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Quantum Electrodynamics

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'''Quantum electrodynamics''' ('''QED''') is a relativistic quantum field theory of electromagnetism. QED mathematically describes all phenomenon phenomena involving electric charge electrically charged particles interacting by means of the electromagnetic force, whether the interaction is between light and matter or between two charged particles. It has been called "the jewel of physics" for its extremely accurate predictions of quantities like the anomalous magnetic moment of the muon, and the Lamb shift of the energy levels of hydrogen.

Physical interpretation of QED
In classical physics, light is observed to Fermat's principle take the quickest path between two points; but how does light `know where it's going'? That is, if the start and end points are known, the path that will take the shortest time can be calculated. However, when light is first emitted, the end point is not known, so how is it that light always takes the ''quickest'' path? The answer is provided by QED. Light doesn't know where it is going, and it doesn't always take the quickest path. In fact, according to QED, light can go slower or faster than the speed of light to get there. Physically, QED describes charged particles (and their antiparticles) interacting with each other by the exchange of photons. The magnitude of these interactions can be computed using perturbation theory (quantum mechanics) perturbation theory; these rather complex formulas have a remarkable pictorial representation as Feynman diagrams [http://www.heyfeynman.com/article_info.php?articles_id=13]. QED was the theory to which Feynman diagrams were first applied. These diagrams were invented on the basis of Lagrangian mechanics. Using a Feynman diagram, one decides every possible path between the start and end points. Each path is assigned a complex number complex-valued probability and the actual path we observe is the weighted average of all possible paths. This average path is the one that the classical theory predicts, the quickest path between the two points. QED doesn't predict what will happen in an experiment. But it can predict the probability of what will happen in an experiment, which is how it is experimentally verified. Near the end of his life, Feynman gave a series of lectures on QED intended for the lay public. These lectures were transcribed and published as Feynman (1985), ''QED: The strange theory of light and matter'', a classic nonmathematical exposition of QED from the point of view articulated above. Much of Feynman's discussion springs from an everyday phenomenon: the way any sheet of glass partly reflects any light shining on it. (The book's cover featured a beautiful photograph of an iridescent soap bubble, another striking example of a phenomenon understood according to QED principles.) Feynman also pays homage to Isaac Newton's struggles to come to terms with the nature of light.

History
Quantum theory began in 1900, when Max Planck assumed that energy is quantized in order to derive a formula predicting the observed frequency dependence of the energy emitted by a black body. This dependence is completely at variance with classical physics. In 1905, Albert Einstein Einstein explained the photoelectric effect by postulating that light energy comes in quanta called photons. In 1913, Niels Bohr Bohr invoked quantization in his proposed explanation of the spectral lines of the hydrogen atom. In 1924, Louis de Broglie proposed a quantum theory of the wave-like nature of subatomic particles. The phrase "quantum physics" was first employed in Johnston's ''Planck's Universe in Light of Modern Physics''. These theories, while they fit the experimental facts to some extent, were strictly phenomenological: they provided no rigorous justification for the quantization they employed. They are collectively known as the "old quantum theory." Modern quantum mechanics was born in 1925 with Werner Heisenberg's matrix mechanics and Erwin Schrödinger's wave mechanics and the Schrödinger equation. Schrödinger subsequently showed that these two approaches were equivalent. In 1927, Heisenberg formulated his uncertainty principle, and the Copenhagen interpretation of quantum mechanics began to take shape. Around this time, Paul Dirac, in work culminating in his 1930 monograph, joined quantum mechanics and special relativity, pioneered the use of operator theory, and devised the bra-ket notation widely used since. In 1932, John von Neumann formulated the rigorous mathematical basis for quantum mechanics as the theory of linear operators on Hilbert spaces. This and other work from the founding period remains valid and widely used. Quantum chemistry began with Walter Heitler and Fritz London's 1927 quantum account of the covalent bond of the hydrogen molecule. Linus Pauling and others contributed to the subsequent development of quantum chemistry. The application of quantum mechanics to fields rather than merely to single particles, resulting in what are known as quantum field theory quantum field theories, began in 1927. Early contributors included Dirac, Wolfgang Pauli, Weisskopf, and Jordan. This line of research culminated in the 1940s in the quantum electrodynamics (QED) of Richard Feynman Feynman, Freeman Dyson, Julian Schwinger, and Sin-Itiro Tomonaga, for which they received the 1965 Nobel Prize in Physics. QED, a quantum theory of electrons, positrons, and the electromagnetic field, was the first satisfactory quantum description of a physical field theory field and of the creation and annihilation of quantum particles. QED involves a covariant and gauge invariance gauge invariant prescription for the calculation of observable quantities. Feynman's mathematical technique, based on his Feynman diagram diagrams, initially seemed very different from the field-theoretic, operator-based approach of Schwinger and Tomonaga, but Freeman Dyson later showed that the two approaches were equivalent. The renormalization procedure for eliminating the awkward infinite predictions of quantum field theory was first implemented in QED. Even though renormalization works very well in practice, Feynman was never entirely comfortable with its mathematical validity, even referring to renormalization as a "shell game" and "hocus pocus". (Feynman, 1985: 128) QED has served as a role model and template for all subsequent quantum field theories. On such subsequent theory is quantum chromodynamics, which began in the early 1960s and attained its present form in the 1975 work by H. David Politzer, David Gross and Frank Wilczek. Building on the pioneering work of Schwinger, Peter Higgs, Goldstone, and others, Sheldon Glashow, Steven Weinberg and Abdus Salam independently showed how the weak nuclear force and quantum electrodynamics could be merged into a single electroweak force.

Mathematics
Mathematically, QED has the structure of an Abelian gauge theory with a U(1) gauge group. The gauge field which mediates the interaction between the charged spin_(physics) spin-1/2 field (physics) fields is the electromagnetic field. The QED Lagrangian for the interaction of electrons and positrons through photons is :$\backslash mathcal\{L\}=\backslash bar\backslash psi(i\backslash gamma^\backslash mu\; D\_\backslash mu-m)\backslash psi\; -\backslash frac\{1\}\{4\}F\_\{\backslash mu\backslash nu\}F^\{\backslash mu\backslash nu\}$ . $\backslash \; \backslash psi$ and its Dirac adjoint $\backslash bar\backslash psi$ are the field (physics) fields representing electrically charged particles, specifically electron and positron fields represented as Dirac spinors. $D\_\backslash mu\; =\; \backslash partial\_\backslash mu+ieA\_\backslash mu\; \backslash ,\backslash !$ is the gauge covariant derivative, with $\backslash \; e$ the coupling strength (equal to the elementary charge), $\backslash \; A\_\backslash mu$ the covariant vector potential of the electromagnetic field and $F\_\{\backslash mu\backslash nu\}\; =\; \backslash partial\_\backslash mu\; A\_\backslash nu\; -\; \backslash partial\_\backslash nu\; A\_\backslash mu\; \backslash ,\backslash !$ the Maxwell's equations electromagnetic field tensor. Also, $\backslash gamma\_\backslash mu$ are Dirac matrices. The part of the Lagrangian containing the Maxwell's equations electromagnetic field tensor describes the free evolution of the electromagnetic field, whereas the Dirac equation Dirac-like equation with the gauge covariant derivative describes the free evolution of the electron and positron fields as well as their interaction with the electromagnetic field. {| | Image:vacuum_polarization.png vacuum polarization.html" title="Meaning of frame frame|The one-loop contribution to the [[vacuum polarization function Π.html" title="Meaning of The one-loop contribution to the [[vacuum polarization">frame|The one-loop contribution to the [[vacuum polarization function Π">The one-loop contribution to the [[vacuum polarization">frame|The one-loop contribution to the [[vacuum polarization function Π | | Image:electron_self_energy.png self-energy.html" title="Meaning of frame frame|The one-loop contribution to the electron [[self-energy function Σ.html" title="Meaning of The one-loop contribution to the electron [[self-energy">frame|The one-loop contribution to the electron [[self-energy function Σ">The one-loop contribution to the electron [[self-energy">frame|The one-loop contribution to the electron [[self-energy function Σ | | Image:vertex_correction.png vertex function.html" title="Meaning of frame frame|The one-loop contribution to the [[vertex function Γ.html" title="Meaning of The one-loop contribution to the [[vertex function">frame|The one-loop contribution to the [[vertex function Γ">The one-loop contribution to the [[vertex function">frame|The one-loop contribution to the [[vertex function Γ |}

See also
*anomalous magnetic moment *Basics of quantum mechanics *Bhabha scattering *Cavity quantum electrodynamics ('''Cavity QED''') *Compton scattering *Gauge theory *Gupta-Bleuler formalism *Lamb shift *Landau pole *Moeller scattering *positronium *quantum chromodynamics *Quantum field theory *quantum gauge theory *Renormalization *scalar electrodynamics *Schwinger model *Schwinger-Dyson equation *self-energy *Standard Model *vacuum polarization *vertex function

References
* Cohen-Tannoudji, Claude, Dupont-Roc, Jacques, and Grynberg, Gilbert, 1997. ''Photons and Atoms: Introduction to Quantum Electrodynamics''. John Wiley & Sons. * Richard Feynman, 1985. ''QED: The strange theory of light and matter''. Princeton Univ. Press. * --------, 1998. ''Quantum Electrodynamics''. Perseus Publishing. * Jauch, J. M., Rohrlich, F., 1980. ''The Theory of Photons and Electrons''. Springer-Verlag. * Miller, Arthur I., 1995. ''Early Quantum Electrodynamics : A Sourcebook''. Cambridge University Press. [ISBN 0521568919] * Schweber, Silvian S., 1994. ''Q.E.D. and the men who made it: Dyson, Feynman, Schwinger, and Tomonaga''. Princeton University Press. [ISBN 0-691-03327-7] * Julian Schwinger, 1958. ''Selected Papers on Quantum Electrodynamics''. Dover Publications. [ISBN 0-486-60444-6]

External links

- Feynman's lecture describing the evolution of QED
- Feynman's lectures on QED for non-physicists {{Physics-footer}} Category:Quantum electronics Category:Electrodynamics Category:Quantum field theory ca:Electrodinàmica quàntica de:Quantenelektrodynamik es:Electrodinámica cuántica fa:الکترودینامیک کوانتوم fr:Électrodynamique quantique gl:Electrodinámica cuántica it:Elettrodinamica quantistica ja:é‡?å­?é›»ç£?力学 pl:Elektrodynamika kwantowa pt:Eletrodinâmica quântica ru:КвантоваÑ? Ñ?лектродинамика sv:Kvantelektrodynamik zh:é‡?å­?電動力學 see Quantum electrodynamics

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