• High Power Laser Science and Engineering
  • Vol. 13, Issue 2, 02000e15 (2025)
Xiao Chen1, Shanmin Huang1, Liangjin Huang1,2,3,*, Zhiping Yan1,2,3..., Zhiyong Pan1,2,3,*, Zongfu Jiang1,2,3 and Pu Zhou1,*|Show fewer author(s)
Author Affiliations
  • 1College of Advanced Interdisciplinary Studies, National University of Defense Technology, Changsha, China
  • 2Nanhu Laser Laboratory, National University of Defense Technology, Changsha, China
  • 3Hunan Provincial Key Laboratory of High Energy Laser Technology, National University of Defense Technology, Changsha, China
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    DOI: 10.1017/hpl.2024.91 Cite this Article Set citation alerts
    Xiao Chen, Shanmin Huang, Liangjin Huang, Zhiping Yan, Zhiyong Pan, Zongfu Jiang, Pu Zhou, "High-fidelity delivery of kilowatt-level single-mode lasers through a tapered multimode fiber over one hundred meters," High Power Laser Sci. Eng. 13, 02000e15 (2025) Copy Citation Text show less
    (a) Calculated results of effective index differences with different fiber parameters. (b) Measured fiber dimension profile of the tapered multimode fiber.
    Fig. 1. (a) Calculated results of effective index differences with different fiber parameters. (b) Measured fiber dimension profile of the tapered multimode fiber.
    Geometric and refractive descriptions of the tapered fiber: (a) geometric dimensions at both ends; (b) measured refractive index profile.
    Fig. 2. Geometric and refractive descriptions of the tapered fiber: (a) geometric dimensions at both ends; (b) measured refractive index profile.
    (a) Experimental setup for high-power delivery. (b) Relationship between the input and output power, and the total transmission efficiency.
    Fig. 3. (a) Experimental setup for high-power delivery. (b) Relationship between the input and output power, and the total transmission efficiency.
    (a) Recorded spectra at different output powers. (b) Beam quality M2 factors of the input and output laser.
    Fig. 4. (a) Recorded spectra at different output powers. (b) Beam quality M2 factors of the input and output laser.
    The evolutions of (a) signal and (b) Stokes power versus the injected Raman noise, and (c) the corresponding signal-to-SRS ratios in uniform fibers or the tapered fiber.
    Fig. 5. The evolutions of (a) signal and (b) Stokes power versus the injected Raman noise, and (c) the corresponding signal-to-SRS ratios in uniform fibers or the tapered fiber.
    Evolution of signal-to-SRS ratios as a function of the injected Raman noise in the tapered multimode fiber with laser power levels of 1000, 2000 and 3000 W.
    Fig. 6. Evolution of signal-to-SRS ratios as a function of the injected Raman noise in the tapered multimode fiber with laser power levels of 1000, 2000 and 3000 W.
    Spatially and spectrally resolved imaging results for the whole delivery path.
    Fig. 7. Spatially and spectrally resolved imaging results for the whole delivery path.
    Relationships between the initial Raman noise and the output properties with different fiber lengths and an injected signal power of 1000 W: (a) output signal power; (b) output Stokes power; (c) output signal-to-Stokes ratio.
    Fig. 8. Relationships between the initial Raman noise and the output properties with different fiber lengths and an injected signal power of 1000 W: (a) output signal power; (b) output Stokes power; (c) output signal-to-Stokes ratio.
    Relationships between the initial Raman noise and the output properties with different fiber lengths and an injected signal power of 2000 W: (a) output signal power; (b) output Stokes power; (c) output signal-to-Stokes ratio.
    Fig. 9. Relationships between the initial Raman noise and the output properties with different fiber lengths and an injected signal power of 2000 W: (a) output signal power; (b) output Stokes power; (c) output signal-to-Stokes ratio.
    Relationships between the initial Raman noise and the output properties with different fiber lengths and an injected signal power of 3000 W: (a) output signal power; (b) output Stokes power; (c) output signal-to-Stokes ratio.
    Fig. 10. Relationships between the initial Raman noise and the output properties with different fiber lengths and an injected signal power of 3000 W: (a) output signal power; (b) output Stokes power; (c) output signal-to-Stokes ratio.
    Xiao Chen, Shanmin Huang, Liangjin Huang, Zhiping Yan, Zhiyong Pan, Zongfu Jiang, Pu Zhou, "High-fidelity delivery of kilowatt-level single-mode lasers through a tapered multimode fiber over one hundred meters," High Power Laser Sci. Eng. 13, 02000e15 (2025)
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