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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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