2015
DOI: 10.1007/s11468-015-9916-3
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High-Efficiency Cross Polarization Converters by Plasmonic Metasurface

Abstract: We have proposed a carefully designed metasurface constructed by the elongated apertures in gold film. This metasurface structure can support only single anomalous refractions for both circular polarization (CP) and linear polarization (LP) incidence, which is also following the generalized Snell's law, whereas the normal refraction can be completely suppressed nearly. Furthermore, the circularly polarized light converted to cross-polarized light and the linearly polarized light decomposed into two CP states w… Show more

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Cited by 30 publications
(11 citation statements)
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“…In general, a phase difference between adjacent elements in the array produces a sloped isophase plane, which deflects the beam and realizes beam steering. The beam deflection angle is proportional to the phase difference, which could be described by the generalized Snell's law [37,38]:…”
Section: Beam Steeringmentioning
confidence: 99%
“…In general, a phase difference between adjacent elements in the array produces a sloped isophase plane, which deflects the beam and realizes beam steering. The beam deflection angle is proportional to the phase difference, which could be described by the generalized Snell's law [37,38]:…”
Section: Beam Steeringmentioning
confidence: 99%
“…Furthermore, each pixel consists of an aperture with a determined orientation angle of θ along the x direction, which is fabricated in the gold film with the thickness of 40 nm, and the aperture dimension is 150 nm × 75 nm. The transmitted lights for the circularly polarized light incidence to the aperture can be decomposed into two circular polarization components, with one component possessing the same helicity as the incident light and a phase that does not depend on the orientation of the aperture, and the other with opposite helicity (cross polarization) to the incident light and a phase (Pancharatnam-Berry phase) [16,17] that is twice the orientation angle of the aperture. Therefore, an arbitrary phase simply can be achieved by controlling the orientation angles of the apertures, which greatly eases the encoding procedure of phase-only metalens.…”
Section: Designsmentioning
confidence: 99%
“…Optical metasurfaces, a two-dimensional planar variation of the concept of metamaterials, have been engineered to realize exotic electromagnetic properties by control of the phase, amplitude, and polarization of incident light, which are capable of being manipulated in a desirable manner [ 1 , 2 ]. A metasurface is usually composed of nano-antennas or nano-apertures because of introduced arbitrary abrupt phase shifts by adjusting geometric sizes [ 3 , 4 , 5 ]. Compared to the conventional optical devices, devices made from metasurfaces have the advantage of ultrathin, highly integrated, versatile, low-cost characteristics [ 6 , 7 , 8 ].…”
Section: Introductionmentioning
confidence: 99%