• Photonics Research
  • Vol. 6, Issue 4, 326 (2018)
Qilai Zhao1, Zhitao Zhang1, Bo Wu2, Tianyi Tan1, Changsheng Yang1、3, Jiulin Gan1, Huihui Cheng1, Zhouming Feng1, Mingying Peng1, Zhongmin Yang1、4、5, and Shanhui Xu1、3、*
Author Affiliations
  • 1State Key Laboratory of Luminescent Materials and Devices and Institute of Optical Communication Materials, South China University of Technology, Guangzhou 510640, China
  • 2College of Optoelectronic Technology, Chengdu University of Information Technology, Chengdu 610225, China
  • 3Guangdong Engineering Technology Research and Development Center of High-Performance Fiber Laser Techniques and Equipments, Zhuhai 519031, China
  • 4Guangdong Engineering Technology Research and Development Center of Special Optical Fiber Materials and Devices, Guangzhou 510640, China
  • 5Guangdong Provincial Key Laboratory of Fiber Laser Materials and Applied Techniques, South China University of Technology, Guangzhou 510640, China
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    DOI: 10.1364/PRJ.6.000326 Cite this Article Set citation alerts
    Qilai Zhao, Zhitao Zhang, Bo Wu, Tianyi Tan, Changsheng Yang, Jiulin Gan, Huihui Cheng, Zhouming Feng, Mingying Peng, Zhongmin Yang, Shanhui Xu. Noise-sidebands-free and ultra-low-RIN 1.5  μm single-frequency fiber laser towards coherent optical detection[J]. Photonics Research, 2018, 6(4): 326 Copy Citation Text show less
    Experimental setup in different structures (a) with BOA without SIL, (b) with SIL without BOA, and (c) with BOA and SIL. FBG, fiber Bragg grating; PM-NB-FBG, PM narrow-band FBG; BB-FBG, broadband FBG; LD, laser diode; PM-WDM, PM wavelength division multiplexer; PM-CIR, PM circulator; PMI, PM isolator; PM-BPF, PM bandpass filter; PMTI, PM tap isolator; VOA, variable optical attenuator.
    Fig. 1. Experimental setup in different structures (a) with BOA without SIL, (b) with SIL without BOA, and (c) with BOA and SIL. FBG, fiber Bragg grating; PM-NB-FBG, PM narrow-band FBG; BB-FBG, broadband FBG; LD, laser diode; PM-WDM, PM wavelength division multiplexer; PM-CIR, PM circulator; PMI, PM isolator; PM-BPF, PM bandpass filter; PMTI, PM tap isolator; VOA, variable optical attenuator.
    RIN spectra of this single-frequency fiber laser with different conditions. The quantum noise limit of −152.9 dB/Hz is also shown for comparison. (a) 0 to 5 MHz. (b) 0 to 50 MHz.
    Fig. 2. RIN spectra of this single-frequency fiber laser with different conditions. The quantum noise limit of 152.9  dB/Hz is also shown for comparison. (a) 0 to 5 MHz. (b) 0 to 50 MHz.
    Measured signals of coherent light detection of this single-frequency fiber laser in different statuses.
    Fig. 3. Measured signals of coherent light detection of this single-frequency fiber laser in different statuses.
    (a) Optical spectra of this fiber laser at different output ports. The inset shows the degree of polarization of the final laser output (red dot) represented by a Poincaré sphere. (b) Measured single-longitudinal-mode characteristic of the final laser output.
    Fig. 4. (a) Optical spectra of this fiber laser at different output ports. The inset shows the degree of polarization of the final laser output (red dot) represented by a Poincaré sphere. (b) Measured single-longitudinal-mode characteristic of the final laser output.
    (a) Measured self-heterodyne spectra of this fiber laser with different conditions. (b) Measured frequency noise spectra and estimation line for evaluation of linewidth.
    Fig. 5. (a) Measured self-heterodyne spectra of this fiber laser with different conditions. (b) Measured frequency noise spectra and estimation line for evaluation of linewidth.
    Qilai Zhao, Zhitao Zhang, Bo Wu, Tianyi Tan, Changsheng Yang, Jiulin Gan, Huihui Cheng, Zhouming Feng, Mingying Peng, Zhongmin Yang, Shanhui Xu. Noise-sidebands-free and ultra-low-RIN 1.5  μm single-frequency fiber laser towards coherent optical detection[J]. Photonics Research, 2018, 6(4): 326
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