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	<title>CPT symmetry - Revision history</title>
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	<updated>2026-04-10T20:10:56Z</updated>
	<subtitle>Revision history for this page on the wiki</subtitle>
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		<id>https://wiki.cern.ch/index.php?title=CPT_symmetry&amp;diff=11490&amp;oldid=prev</id>
		<title>Vigen: Created page with &quot;&#039;&#039;&#039;Charge, parity, and time reversal symmetry&#039;&#039;&#039; is a fundamental symmetry of physical laws under the simultaneous transformations of charge conjugation (C), parity transformation (P), and time reversal (T). CPT is the only combination of C, P, and T that is observed to be an exact symmetry of nature at the fundamental level. The &#039;&#039;&#039;CPT theorem&#039;&#039;&#039; says that CPT symmetry holds for all physical phenomena, or more precisely, that any Lorentz invariant local quantum field th...&quot;</title>
		<link rel="alternate" type="text/html" href="https://wiki.cern.ch/index.php?title=CPT_symmetry&amp;diff=11490&amp;oldid=prev"/>
		<updated>2026-04-09T19:02:21Z</updated>

		<summary type="html">&lt;p&gt;Created page with &amp;quot;&amp;#039;&amp;#039;&amp;#039;Charge, parity, and time reversal symmetry&amp;#039;&amp;#039;&amp;#039; is a fundamental symmetry of physical laws under the simultaneous transformations of charge conjugation (C), parity transformation (P), and time reversal (T). CPT is the only combination of C, P, and T that is observed to be an exact symmetry of nature at the fundamental level. The &amp;#039;&amp;#039;&amp;#039;CPT theorem&amp;#039;&amp;#039;&amp;#039; says that CPT symmetry holds for all physical phenomena, or more precisely, that any Lorentz invariant local quantum field th...&amp;quot;&lt;/p&gt;
&lt;p&gt;&lt;b&gt;New page&lt;/b&gt;&lt;/p&gt;&lt;div&gt;&amp;#039;&amp;#039;&amp;#039;Charge, parity, and time reversal symmetry&amp;#039;&amp;#039;&amp;#039; is a fundamental symmetry of physical laws under the simultaneous transformations of charge conjugation (C), parity transformation (P), and time reversal (T). CPT is the only combination of C, P, and T that is observed to be an exact symmetry of nature at the fundamental level. The &amp;#039;&amp;#039;&amp;#039;CPT theorem&amp;#039;&amp;#039;&amp;#039; says that CPT symmetry holds for all physical phenomena, or more precisely, that any Lorentz invariant local quantum field theory with a Hermitian Hamiltonian must have CPT symmetry. In layman terms, this stipulates that an antimatter, mirrored, and time reversed universe would behave exactly the same as our regular universe.&lt;br /&gt;
&lt;br /&gt;
For more information, see [[wikipedia:CPT symmetry|Wikipedia]].&lt;br /&gt;
[[Category:Scientific terms]]&lt;/div&gt;</summary>
		<author><name>Vigen</name></author>
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