Citation: | Guo J Y, Wang T, Quan B G, Zhao H, Gu C Z et al. Polarization multiplexing for double images display. Opto-Electron Adv 2, 180029 (2019). doi: 10.29026/oea.2019.180029 |
[1] | Waller L, Tian L, Barbastathis G. Transport of intensity phase-amplitude imaging with higher order intensity derivatives. Opt Express 18, 12552-12561(2010). doi: 10.1364/OE.18.012552 |
[2] | de Boer J F, Milner T E, van Gemert M J C, Nelson J S. Two-dimensional birefringence imaging in biological tissue by polarization-sensitive optical coherence tomography. Opt Lett 22, 934-936(1997). doi: 10.1364/OL.22.000934 |
[3] | Cense B, Gao W H, Brown J M, Jones S M, Jonnal R S et al. Retinal imaging with polarization-sensitive optical coherence tomography and adaptive optics. Opt Express 17, 21634-21651(2009). doi: 10.1364/OE.17.021634 |
[4] | Upatnieks J, Marks J, Fedorowicz R. Color holograms for white light reconstruction. Appl Phys Lett 8, 286-287(1966). doi: 10.1063/1.1754441 |
[5] | Kong D Z, Shen X J, Shen Y Q, Wang X. Multi-image encryption based on interference of computer generated hologram. Optik125, 2365-2368(2014). doi: 10.1016/j.ijleo.2013.10.066 |
[6] | Cuche E, Bevilacqua F, Depeursinge C. Digital holography for quantitative phase-contrast imaging. Opt Lett 24, 291-293(1999). doi: 10.1364/OL.24.000291 |
[7] | Yue F Y, Wen D D, Xin J T, Gerardot B D, Li J S et al. Vector vortex beam generation with a single plasmonic metasurface. ACS Photonics 3, 1558-1563(2016). doi: 10.1021/acsphotonics.6b00392 |
[8] | Liu Y C, Ling X H, Yi X N, Zhou X X, Luo H L et al. Realization of polarization evolution on higher-order poincaré sphere with metasurface. Appl Phys Lett 104, 191110(2014). doi: 10.1063/1.4878409 |
[9] | Pors A, Nielsen M G, Della Valle G, Willatzen M, Albrektsen O et al. Plasmonic metamaterial wave retarders in reflection by orthogonally oriented detuned electrical dipoles. Opt Lett 36, 1626-1628(2011). doi: 10.1364/OL.36.001626 |
[10] | Blanchard R, Aoust G, Genevet P, Yu N F, Kats M A et al. Modeling nanoscale v-shaped antennas for the design of optical phased arrays. Phys Rev B 85, 155457(2012). doi: 10.1103/PhysRevB.85.155457 |
[11] | Fan K B, Suen J Y, Liu X Y, Padilla W J. All-dielectric metasurface absorbers for uncooled terahertz imaging. Optica 4, 601-604(2017). doi: 10.1364/OPTICA.4.000601 |
[12] | Chen Z H, Tao J, Gu J H, Li J, Hu D et al. Tunable metamaterial-induced transparency with gate-controlled on-chip graphene metasurface. Opt Express 24, 29216-29225(2016). doi: 10.1364/OE.24.029216 |
[13] | High A A, Devlin R C, Dibos A, Polking M, Wild D S et al. Visible-frequency hyperbolic metasurface. Nature 522, 192-196(2015). doi: 10.1038/nature14477 |
[14] | Arbabi E, Arbabi A, Kamali S M, Horie Y, Faraji-Dana M et al. MEMS-tunable dielectric metasurface lens. Nat Commun 9, 812(2018). doi: 10.1038/s41467-018-03155-6 |
[15] | Arbabi A, Arbabi E, Kamali S M, Horie Y, Han S et al. Miniature optical planar camera based on a wide-angle metasurface doublet corrected for monochromatic aberrations. Nat Commun 7, 13682(2016). doi: 10.1038/ncomms13682 |
[16] | Miyazaki H T, Kasaya T, Iwanaga M, Choi B, Sugimoto Y et al. Dual-band infrared metasurface thermal emitter for CO2 sensing. Appl Phys Lett 105, 121107(2014). doi: 10.1063/1.4896545 |
[17] | Heydari S, Rastan I, Parvin A, Pirooj A, Zarrabi F B. Investigation of novel fractal shape of the nano-aperture as a metasurface for bio sensing application. Phys Lett A 381, 140-144(2017). doi: 10.1016/j.physleta.2016.10.028 |
[18] | Wan W W, Gao J, Yang X D. Metasurface holograms for holographic imaging. Adv Opt Mater 5, 1700541(2017). doi: 10.1002/adom.201700541 |
[19] | Ni X J, Kildishev A V, Shalaev V M. Metasurface holograms for visible light. Nat Commun 4, 2807(2013). doi: 10.1038/ncomms3807 |
[20] | Wan W W, Gao J, Yang X D. Full-color plasmonic metasurface holograms. ACS Nano 10, 10671-10680(2016). doi: 10.1021/acsnano.6b05453 |
[21] | Ye W M, Zeuner F, Li X, Reineke B, He S et al. Spin and wavelength multiplexed nonlinear metasurface holography. Nat Commun 7, 11930(2016). doi: 10.1038/ncomms11930 |
[22] | Walter F, Li G X, Meier C, Zhang S, Zentgraf T. Ultrathin nonlinear metasurface for optical image encoding. Nano Lett 17, 3171-3175(2017). doi: 10.1021/acs.nanolett.7b00676 |
[23] | Li L L, Cui T J, Ji W, Liu S, Ding J et al. Electromagnetic reprogrammable coding-metasurface holograms. Nat Commun 8, 197(2017). doi: 10.1038/s41467-017-00164-9 |
[24] | Li Y B, Li L L, Xu B B, Wu W, Wu R Y et al. Transmission-type 2-bit programmable metasurface for single-sensor and single-frequency microwave imaging. Sci Rep 6, 23731(2016). doi: 10.1038/srep23731 |
[25] | Dong D S, Yang J, Cheng Q, Zhao J, Gao L H et al. Terahertz broadband low-reflection metasurface by controlling phase distributions. Adv Opt Mater 3, 1405-1410(2015). doi: 10.1002/adom.201500156 |
[26] | Orazbayev B, Estakhri N M, Beruete M, Alù A. Terahertz carpet cloak based on a ring resonator metasurface. Phys Rev B 91, 195444(2015). doi: 10.1103/PhysRevB.91.195444 |
[27] | Yao Y, Shankar R, Kats M A, Song Y, Kong J et al. Electrically tunable metasurface perfect absorbers for ultrathin mid-infrared optical modulators. Nano Lett 14, 6526-6532(2014). doi: 10.1021/nl503104n |
[28] | Mehmood M Q, Mei S T, Hussain S, Huang K, Siew S Y et al. Visible-frequency metasurface for structuring and spatially multiplexing optical vortices. Adv Mater 28, 2533-2539(2016). doi: 10.1002/adma.201504532 |
[29] | Deng Z L, Deng J H, Zhuang X, Wang S, Li K F et al. Diatomic metasurface for vectorial holography. Nano Lett 18, 2885-2892(2018). doi: 10.1021/acs.nanolett.8b00047 |
[30] | Almeida E, Bitton O, Prior Y. Nonlinear metamaterials for holography. Nat Commun 7, 12533(2016). doi: 10.1038/ncomms12533 |
[31] | Wang Q, Plum E, Yang Q L, Zhang X Q, Xu Q et al. Reflective chiral meta-holography: multiplexing holograms for circularly polarized waves. Light: Sci Appl 7, 25(2018). doi: 10.1038/s41377-018-0019-8 |
[32] | Zhang F, Pu M B, Li X, Gao P, Ma X L et al. All-dielectric metasurfaces for simultaneous giant circular asymmetric transmission and wavefront shaping based on asymmetric photonic spin-orbit interactions. Adv Funct Mater 27, 1204295(2017). doi: 10.1002/adfm.201704295 |
[33] | Li X P, Cao Y Y, Gu M. Superresolution-focal-volume induced 3.0 Tbytes/disk capacity by focusing a radially polarized beam. Opt Lett 36, 2510-2512(2011). doi: 10.1364/OL.36.002510 |
[34] | Gao H, Rosenberry M, Batelaan H. Light storage with light of arbitrary polarization. Phys Rev A 67, 053807(2003). doi: 10.1103/PhysRevA.67.053807 |
[35] | Rong L, Xiao W, Pan F, Liu S, Li R. Speckle noise reduction in digital holography by use of multiple polarization holograms. Chin Opt Lett 8, 653-655(2010). doi: 10.3788/COL |
[36] | Yuan C J, Situ G H, Pedrini G, Ma J, Osten W. Resolution improvement in digital holography by angular and polarization multiplexing. Appl Opt 50, B6-B11(2011). doi: 10.1364/AO.50.0000B6 |
[37] | Xie Z W, Lei T, Si G Y, Wang X Y, Lin J et al. Meta-holograms with full parameter control of wavefront over a 1000 nm bandwidth. ACS Photonics 4, 2158-2164(2017). doi: 10.1021/acsphotonics.7b00710 |
[38] | Yue F Y, Zhang C M, Zang X F, Wen D D, Gerardot B D et al. High-resolution grayscale image hidden in a laser beam. Light: Sci Appl 7, 17129(2018). doi: 10.1038/lsa.2017.129 |
[39] | Decker M, Staude I, Falkner M, Dominguez J, Neshev D N et al. High-efficiency dielectric huygens' surfaces. Adv Opt Mater 3, 813-820(2015). doi: 10.1002/adom.v3.6 |
[40] | Devlin R C, Khorasaninejad M, Chen W T, Oh J, Capasso F. Broadband high-efficiency dielectric metasurfaces for the visible spectrum. Proc Natl Acad Sci USA 113, 10473-10478(2016). doi: 10.1073/pnas.1611740113 |
[41] | Arbabi E, Arbabi A, Kamali S M, Horie Y, Faraon A. High efficiency double-wavelength dielectric metasurface lenses with dichroic birefringent meta-atoms. Opt Express 24, 18468-18477(2016). doi: 10.1364/OE.24.018468 |
[42] | Arbabi A, Horie Y, Bagheri M, Faraon A. Dielectric metasurfaces for complete control of phase and polarization with subwavelength spatial resolution and high transmission. Nat Nanotechnol 10, 937-943(2015). doi: 10.1038/nnano.2015.186 |
[43] | Mueller J P B, Rubin N A, Devlin R C, Groever B, Capasso F. Metasurface polarization optics: independent phase control of arbitrary orthogonal states of polarization. Phys Rev Lett 118, 113901(2017) doi: 10.1103/PhysRevLett.118.113901 |
(a) Schematics illustrating the principle and structural design of a metasurface. A uniform planar wave with right circular polarization is irradiated on the metasurface of spatial structural changes, the emitted light field will therefore carry varying amplitude and polarization in space. Intensity distribution is different in two orthogonal polarization components, so the patterns detected at different polarization angles will be different as shown in the left graphic. For viewing purpose, two images are staggered in diagram, but in reality, they are in the same position. (b) Front view of part of the metasurface, the nano bars are made of gold with varied sizes and rotations, the substrate is SiO2 with refractive index n=1.45.
All possibilities for binary image (0, 1) synthesis. There are four cases for intensity distributions in the x-polarization and y-polarization, namely, (0, 0), (0, 1), (1, 0) and (1, 1).
Vector composition diagram of binary images.
Experimental setup for polarized detection.
Experimental results of polarization detection.