• High Power Laser Science and Engineering
  • Vol. 11, Issue 1, 01000e10 (2023)
Yulong Cui1、3, Xin Tian1、3, Binyu Rao1、3, Hao Li1、3, Wei Huang1、3, Wenxi Pei1、3, Meng Wang1、2、3, Zilun Chen1、2、3, and Zefeng Wang1、2、3、*
Author Affiliations
  • 1College of Advanced Interdisciplinary Studies, National University of Defense Technology, Changsha, China
  • 2Nanhu Laser Laboratory, National University of Defense Technology, Changsha, China
  • 3State Key Laboratory of Pulsed Power Laser Technology, Changsha, China
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    DOI: 10.1017/hpl.2022.43 Cite this Article Set citation alerts
    Yulong Cui, Xin Tian, Binyu Rao, Hao Li, Wei Huang, Wenxi Pei, Meng Wang, Zilun Chen, Zefeng Wang. A 110 W fiber gas Raman laser at 1153 nm[J]. High Power Laser Science and Engineering, 2023, 11(1): 01000e10 Copy Citation Text show less
    (a) Schematic diagram of the narrow-linewidth fiber oscillator. (b) Measured spectrum of the OC-FBG. (c) Spectrum of the output. Inset: fine spectrum around the central wavelength.
    Fig. 1. (a) Schematic diagram of the narrow-linewidth fiber oscillator. (b) Measured spectrum of the OC-FBG. (c) Spectrum of the output. Inset: fine spectrum around the central wavelength.
    (a) Experimental setup of the H2-filled FGRL. L: lens; R: reflector; PM: power meter; OSA: optical spectrum analyzer. Inset: thermal image of the input end of HC-PCF. (b) HCF end-cap. (c) Measured loss of the HC-PCF. Inset: cross-section of the HC-PCF.
    Fig. 2. (a) Experimental setup of the H2-filled FGRL. L: lens; R: reflector; PM: power meter; OSA: optical spectrum analyzer. Inset: thermal image of the input end of HC-PCF. (b) HCF end-cap. (c) Measured loss of the HC-PCF. Inset: cross-section of the HC-PCF.
    (a) Measured spectrum of the output laser at different pump powers when the fiber length is 5 m with the H2 pressure of 30 bar. (b) Measured spectrum of the output laser at different H2 pressures when the fiber length is 5 m with the maximum pump power. Inset: fine spectra of the pump, first-order Stokes laser and second-order Stokes laser. 3 dB linewidth of the output laser at (c) different pump powers and (d) different gas pressures.
    Fig. 3. (a) Measured spectrum of the output laser at different pump powers when the fiber length is 5 m with the H2 pressure of 30 bar. (b) Measured spectrum of the output laser at different H2 pressures when the fiber length is 5 m with the maximum pump power. Inset: fine spectra of the pump, first-order Stokes laser and second-order Stokes laser. 3 dB linewidth of the output laser at (c) different pump powers and (d) different gas pressures.
    (a) First-order Stokes power, (b) first-order Stokes efficiency and power spectral density of the pump, (c) second-order Stokes power and (d) residual pump power vary with coupled pump power at different gas pressures with the fiber length of 5 m.
    Fig. 4. (a) First-order Stokes power, (b) first-order Stokes efficiency and power spectral density of the pump, (c) second-order Stokes power and (d) residual pump power vary with coupled pump power at different gas pressures with the fiber length of 5 m.
    First-order Stokes power, second-order Stokes power and residual pump power vary with coupled pump power at 36 bar H2 pressure with the fiber length of 5 m. Inset: beam profile of the Stokes laser.
    Fig. 5. First-order Stokes power, second-order Stokes power and residual pump power vary with coupled pump power at 36 bar H2 pressure with the fiber length of 5 m. Inset: beam profile of the Stokes laser.
    (a) Experimental and simulated results of the Stokes and residual pump powers varying with the coupled pump power. The dotted lines represent the simulated results and the scatters represent the measured results. (b) Simulated first-order Stokes power varying with the coupled pump power at different fiber lengths.
    Fig. 6. (a) Experimental and simulated results of the Stokes and residual pump powers varying with the coupled pump power. The dotted lines represent the simulated results and the scatters represent the measured results. (b) Simulated first-order Stokes power varying with the coupled pump power at different fiber lengths.
    Yulong Cui, Xin Tian, Binyu Rao, Hao Li, Wei Huang, Wenxi Pei, Meng Wang, Zilun Chen, Zefeng Wang. A 110 W fiber gas Raman laser at 1153 nm[J]. High Power Laser Science and Engineering, 2023, 11(1): 01000e10
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