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In [[physics]] and [[applied mathematics]], '''analytical regularization''' is a technique used to convert [[boundary value problem]]s which can be written as [[Fredholm integral equation]]s of the first kind involving [[singular integral operator | singular operators]] into equivalent Fredholm integral equations of the second kind which may be easier to solve analytically and which can be studied with [[discretization]] schemes like the [[finite element method]] or the [[finite difference method]] because they are [[pointwise convergence | pointwise convergent]]. In [[computational electromagnetics]], it is known as the '''method of analytical regularization'''. It was first used in mathematics during the development of [[operator theory]] before acquiring a name.<ref name=nosich> Nosich, Alexander I. 'The Method of Analytic Regularization in Wave-Scattering and Eigenvalue Problems: Foundations and Review of Solutions' ''IEEE Antennas and Propagation Magazine''. Vol 41, No. 3. June 1999 </ref>
 
== Method ==
 
Analytical regularization proceeds as follows. First, the boundary value problem is formulated as an integral equation. Written as an operator equation, this will take the form
:<math> G X= Y </math>
with <math> Y </math> representing boundary conditions and [[Inhomogeneous differential equation | inhomogeneities]], <math> X </math> representing the field of interest, and <math> G </math> the integral operator describing how Y is given from X based on the physics of the problem. 
Next, <math> G </math> is split into  <math>G_1 + G_2</math>, where  <math>G_1</math> is invertible and contains all the singularities of <math>G </math> and <math> G_2</math> is regular. After splitting the operator and multiplying by the inverse of  <math> G_1 </math>, the equation becomes
:<math> X + G_1^{-1}  G_2 X=  G_1^{-1} Y </math>
or
:<math> X + A X =  B </math>
which is now a Fredholm equation of the second type because by construction <math> A </math> is [[compact operator | compact]] on the [[Hilbert space]] of which <math> B </math> is a member.
 
In general, several choices for <math>\mathbf{G}_1</math> will be possible for each problem.<ref name=nosich />  
 
== References ==
<references />
* Analytical regularization for confined quantum fields between parallel surfaces F C Santos et al. 2006 J. Phys. A: Math. Gen. 39 6725-6732 doi: [http://dx.doi.org/10.1088/0305-4470/39/21/S73 10.1088/0305-4470/39/21/S73.]
* [http://www.informaworld.com/smpp/content~content=a907381504~db=all~jumptype=rss Regularization of the Dirichlet Problem for Laplace's Equation: Surfaces of Revolution ] Authors: Sergey B. Panin ab; Paul D. Smith a; Elena D. Vinogradova a; Yury A. Tuchkin bc; Sergey S. Vinogradov d
*{{Citation | last1=[[Hagen Kleinert|Kleinert]]| first1=H.| last2=Schulte-Frohlinde| first2=V. | title=Critical Properties of φ<sup>4</sup>-Theories| url=http://www.worldscibooks.com/physics/4733.html|ISBN=  978-981-02-4659-4| year=2001| pages=1–474}}, Paperpack ISBN 978-981-02-4659-4 (also available [http://users.physik.fu-berlin.de/~kleinert/kleinert/?p=booklist&details=6 online]). Read Chapter 8 for Analytic Regularization.
 
== External links ==
* [http://www.circuitechs.com/electromagnatics/electromagnetics.html E-Polarized Wave Scattering from Infinitely Thin and Finitely Width Strip Systems]
* [http://www.springerlink.com/content/q6hj6637nv0815r5/ Yu. A. Tuchkin Analytical Regularization Method for Wave Diffraction by Bowl-Shaped Screen of Revolution]
 
{{DEFAULTSORT:Analytical Regularization}}
[[Category:Diffraction]]
[[Category:Electromagnetism]]

Latest revision as of 21:37, 10 January 2013

In physics and applied mathematics, analytical regularization is a technique used to convert boundary value problems which can be written as Fredholm integral equations of the first kind involving singular operators into equivalent Fredholm integral equations of the second kind which may be easier to solve analytically and which can be studied with discretization schemes like the finite element method or the finite difference method because they are pointwise convergent. In computational electromagnetics, it is known as the method of analytical regularization. It was first used in mathematics during the development of operator theory before acquiring a name.[1]

Method

Analytical regularization proceeds as follows. First, the boundary value problem is formulated as an integral equation. Written as an operator equation, this will take the form

with representing boundary conditions and inhomogeneities, representing the field of interest, and the integral operator describing how Y is given from X based on the physics of the problem. Next, is split into , where is invertible and contains all the singularities of and is regular. After splitting the operator and multiplying by the inverse of , the equation becomes

or

which is now a Fredholm equation of the second type because by construction is compact on the Hilbert space of which is a member.

In general, several choices for will be possible for each problem.[1]

References

  1. 1.0 1.1 Nosich, Alexander I. 'The Method of Analytic Regularization in Wave-Scattering and Eigenvalue Problems: Foundations and Review of Solutions' IEEE Antennas and Propagation Magazine. Vol 41, No. 3. June 1999
  • Analytical regularization for confined quantum fields between parallel surfaces F C Santos et al. 2006 J. Phys. A: Math. Gen. 39 6725-6732 doi: 10.1088/0305-4470/39/21/S73.
  • Regularization of the Dirichlet Problem for Laplace's Equation: Surfaces of Revolution Authors: Sergey B. Panin ab; Paul D. Smith a; Elena D. Vinogradova a; Yury A. Tuchkin bc; Sergey S. Vinogradov d
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