I. Introduction
The perfectly matched layer (PML) introduced by Bérenger [1] is widely accepted as an efficient numerical absorber used in time-domain electromagnetic solvers. PMLs are often used to implement absorbing boundary conditions (ABCs) in the finite-difference time-domain (FDTD) [1]–[3] and finite-element frequency-domain (FEFD) [4], [5] methods for simulating open-region wave propagation problems. Recently, a PML scheme to truncate finite-element time-domain (FETD) meshes for analyzing 2-D [6] and generally for 3-D [7], [8] open-region electromagnetic scattering and radiation problems has been developed.