Chinese Optics Letters, Volume. 22, Issue 1, 011403(2024)

14.1 W continuous-wave dual-end diode-pumped Er:Lu2O3 laser at 2.85 µm

Yangyang Liang1,2, Tao Li1,2,3、*, Baitao Zhang3, Jingliang He3, Sascha Kalusniak4, Xian Zhao2,3, and Christian Kränkel4
Author Affiliations
  • 1Key Laboratory of Laser & Infrared System, Ministry of Education, Shandong University, Qingdao 266237, China
  • 2School of Information Science and Engineering, Shandong Provincial Key Laboratory of Laser Technology and Application, Shandong University, Qingdao 266237, China
  • 3Institute of Novel Semiconductors, State Key Laboratory of Crystal Materials, Shandong University, Jinan 250100, China
  • 4Leibniz-Institut für Kristallzüchtung (IKZ), Berlin 12489, Germany
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    Figures & Tables(8)
    Simplified energy levels of the Er3+ ions and the energy transfer mechanism.
    Laser schemes of (a) the single-end-pumped and (b) the dual-end-pumped Er:Lu2O3 lasers.
    Laser characteristics of (a) the single-end-pumped and (b) the dual-end-pumped setups for different T by using 35:200 and 35:200:200 lens group, respectively.
    Laser characteristics of the TEC-cooled (a) single- and (b) dual-end-pumped setup resonator with different OC transmissions.
    (a) Power instability (PV) of the water-cooled laser at 8 W and the TEC-cooled laser at 12 W. (b) Variation of the power instability (PV) versus the output power of the water- and TEC-cooled lasers.
    Laser spectra of the TEC-cooled dual-end-pumped resonator at 3% OC transmission at different output power levels.
    M2 values versus the output power level for 3% OC transmission in the dual-end-pumped water-cooled resonator configuration. Inset: spatial beam characteristics and M2 values at 2 W.
    • Table 1. Summary of the Results Obtained with Different Er:Lu2O3 Resonator Configurations

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      Table 1. Summary of the Results Obtained with Different Er:Lu2O3 Resonator Configurations

      CoolingLaser SchemeCoupling Lens GroupPump DirectionPolarizationOutput Coupler Transmission (%)Maximum Absorbed Pump Power (W)Highest Output Power (W)Slope Efficiency (%)
      WaterSingle-end-pumped scheme30:150ForwardNon-pol.327.56.024
      532.86.221
      35:200ForwardNon-pol.332.08.128
      532.07.225
      Dual-end-pumped scheme30:150:150Forward & backward/342.78.121
      538.97.221
      Forward onlyp-pol.326.05.222
      526.04.420
      Backward onlys-pol.327.94.819
      527.94.719
      35:200:200Forward & backward/343.610.125
      533.57.325
      Forward onlyp-pol.324.76.628
      525.65.926
      Backward onlys-pol.326.85.322
      527.95.021
      TECSingle-end-pumped scheme35:200ForwardNon-pol.341.910.127
      541.9925
      Dual-end-pumped scheme35:200:200Forward & backward/359.714.126
      559.71222
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    Yangyang Liang, Tao Li, Baitao Zhang, Jingliang He, Sascha Kalusniak, Xian Zhao, Christian Kränkel, "14.1 W continuous-wave dual-end diode-pumped Er:Lu2O3 laser at 2.85 µm," Chin. Opt. Lett. 22, 011403 (2024)

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    Paper Information

    Category: Lasers, Optical Amplifiers, and Laser Optics

    Received: Sep. 5, 2023

    Accepted: Sep. 18, 2023

    Published Online: Jan. 9, 2024

    The Author Email: Tao Li (litao@sdu.edu.cn)

    DOI:10.3788/COL202422.011403

    CSTR:32184.14.COL202422.011403

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