• Infrared and Laser Engineering
  • Vol. 49, Issue 9, 20201030 (2020)
Yaxin Zhang1、2, Mingbo Pu1、2, Yinghui Guo1、2, Jinjin Jin1, Xiong Li1、2, Xiaoliang Ma1、2, and Xiangang Luo1、2、*
Author Affiliations
  • 1State Key Laboratory of Optical Technologies on Nano-Fabrication and Micro-Engineering, Institute of Optics and Electronics, Chinese Academy of Sciences, Chengdu 610209, China
  • 2School of Optoelectronics, University of Chinese Academy of Sciences, Beijing 100049, China
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    DOI: 10.3788/IRLA20201030 Cite this Article
    Yaxin Zhang, Mingbo Pu, Yinghui Guo, Jinjin Jin, Xiong Li, Xiaoliang Ma, Xiangang Luo. Large field-of-view and compact full-Stokes polarimetry based on quadratic phase metasurface[J]. Infrared and Laser Engineering, 2020, 49(9): 20201030 Copy Citation Text show less
    Schematic illustration of metasurface of the compact polarimetry for large field of view. (a) Schematic diagram of rotational-translational symmetry conversion with quadratic phase metasurface; (b) Designed metasurface. The upper one is the top view of the designed metasurface, and the lower picture is illustration of a unit cell; (c) 3D schematic of the compact polarimetry for large field of view
    Fig. 1. Schematic illustration of metasurface of the compact polarimetry for large field of view. (a) Schematic diagram of rotational-translational symmetry conversion with quadratic phase metasurface; (b) Designed metasurface. The upper one is the top view of the designed metasurface, and the lower picture is illustration of a unit cell; (c) 3D schematic of the compact polarimetry for large field of view
    Designed unit cells. (a), (b) Short axis (W) and long axis (L) dimensions of the optimized unit cells; (c) Corresponding phases response of the first eight elements for incident angles of 0°, 10°, 20°, 30°, 40°, and 50°, respectively; (d) Corresponding transmitted amplitudes of all elements for incident angles of 0°, 10°, 20°, 30°, and 40°, respectively
    Fig. 2. Designed unit cells. (a), (b) Short axis (W) and long axis (L) dimensions of the optimized unit cells; (c) Corresponding phases response of the first eight elements for incident angles of 0°, 10°, 20°, 30°, 40°, and 50°, respectively; (d) Corresponding transmitted amplitudes of all elements for incident angles of 0°, 10°, 20°, 30°, and 40°, respectively
    Simulations verification of incident angle detection by the sub-array. (a) Focal focula intensity distribution at z=64 µm; (b) Calculated incident angles from Fig.3(a) and absolute errors
    Fig. 3. Simulations verification of incident angle detection by the sub-array. (a) Focal focula intensity distribution at z=64 µm; (b) Calculated incident angles from Fig.3(a) and absolute errors
    Characterization results of the metasurface. (a), (b), and (c) Simulation results at incident angles of 0°, 20°, and 40°, respectively. The incident light from left to right corresponds to X, Y, A, B, L, and R polarization states. The upper rows of every illustration are facula distributions at the focal plane. The lower rows are calculated normalized Stokes parameters corresponding with the upper one
    Fig. 4. Characterization results of the metasurface. (a), (b), and (c) Simulation results at incident angles of 0°, 20°, and 40°, respectively. The incident light from left to right corresponds to X, Y, A, B, L, and R polarization states. The upper rows of every illustration are facula distributions at the focal plane. The lower rows are calculated normalized Stokes parameters corresponding with the upper one
    Characterization of elliptically polarized light. (a) Diagram of intensity distributions at the focal plane; (b) Normalized Stokes parameters
    Fig. 5. Characterization of elliptically polarized light. (a) Diagram of intensity distributions at the focal plane; (b) Normalized Stokes parameters
    Yaxin Zhang, Mingbo Pu, Yinghui Guo, Jinjin Jin, Xiong Li, Xiaoliang Ma, Xiangang Luo. Large field-of-view and compact full-Stokes polarimetry based on quadratic phase metasurface[J]. Infrared and Laser Engineering, 2020, 49(9): 20201030
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