• Chinese Journal of Lasers
  • Vol. 45, Issue 8, 801001 (2018)
Huang Pei1、2、3, Gan Zebiao1, Li Wenqi1、2、3, Yu Lianghong1, Guo Zhen1、2, Cao He1、2、3, Wang Jianye1、2、3, Liang Xiaoyan1, and Li Ruxin1
Author Affiliations
  • 1[in Chinese]
  • 2[in Chinese]
  • 3[in Chinese]
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    DOI: 10.3788/CJL201845.0801001 Cite this Article Set citation alerts
    Huang Pei, Gan Zebiao, Li Wenqi, Yu Lianghong, Guo Zhen, Cao He, Wang Jianye, Liang Xiaoyan, Li Ruxin. Four-Outputs Nd∶glass Pump Source for Large Aperture Ti∶Sapphire Amplifier[J]. Chinese Journal of Lasers, 2018, 45(8): 801001 Copy Citation Text show less
    Layout of the four-outputs Nd∶glass pump source for 150 mm aperture Ti∶sapphire amplifier
    Fig. 1. Layout of the four-outputs Nd∶glass pump source for 150 mm aperture Ti∶sapphire amplifier
    Layout of regenerative amplifier
    Fig. 2. Layout of regenerative amplifier
    Layout of time-domain dual pulse pump
    Fig. 3. Layout of time-domain dual pulse pump
    Scheme of the combination of the same-polarization pump pulses
    Fig. 4. Scheme of the combination of the same-polarization pump pulses
    Relationship of front-end input and final-end output
    Fig. 5. Relationship of front-end input and final-end output
    Spatial evolutions of the pump source. (a) Front-end spot without amplification; (b) output spot without amplification;(c) output spot amplified by ?40 mm Nd∶glass rod amplifier; (d) output spot amplified by Nd∶glass rod amplifier chain
    Fig. 6. Spatial evolutions of the pump source. (a) Front-end spot without amplification; (b) output spot without amplification;(c) output spot amplified by ?40 mm Nd∶glass rod amplifier; (d) output spot amplified by Nd∶glass rod amplifier chain
    Time-domain wavefront evolutions of the pump source. (a) In the regenerative amplifier; (b) regenerative amplifier output; (c) pre-amplifier output; (d) after ?40 mm Nd∶glass rod amplifier; (e) after ?80 mm Nd∶glass rod amplifier; (f) after beam combination pumped by time-domain dual-pulse
    Fig. 7. Time-domain wavefront evolutions of the pump source. (a) In the regenerative amplifier; (b) regenerative amplifier output; (c) pre-amplifier output; (d) after ?40 mm Nd∶glass rod amplifier; (e) after ?80 mm Nd∶glass rod amplifier; (f) after beam combination pumped by time-domain dual-pulse
    Amplifier identifier40-180-180-280-380-480-580-680-780-8
    Small signal gains22.847.166.406.276.187.287.236.326.22
    RMS error /%2.85.76.89.55.89.72.59.68.9
    Table 1. Small signal gains and RMS error of the Nd∶glass rod amplifier
    ParameterE1-1E1-2E2-1E2-2
    Output average of basicfrequency /J178.0173.4175.6170.1
    Output average of doublefrequency /J77.977.678.274.7
    RMS of doublefrequency /%2.058.413.615.53
    Efficiency of doublefrequency /%43.844.844.543.9
    Table 2. Output of the pump source with front-end input of 13 mJ
    Huang Pei, Gan Zebiao, Li Wenqi, Yu Lianghong, Guo Zhen, Cao He, Wang Jianye, Liang Xiaoyan, Li Ruxin. Four-Outputs Nd∶glass Pump Source for Large Aperture Ti∶Sapphire Amplifier[J]. Chinese Journal of Lasers, 2018, 45(8): 801001
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