• High Power Laser Science and Engineering
  • Vol. 9, Issue 2, 02000e20 (2021)
Wei Gao1、2、3, Wenhui Fan1、3、5, Pei Ju1、3, Gang Li1、3, Yanpeng Zhang2、*, Aifeng He4, Qi Gao1、3, and Zhe Li1、3
Author Affiliations
  • 1State Key Laboratory of Transient Optics and Photonics, Xi’an Institute of Optics and Precision Mechanics, Chinese Academy of Sciences, Xi’an710119, China
  • 2Key Laboratory for Physical Electronics and Devices of the Ministry of Education & Shaanxi Key Laboratory of Information Photonic Technique, Xi’an Jiaotong University, Xi’an710049, China
  • 3University of Chinese Academy of Sciences, Beijing100049, China
  • 4Key Laboratory on Applied Physics and Chemistry, Shaanxi Applied Physics and Chemistry Research Institute, Xi’an710061, China
  • 5Collaborative Innovation Center of Extreme Optics, Shanxi University, Taiyuan030006, China
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    DOI: 10.1017/hpl.2021.13 Cite this Article Set citation alerts
    Wei Gao, Wenhui Fan, Pei Ju, Gang Li, Yanpeng Zhang, Aifeng He, Qi Gao, Zhe Li. Effective suppression of mode distortion induced by stimulated Raman scattering in high-power fiber amplifiers[J]. High Power Laser Science and Engineering, 2021, 9(2): 02000e20 Copy Citation Text show less
    Schematic of the experimental setup. CPS, cladding power stripper; ISO, fiber isolator; LD, laser diode; QBH, quartz block holder; YDF, Yb-doped double-cladding fiber.
    Fig. 1. Schematic of the experimental setup. CPS, cladding power stripper; ISO, fiber isolator; LD, laser diode; QBH, quartz block holder; YDF, Yb-doped double-cladding fiber.
    (a) Seed powers and backward powers under different pump powers. (b) Total output powers and backward powers under different pump powers at the seed power of 260 W.
    Fig. 2. (a) Seed powers and backward powers under different pump powers. (b) Total output powers and backward powers under different pump powers at the seed power of 260 W.
    (a) The far-field beam profile before this abrupt point (695 W). (b) The far-field beam profile after this abrupt point (774 W).
    Fig. 3. (a) The far-field beam profile before this abrupt point (695 W). (b) The far-field beam profile after this abrupt point (774 W).
    (a) Forward spectra near the abrupt point (at the output port). (b) Backward spectra near the abrupt point (at the rear port).
    Fig. 4. (a) Forward spectra near the abrupt point (at the output port). (b) Backward spectra near the abrupt point (at the rear port).
    (a) The total output powers and backward powers under different pump powers at the seed power of 181 W. (b) Beam quality at the total output power of 905 W (before the abrupt point) at the seed power of 181 W.
    Fig. 5. (a) The total output powers and backward powers under different pump powers at the seed power of 181 W. (b) Beam quality at the total output power of 905 W (before the abrupt point) at the seed power of 181 W.
    Threshold powers of the SRS-induced mode distortion under different seed powers.
    Fig. 6. Threshold powers of the SRS-induced mode distortion under different seed powers.
    (a) Total output powers and backward powers under different pump powers at the seed power of 260 W. (b) Beam quality at the total output power of 1001 W (before the abrupt point) at the seed power of 260 W.
    Fig. 7. (a) Total output powers and backward powers under different pump powers at the seed power of 260 W. (b) Beam quality at the total output power of 1001 W (before the abrupt point) at the seed power of 260 W.
    Threshold powers of the SRS-induced mode distortion under different forward feedback coefficients.
    Fig. 8. Threshold powers of the SRS-induced mode distortion under different forward feedback coefficients.
    Wei Gao, Wenhui Fan, Pei Ju, Gang Li, Yanpeng Zhang, Aifeng He, Qi Gao, Zhe Li. Effective suppression of mode distortion induced by stimulated Raman scattering in high-power fiber amplifiers[J]. High Power Laser Science and Engineering, 2021, 9(2): 02000e20
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