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The wave components of equations (16) travel
undisturbed along each axis. This propagation is implemented digitally
using bidirectional delay lines, as depicted in
Fig. 1. We call such a collection of delay lines an
-variable waveguide section. Waveguide sections are then
joined at their endpoints via scattering junctions (discussed in section IV) to form a DWN.
Figure:
An -variable waveguide section.
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