• Opto-Electronic Advances
  • Vol. 6, Issue 8, 220060 (2022)
Xin Li1、2, Qinmiao Chen3, Xue Zhang1, Ruizhe Zhao1, Shumin Xiao3、4、5、*, Yongtian Wang1、**, and Lingling Huang1、***
Author Affiliations
  • 1Beijing Engineering Research Center of Mixed Reality and Advanced Display, School of Optics and Photonics, Beijing Institute of Technology, Beijing 100081, China
  • 2MoE Key Laboratory of Photoelectronic Imaging Technology and System, and MIIT Key Laboratory of Photonics Information Technology, School of Optics and Photonics, Beijing Institute of Technology, Beijing 100081, China
  • 3State Key Laboratory on Tunable Laser Technology, Ministry of Industry and Information Technology Key Lab of Micro-Nano Optoelectronic Information System, Harbin Institute of Technology (Shenzhen), Shenzhen 518055, China
  • 4National Key Laboratory of Science and Technology on Advanced Composites in Special Environments, Harbin Institute of Technology, Harbin 150080, China
  • 5Collaborative Innovation Center of Extreme Optics, Shanxi University, Taiyuan 030006, China
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    DOI: 10.29026/oea.2023.220060 Cite this Article
    Xin Li, Qinmiao Chen, Xue Zhang, Ruizhe Zhao, Shumin Xiao, Yongtian Wang, Lingling Huang. Time-sequential color code division multiplexing holographic display with metasurface[J]. Opto-Electronic Advances, 2022, 6(8): 220060 Copy Citation Text show less
    (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.
    Fig. 1. (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.
    Fig. 2. 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 coefficientstxx of nanorods, respectively.
    Fig. 3. (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. (bg) 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 coefficientstxx 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.
    Fig. 4. (ab) 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).
    Fig. 5. 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).
    Xin Li, Qinmiao Chen, Xue Zhang, Ruizhe Zhao, Shumin Xiao, Yongtian Wang, Lingling Huang. Time-sequential color code division multiplexing holographic display with metasurface[J]. Opto-Electronic Advances, 2022, 6(8): 220060
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