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		<title>Liouville–Neumann series</title>
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		<summary type="html">&lt;p&gt;2001:44C8:6590:3641:A88C:E4FF:FE9A:286D: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;In [[mathematics]], the &#039;&#039;&#039;Liouville–Neumann series&#039;&#039;&#039; is a function series that results from applying the [[resolvent formalism]] to solve [[Fredholm integral equation]]s in [[Fredholm theory]].&lt;br /&gt;
&lt;br /&gt;
==Definition==&lt;br /&gt;
The Liouville–Neumann series is defined as&lt;br /&gt;
:&amp;lt;math&amp;gt;\phi\left(x\right) = \sum^\infty_{n=0} \lambda^n \phi_n \left(x\right)&amp;lt;/math&amp;gt;&lt;br /&gt;
which, provided that &amp;lt;math&amp;gt;\lambda&amp;lt;/math&amp;gt; is small enough so that the series converges, is the unique [[continuous function|continuous]] solution of the [[Fredholm integral equation]] of the second kind,&lt;br /&gt;
&lt;br /&gt;
{{Equation box 1&lt;br /&gt;
|indent =:&lt;br /&gt;
|equation =  &amp;lt;math&amp;gt;f(x)= \phi(x) - \lambda \int_a^bK(x,s)\phi(s)\,ds.&amp;lt;/math&amp;gt;&lt;br /&gt;
|cellpadding= 6&lt;br /&gt;
|border&lt;br /&gt;
|border colour = #0073CF&lt;br /&gt;
|bgcolor=#F9FFF7}}&lt;br /&gt;
&lt;br /&gt;
If the &#039;&#039;n&#039;&#039;th iterated [[Kernel (integral operator)|kernel]] is defined as &#039;&#039;n&#039;&#039;−1 nested integrals of &#039;&#039;n&#039;&#039; operator kernels {{mvar|K}},&lt;br /&gt;
:&amp;lt;math&amp;gt;K_n\left(x,z\right) = \int\int\cdots\int K\left(x,y_1\right)K\left(y_1,y_2\right) \cdots K\left(y_{n-1}, z\right) dy_1 dy_2 \cdots dy_{n-1}&amp;lt;/math&amp;gt;&lt;br /&gt;
then&lt;br /&gt;
:&amp;lt;math&amp;gt;\phi_n\left(x\right) = \int K_n\left(x,z\right)f\left(z\right)dz&amp;lt;/math&amp;gt;&lt;br /&gt;
with&lt;br /&gt;
:&amp;lt;math&amp;gt;\phi_0\left(x\right) = f\left(x\right)~,&amp;lt;/math&amp;gt;&lt;br /&gt;
so &#039;&#039;K&#039;&#039;&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;  may be taken to be {{math|&#039;&#039;δ&#039;&#039;(&#039;&#039;x−z&#039;&#039;)}}, the kernel of the [[identity operator]].&lt;br /&gt;
&lt;br /&gt;
The [[Resolvent formalism|resolvent]], also called the &amp;quot;solution kernel&amp;quot; for the integral operator, is then given by a generalization of the [[Geometric series#Generalizations beyond real and complex values|geometric series]],&lt;br /&gt;
:&amp;lt;math&amp;gt;R\left(x, z;\lambda\right) = \sum^\infty_{n=0} \lambda^n K_{n} \left(x, z\right),&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
where &#039;&#039;K&#039;&#039;&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt; is again {{math|&#039;&#039;δ&#039;&#039;(&#039;&#039;x−z&#039;&#039;)}}.&lt;br /&gt;
&lt;br /&gt;
The solution of the integral equation thus becomes simply&lt;br /&gt;
:&amp;lt;math&amp;gt;\phi\left(x\right) = \int R\left( x, z;\lambda\right) f\left(z\right)dz.&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Similar methods may be used to solve the [[Volterra integral equation]]s.&lt;br /&gt;
&lt;br /&gt;
==See also==&lt;br /&gt;
*[[Neumann series]]&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
* Mathews, Jon; Walker, Robert L. (1970), &#039;&#039;Mathematical methods of physics&#039;&#039; (2nd ed.), New York: W. A. Benjamin, {{isbn|0-8053-7002-1}}&lt;br /&gt;
* {{Citation |last=Fredholm|first=Erik I. | authorlink = Erik Ivar Fredholm |title=Sur une classe d&#039;equations fonctionnelles|journal=Acta Mathematica|date=1903|volume=27|pages=365–390 |doi=10.1007/bf02421317|url=https://zenodo.org/record/1925972|doi-access=free}}&lt;br /&gt;
&lt;br /&gt;
{{DEFAULTSORT:Liouville-Neumann Series}}&lt;br /&gt;
[[Category:Fredholm theory]]&lt;br /&gt;
[[Category:Series (mathematics)]]&lt;br /&gt;
[[Category:Mathematical physics]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{Mathanalysis-stub}}&lt;br /&gt;
{{math-physics-stub}}&lt;/div&gt;</summary>
		<author><name>2001:44C8:6590:3641:A88C:E4FF:FE9A:286D</name></author>
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