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	<id>https://diffgeom.subwiki.org/w/index.php?action=history&amp;feed=atom&amp;title=Scalar_curvature_equation</id>
	<title>Scalar curvature equation - Revision history</title>
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	<updated>2026-04-09T08:51:46Z</updated>
	<subtitle>Revision history for this page on the wiki</subtitle>
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	<entry>
		<id>https://diffgeom.subwiki.org/w/index.php?title=Scalar_curvature_equation&amp;diff=1285&amp;oldid=prev</id>
		<title>Vipul: 2 revisions</title>
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		<updated>2008-05-18T20:08:12Z</updated>

		<summary type="html">&lt;p&gt;2 revisions&lt;/p&gt;
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				&lt;td colspan=&quot;1&quot; style=&quot;background-color: #fff; color: #202122; text-align: center;&quot;&gt;← Older revision&lt;/td&gt;
				&lt;td colspan=&quot;1&quot; style=&quot;background-color: #fff; color: #202122; text-align: center;&quot;&gt;Revision as of 20:08, 18 May 2008&lt;/td&gt;
				&lt;/tr&gt;&lt;tr&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-notice&quot; lang=&quot;en&quot;&gt;&lt;div class=&quot;mw-diff-empty&quot;&gt;(No difference)&lt;/div&gt;
&lt;/td&gt;&lt;/tr&gt;&lt;/table&gt;</summary>
		<author><name>Vipul</name></author>
	</entry>
	<entry>
		<id>https://diffgeom.subwiki.org/w/index.php?title=Scalar_curvature_equation&amp;diff=1284&amp;oldid=prev</id>
		<title>Vipul at 09:58, 25 April 2007</title>
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		<updated>2007-04-25T09:58:41Z</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 09:58, 25 April 2007&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-l21&quot;&gt;Line 21:&lt;/td&gt;
&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 21:&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&amp;lt;math&amp;gt;s(t) = \frac{r}{1 - (1 - r/s_0)e^{rt}}&amp;lt;/math&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&amp;lt;math&amp;gt;s(t) = \frac{r}{1 - (1 - r/s_0)e^{rt}}&amp;lt;/math&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;br&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;br&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;This immediately gives us some lower bounds for the &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;Ricci &lt;/del&gt;curvature at all times.&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;This immediately gives us some lower bounds for the &lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;scalar &lt;/ins&gt;curvature at all times.&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;/table&gt;</summary>
		<author><name>Vipul</name></author>
	</entry>
	<entry>
		<id>https://diffgeom.subwiki.org/w/index.php?title=Scalar_curvature_equation&amp;diff=1283&amp;oldid=prev</id>
		<title>Vipul at 09:58, 25 April 2007</title>
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		<updated>2007-04-25T09:58:34Z</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;==Definition==&lt;br /&gt;
&lt;br /&gt;
The &amp;#039;&amp;#039;&amp;#039;scalar curvature equation&amp;#039;&amp;#039;&amp;#039; is a second-order differential equation that describes the evolution of the [[scalar curvature]] associated with the [[Riemannian metric]] on a [[differential manifold]], under the [[volume-normalized Ricci flow]].&lt;br /&gt;
&lt;br /&gt;
The scalar curvature equation is as follows:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\frac{\partial R}{\partial t} = \Delta R + R(R-r)&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Here &amp;lt;math&amp;gt;r&amp;lt;/math&amp;gt; denotes the [[average scalar curvature]]. In the particular case of a compact orientable surface, &amp;lt;math&amp;gt;r&amp;lt;/math&amp;gt; is a constant computable using the [[Gauss-Bonnet theorem]], and is independent of &amp;lt;math&amp;gt;t&amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
==Analysis of the scalar curvature term==&lt;br /&gt;
&lt;br /&gt;
===As a reaction-diffusion equation===&lt;br /&gt;
&lt;br /&gt;
The scalar curvature equation is a classical example of a reaction-diffusion equation, that is, it describes a flow where the &amp;#039;&amp;#039;reaction&amp;#039;&amp;#039; term is trying to concentrate the curvature at some points, while the &amp;#039;&amp;#039;diffusion&amp;#039;&amp;#039; term is trying to equalize, or diffuse, the curvature. Thus, we can apply a suitable [[maximum principle]] here and study bounds on the PDE in terms of the associated ordinary differential equation for the reaction term:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\frac{ds}{dt} = s(s-r)&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
We can solve this in an exact manner and obtain:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;s(t) = \frac{r}{1 - (1 - r/s_0)e^{rt}}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
This immediately gives us some lower bounds for the Ricci curvature at all times.&lt;/div&gt;</summary>
		<author><name>Vipul</name></author>
	</entry>
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