Advanced Photonics, Volume. 5, Issue 3, 036007(2023)

Submilliwatt, widely tunable coherent microcomb generation with feedback-free operation

Haowen Shu1、†, Lin Chang2, Chenghao Lao3, Bitao Shen1, Weiqiang Xie2, Xuguang Zhang1, Ming Jin1, Yuansheng Tao1, Ruixuan Chen1, Zihan Tao1, Huajin Chang1, Shaohua Yu1,4, Qifan Yang3,5, Xingjun Wang1,4,5、*, and John E. Bowers2、*
Author Affiliations
  • 1Peking University, School of Electronics, State Key Laboratory of Advanced Optical Communication Systems and Networks, Beijing, China
  • 2University of California, Santa Barbara, Department of Electrical and Computer Engineering, Santa Barbara, California, United States
  • 3Peking University, School of Physics, State Key Laboratory for Artificial Microstructure and Mesoscopic Physics, Beijing, China
  • 4Peng Cheng Laboratory, Shenzhen, China
  • 5Peking University, Frontiers Science Center for Nano-Optoelectronics, Beijing, China
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    Figures & Tables(7)
    Resonator characterization. (a) Top-view photograph of the AlGaAsOI microresonator. The radius of the microresonator is 144 μm, corresponding to 91 GHz FSR. Scale bar: 100 μm. (b) Normalized transmission spectrum of a typical resonance at 1552 nm. Lorentzian fitting reveals intrinsic Q factors about 2.36 × 106. (c) Scanning-electron-microscopy image showing the cross section of the microresonator. The AlGaAs core is highlighted in red, and silica forms the substrate and cladding. Scale bar: 200 nm. (d) Calculated dispersion of the TE0 mode in AlGaAsOI microresonators with respect to the width of the core. The thickness of the core is set as 400 nm. The inset shows the corresponding TE0 mode profile. (e) Measured TE0 mode family dispersion. Dint=ωμ−ωo−D1μ=D2μ2/2+O(μ3), where ωμ is the resonant frequency of the μth mode. The index of the mode that is pumped is set to 0, and D1 is the FSR at pump wavelength. Parabolic fitting (red) shows D2/2π=−1.63 MHz. (f) Zoom-in spectrum of the doublet resonances at μ=0 indicated in (e). The frequency is plotted relative to the fitting curve. (g) Pseudo-color plot of the relative frequency shifting of the coupled mode pairs from the ideal resonant frequency without the AMX effect, as a function of temperature.
    Dynamics of mode-locked microcombs. (a) Normalized transmitted total power (blue) and comb power (red). The laser is scanned from the blue side to the red side of the mode. Blue and red shadings indicate CW state and microcomb state, respectively. (b) Typical optical spectra of microcombs at different stages as indicated in (a). Red dashed lines denote the simulated spectral envelope. (c) Simulated intracavity waveforms corresponding to the spectra in (b). (d) Optical spectra of microcombs with spacing from 1 to 4 FSRs (top to bottom). Inset: intensity noise of the 1-FSR microcomb (resolution bandwidth: 100 kHz). The noise floor of the measurement system is also plotted for comparison.
    Power-efficient mode-locked Kerr comb generation. (a) Schematics of different microcomb generation schemes. (b) Comb spectrum at the flat step [shading area in upper panel (c)] under the on-chip pump power of <930 μW. (c) Measured comb power with respect to the frequency tuning. As the increasing of the pump power, the comb existence area could be extended from 0.3 GHz (upper panel) to 1.7 GHz (mid-panel) and then 11 GHz (lower panel). (d) Wide tuning of the dark-pulse microcomb for 97.5 GHz, which is over an entire FSR. (e) Experimental setup of an on-chip semiconductor laser pumped scheme and (f) comb spectrum. The right panel exhibits that dark-pulse spectrum can be repeatedly accessed with the laser current switched on and off, showing the “turnkey” behavior. All the spectra are of 2-FSR (∼180 GHz) frequency spacing. OSA, optical spectrum analyzer.
    Widely tunable frequency-chirped microcomb. (a) Both (i) bright soliton and (ii) dark pulse could act as a parallel frequency chirping source, in which the frequency modulation of the pump laser is transduced to each comb line. The stimulated Raman effects and higher-order dispersion would result in wavelength-dependent chirping copies, which could be mitigated in the efficient dark-pulse scheme with relatively low intracavity power. (b) Experimental setup of the parallel chirping source. WSS, wavelength-selective switch; WM, wavelength meter. (c) Measured time-frequency maps of the pump line (left panel) and the channel-10 sideband (right panel), with the pump laser chirping at 5 GHz (blue) and 10 GHz (red), respectively. (d) Frequency excursion of each channel at 10 GHz frequency chirping. (e) Experimental setup of the fast frequency modulation. An SSB modulator is employed as the chirping pump. The modulated comb lines are then charaterized by a heterodyne measurement. SSB, single-sideband modulator; OSC, oscilloscope. (f) Time-frequency maps of 5-GHz chirping pump and a comb line with modulation frequency of 400 kHz.
    Coherence of mode-locked frequency comb. (a) Experimental setup. PC, polarization controller; NF, notch filter; EDFA, erbium-doped fiber amplifier; BPF, bandpass filter; AOM, acousto-optic modulator; PD, photodetector; ESA, electric spectrum analyzer; OSC, oscilloscope. (b) Optical spectra of dark-pulse comb after NF. The range of telecommunication C-band is also indicated. (c) Left panel: measured RIN of comb teeth indicated in (b). Right panel: RIN at 10 MHz offset frequencies of all comb teeth within C-band. (d) Left panel: measured SSB frequency noise of comb teeth indicated in (b). Right panel: fundamental linewidth of all comb teeth within C-band.
    Long-term stability of the microcomb. The optical spectra of the microcomb are continuously recorded for over 7 h, and the total comb power (red) and power of the 10th comb line (blue) are plotted, showing 1.25 and 1 dB variations, respectively.
    • Table 1. Comparison of coherent microcomb generated with various integrated nonlinear platforms.

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      Table 1. Comparison of coherent microcomb generated with various integrated nonlinear platforms.

      PlatformComb typeQ-factor (106)FSR (GHz)On-chip Power (mW)Soliton Step (GHz)On-chip LaserAccessing Method
      Silica16Bright soliton> 2001525NPower kicking
      Si3N452Bright soliton15996.2NFrequency scanning
      Si3N453Bright soliton1.4a2302001.5NFrequency scanning
      Si3N43Bright soliton161530N/AYInjection locking
      GaN54Bright soliton1.8324136NManual frequency tuning (auxiliary laser)
      LiNbO355Bright soliton1.1a200900.5NBidirectional scanning
      LiNbO356Bright soliton2.2a199.7330.5NBidirectional scanning
      SiC57Bright soliton5.63502.30.014NFrequency tuning in cryostat
      Hydex58Soliton crystal1.548.91100NManual frequency tuning
      AlN59Bright soliton1.437433510.4NManual frequency tuning (auxiliary resonance)
      AlN60Bright soliton1.643339010NFrequency scanning
      Ta2O561Bright soliton0.4a1000363NFrequency scanning
      Si3N434Dark-pulse5.7104.82.50.25NFrequency scanning
      Si3N431Dark-pulse0.77a231.385037.5NThermally tuned resonance
      Si3N44Dark-pulse260520N/AYInjection locking
      Si3N462Dark-pulse>1026.25N/AYInjection locking
      AlGaAsOI (this work)Dark-pulse2.3690<0.93∼1500.397.5 (>1 FSR)YNo tuning, no feedback required
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    Haowen Shu, Lin Chang, Chenghao Lao, Bitao Shen, Weiqiang Xie, Xuguang Zhang, Ming Jin, Yuansheng Tao, Ruixuan Chen, Zihan Tao, Huajin Chang, Shaohua Yu, Qifan Yang, Xingjun Wang, John E. Bowers, "Submilliwatt, widely tunable coherent microcomb generation with feedback-free operation," Adv. Photon. 5, 036007 (2023)

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    Paper Information

    Category: Research Articles

    Received: Apr. 2, 2023

    Accepted: May. 8, 2023

    Published Online: Jun. 14, 2023

    The Author Email: Wang Xingjun (xjwang@pku.edu.cn), Bowers John E. (bowers@ece.ucsb.edu)

    DOI:10.1117/1.AP.5.3.036007

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