PML Implementation for ADI-FDTD in Dispersive Media

Yee K S. Numerical solution of initial boundary problems involving Maxwells equations in isotropic media. IEEE Trans on AP, 1966, 14(4): 302-307.[2]Takefumi Namiki. A new FDTD algorithm based on alternating direction implicit method[J].IEEE Trans. on MTT.1999, 47(10):2003-2007[3]Takefumi Namiki. 3D ADI-FDTD methodunconditionally stable time domain algorithm for solving full vector Maxwells equations[J].IEEE Trans. on MTT.2000, 48(10):1743-1748[4]Zheng Fenghua, Chen Zhizhang, Zhang Jiazong. Toward the development of three-dimensional unconditionally stable finite difference time domain method[J].IEEE Trans. on MTT.2000, 48(9):1550-1558[5]Wang Shumin, Teixeira F L. An efficient PML implementation for the ADI-FDTD method. IEEE MGWL, 2003, 13(2): 72-74.[6]Gedney S D, et al. Perfectly matched layer media with CFS for an[7]unconditionally stable ADI-FDTD method. IEEE Trans on AP,[8]01, 49(11): 1554-1559.[9]Liu Gang, Gedney S D. Perfectly matched layer media for an unconditionally stable three-dimensional ADI-FDTD method. IEEE MGWL, 2000, 10(7): 261-263.[10]Luebbers R. A frequency-dependent finite difference time domain formulation for dispersive materials. IEEE Trans. on EMC, 1990, 32(3): 222-227.[11]Uno T. Perfectly matched layer absorbing boundary condition for dispersive medium. IEEE MGWL, 1997, 7(9): 264-266.