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		<title>en&gt;Yobot: WP:CHECKWIKI error fixes using AWB (9494)</title>
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		<updated>2013-09-26T05:16:39Z</updated>

		<summary type="html">&lt;p&gt;&lt;a href=&quot;/w/index.php?title=WP:CHECKWIKI&amp;amp;action=edit&amp;amp;redlink=1&quot; class=&quot;new&quot; title=&quot;WP:CHECKWIKI (page does not exist)&quot;&gt;WP:CHECKWIKI&lt;/a&gt; error fixes using &lt;a href=&quot;/w/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; (9494)&lt;/p&gt;
&lt;p&gt;&lt;b&gt;New page&lt;/b&gt;&lt;/p&gt;&lt;div&gt;{{no footnotes|date=April 2013}}&lt;br /&gt;
In mathematics, &amp;#039;&amp;#039;&amp;#039;nonlinear realization&amp;#039;&amp;#039;&amp;#039; of a [[Lie group]] &amp;lt;math&amp;gt;G&amp;lt;/math&amp;gt; possessing a [[Cartan subgroup]]  &amp;lt;math&amp;gt;H&amp;lt;/math&amp;gt; is a particular [[induced representation]] of &amp;lt;math&amp;gt;G&amp;lt;/math&amp;gt;. In fact it is a representation of a [[Lie algebra]] &amp;lt;math&amp;gt;\mathfrak g&amp;lt;/math&amp;gt; of &amp;lt;math&amp;gt;G&amp;lt;/math&amp;gt; in a neighborhood of its origin.&lt;br /&gt;
&lt;br /&gt;
A nonlinear realization technique is part and parcel of many [[Field theory (physics)|field theories]] with [[spontaneous symmetry breaking]], e.g., [[nonlinear sigma model]], [[chiral symmetry breaking]], [[Goldstone boson]] theory, [[Higgs field (classical)|classical Higgs field theory]], [[gauge gravitation theory]] and [[supergravity]].&lt;br /&gt;
&lt;br /&gt;
Let &amp;lt;math&amp;gt;G&amp;lt;/math&amp;gt; be a Lie group and &amp;lt;math&amp;gt;H&amp;lt;/math&amp;gt; its Cartan subgroup which admits a linear representation in a vector space &amp;lt;math&amp;gt;V&amp;lt;/math&amp;gt;. A Lie&lt;br /&gt;
algebra &amp;lt;math&amp;gt;\mathfrak g&amp;lt;/math&amp;gt; of &amp;lt;math&amp;gt;G&amp;lt;/math&amp;gt; is split into the sum &amp;lt;math&amp;gt;\mathfrak g=\mathfrak h +\mathfrak f&amp;lt;/math&amp;gt; of the [[Cartan subalgebra]] &amp;lt;math&amp;gt;\mathfrak h&amp;lt;/math&amp;gt;  of &amp;lt;math&amp;gt;H&amp;lt;/math&amp;gt; and its supplement &amp;lt;math&amp;gt;\mathfrak f&amp;lt;/math&amp;gt; so that&lt;br /&gt;
&lt;br /&gt;
:  &amp;lt;math&amp;gt; [\mathfrak f,\mathfrak f]\subset \mathfrak h, \qquad [\mathfrak f,\mathfrak h&lt;br /&gt;
]\subset \mathfrak f. &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
There exists an open neighbourhood &amp;lt;math&amp;gt; U&amp;lt;/math&amp;gt; of the unit of &amp;lt;math&amp;gt; G&amp;lt;/math&amp;gt;  such&lt;br /&gt;
that any element &amp;lt;math&amp;gt; g\in U&amp;lt;/math&amp;gt;  is uniquely brought into the form&lt;br /&gt;
&lt;br /&gt;
: &amp;lt;math&amp;gt; g=\exp(F)\exp(I), \qquad F\in\mathfrak f, \qquad I\in\mathfrak h. &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Let &amp;lt;math&amp;gt;U_G&amp;lt;/math&amp;gt; be an open neighborhood of the unit of &amp;lt;math&amp;gt;G&amp;lt;/math&amp;gt; such that&lt;br /&gt;
&amp;lt;math&amp;gt;U_G^2\subset U&amp;lt;/math&amp;gt;, and let &amp;lt;math&amp;gt;U_0&amp;lt;/math&amp;gt; be an open neighborhood of the&lt;br /&gt;
&amp;lt;math&amp;gt;H&amp;lt;/math&amp;gt;-invariant center &amp;lt;math&amp;gt;\sigma_0&amp;lt;/math&amp;gt; of the quotient &amp;lt;math&amp;gt;G/H&amp;lt;/math&amp;gt; which consists of elements&lt;br /&gt;
&lt;br /&gt;
: &amp;lt;math&amp;gt;\sigma=g\sigma_0=\exp(F)\sigma_0, \qquad g\in U_G. &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Then there is a local section &amp;lt;math&amp;gt;s(g\sigma_0)=\exp(F) &amp;lt;/math&amp;gt; of &amp;lt;math&amp;gt;G\to G/H&amp;lt;/math&amp;gt;&lt;br /&gt;
over &amp;lt;math&amp;gt;U_0&amp;lt;/math&amp;gt;. With this local section, one can define the [[induced representation]], called the &amp;#039;&amp;#039;&amp;#039;nonlinear realization&amp;#039;&amp;#039;&amp;#039;, of elements &amp;lt;math&amp;gt;g\in U_G\subset G&amp;lt;/math&amp;gt; on &amp;lt;math&amp;gt;U_0\times V&amp;lt;/math&amp;gt; given by the expressions&lt;br /&gt;
&lt;br /&gt;
: &amp;lt;math&amp;gt; g\exp(F)=\exp(F&amp;#039;)\exp(I&amp;#039;), \qquad g:(\exp(F)\sigma_0,v)\to (\exp(F&amp;#039;)\sigma_0,\exp(I&amp;#039;)v). &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The corresponding nonlinear realization of a Lie algebra&lt;br /&gt;
&amp;lt;math&amp;gt;\mathfrak g&amp;lt;/math&amp;gt; of &amp;lt;math&amp;gt;G&amp;lt;/math&amp;gt; takes the following form.&lt;br /&gt;
Let &amp;lt;math&amp;gt;\{F_\alpha\}&amp;lt;/math&amp;gt;, &amp;lt;math&amp;gt;\{I_a\}&amp;lt;/math&amp;gt; be the bases for &amp;lt;math&amp;gt;\mathfrak f&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;\mathfrak h&amp;lt;/math&amp;gt;, respectively, together with the commutation relations&lt;br /&gt;
&lt;br /&gt;
: &amp;lt;math&amp;gt; [I_a,I_b]= c^d_{ab}I_d, \qquad [F_\alpha,F_\beta]= c^d_{\alpha\beta}I_d,&lt;br /&gt;
\qquad [F_\alpha,I_b]= c^\beta_{\alpha b}F_\beta. &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Then a desired nonlinear realization of &amp;lt;math&amp;gt;\mathfrak g&amp;lt;/math&amp;gt;  in &amp;lt;math&amp;gt;\mathfrak f\times V&amp;lt;/math&amp;gt;  reads&lt;br /&gt;
&lt;br /&gt;
: &amp;lt;math&amp;gt;F_\alpha: (\sigma^\gamma F_\gamma,v)\to (F_\alpha(\sigma^\gamma)F_\gamma, &lt;br /&gt;
F_\alpha(v)), \qquad  I_a: (\sigma^\gamma F_\gamma,v)\to  (I_a(\sigma^\gamma)F_\gamma,I_av), &amp;lt;/math&amp;gt;,&lt;br /&gt;
&lt;br /&gt;
:  &amp;lt;math&amp;gt;F_\alpha(\sigma^\gamma)=&lt;br /&gt;
\delta^\gamma_\alpha +&lt;br /&gt;
\frac{1}{12}(c^\beta_{\alpha\mu}c^\gamma_{\beta\nu} - 3 c^b_{\alpha\mu}c^\gamma_{\nu&lt;br /&gt;
b})\sigma^\mu\sigma^\nu, \qquad I_a(\sigma^\gamma)=c^\gamma_{a\nu}\sigma^\nu, &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
up to the second order in  &amp;lt;math&amp;gt;\sigma^\alpha&amp;lt;/math&amp;gt;. In physical models, the coefficients &amp;lt;math&amp;gt;\sigma^\alpha&amp;lt;/math&amp;gt; are treated as [[Goldstone boson|Goldstone fields]]. Similarly, nonlinear realization of [[Lie superalgebra]]s  is comsidered.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
*[[Induced representation]]&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
* Coleman S., Wess J., Zumino B., Structure of phenomenological Lagrangians, I, II, &amp;#039;&amp;#039;Phys. Rev.&amp;#039;&amp;#039; &amp;#039;&amp;#039;&amp;#039;177&amp;#039;&amp;#039;&amp;#039; (1969) 2239.&lt;br /&gt;
* Joseph A., Solomon A., Global and infinitesimal nonlinear chiral transformations, &amp;#039;&amp;#039;J. Math. Phys.&amp;#039;&amp;#039; &amp;#039;&amp;#039;&amp;#039;11&amp;#039;&amp;#039;&amp;#039; (1970) 748.&lt;br /&gt;
* Giachetta G., Mangiarotti L., [[Gennadi Sardanashvily|Sardanashvily G.]], &amp;#039;&amp;#039;Advanced Classical Field Theory&amp;#039;&amp;#039;, World Scientific, 2009, ISBN 978-981-283-895-7.&lt;br /&gt;
&lt;br /&gt;
== External links ==&lt;br /&gt;
* [[Gennadi Sardanashvily|Sardanashvily G.]], Reduction of principal superbundles, Higgs superfields, and supermetric. Appendix: Nonlinear realization, [http://xxx.lanl.gov/abs/hep-th/0609070 arXiv: hep-th/0609070].&lt;br /&gt;
&lt;br /&gt;
[[Category:Representation theory]]&lt;br /&gt;
[[Category:Theoretical physics]]&lt;/div&gt;</summary>
		<author><name>en&gt;Yobot</name></author>
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