• Journal of Infrared and Millimeter Waves
  • Vol. 23, Issue 5, 363 (2004)
[in Chinese]1、2, [in Chinese]1, and [in Chinese]1
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  • 1[in Chinese]
  • 2[in Chinese]
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    [in Chinese], [in Chinese], [in Chinese]. ALTERNATING DIRECTION IMPLICIT FINITE-DIFFERENCE TIME-DOMAIN METHOD FOR PLASMAS[J]. Journal of Infrared and Millimeter Waves, 2004, 23(5): 363 Copy Citation Text show less
    References

    [1] Yee K S. Numerical solution of initial boundary value problem involving Maxwell's equations in isotropic media [J] IEEE Trans. A. P., 1966, 14(3): 302-307.

    [2] Krumpholz M, Katehi L P B. MRTD: New time-domain schemes based on multiresolution analysis [J] IEEE Trans. Microwave Theory Tech., 1996, 44(4): 555-571.

    [3] Liu Q H. The pseudospectral time-domain (PSTD) method: A new algorithm for solution of Maxwell's equations [C] Proc. IEEE Antennas and Propag. Soc. Int. Symp., 1997, 1: 122-125.

    [4] Kondylis G D, Flaviis F D, Pottie G J, et al. A memory-efficient formulation of the finite-difference time-domain method for the solution of Maxwell's equations [J]. IEEE Trans. Microwave Theory Tech., 2001, 49(7): 1310-1320.

    [5] Zheng F, Chen Z, Zhang J. A finite-difference time-domain method without the Courant stability conditions [J]. IEEE Microwave Guided Wave Lett., 1999, 9(11): 441-443.

    [6] Namiki T. A new FDTD algorithm based on alternating-direction implicit method [J]. IEEE Trans. Microwave Theory Tech., 1999, 47(10): 2003-2007.

    [7] Liu G, Gedney S D. Perfectly matched layer media for an unconditionally stable three-dimensional ADI-FDTD method [J]. IEEE Microwave Guided Wave Lett., 2000, 10(7): 261-263.

    [in Chinese], [in Chinese], [in Chinese]. ALTERNATING DIRECTION IMPLICIT FINITE-DIFFERENCE TIME-DOMAIN METHOD FOR PLASMAS[J]. Journal of Infrared and Millimeter Waves, 2004, 23(5): 363
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