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2004-04-15
Numerical Dispersion and Impedance Analysis for 3D Perfectly Matched Layers Used for Truncation of the FDTD Computations
By
, Vol. 47, 193-212, 2004
Abstract
The 3D Berenger's and uniaxial perfectly matched layers used for the truncation of the FDTD computations are theoretically investigated respectively in the discrete space, including numerical dispersion and impedance characteristics. Numerical dispersion for both PMLs is different from that of the FDTD equations in the normal medium due to the introduction of loss. The impedance in 3D homogeneous Berenger's PML medium is the same as that in the truncated normal medium even in the discrete space, however, the impedance in 3D homogenous UPML medium is different, but the discrepancy smoothly changes as the loss in the UPML medium slowly change. Those insights acquired can help to understand why both 3D PMLs can absorb the outgoing wave with arbitrary incidence, polarization, and frequency, but with different efficiency.
Citation
Weiliang Yuan, and Er Ping Li, "Numerical Dispersion and Impedance Analysis for 3D Perfectly Matched Layers Used for Truncation of the FDTD Computations," , Vol. 47, 193-212, 2004.
doi:10.2528/PIER03121002
References

1. Taflove, A., Advances in Computational Electrodynamics, the Finite-Difference Time-Domain Method, 1998.

2. Mur, G., "Absorbing boundary conditions for the finitedifference approximation of the time-domain electromagnetic-field equations," IEEE Trans. Electromagn. Compat., Vol. 23, 377-382, 1981.

3. Liao, Z. P., H. L. Wong, B. Yang, and Y. Yuan, "A transmitting boundary for transient wave analyses," Scientia Sinica, Vol. 27, 1063-1076, 1984.

4. Mei, K. K. and J. Fang, "Superabsorption — a method to improve absorbing boundary conditions," IEEE Trans. Antennas Propagat., Vol. 40, 1001-1010, 1992.
doi:10.1109/8.166524

5. Teixeira, F. L. and W. C. Chew, "Differential forms, metrics, and the reflectionless absorption of electromagnetic waves," Journal of Electromagnetic Waves and Applications, Vol. 13, 665-686, 1999.

6. Buksas, M. W., "Implementing the perfectly matched layer absorbing boundary condition with mimetic differencing schemes," Progress In Electromagnetics Research, Vol. 32, 383-411, 2001.
doi:10.2528/PIER00080115

7. Li, L. W., P. S. Kooi, M. S. Leong, and S. T. Chew, "FDTD analysis of sidecoupled microstrip filter," Journal of Electromagnetic Waves and Applications, Vol. 14, 1533-1548, 2000.

8. Berenger, J., "A perfectly matched layer for the absorption of electromagnetic waves," Journal of Computational Physics, Vol. 114, 185-200, 1994.
doi:10.1006/jcph.1994.1159

9. Berenger, J., "Three dimensional perfectly matched layer for the absorption of electromagnetic waves," Journal of Computational Physics, Vol. 127, 363-379, 1996.
doi:10.1006/jcph.1996.0181

10. Chew, W. C. and W. H. Weedon, "A 3D perfectly matched medium from modified Maxwell's equations with stretched coordinates," Microwave and Optical Technology Letters, Vol. 7, 599-604, 1994.

11. Gedney, S. D., "An anisotropic perfectly matched layer absorbing medium for the truncation of FDTD lattices," IEEE Trans. Antennas and Propagat., Vol. 44, 1630-1639, 1996.
doi:10.1109/8.546249

12. Tang, J., K. D. Paulsen, and S. A. Haider, "Perfectly matched layer mesh terminations for nodal-based finite element methods in electromagnetic scattering," IEEE Trans. Antennas and Propagat., Vol. 46, 507-516, 1998.
doi:10.1109/8.664114

13. Pena, N. and M. M. Ney, "Absorbing boundary conditions using perfectly matched layer (PML) technique for three-dimensional TLM simulations," IEEE Trans. Microwave Theory Tech., Vol. 45, 1749-1755, 1997.
doi:10.1109/22.641722

14. Qi, Q. and T. L. Geers, "Evaluation of perfectly matched layer for computational acoustics," Journal of Computational Physics, Vol. 139, 166-183, 1998.
doi:10.1006/jcph.1997.5868

15. Prescott, D. T. and N. V. Shuley, "Reflection analysis of FDTD boundary conditions — Part II: Berenger's PML absorbing layers," IEEE Trans. Microwave Theory Tech., Vol. 45, 1171-1178, 1997.
doi:10.1109/22.618404