Efficient ABC for the Frequency Dependent Alternating Direction-Implicit FDTD Method

Ultra WideBand (UWB) signals have a high potential for a wide range of applications. The Finite-Difference Time-Domain (FDTD) method is widely used in the development of UWB technology but has still two main limitations. One is that material parameters are constant over the whole frequency range. Frequency dependent materials can be accommodated by adopting a Debye model. The other is that the minimum simulation time is bound by the Courant-Friedrichs-Lewy (CFL) condition, which can be solved by the application of the Alternating Direction-Implicit (ADI) scheme. The combination of Debye model and ADI scheme in FDTD results in the Frequency-Dependent (FD) ADI-FDTD method. This paper proposes an adaptation of the most effective Absorbing Boundary Condition (ABC), the Complex Frequency-Shift (CFS) Perfectly Matched Layer (PML), to FD-ADI-FDTD. The formulation of CFS-PML for FD-ADI-FDTD is proposed and its performance is assessed. The influence of the Courant Number (CFLN), the media parameters and the number of layers are investigated.

[1]  Fumie Costen,et al.  Alternative formulation of three dimensional frequency dependent ADI-FDTD method , 2004, IEICE Electron. Express.

[2]  William H. Press,et al.  Numerical Recipes: FORTRAN , 1988 .

[3]  Fumie Costen,et al.  Numerical Noise Introduced by the Alternating Direction-Implicit Scheme in FDTD for UWB Systems , 2006, Int. J. Wirel. Opt. Commun..

[4]  Fenghua Zhen,et al.  Toward the development of a three-dimensional unconditionally stable finite-difference time-domain method , 2000 .

[5]  Jean-Pierre Berenger,et al.  A perfectly matched layer for the absorption of electromagnetic waves , 1994 .

[6]  A. Cangellaris,et al.  A stretched coordinate technique for numerical absorption of evanescent and propagating waves in planar waveguiding structures , 1995, Proceedings of 1995 IEEE MTT-S International Microwave Symposium.

[7]  Raj Mittra,et al.  Frequency dependence of the constitutive parameters of causal perfectly matched anisotropic absorbers , 1996 .

[8]  T. Namiki,et al.  A new FDTD algorithm based on alternating-direction implicit method , 1999 .

[9]  Gang Liu,et al.  Perfectly matched layer media with CFS for an unconditionally stable ADI-FDTD method , 2001 .

[10]  J.A. Roden,et al.  An efficient FDTD implementation of the PML with CFS in general media , 2000, IEEE Antennas and Propagation Society International Symposium. Transmitting Waves of Progress to the Next Millennium. 2000 Digest. Held in conjunction with: USNC/URSI National Radio Science Meeting (C.

[11]  O. Ramadan Unconditionally stable ADI-FDTD implementation of PML for frequency dispersive Debye media , 2004 .

[12]  Jean-Pierre Berenger,et al.  Evanescent waves in PML's: origin of the numerical reflection in wave-structure interaction problems , 1999 .

[13]  K. Yee Numerical solution of initial boundary value problems involving maxwell's equations in isotropic media , 1966 .

[14]  Amelia Rubio Bretones,et al.  Extension of the ADI-FDTD method to Debye media , 2003 .

[15]  Allen Taflove,et al.  Computational Electrodynamics the Finite-Difference Time-Domain Method , 1995 .

[16]  J. Bérenger Perfectly matched layer for the FDTD solution of wave-structure interaction problems , 1996 .