• Chinese Optics Letters
  • Vol. 18, Issue 5, 051402 (2020)
Chencheng Shen1、2, Xianglong Cai1、3, Youbao Sang1、2, Tiancheng Zheng1、2, Zhonghui Li1, Dong Liu1, Wanfa Liu1, and Jingwei Guo1、*
Author Affiliations
  • 1Key Laboratory of Chemical Lasers, Dalian Institute of Chemical Physics, Chinese Academy of Sciences, Dalian 116023, China
  • 2University of Chinese Academy of Sciences, Beijing 100049, China
  • 3School of Science, Changchun University of Science and Technology, Changchun 130022, China
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    DOI: 10.3788/COL202018.051402 Cite this Article Set citation alerts
    Chencheng Shen, Xianglong Cai, Youbao Sang, Tiancheng Zheng, Zhonghui Li, Dong Liu, Wanfa Liu, Jingwei Guo. Investigation of multispectral SF6 stimulated Raman scattering laser[J]. Chinese Optics Letters, 2020, 18(5): 051402 Copy Citation Text show less
    Schematic diagram of (a) cascade SRS and (b) cascade FWM.
    Fig. 1. Schematic diagram of (a) cascade SRS and (b) cascade FWM.
    Schematic diagram of the experimental setup.
    Fig. 2. Schematic diagram of the experimental setup.
    Spectra of the generated Raman frequency comb under the 532 nm pump for SF6 gas.
    Fig. 3. Spectra of the generated Raman frequency comb under the 532 nm pump for SF6 gas.
    Pulse shapes of the S0, AS1 (normalized), S1 (normalized), and S4 (normalized) laser beams.
    Fig. 4. Pulse shapes of the S0, AS1 (normalized), S1 (normalized), and S4 (normalized) laser beams.
    S1 photon conversion efficiencies under different pump energies and pressures of SF6.
    Fig. 5. S1 photon conversion efficiencies under different pump energies and pressures of SF6.
    Photon conversion efficiencies of S1, S2, S3, and AS1 versus the pump energies at 1.5 MPa SF6.
    Fig. 6. Photon conversion efficiencies of S1, S2, S3, and AS1 versus the pump energies at 1.5 MPa SF6.
    S1 conversion efficiencies versus the pump energies under 1.5 MPa H2 and SF6.
    Fig. 7. S1 conversion efficiencies versus the pump energies under 1.5 MPa H2 and SF6.
    S1 conversion efficiencies versus the pump energies of 1.5 MPa SF6 with He carrier gas under a repetition rate of 10 Hz. The pressures of He were 0 MPa, 0.5 MPa, 1.0 MPa, and 1.5 MPa, respectively. The vertical lines represent the error bars.
    Fig. 8. S1 conversion efficiencies versus the pump energies of 1.5 MPa SF6 with He carrier gas under a repetition rate of 10 Hz. The pressures of He were 0 MPa, 0.5 MPa, 1.0 MPa, and 1.5 MPa, respectively. The vertical lines represent the error bars.
    Stokes OrderWavelengthCalculated (nm)WavelengthMeasured (nm)Stokes OrderWavelengthCalculated (nm)WavelengthMeasured (nm)
    S0532.1532.9AS1511.0512.0
    S1555.0556.0AS2491.6493.0
    S2579.9581.0AS3473.5475.1
    S3607.2608.2AS4456.8458.3
    S4637.2638.2AS5441.1441.2
    S5670.3671.8AS6426.6426.9
    S6707.0708.2AS7412.9413.3
    S7748.0748.8AS8400.1400.6
    S8794.1795.4AS9388.1388.6
    S9846.1847.3AS10376.7377.2
    Table 1. SF6 SRS Line’s Wavelength of 532 nm Laser Pump
    Chencheng Shen, Xianglong Cai, Youbao Sang, Tiancheng Zheng, Zhonghui Li, Dong Liu, Wanfa Liu, Jingwei Guo. Investigation of multispectral SF6 stimulated Raman scattering laser[J]. Chinese Optics Letters, 2020, 18(5): 051402
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