• Photonics Research
  • Vol. 10, Issue 9, 2107 (2022)
Ting Wang1、2, Ji-Liang Wu1、2, Xu-Cheng Zhang3, Yang Shi1、2, Yue-De Yang1、2, Jin-Long Xiao1、2, Da-Ming Zhang3, Guan-Shi Qin3, and Yong-Zhen Huang1、2、*
Author Affiliations
  • 1State Key Laboratory of Integrated Optoelectronics, Institute of Semiconductorshttps://ror.org/048dd0611, Chinese Academy of Sciences, Beijing 100083, China
  • 2Center of Materials Science and Optoelectronics Engineering, University of Chinese Academy of Sciences, Beijing 100049, China
  • 3State Key Laboratory of Integrated Optoelectronics, College of Electronic Science and Engineering, Jilin University, Changchun 130012, China
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    DOI: 10.1364/PRJ.462644 Cite this Article Set citation alerts
    Ting Wang, Ji-Liang Wu, Xu-Cheng Zhang, Yang Shi, Yue-De Yang, Jin-Long Xiao, Da-Ming Zhang, Guan-Shi Qin, Yong-Zhen Huang. Octave-spanning frequency comb generation based on a dual-mode microcavity laser[J]. Photonics Research, 2022, 10(9): 2107 Copy Citation Text show less
    Schematic diagram of the proposed octave-spanning OFC generator. EDFA, erbium-doped fiber amplifier; OBPF, optical bandpass filter; CIR, optical circulator; HNLF, highly nonlinear fiber; PC, polarization controller; OC, optical coupler; FBG, fiber Bragg grating.
    Fig. 1. Schematic diagram of the proposed octave-spanning OFC generator. EDFA, erbium-doped fiber amplifier; OBPF, optical bandpass filter; CIR, optical circulator; HNLF, highly nonlinear fiber; PC, polarization controller; OC, optical coupler; FBG, fiber Bragg grating.
    (a) Output power and applied voltage versus injection current. (b) Lasing spectra map versus injection current. (c) Wavelength interval and intensity ratio of dual modes versus injection current. (d) Lasing spectrum at injection current of 46 mA.
    Fig. 2. (a) Output power and applied voltage versus injection current. (b) Lasing spectra map versus injection current. (c) Wavelength interval and intensity ratio of dual modes versus injection current. (d) Lasing spectrum at injection current of 46 mA.
    (a) Output spectra of 50 GHz spaced Brillouin OFCs before and after optical spectral filtering of two FBGs. (b) Measured autocorrelation traces of the optical pulse train before and after optical filtering of two FBGs.
    Fig. 3. (a) Output spectra of 50 GHz spaced Brillouin OFCs before and after optical spectral filtering of two FBGs. (b) Measured autocorrelation traces of the optical pulse train before and after optical filtering of two FBGs.
    (a) Pulse width and pedestal intensity versus EDFA4 power. (b) Measured autocorrelation traces of optical pulses when the pump power is 550 mW. (c) Evolution of the optical spectrum versus EDFA4 power. (d) Optical spectrum of the octave-spanning OFC when pump power is 550 mW. The red line represents the dispersion of HNLF2. The dashed black curve is the simulated octave-spanning OFC spectrum. (e) Degree of coherence of the simulated spectrum.
    Fig. 4. (a) Pulse width and pedestal intensity versus EDFA4 power. (b) Measured autocorrelation traces of optical pulses when the pump power is 550 mW. (c) Evolution of the optical spectrum versus EDFA4 power. (d) Optical spectrum of the octave-spanning OFC when pump power is 550 mW. The red line represents the dispersion of HNLF2. The dashed black curve is the simulated octave-spanning OFC spectrum. (e) Degree of coherence of the simulated spectrum.
    (a) Octave-spanning OFC spectra and (b) corresponding fine spectra around the pump light, using square microcavity lasers with lasing mode frequency intervals of 29, 50, and 65 GHz.
    Fig. 5. (a) Octave-spanning OFC spectra and (b) corresponding fine spectra around the pump light, using square microcavity lasers with lasing mode frequency intervals of 29, 50, and 65 GHz.
    (a) Electrical spectrum characteristic of the 29-GHz octave-spanning OFC and filtered OFC around 1310 nm. (b) Electrical spectrum within 2-MHz span of the octave-spanning OFC. (c) Electrical spectrum within 1.5-MHz span obtained from the filtered OFC around 1310 nm. (d) Relative intensity noise of the octave-spanning OFC.
    Fig. 6. (a) Electrical spectrum characteristic of the 29-GHz octave-spanning OFC and filtered OFC around 1310 nm. (b) Electrical spectrum within 2-MHz span of the octave-spanning OFC. (c) Electrical spectrum within 1.5-MHz span obtained from the filtered OFC around 1310 nm. (d) Relative intensity noise of the octave-spanning OFC.
    Ting Wang, Ji-Liang Wu, Xu-Cheng Zhang, Yang Shi, Yue-De Yang, Jin-Long Xiao, Da-Ming Zhang, Guan-Shi Qin, Yong-Zhen Huang. Octave-spanning frequency comb generation based on a dual-mode microcavity laser[J]. Photonics Research, 2022, 10(9): 2107
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