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Julian Seymour Schwinger (/ ˈ ʃ w ɪ ŋ ər /; 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.
Julian Schwinger (Nova Iorque, 12 de fevereiro de 1918 — Los Angeles, 16 de julho de 1994) foi um físico estadunidense. Foi laureado com o Nobel de Física de 1965, por trabalhos fundamentais em eletrodinâmica quântica, com implicações fundamentais na física de partículas.
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.
8 de abr. de 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
13 de fev. de 2018 · A tribute to the Nobel Prize-winning physicist who taught and inspired many distinguished scientists, including four other Nobel laureates. Learn about his achievements, personality, and legacy from his former students and colleagues.
16 de jul. de 1994 · Learn about the life and achievements of Julian Schwinger, a Nobel laureate and a pioneer of quantum electrodynamics, quantum field theory, and source theory. Explore his publications, students, awards, and legacy in physics research and education.
Julian Schwinger (1918–1994) was one of the giants of 20th Century science. He contributed to a broad range of topics in theoretical physics, ranging from classical electrodynamics to quantum mechanics, from nuclear physics through quantum electrodynamics to the general theory of quantum fields.
