• Chinese Optics Letters
  • Vol. 19, Issue 12, 121401 (2021)
Qiang Zhang1, Boyuan Liu1, Qin Wen1, Jinhui Qin1, Yong Geng1, Qiang Zhou2, Guangwei Deng2, Kun Qiu1, and Heng Zhou1、*
Author Affiliations
  • 1Key Laboratory of Optical Fiber Sensing and Communication Networks, School of Information and Communication Engineering, University of Electronic Science and Technology of China, Chengdu 611731, China
  • 2Information and Quantum Laboratory, Institute of Fundamental and Frontier Sciences, University of Electronic Science and Technology of China, Chengdu 611731, China
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    DOI: 10.3788/COL202119.121401 Cite this Article Set citation alerts
    Qiang Zhang, Boyuan Liu, Qin Wen, Jinhui Qin, Yong Geng, Qiang Zhou, Guangwei Deng, Kun Qiu, Heng Zhou. Low-noise amplification of dissipative Kerr soliton microcomb lines via optical injection locking lasers[J]. Chinese Optics Letters, 2021, 19(12): 121401 Copy Citation Text show less
    Principles of OIL-based low-noise amplification of DKS microcomb lines. (a) Conventional multi-wavelength source consists of a large number of discrete lasers showing severe random frequency drift; (b) DKS microcomb generated by an external cavity laser diode (ECDL) amplified by using an EDFA, but at the sacrifice of OSNR degradation; (c) OIL-laser-based DKS microcomb amplification scheme provides simultaneous low noise and high gain. (d) A conceptual image of an integrated chip-scale optical data transmitter using DKS comb lines as WDM data carriers, which are power boosted using the OIL laser scheme.
    Fig. 1. Principles of OIL-based low-noise amplification of DKS microcomb lines. (a) Conventional multi-wavelength source consists of a large number of discrete lasers showing severe random frequency drift; (b) DKS microcomb generated by an external cavity laser diode (ECDL) amplified by using an EDFA, but at the sacrifice of OSNR degradation; (c) OIL-laser-based DKS microcomb amplification scheme provides simultaneous low noise and high gain. (d) A conceptual image of an integrated chip-scale optical data transmitter using DKS comb lines as WDM data carriers, which are power boosted using the OIL laser scheme.
    Characterization of a DKS microcomb generated in a WGM microcavity. (a) Experimental setup for DKS microcomb generation, linewidth measurement, laser injection locking, and coherent data transmission. (b) Microscopy image of WGM micro-rod resonator used in experiment. (c) Optical spectrum of a single-DKS comb state generated in a WGM micro-resonator. (d) Measured linewidths of 20 DKS comb lines adjacent to the pump laser. (e) Self-heterodyne interferometer beat note spectrum measured for the exemplified comb lines #5 and #10.
    Fig. 2. Characterization of a DKS microcomb generated in a WGM microcavity. (a) Experimental setup for DKS microcomb generation, linewidth measurement, laser injection locking, and coherent data transmission. (b) Microscopy image of WGM micro-rod resonator used in experiment. (c) Optical spectrum of a single-DKS comb state generated in a WGM micro-resonator. (d) Measured linewidths of 20 DKS comb lines adjacent to the pump laser. (e) Self-heterodyne interferometer beat note spectrum measured for the exemplified comb lines #5 and #10.
    Characterization of OIL-based DKS comb line amplification. (a), (b) Measured optical spectra of initial DKS comb lines and slave lasers after OIL. (c) Comparison of the optical spectra between OIL slave lasers and DKS comb lines amplified by two-stage EDFAs. (d), (e) Measured linewidth beat note RF spectra of free-running and OIL slave lasers by using the delayed self-heterodyne interferometer method. (f) Comparison of the beat note between two adjacent DKS micro-comb lines before and after OIL.
    Fig. 3. Characterization of OIL-based DKS comb line amplification. (a), (b) Measured optical spectra of initial DKS comb lines and slave lasers after OIL. (c) Comparison of the optical spectra between OIL slave lasers and DKS comb lines amplified by two-stage EDFAs. (d), (e) Measured linewidth beat note RF spectra of free-running and OIL slave lasers by using the delayed self-heterodyne interferometer method. (f) Comparison of the beat note between two adjacent DKS micro-comb lines before and after OIL.
    Comparison between the OIL-based low-noise amplification scheme and conventional EDFA scheme. The constellation diagrams of the received data plotted with blue represent the OIL scheme, and red is for the EDFA scheme. The BER for each channel is listed under each constellation diagram.
    Fig. 4. Comparison between the OIL-based low-noise amplification scheme and conventional EDFA scheme. The constellation diagrams of the received data plotted with blue represent the OIL scheme, and red is for the EDFA scheme. The BER for each channel is listed under each constellation diagram.
    Qiang Zhang, Boyuan Liu, Qin Wen, Jinhui Qin, Yong Geng, Qiang Zhou, Guangwei Deng, Kun Qiu, Heng Zhou. Low-noise amplification of dissipative Kerr soliton microcomb lines via optical injection locking lasers[J]. Chinese Optics Letters, 2021, 19(12): 121401
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