A Method of Analyzing Transmission Losses in Left-Handed Metamaterials
WANG Jia-Fu1, QU Shao-Bo1,2, XU Zhuo2, ZHANG Jie-Qiu1, MA Hua1, YANG Yi-Ming1, GU Chao1
1College of Science, Air Force Engineering University, Xi'an 7100512Electronic Materials Research Laboratory, Key Laboratory of the Ministry of Education, Xi'an Jiaotong University, Xi'an 710049
A Method of Analyzing Transmission Losses in Left-Handed Metamaterials
WANG Jia-Fu1, QU Shao-Bo1,2, XU Zhuo2, ZHANG Jie-Qiu1, MA Hua1, YANG Yi-Ming1, GU Chao1
1College of Science, Air Force Engineering University, Xi'an 7100512Electronic Materials Research Laboratory, Key Laboratory of the Ministry of Education, Xi'an Jiaotong University, Xi'an 710049
A method of analyzing transmission loss in left-handed metamaterials (LHMs) is proposed. As a demonstration of this method, transmission loss of LHMs composed of split-ring resonators (SRR) and conducting wires is studied. By means of retrieving and analyzing the effective constitutive parameters, different transmission losses as well as their origins are studied. The results show that the left-handed bandwidth is narrowed because of high loss caused by the non-zero high imaginary parts of the effective permeability and permittivity. In the effective left-handed band, the radiation loss is very low and can be neglected, and the transmission losses are the sum of the substrate loss and the ohmic loss. Moreover, when the dielectric loss tangent of the substrate is greater than 0.003, the substrate loss is higher than the ohmic loss.
Abstract:A method of analyzing transmission loss in left-handed metamaterials (LHMs) is proposed. As a demonstration of this method, transmission loss of LHMs composed of split-ring resonators (SRR) and conducting wires is studied. By means of retrieving and analyzing the effective constitutive parameters, different transmission losses as well as their origins are studied. The results show that the left-handed bandwidth is narrowed because of high loss caused by the non-zero high imaginary parts of the effective permeability and permittivity. In the effective left-handed band, the radiation loss is very low and can be neglected, and the transmission losses are the sum of the substrate loss and the ohmic loss. Moreover, when the dielectric loss tangent of the substrate is greater than 0.003, the substrate loss is higher than the ohmic loss.
[1] Veselago V G 1968 it Sov. Phys. Usp. 10 509 [2] Pendry J B et al 1999 it IEEE Trans. Microwaves Theor.Technol. 47 2075 [3] Smith D R et al 2000 it Phys. Rev. Lett. 84 4184 [4] Cai X B et al 2006 it Chin. Phys. Lett. 23 348 [5] Chen H. S et al 2004 it Phys. Rev. E 70 057605 [6] Liu Y H et al 2007 it Acta Phys. Sin. 56 5883 [7] Quan B G et al 2005 it Chin. Phys. Lett. 22 1243 [8] Wang J F et al 2008 it Acta Phys. Sin. 57 5015 [9] Markos P et al 2002 it Phys. Rev. E 66 045601 [10] Ponizovskaya E V et al 2002 it Appl. Phys. Lett. 81 4470 [11] Cui T J et al 2004 it Phys. Lett. A 323 484 [12] Simovski C R and Sauviac B 2004 it Phys. Rev. E 70 046607 [13] Greegor R B et al 2003 it Appl. Phys. Lett. 822356 [14] Chen X D et al 2004 it Phys. Rev. E 70 016608