• Infrared and Laser Engineering
  • Vol. 51, Issue 7, 20210654 (2022)
Wenming Yao1, Lihua Deng2, Yubing Tian1, Aolei Chang1,3..., Peng Wang1, Jiansheng Chen1, Huiming Tan1 and Jing Gao1,3|Show fewer author(s)
Author Affiliations
  • 1Jiangsu Key Laboratory of Medical Optics, Suzhou Institute of Biomedical Engineering and Technology, Chinese Academy of Sciences, Suzhou 215163, China
  • 2Suzhou Institute of Nano-Tech and Nano-Bionics, Chinese Academy of Sciences, Suzhou 215123, China
  • 3Jilin Key Laboratory of Solid Laser Technology and Application, School of Science, Changchun University of Science and Technology, Changchun 130022, China
  • show less
    DOI: 10.3788/IRLA20210654 Cite this Article
    Wenming Yao, Lihua Deng, Yubing Tian, Aolei Chang, Peng Wang, Jiansheng Chen, Huiming Tan, Jing Gao. High-conversion-efficiency continuous-wave near-infrared singly resonant optical parametric oscillator[J]. Infrared and Laser Engineering, 2022, 51(7): 20210654 Copy Citation Text show less
    Experimental setup of the CW MgO:sPPLT-OPO
    Fig. 1. Experimental setup of the CW MgO:sPPLT-OPO
    Spatial beam profile of the pump light in the cavity after focusing by the lens
    Fig. 2. Spatial beam profile of the pump light in the cavity after focusing by the lens
    Signal output power as function of the pump power with different kinds of laser cavity lengths at 27 ℃
    Fig. 3. Signal output power as function of the pump power with different kinds of laser cavity lengths at 27 ℃
    Output power of the different signal light at pump power 13.6 W and temperature 27 ℃
    Fig. 4. Output power of the different signal light at pump power 13.6 W and temperature 27 ℃
    Signal output power and conversion efficiency as functions with pump power when the poling periods are 8.3, 8.4, 8.5 and 8.6 μm at 27 ℃. (a) Signal output power; (b) Conversion efficiency
    Fig. 5. Signal output power and conversion efficiency as functions with pump power when the poling periods are 8.3, 8.4, 8.5 and 8.6 μm at 27 ℃. (a) Signal output power; (b) Conversion efficiency
    Output spectrum curve of the MgO:sPPLT-OPO at 27 ℃
    Fig. 6. Output spectrum curve of the MgO:sPPLT-OPO at 27 ℃
    Polarization periodic tuning curve of the CW MgO:sPPLT-OPO at 27 ℃
    Fig. 7. Polarization periodic tuning curve of the CW MgO:sPPLT-OPO at 27 ℃
    Signal and idler wavelength tuning varies with temperature when the grating periods are 8.3, 8.4, 8.5 and 8.6 μm
    Fig. 8. Signal and idler wavelength tuning varies with temperature when the grating periods are 8.3, 8.4, 8.5 and 8.6 μm
    Temperature tuning rates of signal and idler spectra at poling periods of 8.3, 8.4, 8.5 and 8.6 μm
    Fig. 9. Temperature tuning rates of signal and idler spectra at poling periods of 8.3, 8.4, 8.5 and 8.6 μm
    Grating period8.3 μm X:2.3 mm Y:2.4 mm 8.4 μm X:2.3 mm Y:2.6 mm 8.5 μm X:2.4 mm Y:2.6 mm 8.6 μm X:2.4 mm Y:2.5 mm
    Table 1. Signal beam profile of different periods
    Wenming Yao, Lihua Deng, Yubing Tian, Aolei Chang, Peng Wang, Jiansheng Chen, Huiming Tan, Jing Gao. High-conversion-efficiency continuous-wave near-infrared singly resonant optical parametric oscillator[J]. Infrared and Laser Engineering, 2022, 51(7): 20210654
    Download Citation