Citation: | Li X, Chen QM, Zhang X, Zhao RZ, Xiao SM et al. Time-sequential color code division multiplexing holographic display with metasurface. Opto-Electron Adv 6, 220060 (2023). doi: 10.29026/oea.2023.220060 |
[1] | Ackermann G K, Eichler J. Holography: A Practical Approach (WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim, 2007). |
[2] | Xue GL, Liu J, Li X, Jia J, Zhang Z, et al. Multiplexing encoding method for full-color dynamic 3D holographic display. Opt Express 22, 18473–18482 (2014). doi: 10.1364/OE.22.018473 |
[3] | Zheng HD, Zhou CJ, Shui XH, Yu YJ. Computer-generated full-color phase-only hologram using a multiplane iterative algorithm with dynamic compensation. Appl Opt 61, B262–B270 (2022). doi: 10.1364/AO.444756 |
[4] | Li X, Liu J, Zhao T, Wang YT. Color dynamic holographic display with wide viewing angle by improved complex amplitude modulation. Opt Express 26, 2349–2358 (2018). doi: 10.1364/OE.26.002349 |
[5] | Jia J, Wang YT, Liu J, Li X, Pan YJ, et al. Reducing the memory usage for effectivecomputer-generated hologram calculation using compressed look-up table in full-color holographic display. Appl Opt 52, 1404–1412 (2013). doi: 10.1364/AO.52.001404 |
[6] | Li J, Zhang YT, Li JN, Yan X, Liang LJ, et al. Amplitude modulation of anomalously reflected terahertz beams using all-optical active Pancharatnam–Berry coding metasurfaces. Nanoscale 11, 5746–5753 (2019). doi: 10.1039/C9NR00675C |
[7] | Huang K, Liu H, Garcia-Vidal FJ, Hong MH, Luk’yanchuk B, et al. Ultrahigh-capacity non-periodic photon sieves operating in visible light. Nat Commun 6, 7059 (2015). doi: 10.1038/ncomms8059 |
[8] | Yu NF, Genevet P, Kats MA, Aieta F, Tetienne JP, et al. Light propagation with phase discontinuities: generalized laws of reflection and refraction. Science 334, 333–337 (2011). doi: 10.1126/science.1210713 |
[9] | Decker M, Staude I, Falkner M, Dominguez J, Neshev DN, et al. High‐efficiency dielectric Huygens’ surfaces. Adv Opt Mater 3, 813–820 (2015). doi: 10.1002/adom.201400584 |
[10] | Zhu LX, Liu X, Sain B, Wang MY, Schlickriede C, et al. A dielectric metasurface optical chip for the generation of cold atoms. Sci Adv 6, eabb6667 (2020). doi: 10.1126/sciadv.abb6667 |
[11] | Sain B, Meier C, Zentgraf T. Nonlinear optics in all-dielectric nanoantennas and metasurfaces: a review. Adv Photonics 1, 024002 (2019). |
[12] | Guo XX, Ding YM, Duan Y, Ni XJ. Nonreciprocal metasurface with space–time phase modulation. Light Sci Appl 8, 123 (2019). doi: 10.1038/s41377-019-0225-z |
[13] | Rubin NA, D’Aversa G, Chevalier P, Shi ZJ, Chen WT, et al. Matrix Fourier optics enables a compact full-Stokes polarization camera. Science 365, eaax1839 (2019). doi: 10.1126/science.aax1839 |
[14] | Bao YJ, Wen L, Chen Q, Qiu CW, Li BJ. Toward the capacity limit of 2D planar Jones matrix with a single-layer metasurface. Sci Adv 7, eabh0365 (2021). doi: 10.1126/sciadv.abh0365 |
[15] | Sroor H, Huang YW, Sephton B, Naidoo D, Vallés A, et al. High-purity orbital angular momentum states from a visible metasurface laser. Nat Photonics 14, 498–503 (2020). doi: 10.1038/s41566-020-0623-z |
[16] | Guo XX, Ding YM, Chen X, Duan Y, Ni XJ. Molding free-space light with guided wave–driven metasurfaces. Sci Adv 6, eabb4142 (2020). doi: 10.1126/sciadv.abb4142 |
[17] | Kim J, Yang Y, Badloe T, Kim I, Yoon G, et al. Geometric and physical configurations of meta-atoms for advanced metasurface holography. InfoMat 3, 739–754 (2021). doi: 10.1002/inf2.12191 |
[18] | Jung C, Kim G, Jeong M, Jang J, Dong ZG, et al. Metasurface-driven optically variable devices. Chem Rev 121, 13013–13050 (2021). doi: 10.1021/acs.chemrev.1c00294 |
[19] | Gao H, Fan XH, Xiong W, Hong MH. Recent advances in optical dynamic meta-holography. Opto-Electron Adv 4, 210030 (2021). doi: 10.29026/oea.2021.210030 |
[20] | Zhao RZ, Huang LL, Wang YT. Recent advances in multi-dimensional metasurfaces holographic technologies. PhotoniX 1, 20 (2020). doi: 10.1186/s43074-020-00020-y |
[21] | Wen DD, Cadusch JJ, Meng JJ, Crozier KB. Light field on a chip: metasurface-based multicolor holograms. Adv Photonics 3, 024001 (2021). |
[22] | Fang XY, Ren HR, Gu M. Orbital angular momentum holography for high-security encryption. Nat Photonics 14, 102–108 (2020). doi: 10.1038/s41566-019-0560-x |
[23] | Kim G, Kim S, Kim H, Lee J, Badloe T, et al. Metasurface-empowered spectral and spatial light modulation for disruptive holographic displays. Nanoscale 14, 4380–4410 (2022). doi: 10.1039/D1NR07909C |
[24] | Li X, Chen LW, Li Y, Zhang XH, Pu MB, et al. Multicolor 3D meta-holography by broadband plasmonic modulation. Sci Adv 2, e1601102 (2016). doi: 10.1126/sciadv.1601102 |
[25] | Wan WW, Gao J, Yang XD. Full-color plasmonic metasurface holograms. ACS Nano 10, 10671–10680 (2016). doi: 10.1021/acsnano.6b05453 |
[26] | Deng ZL, Jin MK, Ye X, Wang S, Shi T, et al. Full-color complex-amplitude vectorial holograms based on multi-freedom metasurfaces. Adv Funct Mater 30, 1910610 (2020). doi: 10.1002/adfm.201910610 |
[27] | Hu YQ, Li L, Wang YJ, Meng M, Jin L, et al. Trichromatic and tripolarization-channel holography with noninterleaved dielectric metasurface. Nano Lett 20, 994–1002 (2020). doi: 10.1021/acs.nanolett.9b04107 |
[28] | Wang B, Dong FL, Li QT, Yang D, Sun CW, et al. Visible-frequency dielectric metasurfaces for multiwavelength achromatic and highly dispersive holograms. Nano Lett 16, 5235–5240 (2016). doi: 10.1021/acs.nanolett.6b02326 |
[29] | Huang YW, Chen WT, Tsai WY, Wu PC, Wang CM, et al. Aluminum plasmonic multicolor meta-hologram. Nano Lett 15, 3122–3127 (2015). doi: 10.1021/acs.nanolett.5b00184 |
[30] | Bao YJ, Yu Y, Xu HF, Guo C, Li JT, et al. Full-colour nanoprint-hologram synchronous metasurface with arbitrary hue-saturation-brightness control. Light Sci Appl 8, 95 (2019). doi: 10.1038/s41377-019-0206-2 |
[31] | Wei QS, Sain B, Wang YT, Reineke B, Li XW, et al. Simultaneous spectral and spatial modulation for color printing and holography using all-dielectric metasurfaces. Nano Lett 19, 8964–8971 (2019). doi: 10.1021/acs.nanolett.9b03957 |
[32] | Kim I, Jeong H, Kim J, Yang Y, Lee D, et al. Dual-band operating metaholograms with heterogeneous meta-atoms in the visible and near-infrared. Adv Opt Mater 9, 2100609 (2021). doi: 10.1002/adom.202100609 |
[33] | Kim J, Jeon D, Seong J, Badloe T, Jeon N, et al. Photonic encryption platform via dual-band vectorial metaholograms in the ultraviolet and visible. ACS Nano 16, 3546–3553 (2022). doi: 10.1021/acsnano.1c10100 |
[34] | Frese D, Wei QS, Wang YT, Cinchetti M, Huang LL, et al. Nonlinear bicolor holography using plasmonic metasurfaces. ACS Photonics 8, 1013–1019 (2021). doi: 10.1021/acsphotonics.1c00028 |
[35] | Yoon G, Kim J, Mun J, Lee D, Nam KT, et al. Wavelength-decoupled geometric metasurfaces by arbitrary dispersion control. Commun Phys 2, 129 (2019). doi: 10.1038/s42005-019-0232-7 |
[36] | Shi ZJ, Khorasaninejad M, Huang YW, Roques-Carmes C, Zhu AY, et al. Single-layer metasurface with controllable multiwavelength functions. Nano Lett 18, 2420–2427 (2018). doi: 10.1021/acs.nanolett.7b05458 |
[37] | Shaltout AM, Shalaev VM, Brongersma ML. Spatiotemporal light control with active metasurfaces. Science 364, eaat3100 (2019). doi: 10.1126/science.aat3100 |
[38] | Kim J, Seong J, Yang Y, Moon SW, Badloe T, et al. Tunable metasurfaces towards versatile metalenses and metaholograms: a review. Adv Photonics 4, 024001 (2022). |
[39] | Kim I, Kim WS, Kim K, Ansari MA, Mehmood MQ, et al. Holographic metasurface gas sensors for instantaneous visual alarms. Sci Adv 7, eabe9943 (2021). doi: 10.1126/sciadv.abe9943 |
[40] | Kim I, Jang J, Kim G, Lee J, Badloe T, et al. Pixelated bifunctional metasurface-driven dynamic vectorial holographic color prints for photonic security platform. Nat Commun 12, 3614 (2021). doi: 10.1038/s41467-021-23814-5 |
[41] | Li X, Zhao RZ, Wei QS, Geng GZ, Li JJ, et al. Code division multiplexing inspired dynamic metasurface holography. Adv Funct Mater 31, 2103326 (2021). doi: 10.1002/adfm.202103326 |
[42] | Rao R, Dianat S. Basics of Code Division Multiple Access (CDMA) (SPIE, Bellingham, Washington, 2005). |
[43] | Cox IJ, Sheppard CJR. Information capacity and resolution in an optical system. J Opt Soc Am A 3, 1152–1158 (1986). doi: 10.1364/JOSAA.3.001152 |
[44] | Zhan T, Xiong JH, Zou JY, Wu ST. Multifocal displays: review and prospect. PhotoniX 1, 10 (2020). doi: 10.1186/s43074-020-00010-0 |
[45] | Bao YJ, Yan JH, Yang XG, Qiu CW, Li BJ. Point-source geometric metasurface holography. Nano Lett 21, 2332–2338 (2021). doi: 10.1021/acs.nanolett.0c04485 |
[46] | Ren HR, Fang XY, Jang J, Bürger J, Rho J, et al. Complex-amplitude metasurface-based orbital angular momentum holography in momentum space. Nat Nanotechnol 15, 948–955 (2020). doi: 10.1038/s41565-020-0768-4 |
Supplementary information for Time-sequential color code division multiplexing holographic display with metasurface | |
Supplementary video |
(a) The schematic of color holographic display based on CDM and polarization multiplexing. The target color image can be reconstructed only when the correct code key reference illuminates on the metasurface with a correct linear polarization state. (b) Exhibits eight color code references. (c) and (d) Color images encoded and recorded for horizontal and vertical polarization channels, respectively.
Flowchart of optimization algorithm for dynamic multiwavelength CDM CGHs generation. MFA represents modified Fidoc algorithm for CDM holography according to ref.41. The target images are divided into three series of monochromic images for different color components, and they are encoded and synthesized as a multiwavelength CDM CGH.
(a) Schematic illustration of a titanium dioxide nanorod fabricated on a glass substrate, where H represents the height (600 nm for the samples), P denotes the period of a unit cell (360 nm in our verification), and W and L are the width and length of nanorods, respectively, whose ranges are from 50 nm to 310 nm. (b–g) The simulation scanning results obtained via RCWA for parameters optimizations involving incident wavelengths of 633 nm, 532 nm, and 460 nm. (b–d) and (e–g) are amplitude and phase transmission coefficients txx of nanorods, respectively.
(a–b) Top and oblique views of scanning electron microscopy images of fabricated samples, where the scale bar represents denotes 1 μm. (c) Experimental setup. LS, the supercontinuum laser source; OB1 and OB2, objective lens; PH, pinhole; L1–L4, convex lenses; P1 and P2, polarizer and analyzer; HWP, half-wave plate; DMD, digital micro-mirror device; AP, continuously variable iris diaphragm; MS, metasurface; CCD, charge coupled device.
Experimental results of multiplexing metasurface holographic color display. The images on the first row are reconstructed with horizontal linear polarization state and four frames from a video with vertical linear polarization are shown on the second row (see Movie S1).