2012
DOI: 10.1021/nl300204s
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Out-of-Plane Reflection and Refraction of Light by Anisotropic Optical Antenna Metasurfaces with Phase Discontinuities

Abstract: Experiments on ultrathin anisotropic arrays of subwavelength optical antennas display out-of-plane refraction. A powerful three-dimensional (3D) extension of the recently demonstrated generalized laws of refraction and reflection shows that the interface imparts a tangential wavevector to the incident light leading to anomalous beams, which in general are noncoplanar with the incident beam. The refracted beam direction can be controlled by varying the angle between the plane of incidence and the antenna array.

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Cited by 507 publications
(383 citation statements)
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“…[7][8][9][10][11][12][13][14] An array of such nanoantennas can form a metasurface to bend the light abnormally 7,8 in a fairly broad range of wavelengths and can create, for example, an optical vortex beam. 7,12 In addition, a metasurface arranged of plasmonic nano-antennas can be used as a very efficient coupler between propagating waves and surface waves.…”
Section: Introductionmentioning
confidence: 99%
“…[7][8][9][10][11][12][13][14] An array of such nanoantennas can form a metasurface to bend the light abnormally 7,8 in a fairly broad range of wavelengths and can create, for example, an optical vortex beam. 7,12 In addition, a metasurface arranged of plasmonic nano-antennas can be used as a very efficient coupler between propagating waves and surface waves.…”
Section: Introductionmentioning
confidence: 99%
“…This strategy resembles reflectarrays and transmit--arrays used at much lower frequencies [16--18]. Linear gradients of phase discontinuities lead to planar reflected and refracted wavefronts [15,19,20]. On the other hand, nonlinear phase gradients 3 lead to the formation of complex wavefronts such as helicoidal ones, which characterize vortex beams [21].…”
mentioning
confidence: 99%
“…7 It should be noted that a single layer of scatterers (due to their Lorentzian-shaped polarizability) only allow for full 2π-phase control of the cross-polarized light component, 8 meaning that such metasurfaces have a theoretical efficiency of maximum 25%, 9 though most realizations show efficiencies of a few percent. 10,11 In order to improve the efficiency of plasmonic metasurfaces, the low-frequency concept of transmit-and reflectarrays has been generalized and adopted to the visible and infrared regimes, where metasurfaces working in transmission consist of several layers in order to reach full phase control and proper impedance matching with surroundings. 9,12 Accordingly, such metasurfaces are quite complex to fabricate at near-infrared and visible frequencies, with a moderate efficiency of ∼ 20 − 50% due to Ohmic losses in the metal.…”
mentioning
confidence: 99%