Dielectric and Ohmic losses in perfectly absorbingmetamaterials

Abstract We investigated two mechanisms of the heat generation to enhance the absorption peak of metamaterials (MMs) at the normal incidence of electromagnetic radiation. The metal–dielectric–metal sandwich-type model, in which an array of copper squares at the front and a copper plane at the back were separated by a dielectric layer, was studied for GHz frequencies. Firstly, we studied the effect of the thickness of copper square to obtain the absorption peak. The obtained results showed that absorption can be enhanced to be nearly 100% at 16 GHz by increasing the sheet resistance of the copper square. In this case, the Ohmic-loss perfect-absorption (PA) MM was devised. The PA effect was also achieved by using the loss-tangent of dielectric layer as a dissipation factor. For this purpose, we studied complex the dielectric constant of dielectric layer. The PA peak was demonstrated at the same frequency. In the second case, the dielectric-loss turns out to be dominant. The comparison between TE and TM polarizations for the PA peaks was also elucidated.

[1]  M. Wegener,et al.  Magnetic Response of Metamaterials at 100 Terahertz , 2004, Science.

[2]  Christos Christopoulos,et al.  Customised broadband metamaterial absorbers for arbitrary polarisation. , 2010, Optics express.

[3]  M. Hentschel,et al.  Infrared perfect absorber and its application as plasmonic sensor. , 2010, Nano letters.

[4]  Xiao Liang,et al.  Electrically tunable negative permeability metamaterials based on nematic liquid crystals , 2007 .

[5]  Negative Refractive Index at the Third-Order Resonance of Flower-Shaped Metamaterial , 2012, Journal of Lightwave Technology.

[6]  K. Aydin,et al.  Negative refraction through an impedance-matched left-handed metamaterial slab , 2006 .

[7]  J. Hao,et al.  Nearly total absorption of light and heat generation by plasmonic metamaterials , 2011 .

[8]  David R. Smith,et al.  Metamaterial Electromagnetic Cloak at Microwave Frequencies , 2006, Science.

[9]  J. W. Park,et al.  Simplified perfect absorber structure , 2012 .

[10]  Willie J Padilla,et al.  Perfect metamaterial absorber. , 2008, Physical review letters.

[11]  Eleftherios N. Economou,et al.  Left-handed metamaterials: The fishnet structure and its variations , 2007 .

[12]  David R. Smith,et al.  Metamaterial-enhanced coupling between magnetic dipoles for efficient wireless power transfer , 2011, 1102.2281.

[13]  Koray Aydin,et al.  Broadband polarization-independent resonant light absorption using ultrathin plasmonic super absorbers. , 2011, Nature communications.

[14]  Wang‐Sang Lee,et al.  Uniform magnetic field distribution of a spatially structured resonant coil for wireless power transfer , 2012 .

[15]  J. Pendry,et al.  Negative refraction makes a perfect lens , 2000, Physical review letters.

[16]  M. Wegener,et al.  Metamaterial metal-based bolometers , 2012, 1204.0966.

[17]  Xiong Li,et al.  Investigation on the role of the dielectric loss in metamaterial absorber. , 2010, Optics express.

[18]  Willie J Padilla,et al.  Infrared spatial and frequency selective metamaterial with near-unity absorbance. , 2010, Physical review letters.

[19]  M. Wegener,et al.  Negative-index metamaterial at 780 nm wavelength. , 2006, Optics letters.

[20]  David R. Smith,et al.  Electric-field-coupled resonators for negative permittivity metamaterials , 2006 .

[21]  U. Chettiar,et al.  Negative index of refraction in optical metamaterials. , 2005, Optics letters.

[22]  Meissner,et al.  Complete one-loop analysis of the Nucleon's spin polarizabilities , 2000, Physical review letters.

[23]  D. Larkman,et al.  Microstructured magnetic materials for RF flux guides in magnetic resonance imaging. , 2001, Science.

[24]  K. Malloy,et al.  Experimental demonstration of near-infrared negative-index metamaterials. , 2005, Physical review letters.