I. Introduction
As a natural domain decomposition method (DDM), discontinuous Galerkin (DG) method is extensively utilized in modeling complex electromagnetic problems due to its various valuable features such as the capability of irregular geometry modeling, the domain decomposition ability and flexibility in choosing the type and the order of basis functions [1][2], etc. However, in the conventional Maxwell’s equation-based DG (ME-DG) method, both Eand H-field need to be solved in the entire computational domain, which renders a great challenge to the computational performance.