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	<title>Power closed - Revision history</title>
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	<updated>2026-04-18T06:05:40Z</updated>
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		<title>en&gt;Trappist the monk: /* References */replace mr template with mr parameter in CS1 templates; using AWB</title>
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		<updated>2014-09-25T13:28:10Z</updated>

		<summary type="html">&lt;p&gt;&lt;span class=&quot;autocomment&quot;&gt;References: &lt;/span&gt;replace mr template with mr parameter in CS1 templates; using &lt;a href=&quot;/index.php?title=Testwiki:AWB&amp;amp;action=edit&amp;amp;redlink=1&quot; class=&quot;new&quot; title=&quot;Testwiki:AWB (page does not exist)&quot;&gt;AWB&lt;/a&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 15:28, 25 September 2014&lt;/td&gt;
				&lt;/tr&gt;&lt;tr&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot; id=&quot;mw-diff-left-l1&quot;&gt;Line 1:&lt;/td&gt;
&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 1:&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;−&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;In [[mathematics]], &#039;&#039;&#039;Cartan&#039;s equivalence method&#039;&#039;&#039; &lt;/del&gt;is &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;a technique in [[differential geometry]] for determining whether two geometrical structures are the same up to a [[diffeomorphism]].  For example, if &#039;&#039;M&#039;&#039; and &#039;&#039;N&#039;&#039; are two [[Riemannian manifold]]s with metrics &#039;&#039;g&#039;&#039; and &#039;&#039;h&#039;&#039;, respectively, &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 style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;== Zeven &lt;/ins&gt;is &lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;wanneer de kinderen terug naar huis Beats Nep ==&lt;/ins&gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
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&lt;tr&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;−&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;:&amp;lt;math&amp;gt;\phi^*h=g&amp;lt;/math&amp;gt;?&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 style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;   &amp;lt;li&amp;gt;&lt;/ins&gt;[&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;http://www.shanghai30p.com/news/html/?118037&lt;/ins&gt;.&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;html http://www&lt;/ins&gt;.&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;shanghai30p&lt;/ins&gt;.&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;com/news/html/?118037&lt;/ins&gt;.&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;html&lt;/ins&gt;]&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;&amp;lt;/li&amp;gt;&lt;/ins&gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;−&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt; &lt;/div&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;+&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;  &lt;/ins&gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;−&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;Although the answer to this particular question was known &lt;/del&gt;in &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;dimension 2 to [[Carl Friedrich Gauss|Gauss]] and &lt;/del&gt;in &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;higher dimensions to [[Christoffel]] and perhaps [[Riemann]] as well&lt;/del&gt;, [&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;[Élie Cartan]] and his intellectual heirs developed a technique for answering similar questions for radically different geometric structures&lt;/del&gt;. &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;(For example see the [[Cartan&lt;/del&gt;-&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;Karlhede algorithm]&lt;/del&gt;]&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;.) &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 style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;   &amp;lt;li&amp;gt;[http://www.eagleq&lt;/ins&gt;.&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;com/bbs/forum&lt;/ins&gt;.&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;php?mod=viewthread&lt;/ins&gt;&amp;amp;&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;tid=114109&lt;/ins&gt;&amp;amp;&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;fromuid&lt;/ins&gt;=&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;7519 http://www&lt;/ins&gt;.&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;eagleq&lt;/ins&gt;.&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;com/bbs/forum&lt;/ins&gt;.&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;php?mod&lt;/ins&gt;=&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;viewthread&amp;amp;tid&lt;/ins&gt;=&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;114109&amp;amp;fromuid&lt;/ins&gt;=&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;7519]&amp;lt;/li&amp;gt;&lt;/ins&gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;−&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt; &lt;/div&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;+&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;  &lt;/ins&gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;−&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;Cartan successfully applied his equivalence method to many such structures&lt;/del&gt;, &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;including [[projective structure]]s&lt;/del&gt;, &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;[[CR structure]]s&lt;/del&gt;, &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;and [[complex structure]]s{{dn|date=September 2012}}&lt;/del&gt;, &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;as well as ostensibly non-geometrical structures such as the equivalence of [[Lagrangian]]s and [[ordinary differential equation]]s.  (His techniques were later developed more fully by many others&lt;/del&gt;, &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;such as [[D&lt;/del&gt;. &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;C&lt;/del&gt;. &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;Spencer]] and [[Shiing-Shen Chern]].)&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 style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;   &amp;lt;li&amp;gt;[http://www.canyinmao&lt;/ins&gt;.&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;com/bbs/home&lt;/ins&gt;.&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;php?mod&lt;/ins&gt;=&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;space&amp;amp;uid&lt;/ins&gt;=&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;128272 http://www.canyinmao.com/bbs/home.php?mod&lt;/ins&gt;=&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;space&amp;amp;uid&lt;/ins&gt;=&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;128272]&amp;lt;/li&amp;gt;&lt;/ins&gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;−&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt; &lt;/div&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;+&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;  &lt;/ins&gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;−&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;The equivalence method &lt;/del&gt;is &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;an essentially [[algorithm]]ic procedure for determining when two geometric structures are identical&lt;/del&gt;. &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt; For Cartan, the primary geometrical information was expressed in a [[coframe]] or collection &lt;/del&gt;of &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;coframes on a [[differentiable manifold]]&lt;/del&gt;. &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;See [[method of moving frames]]&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 style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt; &amp;lt;/ul&amp;gt;&lt;/ins&gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;−&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt; &lt;/div&gt;&lt;/td&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-side-added&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;−&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;== Overview of Cartan&#039;s method ==&lt;/del&gt;&lt;/div&gt;&lt;/td&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-side-added&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;−&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;Specifically&lt;/del&gt;, &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;suppose that &#039;&#039;M&#039;&#039; and &#039;&#039;N&#039;&#039; are a pair of manifolds each carrying a &lt;/del&gt;[&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;[G&lt;/del&gt;-&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;structure]] for a structure group &#039;&#039;G&#039;&#039;&lt;/del&gt;. &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt; This amounts to giving a special class of coframes on &#039;&#039;M&#039;&#039; and &#039;&#039;N&#039;&#039;&lt;/del&gt;. &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt; Cartan&#039;s method addresses the question of whether there exists a local diffeomorphism &amp;amp;phi;:&#039;&#039;M&#039;&#039;&amp;amp;rarr;&#039;&#039;N&#039;&#039; under which the &#039;&#039;G&#039;&#039;&lt;/del&gt;-&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;structure on &#039;&#039;N&#039;&#039; pulls back to the given &#039;&#039;G&#039;&#039;&lt;/del&gt;-&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;structure on &#039;&#039;M&#039;&#039;.  An equivalence problem has been &#039;&#039;&quot;solved&quot;&#039;&#039; if one can give a complete set of structural invariants for the &#039;&#039;G&#039;&#039;&lt;/del&gt;-&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;structure: meaning that such a diffeomorphism exists if and only if all of the structural invariants agree in a suitably defined sense&lt;/del&gt;.&lt;/div&gt;&lt;/td&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-side-added&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;−&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt; &lt;/div&gt;&lt;/td&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-side-added&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;−&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;Explicitly, local systems of one-forms &amp;amp;theta;&lt;/del&gt;&amp;lt;&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;sup&lt;/del&gt;&amp;gt;&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;&#039;&#039;i&#039;&#039;&lt;/del&gt;&amp;lt;&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;/sup&lt;/del&gt;&amp;gt; &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;and &amp;amp;gamma;&amp;lt;sup&amp;gt;&#039;&#039;i&#039;&#039;&amp;lt;/sup&amp;gt; are given on &#039;&#039;M&#039;&#039; and &#039;&#039;N&#039;&#039;&lt;/del&gt;, &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;respectively, which span the respective cotangent bundles (i&lt;/del&gt;.&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;e&lt;/del&gt;., &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;are [[coframe]]s)&lt;/del&gt;. &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt; The question is whether there is a local diffeomorphism &amp;amp;phi;:&#039;&#039;M&#039;&#039;&amp;amp;rarr;&#039;&#039;N&#039;&#039; such that the [[pullback_(differential geometry)|pullback]] of the coframe on &#039;&#039;N&#039;&#039; satisfies&lt;/del&gt;&lt;/div&gt;&lt;/td&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-side-added&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;−&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;:&amp;lt;math&amp;gt;\phi^*\gamma^i(y)=g^i_j(x)\theta^j(x)&lt;/del&gt;,&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;\ (g^i_j)\&lt;/del&gt;in &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;G&amp;lt;/math&amp;gt;  (1)&lt;/del&gt;&lt;/div&gt;&lt;/td&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-side-added&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;−&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;where the coefficient &#039;&#039;g&#039;&#039; is a function on &#039;&#039;M&#039;&#039; taking values &lt;/del&gt;in &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;the [[Lie group]] &#039;&#039;G&#039;&#039;&lt;/del&gt;. &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt; For example, if &#039;&#039;M&#039;&#039; and &#039;&#039;N&#039;&#039; are Riemannian manifolds, then &#039;&#039;G&#039;&#039;=&#039;&#039;O&#039;&#039;(&#039;&#039;n&#039;&#039;) is the orthogonal group and &amp;amp;theta;&amp;lt;sup&amp;gt;&#039;&#039;i&#039;&#039;&lt;/del&gt;&amp;lt;&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;/sup&lt;/del&gt;&amp;gt; &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;and &amp;amp;gamma;&lt;/del&gt;&amp;lt;&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;sup&lt;/del&gt;&amp;gt;&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;&#039;&#039;i&#039;&#039;&amp;lt;/sup&amp;gt; are [[orthonormal]] coframes of &#039;&#039;M&#039;&#039; and &#039;&#039;N&#039;&#039; respectively.  The question of whether two Riemannian manifolds are isometric is then a question of whether there exists a diffeomorphism &amp;amp;phi; satisfying (1)&lt;/del&gt;.&lt;/div&gt;&lt;/td&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-side-added&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;−&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt; &lt;/div&gt;&lt;/td&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-side-added&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;−&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;The first step in the Cartan method is to express the pullback relation (1) &lt;/del&gt;in &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;as invariant a way as possible through the use of a &quot;&#039;&#039;prolongation&#039;&#039;&quot;&lt;/del&gt;. &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt; The most economical way to do this is to use a &#039;&#039;G&#039;&#039;-subbundle &#039;&#039;PM&#039;&#039; of the principal bundle of linear coframes &#039;&#039;LM&#039;&lt;/del&gt;&#039;, &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;although this approach can lead to unnecessary complications when performing actual calculations&lt;/del&gt;. &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt; In particular, later on this article uses a different approach&lt;/del&gt;. &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt; But for the purposes of an overview, it is convenient to stick with the principal bundle viewpoint.&lt;/del&gt;&lt;/div&gt;&lt;/td&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-side-added&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;−&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt; &lt;/div&gt;&lt;/td&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-side-added&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;−&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;The second step is to use the diffeomorphism invariance of the &lt;/del&gt;[&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;[exterior derivative]] to try to isolate any other higher-order invariants of the &#039;&#039;G&#039;&#039;-structure&lt;/del&gt;. &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt; Basically one obtains a connection in the principal bundle &#039;&#039;PM&#039;&#039;, with some torsion&lt;/del&gt;. &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt; The components of the connection and of the torsion are regarded as invariants of the problem&lt;/del&gt;.&lt;/div&gt;&lt;/td&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-side-added&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;−&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt; &lt;/div&gt;&lt;/td&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-side-added&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;−&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;The third step is that if the remaining torsion coefficients are not constant in the fibres of the principal bundle &#039;&#039;PM&#039;&#039;, it is often possible (although sometimes difficult), to &#039;&#039;&#039;normalize&#039;&#039;&#039; them by setting them equal to a convenient constant value and solving these normalization equations, thereby reducing the effective dimension of the Lie group &#039;&#039;G&#039;&#039;.  If this occurs, one goes back to step one, now having a Lie group of one lower dimension to work with.&lt;/del&gt;&lt;/div&gt;&lt;/td&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-side-added&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;−&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt; &lt;/div&gt;&lt;/td&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-side-added&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;−&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;=&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;== The fourth step ===  &lt;/del&gt;&lt;/div&gt;&lt;/td&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-side-added&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;−&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;The main purpose of the first three steps was to reduce the structure group itself as much as possible.  Suppose that the equivalence problem has been through the loop enough times that no further reduction &lt;/del&gt;is &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;possible.  At this point, there are various possible directions in which the equivalence method leads.  For most equivalence problems, there are only four cases&lt;/del&gt;: &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;complete reduction, involution, prolongation, and degeneracy&lt;/del&gt;.&lt;/div&gt;&lt;/td&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-side-added&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;−&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt; &lt;/div&gt;&lt;/td&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-side-added&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;−&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;&#039;&#039;&#039;Complete reduction&lt;/del&gt;.&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;&#039;&#039;&#039;  Here the structure group has been reduced completely to the [[trivial group]]&lt;/del&gt;. &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt; The problem can now be handled by methods such as the [[Frobenius theorem (differential topology)|Frobenius theorem]&lt;/del&gt;]. &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt; In other words, the algorithm has successfully terminated&lt;/del&gt;.&lt;/div&gt;&lt;/td&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-side-added&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;−&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt; &lt;/div&gt;&lt;/td&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-side-added&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;−&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;On the other hand, it is possible that the torsion coefficients are constant on the fibres of &#039;&#039;PM&#039;&lt;/del&gt;&#039;. &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt; Equivalently, they no longer depend on the Lie group &#039;&#039;G&#039;&#039; because there &lt;/del&gt;is &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;nothing left to normalize&lt;/del&gt;, &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;although there may still be some torsion.  The three remaining cases assume this&lt;/del&gt;.&lt;/div&gt;&lt;/td&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-side-added&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;−&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt; &lt;/div&gt;&lt;/td&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-side-added&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;−&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;&#039;&#039;&#039;Involution.&#039;&#039;&#039;  The equivalence problem &lt;/del&gt;is &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;said to be &#039;&#039;&#039;involutive&#039;&#039;&#039; (or &#039;&#039;&lt;/del&gt;in &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;involution&#039;&#039;) if it passes [[Cartan&#039;s test]]&lt;/del&gt;. &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt; This &lt;/del&gt;is &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;essentially a rank condition on the connection obtained in the first three steps of the procedure.  The Cartan test generalizes the [[Frobenius theorem (differential topology)|Frobenius theorem]] on the solubility of first&lt;/del&gt;-&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;order linear systems of partial differential equations&lt;/del&gt;. &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt; If the coframes on &lt;/del&gt;&#039;&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;&#039;M&#039;&#039; and &#039;&#039;N&#039;&#039; (obtained by a thorough application of the first three steps of the algorithm) agree and satisfy the Cartan test&lt;/del&gt;, &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;then the two &#039;&#039;G&#039;&#039;-structures are equivalent&lt;/del&gt;. &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt; (Actually&lt;/del&gt;, &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;to the best of the author&#039;s knowledge&lt;/del&gt;, &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;the coframes must be [[real analytic]] in order for this to hold&lt;/del&gt;, &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;because the [[Cartan-Kähler theorem]] requires analyticity&lt;/del&gt;.&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;)&lt;/del&gt;&lt;/div&gt;&lt;/td&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-side-added&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;−&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt; &lt;/div&gt;&lt;/td&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-side-added&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;−&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;&#039;&#039;&#039;Prolongation&lt;/del&gt;.&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;&#039;&#039;&#039;  This is the most intricate case&lt;/del&gt;. &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt; In fact there are two sub-cases&lt;/del&gt;. &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt; In the first sub-case, all of the torsion can be uniquely absorbed into the connection form&lt;/del&gt;. &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt; (Riemannian manifolds are an example, since the Levi-Civita connection absorbs all of the torsion)&lt;/del&gt;. &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt; The connection coefficients and their invariant derivatives form a complete set of invariants of the structure, and the equivalence problem is solved&lt;/del&gt;. &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt; In the second subcase, however, it is either impossible to absorb all of the torsion, or there is some ambiguity (as is often the case in &lt;/del&gt;[&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;[Gaussian elimination]], for example)&lt;/del&gt;. &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt; Here, just as in Gaussian elimination, there are additional parameters which appear in attempting to absorb the torsion&lt;/del&gt;. &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt; These parameters themselves turn out to be additional invariants of the problem, so the structure group &#039;&#039;G&#039;&#039; must be &#039;&#039;prolonged&#039;&#039; into a subgroup of a [[jet group]]&lt;/del&gt;. &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt; Once this is done, one obtains a new coframe on the prolonged space and has to return to the first step of the equivalence method&lt;/del&gt;. &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt; (See also [[prolongation of G-structures&lt;/del&gt;]&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;].)&lt;/del&gt;&lt;/div&gt;&lt;/td&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-side-added&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;−&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt; &lt;/div&gt;&lt;/td&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-side-added&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;−&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;&#039;&#039;&#039;Degeneracy&lt;/del&gt;.&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;&#039;&#039;&#039;  Because of a non-uniformity of some rank condition, the equivalence method is unsuccessful in handling this particular equivalence problem&lt;/del&gt;. &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt; For example, consider the equivalence problem of mapping a manifold &#039;&#039;M&#039;&#039; with a single one-form &lt;/del&gt;&amp;amp;&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;theta; to another manifold with a single one-form &amp;amp;gamma; such that &amp;amp;phi;*&lt;/del&gt;&amp;amp;&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;gamma;&lt;/del&gt;=&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;&amp;amp;theta;&lt;/del&gt;. &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt; The zeros of these one forms, as well as the rank of their exterior derivatives at each point need to be taken into account&lt;/del&gt;. &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt; The equivalence method can handle such problems if all of the ranks are uniform, but it is not always suitable if the rank changes&lt;/del&gt;. &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt; Of course, depending on the particular application, a great deal of information can still be obtained with the equivalence method.&lt;/del&gt;&lt;/div&gt;&lt;/td&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-side-added&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;−&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt; &lt;/div&gt;&lt;/td&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-side-added&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;−&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;==&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;References=&lt;/del&gt;=&lt;/div&gt;&lt;/td&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-side-added&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;−&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;*{{cite book|author=Olver, P&lt;/del&gt;.&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;J&lt;/del&gt;.&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;|title&lt;/del&gt;=&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;Equivalence, invariants, and symmetry|publisher&lt;/del&gt;=&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;Oxford University Press|year&lt;/del&gt;=&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;1995|isbn&lt;/del&gt;=&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;0-521-47811-1}}&lt;/del&gt;&lt;/div&gt;&lt;/td&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-side-added&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;−&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt; &lt;/div&gt;&lt;/td&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-side-added&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;−&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;[[Category:Differential geometry]]&lt;/del&gt;&lt;/div&gt;&lt;/td&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-side-added&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;−&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;[[Category:Diffeomorphisms]]&lt;/del&gt;&lt;/div&gt;&lt;/td&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-side-added&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;/table&gt;</summary>
		<author><name>en&gt;Trappist the monk</name></author>
	</entry>
	<entry>
		<id>https://en.formulasearchengine.com/index.php?title=Power_closed&amp;diff=9431&amp;oldid=prev</id>
		<title>en&gt;Qetuth: more specific stub type</title>
		<link rel="alternate" type="text/html" href="https://en.formulasearchengine.com/index.php?title=Power_closed&amp;diff=9431&amp;oldid=prev"/>
		<updated>2012-01-01T12:29:56Z</updated>

		<summary type="html">&lt;p&gt;more specific stub type&lt;/p&gt;
&lt;p&gt;&lt;b&gt;New page&lt;/b&gt;&lt;/p&gt;&lt;div&gt;In [[mathematics]], &amp;#039;&amp;#039;&amp;#039;Cartan&amp;#039;s equivalence method&amp;#039;&amp;#039;&amp;#039; is a technique in [[differential geometry]] for determining whether two geometrical structures are the same up to a [[diffeomorphism]].  For example, if &amp;#039;&amp;#039;M&amp;#039;&amp;#039; and &amp;#039;&amp;#039;N&amp;#039;&amp;#039; are two [[Riemannian manifold]]s with metrics &amp;#039;&amp;#039;g&amp;#039;&amp;#039; and &amp;#039;&amp;#039;h&amp;#039;&amp;#039;, respectively, &lt;br /&gt;
when is there a diffeomorphism &lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\phi:M\rightarrow N&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
such that &lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\phi^*h=g&amp;lt;/math&amp;gt;?&lt;br /&gt;
&lt;br /&gt;
Although the answer to this particular question was known in dimension 2 to [[Carl Friedrich Gauss|Gauss]] and in higher dimensions to [[Christoffel]] and perhaps [[Riemann]] as well, [[Élie Cartan]] and his intellectual heirs developed a technique for answering similar questions for radically different geometric structures. (For example see the [[Cartan-Karlhede algorithm]].) &lt;br /&gt;
&lt;br /&gt;
Cartan successfully applied his equivalence method to many such structures, including [[projective structure]]s, [[CR structure]]s, and [[complex structure]]s{{dn|date=September 2012}}, as well as ostensibly non-geometrical structures such as the equivalence of [[Lagrangian]]s and [[ordinary differential equation]]s.  (His techniques were later developed more fully by many others, such as [[D. C. Spencer]] and [[Shiing-Shen Chern]].)&lt;br /&gt;
&lt;br /&gt;
The equivalence method is an essentially [[algorithm]]ic procedure for determining when two geometric structures are identical.  For Cartan, the primary geometrical information was expressed in a [[coframe]] or collection of coframes on a [[differentiable manifold]]. See [[method of moving frames]].&lt;br /&gt;
&lt;br /&gt;
== Overview of Cartan&amp;#039;s method ==&lt;br /&gt;
Specifically, suppose that &amp;#039;&amp;#039;M&amp;#039;&amp;#039; and &amp;#039;&amp;#039;N&amp;#039;&amp;#039; are a pair of manifolds each carrying a [[G-structure]] for a structure group &amp;#039;&amp;#039;G&amp;#039;&amp;#039;.  This amounts to giving a special class of coframes on &amp;#039;&amp;#039;M&amp;#039;&amp;#039; and &amp;#039;&amp;#039;N&amp;#039;&amp;#039;.  Cartan&amp;#039;s method addresses the question of whether there exists a local diffeomorphism &amp;amp;phi;:&amp;#039;&amp;#039;M&amp;#039;&amp;#039;&amp;amp;rarr;&amp;#039;&amp;#039;N&amp;#039;&amp;#039; under which the &amp;#039;&amp;#039;G&amp;#039;&amp;#039;-structure on &amp;#039;&amp;#039;N&amp;#039;&amp;#039; pulls back to the given &amp;#039;&amp;#039;G&amp;#039;&amp;#039;-structure on &amp;#039;&amp;#039;M&amp;#039;&amp;#039;.  An equivalence problem has been &amp;#039;&amp;#039;&amp;quot;solved&amp;quot;&amp;#039;&amp;#039; if one can give a complete set of structural invariants for the &amp;#039;&amp;#039;G&amp;#039;&amp;#039;-structure: meaning that such a diffeomorphism exists if and only if all of the structural invariants agree in a suitably defined sense.&lt;br /&gt;
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Explicitly, local systems of one-forms &amp;amp;theta;&amp;lt;sup&amp;gt;&amp;#039;&amp;#039;i&amp;#039;&amp;#039;&amp;lt;/sup&amp;gt; and &amp;amp;gamma;&amp;lt;sup&amp;gt;&amp;#039;&amp;#039;i&amp;#039;&amp;#039;&amp;lt;/sup&amp;gt; are given on &amp;#039;&amp;#039;M&amp;#039;&amp;#039; and &amp;#039;&amp;#039;N&amp;#039;&amp;#039;, respectively, which span the respective cotangent bundles (i.e., are [[coframe]]s).  The question is whether there is a local diffeomorphism &amp;amp;phi;:&amp;#039;&amp;#039;M&amp;#039;&amp;#039;&amp;amp;rarr;&amp;#039;&amp;#039;N&amp;#039;&amp;#039; such that the [[pullback_(differential geometry)|pullback]] of the coframe on &amp;#039;&amp;#039;N&amp;#039;&amp;#039; satisfies&lt;br /&gt;
:&amp;lt;math&amp;gt;\phi^*\gamma^i(y)=g^i_j(x)\theta^j(x),\ (g^i_j)\in G&amp;lt;/math&amp;gt;  (1)&lt;br /&gt;
where the coefficient &amp;#039;&amp;#039;g&amp;#039;&amp;#039; is a function on &amp;#039;&amp;#039;M&amp;#039;&amp;#039; taking values in the [[Lie group]] &amp;#039;&amp;#039;G&amp;#039;&amp;#039;.  For example, if &amp;#039;&amp;#039;M&amp;#039;&amp;#039; and &amp;#039;&amp;#039;N&amp;#039;&amp;#039; are Riemannian manifolds, then &amp;#039;&amp;#039;G&amp;#039;&amp;#039;=&amp;#039;&amp;#039;O&amp;#039;&amp;#039;(&amp;#039;&amp;#039;n&amp;#039;&amp;#039;) is the orthogonal group and &amp;amp;theta;&amp;lt;sup&amp;gt;&amp;#039;&amp;#039;i&amp;#039;&amp;#039;&amp;lt;/sup&amp;gt; and &amp;amp;gamma;&amp;lt;sup&amp;gt;&amp;#039;&amp;#039;i&amp;#039;&amp;#039;&amp;lt;/sup&amp;gt; are [[orthonormal]] coframes of &amp;#039;&amp;#039;M&amp;#039;&amp;#039; and &amp;#039;&amp;#039;N&amp;#039;&amp;#039; respectively.  The question of whether two Riemannian manifolds are isometric is then a question of whether there exists a diffeomorphism &amp;amp;phi; satisfying (1).&lt;br /&gt;
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The first step in the Cartan method is to express the pullback relation (1) in as invariant a way as possible through the use of a &amp;quot;&amp;#039;&amp;#039;prolongation&amp;#039;&amp;#039;&amp;quot;.  The most economical way to do this is to use a &amp;#039;&amp;#039;G&amp;#039;&amp;#039;-subbundle &amp;#039;&amp;#039;PM&amp;#039;&amp;#039; of the principal bundle of linear coframes &amp;#039;&amp;#039;LM&amp;#039;&amp;#039;, although this approach can lead to unnecessary complications when performing actual calculations.  In particular, later on this article uses a different approach.  But for the purposes of an overview, it is convenient to stick with the principal bundle viewpoint.&lt;br /&gt;
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The second step is to use the diffeomorphism invariance of the [[exterior derivative]] to try to isolate any other higher-order invariants of the &amp;#039;&amp;#039;G&amp;#039;&amp;#039;-structure.  Basically one obtains a connection in the principal bundle &amp;#039;&amp;#039;PM&amp;#039;&amp;#039;, with some torsion.  The components of the connection and of the torsion are regarded as invariants of the problem.&lt;br /&gt;
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The third step is that if the remaining torsion coefficients are not constant in the fibres of the principal bundle &amp;#039;&amp;#039;PM&amp;#039;&amp;#039;, it is often possible (although sometimes difficult), to &amp;#039;&amp;#039;&amp;#039;normalize&amp;#039;&amp;#039;&amp;#039; them by setting them equal to a convenient constant value and solving these normalization equations, thereby reducing the effective dimension of the Lie group &amp;#039;&amp;#039;G&amp;#039;&amp;#039;.  If this occurs, one goes back to step one, now having a Lie group of one lower dimension to work with.&lt;br /&gt;
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=== The fourth step ===  &lt;br /&gt;
The main purpose of the first three steps was to reduce the structure group itself as much as possible.  Suppose that the equivalence problem has been through the loop enough times that no further reduction is possible.  At this point, there are various possible directions in which the equivalence method leads.  For most equivalence problems, there are only four cases: complete reduction, involution, prolongation, and degeneracy.&lt;br /&gt;
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&amp;#039;&amp;#039;&amp;#039;Complete reduction.&amp;#039;&amp;#039;&amp;#039;  Here the structure group has been reduced completely to the [[trivial group]].  The problem can now be handled by methods such as the [[Frobenius theorem (differential topology)|Frobenius theorem]].  In other words, the algorithm has successfully terminated.&lt;br /&gt;
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On the other hand, it is possible that the torsion coefficients are constant on the fibres of &amp;#039;&amp;#039;PM&amp;#039;&amp;#039;.  Equivalently, they no longer depend on the Lie group &amp;#039;&amp;#039;G&amp;#039;&amp;#039; because there is nothing left to normalize, although there may still be some torsion.  The three remaining cases assume this.&lt;br /&gt;
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&amp;#039;&amp;#039;&amp;#039;Involution.&amp;#039;&amp;#039;&amp;#039;  The equivalence problem is said to be &amp;#039;&amp;#039;&amp;#039;involutive&amp;#039;&amp;#039;&amp;#039; (or &amp;#039;&amp;#039;in involution&amp;#039;&amp;#039;) if it passes [[Cartan&amp;#039;s test]].  This is essentially a rank condition on the connection obtained in the first three steps of the procedure.  The Cartan test generalizes the [[Frobenius theorem (differential topology)|Frobenius theorem]] on the solubility of first-order linear systems of partial differential equations.  If the coframes on &amp;#039;&amp;#039;M&amp;#039;&amp;#039; and &amp;#039;&amp;#039;N&amp;#039;&amp;#039; (obtained by a thorough application of the first three steps of the algorithm) agree and satisfy the Cartan test, then the two &amp;#039;&amp;#039;G&amp;#039;&amp;#039;-structures are equivalent.  (Actually, to the best of the author&amp;#039;s knowledge, the coframes must be [[real analytic]] in order for this to hold, because the [[Cartan-Kähler theorem]] requires analyticity.)&lt;br /&gt;
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&amp;#039;&amp;#039;&amp;#039;Prolongation.&amp;#039;&amp;#039;&amp;#039;  This is the most intricate case.  In fact there are two sub-cases.  In the first sub-case, all of the torsion can be uniquely absorbed into the connection form.  (Riemannian manifolds are an example, since the Levi-Civita connection absorbs all of the torsion).  The connection coefficients and their invariant derivatives form a complete set of invariants of the structure, and the equivalence problem is solved.  In the second subcase, however, it is either impossible to absorb all of the torsion, or there is some ambiguity (as is often the case in [[Gaussian elimination]], for example).  Here, just as in Gaussian elimination, there are additional parameters which appear in attempting to absorb the torsion.  These parameters themselves turn out to be additional invariants of the problem, so the structure group &amp;#039;&amp;#039;G&amp;#039;&amp;#039; must be &amp;#039;&amp;#039;prolonged&amp;#039;&amp;#039; into a subgroup of a [[jet group]].  Once this is done, one obtains a new coframe on the prolonged space and has to return to the first step of the equivalence method.  (See also [[prolongation of G-structures]].)&lt;br /&gt;
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&amp;#039;&amp;#039;&amp;#039;Degeneracy.&amp;#039;&amp;#039;&amp;#039;  Because of a non-uniformity of some rank condition, the equivalence method is unsuccessful in handling this particular equivalence problem.  For example, consider the equivalence problem of mapping a manifold &amp;#039;&amp;#039;M&amp;#039;&amp;#039; with a single one-form &amp;amp;theta; to another manifold with a single one-form &amp;amp;gamma; such that &amp;amp;phi;*&amp;amp;gamma;=&amp;amp;theta;.  The zeros of these one forms, as well as the rank of their exterior derivatives at each point need to be taken into account.  The equivalence method can handle such problems if all of the ranks are uniform, but it is not always suitable if the rank changes.  Of course, depending on the particular application, a great deal of information can still be obtained with the equivalence method.&lt;br /&gt;
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==References==&lt;br /&gt;
*{{cite book|author=Olver, P.J.|title=Equivalence, invariants, and symmetry|publisher=Oxford University Press|year=1995|isbn=0-521-47811-1}}&lt;br /&gt;
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[[Category:Differential geometry]]&lt;br /&gt;
[[Category:Diffeomorphisms]]&lt;/div&gt;</summary>
		<author><name>en&gt;Qetuth</name></author>
	</entry>
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