In mode analysis it is usually the primary goal to find a propagation constant. This quantity is often, but not always, real valued if the analysis involves some lossy part, such as a nonzero conductivity or an open boundary, the eigenvalue is complex. In such situations, the real and imaginary parts have separate interpretations: • The real part is the propagation constant • The imaginary part is the attenuation constant, measuring the damping in space

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