1Taflove A. Computational Electrodynamics: The Finite Diff erence Time Domain Method[M]. Norwood, MA: Artech Hou se, 1995:45-300.
2Taflove A.Advances in Computational Electromagnetics: Th e FDTD Method [M]. Norwood, MA: Artech House, 1998: 150-244.
3S. Zhao, G. W. Wei, High-order FDTD methods via deft vative matching for MaxweU's equations with material interfaces [J]. Comput. Phys., 2004,200( 1 ), 60-103.
4N. Kaneda, B. Houshmand, and T. Itoh, FDTD analysis of dielectric resonators with curved surfaces [J]. IEEE Trans. Microwave Theory Tech., 1997,45 (9) z 1645-1649.
5S. Dey and R. Mittra, A conformal finite-difference time-domain for modeling cylindrical dielectric resonators [J].IEEE Microwave Theory Tech., 1999, 47(9):1737-1739.
6W. Yu and R. Mittra, A conformal finite difference time domain technique for modeling curved dielectric surfaces [J]. IF.F.F, Micrnw Wireless Common. Lett.. 2001. 11(1):25-27.
7M. Fujii, D. Lukashevich, I. Sakagami, and P. Kusser, Convergence of FDTD and wavelet-collocation modeling of curved dielectric interface with the effective dielectric constant technique [J]. IEEE Microw.Wireless Compon. Lett.,2003,13 ( 11 ) : 469-471.
8Gedney S D. An anisotropic perfectly matched layer absorbing media for the truncation of FDTD lattices [J]. IEEE Trans. Antennas Propagat, Dec. 1996, AP- 44(12): 1630-163 9.