The authors present a new complexification scheme for solving the Helmholtz equation with Dirichlet boundary conditions in compactly perturbed half-spaces in two and three dimensions. The key idea is to exploit the analytic continuation properties of the double layer potential kernel to show that the solution to the boundary integral equation itself admits an analytic continuation into specific regions of the complex plane.
The authors prove that for incident data that are analytic and satisfy a precise asymptotic estimate, the solution to the boundary integral equation can be uniquely extended to the complex plane. This class of data includes both plane waves and fields induced by point sources. The authors then show that by carefully choosing a contour deformation, the oscillatory integrals can be converted to exponentially decaying integrals, effectively reducing the infinite domain to a domain of finite size.
This approach is different from existing methods that use complex coordinate transformations, such as perfectly matched layers or absorbing regions. In the proposed method, the authors are still solving a boundary integral equation, but on a truncated, complexified version of the original boundary. No volumetric/domain modifications are introduced. The scheme can be extended to other boundary conditions, open waveguides, and layered media.
The authors provide a rigorous analysis of the well-posedness and invertibility of the complexified integral equation, as well as numerical examples in two and three dimensions demonstrating the performance of the scheme.
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