• High Power Laser Science and Engineering
  • Vol. 11, Issue 6, 06000e72 (2023)
Yuxuan Liu1,2, Chengjie Zhu1,2, Yuxiang Sun1, Richard P. Mildren3..., Zhenxu Bai4, Baitao Zhang5, Weibiao Chen1,2, Dijun Chen1,2, Muye Li1,*, Xuezong Yang1,5,* and Yan Feng1,2|Show fewer author(s)
Author Affiliations
  • 1Hangzhou Institute for Advanced Study, University of Chinese Academy of Sciences, Hangzhou, China
  • 2Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Shanghai, China
  • 3MQ Photonics Research Centre, School of Mathematical and Physical Sciences, Macquarie University, Sydney, Australia
  • 4Center for Advanced Laser Technology, Hebei University of Technology, Tianjin, China
  • 5State Key Laboratory of Crystal Materials, Shandong University, Jinan, China
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    DOI: 10.1017/hpl.2023.67 Cite this Article Set citation alerts
    Yuxuan Liu, Chengjie Zhu, Yuxiang Sun, Richard P. Mildren, Zhenxu Bai, Baitao Zhang, Weibiao Chen, Dijun Chen, Muye Li, Xuezong Yang, Yan Feng, "High-power free-running single-longitudinal-mode diamond Raman laser enabled by suppressing parasitic stimulated Brillouin scattering," High Power Laser Sci. Eng. 11, 06000e72 (2023) Copy Citation Text show less
    Schematic of the free-running SLM diamond Raman laser. HR, high reflectivity mirror; HWP, half-wave plate; LP1200, long-pass filter cut at 1200 nm; BS, beam splitter; PM, power meter; FPI, scanning Fabry–Pérot interferometer.
    Fig. 1. Schematic of the free-running SLM diamond Raman laser. HR, high reflectivity mirror; HWP, half-wave plate; LP1200, long-pass filter cut at 1200 nm; BS, beam splitter; PM, power meter; FPI, scanning Fabry–Pérot interferometer.
    (a) The powers of the Stokes output (red spot) and residual pump (blue square) as a function of pump power. The inset is the Stokes beam profile at the maximum output power. (b) Long-term power stability of pump and Stokes output for 1 hour.
    Fig. 2. (a) The powers of the Stokes output (red spot) and residual pump (blue square) as a function of pump power. The inset is the Stokes beam profile at the maximum output power. (b) Long-term power stability of pump and Stokes output for 1 hour.
    (a), (c), (e) Plots of the spectral characteristics of Stokes outputs for different cavity lengths. (b), (d), (f) Plots of the FPI trace of Stokes outputs for different cavity lengths corresponding to (a), (c) and (e), respectively.
    Fig. 3. (a), (c), (e) Plots of the spectral characteristics of Stokes outputs for different cavity lengths. (b), (d), (f) Plots of the FPI trace of Stokes outputs for different cavity lengths corresponding to (a), (c) and (e), respectively.
    The linewidth of (a) pump and (b) Stokes outputs in the free-running V-shaped DRL. The red solid lines represent Lorentzian fits to the experimental data.
    Fig. 4. The linewidth of (a) pump and (b) Stokes outputs in the free-running V-shaped DRL. The red solid lines represent Lorentzian fits to the experimental data.
    (a) Wavelength stability of the Stokes and pump outputs for 1 hour. (b) Four typical FPI traces of the SLM Stokes output after multiple acquisitions.
    Fig. 5. (a) Wavelength stability of the Stokes and pump outputs for 1 hour. (b) Four typical FPI traces of the SLM Stokes output after multiple acquisitions.
    Yuxuan Liu, Chengjie Zhu, Yuxiang Sun, Richard P. Mildren, Zhenxu Bai, Baitao Zhang, Weibiao Chen, Dijun Chen, Muye Li, Xuezong Yang, Yan Feng, "High-power free-running single-longitudinal-mode diamond Raman laser enabled by suppressing parasitic stimulated Brillouin scattering," High Power Laser Sci. Eng. 11, 06000e72 (2023)
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