• Photonics Research
  • Vol. 5, Issue 3, 207 (2017)
Xiaohong Hu1、2, Weiqiang Wang1、2、3, Leiran Wang1、2, Wenfu Zhang1、2、3、4、*, Yishan Wang1、5、*, and Wei Zhao1
Author Affiliations
  • 1State Key Laboratory of Transient Optics and Photonics, Xi’an Institute of Optics and Precision Mechanics, Chinese Academy of Science, Xi’an 710119, China
  • 2University of Chinese Academy of Sciences, Beijing 100049, China
  • 3China-UK Joint Research Center on Micro/Nano Photonics, Xi’an Institute of Optics and Precision Mechanics, Chinese Academy of Science, Xi’an 710119, China
  • 4e-mail: wfuzhang@opt.ac.cn
  • 5e-mail: Yshwang@opt.ac.cn
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    DOI: 10.1364/PRJ.5.000207 Cite this Article Set citation alerts
    Xiaohong Hu, Weiqiang Wang, Leiran Wang, Wenfu Zhang, Yishan Wang, Wei Zhao. Numerical simulation and temporal characterization of dual-pumped microring-resonator-based optical frequency combs[J]. Photonics Research, 2017, 5(3): 207 Copy Citation Text show less
    (a) Schematic diagram of dual-pumped OFC generation system. The two pump fields are coupled into a four-port MRR through the input port, and the generated OFC is measured at the drop port. (b) Energy diagram of non-degenerate FWM in the MRR.
    Fig. 1. (a) Schematic diagram of dual-pumped OFC generation system. The two pump fields are coupled into a four-port MRR through the input port, and the generated OFC is measured at the drop port. (b) Energy diagram of non-degenerate FWM in the MRR.
    Calculated GVD curve of the MRR used in the experiment.
    Fig. 2. Calculated GVD curve of the MRR used in the experiment.
    Numerically calculated 40 FSR comb spectra (left column) and field profiles (right column) at different pump powers. For clear viewing, only a part of the field profile is shown at each pump power. A cosine fit to the field intensity profile is exhibited as the blue circles.
    Fig. 3. Numerically calculated 40 FSR comb spectra (left column) and field profiles (right column) at different pump powers. For clear viewing, only a part of the field profile is shown at each pump power. A cosine fit to the field intensity profile is exhibited as the blue circles.
    Schematic diagram of the self-locked and dual-pumped OFC generation system. ISO, isolator; DL, delay line; D-PBF, dual passbands filter; OSA, optical spectrum analyzer; PM, power meter.
    Fig. 4. Schematic diagram of the self-locked and dual-pumped OFC generation system. ISO, isolator; DL, delay line; D-PBF, dual passbands filter; OSA, optical spectrum analyzer; PM, power meter.
    Experimentally measured (a) 10 FSR comb spectra and (b) the corresponding autocorrelation trace.
    Fig. 5. Experimentally measured (a) 10 FSR comb spectra and (b) the corresponding autocorrelation trace.
    (a) 40 FSR comb spectra. The experimentally measured and numerically calculated comb spectra based on Eq. (1a) are represented by the black solid and red dashed lines, respectively. (b) MRR output temporal intensity waveform measured with a fast photodetector. The inset shows the details of the temporal waveform resulting from the supermode beating.
    Fig. 6. (a) 40 FSR comb spectra. The experimentally measured and numerically calculated comb spectra based on Eq. (1a) are represented by the black solid and red dashed lines, respectively. (b) MRR output temporal intensity waveform measured with a fast photodetector. The inset shows the details of the temporal waveform resulting from the supermode beating.
    ItemSymbolValue
    Quality factorQ1.45×106
    Cavity lengthL3.72 mm
    Mode field areaAeff4.8  μm2
    Mode linewidthκ134  MHz
    Refractive indexn01.6
    FSRFSR49 GHz
    FinesseF367
    Nonlinearityγ110  W1km1
    GVDβ225  ps2/km
    Linear propagation lossαdB0.06  dB/cm
    Power coupling coefficientTc1.2×102
    Table 1. Physical Parameters of the MRR
    Xiaohong Hu, Weiqiang Wang, Leiran Wang, Wenfu Zhang, Yishan Wang, Wei Zhao. Numerical simulation and temporal characterization of dual-pumped microring-resonator-based optical frequency combs[J]. Photonics Research, 2017, 5(3): 207
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