[1] [1] BERENGER J P. A perfectly matched layer for the absorption of electromagnetic waves[J]. Journal of Computational Physics, 1994, 114(2): 185-200.

[2] [2] XU Jing, DAI Dao-xin, HE Sai-ling. A finite difference method with a PML boundary treatment and its application to the calculation of the optical waveguider[J]. Acta Photonic Sinica, 2003, 32(12): 1426-1429.

[3] [3] SONG Lei, LI Kang, KONG Fan-min,et al. Analysis of negative refractive index materials with the PML-FDTD mehod[J]. Acta Photonic Sinica, 2007, 36(8): 1422-1425.

[4] [4] GEDNEY S D. An anisotropic PML absorbing media fir the FDTD simulation of fields in lossy and dispersive media[J]. Electromagnetics, 1996, 16(4): 399-415.

[5] [5] RAMADA O. Digital filtering technique for the FDTD implementation of anisotropic perfectly matched layer[J]. IEEE Microwave and Wireless Components Letters, 2003, 13(8): 499-501.

[6] [6] SEMICHAEVSKY A, AKYURTLU A. A new uniaxial perfectly matched layer absorbing boundary condition for chiral metamaterials[J]. IEEE Antennas and Wireless Propagation Letters, 2005, 4(1): 51-54.

[7] [7] RODEN J A, GENDEY S D. Convolutional PML (CPML): an efficient FDTD implementation of CFS-PML for arbitrary media[J]. Microwave and Optical technology letters, 2000, 27(5): 334-339.

[8] [8] LI Jian-xiong, DAI Jun-feng. Z-transform implementation of the CFS-PML[J]. IEEE Antennas and Wireless Propagation Letters, 2006, 42(17): 953-955.

[9] [9] GEDNEY S D, ZHAO Bo. An auxiliary differential equation formulation for the complex-frequency shifted PML[J]. IEEE Transactions on Antennas and Propagation, 2010, 58(3): 838-847.

[10] [10] GE De-biao, YAN Yu-bo. Finite-difference time-domain method for electromagnetic waves[M]. 3rd ed., Xi′an: Xidian University Press, 2011,

[11] [11] MIN Zhu, CAO Qun-sheng, ZHAO Lei. Study and analysis of a novel Runge-Kutta high order finite-difference time-domain[J]. IEEE IET, Microwave Antenna & Propagation, 2014, 8(12): 951-958.

[12] [12] GIANNAKIS I, GIANNOPOULOS A A. Time-synchronized convolutional perfectly matched layer for improved absorbing performance in FDTD[J]. IEEE Antennas and wireless propagation letters, 2015, 14: 690-693.

[13] [13] TAFIOVE A, HAGNESS S C. Computational Electrodynamics:The finite difference time domain method[M]. 3nd ed. Boston: American, 2005.

[14] [14] OSKOOI A F, ZHANG L, AVNIEL Y, et al. The failure of perfectly matched layers, and towards their redemption by adiabatic absorbers[J]. Optics Express, 2008, 16(15): 11376-11392.

[15] [15] ZENG Chong, XIA Jiang-hai, RICHARD D M, et al. Application of the multiaxial perfect matched layer (M-PML) to near-surface seismic modeling with Rayleigh waves[J]. Geophysis, 2011, 76(3): T43-T52.

[16] [16] WANG Yue, WANG Jian-guo, ZHANG Dian-hui, et al. Conformal convolutional perfectly matchedlayer with uniform stability [J]. High Power laser and Particle Beams, 2013, 2(25):441-445.

[17] [17] ZHOU Li-bin, HU Man-li, JIA Fang, et al. Effect on bandgap of two-dimensional square photonic crystal with different incidence angle[J]. Acta Photonic Sinica, 2008, 37(11): 2213-2216.

[18] [18] WU Zhen-hua, LI Si-min, ZHANG Wen-tao, et al. Back reflector solar cells consisting of one-dimensional photonic crystal and double-layer two-dimensional photonic crystal[J]. Acta Photonic Sinica, 2016, 45(2): 0223003.

[19] [19] HE Feng-tao, SUN Li, XI Zhan-qiang, et al. Design and research of polarization optical splitter based on fluorine doped dual core photonic crystal fiber[J]. Acta Photonic Sinica, 2016, 45(9): 0923002.