No data available.
Please log in to see this content.
You have no subscription access to this content.
No metrics data to plot.
The attempt to load metrics for this article has failed.
The attempt to plot a graph for these metrics has failed.
The full text of this article is not currently available.
Low-frequency metamaterial absorber with small-size unit cell based on corrugated surface
4.J. B. Pendry, A. J. Holden, D. J. Robbins, and W. J. Stewart, “Magnetism from conductors, and enhanced non-linear phenomena,” IEEE Trans. Microw. Theory Tech. 47(11), 2075–2084 (1999).
9.S. Chen, H. Cheng, H. Yang, J. Li, X. Duan, C. Gu, and J. Tian, “Polarization insensitive and omnidirectional broadband near perfect planar metamaterial absorber in the near infrared regime,” Appl. Phys. Lett. 99(25), 253104 (2011).
10.X. Shen, T. J. Cui, J. Zhao, H. F. Ma, W. X. Jiang, and H. Li, “Polarization-independent wide-angle triple-band metamaterial absorber,” Opt. Express 19(10), 9401-9407 (2011).
11.X. Shen, Y. Yang, Y. Zang, J. Gu, J. Han, W. Zhang, and T. J. Cui, “Triple-band terahertz metamaterial absorber: Design, experiment, and physical interpretation,” Appl. Phys. Lett. 101(15), 154102 (2012).
12.F. Ding, Y. Cui, X. Ge, Y. Jin, and S. He, “Ultra-broadband microwave metamaterial absorber,” Appl. Phys. Lett. 100(10), 103506 (2012).
13.J. Sun, L. Liu, G. Dong, and J. Zhou, “An extremely broad band metamaterial absorber based on destructive interference,” Opt. Express 19(22), 21155-21162 (2011).
14.B. Zhu, Y. Feng, J. Zhao, C. Huang, and T. Jiang, “Switchable metamaterial reflector/absorber for different polarized electromagnetic waves,” Appl. Phys. Lett. 97(5), 051906 (2010).
15.H. X. Xu, G. M. Wang, M. Q. Qi, J. G. Liang, J. Q. Gong, and Z. M. Xu, “Triple-band polarization-insensitive wide-angle ultra-miniature metamaterial transmission line absorber,” Phys. Rev. B 86(20), 205104 (2012).
16.H. Cheng, S. Chen, H. Yang, J. Li, X. An, C. Gu, and J. Tian, “A polarization insensitive and wide-angle dualband nearly perfect absorber in the infrared regime,” J. Opt. 14(8), 085102 (2012).
17.J. Zhong, Y. Huang, G. Wen, H. Sun, P. Wang, and O. Gordon, “Single-/dual-band metamaterial absorber based on cross-circular-loop resonator with shorted stubs,” Appl. Phys., A Mater. Sci. Process. 108(2), 329-335 (2012).
19.H. Tao, N. I. Landy, C. M. Bingham, X. Zhang, R. D. Averitt, and W. J. Padilla, “A metamaterial absorber for the terahertz regime: Design, fabrication and characterization,” Opt. Express 16(10), 7181-7188 (2008).
21.X. Y. Peng, B. Wang, S. Lai, D. H. Zhang, and J. H. Teng, “Ultrathin multi-band planar metamaterial absorber based on standing wave resonances,” Opt. Express 20(25), 27756-27765 (2012).
22.H. Shi et al., “A new surface wave antenna-based spoof surface plasmon mechanism,” Microwave and Optical Technology Letters 52, 2179 (2010).
23.A. S. Stender et al., “Plasmonic Behavior of Single Gold Dumbbells and Simple Dumbbell Geometries,” J. Phys. Chem. C 117, 16195–16202 (2013).
24.J. N. Munday and H. A. Atwater, “Large integrated absorption enhancement in plasmonic solar cells by combining metallic gratings and antireflection coatings,” Nano Lett. 11(6), 2195-2201 (2011).
26.N. Liu, M. Mesch, T. Weiss, M. Hentschel, and H. Giessen, “Infrared perfect absorber and its application as plasmonic sensor,” Nano Lett. 10(7), 2342-2348 (2010).
27.D. R. Smith, D. C. Vier, Th. Koschny, and C. M. Soukoulis, “Electromagnetic parameter retrieval from inhomogeneous metamaterials,” Phys. Rev. E Stat. Nonlin. Soft Matter Phys. 71(3 3 Pt 2B), 036617 (2005).
Article metrics loading...
In this paper, we report the design, analysis, and simulation of the low-frequency perfect metamaterial absorber (MMA) based on corrugated surface, which has very small unit-cell size. The proposed MMA consist of a regular square-array and a metallic background plane, separated by a corrugated surface with periodic square-pillar-array. Through the optimized design, the ratios between lattice constant and resonance wavelength for nearly-perfect and high absorption MMA are close to 1/15 and 1/21, respectively. To explain the absorption mechanism of suggested structures, the surface current and electromagnetic field distributions are given. Moreover, the absorption peaks remain high with large angles of incidence for both transverse electric and transverse magnetic polarizations, which provide more efficient absorptions for oblique incident electromagnetic wave.
Full text loading...
Most read this month