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The piecewise linear current density recursive convolution finite-difference time-domain method of plasma is used to study the defect mode properties of transverse magnetic wave propagation in the two-dimensional unmagnetized plasma photonic crystals with a line-defect layer. In frequency domain, the transmission coefficients of electromagnetic differential Gaussian pulses are computed, and the effect of lattice constant, dielectric column radius, periodic constant, parameters of plasma and parameters of line-defect layer on defect mode properties of two-dimensional unmagnetized plasma photonic crystals are analyzed. The results illustrate that the frequency of defect mode cannot be tuned by changing periodic constant, position of the defect layer and plasma collision frequency, but be tuned by changing relative permittivity and radius of dielectric column in the defect layer, and central distance between defect layer and dielectric layer with the width of prohibit band gaps fixed. Furthermore, the defect mode and the width of prohibit band gaps can also be tuned by changing lattice constant, dielectric column radius and plasma frequency.
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Keywords:
- plasma /
- photonic crystals /
- defect mode /
- finite-difference time-domain method
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[22] Liu S B, Yuan N C, Liu S Q, Mo J J 2003 IEEE Proc. Microw. Anten. Propag. 152 189
[23] Zhuang Z W, Yuan N C, Liu S B, Mo J J 2005 Plasma Stealth Technology( Beijing: Science Press) p13 (in Chinese) [庄钊文、 袁乃昌、 刘少斌、 莫锦军 2005 等离子体隐身技术 (北京:科学出版社) 第13页]
[24] Liu S B, Liu S, Hong W 2010 Finite Difference Time Domain Method for Dispersive Media ( Beijing: Science Press) p315 (in Chinese)[刘少斌、 刘 崧、 洪 伟 2010 色散介质的时域有限差分算法(北京:科学出版社) 第315页]
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[1] John S 1987 Phys. Rev. Lett. 58 2486
[2] Yablonovitch E 1987 Phys. Rev. Lett. 58 2059
[3] Yakoyama H, Nishi K, Anan T 1992 Opt. Quant. Electron. 24 245
[4] Zhou W D, Sabarinathan J, Bhattacharya P, Kochman B, Berg E W, Yu P C, Pang S W 2001 IEEE J.Quant. Electron. 37 1153
[5] Villeneuve P R, Fan S, Joannopoulos J D 1996 Phys. Rev. B 54 7837
[6] Feng T H, Dai Q F, Wu L J, Guo Q, Hu W, Lan S 2008 Chin. Phys. B 17 4533
[7] Zhao X X, Zhu Q F, Zhang Y 2009 Chin. Phys. B 18 2864
[8] Ma J Y, Liu S J, Zhang D W, Yao J K, Xu C, Jin Y X, Shao J D, Fan Z X 2008 Chin. Phys. B 17 3704
[9] Fan S, Villeneuve P R, Joannopoulos J D 1997 Phys. Rev. Lett. 78 3294
[10] Hojo H, Mase A 2004 J. Plasma Fusion Res. 80 89
[11] Liu S B, Hong W, Yuan N C 2006 Int. J. Infrar. Millim. Waves 27 403
[12] Liu S B, Mo J J, Yuan N C 2005 Acta Phys. Sin. 54 2804 (in Chinese) [刘少斌、 莫锦军、 袁乃昌 2005 54 2804]
[13] Hojo H, Mase A 2009 J. Plasma Fusion Res. 8 477
[14] Shiveshwari L, Mahto P 2006 Solid State Communications 138 160
[15] Li W, Gao H, Gong M L, Liu S G 2004 Chin. Phys. 13 1296
[16] Ma L, Zhang H F, Liu S B 2008 Acta Phys. Sin. 57 5089 (in Chinese)[马 力、 章海锋、 刘少斌 2008 57 5089]
[17] Zhang H F, Ma Li, Liu S B 2009 Acta Phys. Sin. 58 1071 (in Chinese) [章海锋、 马 力、 刘少斌 2009 58 1071]
[18] Qi L M, Yang Z Q, Lan F, Gao X, Li D Z 2010 Chin. Phys. B 19 034210
[19] Qi L M, Yang Z Q, Lan F, Gao X, Shi Z J, Liang Z 2010 Acta Phys. Sin. 59 0351 (in Chinese) [亓丽梅、 杨梓强、 兰 峰、 高 喜、 史宗君、 梁 正 2010 59 0351]
[20] Sakai O, Sakaguchi T, Tachibana K 2007 Contrib. Plasma Phys. 47 96
[21] Liu S B, Yuan N C, Mo J J 2003 IEEE Microw. Wireless Compon. Lett. 13 187
[22] Liu S B, Yuan N C, Liu S Q, Mo J J 2003 IEEE Proc. Microw. Anten. Propag. 152 189
[23] Zhuang Z W, Yuan N C, Liu S B, Mo J J 2005 Plasma Stealth Technology( Beijing: Science Press) p13 (in Chinese) [庄钊文、 袁乃昌、 刘少斌、 莫锦军 2005 等离子体隐身技术 (北京:科学出版社) 第13页]
[24] Liu S B, Liu S, Hong W 2010 Finite Difference Time Domain Method for Dispersive Media ( Beijing: Science Press) p315 (in Chinese)[刘少斌、 刘 崧、 洪 伟 2010 色散介质的时域有限差分算法(北京:科学出版社) 第315页]
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