• Chinese Journal of Lasers
  • Vol. 49, Issue 12, 1201005 (2022)
Xiahui Tang1, Yingxiong Qin1, Hao Peng1、*, Yujie Li1, Yang Wu1, Longsheng Xiao2, Yu Xiao1, and Juan Liu3
Author Affiliations
  • 1School of Optics and Electronic Information, Huazhong University of Science and Technology, Wuhan 430074, Hubei, China
  • 2College of Physics and Electromechanical Engineering, Hubei University of Education, Wuhan 430205, Hubei, China
  • 3College of Aeronautics and Astronautics, Xiamen University, Xiamen 361005, Fujian, China
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    DOI: 10.3788/CJL202249.1201005 Cite this Article Set citation alerts
    Xiahui Tang, Yingxiong Qin, Hao Peng, Yujie Li, Yang Wu, Longsheng Xiao, Yu Xiao, Juan Liu. High-Power Radio-Frequency Slab CO2 Laser[J]. Chinese Journal of Lasers, 2022, 49(12): 1201005 Copy Citation Text show less
    German Rofin radio frequency (RF) slab CO2 laser products
    Fig. 1. German Rofin radio frequency (RF) slab CO2 laser products
    Schematic of RF slab CO2 gas laser
    Fig. 2. Schematic of RF slab CO2 gas laser
    Temperature distribution of discharge electrode
    Fig. 3. Temperature distribution of discharge electrode
    Actual structure drawing of lath
    Fig. 4. Actual structure drawing of lath
    Schematic of three-channel parallel serpentine-like runner structure and its machining pattern. (a) Structural diagram; (b) machining pattern
    Fig. 5. Schematic of three-channel parallel serpentine-like runner structure and its machining pattern. (a) Structural diagram; (b) machining pattern
    Temperature field distribution maps. (a) Temperature field distribution diagram of front shaft side; (b) temperature field distribution diagram of opposite shaft side
    Fig. 6. Temperature field distribution maps. (a) Temperature field distribution diagram of front shaft side; (b) temperature field distribution diagram of opposite shaft side
    Structural diagram of waveguide unstable mixing cavity
    Fig. 7. Structural diagram of waveguide unstable mixing cavity
    Schematic of one-dimensional negative branch axis confocal unstable resonator
    Fig. 8. Schematic of one-dimensional negative branch axis confocal unstable resonator
    Schematic of light field in slab waveguide direction
    Fig. 9. Schematic of light field in slab waveguide direction
    Schematic of negative axis confocal unstable intracavity beam
    Fig. 10. Schematic of negative axis confocal unstable intracavity beam
    Comparison between numerical simulation and experimental results of two unstable cavity light field modes[20]
    Fig. 11. Comparison between numerical simulation and experimental results of two unstable cavity light field modes[20]
    Schematic of external light path shaping
    Fig. 12. Schematic of external light path shaping
    Change rule of output beam in two directions behind the cylindrical mirror M2
    Fig. 13. Change rule of output beam in two directions behind the cylindrical mirror M2
    Theoretical simulation diagrams and experimental diagram of intensity distribution of shaped beam in front of spherical mirror 8. (a) Light intensity distribution in unstable direction; (b) light intensity distribution in waveguide direction; (c) top view of light intensity distribution; (d) experimental results
    Fig. 14. Theoretical simulation diagrams and experimental diagram of intensity distribution of shaped beam in front of spherical mirror 8. (a) Light intensity distribution in unstable direction; (b) light intensity distribution in waveguide direction; (c) top view of light intensity distribution; (d) experimental results
    Light intensity distributions of shaped beam transmitted to different distances after passing through cylindrical lens M2. (a) z=200 mm; (b) z=400 mm; (c) z=800 mm; (d) z=1500 mm
    Fig. 15. Light intensity distributions of shaped beam transmitted to different distances after passing through cylindrical lens M2. (a) z=200 mm; (b) z=400 mm; (c) z=800 mm; (d) z=1500 mm
    Beam radius changes in two directions of shaped beam after passing through spherical mirror 8
    Fig. 16. Beam radius changes in two directions of shaped beam after passing through spherical mirror 8
    Numerical simulation and experimental diagrams of light intensity distribution after shaped beam transmits 2000 mm
    Fig. 17. Numerical simulation and experimental diagrams of light intensity distribution after shaped beam transmits 2000 mm
    Numerical simulation and experimental results of intensity distribution of shaped beam at 800 mm and 3800 mm. (a) Numerical simulation at 800 mm; (b) numerical simulation at 3800 mm; (c) experimental result at 800 mm; (d) experimental result at 3800 mm
    Fig. 18. Numerical simulation and experimental results of intensity distribution of shaped beam at 800 mm and 3800 mm. (a) Numerical simulation at 800 mm; (b) numerical simulation at 3800 mm; (c) experimental result at 800 mm; (d) experimental result at 3800 mm
    SlabPower /kWRadio frequency power /kWRadio frequency tubeLaser head air pressure /hPaTotal output power after filter /WBeam size /mmTotal output photoelectric efficiency /%Beam quality(K)
    DC0254524CTK 15-220030002211.00.94
    DC030n4527CTK 15-2>20033002211.0>0.9
    DC0354529CTK 15-2190400022110.93
    DC045n8537CTK 25-4≫20048002211.0>0.9
    DC0458537CTK 25-420048002210.10.94
    DC050n8542CTK 25-4>20053002210.1>0.9
    DC0508542CTK 25-42005230229.1>0.9
    DC0608551CTK 25-42006500248.20.9
    DC08014065CTK 35-22008400279.00.9
    Table 1. Main parameters of Rofin RF slab CO2 laser
    Xiahui Tang, Yingxiong Qin, Hao Peng, Yujie Li, Yang Wu, Longsheng Xiao, Yu Xiao, Juan Liu. High-Power Radio-Frequency Slab CO2 Laser[J]. Chinese Journal of Lasers, 2022, 49(12): 1201005
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