• Photonics Research
  • Vol. 9, Issue 8, 1470 (2021)
Youpeng Xie1, Ting Lei1, Dawei Wang2, Jianxin Ren3, Yanmeng Dai1, Yanjun Chen2, Luping Du1, Bo Liu3、4、*, Zhaohui Li2、5、*, and Xiaocong Yuan1、6、*
Author Affiliations
  • 1Nanophotonics Research Centre, Shenzhen University, Shenzhen 518060, China
  • 2State Key Laboratory of Optoelectronic Material and Technologies and School of Electronics and Information Technology, Sun Yat-sen University, Guangzhou 510006, China
  • 3Institute of Optics and Electronics, Nanjing University of Information Science and Technology, Nanjing 210044, China
  • 4e-mail: bo@nuist.edu.cn
  • 5e-mail: lzhh88@mail.sysu.edu.cn
  • 6e-mail: xcyuan@szu.edu.cn
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    DOI: 10.1364/PRJ.416376 Cite this Article Set citation alerts
    Youpeng Xie, Ting Lei, Dawei Wang, Jianxin Ren, Yanmeng Dai, Yanjun Chen, Luping Du, Bo Liu, Zhaohui Li, Xiaocong Yuan. High-speed Stokes vector receiver enabled by a spin-dependent optical grating[J]. Photonics Research, 2021, 9(8): 1470 Copy Citation Text show less
    Schematic and phase distribution of the spin-dependent grating for LCP light. (a) Schematic of the spin-dependent grating. (b) Calculated phase distribution of the spin-dependent grating along with two magnified pictures of the liquid crystal molecule distributions and their phase distributions. (c) Phase distribution of the spin-dependent grating under a polarizing microscope.
    Fig. 1. Schematic and phase distribution of the spin-dependent grating for LCP light. (a) Schematic of the spin-dependent grating. (b) Calculated phase distribution of the spin-dependent grating along with two magnified pictures of the liquid crystal molecule distributions and their phase distributions. (c) Phase distribution of the spin-dependent grating under a polarizing microscope.
    (a) Setup for device characterization by measuring the arbitrary polarization states of light. (b) Experimental results for 72 sets of Stokes parameter measurements. PC, polarization controller; HWP, half-wave plate; QWP, quarter-wave plate; POL, polarizer; PD, photodetector.
    Fig. 2. (a) Setup for device characterization by measuring the arbitrary polarization states of light. (b) Experimental results for 72 sets of Stokes parameter measurements. PC, polarization controller; HWP, half-wave plate; QWP, quarter-wave plate; POL, polarizer; PD, photodetector.
    High-speed Stokes optical communication system. PMF, polarization-maintaining fiber; DP-IQ modulator, dual-polarization in-phase/quadrature modulator; AWG, arbitrary waveform generator; SMF, single-mode fiber; PC, polarization controller; EDFA, erbium-doped fiber amplifier; OTF, optical tunable filter; VOA, variable optical attenuator; POL, polarizer; Col, collimator; PD, photodetector.
    Fig. 3. High-speed Stokes optical communication system. PMF, polarization-maintaining fiber; DP-IQ modulator, dual-polarization in-phase/quadrature modulator; AWG, arbitrary waveform generator; SMF, single-mode fiber; PC, polarization controller; EDFA, erbium-doped fiber amplifier; OTF, optical tunable filter; VOA, variable optical attenuator; POL, polarizer; Col, collimator; PD, photodetector.
    Normalized polarizations of the 16QAM signals in the Stokes space.
    Fig. 4. Normalized polarizations of the 16QAM signals in the Stokes space.
    Stokes communication when using the spin-dependent grating as a receiver. (a) Plots of retrieved Stokes vectors on the Poincaré sphere for 32 GBd QPSK, 16 GBd 8PSK, and 16 GBd 16QAM signals. (b) Corresponding constellation diagrams for the vectors in (a). (c) Bit error rate (BER) curves of the 32 GBd QPSK, 16 GBd 8PSK, and 16 GBd 16QAM signals with received power. (d) BER curves of the 32 GBd QPSK, 16 GBd 8PSK, and 16 GBd 16QAM signals with different wavelengths.
    Fig. 5. Stokes communication when using the spin-dependent grating as a receiver. (a) Plots of retrieved Stokes vectors on the Poincaré sphere for 32 GBd QPSK, 16 GBd 8PSK, and 16 GBd 16QAM signals. (b) Corresponding constellation diagrams for the vectors in (a). (c) Bit error rate (BER) curves of the 32 GBd QPSK, 16 GBd 8PSK, and 16 GBd 16QAM signals with received power. (d) BER curves of the 32 GBd QPSK, 16 GBd 8PSK, and 16 GBd 16QAM signals with different wavelengths.
    Youpeng Xie, Ting Lei, Dawei Wang, Jianxin Ren, Yanmeng Dai, Yanjun Chen, Luping Du, Bo Liu, Zhaohui Li, Xiaocong Yuan. High-speed Stokes vector receiver enabled by a spin-dependent optical grating[J]. Photonics Research, 2021, 9(8): 1470
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