• Photonics Research
  • Vol. 12, Issue 3, 514 (2024)
Chenglong Zheng1, Hui Li2, Jingyu Liu3, Mengguang Wang4, Huaping Zang1、5、*, Yan Zhang3、6、*, and Jianquan Yao2
Author Affiliations
  • 1Key Laboratory of Material Physics, Ministry of Education, School of Physics and Microelectronics, Zhengzhou University, Zhengzhou 450052, China
  • 2Key Laboratory of Opto-Electronics Information Technology (Tianjin University), Ministry of Education, School of Precision Instruments and Opto-Electronics Engineering, Tianjin University, Tianjin 300072, China
  • 3Beijing Key Laboratory for Metamaterials and Devices, Key Laboratory of Terahertz Optoelectronics, Ministry of Education, and Beijing Advanced Innovation Center for Imaging Technology, Department of Physics, Capital Normal University, Beijing 100048, China
  • 4State Key Laboratory of Modern Optical Instrumentation, College of Optical Science and Engineering, Zhejiang University, Hangzhou 310027, China
  • 5e-mail: zanghuaping@zzu.edu.cn
  • 6e-mail: yzhang@mail.cnu.edu.cn
  • show less
    DOI: 10.1364/PRJ.512204 Cite this Article Set citation alerts
    Chenglong Zheng, Hui Li, Jingyu Liu, Mengguang Wang, Huaping Zang, Yan Zhang, Jianquan Yao. Full-Stokes metasurface polarimetry requiring only a single measurement[J]. Photonics Research, 2024, 12(3): 514 Copy Citation Text show less
    Schematic of the proposed multifocus metalens for polarization detection. For arbitrarily polarized wave incidence, this metalens converts each of the six polarized components (x-polarized, y-polarized, 45°-polarized, 135°-polarized, LCP, and RCP) of the incident wave into x polarization and focuses them individually at six positions on the same focal plane.
    Fig. 1. Schematic of the proposed multifocus metalens for polarization detection. For arbitrarily polarized wave incidence, this metalens converts each of the six polarized components (x-polarized, y-polarized, 45°-polarized, 135°-polarized, LCP, and RCP) of the incident wave into x polarization and focuses them individually at six positions on the same focal plane.
    Characterization of the selected meta-atoms. (a) Simulated phase shifts of the transmitted x-polarized (y-polarized) component under the x-polarized (y-polarized) incidence; (b) simulated transmission amplitudes and phase shifts of the transmitted x-polarized component under the y-polarized incidence; (c) transmission amplitudes and phase shifts of the transmitted x-polarized component under the 45°-polarized incidence; (d) transmission amplitudes and phase shifts of the transmitted x-polarized component under the 135°-polarized incidence; (e) transmission amplitudes and phase shifts of the transmitted x-polarized component under the LCP incidence; (f) transmission amplitudes and phase shifts of the transmitted x-polarized component under the RCP incidence.
    Fig. 2. Characterization of the selected meta-atoms. (a) Simulated phase shifts of the transmitted x-polarized (y-polarized) component under the x-polarized (y-polarized) incidence; (b) simulated transmission amplitudes and phase shifts of the transmitted x-polarized component under the y-polarized incidence; (c) transmission amplitudes and phase shifts of the transmitted x-polarized component under the 45°-polarized incidence; (d) transmission amplitudes and phase shifts of the transmitted x-polarized component under the 135°-polarized incidence; (e) transmission amplitudes and phase shifts of the transmitted x-polarized component under the LCP incidence; (f) transmission amplitudes and phase shifts of the transmitted x-polarized component under the RCP incidence.
    Characteristic of the proposed multifocus metalens for polarization detection: eight linearly polarized incidences. (a) Representation as points on the Poincaré sphere of the detected polarizations (*) and the incident ones (hexagrams); (b) comparison of the simulated azimuth angles and the theoretical ones; (c)–(j) intensity distribution of the transmitted x-polarized component and the comparison of polarization ellipses between the detected polarization states (red) and the incident ones (blue).
    Fig. 3. Characteristic of the proposed multifocus metalens for polarization detection: eight linearly polarized incidences. (a) Representation as points on the Poincaré sphere of the detected polarizations (*) and the incident ones (hexagrams); (b) comparison of the simulated azimuth angles and the theoretical ones; (c)–(j) intensity distribution of the transmitted x-polarized component and the comparison of polarization ellipses between the detected polarization states (red) and the incident ones (blue).
    Characteristic of the proposed multifocus metalens for polarization detection: eight elliptically polarized incidences (along the meridian direction). (a) Representation as points on the Poincaré sphere of the detected polarizations (*) and the incident ones (hexagrams); (b) full-Stokes parameters of the detected polarization states (purple) and the incident ones (orange); (c)–(j) intensity distributions of the transmitted x-polarized component and the comparisons of polarization ellipses between the detected polarization states (red) and the incident ones (blue).
    Fig. 4. Characteristic of the proposed multifocus metalens for polarization detection: eight elliptically polarized incidences (along the meridian direction). (a) Representation as points on the Poincaré sphere of the detected polarizations (*) and the incident ones (hexagrams); (b) full-Stokes parameters of the detected polarization states (purple) and the incident ones (orange); (c)–(j) intensity distributions of the transmitted x-polarized component and the comparisons of polarization ellipses between the detected polarization states (red) and the incident ones (blue).
    Characteristic of the proposed multifocus metalens for polarization detection: eight arbitrarily elliptically polarized incidences. (a) Full-Stokes parameters of the detected polarization states (purple) and the incident ones (orange); (b) representation as points on the Poincaré sphere of the detected polarizations (*) and the incident ones (hexagrams); (c)–(j) comparisons of polarization ellipses between the detected polarization states (red) and the incident ones (blue).
    Fig. 5. Characteristic of the proposed multifocus metalens for polarization detection: eight arbitrarily elliptically polarized incidences. (a) Full-Stokes parameters of the detected polarization states (purple) and the incident ones (orange); (b) representation as points on the Poincaré sphere of the detected polarizations (*) and the incident ones (hexagrams); (c)–(j) comparisons of polarization ellipses between the detected polarization states (red) and the incident ones (blue).
    Experimental characterization of the proposed multifocus metalens for polarization detection. (a), (b) SEM images of the fabricated metasurface; (c) representation as points on the Poincaré sphere of the measured polarizations (*) and the incident ones (hexagrams); (d)–(i) measured intensity distributions of the transmitted x-polarized component, and full-Stokes parameters of the measured polarization states and the incident ones.
    Fig. 6. Experimental characterization of the proposed multifocus metalens for polarization detection. (a), (b) SEM images of the fabricated metasurface; (c) representation as points on the Poincaré sphere of the measured polarizations (*) and the incident ones (hexagrams); (d)–(i) measured intensity distributions of the transmitted x-polarized component, and full-Stokes parameters of the measured polarization states and the incident ones.
    Intensity distributions of the transmitted x-polarized component under the different polarized incidences.
    Fig. 7. Intensity distributions of the transmitted x-polarized component under the different polarized incidences.
    Full-Stokes parameters of the detected polarization states (purple) and the incident ones (orange).
    Fig. 8. Full-Stokes parameters of the detected polarization states (purple) and the incident ones (orange).
    Intensity distributions of the transmitted x-polarized component under arbitrarily elliptically polarized incidences.
    Fig. 9. Intensity distributions of the transmitted x-polarized component under arbitrarily elliptically polarized incidences.
    y
    x12345678
    16670748854586264
    258140667648505658
    35012212264138444848
    43036981121221283030
    5128140808094102114116
    6981101206874808690
    778829813864707476
    872768212058626868
    Table 1. Detailed Structural Parameters (Length L1) of the Selected 64 Meta-atoms
    y
    x12345678
    166585036128967872
    27014052381381128274
    37414012640801209082
    4104781321088270140120
    5544813612690746460
    6585044132102827064
    762564432116867268
    864564830126967470
    Table 2. Detailed Structural Parameters (Width L2) of the Selected 64 Meta-atoms
    Chenglong Zheng, Hui Li, Jingyu Liu, Mengguang Wang, Huaping Zang, Yan Zhang, Jianquan Yao. Full-Stokes metasurface polarimetry requiring only a single measurement[J]. Photonics Research, 2024, 12(3): 514
    Download Citation