• Photonics Research
  • Vol. 9, Issue 1, 66 (2021)
Xinyu Wang1、2, Peng Xie1、2, Weiqiang Wang1、2、4、*, Yang Wang1、2, Zhizhou Lu1、2, Leiran Wang1、2, Sai T. Chu3, Brent E. Little1、2, Wei Zhao1、2, and Wenfu Zhang1、2、5、*
Author Affiliations
  • 1State Key Laboratory of Transient Optics and Photonics, Xi’an Institute of Optics and Precision Mechanics (XIOPM), Chinese Academy of Sciences (CAS), Xi’an 710119, China
  • 2University of Chinese Academy of Sciences, Beijing 100049, China
  • 3Department of Physics and Materials Science, City University of Hong Kong, Hong Kong, China
  • 4e-mail: wwq@opt.ac.cn
  • 5e-mail: wfuzhang@opt.ac.cn
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    DOI: 10.1364/PRJ.408612 Cite this Article Set citation alerts
    Xinyu Wang, Peng Xie, Weiqiang Wang, Yang Wang, Zhizhou Lu, Leiran Wang, Sai T. Chu, Brent E. Little, Wei Zhao, Wenfu Zhang. Program-controlled single soliton microcomb source[J]. Photonics Research, 2021, 9(1): 66 Copy Citation Text show less
    Schematic of program-controlled single SMC generation. (a) Diagram of program-controlled single SMC generation. A controller is used for microcomb data acquisition, microcomb states discrimination, and pump condition adjustment. An auxiliary laser is counter coupled into the cavity to stabilize the intracavity power for tuning speed independent single SMC generation. (b) Diagram of the intracavity power evolution while the pump laser sweeps across the peak of resonance. (c) The lower boundary of the soliton existing range is nondegenerate while backward tuning the pump frequency or microcavity operation temperature, which provides an effective approach for deterministic soliton switching. (d) The soliton steps when intracavity solitons annihilate one by one. All the solitons have similar power under the same pump condition, which provides a simple soliton state discrimination criterion for program-controlled single SMC generation. ECDL: external cavity diode laser.
    Fig. 1. Schematic of program-controlled single SMC generation. (a) Diagram of program-controlled single SMC generation. A controller is used for microcomb data acquisition, microcomb states discrimination, and pump condition adjustment. An auxiliary laser is counter coupled into the cavity to stabilize the intracavity power for tuning speed independent single SMC generation. (b) Diagram of the intracavity power evolution while the pump laser sweeps across the peak of resonance. (c) The lower boundary of the soliton existing range is nondegenerate while backward tuning the pump frequency or microcavity operation temperature, which provides an effective approach for deterministic soliton switching. (d) The soliton steps when intracavity solitons annihilate one by one. All the solitons have similar power under the same pump condition, which provides a simple soliton state discrimination criterion for program-controlled single SMC generation. ECDL: external cavity diode laser.
    Experimental setup. (a) Experimental setup of program-controlled single SMC generation. An auxiliary laser assisted thermal balance scheme is employed for tuning speed independent single SMC generation. The microcomb states are discriminated by the microcomb power, and the pump condition is exactly controlled by a computer program. EFDA: erbium doped fiber amplifier; FPC: fiber polarization control; TEC: thermoelectric cooler; OSA: optical spectrum analyzer; BPF: band pass filter; and PC: personal computer. (b) A 14-pin butterfly packaged MRR device whose operation temperature can be precisely tuned using an external TEC controller. (c) Microscope image of the 49 GHz high-index doped silica glass microring resonators. (d) Flowchart of the control program. There are four microcomb power criteria for different microcomb states discrimination.
    Fig. 2. Experimental setup. (a) Experimental setup of program-controlled single SMC generation. An auxiliary laser assisted thermal balance scheme is employed for tuning speed independent single SMC generation. The microcomb states are discriminated by the microcomb power, and the pump condition is exactly controlled by a computer program. EFDA: erbium doped fiber amplifier; FPC: fiber polarization control; TEC: thermoelectric cooler; OSA: optical spectrum analyzer; BPF: band pass filter; and PC: personal computer. (b) A 14-pin butterfly packaged MRR device whose operation temperature can be precisely tuned using an external TEC controller. (c) Microscope image of the 49 GHz high-index doped silica glass microring resonators. (d) Flowchart of the control program. There are four microcomb power criteria for different microcomb states discrimination.
    Experimental results of program-controlled SMC generation. (a) The measured power trace of microcomb evolutionary process. The power of a single SMC is clamped in a range between −12 and −10 dBm. (b) The control signal waveforms of the TEC operation temperature and pump frequency. ① Forward tuning for microcomb generation. ② Backward tuning for deterministic single SMC generation. ③ Single SMC. (c) The typical optical spectra of different microcomb states. I, FWM frequency lines; II, modulational instability microcomb; III, four solitons; IV, two solitons; and V, single soliton. (d) The oscilloscope measured microcomb power trace when the program consecutively recycles.
    Fig. 3. Experimental results of program-controlled SMC generation. (a) The measured power trace of microcomb evolutionary process. The power of a single SMC is clamped in a range between 12 and 10  dBm. (b) The control signal waveforms of the TEC operation temperature and pump frequency. ① Forward tuning for microcomb generation. ② Backward tuning for deterministic single SMC generation. ③ Single SMC. (c) The typical optical spectra of different microcomb states. I, FWM frequency lines; II, modulational instability microcomb; III, four solitons; IV, two solitons; and V, single soliton. (d) The oscilloscope measured microcomb power trace when the program consecutively recycles.
    Performance of a single SMC. (a) The radio frequency spectrum. (b) The waveform of a single SMC, which has an intensity modulation of approximately 1%. (c) and (d) The repetition rate fluctuation of single SMC without and with the beating frequency locking, respectively.
    Fig. 4. Performance of a single SMC. (a) The radio frequency spectrum. (b) The waveform of a single SMC, which has an intensity modulation of approximately 1%. (c) and (d) The repetition rate fluctuation of single SMC without and with the beating frequency locking, respectively.
    Frequency shift of a single SMC. (a) The overlap optical spectra of a single SMC with frequency shift. (b) The beating RF spectra of the pump and reference lasers.
    Fig. 5. Frequency shift of a single SMC. (a) The overlap optical spectra of a single SMC with frequency shift. (b) The beating RF spectra of the pump and reference lasers.
    Xinyu Wang, Peng Xie, Weiqiang Wang, Yang Wang, Zhizhou Lu, Leiran Wang, Sai T. Chu, Brent E. Little, Wei Zhao, Wenfu Zhang. Program-controlled single soliton microcomb source[J]. Photonics Research, 2021, 9(1): 66
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