Abstract
Abstract In this paper, we consider a special approach to the investigation of a mixed boundary value problem (BVP) for the Laplace equation in the case of a three-dimensional bounded domain Ω ⊂ ℝ 3 {\Omega\subset\mathbb{R}^{3}} , when the boundary surface S = ∂ Ω {S=\partial\Omega} is divided into two disjoint parts S D {S_{D}} and S N {S_{N}} where the Dirichlet—Neumann-type boundary conditions are prescribed, respectively. Our approach is based on the potential method. We look for a solution to the mixed boundary value problem in the form of a linear combination of the single layer and double layer potentials with the densities supported respectively on the Dirichlet and Neumann parts of the boundary. This approach reduces the mixed BVP under consideration to a system of pseudodifferential equations. The corresponding pseudodifferential matrix operator is bounded and coercive in the appropriate L 2 {L_{2}} -based Bessel potential spaces. Consequently, the operator is invertible, which implies the unconditional unique solvability of the mixed BVP in the Sobolev space W 2 1 ( Ω ) {W^{1}_{2}(\Omega)} . Using a special structure of the obtained pseudodifferential matrix operator, it is also shown that it is invertible in the L p {L_{p}} -based Besov spaces, which under appropriate boundary data implies C α {C^{\alpha}} -Hölder continuity of the solution to the mixed BVP in the closed domain Ω ¯ {\overline{\Omega}} with α = 1 2 - ε {\alpha=\frac{1}{2}-\varepsilon} , where ε > 0 {\varepsilon>0} is an arbitrarily small number.
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