- Julian Schwinger
Infobox_Scientist

name =Julian Schwinger

imagesize = 180px

caption =

birth_date = birth date|1918|2|12|mf=y

birth_place =New York City, New York , USA

death_date = death date and age|1994|7|16|1918|2|12

death_place =Los Angeles, California , USA

nationality =United States

field =Physics

work_institution =University of California, Berkeley Purdue University Massachusetts Institute of Technology Harvard University University of California, Los Angeles

alma_mater =City College of New York Columbia University

doctoral_advisor =Isidor Isaac Rabi

doctoral_students =Roy Glauber Ben R. Mottelson Sheldon Lee Glashow Walter Kohn Bryce DeWitt Daniel Kleitman

known_for =Quantum electrodynamics

prizes = nowrap|Nobel Prize in Physics (1965)

religion =

footnotes =**Julian Seymour Schwinger**(February 12 ,1918 –July 16 ,1994 ) was an Americantheoretical physicist . He is best known for his work on thetheory ofquantum electrodynamics , in particular for developing a relativistically invariant perturbation theory, and for renormalizing QED to one loop order.Schwinger is recognized as one of the greatest physicists of the twentieth century, responsible for much of modern quantum field theory, including a differential form of path integration, and the equations of motion for quantum fields. He developed the first electroweak model, and the first example of confinement in 1+1 dimensions. He is responsible for the theory of multiple neutrinos, Schwinger terms, and the theory of the spin 3/2 field.

**Biography**Schwinger was born in New York City where he attended

Townsend Harris High School and then theCity College of New York as an undergraduate before transferring toColumbia University , where he received his B.A. in 1936 and his Ph.D. (overseen byI.I. Rabi ) in 1939. He worked at theUniversity of California, Berkeley (underJ. Robert Oppenheimer ) and was later appointed to a position atPurdue University .**Career**During

World War II Schwinger worked at theRadiation Laboratory at MIT, providing theoretical support for the development ofradar . After the war, Schwinger left Purdue forHarvard University , where he taught from 1945 to 1974.Schwinger developed an affinity for

Green's function s from his radar work, and he used these methods to formulate quantum field theory in terms of local Green's functions in a relativistically invariant way. This allowed him to unambiguously calculate the first corrections to the electron magnetic moment inquantum electrodynamics . Earlier noncovariant work had arrived at infinite answers, but the extra symmetry in his methods allowed Schwinger to isolate the correct finite corrections.Schwinger developedrenormalization , formulatingquantum electrodynamics unambiguously to one-loop order.In the same era, he introduced nonperturbative methods into quantum field theory, by calculating the rate at which

electron -positron pairs are created by tunneling in an electric field, a process now known as theSchwinger effect . This effect could not be seen in any finite order in perturbation theory.Schwinger's foundational work on quantum field theory constructed the modern framework of field correlation functions and their equations of motion. He expressed the

Feynman path integral in differential form, a formalism which allowed bosons and fermions to be treated equally for the first time, a differential form of Grassman integration. He gave elegant proofs for thespin-statistics theorem and theCPT theorem , and noted that the field algebra lead to anomalousSchwinger terms in various classical identities, because of short distance singularities. This were foundational results in field theory, instrumental for the proper understanding of anomalies.In other notable early work, Rarita and Schwinger formulated the abstract Pauli and Fierz theory of the spin 3/2 field in a concrete form, as a vector of Dirac spinors. In order for the spin-3/2 field to interact consistently, some form of supersymmetry is required, and Schwinger later regretted that he had not followed up on this work far enough to discover supersymmetry.

Schwinger discovered that

neutrino s come in multiple varieties, one for theelectron and one for themuon . Nowadays there is known to be exactly three neutrinos, the third is the partner thetau lepton .In the 1960s, Schwinger formulated and analyzed what is now known as the

Schwinger model , quantum electrodynamics in one space and one time dimension, the first example of a confining theory. He was also the first to suggest an electroweak gauge theory, an SU(2) gauge group spontaneously broken to electromagnetic U(1) at long distances. This was extended by his studentSheldon Glashow into the accepted pattern of electroweak unification. He attempted to formulate a theory of quantum electrodynamics with pointmagnetic monopoles , a program which met with limited success because monopoles are strongly interacting when the quantum of charge is small.Having supervised more than seventy doctoral dissertations, Schwinger is known as one of the most prolific graduate advisors in physics. Four of his students won Nobel prizes:

Roy Glauber ,Benjamin Roy Mottelson ,Sheldon Glashow andWalter Kohn (in chemistry).Schwinger had a mixed relationship with his colleagues, largely because of his

**source theory**. Schwinger considered source theory as a substitute for field theory, although it is only a different point of view, a version ofeffective field theory . It treats quantum fields as long-distance phenomena, and does not require a well defined continuum limit. Source theory was considered overly formal and lacking in distinctness from quantum field theory, and the criticisms by his Harvard colleagues led Schwinger to leave the faculty in 1972 for UCLA. His work there was further from the mainstream, but he continued to find source theory reformulations of quantum field theoretic results for the rest of his career.After 1989 Schwinger took a keen interest in the non-mainstream research of low-energy nuclear fusion reactions (AKA

cold fusion ). He wrote eight theory papers about it. He resigned from theAmerican Physical Society after their refusal to publish his papers. He felt that cold fusion research was being suppressed and academic freedom violated. He wrote: "The pressure for conformity is enormous. I have experienced it in editors’ rejection of submitted papers, based on venomous criticism of anonymous referees. The replacement of impartial reviewing by censorship will be the death of science."In his last publications, Schwinger proposed a theory of sonoluminescence as a long distance quantum radiative phenomenon associated not with atoms, but with fast-moving surfaces in the collapsing bubble, where there are discontinuities in the dielectric constant. Standard explanations, now supported by experiments, focus on superheated gas atoms inside the bubble as the source of the light, but Schwinger's methods tie back to his old quantum electrodynamic papers.

Schwinger was jointly awarded the

Nobel Prize in Physics in 1965 for his work onquantum electrodynamics (QED), along withRichard Feynman andShinichiro Tomonaga .**Schwinger and**Feynman As a famous physicist, Schwinger was often compared to another legendary physicist of his generation,

Richard Feynman . Schwinger was more formally inclined and favored symbolic manipulations inQuantum Field Theory . He worked with local field operators, and found relations between them, and he felt that physicists should understand the algebra of local fields, no matter how paradoxical.By contrast, Feynman was more intuitive, believing that the physics could be extracted entirely from the

Feynman diagram s, which gave a particle picture. Schwinger commented on Feynman diagrams in the following way,Schwinger disliked Feynman diagrams, because he felt that they made the student focus on the particles and forget about local fields, which in his view inhibited understanding. He went so far as to ban them altogether from his class, although he understood them perfectly well and was observed to use them in private.

Despite sharing the Nobel Prize, Schwinger and Feynman had a different approach to quantum electrodynamics and to quantum field theory in general. Feynman used a regulator, while Schwinger was able to formally renormalize to one loop without an explicit regulator. Schwinger believed in the formalism of local fields, while Feynman had faith in the particle paths. They followed each other's work closely, and each respected the other. On Feynman's death, Schwinger described him as

**Personal life**Schwinger is buried at

Mount Auburn Cemetery ; $frac\{alpha\}\{2pi\}$ is engraved above his name on histombstone .These symbols refer to his calculation of the correction ("anomalous") to the magnetic moment of the electron.**ee also***

Schwinger model

*Schwinger-Dyson equation s

*Schwinger's variational principle

*Rarita-Schwinger action

*Lippmann-Schwinger equation

*Schwinger parametrization **References****Publications***Feshbach, H., Schwinger, J. & J. A. Harr. [

*http://www.osti.gov/cgi-bin/rd_accomplishments/display_biblio.cgi?id=ACC0109&numPages=57&fp=N "Effect of Tensor Range in Nuclear Two-Body Problems"*] , Computation Laboratory ofHarvard University ,United States Department of Energy (through predecessor agency theAtomic Energy Commission ), (November 1949).

*Schwinger, J. [*http://www.osti.gov/cgi-bin/rd_accomplishments/display_biblio.cgi?id=ACC0111&numPages=92&fp=N "On Angular Momentum"*] ,Harvard University , Nuclear Development Associates, Inc.,United States Department of Energy (through predecessor agency theAtomic Energy Commission ), (January 26, 1952).

*Schwinger, J. [*http://www.osti.gov/cgi-bin/rd_accomplishments/display_biblio.cgi?id=ACC0110&numPages=51&fp=N "The Theory of Quantized Fields. II"*] ,Harvard University ,United States Department of Energy (through predecessor agency theAtomic Energy Commission ), (1951).

*Schwinger, J. [*http://www.osti.gov/cgi-bin/rd_accomplishments/display_biblio.cgi?id=ACC0112&numPages=35&fp=N "The Theory of Quantizied Fields. III"*] ,Harvard University ,United States Department of Energy (through predecessor agency theAtomic Energy Commission ), (May 1953).**Further reading***Mehra, Jagdish and Milton, Kimball A. "Climbing the Mountain: the scientific biography of Julian Schwinger", Oxford University Press, 2000.

*cite web |last=Milton |first=Kimball |title=Julian Schwinger: Nuclear Physics, the Radiation Laboratory, Renormalized QED, Source Theory, and Beyond |date=2006-10-09 |publisher=arXiv |url=http://arxiv.org/abs/physics/0610054; revised version published as "Julian Schwinger: From Nuclear Physics and Quantum Electrodynamics to Source Theory and Beyond," Physics in Perspective,**9**, 70-114 (2007)

*Schweber, Sylvan S., "QED and the men who made it : Dyson, Feynman, Schwinger, and Tomonaga". Princeton Univ. Press, 1994.

*Ng, Y. Jack, Ed., "Julian Schwinger; the Physicist, the Teacher, and the Man" ,World Scientific, Singapore , 1996 ISBN 9810225318**External links*** [

*http://www.osti.gov/accomplishments/schwinger.html Photograph, Biography and Bibliographic Resources*] , from theOffice of Scientific and Technical Information ,United States Department of Energy

* [*http://www.nobel-winners.com/Physics/julian_seymour_schwinger.html Julian Schwinger*]

* [*http://www.nobel.se/physics/laureates/1965/schwinger-bio.html Nobel Museum Biography*]

* [*http://holiker.narod.ru/five/schwinger-press.html fundamental work in quantum electrodynamics, with deep-ploughing consequences for the physics of elementary particles*]Persondata

NAME= Schwinger, Julian

ALTERNATIVE NAMES=

SHORT DESCRIPTION=Physicist

DATE OF BIRTH=February 12 ,1918

PLACE OF BIRTH=New York City , U.S.

DATE OF DEATH=July 16 ,1994

PLACE OF DEATH=Los Angeles , U.S.

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**Julian Schwinger**— Julian Seymour Schwinger, 1965 Julian Seymour Schwinger (* 12. Februar 1918 in New York; † 16. Juli 1994 in Los Angeles) war einer der führenden US amerikanischen theoretischen Physiker. Zusammen mit Richard P. Feynman und … Deutsch Wikipedia**Julian Schwinger**— Nacimiento 12 de febrero de 1918 New York City, Estados Unidos … Wikipedia Español**Julian Schwinger**— Julian Seymour Schwinger, 1965 Julian Seymour Schwinger (12 février 1918 16 juillet 1994) est un physicien américain. Il formule la théorie de la renormalisation et décrit un phénomène de paire d électron positron connu sous… … Wikipédia en Français**Physiknobelpreis 1965: Richard Feynman — Julian Schwinger — Shin-Ichirō Tomonaga**— Die drei Physiker aus den USA und Japan erhielten den Nobelpreis für ihre fundamentalen Leistungen in der Quantenelektrodynamik, die tief gehende Konsequenzen für die Elementarteilchenphysik hatten. Biografien Richard Feynman, * New York… … Universal-Lexikon**Julian Seymour Schwinger**— Julian Seymour Schwinger, 1965 Julian Seymour Schwinger (* 12. Februar 1918 in New York; † 16. Juli 1994 in Los Angeles) war einer der führenden US amerikanischen theoretischen Physiker. Zusammen mit Richard P. Feynman und Shinichirō Tomonaga… … Deutsch Wikipedia**Julian Seymour Schwinger**— Julian Schwinger Julian Seymour Schwinger (12 février 1918 16 juillet 1994) est un physicien américain. Il formule la théorie de la renormalisation et décrit un phénomène de paire d électron positron connu sous le nom d Effet… … Wikipédia en Français**Schwinger parametrization**— is a technique for evaluating loop integrals which arise from Feynman diagrams with one or more loops.Using the well known observation that:frac{1}{A^n}=frac{1}{(n 1)!}int^infty 0 du , u^{n 1}e^{ uA},Julian Schwinger noticed that one may simplify … Wikipedia**Schwinger, Julian Seymour**— ▪ 1995 U.S. physicist (b. Feb. 12, 1918, New York, N.Y. d. July 16, 1994, Los Angeles, Calif.), was a brilliant theoretician whose studies helped define the basic principles of quantum electrodynamics, a theoretical description of the… … Universalium**Schwinger's variational principle**— In Schwinger s variational approach to quantum field theory, introduced by Julian Schwinger, the quantum action is an operator. Although this approachis superficially different from the functional integral(path integral) where the action is a… … Wikipedia**Schwinger-Dyson equation**— The Schwinger Dyson equation, named after Julian Schwinger and Freeman Dyson, is an equation of quantum field theory (QFT). Given a polynomially bounded functional F over the field configurations, then, for any state vector (which is a solution… … Wikipedia