• High Power Laser Science and Engineering
  • Vol. 9, Issue 1, 010000e8 (2021)
Enmao Song1、2, Guangzhi Zhu1、2、*, Hailin Wang1、2, Hantian Chen1、2, Yefeng Qian1、2, Kozlov Aleksei3, and Xiao Zhu1、2
Author Affiliations
  • 1School of Optical and Electronic Information, Huazhong University of Science andTechnology, Wuhan430074, China
  • 2National Engineering Research Center for Laser Processing, Wuhan430074, China
  • 3POLYUS Research Institute of M.F. Stelmakh Joint Stock Company, Moscow117342, Russia
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    DOI: 10.1017/hpl.2020.55 Cite this Article Set citation alerts
    Enmao Song, Guangzhi Zhu, Hailin Wang, Hantian Chen, Yefeng Qian, Kozlov Aleksei, Xiao Zhu. Up conversion and excited state absorption analysis in the Tm:YAG disk laser multi-pass pumped by 1 μm laser[J]. High Power Laser Science and Engineering, 2021, 9(1): 010000e8 Copy Citation Text show less
    Energy diagram of a Tm:YAG crystal.
    Fig. 1. Energy diagram of a Tm:YAG crystal.
    Fluorescence spectrum of a Tm:YAG crystal.
    Fig. 2. Fluorescence spectrum of a Tm:YAG crystal.
    Layout of the (a)20-pass pumping head and (b) 2 μm Tm:YAG disk laser multi-pass pumped by a 1 μm laser.
    Fig. 3. Layout of the (a)20-pass pumping head and (b) 2 μm Tm:YAG disk laser multi-pass pumped by a 1 μm laser.
    Absorption cross section of Tm:YAG and spectrum of pump light. Inset is the spectrum of output laser.
    Fig. 4. Absorption cross section of Tm:YAG and spectrum of pump light. Inset is the spectrum of output laser.
    Absorbed pump power of a Tm:YAG crystal versus input pump power under non-lasing and lasing conditions for 0.5 and 1 mm thickness of gain medium.
    Fig. 5. Absorbed pump power of a Tm:YAG crystal versus input pump power under non-lasing and lasing conditions for 0.5 and 1 mm thickness of gain medium.
    Output power of a Tm:YAG disk laser versus absorbed pump power for 0.5 and 1 mm thickness of gain medium. The inset shows the measured beam caustic and calculated beam quality at the output power of 1.05 W.
    Fig. 6. Output power of a Tm:YAG disk laser versus absorbed pump power for 0.5 and 1 mm thickness of gain medium. The inset shows the measured beam caustic and calculated beam quality at the output power of 1.05 W.
    Proportions of all the transitions for (a) 0.5 mm Tm:YAG disk laser and (b) 1 mm Tm:YAG thick disk laser under the lasing condition.
    Fig. 9. Proportions of all the transitions for (a) 0.5 mm Tm:YAG disk laser and (b) 1 mm Tm:YAG thick disk laser under the lasing condition.
    Fractional thermal loads of all transitions for (a) 0.5 mm Tm:YAG disk laser and (b) 1 mmTm:YAG thick disk laser under the lasing condition.
    Fig. 10. Fractional thermal loads of all transitions for (a) 0.5 mm Tm:YAG disk laser and (b) 1 mmTm:YAG thick disk laser under the lasing condition.
    Starting levelEnding levelSymbolValue
    1G43F2,3${\beta}_5^6$0.030
    1G43H4${\beta}_4^6$0.092
    1G43H5${\beta}_3^6$0.375
    1G43F4${\beta}_2^6$0.131
    1G43H6${\beta}_1^6$0.373
    Table 1. The branch ratios of a Tm:YAG crystal in the 1G4 state.
    ParametersValue
    Loss factor for laser in resonator(${L}_{loss}$)2%
    Cu–W plate thickness (${d}_{CuW}$)2 mm
    Thermal conductivity of Cu–W plate(${k}_{CuW}$)385 W/(m·K)
    Thermal conductivity of Tm:YAG crystal(${k}_{Tm: YAG}$)7 W/(m·K)[19]
    Convective heat transfer coefficient(${K}_{heat}$)10 W/(m2·K)[20]
    Radiative quantum efficiency of3F4 state (${\eta}_R^{3F4}$)0.98[21]
    Temperature of coolant fluid (${T}_{cool}$)292 K
    Table 2. Basic parameters used for the model.
    Enmao Song, Guangzhi Zhu, Hailin Wang, Hantian Chen, Yefeng Qian, Kozlov Aleksei, Xiao Zhu. Up conversion and excited state absorption analysis in the Tm:YAG disk laser multi-pass pumped by 1 μm laser[J]. High Power Laser Science and Engineering, 2021, 9(1): 010000e8
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