Gw. Hanson et Ab. Yakovlev, Investigation of mode interaction on planar dielectric waveguides with loss and gain, RADIO SCI, 34(6), 1999, pp. 1349-1359
On lossless isotropic planar waveguides the discrete proper modes of propag
ation form independent transverse electric and transverse magnetic sets suc
h that there is no mode coupling or interaction between modes. In the event
of material loss or gain, mode interactions are possible, leading to a com
plicated spectrum and apparent nonuniqueness of the modes. In this paper we
analyze for the first time the cause of these modal interactions by studyi
ng the simplest canonical planar waveguide which exhibits these effects, th
e symmetric-slab waveguide. We show that mode interactions are due to the m
igration of complex-frequency-plane branch points associated with specific
wave phenomena, with varying loss or gain. As these singularities move near
the real-frequency axis they influence the modal behavior for time-harmoni
c (real-valued) frequencies, crossing the real axis at some critical value
of loss or gain. It is shown that as time-harmonic frequency varies, passin
g above, below, or through these branch points results in different modal b
ehavior. Passing above or below, and near to, the branch point yields mode
coupling behavior, while passing through the branch point results in modal
degeneracy. The result of this branch point migration is that the associati
on of a particular mode with a certain branch of the dispersion function de
pends not only on the value of material loss or gain, but also on the order
in which physical parameters of the problem are varied. Three different br
anch point types are identified and discussed, which leads to an understand
ing of the relevant wave phenomena and to a method for organizing the mode
spectrum in a consistent and unique manner. While many of the observations
described here are based on careful numerical analysis of the transverse ma
gnetic modes existing on a certain symmetric-slab waveguide, the described
phenomena are reasonably expected to be generally found in other open diele
ctric waveguiding structures.