I. Introduction
It is well known that the finite-difference time-domain (FDTD) method (also called the Yee Scheme) [1] is a very popular and efficient method for numerical solutions of Maxwell's equations and applied to a broad ranges of problems in electromagnetics [2]. In FDTD the way of time marching is frog-jumping and the time step is confined to the Courant-Friedrichs-Lewy (CFL) condition [3]. To overcome this limitation, the alternating direction implicit FDTD (ADI-FDTD) methods [4], [5] were proposed by implicitly discretizing the equations and proven that the time step does not depend on the spatial increments [4]–[6]. However the time step size is limited by the errors from numerical dispersion and the accuracy of time [7]. Improvement of the time accuracy of ADI-FDTD by extrapolation can be seen in [8]. Thus, it is important to study time marching ways and methods to improve the accuracy in time.