[2] TAFLOVE A,HAGNESS S H. Computational electrodynamics: the finite-difference time-domain method[M]. London: Artech House,2000: 1-10.
[4] HARMS P,MITTRA R,KO W. Implementation of the periodic boundary condition in the finite-difference time-domain algorithm for FSS structures[J]. IEEE Transactions on Antennas and Propagation,1994,42(9): 1317-1324.
[5] AMINIAN A,SAMII Y R. Spectral FDTD: A novel technique for the analysis of oblique incident plane wave on periodic structures[J]. IEEE Transactions on Antennas and Propagation,2006,54(6): 1818-1825.
[7] VALUEV I,DEINEGA A,BELOUSOV S. Iterative technique for analysis of periodic structures at oblique incidence in the finite-difference time-domain method[J]. Optics Letters,2008,33(13): 1491-1493.
[8] VALUEV I,DEINEGA A,BELOUSOV S. Implementation of the iterative finite-difference time-domain technique for simulation of periodic structures at oblique incidence[J]. Computer Physics Communications,2014,185: 1273-1281.
[10] FARAHAT N,MITTRA R. Analysis of frequency selective surfaces using the finite difference time domain method[J]. IEEE Transactions on Antennas and Propagation,2002,2(8): 568-571.
[11] DEINEGA A,VALUEV I. Subpixel smoothing for conductive and dispersive media in the FDTD method[J]. Optics Letters,2007,32(23): 3429-3431.
[12] DEINEGA A,JOHN S. Effective optical response of silicon to sunlight in the finite-difference time-domain method[J]. Optics Letters,2012,37(1): 112-114.
[13] ZHAO Qian,ZHOU Ji,ZHANG Fu-li,et al. Mie resonance-based dielectric metamaterials[J]. Materialstoday,2009,12(9): 60-69.
[14] SPINELLI P,VERSCHUUREN M A,POLMAN A. Broadband omnidirectional antireflection coating based on subwavelength surface Mie resonators[J]. Nature Communications,2012,3: 1-5.
[15] TSKHAKAYA D,MATYASH K,SCHNEIDER R,et al. The particle-in-cell method[J]. Contribution to Plasma Physics,2007,47: 563-594.