1 Introduction
The electromagnetic wave field can be trapped and guided via reflections against electromagnetically impenetrable boundaries. One of the simplest guiding configurations treated in most books on introductory electromagnetics [1], [2] is the parallel-plate waveguide. It consists of two parallel perfectly electrically conducting (PEC) planes of infinite extent that confine the propagating wave field. The solution of such a problem is well known in the frequency domain, and its detailed description can be found in several books (e.g., [3, Section 5.5]). On this subject, the eigenfunction representation over the direction perpendicular to the boundaries of the planes, and the alternative hybrid ray-mode representation employing the Fourier representation parallel to them, were illustratively discussed by Felsen et al. [4].