Reflect the source across the plane, defining for an interior point . Superpose the direct Green function from part (b) and an image of opposite sign:
The direct term supplies the delta source in the upper half-space; the image singularity lies outside that domain and contributes no source there. On the two distances are equal, so the terms cancel, giving homogeneous Dirichlet boundary conditions. Both decay at infinity, which is the additional condition selecting this half-space solution. This is the method of images realization of the Dirichlet image kernel for the three-dimensional modified Helmholtz equation. It includes the unscreened case .

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