Journal of Applied Mathematics

Volume 2012, Article ID 969685, 10 pages

http://dx.doi.org/10.1155/2012/969685

## Some Notes on the Poincaré-Bertrand Formula

Department of Mathematics, Izmir University of Economics, 35330 Izmir, Turkey

Received 18 February 2012; Revised 25 February 2012; Accepted 27 February 2012

Academic Editor: Renat Zhdanov

Copyright © 2012 Baruch Schneider. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

#### Abstract

The aim of this present paper is to establish the Poincaré-Bertrand formula for the double-layer potential on piecewise Lyapunov curve of integration.

#### 1. Introduction

For repeated singular integrals, the celebrated Poincaré-Bertrand formula of Hardy [1] and Poincaré [2] plays a fundamentally important role in the theory of one-dimensional singular integral equations: where is a smooth curve in , is a fixed point on , and lies on some appropriate function space.

There have been different extensions of this Poincaré-Bertrand formula for problems with different backgrounds. For example, Mitelman and Shapiro [3] established a Poincaré-Bertrand formula for quaternion singular integrals of Cauchy type over a smooth Lyapunov surface, Kytmanov [4] has an extension for the Bochner-Martinelli integral over a smooth manifolds.

Generalizations of the Poincaré-Bertrand theorem has been the subject of research in a number of papers (see [5, 6]). Important applications of the Poincaré-Bertrand theorem to nuclear physics, transport theory, condensed matter physics have been established by Davies et al. [6, 7].

Another important extension has been achieved by Hang and Jiang [8] on a smooth hypersurfaces in higher dimensions and for more recent references under different contexts, see for instance [9–14].

The Poincaré-Bertrand formula concerning two repeated integral operators of the double-layer potential on a piecewise Lyapunov curve in the plane is not generally known. Indeed, the author has been unable to find any explicit reference to such a result at all.

In this paper, we obtain the Poincaré-Bertrand formula for the double layer potential on a piecewise Lyapunov curve in the plane.

#### 2. Preliminary Material

In this section, we provide some well-known facts from classical complex analysis to be used in this paper. For more information, we refer the reader to [15, 16].

##### 2.1. The Cauchy-Type Integrals

We will denote by a closed curve in the complex plane which contains a finite number of conical points. If the complement (in ) of the union of conical points is a Lyapunov curve, then we shall refer to as piecewise Lyapunov curve in . Suppose that a domain with boundary is given in the complex plane . Let and be, respectively, the interior and exterior domains bounded by . Suppose that is a continuous complex-valued function on .

The Cauchy-type integral of will be denoted by and defined by We now define the singular Cauchy-type integral of as We say that is of Hölder class with exponent , denoted by , where , if there exist a constant such that

The following theorem gives the classical Sokhotski-Plemelj formulae.

Theorem 2.1 (see [16]). *Let be a bounded domain in with a piecewise Lyapunov boundary, and let , . Then the following limits exist:
**
and moreover, the following equalities hold:
**
here,
**
is the modified Cauchy singular integral, and is the angle between the one-sided tangents at point .*

As was proved in Privalov’s book, page 199 [17] and in the article by Alekseev [18] and also in [19], the limit values of the Cauchy-type integral satisfy a Hölder condition. Thus, we have that the modified singular integral operator in (2.7) acting invariantly on , and we have where is the identity operator.

Adding equalities (2.5) and (2.6), and subtracting them from each other, we arrive at the formulas:

Theorem 2.2 (follows from Lemma 4.3 of [10]). *Let be a piecewise Lyapunov curve. If , then
*

In two repeated Cauchy’s principal integrals over piecewise Lyapunov curves, the order of integration can be changed according to the following Poincaré-Bertrand formula (see, e.g., [12]) for all : where the integrals being understood in the sense of the Cauchy principal value, is the angle between the one-sided tangents at the point , and lies on some appropriate function space. Noting that we find that the formula (2.11) can be presented in the form: where .

*Remark 2.3 (2.6). *It is possible, and indeed desirable, to consider the analogous formulas in other spaces than the Hölder space, for example, the Banach space . If , , then the Sokhotski-Plemelj formulas and the Poincaré-Bertrand formula are valid almost everywhere on .

*Remark 2.4 (2.7). *Another class of interesting examples is rectifiable curves. The class of rectifiable curves includes as proper subclasses many other important classes of curves, in particular, smooth (Lyapunov) curves, piecewise Lyapunov curves, and Lipschitz curves. Various properties and applications of the Cauchy type integral for hyperholomorphic functions along rectifiable curves (and domains with rectifiable boundary) can be found, for instance, in [20].

Our purpose is to study the Poincaré-Bertrand formula associated with double-layer potential for piecewise Lyapunov curve. Before introducing the main results, we need a few standard facts from potential theory. For a detailed exposition, we refer the reader to for example, [15, 21].

##### 2.2. Simple and Double Potentials

Suppose that is a continuous function, and we refer to the functions and , given by the formulae: as the simple- and double-layer potentials, respectively. Here denotes partial differentiation with respect to the outward directed normal unit vector to the curve at a point , and denotes arc-length on . Clearly, the simple-layer potential and double layer potential are holomorphic in the interior of for any integrable .

Another option (see, e.g., [16]) is to use the simple layer potential of the form: where is a unit tangent vector.

For define

#### 3. Elementary Observations

It is easy to verify that if is real-valued then where We have already noted that for real-valued function we have where the complex conjugation, denoted by .

Thus, for , real we have Then, we may write

#### 4. Main Results

This section is devoted to the main results of the paper.

Theorem 4.1 (Sokhotski-Plemelj Formulas). *Let be a piecewise Lyapunov curve and a complex-valued function defined on which belongs to , . Then the following limits exist:
**
and moreover, the Sokhotski-Plemelj formulas hold:
**
where
**
is the modified singular double layer potential, and is the angle between the one-sided tangents at point , and the integral exists as an improper integral.*

*Proof. *For a function with , real-valued, we can write:
Note that is the real part of , and is the real part of . Now the conclusion follows directly from Section 2 and the Sokhotski-Plemelj formulas (2.5) and (2.6).

Suppose that density in (2.2) is real-valued and belongs to . By formula (2.13) we have for each :

Multiplying both sides of (2.10) by , integrating over with respect to and separate complex coordinates, the following equalities can be easily obtained:

Assume that a function depends on only, then using (4.5)–(4.9) we have

Now, in terms of double layer potential and simple-layer potential we can easily represent the very important properties:

*Remark 4.2. *When is a smooth Lyapunov curve, the properties (4.9) coincide with properties given in [22, Section 4.1.].

The proof of following lemma is straightforward.

Lemma 4.3. *Assume that is a piecewise Lyapunov curve. Then for *

Thus, we remark also that (4.7) implies that The following theorem is provided by using (4.11). Its proof is virtually identical to that of [10, Theorem 4.4], and is omitted.

Theorem 4.4. *Let be a piecewise Lyapunov curve. Then for :
**
If we now take a -valued function as (see Section 3), then comparing Theorem 4.4 and formula (4.5) we have one of our main results, analog of the Poincaré-Bertrand formula for double layer potential.*

Theorem 4.5 (Poincaré-Bertrand formula). * Let be a bounded domain in with piecewise Lyapunov curve. Assume that . Then for all :
**
where the integrals exist in the sense of the Cauchy principal value.*

An easy consequence of Theorem 4.5 is the following corollary.

Corollary 4.6. *Let be a bounded domain in with piecewise Lyapunov curve. Suppose that , . Then for all :
*

* Proof. *Suppose that , , then by using formula (4.10) we obtain (4.14).

Note that in the previous theorems, we assumed that was a bounded region in . Let now and we consider a function on , of the class . So, we have to understand as the Lebesgue integral. In fact, the proof of the Poincaré-Bertrand formula is essentially local, and is valid almost everywhere. Thus, the following theorems hold.

Theorem 4.7. *If , , then, for almost all :
**
where the integrals exist in the sense of the Cauchy principal value.*

Corollary 4.8. *Suppose that , . Then for almost all :
*

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