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	<title>Coercive function - Revision history</title>
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		<title>imported&gt;MichaelMaggs: Adding local short description: &quot;Mathematical function&quot;, overriding Wikidata description &quot;mathematical function that &quot;grows rapidly&quot; at the extremes of the space on which it is defined&quot;</title>
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		<updated>2024-11-21T19:21:37Z</updated>

		<summary type="html">&lt;p&gt;Adding local &lt;a href=&quot;https://en.wikipedia.org/wiki/Short_description&quot; class=&quot;extiw&quot; title=&quot;wikipedia:Short description&quot;&gt;short description&lt;/a&gt;: &amp;quot;Mathematical function&amp;quot;, overriding Wikidata description &amp;quot;mathematical function that &amp;quot;grows rapidly&amp;quot; at the extremes of the space on which it is defined&amp;quot;&lt;/p&gt;
&lt;p&gt;&lt;b&gt;New page&lt;/b&gt;&lt;/p&gt;&lt;div&gt;{{Short description|Mathematical function}}&lt;br /&gt;
{{no footnotes|date=April 2023}}&lt;br /&gt;
In [[mathematics]], a &amp;#039;&amp;#039;&amp;#039;coercive function&amp;#039;&amp;#039;&amp;#039; is a function that &amp;quot;grows rapidly&amp;quot; at the extremes of the space on which it is defined. Depending on the context different exact definitions of this idea are in use.&lt;br /&gt;
&lt;br /&gt;
==Coercive vector fields ==&lt;br /&gt;
A vector field {{math|&amp;#039;&amp;#039;f&amp;#039;&amp;#039; : &amp;#039;&amp;#039;&amp;#039;R&amp;#039;&amp;#039;&amp;#039;&amp;lt;sup&amp;gt;&amp;#039;&amp;#039;n&amp;#039;&amp;#039;&amp;lt;/sup&amp;gt; &amp;amp;rarr; &amp;#039;&amp;#039;&amp;#039;R&amp;#039;&amp;#039;&amp;#039;&amp;lt;sup&amp;gt;&amp;#039;&amp;#039;n&amp;#039;&amp;#039;&amp;lt;/sup&amp;gt;}} is called &amp;#039;&amp;#039;&amp;#039;coercive&amp;#039;&amp;#039;&amp;#039; if&lt;br /&gt;
&amp;lt;math display=&amp;quot;block&amp;quot;&amp;gt;\frac{f(x) \cdot x}{\| x \|} \to + \infty \text{ as } \| x \| \to + \infty,&amp;lt;/math&amp;gt;&lt;br /&gt;
where &amp;quot;&amp;lt;math&amp;gt;\cdot&amp;lt;/math&amp;gt;&amp;quot; denotes the usual [[dot product]] and &amp;lt;math&amp;gt;\|x\|&amp;lt;/math&amp;gt; denotes the usual Euclidean [[norm (mathematics)|norm]] of the vector &amp;#039;&amp;#039;x&amp;#039;&amp;#039;.&lt;br /&gt;
&lt;br /&gt;
A coercive vector field is in particular norm-coercive since &amp;lt;math&amp;gt;\|f(x)\| \geq  (f(x) \cdot x) / \| x \|&amp;lt;/math&amp;gt; for &amp;lt;math&amp;gt;x \in \mathbb{R}^n \setminus \{0\} &amp;lt;/math&amp;gt;, by [[Cauchy–Schwarz inequality]].&lt;br /&gt;
However a norm-coercive mapping {{math|&amp;#039;&amp;#039;f&amp;#039;&amp;#039; : &amp;#039;&amp;#039;&amp;#039;R&amp;#039;&amp;#039;&amp;#039;&amp;lt;sup&amp;gt;&amp;#039;&amp;#039;n&amp;#039;&amp;#039;&amp;lt;/sup&amp;gt; &amp;amp;rarr; &amp;#039;&amp;#039;&amp;#039;R&amp;#039;&amp;#039;&amp;#039;&amp;lt;sup&amp;gt;&amp;#039;&amp;#039;n&amp;#039;&amp;#039;&amp;lt;/sup&amp;gt;}} is not necessarily a coercive vector field. For instance the rotation {{math|1=&amp;#039;&amp;#039;f&amp;#039;&amp;#039; : &amp;#039;&amp;#039;&amp;#039;R&amp;#039;&amp;#039;&amp;#039;&amp;lt;sup&amp;gt;&amp;#039;&amp;#039;2&amp;#039;&amp;#039;&amp;lt;/sup&amp;gt; &amp;amp;rarr; &amp;#039;&amp;#039;&amp;#039;R&amp;#039;&amp;#039;&amp;#039;&amp;lt;sup&amp;gt;&amp;#039;&amp;#039;2&amp;#039;&amp;#039;&amp;lt;/sup&amp;gt;, &amp;#039;&amp;#039;f&amp;#039;&amp;#039;(&amp;#039;&amp;#039;x&amp;#039;&amp;#039;) = (−&amp;#039;&amp;#039;x&amp;#039;&amp;#039;&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, &amp;#039;&amp;#039;x&amp;#039;&amp;#039;&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;)}} by 90° is a norm-coercive mapping which fails to be a coercive vector field since &amp;lt;math&amp;gt;f(x) \cdot x = 0&amp;lt;/math&amp;gt; for every &amp;lt;math&amp;gt;x \in \mathbb{R}^2&amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
==Coercive operators and forms==&lt;br /&gt;
A [[self-adjoint operator]] &amp;lt;math&amp;gt;A:H\to H,&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt;H&amp;lt;/math&amp;gt; is a real [[Hilbert space]], is called &amp;#039;&amp;#039;&amp;#039;coercive&amp;#039;&amp;#039;&amp;#039; if there exists a constant &amp;lt;math&amp;gt;c&amp;gt;0&amp;lt;/math&amp;gt; such that&lt;br /&gt;
&amp;lt;math display=&amp;quot;block&amp;quot;&amp;gt;\langle Ax, x\rangle \ge c\|x\|^2&amp;lt;/math&amp;gt;&lt;br /&gt;
for all &amp;lt;math&amp;gt;x&amp;lt;/math&amp;gt; in &amp;lt;math&amp;gt;H.&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
A [[bilinear form]] &amp;lt;math&amp;gt;a:H\times H\to \mathbb R&amp;lt;/math&amp;gt; is called &amp;#039;&amp;#039;&amp;#039;coercive&amp;#039;&amp;#039;&amp;#039; if there exists a constant &amp;lt;math&amp;gt;c&amp;gt;0&amp;lt;/math&amp;gt; such that&lt;br /&gt;
&amp;lt;math display=&amp;quot;block&amp;quot;&amp;gt;a(x, x)\ge c\|x\|^2&amp;lt;/math&amp;gt;&lt;br /&gt;
for all &amp;lt;math&amp;gt;x&amp;lt;/math&amp;gt; in &amp;lt;math&amp;gt;H.&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
It follows from the [[Riesz representation theorem]] that any symmetric (defined as &amp;lt;math&amp;gt;a(x, y)=a(y, x)&amp;lt;/math&amp;gt; for all &amp;lt;math&amp;gt;x, y&amp;lt;/math&amp;gt; in &amp;lt;math&amp;gt;H&amp;lt;/math&amp;gt;), continuous (&amp;lt;math&amp;gt;|a(x, y)|\le k\|x\|\,\|y\|&amp;lt;/math&amp;gt; for all &amp;lt;math&amp;gt;x, y&amp;lt;/math&amp;gt; in &amp;lt;math&amp;gt;H&amp;lt;/math&amp;gt; and some constant &amp;lt;math&amp;gt;k&amp;gt;0&amp;lt;/math&amp;gt;) and coercive bilinear form &amp;lt;math&amp;gt;a&amp;lt;/math&amp;gt; has the representation&lt;br /&gt;
&amp;lt;math display=&amp;quot;block&amp;quot;&amp;gt;a(x, y)=\langle Ax, y\rangle&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
for some self-adjoint operator &amp;lt;math&amp;gt;A:H\to H,&amp;lt;/math&amp;gt; which then turns out to be a coercive operator. Also, given a coercive self-adjoint operator &amp;lt;math&amp;gt;A,&amp;lt;/math&amp;gt; the bilinear form &amp;lt;math&amp;gt;a&amp;lt;/math&amp;gt; defined as above is coercive.&lt;br /&gt;
&lt;br /&gt;
If &amp;lt;math&amp;gt;A:H\to H&amp;lt;/math&amp;gt; is a coercive operator then it is a coercive mapping (in the sense of coercivity of a vector field, where one has to replace the dot product with the more general inner product). Indeed, &amp;lt;math&amp;gt;\langle Ax, x\rangle \ge C\|x\|&amp;lt;/math&amp;gt; for big &amp;lt;math&amp;gt;\|x\|&amp;lt;/math&amp;gt; (if &amp;lt;math&amp;gt;\|x\|&amp;lt;/math&amp;gt; is bounded, then it readily follows); then replacing &amp;lt;math&amp;gt;x&amp;lt;/math&amp;gt; by &amp;lt;math&amp;gt;x\|x\|^{-2}&amp;lt;/math&amp;gt; we get that &amp;lt;math&amp;gt;A&amp;lt;/math&amp;gt; is a coercive operator.&lt;br /&gt;
One can also show that the converse holds true if &amp;lt;math&amp;gt;A&amp;lt;/math&amp;gt; is self-adjoint. The definitions of coercivity for vector fields, operators, and bilinear forms are closely related and compatible.&lt;br /&gt;
&lt;br /&gt;
==Norm-coercive mappings==&lt;br /&gt;
A mapping &amp;lt;math&amp;gt;f : X \to X&amp;#039; &amp;lt;/math&amp;gt; between two normed vector spaces &amp;lt;math&amp;gt;(X, \| \cdot \|)&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;(X&amp;#039;, \| \cdot \|&amp;#039;)&amp;lt;/math&amp;gt; is called &amp;#039;&amp;#039;&amp;#039;norm-coercive&amp;#039;&amp;#039;&amp;#039; if and only if&lt;br /&gt;
&amp;lt;math display=&amp;quot;block&amp;quot;&amp;gt; \|f(x)\|&amp;#039; \to + \infty \mbox{ as } \|x\| \to +\infty .&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
More generally, a function &amp;lt;math&amp;gt;f : X \to X&amp;#039; &amp;lt;/math&amp;gt; between two [[topological space]]s &amp;lt;math&amp;gt;X&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;X&amp;#039;&amp;lt;/math&amp;gt; is called &amp;#039;&amp;#039;&amp;#039;coercive&amp;#039;&amp;#039;&amp;#039; if for every [[compact space|compact subset]] &amp;lt;math&amp;gt;K&amp;#039;&amp;lt;/math&amp;gt; of &amp;lt;math&amp;gt;X&amp;#039;&amp;lt;/math&amp;gt; there exists a compact subset &amp;lt;math&amp;gt;K&amp;lt;/math&amp;gt; of &amp;lt;math&amp;gt;X&amp;lt;/math&amp;gt; such that&lt;br /&gt;
&amp;lt;math display=&amp;quot;block&amp;quot;&amp;gt;f (X \setminus K) \subseteq X&amp;#039; \setminus K&amp;#039;.&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The [[function composition|composition]] of a [[bijection|bijective]] [[proper map]] followed by a coercive map is coercive.&lt;br /&gt;
&lt;br /&gt;
==(Extended valued) coercive functions==&lt;br /&gt;
An (extended valued) function &amp;lt;math&amp;gt;f: \mathbb{R}^n \to \mathbb{R} \cup \{- \infty, + \infty\}&amp;lt;/math&amp;gt; is called &amp;#039;&amp;#039;&amp;#039;coercive&amp;#039;&amp;#039;&amp;#039; if&lt;br /&gt;
&amp;lt;math display=&amp;quot;block&amp;quot;&amp;gt; f(x) \to + \infty \mbox{ as } \| x \| \to + \infty.&amp;lt;/math&amp;gt;&lt;br /&gt;
A real valued coercive function &amp;lt;math&amp;gt;f:\mathbb{R}^n \to \mathbb{R} &amp;lt;/math&amp;gt; is, in particular, norm-coercive. However, a norm-coercive function &amp;lt;math&amp;gt;f:\mathbb{R}^n \to \mathbb{R} &amp;lt;/math&amp;gt; is not necessarily coercive.&lt;br /&gt;
For instance, the identity function on &amp;lt;math&amp;gt; \mathbb{R} &amp;lt;/math&amp;gt; is norm-coercive but not coercive.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
* [[Radially unbounded function]]s&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
* {{cite book|author1=Renardy, Michael  |author2=Rogers, Robert C. | title=An introduction to partial differential equations | edition=Second | publisher=Springer-Verlag | location=New York, NY | year=2004 | pages=xiv+434 | isbn=0-387-00444-0 }}&lt;br /&gt;
* {{cite book&lt;br /&gt;
 | last       = Bashirov&lt;br /&gt;
 | first      = Agamirza E&lt;br /&gt;
 | title      = Partially observable linear systems under dependent noises&lt;br /&gt;
 | publisher  = Basel; Boston: Birkhäuser Verlag&lt;br /&gt;
 | year       = 2003&lt;br /&gt;
 | pages      = &lt;br /&gt;
 | isbn       = 0-8176-6999-X&lt;br /&gt;
}}&lt;br /&gt;
*{{cite book&lt;br /&gt;
 | author2-link=Neil Trudinger&lt;br /&gt;
 | first1=D.&lt;br /&gt;
 | last1=Gilbarg&lt;br /&gt;
 | first2=N.&lt;br /&gt;
 | last2=Trudinger&lt;br /&gt;
 | title      = Elliptic partial differential equations of second order, 2nd ed&lt;br /&gt;
 | publisher  = Berlin; New York: Springer&lt;br /&gt;
 | year       = 2001&lt;br /&gt;
 | pages      = &lt;br /&gt;
 | isbn       = 3-540-41160-7&lt;br /&gt;
}}&lt;br /&gt;
&lt;br /&gt;
{{PlanetMath attribution|id=7154|title=Coercive Function}}&lt;br /&gt;
&lt;br /&gt;
[[Category:Functional analysis]]&lt;br /&gt;
[[Category:General topology]]&lt;br /&gt;
[[Category:Types of functions]]&lt;/div&gt;</summary>
		<author><name>imported&gt;MichaelMaggs</name></author>
	</entry>
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