I. Introduction
The dyadic Green's functions (DGFs) technique [1]–[3] has been widely used to characterize electromagnetic wave propagation and to solve electromagnetic boundary value problems for the last decades. The dyadic Green's function serves as a kernel of the integral and has to be defined or formulated beforehand. However, with the complexity of media growing, the dyadic Green's function representations for media also become more complicated. In recent years, due to the advances in material science and technology which have manifested fabrication of various kinds of complex materials, considerable attention has been paid to the interaction of electromagnetic waves with anisotropic materials [4]–[6], bianisotropic media [7] and chirowaveguides [8].