• High Power Laser Science and Engineering
  • Vol. 5, Issue 4, 04000e31 (2017)
Xiang Zhao1、2, Yifeng Yang1, Hui Shen1, Xiaolong Chen1, Gang Bai1、2, Jingpu Zhang1、2, Yunfeng Qi1, Bing He1、3, and Jun Zhou1、3、4、†
Author Affiliations
  • 1Shanghai Key Laboratory of All Solid-State Laser and Applied Techniques, Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Shanghai 201800, China
  • 2University of Chinese Academy of Sciences, Beijing 10049, China
  • 3Nanjing Institute of Advanced Laser Technology, Nanjing 210038, China
  • 4Nanjing Zhongke Shenguang Technology Co. Ltd., Nanjing 210038, China
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    DOI: 10.1017/hpl.2017.29 Cite this Article Set citation alerts
    Xiang Zhao, Yifeng Yang, Hui Shen, Xiaolong Chen, Gang Bai, Jingpu Zhang, Yunfeng Qi, Bing He, Jun Zhou. 302 W triple-frequency, single-mode, linearly polarized Yb-doped all-fiber amplifier[J]. High Power Laser Science and Engineering, 2017, 5(4): 04000e31 Copy Citation Text show less
    Experimental setup of monolithic fiber amplifier system (MO: master oscillator; PA, pre-amplifier; CO, collimator).
    Fig. 1. Experimental setup of monolithic fiber amplifier system (MO: master oscillator; PA, pre-amplifier; CO, collimator).
    (a) Simulated spectra and (b) experimental spectra of phase-modulated triple-frequency seed laser.
    Fig. 2. (a) Simulated spectra and (b) experimental spectra of phase-modulated triple-frequency seed laser.
    (a) Strain distribution along the active fiber. (b) SBS gain spectra of strained and unstrained fiber.
    Fig. 3. (a) Strain distribution along the active fiber. (b) SBS gain spectra of strained and unstrained fiber.
    Backward power as a function of the output power.
    Fig. 4. Backward power as a function of the output power.
    Overlap of the SBS gain spectra (a) without the modulation frequency; (b) with the modulation frequency of 1 GHz; (c) with the modulation frequency of 2 GHz [the short dashed line in (b) represents envelope of the total SBS gain].
    Fig. 5. Overlap of the SBS gain spectra (a) without the modulation frequency; (b) with the modulation frequency of 1 GHz; (c) with the modulation frequency of 2 GHz [the short dashed line in (b) represents envelope of the total SBS gain].
    Backward power as a function of the output power with different modulated frequencies.
    Fig. 6. Backward power as a function of the output power with different modulated frequencies.
    (a) Output power and backscattering power versus pump power. (b) Emission spectra of backward scattering. (c) Emission spectra of forward output laser. (d) FPI scanning spectra of triple frequency at the maximum output power.
    Fig. 7. (a) Output power and backscattering power versus pump power. (b) Emission spectra of backward scattering. (c) Emission spectra of forward output laser. (d) FPI scanning spectra of triple frequency at the maximum output power.
    Xiang Zhao, Yifeng Yang, Hui Shen, Xiaolong Chen, Gang Bai, Jingpu Zhang, Yunfeng Qi, Bing He, Jun Zhou. 302 W triple-frequency, single-mode, linearly polarized Yb-doped all-fiber amplifier[J]. High Power Laser Science and Engineering, 2017, 5(4): 04000e31
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