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	<title>Hyperon - Revision history</title>
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	<updated>2026-04-21T17:49:52Z</updated>
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		<id>https://www.stf-wiki.com/index.php?title=Hyperon&amp;diff=22875&amp;oldid=prev</id>
		<title>Nicesociety at 04:18, 18 February 2009</title>
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		<updated>2009-02-18T04:18:39Z</updated>

		<summary type="html">&lt;p&gt;&lt;/p&gt;
&lt;p&gt;&lt;b&gt;New page&lt;/b&gt;&lt;/p&gt;&lt;div&gt;In particle physics, a hyperon is any baryon containing one or more strange quarks, but no charm quarks or bottom quarks.&lt;br /&gt;
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Being baryons, all hyperons are fermions. That is, they have half-integer spin and obey Fermi-Dirac statistics. They all interact via the strong nuclear force, making them types of hadron. They are composed of three light quarks, at least one of which is a strange quark, which makes them strange baryons. Hyperons decay weakly with non-conserved parity.&lt;br /&gt;
&lt;br /&gt;
Since strangeness is conserved by the strong interactions, the ground-state hyperons cannot decay strongly. However, they do participate in strong interactions.&lt;br /&gt;
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[[Category: Science]]&lt;/div&gt;</summary>
		<author><name>Nicesociety</name></author>
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