International Journal of Mathematics and Mathematical Sciences

Volume 2008, Article ID 746946, 19 pages

http://dx.doi.org/10.1155/2008/746946

## Generalized Moisil-Théodoresco Systems and Cauchy Integral Decompositions

^{1}Facultad de Informática y Matemática, Universidad de Holguín, Holguín 80100, Cuba^{2}Departamento de Matemática, Facultad de Matemática y Computación, Universidad de Oriente, Santiago de Cuba 90500, Cuba^{3}Department of Mathematical Analysis, Ghent University, 9000 Ghent, Belgium

Received 20 September 2007; Revised 13 January 2008; Accepted 17 February 2008

Academic Editor: Heinrich Begehr

Copyright © 2008 Ricardo Abreu Blaya et al. 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

Let be the space of -vectors in the Clifford algebra constructed over the quadratic vector space , let with , and , and let . Then, an -valued smooth function defined in an open subset is said to satisfy the generalized Moisil-Théodoresco system of type if in , where is the Dirac operator in . A structure theorem is proved for such functions, based on the construction of conjugate harmonic pairs. Furthermore, if is bounded with boundary , where is an Ahlfors-David regular surface, and if is a -valued Hölder continuous function on , then necessary and sufficient conditions are given under which admits on a Cauchy integral decomposition .

#### 1. Introduction

Clifford analysis, a function theory for the Dirac operator in Euclidean space (), generalizes in an elegant way the theory of holomorphic functions in the complex plane to a higher dimension and provides at the same time a refinement of the theory of harmonic functions. One of the basic properties relied upon in building up this function theory is the fact that the Dirac operator in factorizes the Laplacian through the relation . The Dirac operator is defined by , where and is an orthogonal basis for the quadratic space , the latter being the space equipped with a quadratic form of signature . By virtue of the basic multiplication rulesvalid in the universal Clifford algebra constructed over , the factorization is thus obtained.

Notice that is a real linear associative algebra of dimension , having as standard basis the set where , , , and , the identity element in .

Now let be open and let be a -function in . Then, is said to be left monogenic in if in . The equation gives rise to a first-order linear elliptic system of partial differential equations in the components of By choosing as an orthogonal basis for the quadratic space , then inside , thus generates the Clifford algebra . It is then easily seen thatwhere . If the -valued -function in is decomposed following (1.2), that is where and are -valued -functions in , then in where is the Cauchy-Riemann operator in and is the Dirac operator in .

Obviously the system (1.3) generalizes the classical Cauchy-Riemann system in the plane: it indeed suffices in the case to take -valued and -valued.

Left monogenic functions in are real analytic, whence by virtue of , they are in particular -valued and harmonic in .

As the algebra is noncommutative, one could as well consider right monogenic functions in , that is satisfies the equation in . If both and in , then is said to be two-sided monogenic in .

Notice also that through a natural linear isomorphism (see Section 2), the spaces and of smooth -valued functions and smooth differential forms in may be identified. The left and right actions of on then correspond to the actions of and on , where and denote, respectively, the exterior derivative and the coderivative operators. For the sake of completeness, let us recall the definition of and on the space of smooth -forms in , (see [1]).

For with where , , and are defined by A smooth differential form satisfying in was called in [2] a self-conjugate differential form.

It thus becomes clear that through the identifications mentioned (see again Section 2) a subsystem of (1.3) corresponds to a subsystem of self-conjugate differential forms and vice versa. For instance, for fixed, the study of left monogenic -vector valued functions thus corresponds to the study of -forms satisfying the Hodge-de Rham system and .

Let us recall that the space of -vectors in () is defined byFor an account on recent investigations on subsystems of (1.3) or, equivalently, on the study of particular systems of self-conjugate differential forms, we refer to [2–10].

Now fix , take such that and , and putThe present paper is devoted to the study of -valued smooth functions in which are left monogenic in (i.e., which satisfy in ). The space of such functions is henceforth denoted by . The system defines a subsystem of (1.3), called the generalized Moisil-Théodoresco system of type in .

To be more precise, let us first recall the definition of the differential operators and acting on smooth -valued functions in . Call the space of smooth -valued functions in and put for , Note that is -valued while is -valued and that through the isomorphism , the action of and on corresponds to, respectively, the action of and on the space .

If is written aswe then have that the generalized Moisil-Théodoresco system of type reads as follows (see also Section 2):Note that for and fixed, the system (1.9) reduces to the generalized Riesz system Its solutions are called harmonic multivector fields (see also [11]). We haveFurthermore, for , and fixed, the system (1.9) reduces to the Moisil-Théodoreco system in (see, e.g., [3]):In the particular case, where , and , the original Moisil-Théodoresco system introduced in [12] is reobtained (see also [4]).

In this paper, two problems are dealt with; we list them as follows.

(i)To characterize the structure of solutions to the system (1.9).

It is proved in Section 4 (see Theorem 3.2) that, under certain geometric conditions upon , each corresponds to a harmonic potential belonging to a particular subspace of the space of harmonic -valued functions in .

The proof of Theorem 3.2 relies heavily on the construction of conjugate harmonic pairs elaborated in Section 3.

(ii)To characterize those which admit a Cauchy-type integral decomposition on of the form where is the boundary of a bounded open domain in and denotes the space of -valued Hölder continuous functions of order on , . Putting , the elements and should also belong to and as such should be the boundary values of solutions and of (1.9) in and , respectively.

In Section 5, this problem is solved in terms of the Cauchy transform on , being an -dimensional Ahlfors-David regular surface (see Theorem 4.2).

In order to make the paper self-contained, we include in Section 2 some basic properties of Clifford algebras and Clifford analysis. For a general account of this function theory, we refer, for example, to the monographs [13–15].

#### 2. Clifford Analysis: Notations and Some Basic Properties

Let again be an orthogonal basis for and let be the universal Clifford algebra over . As has already been mentioned in Section 1, is a real linear associative but noncommutative algebra of dimension ; its standard basis is given by the set and the basic multiplication rules are governed by (1.1). For fixed, the space of -vectors is defined by (1.5), leading to the decompositionand the associated projection operators .

Note in particular that for , and that for , .

An element is therefore usually identified with .

For , the product splits in two parts, namely,where is the scalar part of and is the 2-vector or bivector part of . They are given by More generally, for and (), we have that the product decomposes intowhere Another useful decomposition of may be obtained by splitting it “along the -direction,” as indicated in (1.2). This in fact means that we split following and that within , the Clifford algebra is generated by the orthogonal basis of . denotes the space to which the original quadratic form of signature on has been restricted.

Following the decomposition (1.2), the element is then often identified with the so-called paravector .

Let us also recall that if is open and is an -valued -function in , then is said to be left monogenic in if in , being the Dirac operator in .

As already mentioned in (1.3), by putting , being the Dirac operator in , we have for ,Let us recall that a pair of -valued harmonic functions in is said to be conjugate harmonic if is left monogenic in (see [16]).

Notice also that, when defining the conjugate of by , we have that .

If is a subspace of , then and denote, respectively, the spaces of left monogenic and harmonic -valued functions in . As we have that .

In particular, for such that , with , we have put in Section 1 (see (1.6)), and .

Furthermore, for fixed, a natural isomorphismmay be then defined as follows.

Put for ,where for each with , and for all .

By means of the decomposition (2.1), may be extended by linearity to , thus leading to the isomorphism , where as usual .

It may be easily checked that the action of the exterior derivative and the co-derivative on then corresponds through to the left action of and on . For the definition of and (resp., and ) we refer to (1.4) and (1.7). In fact, taking into account the relations (2.5), the expressions (1.7) mean that for , Consequently, for , splits intoIt thus follows that for , the system is given by (1.9).

Obviously, for , , while for , . Finally, notice that and that hence, as mentioned in Section 1, through , the left action of on corresponds to the action of on . We thus have on that .

The following notations will also be used: Let us recall that if is contractible to a point, a refined version of the inverse Poincaré lemma then implies that are surjective operators.

For the inverse Poincaré lemma and its refined version we refer to, respectively, [1, 17]. For more information concerning the interplay between differential forms and multivectors, the reader is referred to [17, 18].

Obviously, all notions, notations, and properties introduced above may be easily adapted to the case where is the orthogonal projection of on and and are the Dirac and Laplace operators in .

#### 3. Conjugate Harmonic Pairs

Let be as in Section 1, let with , and decompose each following (1.2), that iswhere and .

Then, with Now suppose that , that is, is a conjugate harmonic pair in in the sense of [16]. Then, as already stated in (1.3),By virtue of (2.10) and (3.2), the equations in (3.3) lead to the systemsFrom (3.5) it thus follows that implies that in .

We now claim that, under certain geometric conditions upon , given , harmonic and -valued in , the condition in is sufficient to ensure the existence of a , harmonic and -valued in , which is conjugate harmonic to , that is .

In proving this statement, we will adapt where necessary the techniques worked out in [16] for constructing conjugate harmonic pairs.

Let again denote the orthogonal projection of on . Then, we suppose henceforth that satisfies the following conditions (C1) and (C2):

(C1) is normal with respect to the direction, that is, there exists such that for all , is connected and it contains the element ;(C2) is contractible to a point. The condition (C1) is sufficient for constructing harmonic conjugates to (see [16]), while the condition (C2) ensures the applicability of the inverse Poincaré lemma and its consequences in (see [17]).

As is well known, classical results of cohomology theory provide necessary and sufficient conditions for the validity of the inverse Poincaré lemma in . For convenience of the reader, we restrict ourselves to the condition (C2), thus making the inverse Poincaré lemma applicable for any closed or coclosed form in ().

Now assume that harmonic and that -valued in satisfies the condition in .

Putwhere is a smooth -valued solution in of the equationAs is surjective (see [19]), such indeed exists and any other similar solution of (3.7) has the form where .

Fix a solution of (3.7). Then by construction, the corresponding determined by (3.6) belongs to (see [16]).

We now prove that there exists such that in ,To this end, first notice that, as by assumption in , we have that in , whence .

As is surjective (see also (2.12)) there exists such that , that is, satisfies in the relationsFurthermore, put . Then, on the one hand,while on the other handConsequently, in and is -valued in .

Now define byThen by construction, and clearly in , .

Furthermore, as in , is -valued and obviously is -valued. As moreover , we get that is -valued.

Consequently, as , , that is, is a conjugate harmonic pair in .

We have thus proved the following theorem.

Theorem 3.1. *Let be open and
normal with respect to the -direction and
let be contractible
to a point. Furthermore, let be given. Then, admits a
conjugate harmonic if and only if in .*

*Remarks*

(1) If , then in , thus implying that the condition is
automatically satisfied and that in constructing , no correction term should be added
to (i.e., we may
take in
(3.12)).

(2) It is of course
tacitly understood that if , then in the expression of (see (3.2)), the
first term is taken to be
identically zero in .

(3) The systems (3.4) and (3.5) show a lot of symmetry.

The following theorem (Theorem 3.2) holds, the proof of which is omitted.

Theorem 3.2. *Let be open and
normal with respect to the -direction and
let be contractible
to a point. Furthermore, let be given. Then, admits a
conjugate harmonic if and only if in .*

#### 4. Structure Theorems

Assume that are such that and that with .

This section essentially deals with the construction of harmonic potentials corresponding to solutions of the generalized Moisil-Théodoresco system.

We start with the following lemma.

Lemma 4.1. *Let be open and
contractible to a point and let . The following properties are equivalent:*

(i)*,*(ii)*there exists such that .*

*Proof. *It is clear that if , then is -valued. As
moreover , ; whence (ii)*⇒*(i) is proved.

Conversely, assume that and put . From it follows
thatBy a refined version of the
inverse Poincaré lemma (see [17]) we obtain from the first equation in (4.1) that there
exists such that in Analogously, the third equation
in (4.1) implies the existence ofsuch that in Put . Then,and by virtue of (4.2) and (4.4), But where is -valued and
harmonic in . As is surjective
(see [19]), there
exists that such that .

Put . Then, clearly andFinally, put . Then, is -valued
andAs is obviously
harmonic in , the proof is done.

*Remarks*

(1) In the case
where and , we have that in (4.1) the equation is
automatically satisfied. Putting , take such that and define by . Then, .

In the case where , the equation is
automatically satisfied. An analogous reasoning to the one just made then leads
to an appropriate such that .

(2) Obviously, in
the case where as well as , the technique
suggested in Remark (1) then produces such that .

(3) A particularly important
example where as well as occurs when . Indeed, put for given real valued smooth functions in , ,Then, for ,Both equations in (4.10) give rise
to the same system to be satisfied by , namelyThe system (4.11) is the Fueter
system in for so-called
left regular functions of a quaternion variable; it lies at the basis of
quaternionic analysis (see [20, 21]).

We have taken this example from [2], where it was proved in the
framework of self-conjugate differential forms. We have inserted it here
because it demonstrates how quaternionic analysis can be viewed upon as part of
Clifford analysis in , namely as the theory of special solutions to a
generalized Moisil-Théodoresco system in of type .

(4) In the case
where and , Lemma 4.1 tells us that, given , there exists such that . This result was already obtained in [3, Lemma 3.1].

Theorem 4.2. *Let be open and
normal with respect to the -direction, let be contractible
to a point, and let . The following properties are equivalent:*

(i)*,*(ii)*there exists with in such that .*

*Proof. *(i)*→*(ii). Let and put,
following (1.2), . Then, the pair is conjugate
harmonic in with and .

Associate with the harmonic -valued
potential given by (3.12),
that is,where in , , and .

As moreover in (see Theorem
3.1), it thus follows from (4.12) that in . Consequently, with and .

From , it is then easily obtained that is independent
of and that in , , that is, . By virtue of Lemma 4.1, there exists such that ; whence .

Put . Then by construction,

(i),(ii),(iii);
whence (i)*→*(ii) is proved.

Conversely, let with . Then clearly .

*Remarks*

(1) Theorem 4.2 tells
us that each admits an - valued
harmonic potential in satisfying .

(2) Let , that is, we take and . Then from Theorem 4.2, it follows that the following
properties are equivalent:

(i),(ii)there
exists with such that .

This
characterization was already obtained in [3, Theorem 3.1].

#### 5. Cauchy Integral Decompositions

Let be a bounded open subset with boundary where is a rectifiable closed Jordan curve such that for some constant and this for all and , where is the closed disc with center and radius and is the 1-dimensional Hausdorff measure on . Furthermore, let and let , .

In classical complex analysis, the following jump problem (5.1) is solved by means of the Cauchy transform:

“Find a pair of functions and , holomorphic in and with , such that are continuously extendable to and that on where in (5.1), .”

Let be the Cauchy transform on , that is, for ,where is the outward pointing unit normal at and is the elementary Lebesgue measure on .

Then, the following fundamental properties hold (see, e.g., [22]):

(i) is holomorphic and of the class on with ;(ii)Plemelj-Sokhotzki formulae:where for ,define the Hilbert transform on ;(iii) on .

It thus follows that the answer to the jump problem (5.1) is indeed given by .

The decomposition (iii) thus obtained is known as the Cauchy integral decomposition of on .

Now let be a bounded and open subset of with boundary . Then, in Clifford analysis, for suitable pairs of boundaries and -valued functions on , the Cauchy transform is defined by where the following conditions hold.

(i), , is the fundamental solution of the Dirac operator , where is the area of the unit sphere in . is -valued and monogenic in .(ii) is the outward pointing unit normal at .(iii) is the -dimensional Hausdorff measure on . For the definition of , see, for example, [23, 24]. In what follows we restrict ourselves to the following conditions on the pair (see also the remarks made at the end of this section).

(C1) is an -dimensional Ahlfors-David regular surface, that is, there exists a constant such that for all and ,where is the closed ball in with center and radius and is the diameter of .For the definition of AD-regular surfaces, see, for example, [24, 25].(C2), , being the space of -valued Hölder continuous functions of order on .

Under the conditions (C1) and (C2), the following properties hold (see, e.g., [26–28]):

(i) is left monogenic in and ;(ii)(Plemelj-Sokhotzki formulae) the functions determined bybelong to , wherethe integral being taken in the sense of principal values;(iii), . It thus follows that, given a Hölder continuous -valued density on , the jump problem (5.9)

“Find and , belonging to and which are the boundary values of left monogenic functions and in, respectively, and with such that on is solved by considering the Cauchy transform . Indeed, we can take in and in .

Now let again be a triplet satisfying and with , and let .

As is -valued, it is easily seen that is -valued. Consequently, if the jump problem (5.9) is formulated in terms of -valued Hölder continuous functions , , and on , then if we wish to solve it by means of the Cauchy transform , restrictions on have to be imposed, namely, in we should have The very heart of the following theorem (Theorem 5.1) tells us that the conditions (5.10) are necessary and sufficient. Although the arguments used in proving Theorem 5.1 are similar to the ones given in the proof of [29, Theorem 4.1], for convenience of the reader we write them out in full detail.

Theorem 5.1. *Let be open and
bounded such that is an -dimensional
Ahlfors-David regular surface and let with and . The following properties are equivalent:*

(i)* admits on *