• Chinese Optics Letters
  • Vol. 21, Issue 9, 090002 (2023)
Can Li1、*, Yue Tao1, Man Jiang1, Pengfei Ma1、2、3, Wei Liu1、2、3, Rongtao Su1、2、3, Jiangming Xu1, Jinyong Leng1、2、3, and Pu Zhou1、**
Author Affiliations
  • 1College of Advanced Interdisciplinary Studies, National University of Defense Technology, Changsha 410073, China
  • 2Nanhu Laser Laboratory, National University of Defense Technology, Changsha 410073, China
  • 3Hunan Provincial Key Laboratory of High Energy Laser Technology, National University of Defense Technology, Changsha 410073, China
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    DOI: 10.3788/COL202321.090002 Cite this Article Set citation alerts
    Can Li, Yue Tao, Man Jiang, Pengfei Ma, Wei Liu, Rongtao Su, Jiangming Xu, Jinyong Leng, Pu Zhou. High-power single-frequency fiber amplifiers: progress and challenge [Invited][J]. Chinese Optics Letters, 2023, 21(9): 090002 Copy Citation Text show less
    Schematic configuration of a typical fiber MOPA system.
    Fig. 1. Schematic configuration of a typical fiber MOPA system.
    (a) Applied strain distribution along the gain fiber. (b) Calculated effective SBS gain spectra with and without strain[23].
    Fig. 2. (a) Applied strain distribution along the gain fiber. (b) Calculated effective SBS gain spectra with and without strain[23].
    Beam quality (M2 factor) versus the output power of a typical SFFA. Insets: beam profiles at selected output powers[35].
    Fig. 3. Beam quality (M2 factor) versus the output power of a typical SFFA. Insets: beam profiles at selected output powers[35].
    TMI threshold as a function of the relative intensity noise (RIN) of the pump and the seed. The artificially imprinted noise contains frequencies from 1 Hz up to 2 kHz. The impact of the pump intensity noise (blue dots) on the TMI threshold is significantly stronger than that of the seed intensity noise (red dots)[61].
    Fig. 4. TMI threshold as a function of the relative intensity noise (RIN) of the pump and the seed. The artificially imprinted noise contains frequencies from 1 Hz up to 2 kHz. The impact of the pump intensity noise (blue dots) on the TMI threshold is significantly stronger than that of the seed intensity noise (red dots)[61].
    Output power evolution of the CW single-frequency amplifiers in an all-fiber format operating in 1 µm, 1.5 µm, and 2 µm regions (an updated version of Fig. 7 in Ref. [13]).
    Fig. 5. Output power evolution of the CW single-frequency amplifiers in an all-fiber format operating in 1 µm, 1.5 µm, and 2 µm regions (an updated version of Fig. 7 in Ref. [13]).
    Experimental setup of the tapered YDF-based SFFA at 1030 nm. P-A, pre-amplifier; BPF, bandpass filter; LD, laser diode; PM, polarization maintaining; YDF, Yb-doped fiber[35].
    Fig. 6. Experimental setup of the tapered YDF-based SFFA at 1030 nm. P-A, pre-amplifier; BPF, bandpass filter; LD, laser diode; PM, polarization maintaining; YDF, Yb-doped fiber[35].
    Example of a transfer function for the pump and seed power modulation[110].
    Fig. 7. Example of a transfer function for the pump and seed power modulation[110].
    Phase-noise measurements of the fiber amplifier scaled as frequency noise[114].
    Fig. 8. Phase-noise measurements of the fiber amplifier scaled as frequency noise[114].
    Relative power noise of the combined beam in comparison with the single amplifier performance. Relative power noise variations are caused by the amplifier pumps[133].
    Fig. 9. Relative power noise of the combined beam in comparison with the single amplifier performance. Relative power noise variations are caused by the amplifier pumps[133].
    Can Li, Yue Tao, Man Jiang, Pengfei Ma, Wei Liu, Rongtao Su, Jiangming Xu, Jinyong Leng, Pu Zhou. High-power single-frequency fiber amplifiers: progress and challenge [Invited][J]. Chinese Optics Letters, 2023, 21(9): 090002
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