• Acta Optica Sinica
  • Vol. 40, Issue 16, 1614001 (2020)
Zhiyue Zhou1、2、3, Hao Li1、2、3, Yulong Cui1、2、3, Wei Huang1、2、3, and Zefeng Wang1、2、3、*
Author Affiliations
  • 1College of Advanced Interdisciplinary Studies, National University of Defense Technology, Changsha, Hunan 410073, China
  • 2State Key Laboratory of Pulsed Power Laser Technology, Changsha, Hunan 410073, China
  • 3Hunan Provincial Key Laboratory of High Energy Laser Technology, Changsha, Hunan 410073, China
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    DOI: 10.3788/AOS202040.1614001 Cite this Article Set citation alerts
    Zhiyue Zhou, Hao Li, Yulong Cui, Wei Huang, Zefeng Wang. Optically Pumped 4 μm CW HBr Gas Laser Based on Hollow-Core Fiber[J]. Acta Optica Sinica, 2020, 40(16): 1614001 Copy Citation Text show less
    Characteristics of HBr. (a) Schematic diagram of energy level transition of HBr molecules depicting 4 μm laser; (b) absorption spectrum of H79Br molecules at 2 μm band; (c) emission spectrum of H79Br molecules at 4 μm band
    Fig. 1. Characteristics of HBr. (a) Schematic diagram of energy level transition of HBr molecules depicting 4 μm laser; (b) absorption spectrum of H79Br molecules at 2 μm band; (c) emission spectrum of H79Br molecules at 4 μm band
    Tunable narrow linewidth 2 μm fiber pump source
    Fig. 2. Tunable narrow linewidth 2 μm fiber pump source
    Output characteristics of the tunable 2 μm fiber pump source. (a) Tunable output spectrum; (b) fine spectrum at R(2) absorption line; (c) measured wavelength change with the normalized tuning voltage; (d) output laser power change with the power of 793 nm LD
    Fig. 3. Output characteristics of the tunable 2 μm fiber pump source. (a) Tunable output spectrum; (b) fine spectrum at R(2) absorption line; (c) measured wavelength change with the normalized tuning voltage; (d) output laser power change with the power of 793 nm LD
    Characteristics of the pump laser linewidth. (a) Experimental setup for the measurement of the pump laser linewidth by F-P interferometer; (b) measured results of laser linewidth
    Fig. 4. Characteristics of the pump laser linewidth. (a) Experimental setup for the measurement of the pump laser linewidth by F-P interferometer; (b) measured results of laser linewidth
    Experimental setup (inset is the electron micrograph of hollow fiber cross section)
    Fig. 5. Experimental setup (inset is the electron micrograph of hollow fiber cross section)
    Absorption linewidth of HBr and the wavelength stability of pump source. (a) Measured HBr molecule absorption linewidth around R(2) absorption line at 1.8 mbar and 4.1 mbar; (b) residual pump power with respect to time when tuned at center of R(2) absorption line
    Fig. 6. Absorption linewidth of HBr and the wavelength stability of pump source. (a) Measured HBr molecule absorption linewidth around R(2) absorption line at 1.8 mbar and 4.1 mbar; (b) residual pump power with respect to time when tuned at center of R(2) absorption line
    Output 4 μm spectrum(inset is energy transition diagram of HBr for P(4) and R(2) emissions when pumped at R(2) absorption line)
    Fig. 7. Output 4 μm spectrum(inset is energy transition diagram of HBr for P(4) and R(2) emissions when pumped at R(2) absorption line)
    Characteristics of 4 μm laser output power. (a) Measured output 4 μm power and (b) optic-to-optic efficiency varies with incident pump power at different pressures; (c) measured 4 μm power and (d) optic-to-optic efficiency varies with coupled pump power at different pressures; (e) absorbed pump power as a function of coupled pump power; (f) measured absorbed pump power and the maximum output 4 μm laser power as a function of HBr pressures
    Fig. 8. Characteristics of 4 μm laser output power. (a) Measured output 4 μm power and (b) optic-to-optic efficiency varies with incident pump power at different pressures; (c) measured 4 μm power and (d) optic-to-optic efficiency varies with coupled pump power at different pressures; (e) absorbed pump power as a function of coupled pump power; (f) measured absorbed pump power and the maximum output 4 μm laser power as a function of HBr pressures
    Host glassDopantsPump wavelength /nmLaser wavelength /μmOutput power /WSlope efficiency /%Reference
    SilicateTm3+7932.05105053[3]
    SilicateTm3+, Ho3+7932.18342[4]
    SilicateHo3+19502.1414055[5]
    ZBLANTm3+10642.310.158[6]
    ZrF4Er3+9802.82441.622.9[7]
    FluorideEr3+9802.93830.516[8]
    ZBLANHo3+11503.0020.7712.4[9]
    ZBLANDy3+28303.151.0673[10]
    FluorideDy3+28303.2410.158[11]
    ZrF4Er3+976, 19763.423.438.6[12]
    ZrF4Er3+976, 19763.555.626.4[13]
    ZBLANEr3+970, 19733.52--3.680.62@3.68 μm25.1[14]
    ZBLANEr3+980, 19733.33--3.780.004@3.78 μm27[15]
    InF3Ho3+8883.920.210.2[16]
    Table 1. Characteristics of rare-earth-doped CW fiber lasers with emission wavelength above 2 μm
    R-branch absorptionWavelength /nmP-branch absorptionWavelength /nmR-branch emissionWavelength /nmP-branch emissionWavelength /nm
    R(11)1940.53P(1)1995.75R(11)3809.67P(1)4077.99
    R(10)1942.44P(2)2002.80R(10)3824.48P(2)4105.94
    R(9)1944.74P(3)2010.26R(9)3840.21P(3)4135.04
    R(8)1947.42P(4)2018.14R(8)3856.88P(4)4165.31
    R(7)1950.49P(5)2026.45R(7)3874.49P(5)4196.78
    R(6)1953.95P(6)2035.20R(6)3893.06P(6)4229.49
    R(5)1957.79P(7)2044.39R(5)3912.60P(7)4263.46
    R(4)1962.02P(8)2054.02R(4)3933.13P(8)4298.73
    R(3)1966.65P(9)2064.12R(3)3954.66P(9)4335.34
    R(2)1971.67P(10)2074.68R(2)3977.21P(10)4373.31
    R(1)1977.09P(11)2085.71R(1)4000.80P(11)4412.69
    R(0)1982.90P(12)2097.22R(0)4025.44P(12)4453.52
    Table 2. Absorption lines at 2 μm band and corresponding emission lines at 4 μm band of H79Br
    Zhiyue Zhou, Hao Li, Yulong Cui, Wei Huang, Zefeng Wang. Optically Pumped 4 μm CW HBr Gas Laser Based on Hollow-Core Fiber[J]. Acta Optica Sinica, 2020, 40(16): 1614001
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