I. Introduction
Currently, there exists great interest in developing state-of-the-art numerical techniques for efficient simulation of multiscale electromagnetic problems involving electrically large and/or geometrically complex objects. Domain decomposition technique is an efficient way of handling problems of this type, and, over the last decade, a number of domain decomposition schemes have been proposed in the area of electromagnetics [1]–[8]. The characteristic basis function method (CBFM), which has been initially introduced in the context of method of moments (MoM) [9], is a relatively new domain decomposition approach for solving large-scale electromagnetic problems that utilizes high-level basis functions, called the characteristic basis functions (CBFs). In this approach, the CBFs are generated for each subdomain by considering the physics of the problem. They are used to transform the original matrix into a “smaller” one, called the reduced matrix. Another CBF-based approach has been utilized for the first time in FEM, and has been named characteristic basis finite-element method (CBFEM). This method, whose details of its implementation are considerably different from those followed in the previous MoM-based approaches, has been applied to a number of representative problems in both the quasi-static [10] and time-harmonic regimes [11], [12]. The CBFs have been generated in the above works by using point charges and dipole-type sources, for quasi-static and time-harmonic problems, respectively. Recently, another type of CBFEM has been proposed by using the principles of physical optics (PO) for the generation of the CBFs [13].