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Planewave pr - #3
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Solve for the scattered field directly when a Boundaries.PlaneWave source is present: the incident field enters through the PEC boundary condition n x E_s = -n x E_inc and through volume contrast sources in dielectric (lossless or lossy) regions, while the absorbing boundary condition is homogeneous. Add far-field postprocessing of the scattered field with a farfield-rcs.csv table and Monostatic backscatter rows, a Bayliss-Turkel curvature term (Absorbing.Radius) for spherical or circular boundaries, and a 2D equivalence-principle line-integral far-field transform reporting the scattering width. Bump the configuration schema to 2-2-0. Part of awslabs#690.
Add PEC sphere, lossy Debye sphere and 2D PEC cylinder examples, each comparing the computed RCS or scattering width with the analytic Mie series, with mesh generation scripts, configuration files and documentation pages. Part of awslabs#690.
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