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ZHAI Yi-lin, XIN Shi-cheng, SUN Jia-ze, LI Zhao-yu, CUI Jian-feng, DAI Qin. Parameter optimization of Gaussian unstable resonators for high-brightness laser output[J]. Chinese Optics. doi: 10.37188/CO.2025-0110
Citation: ZHAI Yi-lin, XIN Shi-cheng, SUN Jia-ze, LI Zhao-yu, CUI Jian-feng, DAI Qin. Parameter optimization of Gaussian unstable resonators for high-brightness laser output[J]. Chinese Optics. doi: 10.37188/CO.2025-0110

Parameter optimization of Gaussian unstable resonators for high-brightness laser output

cstr: 32171.14.CO.2025-0110
Funds:  Supported by National Key R&D Program (No. 2022YFB4601603); Funded by the Optical Selection Research Team Construction Project of Shenyang Ligong University
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  • Corresponding author: daiqin2003@126.com
  • Received Date: 24 Aug 2025
  • Accepted Date: 29 Oct 2025
  • Available Online: 11 Nov 2025
  • To achieve high-power and high-beam-quality laser output from a laser-diode side-pumped solid-state laser, this study investigates an unstable resonator incorporating a Gaussian output mirror. The boundary finite element method was utilized to analyze the effects of the resonant cavity length, Gaussian mirror membrane spot radius, and curvature radius on high-order mode suppression. The functional theory of mode loss difference was applied to determine the mode-matching range and the optimal parameters for the spot radius. Furthermore, an output power model was established to derive the theoretical optimal central transmittance for compensating loss. Based on the theoretical and simulation results, the resonator parameters were optimized, and the output beam’s mode distribution and quality were experimentally characterized using different Gaussian mirrors. Under the operational conditions of a 400 mm resonator length, 7.3 A pump current, and 100 Hz repetition frequency, the implementation of a Gaussian mirror with a 3 mm spot radius, 1.5 m curvature radius, and 17% central transmittance produced a high-quality 1064 nm laser output with beam quality factors of Mx2=2.09 and My2=2.20.

     

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