• Chinese Optics Letters
  • Vol. 15, Issue 9, 091402 (2017)
Encai Ji, Mingming Nie, and Qiang Liu*
Author Affiliations
  • State Key Laboratory of Precision Measurement Technology and Instruments, Department of Precision Instrument, Tsinghua University, Beijing 100084, China
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    DOI: 10.3788/COL201715.091402 Cite this Article Set citation alerts
    Encai Ji, Mingming Nie, Qiang Liu. 13.5 mJ polarized 2.09 μm fiber-bulk holmium laser and its application to a mid-infrared ZnGeP2 optical parametric oscillator[J]. Chinese Optics Letters, 2017, 15(9): 091402 Copy Citation Text show less
    Layout of the TDFL-pumped Ho:YAG oscillator and amplifier system. (DM1, HT at 0.79 μm and HR at 1.91 μm; DM2, HT at 1.91 μm and HR at 2.09 μm; DM3, HT at p-polarized 2.09 μm and HR at 1.91 μm.)
    Fig. 1. Layout of the TDFL-pumped Ho:YAG oscillator and amplifier system. (DM1, HT at 0.79 μm and HR at 1.91 μm; DM2, HT at 1.91 μm and HR at 2.09 μm; DM3, HT at p-polarized 2.09 μm and HR at 1.91 μm.)
    (Color online) Typical output spectra of TDFL1. (a) The pump current was set at 1.40, 1.60, and 1.90 A, respectively; (b) the pump current was set at 1.45, 1.65, and 1.98 A, respectively.
    Fig. 2. (Color online) Typical output spectra of TDFL1. (a) The pump current was set at 1.40, 1.60, and 1.90 A, respectively; (b) the pump current was set at 1.45, 1.65, and 1.98 A, respectively.
    (Color online) CW output characteristics of polarized the Ho:YAG oscillator. (a) The pump absorption efficiency of the Ho:YAG crystal, the CW output power, and the transmittance of DM3; (b) the beam quality measurement and spectrum of the output laser.
    Fig. 3. (Color online) CW output characteristics of polarized the Ho:YAG oscillator. (a) The pump absorption efficiency of the Ho:YAG crystal, the CW output power, and the transmittance of DM3; (b) the beam quality measurement and spectrum of the output laser.
    (Color online) Pulsed output characteristics of the polarized Ho:YAG oscillator. (a) Pulse energy and pulse duration versus PRF with pump power of 51.6 W; (b) the pulse profiles at eight different PRFs.
    Fig. 4. (Color online) Pulsed output characteristics of the polarized Ho:YAG oscillator. (a) Pulse energy and pulse duration versus PRF with pump power of 51.6 W; (b) the pulse profiles at eight different PRFs.
    (Color online) Output characteristics of the polarized Ho:YAG amplifier. (a) Amplified output CW power versus pump power from TDFL2; (b) amplifier pulse energy and pulse duration versus PRF with TDFL1 power of 51.6 W and TDFL2 power of 37 W.
    Fig. 5. (Color online) Output characteristics of the polarized Ho:YAG amplifier. (a) Amplified output CW power versus pump power from TDFL2; (b) amplifier pulse energy and pulse duration versus PRF with TDFL1 power of 51.6 W and TDFL2 power of 37 W.
    Layout of the TDFL-pumped Ho:YAG oscillator and amplifier system. (DM4, T≈90% at 3–5 μm and HR at p-polarized 2.09 μm).
    Fig. 6. Layout of the TDFL-pumped Ho:YAG oscillator and amplifier system. (DM4, T90% at 3–5 μm and HR at p-polarized 2.09 μm).
    (Color online) (a) Comparison of typical pump pulse profile and parametric pulse profile; (b) the beam quality measurement of parametric light.
    Fig. 7. (Color online) (a) Comparison of typical pump pulse profile and parametric pulse profile; (b) the beam quality measurement of parametric light.
    (Color online) (a) Total parametric output average power versus incident pump average power at a PRF of 3 kHz; (b) the beam quality measurements at three typical parametric pulse energies.
    Fig. 8. (Color online) (a) Total parametric output average power versus incident pump average power at a PRF of 3 kHz; (b) the beam quality measurements at three typical parametric pulse energies.
    Encai Ji, Mingming Nie, Qiang Liu. 13.5 mJ polarized 2.09 μm fiber-bulk holmium laser and its application to a mid-infrared ZnGeP2 optical parametric oscillator[J]. Chinese Optics Letters, 2017, 15(9): 091402
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