I. Introduction
Periodic structure of dispersive media has become the focus of attention in the electromagnetic field due to the special properties of materials [1]. Numerous time domain algorithms have been developed for this topic [2]–[4]. However, the finite-difference time-domain (FDTD) method may not fit the fine and complex structure. On the other hand, even though the finite-element time-domain method (FETD) shows advantage in tetrahedral meshing flexibility, it needs to solve large linear algebraic equations in each time step. In contrast, the FETD method with discontinuous Galerkin technology (DG-FETD) can not only inherit the superiority of reducing modeling errors, but also avoids the shortcoming by forming block diagonal coefficient matrix.