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3. Representation Formulae, Local Coordinates
                           and Direct Boundary Integral Equations











                           In order to generalize the direct approach for the reduction of more general
                           boundary value problems to boundary integral equations than those pre-
                           sented in Chapters 1 and 2 we consider here the 2m–th order positive elliptic
                           systems with real C –coefficients. We begin by collecting all the necessary
                                             ∞
                           machinery. This includes the basic definitions and properties of classical func-
                           tion spaces and distributions, the Fourier transform and the definition of
                           Hadamard’s finite part integrals which, in fact, represent the natural regu-
                           larization of homogeneous distributions and of the hypersingular boundary
                           integral operators. For the definition of boundary integral operators one needs
                           the appropriate representation of the boundary manifold Γ involving local
                           coordinates. Moreover, the calculus of vector fields on Γ requires some basic
                           knowledge in classical differential geometry. For this purpose, a short excur-
                           sion into differential geometry is included. Once the fundamental solution
                           is available, the representation of solutions to the boundary value problems
                           is based on general Green’s formulae which are formulated in terms of dis-
                           tributions and multilayer potentials on Γ. The latter leads us to the direct
                           boundary integral equations of the first and second kind for interior and
                           exterior boundary value problems as well as for transmission problems. As
                           expected, the hypersingular integral operators are given by direct values in
                           terms of Hadamard’s finite part integrals.
                              The results obtained in this chapter will serve as examples of the class of
                           pseudodifferential operators to be considered in Chapters 6–10.



                           3.1 Classical Function Spaces and Distributions

                           For rigorous definitions of classical as well as generalized function spaces we
                           first collect some standard results and notations.
                           Multi–Index Notation
                                                                                 n
                              Let IN 0 be the set of all non–negative integers and let IN be the set of
                                                                                 0
                           all ordered n–tuples α =(α 1 , ··· ,α n ) of non–negative integers α i ∈ IN 0 .
                                                                                n
                           Such an n–tuple α is called a multi–index. For all α ∈ IN , we denote by
                                                                                0
                                                                                    n
                           |α| = α 1 +α 2 +···+α n the order of the multi-index α.If α, β ∈ IN , we define
                                                                                    0
                           α + β =(α 1 + β 1 , ··· ,α n + β n ). The notation α ≤ β means that α i ≤ β i for
                           1 ≤ i ≤ n.Weset
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