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	<title>Biography:Julian Schwinger - Revision history</title>
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		<title>Maintenance script: Create quantum physics biography page</title>
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		<summary type="html">&lt;p&gt;Create quantum physics biography page&lt;/p&gt;
&lt;p&gt;&lt;b&gt;New page&lt;/b&gt;&lt;/p&gt;&lt;div&gt;﻿{{Infobox scientist&lt;br /&gt;
| name              = Julian Schwinger&lt;br /&gt;
| image             = Julian_Schwinger.jpg&lt;br /&gt;
| caption           = Julian Schwinger&lt;br /&gt;
| birth_date        = 12 February 1918&lt;br /&gt;
| birth_place       = New York City, U.S.&lt;br /&gt;
| death_date        = 16 July 1994&lt;br /&gt;
| death_place       = Los Angeles, California, U.S.&lt;br /&gt;
| fields            = Theoretical physics&lt;br /&gt;
| workplaces        = Harvard University; University of California, Los Angeles&lt;br /&gt;
| alma_mater        = Columbia University&lt;br /&gt;
| doctoral_advisor  = Isidor Isaac Rabi&lt;br /&gt;
| known_for         = Quantum electrodynamics; Schwinger effect; source theory; variational methods&lt;br /&gt;
| awards            = Nobel Prize in Physics (1965)&lt;br /&gt;
}}&lt;br /&gt;
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&amp;#039;&amp;#039;&amp;#039;Julian Schwinger&amp;#039;&amp;#039;&amp;#039; (12 February 1918 - 16 July 1994) was an American theoretical physicist whose work helped establish modern [[Physics:Quantum Electrodynamics (QED)|quantum electrodynamics]]. He shared the 1965 Nobel Prize in Physics with [[Biography:Richard Feynman|Richard Feynman]] and Sin-Itiro Tomonaga for fundamental work in QED, including methods for calculating the interaction of light and charged particles with high precision.&amp;lt;ref&amp;gt;{{cite web |url=https://www.nobelprize.org/prizes/physics/1965/schwinger/biographical/ |title=Julian Schwinger - Biographical |publisher=Nobel Prize Outreach |access-date=20 May 2026}}&amp;lt;/ref&amp;gt;&lt;br /&gt;
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Schwinger was known for a highly formal and operator-based style of physics. During and after World War II he developed techniques that became part of the standard language of [[Physics:Quantum electromagnetic field|quantized electromagnetic fields]]. His calculation of the electron&amp;#039;s anomalous magnetic moment was a landmark result, showing how quantum field theory could produce precise measurable predictions.&lt;br /&gt;
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== Quantum field theory ==&lt;br /&gt;
Schwinger&amp;#039;s work sits at the center of the transition from early quantum mechanics to renormalized [[Physics:Quantum field theory (QFT) core|quantum field theory]]. He developed operator methods, Green-function techniques, and variational principles that influenced particle physics, many-body theory, and later field-theoretic approaches.&lt;br /&gt;
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The Schwinger effect, the predicted creation of particle-antiparticle pairs by an extremely strong electric field, remains an important theoretical idea in high-field physics and quantum vacuum studies. It connects QED with [[Physics:Quantum vacuum field|vacuum field]] behavior and the limits of classical electromagnetic description.&lt;br /&gt;
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== See also ==&lt;br /&gt;
* [[Physics:Quantum Electrodynamics (QED)]]&lt;br /&gt;
* [[Physics:Quantum electromagnetic field]]&lt;br /&gt;
* [[Physics:Quantum field theory (QFT) basics]]&lt;br /&gt;
* [[Biography:Richard Feynman]]&lt;br /&gt;
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== References ==&lt;br /&gt;
{{reflist|3}}&lt;br /&gt;
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{{DEFAULTSORT:Schwinger, Julian}}&lt;br /&gt;
[[Category:Nobel laureates in Physics]]&lt;br /&gt;
[[Category:Quantum physicists]]&lt;br /&gt;
[[Category:Theoretical physicists]]&lt;br /&gt;
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{{Sourceattribution|Biography:Julian Schwinger|1}}&lt;/div&gt;</summary>
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