• High Power Laser Science and Engineering
  • Vol. 9, Issue 2, 02000e11 (2021)
Jörg Körner1、2、3、*, Venkatesan Jambunathan1, Fangxin Yue1, Jürgen Reiter2、3, Ondřej Slezák1, Petr Navrátil1, Samuel Paul David1, Antonio Lucianetti1, Joachim Hein2、3, Tomáš Mocek1, and Malte C. Kaluza2、3
Author Affiliations
  • 1HiLASE Centre, Institute of Physics of the Czech Academy of Sciences, Dolní Břežany, Czech Republic
  • 2Institute of Optics and Quantum Electronics, Friedrich Schiller University Jena, Jena, Germany
  • 3Helmholz Institute Jena, Jena, Germany
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    DOI: 10.1017/hpl.2020.53 Cite this Article Set citation alerts
    Jörg Körner, Venkatesan Jambunathan, Fangxin Yue, Jürgen Reiter, Ondřej Slezák, Petr Navrátil, Samuel Paul David, Antonio Lucianetti, Joachim Hein, Tomáš Mocek, Malte C. Kaluza. Diode-pumped, electro-optically Q-switched, cryogenic Tm:YAG laser operating at 1.88 μm[J]. High Power Laser Science and Engineering, 2021, 9(2): 02000e11 Copy Citation Text show less
    Results from the numerical simulation of the pump process in an 8% (atomic fraction) doped Tm:YAG crystal with a pump duration of 15 ms assuming a fluorescence lifetime of 15 ms. Upper left graph: relative inversion density as a function of the penetration depth in the laser crystal for different pump intensities at the end of the pump pulse. Upper right graph: relative inversion density on the crystal’s entrance surface as a function of the pump duration for various pump intensities. Lower graphs: relative inversion density as a function of the penetration depth (horizontal) and pump duration (vertical) for a pump intensity of 1 kW/cm2 (left) and 5 kW/cm2 (right).
    Fig. 1. Results from the numerical simulation of the pump process in an 8% (atomic fraction) doped Tm:YAG crystal with a pump duration of 15 ms assuming a fluorescence lifetime of 15 ms. Upper left graph: relative inversion density as a function of the penetration depth in the laser crystal for different pump intensities at the end of the pump pulse. Upper right graph: relative inversion density on the crystal’s entrance surface as a function of the pump duration for various pump intensities. Lower graphs: relative inversion density as a function of the penetration depth (horizontal) and pump duration (vertical) for a pump intensity of 1 kW/cm2 (left) and 5 kW/cm2 (right).
    Schematic of the laser setup. The dashed box inset shows the hit points of the pump beam on L2 and P. Cryo, high-vacuum cryostat; DM, dichroic mirror; FCLD, fiber-coupled laser diode; L1 and L2, lenses; LM, active mirror laser medium; M1, M2, M3, turning mirrors; P, retro-reflector prism; PC, Pockels cell; PM, pump turning mirror; QWP, quarter wave plate; SM1 and SM2, spherical mirrors; TFP, thin-film polarizer.
    Fig. 2. Schematic of the laser setup. The dashed box inset shows the hit points of the pump beam on L2 and P. Cryo, high-vacuum cryostat; DM, dichroic mirror; FCLD, fiber-coupled laser diode; L1 and L2, lenses; LM, active mirror laser medium; M1, M2, M3, turning mirrors; P, retro-reflector prism; PC, Pockels cell; PM, pump turning mirror; QWP, quarter wave plate; SM1 and SM2, spherical mirrors; TFP, thin-film polarizer.
    Output energy , optical-to-optical efficiency and full width at half maximum output pulse duration as functions of the pump pulse duration in Q-switch operation. The pump diode was operated at 28 W peak power and 1 Hz repetition rate. The secondary x-axis on top indicates the total pump energy applied.
    Fig. 3. Output energy , optical-to-optical efficiency and full width at half maximum output pulse duration as functions of the pump pulse duration in Q-switch operation. The pump diode was operated at 28 W peak power and 1 Hz repetition rate. The secondary x-axis on top indicates the total pump energy applied.
    Temporal pulse shapes of the intracavity signal and the output pulse at maximum energy.
    Fig. 4. Temporal pulse shapes of the intracavity signal and the output pulse at maximum energy.
    Output laser profile in Q-switch operation. The black curves at the sides are the averaged cross-sections.
    Fig. 5. Output laser profile in Q-switch operation. The black curves at the sides are the averaged cross-sections.
    Jörg Körner, Venkatesan Jambunathan, Fangxin Yue, Jürgen Reiter, Ondřej Slezák, Petr Navrátil, Samuel Paul David, Antonio Lucianetti, Joachim Hein, Tomáš Mocek, Malte C. Kaluza. Diode-pumped, electro-optically Q-switched, cryogenic Tm:YAG laser operating at 1.88 μm[J]. High Power Laser Science and Engineering, 2021, 9(2): 02000e11
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