Acta Optica Sinica (Online), Volume. 1, Issue 3, 0302001(2024)

Application of Polarization Holography in Fabrication of Optical Field Manipulation and Detection Devices (Invited)

Yi Yang1,2, Zhengyu Li1, Peiliang Qi1, Xueyan Chen1, Tian Ye1, Jinyu Wang1, Xinyi Yuan1, Shujun Zheng1, Xianmiao Xu1, and Xiaodi Tan1,2、*
Author Affiliations
  • 1Information Photonics Research Center, Fujian Normal University, Fuzhou 350117, Fujian , China
  • 2College of Photonic and Electronic Engineering, Key Laboratory of Optoelectronic Science and Technology for Medicine of Ministry of Education, Fujian Provincial Key Laboratory of Photonics Technology, Fujian Normal University, Fuzhou 350007, Fujian , China
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    Figures & Tables(24)
    Schematic of polarization holography. (a) Recording process of the polarization hologram; (b) process of reconstructed lightwave generated by the polarization hologram
    Schematic of experimental light path for fabricating a circular polarization generator[48]
    Fabrication process of a right circular polarization generator by p- polarization light as the reference light, depicting s and p+ components of the reconstructed light, respectively, and the upper right figures are the verification results of polarization handedness during faithful reconstruction[48]. (a) Reading light is s polarization light; (b) reading light is p- polarization light; (c) reading light is s+ip-; (d) reading light is s-ip-
    Schematic of polarization beam splitter[49]. (a) Schematic of polarization beam splitter preparation process; (b) schematic of functional realization of polarization beam splitter
    Reading waves are linear polarization light[49]. (a) Normalized diffraction efficiency of two reconstructed light with p and s polarized reconstruction light varies with polarization angle of reading light; (b) corresponding extinction ratio varies with polarization angle of reading light
    Principle of generating vector beam
    Experimental setup for fabricating vector beam generator[51]
    Results of generating vector beams[51]. (a) α=0; (b) α=π/4; (c) α=π/2; (d) α=3π/4
    Experimental setup for the preparation of vortex half-wave plates[52]
    Interference patterns of reconstruction waves with different topological charges[52].(a) Left-handed circular polarization reading light, m=0.5; (b) right-handed circular polarization reading light, m=0.5; (c) left-handed circular polarization reading light, m=1; (d) right-handed circular polarization reading light, m=1
    Experimental setup for generating vector vortex beams using an equivalent spiral half-wave plate[53]
    Vector vortex beams generated by a higher-order Poincaré sphere (l=0, p=1) [53]
    Vector vortex beams produced by a hybrid Poincaré sphere (l=2, p=-1)[53]
    Schematic of the experiment for preparing a circular polarization light detector[54]
    Diffracted images and intensity illuminated by various reading wave[54]. (a) 0°; (b) 15°; (c) 30°; (d) 45°; (e) 60°; (f) 75°; (g) 90°; (h) 105°; (i) 120°; (j) 135°; (k) 150°; (l) 165°
    Schematic of the polarization detector[55]. (a) Fabrication process; (b) polarization detection process
    Recording process of four polarization holograms[55]. (a) Polarization hologram l resembles a polarizer of transmission axis at 0°; (b) polarization hologram 2 resembles a polarizer of transmission axis at 45°; (c) polarization hologram 3 resembles a polarizer of transmission axis at 90°; (d) polarization hologram 4 resembles the combination of a QWP with fast axis at 45° and a polarizer of transmission axis at 0°
    Detection results of Stokes parameters for arbitrary polarization light[55]. (a) Reading light with different polarization states; (b) variations in the intensities of four reconstructed light with polarization state of reading light; (c) representation of the measured polarization states of reading light and their theoretical values on the Poincaré sphere
    • Table 1. Recording condition for circular polarization generator

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      Table 1. Recording condition for circular polarization generator

      RecordingReconstruction (A+B=0)
      G+G-F-F
      r+p-αs+βp-(-αiBcos ϑ+βBr+
      s-αB+βiB cos ϑr+
      l+p-αiBcos ϑ+βBl+
      s-αB-βiBcos ϑl+
    • Table 2. Recording conditions for the reproduction of linearly polarized light rotation

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      Table 2. Recording conditions for the reproduction of linearly polarized light rotation

      RecordingReconstruction
      G+G-F-F
      cos βp++sin βscos γp-+sin γscos αp-+sin αscos αp++sin αs
    • Table 3. Recording conditions for equivalent half-wave plates

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      Table 3. Recording conditions for equivalent half-wave plates

      RecordingReconstruction
      G+G-F-F
      cos βp++sin βssin βp--cos βsp-±isBe±iβp+∓is
    • Table 4. Recording conditions for vector beam generators based on equivalent vortex half-wave plates

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      Table 4. Recording conditions for vector beam generators based on equivalent vortex half-wave plates

      RecordingReconstruction
      G+G-F-F
      ei(cosβp++sinβssinβp--cosβsψr0p--is+ψl0p-+isBeilφe-2iβψr0p++is+e2iβψl0p+-is
    • Table 5. Preparation parameters of circular polarization detector based on null reconstruction effect

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      Table 5. Preparation parameters of circular polarization detector based on null reconstruction effect

      RecordingReconstruction
      G+G-F-F
      s-(1/cos θ)ip+l-r-0
      l-2Bs-(1/cos θ)ip+]+2Bs-cos θ ip+
      s+(1/cos θ)ip+r-r-2Bs+(1/cos θ)ip+]+2Bs+cos θ ip+
      l-0
    • Table 6. Recording conditions for four polarization holograms

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      Table 6. Recording conditions for four polarization holograms

      No.1234
      ϑ /(°)6.659.9313.1816.36
      G+0.76p++0.65s0.08p++1.00s-0.65p++0.76s0.72p++0.69is
      G--0.64p-+0.77s1.00p-+0.08s0.64p-+0.77s0.71p-+0.71is
      F--0.64p-+0.77s1.00p-+0.08s0.64p-+0.77s0.71p-+0.71is
      F+1.00p++0.00s0.70p++0.71s0.01p++1.00s0.71p+-0.71is
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    Yi Yang, Zhengyu Li, Peiliang Qi, Xueyan Chen, Tian Ye, Jinyu Wang, Xinyi Yuan, Shujun Zheng, Xianmiao Xu, Xiaodi Tan. Application of Polarization Holography in Fabrication of Optical Field Manipulation and Detection Devices (Invited)[J]. Acta Optica Sinica (Online), 2024, 1(3): 0302001

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    Paper Information

    Category: Research Articles

    Received: Jul. 2, 2024

    Accepted: Sep. 23, 2024

    Published Online: Nov. 8, 2024

    The Author Email: Tan Xiaodi (xtan@fjnu.edu.com)

    DOI:10.3788/AOSOL240437

    CSTR:32394.14.AOSOL240437

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