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	<title>CKM matrix - Revision history</title>
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	<updated>2026-04-04T15:44:57Z</updated>
	<subtitle>Revision history for this page on the wiki</subtitle>
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	<entry>
		<id>https://wiki.cern.ch/index.php?title=CKM_matrix&amp;diff=10474&amp;oldid=prev</id>
		<title>Vigen at 14:36, 30 March 2026</title>
		<link rel="alternate" type="text/html" href="https://wiki.cern.ch/index.php?title=CKM_matrix&amp;diff=10474&amp;oldid=prev"/>
		<updated>2026-03-30T14:36:10Z</updated>

		<summary type="html">&lt;p&gt;&lt;/p&gt;
&lt;table style=&quot;background-color: #fff; color: #202122;&quot; data-mw=&quot;interface&quot;&gt;
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				&lt;td colspan=&quot;2&quot; style=&quot;background-color: #fff; color: #202122; text-align: center;&quot;&gt;← Older revision&lt;/td&gt;
				&lt;td colspan=&quot;2&quot; style=&quot;background-color: #fff; color: #202122; text-align: center;&quot;&gt;Revision as of 14:36, 30 March 2026&lt;/td&gt;
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		<author><name>Vigen</name></author>
	</entry>
	<entry>
		<id>https://wiki.cern.ch/index.php?title=CKM_matrix&amp;diff=7285&amp;oldid=prev</id>
		<title>Vigen: Created page with &quot;In the Standard Model of particle physics, the &#039;&#039;&#039;Cabibbo–Kobayashi–Maskawa matrix&#039;&#039;&#039;, &#039;&#039;&#039;CKM matrix&#039;&#039;&#039;, &#039;&#039;&#039;quark mixing matrix&#039;&#039;&#039;, or &#039;&#039;&#039;KM matrix&#039;&#039;&#039; is a unitary matrix that contains information on the strength of the flavour-changing weak interaction. Technically, it specifies the mismatch of quantum states of quarks when they propagate freely and when they take part in the weak interactions. It is important in the understanding of CP violation. This matrix was in...&quot;</title>
		<link rel="alternate" type="text/html" href="https://wiki.cern.ch/index.php?title=CKM_matrix&amp;diff=7285&amp;oldid=prev"/>
		<updated>2026-02-02T13:55:37Z</updated>

		<summary type="html">&lt;p&gt;Created page with &amp;quot;In the Standard Model of particle physics, the &amp;#039;&amp;#039;&amp;#039;Cabibbo–Kobayashi–Maskawa matrix&amp;#039;&amp;#039;&amp;#039;, &amp;#039;&amp;#039;&amp;#039;CKM matrix&amp;#039;&amp;#039;&amp;#039;, &amp;#039;&amp;#039;&amp;#039;quark mixing matrix&amp;#039;&amp;#039;&amp;#039;, or &amp;#039;&amp;#039;&amp;#039;KM matrix&amp;#039;&amp;#039;&amp;#039; is a unitary matrix that contains information on the strength of the flavour-changing weak interaction. Technically, it specifies the mismatch of quantum states of quarks when they propagate freely and when they take part in the weak interactions. It is important in the understanding of CP violation. This matrix was in...&amp;quot;&lt;/p&gt;
&lt;p&gt;&lt;b&gt;New page&lt;/b&gt;&lt;/p&gt;&lt;div&gt;In the Standard Model of particle physics, the &amp;#039;&amp;#039;&amp;#039;Cabibbo–Kobayashi–Maskawa matrix&amp;#039;&amp;#039;&amp;#039;, &amp;#039;&amp;#039;&amp;#039;CKM matrix&amp;#039;&amp;#039;&amp;#039;, &amp;#039;&amp;#039;&amp;#039;quark mixing matrix&amp;#039;&amp;#039;&amp;#039;, or &amp;#039;&amp;#039;&amp;#039;KM matrix&amp;#039;&amp;#039;&amp;#039; is a unitary matrix that contains information on the strength of the flavour-changing weak interaction. Technically, it specifies the mismatch of quantum states of quarks when they propagate freely and when they take part in the weak interactions. It is important in the understanding of CP violation. This matrix was introduced for three generations of quarks by Makoto Kobayashi and Toshihide Maskawa, adding one generation to the matrix previously introduced by Nicola Cabibbo. This matrix is also an extension of the GIM mechanism, which only includes two of the three current families of quarks.&lt;br /&gt;
&lt;br /&gt;
For more information, see [[wikipedia:Cabibbo–Kobayashi–Maskawa matrix|Wikipedia]].&lt;br /&gt;
[[Category:Abbreviations]]&lt;br /&gt;
[[Category:Pages linking to Wikipedia]]&lt;/div&gt;</summary>
		<author><name>Vigen</name></author>
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