• Acta Optica Sinica
  • Vol. 43, Issue 11, 1114003 (2023)
Yuhang Ma1, Hao Wu2,*, Zaijin Li1,**, Jianwei Zhang2..., Xing Zhang2, Chao Chen2, Yongqiang Ning2, Yi Qu1, Hangyu Peng2, Li Qin2 and Lijun Wang2|Show fewer author(s)
Author Affiliations
  • 1Hainan Academician Team Innovation Center, Hainan Key Laboratory of Laser Technology and Optoelectronic Functional Materials, College of Physics and Electronic Engineering, Hainan Normal University, Haikou 571158, Hainan, China
  • 2State Key Laboratory of Luminescence and Application, Changchun Institute of Optics, Fine Mechanics and Physics, Chinese Academy of Sciences, Changchun 130033, Jilin, China
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    DOI: 10.3788/AOS222096 Cite this Article Set citation alerts
    Yuhang Ma, Hao Wu, Zaijin Li, Jianwei Zhang, Xing Zhang, Chao Chen, Yongqiang Ning, Yi Qu, Hangyu Peng, Li Qin, Lijun Wang. An Ultra-Broad Tunable Mid-Infrared Laser Based on Beam Combination of Dual Gain Chips[J]. Acta Optica Sinica, 2023, 43(11): 1114003 Copy Citation Text show less
    Energy band diagram of QCL
    Fig. 1. Energy band diagram of QCL
    Schematic of EC-QCL with Littrow structure
    Fig. 2. Schematic of EC-QCL with Littrow structure
    Structure diagram of ultra-broad tunable external cavity mid-infrared laser (QCL chip 1 is a 4.0 μm waveband gain chip and QCL chip 2 is a 4.6 μm waveband gain chip)
    Fig. 3. Structure diagram of ultra-broad tunable external cavity mid-infrared laser (QCL chip 1 is a 4.0 μm waveband gain chip and QCL chip 2 is a 4.6 μm waveband gain chip)
    Diffraction efficiency of blazed grating (grating model is GR1325-30035, the size is 12.5 mm×25 mm×9.5 mm, the design wavelength is 3.5 μm, the grating constant is 300 lines/mm, and the blazed angle is 26.5°)
    Fig. 4. Diffraction efficiency of blazed grating (grating model is GR1325-30035, the size is 12.5 mm×25 mm×9.5 mm, the design wavelength is 3.5 μm, the grating constant is 300 lines/mm, and the blazed angle is 26.5°)
    3-5 μm ultra-wide wavelength tuning spectra. The dotted line is the splitter transmittance curve and the solid lines are normalized intensity
    Fig. 5. 3-5 μm ultra-wide wavelength tuning spectra. The dotted line is the splitter transmittance curve and the solid lines are normalized intensity
    Side-mode suppression ratio of EC-QCL under different wave bands. (a) 4.0 μm; (b) 4.6 μm
    Fig. 6. Side-mode suppression ratio of EC-QCL under different wave bands. (a) 4.0 μm; (b) 4.6 μm
    Power curves of two waveband lasers
    Fig. 7. Power curves of two waveband lasers
    Curves of laser power changing with wavelength
    Fig. 8. Curves of laser power changing with wavelength
    Spot shape obtained by spot analyzer at 20 cm
    Fig. 9. Spot shape obtained by spot analyzer at 20 cm
    Intensity characterization of spot shape in x and y directions (spot size at 1/e2 has been marked). (a) x direction; (b) y direction
    Fig. 10. Intensity characterization of spot shape in x and y directions (spot size at 1/e2 has been marked). (a) x direction; (b) y direction

    Wavelength tuning

    range /nm

    Spectral width /nmIncident angle of grating /(°)

    Maximum output

    power /mW

    SMSR /dB
    3779-407629734.54–37.695.2420
    4255-483658139.67–46.5014.1220
    Table 1. Performance parameters of laser system under 300 lines/mm grating
    Yuhang Ma, Hao Wu, Zaijin Li, Jianwei Zhang, Xing Zhang, Chao Chen, Yongqiang Ning, Yi Qu, Hangyu Peng, Li Qin, Lijun Wang. An Ultra-Broad Tunable Mid-Infrared Laser Based on Beam Combination of Dual Gain Chips[J]. Acta Optica Sinica, 2023, 43(11): 1114003
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