Chinese Journal of Lasers, Volume. 52, Issue 7, 0708002(2025)

Dual‑Pumped Optical Frequency Comb Based on Cavity‑Less Normal Dispersion Silicon Nitride Waveguides

Yao Zhang1, Yu Liu1, Yi Deng1, Kangping Zhong2, Suchun Feng1、*, and Fengping Yan3
Author Affiliations
  • 1Key Laboratory of All Optical Network and Advanced Telecommunication Network, Ministry of Education, Institute of Lightwave Technology, School of Electronic and Information Engineering, Beijing Jiaotong University, Beijing 100044, China
  • 2Department of Electrical and Electronic Engineering & Photonics Research Institute, the Hong Kong Polytechnic University, Hong Kong 999077, China
  • 3School of Electronic and Information Engineering, Beijing Jiaotong University, Beijing 100044, China
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    Figures & Tables(9)
    Dispersion engineering of Si3N4 waveguide. (a) Cross-section of Si3N4 waveguide; (b) simulated group velocity dispersion (GVD) varies with waveguide width when the waveguide height is fixed at 0.7 μm; (c) simulated GVD varies with waveguide height when the waveguide width is fixed at 2.8 μm; (d) Aeff and γ of TE0 mode in Si3N4 waveguide with 2.8 μm×0.7 μm cross section
    Generating optical frequency comb by utilizing two-stage pulse-compressed phase-locked dual-frequency laser injection into the cavity-less normal dispersion Si3N4 waveguide
    Time/frequency domain of the optical frequency comb (OFC) generated by directly pumping a normal-dispersion Si3N4 waveguide with a phase-locked dual-frequency laser without pulse compression. (a) Time domain; (b) frequency domain
    Time/frequency domain of the OFC generated by injecting the phase-locked dual-frequency laser with pulse compression into the normal dispersion Si3N4 waveguide at different stages of the scheme in Fig.2. (a) Position ①; (b) position ②; (c) position ③; (d) position ④; (e) position ⑤, before injecting phase-locked dual-frequency laser into Si3N4 waveguide; (f) output of Si3N4 waveguide
    Comparison of the OFCs generated by injecting different shapes of pulses into the Si3N4 waveguide. (a) Time/frequency domain of the pulses before injecting into the Si3N4 waveguide; (b) time/frequency domain of the OFCs output after injecting different pulses into the Si3N4 waveguide
    Time/frequency domain evolution of the OFC generated by the phase-locked dual-frequency laser with power ratio of 0.1at different stages of the scheme in Fig.2. (a) Position ①; (b) position ③; (c) position ⑤, before injecting phase-locked dual-frequency laser into Si3N4 waveguide; (d) OFC output by Si3N4 waveguide
    3 dB bandwidth of the OFC generated by phase-locked dual-frequency laser with different power ratios after Gaussian shaping
    Time/frequency domain evolution of the OFC generated by phase-locked dual-frequency laser with frequency spacing νm=0.2 THz at different stages of the scheme in Fig.2. (a) Position ①; (b) OFC output by Si3N4 waveguide
    3 dB bandwidth of the OFC generated by phase-locked dual-frequency laser with different frequency spacings after Gaussian shaping
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    Yao Zhang, Yu Liu, Yi Deng, Kangping Zhong, Suchun Feng, Fengping Yan. Dual‑Pumped Optical Frequency Comb Based on Cavity‑Less Normal Dispersion Silicon Nitride Waveguides[J]. Chinese Journal of Lasers, 2025, 52(7): 0708002

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    Paper Information

    Category: nonlinear optics

    Received: Nov. 27, 2024

    Accepted: Feb. 20, 2025

    Published Online: Apr. 15, 2025

    The Author Email: Suchun Feng (schfeng@bjtu.edu.cn)

    DOI:10.3788/CJL241394

    CSTR:32183.14.CJL241394

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