.

In the years following the creation of the general theory, a large number of physicists and mathematicians enthusiastically participated in the attempt to unify the then-known fundamental interactions.[7] Given later developments in this domain, of particular interest are the theories of Hermann Weyl of 1919, who introduced the concept of an (electromagnetic) gauge field in a classical field theory[8] and, two years later, that of Theodor Kaluza, who extended General Relativity to five dimensions.[9] Continuing in this latter direction, Oscar Klein proposed in 1926 that the fourth spatial dimension be curled up into a small, unobserved circle. In Kaluza–Klein theory, the gravitational curvature of the extra spatial direction behaves as an additional force similar to electromagnetism. These and other models of electromagnetism and gravity were pursued by Albert Einstein in his attempts at a classical unified field theory. By 1930 Einstein had already considered the Einstein-Maxwell–Dirac System [Dongen]. This system is (heuristically) the super-classical [Varadarajan] limit of (the not mathematically well-defined) quantum electrodynamics. One can extend this system to include the weak and strong nuclear forces to get the Einstein–Yang-Mills–Dirac System. The French physicist Marie-Antoinette Tonnelat published a paper in the early 1940s on the standard commutation relations for the quantized spin-2 field. She continued this work in collaboration with Erwin Schrödinger after World War II. In the 1960s Mendel Sachs proposed a generally covariant field theory that did not require recourse to renormalization or perturbation theory. In 1965, Tonnelat published a book on the state of research on unified field theories.

Modern progress

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In 1963, American physicist Sheldon Glashow proposed that the weak nuclear force, electricity, and magnetism could arise from a partially unified electroweak theory. In 1967, Pakistani Abdus Salam and American Steven Weinberg independently revised Glashow's theory by having the masses for the W particle and Z particle arise through spontaneous symmetry breaking with the Higgs mechanism. This unified theory modelled the electroweak interaction as a force mediated by four particles: the photon for the electromagnetic aspect, a neutral Z particle, and two charged W particles for the weak aspect. As a result of the spontaneous symmetry breaking, the weak force becomes short-range and the W and Z bosons acquire masses of 80.4 and 91.2 GeV/c2, respectively. Their theory was first given experimental support by the discovery of weak neutral currents in 1973. In 1983, the Z and W bosons were first produced at CERN by Carlo Rubbia's team. For their insights, Glashow, Salam, and Weinberg were awarded the Nobel Prize in Physics in 1979. Carlo Rubbia and Simon van der Meer received the Prize in 1984.

After Gerardus 't Hooft showed the Glashow–Weinberg–Salam electroweak interactions to be mathematically consistent, the electroweak theory became a template for further attempts at unifying forces. In 1974, Sheldon Glashow and Howard Georgi proposed unifying the strong and electroweak interactions into the Georgi–Glashow model, the first Grand Unified Theory, which would have observable effects for energies much above 100 GeV.

Since then there have been several proposals for Grand Unified Theories, e.g. the Pati–Salam model, although none is currently universally accepted. A major problem for experimental tests of such theories is the energy scale involved, which is well beyond the reach of current accelerators. Grand Unified Theories make predictions for the relative strengths of the strong, weak, and electromagnetic forces, and in 1991 LEP determined that supersymmetric theories have the correct ratio of couplings for a Georgi–Glashow Grand Unified Theory.

Many Grand Unified Theories (but not Pati–Salam) predict that the proton can decay, and if this were to be seen, details of the decay products could give hints at more aspects of the Grand Unified Theory. It is at present unknown if the proton can decay, although experiments have determined a lower bound of 1035 years for its lifetime.

Current status

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Theoretical physicists have not yet formulated a widely accepted, consistent theory that combines general relativity and quantum mechanics to form a theory of everything. Trying to combine the graviton with the strong and electroweak interactions leads to fundamental difficulties and the resulting theory is not renormalizable. The incompatibility of the two theories remains an outstanding problem in the field of physics.

Einstein's Theory

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Maxwell's unified field theory of electromagnetic and Einstein's own general theory of relativity—which is essentially a field theory on gravitation—were purportedly at odds when Einstein began working on a unified field theory in the 1930s. Einstein hoped to unite gravity and electromagnetism as distinct facets of the same fundamental field, which were thought to be the only two universal forces known at the time. Such a theory would make fundamental, logical sense of what we see in the cosmos and seemed to be a logical extension of his work.  

The General Theory of Relativity

As part of the elaborating physical theory of relativity formed by the German-born physicist Albert Einstein, general relativity has distinguished the field of quantum mechanics, contributing to a large change in the space-time understanding. In this theory, Einstein recognizes the union of space and time, calling it a space-time dimension, proposed by the mathematician Hermann Minkowski in 1908 as a way to reformulate Albert Einstein's special theory of relativity, during the year of 1905.

  1. Spacetime: In General Relativity, the fabric of the universe is described as a four-dimensional spacetime, which combines the three spatial dimensions and one-time dimension into a single continuum. Objects and events exist within this spacetime.
  2. Curvature of Spacetime: Einstein proposed that mass and energy cause spacetime to curve. Rather than thinking of gravity as a force between two objects, General Relativity describes it as the result of objects moving along curved paths in this curved spacetime.
  3. Geodesics: In curved spacetime, objects follow paths called geodesics, which are the shortest paths between two points. For instance, planets orbit stars because they are following curved paths in the spacetime distorted by the star's mass.

The Einstein Field Equations

The core of General Relativity is encapsulated in the Einstein Field Equations:

  • Ricci curvature tensor, which represents the degree to which spacetime is curved.
  • Metric tensor, describing the geometry of spacetime.
  • Scalar curvature, a measure of the curvature of spacetime.
  • Cosmological constant, which Einstein originally introduced and later discarded, but which has gained relevance in the context of dark energy.
  • Gravitational constant.
  • Speed of light.
  • Stress-energy tensor, representing the distribution of matter and energy in spacetime.

Key Predictions and Confirmations

  1. Gravitational Time Dilation: Time runs slower in stronger gravitational fields. This has been confirmed through experiments with atomic clocks at different altitudes.
  2. Light Deflection: Light bends when it passes near a massive object, like the bending of starlight around the sun observed during a solar eclipse.
  3. Gravitational Waves: Ripples in spacetime caused by accelerating masses, such as binary black hole mergers, were directly detected by LIGO in 2015.
  4. Black Holes: Extremely dense objects where spacetime curvature becomes so intense that not even light can escape. The existence of black holes has been confirmed through various astronomical observations.

Implications

General Relativity has profound implications for our understanding of the universe. It accurately predicts phenomena that Newtonian gravity cannot, such as the precession of Mercury’s orbit, gravitational lensing by galaxies, and the expansion of the universe.

It also provides the framework for modern cosmology, including the Big Bang theory, the study of black holes, and the behavior of objects in strong gravitational fields.

Einstein’s General Theory of Relativity remains a cornerstone of modern physics, influencing both theoretical research and practical applications like GPS technology, which accounts for relativistic time dilation to provide accurate positioning.

See also

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References

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  1. ^ "Unified field theory | Einstein's Theory of Relativity | Britannica". www.britannica.com. Retrieved 2024-10-10.
  2. ^ Ernan McMullin (2002). "The Origins of the Field Concept in Physics" (PDF). Phys. Perspect. 4 (1): 13–39. Bibcode:2002PhP.....4...13M. doi:10.1007/s00016-002-8357-5. S2CID 27691986.
  3. ^ "How the search for a unified theory stumped Einstein to his dying day". phys.org.
  4. ^ Stephen W. Hawking (28 February 2006). The Theory of Everything: The Origin and Fate of the Universe. Phoenix Books; Special Anniv. ISBN 978-1-59777-508-3.
  5. ^ Ross, G. (1984). Grand Unified Theories. Westview Press. ISBN 978-0-8053-6968-7.
  6. ^ Goenner, Hubert F. M. (2004-12-01). "On the History of Unified Field Theories". Living Reviews in Relativity. 7 (1): 2. Bibcode:2004LRR.....7....2G. doi:10.12942/lrr-2004-2. ISSN 1433-8351. PMC 5256024. PMID 28179864.
  7. ^ See Catherine Goldstein & Jim Ritter (2003) "The varieties of unity: sounding unified theories 1920-1930" in A. Ashtekar, et al. (eds.), Revisiting the Foundations of Relativistic Physics, Dordrecht, Kluwer, p. 93-149; Vladimir Vizgin (1994), Unified Field Theories in the First Third of the 20th Century, Basel, Birkhäuser; Hubert Goenner On the History of Unified Field Theories Archived 2011-08-05 at the Wayback Machine.
  8. ^ Erhard Scholtz (ed) (2001), Hermann Weyl's Raum - Zeit- Materie and a General Introduction to His Scientific Work, Basel, Birkhäuser.
  9. ^ Daniela Wuensch (2003), "The fifth dimension: Theodor Kaluza's ground-breaking idea", Annalen der Physik, vol. 12, p. 519–542.

Further reading

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