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	<id>http://localhost/mediawiki/index.php?action=history&amp;feed=atom&amp;title=Quantum_Entanglement</id>
	<title>Quantum Entanglement - Revision history</title>
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	<updated>2026-04-08T11:24:39Z</updated>
	<subtitle>Revision history for this page on the wiki</subtitle>
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	<entry>
		<id>http://localhost/mediawiki/index.php?title=Quantum_Entanglement&amp;diff=848&amp;oldid=prev</id>
		<title>Jess at 22:49, 17 September 2022</title>
		<link rel="alternate" type="text/html" href="http://localhost/mediawiki/index.php?title=Quantum_Entanglement&amp;diff=848&amp;oldid=prev"/>
		<updated>2022-09-17T22:49:40Z</updated>

		<summary type="html">&lt;p&gt;&lt;/p&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 22:49, 17 September 2022&lt;/td&gt;
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  &lt;td class=&quot;diff-context diff-side-deleted&quot;&gt;&lt;div&gt;Characteristic &quot;F&amp;amp;micro;F&quot; signals in a variety of insulating fluorides.|}&lt;/div&gt;&lt;/td&gt;
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  &lt;td class=&quot;diff-context diff-side-added&quot;&gt;&lt;div&gt;Characteristic &quot;F&amp;amp;micro;F&quot; signals in a variety of insulating fluorides.|}&lt;/div&gt;&lt;/td&gt;
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  &lt;td class=&quot;diff-addedline diff-side-added&quot;&gt;&lt;div&gt;The role of &amp;lt;SUP&amp;gt;19&amp;lt;/SUP&amp;gt;F in such coupled evolution can be played by any spin-1/2 nucleus, but few have a large enough magnetic moment or are sufficiently near the &amp;amp;micro;&amp;lt;SUP&amp;gt;+&amp;lt;/SUP&amp;gt; to show themselves so vividly.  &lt;/div&gt;&lt;/td&gt;
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  &lt;td class=&quot;diff-addedline diff-side-added&quot;&gt;&lt;div&gt;However, even a system as complicated as the &amp;amp;micro;&amp;lt;SUP&amp;gt;+&amp;lt;/SUP&amp;gt; surrounded by 8 copper nuclei in the octahedral site exhibits enhanced relaxation when the muon&#039;s Zeeman splitting matches the electric quadrupolar splitting of the Cu nuclei in the muon&#039;s electric field.  This phenomenon is known as [[Resonant Relaxation]], which see.&lt;/div&gt;&lt;/td&gt;
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&lt;/table&gt;</summary>
		<author><name>Jess</name></author>
	</entry>
	<entry>
		<id>http://localhost/mediawiki/index.php?title=Quantum_Entanglement&amp;diff=845&amp;oldid=prev</id>
		<title>Jess at 22:39, 17 September 2022</title>
		<link rel="alternate" type="text/html" href="http://localhost/mediawiki/index.php?title=Quantum_Entanglement&amp;diff=845&amp;oldid=prev"/>
		<updated>2022-09-17T22:39:45Z</updated>

		<summary type="html">&lt;p&gt;&lt;/p&gt;
&lt;table class=&quot;diff diff-contentalign-left diff-editfont-monospace&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 22:39, 17 September 2022&lt;/td&gt;
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  &lt;td class=&quot;diff-deletedline diff-side-deleted&quot;&gt;&lt;div&gt;Most muon spin relaxation is caused by &#039;&#039;&#039;R&#039;&#039;&#039;andom &#039;&#039;&#039;L&#039;&#039;&#039;ocal &#039;&#039;&#039;M&#039;&#039;&#039;agnetic &#039;&#039;&#039;F&#039;&#039;&#039;ields [&#039;&#039;&#039;RLMF&#039;&#039;&#039;] due to the magnetic moments of nearby particles, either nuclei or electrons.  (I count atomic orbitals with nonzero angular momentum as &quot;electrons&quot;.)  But this description ignores the fact that whatever spin hamiltonian operates on the muon spin due to the other spins also acts on the other spins due to the muon spin.  In reality, all the coupled spins evolve together until interrupted by fluctuations or&lt;del class=&quot;diffchange diffchange-inline&quot;&gt; hopping.  The result is most vividly obvious when the&lt;/del&gt; muon &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;captures a single electron to form the [[Muonium]] atom, which see&lt;/del&gt;.&lt;del class=&quot;diffchange diffchange-inline&quot;&gt;  But it is also clearly evident in cases where the muon couples to a small number of spin-1/2 nuclei, as in fluoride insulators, where the &amp;lt;math&amp;gt;\mu^+&amp;lt;/math&amp;gt; takes up a position between two &amp;lt;SUP&amp;gt;19&amp;lt;/SUP&amp;gt;F nuclei and the 3-spin system exhibits oscillations at three characteristic frequencies in ZF:&lt;/del&gt;  &lt;/div&gt;&lt;/td&gt;
  &lt;td class=&quot;diff-marker&quot; data-marker=&quot;+&quot;&gt;&lt;/td&gt;
  &lt;td class=&quot;diff-addedline diff-side-added&quot;&gt;&lt;div&gt;Most muon spin relaxation is caused by &#039;&#039;&#039;R&#039;&#039;&#039;andom &#039;&#039;&#039;L&#039;&#039;&#039;ocal &#039;&#039;&#039;M&#039;&#039;&#039;agnetic &#039;&#039;&#039;F&#039;&#039;&#039;ields [&#039;&#039;&#039;RLMF&#039;&#039;&#039;] due to the magnetic moments of nearby particles, either nuclei or electrons.  (I count atomic orbitals with nonzero angular momentum as &quot;electrons&quot;.)  But this description ignores the fact that whatever spin hamiltonian operates on the muon spin due to the other spins also acts on the other spins due to the muon spin.  In reality, all the coupled spins evolve together until interrupted by fluctuations or muon &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;hopping&lt;/ins&gt;.  &lt;/div&gt;&lt;/td&gt;
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  &lt;td class=&quot;diff-addedline diff-side-added&quot;&gt;&lt;div&gt;The result is most vividly obvious when the muon captures a single electron to form the [[Muonium]] atom, which see.  &lt;/div&gt;&lt;/td&gt;
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  &lt;td class=&quot;diff-marker&quot; data-marker=&quot;+&quot;&gt;&lt;/td&gt;
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  &lt;td class=&quot;diff-marker&quot; data-marker=&quot;+&quot;&gt;&lt;/td&gt;
  &lt;td class=&quot;diff-addedline diff-side-added&quot;&gt;&lt;div&gt;But it is also clearly evident in cases where the muon couples to a small number of spin-1/2 nuclei, as in fluoride insulators, where the &amp;lt;math&amp;gt;\mu^+&amp;lt;/math&amp;gt; takes up a position between two &amp;lt;SUP&amp;gt;19&amp;lt;/SUP&amp;gt;F nuclei and the 3-spin system exhibits oscillations at three characteristic frequencies in ZF:  &lt;/div&gt;&lt;/td&gt;
&lt;/tr&gt;
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&lt;tr&gt;
  &lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;
  &lt;td class=&quot;diff-context diff-side-deleted&quot;&gt;&lt;div&gt;&amp;lt;center&amp;gt;&lt;/div&gt;&lt;/td&gt;
  &lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;
  &lt;td class=&quot;diff-context diff-side-added&quot;&gt;&lt;div&gt;&amp;lt;center&amp;gt;&lt;/div&gt;&lt;/td&gt;
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&lt;/table&gt;</summary>
		<author><name>Jess</name></author>
	</entry>
	<entry>
		<id>http://localhost/mediawiki/index.php?title=Quantum_Entanglement&amp;diff=843&amp;oldid=prev</id>
		<title>Jess: Created page with &quot;Relaxonomy --&gt; here ----  Most muon spin relaxation is caused by &#039;&#039;&#039;R&#039;&#039;&#039;andom &#039;&#039;&#039;L&#039;&#039;&#039;ocal &#039;&#039;&#039;M&#039;&#039;&#039;agnetic &#039;&#039;&#039;F&#039;&#039;&#039;ields [&#039;&#039;&#039;RLMF&#039;&#039;&#039;] due to the magnetic moments of nearby pa...&quot;</title>
		<link rel="alternate" type="text/html" href="http://localhost/mediawiki/index.php?title=Quantum_Entanglement&amp;diff=843&amp;oldid=prev"/>
		<updated>2022-09-17T22:35:00Z</updated>

		<summary type="html">&lt;p&gt;Created page with &amp;quot;&lt;a href=&quot;/mediawiki/index.php/Relaxonomy&quot; title=&quot;Relaxonomy&quot;&gt;Relaxonomy&lt;/a&gt; --&amp;gt; here ----  Most muon spin relaxation is caused by &amp;#039;&amp;#039;&amp;#039;R&amp;#039;&amp;#039;&amp;#039;andom &amp;#039;&amp;#039;&amp;#039;L&amp;#039;&amp;#039;&amp;#039;ocal &amp;#039;&amp;#039;&amp;#039;M&amp;#039;&amp;#039;&amp;#039;agnetic &amp;#039;&amp;#039;&amp;#039;F&amp;#039;&amp;#039;&amp;#039;ields [&amp;#039;&amp;#039;&amp;#039;RLMF&amp;#039;&amp;#039;&amp;#039;] due to the magnetic moments of nearby pa...&amp;quot;&lt;/p&gt;
&lt;p&gt;&lt;b&gt;New page&lt;/b&gt;&lt;/p&gt;&lt;div&gt;[[Relaxonomy]] --&amp;gt; here&lt;br /&gt;
----&lt;br /&gt;
&lt;br /&gt;
Most muon spin relaxation is caused by &amp;#039;&amp;#039;&amp;#039;R&amp;#039;&amp;#039;&amp;#039;andom &amp;#039;&amp;#039;&amp;#039;L&amp;#039;&amp;#039;&amp;#039;ocal &amp;#039;&amp;#039;&amp;#039;M&amp;#039;&amp;#039;&amp;#039;agnetic &amp;#039;&amp;#039;&amp;#039;F&amp;#039;&amp;#039;&amp;#039;ields [&amp;#039;&amp;#039;&amp;#039;RLMF&amp;#039;&amp;#039;&amp;#039;] due to the magnetic moments of nearby particles, either nuclei or electrons.  (I count atomic orbitals with nonzero angular momentum as &amp;quot;electrons&amp;quot;.)  But this description ignores the fact that whatever spin hamiltonian operates on the muon spin due to the other spins also acts on the other spins due to the muon spin.  In reality, all the coupled spins evolve together until interrupted by fluctuations or hopping.  The result is most vividly obvious when the muon captures a single electron to form the [[Muonium]] atom, which see.  But it is also clearly evident in cases where the muon couples to a small number of spin-1/2 nuclei, as in fluoride insulators, where the &amp;lt;math&amp;gt;\mu^+&amp;lt;/math&amp;gt; takes up a position between two &amp;lt;SUP&amp;gt;19&amp;lt;/SUP&amp;gt;F nuclei and the 3-spin system exhibits oscillations at three characteristic frequencies in ZF:  &lt;br /&gt;
&lt;br /&gt;
&amp;lt;center&amp;gt;&lt;br /&gt;
[[Image:FmuFx3.png|600px|inline image (click to see full size)]]&lt;br /&gt;
{| width=&amp;quot;80%&amp;quot; &lt;br /&gt;
! align=&amp;quot;center&amp;quot; |&lt;br /&gt;
Characteristic &amp;quot;F&amp;amp;micro;F&amp;quot; signals in a variety of insulating fluorides.|}&lt;br /&gt;
&amp;lt;/center&amp;gt;&lt;/div&gt;</summary>
		<author><name>Jess</name></author>
	</entry>
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