[1] Yee K S.Numerical solution of initial boundary value problems involving Maxwell’s equations in isotropic media [J].IEEE Transactions on Antennas and Propagation, 1966, 14(3):302-307.
[2] Taflove A, Hagness S C.Computational electrodynamics:the finite-difference time-domain method [M].Boston:Artech House, 2000.
[3] Zheng F, Chen Z, Zhang J.Toward the development of a three-dimensional unconditionally stable finite-difference time-domain method [J].IEEE Transactions on Microwave Theory and Techniques, 2000, 48(9):1550-1558.
[4] Namiki T.3-D ADI-FDTD method—unconditionally stable time domain algorithm for solving full vector Maxwell’s equations [J].IEEE Transactions on Microwave Theory and Techniques, 2000, 48(10):1743-1748.
[5] Mur G.Absorbing boundary conditions for the finite-difference approximation of the time-domain electromagnetic field equations [J].IEEE Transactions on Electromagnetic Compatibility, 1981, 23(11):377-382.
[6] Zhou J Y, Hong W.Construction of the absorbing boundary conditions for the FDTD method with transfer functions [J].IEEE Transactions on Microwave Theory and Techniques, 1998, 46(11):1807-1809.
[7] Shao Z H, Hong W, Zhou J Y.Generalized Z-domain absorbing boundary conditions for the analysis of electromagnetic problems with finite-difference time-domain method [J].IEEE Transactions on Microwave Theory and Techniques, 2003, 51(1):82-90.
[8] Berenger J P.A perfectly matched layer for absorption of electromagnetic waves [J].J Compu Phys, 1994, 114(10):185-200.
[9] Wang S, Teixeira F L.An efficient PML implementation for the ADI-FDTD method [J].IEEE Microwave and Wireless Component Letter, 2003, 13(2):72-74.
[10] Li J, Dai J.An efficient implementation of the stretched coordinate perfectly matched layer [J].IEEE Microwave and Wireless Component Letter, 2007, 17(5):322-324.
[11] Hwang J, Chen F C.Numerical performances of absorbing boundary conditions for ADI-FDTD method [C]//IEEE Antennas and Propagation Society International Symposium.New Mexico, USA, 2006:2723-2726.