• Chinese Optics Letters
  • Vol. 20, Issue 9, 091401 (2022)
Jun Meng1, Chen Li1, Zhenhua Cong1、2、3, Zhigang Zhao1、2、3, Shang Wang3, Gaoyou Liu2、3、4, and Zhaojun Liu1、2、3、*
Author Affiliations
  • 1School of Information Science and Engineering, Shandong University, Qingdao 266237, China
  • 2Shandong Provincial Key Laboratory of Laser Technology and Application, Qingdao 266237, China
  • 3Key Laboratory of Laser & Infrared System (Shandong University), Ministry of Education, Qingdao 266237, China
  • 4Center for Optics Research and Engineering, Shandong University, Qingdao 266237, China
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    DOI: 10.3788/COL202220.091401 Cite this Article Set citation alerts
    Jun Meng, Chen Li, Zhenhua Cong, Zhigang Zhao, Shang Wang, Gaoyou Liu, Zhaojun Liu. Investigations on beam quality improvement of an NCPM-KTA-based high energy optical parametric oscillator using an unstable resonator with a Gaussian reflectivity mirror [Invited][J]. Chinese Optics Letters, 2022, 20(9): 091401 Copy Citation Text show less
    (a) Conversion efficiency versus crystal length at 50% transmittance of the OC. (b) Conversion efficiency versus transmittance of the OC at the crystal length of 33 mm.
    Fig. 1. (a) Conversion efficiency versus crystal length at 50% transmittance of the OC. (b) Conversion efficiency versus transmittance of the OC at the crystal length of 33 mm.
    Schematic diagram of the experimental setup of the KTA-OPO system. HR, high reflection; 90°QR, 90° quartz rotator; BP, beam polarizer; GRM1, Gaussian reflectivity mirror for 1.06 µm; ISO, isolator; M1, mirror 1; GRM2, Gaussian reflectivity mirror for 1.5 µm; M2, 45° beam splitter.
    Fig. 2. Schematic diagram of the experimental setup of the KTA-OPO system. HR, high reflection; 90°QR, 90° quartz rotator; BP, beam polarizer; GRM1, Gaussian reflectivity mirror for 1.06 µm; ISO, isolator; M1, mirror 1; GRM2, Gaussian reflectivity mirror for 1.5 µm; M2, 45° beam splitter.
    (a) Output energy change with the pump current. Inset shows the temporal pulse profile at maximum output power. (b) Beam quality of the energy at 480 mJ. Inset shows the beam profile.
    Fig. 3. (a) Output energy change with the pump current. Inset shows the temporal pulse profile at maximum output power. (b) Beam quality of the energy at 480 mJ. Inset shows the beam profile.
    OPO output pulse energies (sum of signal and idler) for unstable and stable resonators. (a) Output energies versus the incident pump energy at the cavity length of 90 mm. (b) Output energies under different cavity lengths at the pump energy of 480 mJ.
    Fig. 4. OPO output pulse energies (sum of signal and idler) for unstable and stable resonators. (a) Output energies versus the incident pump energy at the cavity length of 90 mm. (b) Output energies under different cavity lengths at the pump energy of 480 mJ.
    Beam quality of the signal and idler at the pump energy of 480 mJ. Inset shows the beam profile. (a) Signal of the OPO based on the plane-parallel cavity; (b) idler of the OPO based on the plane-parallel cavity; (c) signal of the OPO based on the unstable cavity with GRM; (d) idler of the OPO based on the unstable cavity with GRM.
    Fig. 5. Beam quality of the signal and idler at the pump energy of 480 mJ. Inset shows the beam profile. (a) Signal of the OPO based on the plane-parallel cavity; (b) idler of the OPO based on the plane-parallel cavity; (c) signal of the OPO based on the unstable cavity with GRM; (d) idler of the OPO based on the unstable cavity with GRM.
    Spectrum of the signal light.
    Fig. 6. Spectrum of the signal light.
    Typical pulse shapes of OPO based on the unstable cavity with GRM at the output energy of 101 mJ. (a) Temporal profile of the signal in the experiment; (b) temporal profile of the idler in the experiment; (c) the simulation of the temporal profile.
    Fig. 7. Typical pulse shapes of OPO based on the unstable cavity with GRM at the output energy of 101 mJ. (a) Temporal profile of the signal in the experiment; (b) temporal profile of the idler in the experiment; (c) the simulation of the temporal profile.
     M2 FactorsEnergy (mJ)
    StableUnstableStableUnstable
    Signal39.8/38.49.8/9.912875
    Idler32.1/31.411.2/11.54826
    Table 1. Beam Quality Values and Output Energy Achieved with the Described Resonators
    Jun Meng, Chen Li, Zhenhua Cong, Zhigang Zhao, Shang Wang, Gaoyou Liu, Zhaojun Liu. Investigations on beam quality improvement of an NCPM-KTA-based high energy optical parametric oscillator using an unstable resonator with a Gaussian reflectivity mirror [Invited][J]. Chinese Optics Letters, 2022, 20(9): 091401
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