• Acta Optica Sinica
  • Vol. 41, Issue 8, 0823014 (2021)
Xinliang Zhang1、* and Yanjing Zhao1、2
Author Affiliations
  • 1Wuhan National Laboratory for Optoelectronics & School of Optical and Electronic Information,Huazhong University of Science and Technology, Wuhan, Hubei 430074, China;
  • 2Department of Photonics Engineering, Technical University of Denmark, Lyngby DK- 2800, Denmark
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    DOI: 10.3788/AOS202141.0823014 Cite this Article Set citation alerts
    Xinliang Zhang, Yanjing Zhao. Research Progress of Microresonator-Based Optical Frequency Combs[J]. Acta Optica Sinica, 2021, 41(8): 0823014 Copy Citation Text show less
    Soliton microcavity optical frequency comb generation platforms
    Fig. 1. Soliton microcavity optical frequency comb generation platforms
    Soliton microcavity optical frequency comb generation methods
    Fig. 2. Soliton microcavity optical frequency comb generation methods
    Frequency tuning scheme. (a) Experimental setup of frequency tuning scheme[15]; (b) transmission power curve of microcavity[15]; (c) microcavity optical frequency comb spectra of primary comb, sub-comb, and MI state[15]; (d) superposition of transmission power curves of microcavity corresponding to multiple forward tuning[31]; (e) transmission power curves of microcavity during forward and reverse tuning [31]; (f) spectrum of multi solitons[15]; (g) spectrum of one soliton, inset shows the radio frequency signal from beat frequency[15]
    Fig. 3. Frequency tuning scheme. (a) Experimental setup of frequency tuning scheme[15]; (b) transmission power curve of microcavity[15]; (c) microcavity optical frequency comb spectra of primary comb, sub-comb, and MI state[15]; (d) superposition of transmission power curves of microcavity corresponding to multiple forward tuning[31]; (e) transmission power curves of microcavity during forward and reverse tuning [31]; (f) spectrum of multi solitons[15]; (g) spectrum of one soliton, inset shows the radio frequency signal from beat frequency[15]
    Auxiliary photothermal compensation scheme[51]. (a) Principle of auxiliary photothermal compensation scheme, the arrows indicate the position of pump and auxiliary laser during the frequency tuning; (b) transmission power curves of pump light, auxiliary light, and generated microcavity comb
    Fig. 4. Auxiliary photothermal compensation scheme[51]. (a) Principle of auxiliary photothermal compensation scheme, the arrows indicate the position of pump and auxiliary laser during the frequency tuning; (b) transmission power curves of pump light, auxiliary light, and generated microcavity comb
    Photorefractive effect[37]. (a) Transmission power curve of microcavity in reverse tuning process; (b) transmission power curve of microcavity in forward tuning process; (c) experimental results of soliton self starting and bidirectional conversion
    Fig. 5. Photorefractive effect[37]. (a) Transmission power curve of microcavity in reverse tuning process; (b) transmission power curve of microcavity in forward tuning process; (c) experimental results of soliton self starting and bidirectional conversion
    Physical mechanism of microcavity optical frequency comb
    Fig. 6. Physical mechanism of microcavity optical frequency comb
    Spectral characterizations of microcavity optical frequency comb. (a) Static spectra of primary comb, sub-comb, and MI state[15]; (b) static spectra of single-soliton, dual-soliton, and five-soliton[15]; (c) static spectrum of breather[69]; (d) intensity evolution of comb line at center and wing for breather[69]
    Fig. 7. Spectral characterizations of microcavity optical frequency comb. (a) Static spectra of primary comb, sub-comb, and MI state[15]; (b) static spectra of single-soliton, dual-soliton, and five-soliton[15]; (c) static spectrum of breather[69]; (d) intensity evolution of comb line at center and wing for breather[69]
    Temporal characterizations of microcavity optical frequency comb. (a) Measured results of autocorrelator[14]; (b) measured results of FROG method[80]; (c) measured result of dual-comb detection[81]; (d) measured results of temporal magnified system[83]
    Fig. 8. Temporal characterizations of microcavity optical frequency comb. (a) Measured results of autocorrelator[14]; (b) measured results of FROG method[80]; (c) measured result of dual-comb detection[81]; (d) measured results of temporal magnified system[83]
    RF spectral characterizations of microcavity optical frequency comb. (a) Low frequency noise measured by electric spectrum analyzer for single frequency pump, MI state and soliton state[14]; (b) fundamental frequency noise measured by electric spectrum analyzer for soliton state[15]; (c) RF spectrum measured by LISA system[35]; (d) harmonic evolution measured by LISA system for MI state and soliton state[85]
    Fig. 9. RF spectral characterizations of microcavity optical frequency comb. (a) Low frequency noise measured by electric spectrum analyzer for single frequency pump, MI state and soliton state[14]; (b) fundamental frequency noise measured by electric spectrum analyzer for soliton state[15]; (c) RF spectrum measured by LISA system[35]; (d) harmonic evolution measured by LISA system for MI state and soliton state[85]
    Micro-comb applications
    Fig. 10. Micro-comb applications
    Xinliang Zhang, Yanjing Zhao. Research Progress of Microresonator-Based Optical Frequency Combs[J]. Acta Optica Sinica, 2021, 41(8): 0823014
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