[1] SARID D, CHALLENER W. Modern introduction to surface plasmons: theory, mathematica modeling, and applications[M]. New York: Cambridge University, 2010: 4-14.
[3] TAFLOVE A, HAGNESS S C. Computational electrodynamics: the finite-difference time-domain method[M]. 3rd ed. Norwood, MA: Artech House, 2005.
[4] VOLAKIS J, HATERJEE A, EMPEL L C. Finite element method for electromagnetic: antennas, microwave circuits, and scattering applications[M]. New York: IEEE Press, 1998.
[5] LI Yu-kui, WANG Feng-ge, ZANG Fan-guang, et al. Preparation and characteristic of second-printing type carbon nanotube cathode for triode field emission display[J]. Acta Photonica Sinica, 2013, 42(5): 570-575.
[6] HAI Lin, MARIO F. An FDTD thin-wire model for modeling carbon nanotube dipoles at THz regime[J]. IEEE Antenna and Wireless Propagation Letters, 2012, 11: 708-711.
[7] RASGHIDI A, MOSALLAEI H, MITTRA R. Scattering analysis of plasmonic nanorod antennas: A novel numerically efficient computational scheme utilizing macro basis functions[J]. Journal of Applied Physics, 2011, 109(12): 123109.
[9] RASHIDI A. Scattering performance of plasmonic nanorod antennas in randomly tilted disordered and Fibonacci configurations[J]. Applied Physics Letters, 2012, 101(6): 062401.
[10] ALU A. Multifrequency optical invisibility cloak with layered plasmonic shells[J]. Physical Review Letters, 2008, 100(11): 113901.
[11] RAETHER H. Surface plasmons[M]. Berlin:Springer Verlage,1988.
[12] HARRIGTON R. Time-harmonic electromagnetic fields[M]. New York: IEEE Press, 2001.
[13] HARRIGTON R. Field computation by moment method[M]. New York: IEEE Press, 1992.
[14] WANG Yi-ping. 2002 Fundamentals of electromagnetic fields and waves[M]. Xi′an: Xi′an University, 2002: 38-44.
[15] CAO Zhen-xin, XIA Ji-jiang. Resonant wavelength red shifting of optical fiber surface plasmon resonance sensing system[J]. Acta Photonica Sinica, 2008, 37(10): 1997-2000.
[16] SADIKU M N O. Numerical techniques in electroagnetics[M]. Boca Raton:CRC Press, 2000.