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    This chapter has been cited by the following publications. This list is generated based on data provided by CrossRef.

    Papaioannou, Maria Plum, Eric Valente, João Rogers, Edward T. F. and Zheludev, Nikolay I. 2016. All-optical multichannel logic based on coherent perfect absorption in a plasmonic metamaterial. APL Photonics, Vol. 1, Issue. 9, p. 090801.

    Dimitriadis, Alexandros I. and Tsiboukis, Theodoros D. 2013. Generalized fresnel coefficients for arbitrary periodic metafilms. p. 286.

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  • Print publication year: 2011
  • Online publication date: June 2011

4 - Chirality and anisotropy of planar metamaterials

Summary

Introduction

In recent years it has emerged that planar metamaterials offer a vast range of custom-designed electromagnetic functionalities. The best known are wire grid polarizers, which are established standard components for microwaves, terahertz waves, and the far-infrared. They are expected to be of increasing importance also for the near-infrared [1] and visible light [2]. Equally well developed are frequency selective surfaces [3–6], which are used as filters in radar systems, antenna technology [7], broadband communications, and terahertz technology [8, 9]. However, the range of optical effects observable in planar metamaterials and the variety of potential applications have only become clear since metamaterials research took off in 2000 [10]. Wave plate [11, 12] as well as polarization rotator and circular polarizer [13–15] functionalities have been demonstrated in metamaterials of essentially zero thickness. Traditionally, such components are large as they rely on integrating weak effects over thick functional materials. Polarization rotation has also been seen at planar chiral diffraction gratings [16, 17] and thin layered stereometamaterials [18, 19]. Electromagnetically induced transparency (EIT) [20–24] and high quality factor resonances [20] have been observed at planar structured interfaces. And finally, new fundamental electromagnetic effects leading to directionally asymmetric transmission of circularly [25–29] and linearly polarized waves have been discovered in planar metamaterials.

Planar metamaterials derive their properties from artificial structuring rather than atomic or molecular resonances, and therefore appropriately scaled versions of such structures will show similar properties for radio waves, microwaves, terahertz waves, and, to some extent, in the infrared and optical spectral regions where losses are becoming more important.

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Structured Surfaces as Optical Metamaterials
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References
[1] Tamada, H., Doumuki, T., Yamaguchi, T., and Matsumoto, S., “Al wire-grid polarizer using the s-polarization resonance effect at the 0.8-μm-wavelength band,Opt. Lett. 22, 419–421 (1997).
[2] Ahn, S. W., Lee, K. D., Kim, J. S., Kim, S. H., Park, J. D., Lee, S. H., and Yoon, P. W., “Fabrication of a 50 nm half-pitch wire grid polarizer using nanoimprint lithography,Nanotechnol. 16, 1874–1877 (2005).
[3] Ott, R., Kouyoumjian, R., and Peters, L. Jr., “Scattering by a two-dimensional periodic array of narrow plates,Radio Sci. 2, 1347–1359 (1967).
[4] Chen, C., “Scattering by a two-dimensional periodic array of conducting plates,IEEE Trans. Antenn. Propag. AP-18, 660–665 (1970).
[5] Munk, B., Kouyoumjian, R., and Peters, L. Jr., “Reflection properties of periodic surfaces of loaded dipoles,IEEE Trans. Antenn. Propag. AP-19, 612–617 (1971).
[6] Munk, B. A., Frequency Selective Surfaces: Theory and Design, 1st edn (New York: Wiley-Interscience, 2000).
[7] Huang, J., Wu, T. K., and Lee, S. W., “Tri-band frequency-selective surface with circular ring elements,IEEE Trans. Antenn. Propag. AP-42, 166–175 (1994).
[8] Ulrich, R., “Far infrared properties of metallic mesh and its complementary structure,Infrared Phys. 7, 37–55 (1967).
[9] Tomaselli, V. P., Edewaard, D. C., Gillan, P., and Möller, K. D., “Far infrared bandpass filters from cross shaped grids,Appl. Opt. 20, 1361–1366 (1981).
[10] Smith, D. R., Padilla, W. J., Vier, D. C., Nemat-Nasser, S. C., and Schultz, S., “Composite medium with simultaneously negative permeability and permittivity,Phys. Rev. Lett. 84, 4184–4187 (2000).
[11] Fedotov, V. A., Mladyonov, P. L., Prosvirnin, S. L., and Zheludev, N. I., “Planar electromagnetic metamaterial with a fish scale structure,Phys. Rev. E 72, 056613(1-4) (2005).
[12] Peralta, X. G., Smirnova, E. I., Azad, A. K., Chen, H.-T., Taylor, A. J., Brener, I., and O'Hara, J. F., “Metamaterials for THz polarimetric devices,Opt. Express 17, 773–783 (2009).
[13] Plum, E., Fedotov, V. A., and Zheludev, N. I., “Optical activity in extrinsically chiral metamaterial,Appl. Phys. Lett. 93, 191911(1-3) (2008).
[14] Plum, E., Liu, X.-X., Fedotov, V. A., Chen, Y., Tsai, D. P., and Zheludev, N. I., “Metamaterials: optical activity without chirality,Phys. Rev. Lett. 102, 113902(1-4) (2009).
[15] Singh, R., Plum, E., Zhang, W., and Zheludev, N. I., “Highly tunable optical activity in planar achiral terahertz metamaterials,Opt. Exp. 18, 13425 (2010).
[16] Papakostas, A., Potts, A., Bagnall, D. M., Prosvirnin, S. L., Coles, H. J., and Zheludev, N. I., “Optical manifestations of planar chirality,Phys. Rev. Lett. 90, 107404(1-4) (2003).
[17] Prosvirnin, S. L. and Zheludev, N. I., “Polarization effects in the diffraction of light by a planar chiral structure,Phys. Rev. E 71, 037603(1-4) (2005).
[18] Svirko, Y., Zheludev, N., and Osipov, M., “Layered chiral metallic microstructures with inductive coupling,Appl. Phys. Lett. 78, 498–500 (2001).
[19] Plum, E., Fedotov, V. A., Schwanecke, A. S., Zheludev, N. I., and Chen, Y., “Giant optical gyrotropy due to electromagnetic coupling,Appl. Phys. Lett. 90, 223113(1-3) (2007).
[20] Fedotov, V. A., Rose, M., Prosvirnin, S. L., Papasimakis, N., and Zheludev, N. I., “Sharp trapped-mode resonances in planar metamaterials with a broken structural symmetry,Phys. Rev. Lett. 99, 147401(1-4) (2007).
[21] Zhang, S., Genov, D. A., Wang, Y., Liu, M., and Zhang, X., “Plasmon-induced transparency in metamaterials,Phys. Rev. Lett. 101, 047401(1-4) (2008).
[22] Luk'yanchuk, B., Zheludev, N. I., Maier, S. A., Halas, N. J., Nordlander, P., Giessen, H., and Chong, C. T., “The Fano resonance in plasmonic nanostructures and metamaterials,Nat. Mater. 9, 707 (2010).
[23] Tassin, P., Zhang, L., Koschny, T., Economou, E. N., and Soukoulis, C. M., “Low-loss metamaterials based on classical electromagnetically induced transparency,Phys. Rev. Lett. 102, 053901(1-4) (2009).
[24] Papasimakis, N. and Zheludev, N. I., “Metamaterial-induced transparency,Opt. Photon. News 20, 22 (2009).
[25] Fedotov, V. A., Mladyonov, P. L., Prosvirnin, S. L., Rogacheva, A. V., Chen, Y., and Zheludev, N. I., “Asymmetric propagation of electromagnetic waves through a planar chiral structure,Phys. Rev. Lett. 97, 167401(1-4) (2006).
[26] Schwanecke, A. S., Fedotov, V. A., Khardikov, V. V., Prosvirnin, S. L., Chen, Y., and Zheludev, N. I., “Nanostructured metal film with asymmetric optical transmission,Nano Lett. 8, 2940–2943 (2008).
[27] Plum, E., Fedotov, V. A., and Zheludev, N. I., “Planar metamaterial with transmission and reflection that depend on the direction of incidence,Appl. Phys. Lett. 94, 131901(1-3) (2009).
[28] Plum, E., Fedotov, V. A., and Zheludev, N. I., “Extrinsic electromagnetic chirality in metamaterials,J. Opt. A: Pure Appl. Opt. 11, 074009(1-7) (2009).
[29] Plum, E., Fedotov, V. A., and Zheludev, N. I., “Asymmetric transmission: a generic property of two-dimensional periodic patterns,J. Opt. 13, 024006 (2011).
[30] Plum, E., Fedotov, V. A., and Zheludev, N. I., “Metamaterial optical diodes for linearly and circularly polarized light,arXiv.org. 1006.0870 (2010).
[31] Kong, J. A., Electromagnetic Wave Theory (Cambridge, MA: EMW Publishing, 2005).
[32] Falcone, F., Lopetegi, T., Laso, M. A. G.et al. “Babinet principle applied to the design of metasurfaces and metamaterials,Phys. Rev. Lett. 93, 197401(1-4) (2004).
[33] Jackson, J. D., Classical Electrodynamics (New York: Wiley, 1999).
[34] Potts, A., Bagnall, D. M., and Zheludev, N. I., “A new model of geometric chirality for two-dimensional continuous media and planar meta-materials,J. Opt. A: Pure Appl. Opt. 6, 193–203 (2004).
[35] Osipov, M. A., Pickup, B. T., Fehervari, M., and Dunmur, D. A., “Chirality measure and chiral order parameter for a two-dimensional system,Mol. Phys. 94, 283–287 (1998).
[36] Padilla, W. J., “Group theoretical description of artificial electromagnetic metamaterials,Opt. Express 15, 1639–1646 (2007).
[37] Bingham, C. M., Tao, H., Liu, X., Averitt, R. D., Zhang, X., and Padilla, W. J., “Planar wallpaper group metamaterials for novel terahertz applications,Opt. Express 16, 18565–18575 (2008).
[38] Schattschneider, D., “The plane symmetry groups: their recognition and notation,Am. Math. Mon. 85, 439–450 (1978).
[39] Bunn, C. W., Chemical Crystallography (New York: Oxford University Press, 1945).
[40] Williams, R., “Optical rotatory effect in the nematic liquid phase of p-azoxyanisole,Phys. Rev. Lett. 21, 342–344 (1968).
[41] Williams, R., “Optical-rotary power and linear electro-optic effect in nematic liquid crystals of p-azoxyanisole,J. Chem. Phys. 50, 1324–1332 (1969).
[42] Singh, R., Plum, E., Menzel, C.et al. “Terahertz metamaterial with asymmetric transmission,Phys. Rev. B 80, 153104(1-4) (2009).
[43] Fedotov, V. A., Schwanecke, A. S., Zheludev, N. I., Khardikov, V. V., and Prosvirnin, S. L., “Asymmetric transmission of light and enantiomerically sensitive plasmon resonance in planar chiral nanostructures,Nano Lett. 7, 1996–1999 (2007).
[44] Drezet, A., Genet, C., Laluet, J.-Y., and Ebbesen, T. W., “Optical chirality without optical activity: how surface plasmons give a twist to light,Opt. Express 16, 12559–12570 (2008).
[45] Zhukovsky, S. V., Novitsky, A. V., and Galynsky, V. M., “Elliptical dichroism: operating principle of planar chiral metamaterials,Opt. Lett. 34, 1988–1991 (2009).
[46] Menzel, C., Helgert, C., Rockstuhl, C., Kley, E.-B., Tünnermann, A., Pertsch, T., and Lederer, F., “Asymmetric transmission of linearly polarized light at optical metamaterials,Phys. Rev. Lett. 104, 253902 (2010).