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	<title>Biography:Eugene Wigner - Revision history</title>
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&lt;p&gt;&lt;b&gt;New page&lt;/b&gt;&lt;/p&gt;&lt;div&gt;﻿{{Infobox scientist&lt;br /&gt;
| name              = Eugene Wigner&lt;br /&gt;
| image             = Eugene_Wigner.jpg&lt;br /&gt;
| caption           = Eugene Wigner&lt;br /&gt;
| birth_date        = 17 November 1902&lt;br /&gt;
| birth_place       = Budapest, Kingdom of Hungary, Austria-Hungary&lt;br /&gt;
| death_date        = 1 January 1995&lt;br /&gt;
| death_place       = Princeton, New Jersey, U.S.&lt;br /&gt;
| fields            = Theoretical physics; mathematical physics&lt;br /&gt;
| workplaces        = Princeton University&lt;br /&gt;
| alma_mater        = Technical University of Berlin&lt;br /&gt;
| known_for         = Symmetry in quantum mechanics; Wigner theorem; Wigner distribution; nuclear physics&lt;br /&gt;
| awards            = Nobel Prize in Physics (1963)&lt;br /&gt;
}}&lt;br /&gt;
&lt;br /&gt;
&amp;#039;&amp;#039;&amp;#039;Eugene Wigner&amp;#039;&amp;#039;&amp;#039; (17 November 1902 - 1 January 1995) was a Hungarian-American theoretical physicist and mathematician who made symmetry a central language of modern quantum physics. His work showed how group theory could classify quantum states, selection rules, angular momentum, and the behavior of atomic and nuclear systems.&amp;lt;ref&amp;gt;{{cite web |url=https://www.nobelprize.org/prizes/physics/1963/wigner/biographical/ |title=Eugene Wigner - Biographical |publisher=Nobel Prize Outreach |access-date=20 May 2026}}&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Wigner received the 1963 Nobel Prize in Physics for contributions to nuclear and elementary-particle theory, especially through symmetry principles. His mathematical style influenced spectroscopy, quantum mechanics, nuclear physics, and quantum information.&lt;br /&gt;
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== Symmetry and quantum theory ==&lt;br /&gt;
In [[Physics:Quantum mechanics|quantum mechanics]], symmetries are represented by transformations acting on states in Hilbert space. Wigner&amp;#039;s theorem formalized how physical symmetries correspond to unitary or antiunitary transformations, a result that remains basic in quantum foundations.&lt;br /&gt;
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The Wigner distribution connects quantum states with phase-space descriptions, while Wigner&amp;#039;s broader work on representations helped organize spin, angular momentum, and conservation laws. These ideas connect directly with [[Physics:Quantum Symmetry in quantum mechanics|symmetry in quantum mechanics]] and [[Physics:Quantum Angular momentum operator|angular momentum operators]].&lt;br /&gt;
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== See also ==&lt;br /&gt;
* [[Physics:Quantum Symmetry in quantum mechanics]]&lt;br /&gt;
* [[Physics:Quantum Angular momentum operator]]&lt;br /&gt;
* [[Physics:Quantum Hilbert space]]&lt;br /&gt;
* [[Biography:John von Neumann]]&lt;br /&gt;
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== References ==&lt;br /&gt;
{{reflist|3}}&lt;br /&gt;
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{{DEFAULTSORT:Wigner, Eugene}}&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:Eugene Wigner|1}}&lt;/div&gt;</summary>
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