Abstract
The waveguide tee junction differs from its wye counterpart in that its scattering matrix contains four instead of two parameters. Its symmetry may be recovered by either introducing a septum or a dielectric post along its symmetry plane. This chapter develops this problem as a preamble to constructing the two circulation conditions of the device. The eigenvalue problem of the H ‐plane tee junction is complicated because two if its three eigenvectors are not unique. The main task of the chapter is to construct the eigenvalue diagram of the H ‐plane tee junction at the Dicke plane. The chapter summarizes the boundary conditions of the electrically symmetric H ‐plane tee junction proposed by Altman. The waveguide tee junction has a symmetry plane across its side waveguide. It may be loaded with either a septum or a dielectric post resonator in order to recover the electrical symmetry of a wye junction.
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