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The piecewise linear current density recursive convolution (PLCDRC) on finite-difference time-domain (FDTD) method is applied to study the properties of prohibited band gaps for TM wave propagation in the two-dimensional unmagnetized plasma photonic crystal. In frequency-domain, the transmission coefficient of electromagnetic differential Gaussian pulses are computed and we analyzed the effect on properties of tunable prohibited band gaps for the two-dimensional unmagnetized plasma photonic crystals by its relative permittivity of column, lattic constant, dielectric column radius, periodic constant and parameters of plasma. The results showed that the prohibited band gaps can not be broadened by inceasing periodic constant and plasma collision frequency, but can be broadened by increasing relative permittivity of column and plasma frequency. The prohibited gaps also can be widened by decreasing the lattic constant and dielectric column radius for fill rate of a certain value.
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Keywords:
- plasma /
- photonic crystals /
- prohibit band gaps /
- piecewise linear current density recursive convolution method
[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] Villeneuve P R, Fan S , Joannopoulos J D 1996 Phys. Rev. B 54 7837
[5] Fan S, Villeneuve P R , Joannopoulos J D 1997 Phys. Rev. Lett. 78 3294
[6] Hojo H , Mase A 2004 J. Plasma Fusion Res. 80 89
[7] Qi L M, Yang Z Q , Lan Feng, Gao X, Li D Z 2010 Chin.Phys.B 19 034210
[8] Liu S B , Mo J J , Yuan N C 2005 Acte. Phys. Sin. 54 2804 (in Chinese) [刘少斌、莫锦军、袁乃昌2005 54 2804]
[9] Shiveshwari L, Mahto P 2006 Solid State Communications 138 160
[10] Li W, Wei Y Y, Xie H Q, Liu S G, Gong M L 2003 Chin. Phys. 12 532
[11] Ma Li, Zhang H F, Liu S B 2008 Acte. Phys. Sin. 57 5089 (in Chinese)[马 力、章海锋、刘少斌 2008 57 5089]
[12] Zhang H F, Ma Li, Liu S B 2009 Acte. Phys. Sin. 58 1071 (in Chinese) [章海锋、马 力、刘少斌 2009 58 1071]
[13] Qi L M, Yang Z Q, Lan F, Gao X, Shi Z J 2010 Phys. Plasmas 17 042501
[14] Guo B 2009 Phys. Plasmas 16 043508
[15] Hojo H , Mase A 2009 J. Plasma Fusion Res. 8 477
[16] Liu S B, Yuan N C , Mo J J 2003 IEEE Microwave and Wireless Components Lett. 13 187
[17] Liu S B ,Yuan N C, Liu S Q , Mo J J 2003 IEEE Proc. Microw. Antennas. Propag. 152 189
[18] L iu 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] Villeneuve P R, Fan S , Joannopoulos J D 1996 Phys. Rev. B 54 7837
[5] Fan S, Villeneuve P R , Joannopoulos J D 1997 Phys. Rev. Lett. 78 3294
[6] Hojo H , Mase A 2004 J. Plasma Fusion Res. 80 89
[7] Qi L M, Yang Z Q , Lan Feng, Gao X, Li D Z 2010 Chin.Phys.B 19 034210
[8] Liu S B , Mo J J , Yuan N C 2005 Acte. Phys. Sin. 54 2804 (in Chinese) [刘少斌、莫锦军、袁乃昌2005 54 2804]
[9] Shiveshwari L, Mahto P 2006 Solid State Communications 138 160
[10] Li W, Wei Y Y, Xie H Q, Liu S G, Gong M L 2003 Chin. Phys. 12 532
[11] Ma Li, Zhang H F, Liu S B 2008 Acte. Phys. Sin. 57 5089 (in Chinese)[马 力、章海锋、刘少斌 2008 57 5089]
[12] Zhang H F, Ma Li, Liu S B 2009 Acte. Phys. Sin. 58 1071 (in Chinese) [章海锋、马 力、刘少斌 2009 58 1071]
[13] Qi L M, Yang Z Q, Lan F, Gao X, Shi Z J 2010 Phys. Plasmas 17 042501
[14] Guo B 2009 Phys. Plasmas 16 043508
[15] Hojo H , Mase A 2009 J. Plasma Fusion Res. 8 477
[16] Liu S B, Yuan N C , Mo J J 2003 IEEE Microwave and Wireless Components Lett. 13 187
[17] Liu S B ,Yuan N C, Liu S Q , Mo J J 2003 IEEE Proc. Microw. Antennas. Propag. 152 189
[18] L iu 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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