• High Power Laser Science and Engineering
  • Vol. 7, Issue 3, 03000e42 (2019)
Issa Tamer1、2、†, Sebastian Keppler1、2, Jörg Körner2, Marco Hornung1、2, Marco Hellwing2, Frank Schorcht1, Joachim Hein1、2, and Malte C. Kaluza1、2
Author Affiliations
  • 1Helmholtz-Institute Jena, Fröbelstieg 3, 07743 Jena, Germany
  • 2Friedrich-Schiller-University Jena, Max-Wien Platz 1, 07743 Jena, Germany
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    DOI: 10.1017/hpl.2019.32 Cite this Article Set citation alerts
    Issa Tamer, Sebastian Keppler, Jörg Körner, Marco Hornung, Marco Hellwing, Frank Schorcht, Joachim Hein, Malte C. Kaluza. Modeling of the 3D spatio-temporal thermal profile of joule-class -based laser amplifiers[J]. High Power Laser Science and Engineering, 2019, 7(3): 03000e42 Copy Citation Text show less
    Numerical calculation of the normalized pump intensity within a Yb:YAG crystal in comparison to the Lambert–Beer and saturated absorption models.
    Fig. 1. Numerical calculation of the normalized pump intensity within a Yb:YAG crystal in comparison to the Lambert–Beer and saturated absorption models.
    A slice through the pumped Yb:YAG model in COMSOL.
    Fig. 2. A slice through the pumped Yb:YAG model in COMSOL.
    Pump profile (a) and thermal image (b) of the end-pumped and water-cooled $\text{Yb:CaF}_{2}$.
    Fig. 3. Pump profile (a) and thermal image (b) of the end-pumped and water-cooled $\text{Yb:CaF}_{2}$.
    Comparison of measured (solid) and simulated (dashed) thermal profiles. The measured temperature profiles for (a) Yb:YAG and (b) $\text{Yb:CaF}_{2}$ on both the front and back surfaces were compared to the simulated temperature profiles averaged over the pump cycle. (c) The front and back Yb:FP15 profiles are displayed for times 0 (directly before the 1.4 ms pump pulse), 0.1, 1, 2.5, and 5 s within the pump cycle (repetition rate 0.2 Hz).
    Fig. 4. Comparison of measured (solid) and simulated (dashed) thermal profiles. The measured temperature profiles for (a) Yb:YAG and (b) $\text{Yb:CaF}_{2}$ on both the front and back surfaces were compared to the simulated temperature profiles averaged over the pump cycle. (c) The front and back Yb:FP15 profiles are displayed for times 0 (directly before the 1.4 ms pump pulse), 0.1, 1, 2.5, and 5 s within the pump cycle (repetition rate 0.2 Hz).
    Schematic of the 3D pumping configuration of the Yb:FP15-based (perimeter in blue) A4 multi-pass amplifier at POLARIS with thermal images of an example of a single pump spot (top left) and the full pump profile (top right).
    Fig. 5. Schematic of the 3D pumping configuration of the Yb:FP15-based (perimeter in blue) A4 multi-pass amplifier at POLARIS with thermal images of an example of a single pump spot (top left) and the full pump profile (top right).
    Comparison of measured (solid) and simulated (dashed) thermal profiles of the pumped and thermalized Yb:FP15 within the A4 amplifier. A slice through the pumped Yb:FP15 model in COMSOL is shown in (a). The front and back Yb:FP15 profiles are displayed in (b) for times 0 (directly before the 2.7 ms pump pulse), 0.1, 5, 10, 25, and 50 s within the pump cycle (repetition rate 0.02 Hz). The temperature on the front and back centers of the Yb:FP15 material is plotted in (c) throughout the pump cycle.
    Fig. 6. Comparison of measured (solid) and simulated (dashed) thermal profiles of the pumped and thermalized Yb:FP15 within the A4 amplifier. A slice through the pumped Yb:FP15 model in COMSOL is shown in (a). The front and back Yb:FP15 profiles are displayed in (b) for times 0 (directly before the 2.7 ms pump pulse), 0.1, 5, 10, 25, and 50 s within the pump cycle (repetition rate 0.02 Hz). The temperature on the front and back centers of the Yb:FP15 material is plotted in (c) throughout the pump cycle.
    Comparison of the measured (solid) and simulated (dashed) front, back, and middle thermal profiles of the pumped Yb:FP15 within the A4 amplifier.
    Fig. 7. Comparison of the measured (solid) and simulated (dashed) front, back, and middle thermal profiles of the pumped Yb:FP15 within the A4 amplifier.
    Material$\text{Yb}^{3+}$-Doping $\left[\displaystyle \frac{\text{ions}}{\text{cm}^{3}}\right]$$K_{\text{th}}$ $\left[\displaystyle \frac{\text{W}}{\text{m}\cdot \text{K}}\right]$$\unicode[STIX]{x1D70C}$ $\left[\displaystyle \frac{\text{kg}}{\text{m}^{3}}\right]$$\unicode[STIX]{x1D6FC}_{T}$ $\left[10^{-6}\displaystyle \frac{1}{\text{K}}\right]$$C_{p}$ $\left[\displaystyle \frac{\text{J}}{\text{kg}\cdot \text{K}}\right]$$\unicode[STIX]{x1D6FC}$ $\left[\displaystyle \frac{1}{\text{m}}\right]$$\unicode[STIX]{x1D702}_{h}$
    Yb:YAG$4.2\times 10^{20}$9.2[16]4660[16]7[16]615[16]296[19]0.07[19]
    $\text{Yb:CaF}_{2}$$3.8\times 10^{20}$6.3[17]3180[18]18.5[18]816[16]67[19]0.06[19]
    Yb:FP15$6\times 10^{20}$0.88[20]3800[20]14[20]720[20]187[15]0.13[15]
    Table 1. Relevant optical and thermal properties of the considered active materials.
    Issa Tamer, Sebastian Keppler, Jörg Körner, Marco Hornung, Marco Hellwing, Frank Schorcht, Joachim Hein, Malte C. Kaluza. Modeling of the 3D spatio-temporal thermal profile of joule-class -based laser amplifiers[J]. High Power Laser Science and Engineering, 2019, 7(3): 03000e42
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