Acta Optica Sinica, Volume. 44, Issue 10, 1026030(2024)

Mid-Infrared Polarized Beam Combiner Based on Anomalous Reflective Metasurface

Lulu Yang1,2, Xin Wang1,2、*, Meng Zhang1,3, Suhui Yang1,3, and Jinying Zhang1,2
Author Affiliations
  • 1School of Optics and Photonics, Beijing Institute of Technology, Beijing 100081, China
  • 2Beijing Key Laboratory for Precision Optoelectronic Measurement Instrument and Technology, Beijing 100081, China
  • 3Key Laboratory of Photonics Information Technology, Ministry of Industry and Information Technology, Beijing 100081, China
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    Figures & Tables(8)
    Working principle and structure of metasurface polarized beam combiner. (a) Working principle of mid-infrared metasurface polarized beam combiner; (b) metasurface structure; (c) three-dimensional structure (left) and top view (right) of the unit cell
    Design principle of metasurface. (a) Reflection phases and (b) reflectivity of X-LP and Y-LP incident light induced by Si nano-antennas with different length L and width W; (c) comparison of the desired phase (Des. X and Des. Y ), the localized cell induced phase (Sim. X and Sim. Y), and the reflectance (Amp. X and Amp. Y) for X-LP and Y-LP incident light at 4.0 μm wavelength
    Simulation results at 4.0 μm wavelength. (a) Normalized far-field intensity distribution and (b) near-field transmission phase distribution of the reflected field when X-LP and Y-LP light incident on the metasurface at 11.54° and -11.54°, respectively; (c) normalized far-field intensity distribution and (d) near-field transmission phase distribution of the reflected field when both of X-LP and Y-LP light incident on the metasurface perpendicularly; (e) normalized far-field intensity distribution of 50 mrad divergence angle at 4.0 μm wavelength
    Simulation results in 3.9-4.1 μm wavelength band. Reflectance of (a) X-LP and Y-LP light within 3.9-4.1 μm wavelength band; (b) normalized far-field intensity distribution and (c) near-field transmission phase distribution of reflected field when X-LP and Y-LP light wavelengths are 3.9 μm and 4.1 μm.
    Transmission performance of the reflected beam. (a) Near filed intensity distribution and (b) phase distribution of reflected X-LP and Y-LP light; spot radii of reflected (c) X-LP and (d) Y-LP light transmitting to different distances
    Performance of polarized beam combining. (a) Variation of beam width with transmission distance after polarized beam combining; (b) comparison of output spectra before and after polarized beam combining
    • Table 1. Length L and width W of Si nano-antennas at different X positions

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      Table 1. Length L and width W of Si nano-antennas at different X positions

      Position /μm0-22-44-66-88-1010-1212-1414-1616-1818-20
      Length L /μm0.8751.1001.3000.8250.9251.1751.3250.5000.5500.725
      Width W /μm0.7250.5500.5001.3251.1750.9250.8251.3001.1000.875
    • Table 2. Response characteristics of metasurface beam combiner in the 3.9-4.1 μm band

      View table

      Table 2. Response characteristics of metasurface beam combiner in the 3.9-4.1 μm band

      Polarized lightTotal reflection efficiency /%Intensity in beam combiner direction /%Intensity in normal reflection direction /%Absorded intensity /%Transmitted intensity /%
      X-LP97.596.60.92.50
      Y-LP98.497.70.71.60
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    Lulu Yang, Xin Wang, Meng Zhang, Suhui Yang, Jinying Zhang. Mid-Infrared Polarized Beam Combiner Based on Anomalous Reflective Metasurface[J]. Acta Optica Sinica, 2024, 44(10): 1026030

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    Paper Information

    Category: Physical Optics

    Received: Dec. 28, 2023

    Accepted: Feb. 26, 2024

    Published Online: May. 6, 2024

    The Author Email: Wang Xin (wangxin@bit.edu.cn)

    DOI:10.3788/AOS232007

    CSTR:32393.14.AOS232007

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