Chinese Journal of Lasers, Volume. 49, Issue 12, 1206003(2022)

Nonlinear Fourier Transform and Its Applications in Optical Communications and Pulse Characterizations

Fanglin Chen1, Yiqing Cao1, Yutian Wang1, Xiahui Tang1, Ming Tang1, Songnian Fu2, and Luming Zhao1、*
Author Affiliations
  • 1School of Optical and Electronic Information & Wuhan National Laboratory for Optoelectronics, Optics Valley Laboratory, Huazhong University of Science and Technology, Wuhan 430074, Hubei, China
  • 2Advanced Institute of Photonics Technology, School of Information Engineering, Guangdong University of Technology, Guangzhou 510006, Guangdong, China
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    Figures & Tables(16)
    Schemes of Fourier transform,inverse scattering transform and nonlinear Fourier transform[40]. (a) Fourier transform;(b) inverse scattering transform;(c) nonlinear Fourier transform
    Nonlinear spectrum of optical signal[43]
    Nonlinear frequency division multiplexing (NFDM) system[52]. (a) Block diagram of NFDM transmission system;(b) pre-compensation signal;(c)-(e) comparison of OFDM and NFDM transmission performance under different constellations
    Relationship between the ratio of discrete spectral energy to total pulse energy and chirp parameters C and product of Aτ [74]
    Evolution of non-steady state soliton pulse[74]. (a) Evolution of pulse;(b)-(c) evolution of discrete eigenvalues and continuous spectrum;(d) evolution of total energy,discrete spectrum energy and their ratio
    Evolution of steady-state soliton pulse[74]. (a) Evolution of pulse;(b)-(c) evolution of discrete eigenvalues and continuous spectrum;(d) evolution of total energy,discrete spectrum energy and their ratio
    NFT characterization and reconstruction of single soliton pulse[76]. (a) Continuous wave background;(b) evolution of dissipative soliton;(c) discrete eigenvalues;(d) pulse evolution reconstructed from discrete eigenvalues;(e) ratio of discrete spectrum energy to total pulse energy
    NFT reconstruction of three soliton pulses[76]. (a) Original pulse evolution;(b) pulse evolution obtained by NFT reconstruction
    Experimental setup of dissipative soliton full-field information collection[78]
    Eigenvalue distribution of unstable soliton[78]. (a)-(b) Eigenvalue distribution correspond to different states in breath cycle;(c)-(d) eigenvalue distribution correspond to double soliton and three-soliton cases
    Calculation process of nonlinear spectrum of mode-locked fiber laser[35]. (a) Experimental setup;(b) full-field reconstruction of mode-locked pulse obtained from single-sided spectrum;(c) relationship between time domain and nonlinear domain;(d) eigenvalue of pulse
    Real-time NFT data evolution obtained from measurement of fibre laser field[35]. (a)(e) Real-time spatio-temporal dynamics of laser evolution obtained from full-field measurements;(b)(c)(f)(g) instantaneous NFT spectra obtained in different round trips;(d)(h) real-time evolution of imaginary parts of two largest discrete eigenvalues
    Temporal profile and eigenvalue of a theoretical soliton and a mode-locked laser pulse[33]. (a) Temporal profile of a theoretical soliton;(b) eigenvalue of a theoretical soliton;(c) temporal profile arising in a mode-locked laser pulse;(d) eigenvalue distribution of a mode-locked laser pulse
    Temporal profiles and optical spectra of laser pulse,filtered soliton and theoretical soliton[33]. (a)Temporal profiles;(b) optical spectra
    NFT data evolution obtained from double pulses under unstable (a)-(d) and stable (e)-(l) states[34]. (a)(e)(i) Real-time spatial-temporal dynamics of laser evolution from full-field measurements;(b)(f)(j) evolution of imaginary parts of eigenvalues;(c)(g)(k) temporal profiles of laser pulse;(d)(h)(l) temporal profiles with soliton distillation
    • Table 1. Research progress of NFDM system

      View table

      Table 1. Research progress of NFDM system

      Multiplexing methodModulationSchemeResultYear
      Continuous spectrumQPSKCross-sea transmission7344 km2016[57]
      Continuous spectrum32QAMPre-compensation125 Gb/s,976 km2017[58]
      Continuous spectrum32QAMB-modulation100 Gb/s,976 km2017[60]
      Continuous spectrum32QAMDual-polarisation400 Gb/s,960 km2018[61]
      Continuous spectrumQPSKDual-polarisation200 Gb/s2019[62]
      Continuous spectrum16QAMWDM6.4 Tb/s,640 km2021[59]
      Discrete spectrumQPSKSpectral phase multiplexing7 Gb/s,1440 km2016[54]
      Discrete spectrum16APSKHigh-order modulation24 Gb/s,1050 km2017[63]
      Discrete spectrumQPSK/16QAMCarrier frequency offset estimationsCarrier frequency offset compensate2019[64]
      Discrete spectrumOOKANN demodulator2.5 Gb/s,3000 km2020[65]
      Discrete spectrum64APSKConstellation shaping960 km2021[55]
      Discrete spectrum16QAM/16APSKNIS54.4 Gb/s,1400 km2021[56]
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    Fanglin Chen, Yiqing Cao, Yutian Wang, Xiahui Tang, Ming Tang, Songnian Fu, Luming Zhao. Nonlinear Fourier Transform and Its Applications in Optical Communications and Pulse Characterizations[J]. Chinese Journal of Lasers, 2022, 49(12): 1206003

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    Paper Information

    Category: fiber optics and optical communications

    Received: Dec. 28, 2021

    Accepted: Feb. 28, 2022

    Published Online: Jun. 13, 2022

    The Author Email: Luming Zhao (lmzhao@hust.edu.cn)

    DOI:10.3788/CJL202249.1206003

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