• 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

    Abstract

    Beam quality improvements by a large margin for signal and idler beams of a high energy 100 Hz KTiOAsO4 (KTA) non-critical phase matching (NCPM) optical parametric oscillator (OPO) were demonstrated using an unstable resonator configuration instead of a plane-parallel one. Theoretically, influences of cavity lengths and transmission of an output coupler on the OPO conversion efficiency for both were numerically simulated. For OPO based on an unstable resonator with a Gaussian reflectivity mirror, the maximum pulse energies at the signal (1.53 µm) and idler (3.47 µm) were about 75 mJ and 26 mJ, respectively. The corresponding beam quality factors of the signal were Mx2 = 9.8 and My2 = 9.9, and Mx2 = 11.2 and My2 = 11.5 for the idler. As a comparison, 128 mJ of signal and 48 mJ of idler were obtained with the plane-parallel resonator, and the M2 factors of the signal were Mx2 = 39.8 and My2 = 38.4, and Mx2 = 32.1 and My2 = 31.4 for the idler. Compared with a plane-parallel cavity, over eight times and three times brightness improvements were realized for the signal and idler light, respectively.
    Es(x,y,z)z=iωscnsdeffEp(x,y,z)Ei*(x,y,z)eiΔkz+i2ks(x2+y2)Es(x,y,z),(1a)

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    Ei(x,y,z)z=iωicnideffEp(x,y,z)Es*(x,y,z)eiΔkz+i2ki(x2+y2)Ei(x,y,z),(1b)

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    Ep(x,y,z)z=iωpcnpdeffEs(x,y,z)Ei(x,y,z)eiΔkz+i2kp(x2+y2)Es(x,y,z),(1c)

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    Pp=2ln2Wpπτe(2ln2tτ)2,

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    I=2Ppπω0,p2e2(x2+y2)ω0,p2,

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    Ep=(8ln2npcε0πω0,p2πτ)12e(x2+y2)ω0,p2e2(ln2tτ)2.

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    Iso=ωsπω0,s2τs,

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    T(r)=Tmaxe2r2ωm2,

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    Wq=dt12nqcε0|Eq|2dxdy,q=s,i.

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    η=Ws+WiWin,

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    B=P(λM2)2,

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    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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