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 <title>Plemelj formulas</title>
 <name>PlemeljFormulas</name>
 <created>2006-06-24 01:41:25</created>
 <modified>2006-08-24 00:18:57</modified>
 <type>Definition</type>
 <creator id="2192" name="perucho"/>
 <author id="2192" name="perucho"/>
 <classification>
	<category scheme="msc" code="30D10"/>
 </classification>
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 <content>Let $\psi(\zeta)$ be a density function of a complex variable satisfying the H\"older condition (the Lipschitz condition of order $\alpha$){\footnote{A function $f(\zeta)$ satisfies the H\"older condition on a smooth curve $C$ if for every $\zeta_1,\zeta_2\in C$ $|f(\zeta_2)-f(\zeta_1)|\leq M|\zeta_2-\zeta_1|^\alpha$, $M&gt;0$, $0&lt;\alpha\leq 1$. It is clear that the H\"older condition is a weaker restriction than a bounded derivative for $f(\zeta)$.}} on a smooth closed contour $C$ in the integral
\begin{align}
\Psi(z)=\frac{1}{2\pi i}\int_C\frac{\psi(\zeta)}{\zeta-z}d\zeta,
\end{align}
then the limits $\Psi^+(t)$ and $\Psi^-(t)$ as $z$ approaches an arbitrary point $t$ on $C$ from the interior and the exterior of $C$, respectively, are
\begin{align}
\left\{ \begin{array}{ll}
\Psi^+(t) \equiv \frac{1}{2}\psi(t)+
\frac{1}{2\pi i}\int_C\frac{\psi(\zeta)}{\zeta-t}d\zeta, \\ 
\Psi^-(t) \equiv -\frac{1}{2}\psi(t)+
\frac{1}{2\pi i}\int_C\frac{\psi(\zeta)}{\zeta-t}d\zeta.
\end{array}
\right.
\end{align}
These are the Plemelj\cite{cite:Plemelj} formulas {\footnote{cf.\cite{cite:Musk}, where restrictions that Plemelj made, were relaxed.}}  and the improper integrals in (2) must be interpreted as Cauchy's principal values.
\begin{thebibliography}{99}
\bibitem{cite:Plemelj}
J. Plemelj, {\em Monatshefte f\"ur Mathematik und Physik,} vol. 19, pp. 205- 210, 1908.
\bibitem{cite:Musk}
N. I. Muskhelishvili, {\em Singular Integral Equations,} Groningen: Noordhoff (based on the second Russian edition published in 1946), 1953.
\end{thebibliography} 
	


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