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Julian Seymour Schwinger ( / ˈʃwɪŋər /; February 12, 1918 – July 16, 1994) was a Nobel Prize -winning American theoretical physicist. He is best known for his work on quantum electrodynamics (QED), in particular for developing a relativistically invariant perturbation theory, and for renormalizing QED to one loop order.
Biographical. Julian Schwinger was born on 12th February 1918 in New York City. The principal direction of his life was fixed at an early age by an intense awareness of physics, and its study became an all-engrossing activity. To judge by a first publication, he debuted as a professional physicist at the age of sixteen.
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Apr 8, 2024 · Julian Seymour Schwinger (born Feb. 12, 1918, New York, N.Y., U.S.—died July 16, 1994, Los Angeles, Calif.) was an American physicist and joint winner, with Richard P. Feynman and Tomonaga Shin’ichirō, of the Nobel Prize for Physics in 1965 for introducing new ideas and methods into quantum electrodynamics.
- Silvan Schweber
Feb 13, 2018 · Schwinger shared the 1965 Nobel in physics for work in quantum electrodynamics. Four of his students also became Nobel laureates—Glauber, Ben Roy Mottelson, Ph.D. ’50, and Sheldon Glashow in physics, and Walter Kohn in chemistry—as did his onetime assistant, Walter Gilbert, also in chemistry.
Jul 16, 1994 · 12 February 1918. New York, USA. Died. 16 July 1994. Los Angeles, California, USA. Summary. Schwinger formulated quantum electrodynamics and thus reconciled quantum mechanics with Einstein's special theory of relativity. View four larger pictures. Biography. Julian Schwinger progressed rapidly through the public school system of New York City.
Jul 16, 1994 · Julian Schwinger The Nobel Prize in Physics 1965 . Born: 12 February 1918, New York, NY, USA . Died: 16 July 1994, Los Angeles, CA, USA . Affiliation at the time of the award: Harvard University, Cambridge, MA, USA
Julian Seymour Schwinger ( / ˈʃwɪŋər /; February 12, 1918 – July 16, 1994) was a Nobel Prize -winning American theoretical physicist. He is best known for his work on quantum electrodynamics (QED), in particular for developing a relativistically invariant perturbation theory, and for renormalizing QED to one loop order.
