• High Power Laser Science and Engineering
  • Vol. 11, Issue 2, 02000e31 (2023)
Ning Wen1、3、5, Nan Wang2, Nan Zong1、3、4、*, Xue-Chun Lin2、*, Hong-Wei Gao1、3、4, Yong Bo1、3、4, Qin-Jun Peng1、3、4, Da-Fu Cui1、3、4, and Zu-Yan Xu1、3、4
Author Affiliations
  • 1Key Laboratory of Functional Crystal and Laser Technology, Technical Institute of Physics and Chemistry, Chinese Academy of Sciences, Beijing, China
  • 2Laboratory of All-Solid-State Light Source, Institute of Semiconductors, Chinese Academy of Sciences, Beijing, China
  • 3Key Laboratory of Solid-State Laser, Technical Institute of Physics and Chemistry, Chinese Academy of Sciences, Beijing, China
  • 4Institute of Optical Physics and Engineering Technology, Qilu Zhongke, Jinan, China
  • 5University of Chinese Academy of Sciences, Beijing, China
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    DOI: 10.1017/hpl.2023.22 Cite this Article Set citation alerts
    Ning Wen, Nan Wang, Nan Zong, Xue-Chun Lin, Hong-Wei Gao, Yong Bo, Qin-Jun Peng, Da-Fu Cui, Zu-Yan Xu. High-energy, hundred-picosecond pulsed 266 nm mid-ultraviolet generation by a barium borate crystal[J]. High Power Laser Science and Engineering, 2023, 11(2): 02000e31 Copy Citation Text show less

    Abstract

    We present a high-energy, hundred-picosecond (ps) pulsed mid-ultraviolet solid-state laser at 266 nm by a direct second harmonic generation (SHG) in a barium borate (BaB2O4, BBO) nonlinear crystal. The green pump source is a 710 mJ, 330 ps pulsed laser at a wavelength of 532 nm with a repetition rate of 1 Hz. Under a green pump energy of 710 mJ, a maximum output energy of 253.3 mJ at 266 nm is achieved with 250 ps pulse duration resulting in a peak power of more than 1 GW, corresponding to an SHG conversion efficiency of 35.7% from 532 to 266 nm. The experimental data were well consistent with the theoretical prediction. To the best of our knowledge, this laser exhibits both the highest output energy and highest peak power ever achieved in a hundred-ps/ps regime at 266 nm for BBO-SHG.
    $$\begin{align}\begin{array}{l}\dfrac{\partial {A}_1\left(x,y,z,t\right)}{\partial z}=-\dfrac{\gamma_1}{2}{A}_1\left(x,y,z,t\right)+{P}_1\left(x,y,z,t\right),\\\\[-7pt] {}\dfrac{\partial {A}_2\left(x,y,z,t\right)}{\partial z}=-\tan \rho \dfrac{\partial {A}_2\left(x,y,z,t\right)}{\partial x}\\\\[-7pt]\hspace{4.5pt}\qquad\qquad\qquad-\dfrac{1}{2}\left({\gamma}_2+\beta {\left|{A}_2\right|}^2\right){A}_2\left(x,y,z,t\right)+{P}_2\left(x,y,z,t\right),\end{array}\end{align}$$ ((1))

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    $$\begin{align} {P}_1\left(x,y,z,t\right)&=j{\sigma}_1{A}_2{A}_1^{\ast}\exp \left(i\Delta kz\right),\nonumber\\ {}{P}_2\left(x,y,z,t\right)&=j{\sigma}_2{A}_1^2\exp \left(-i\Delta kz\right),\end{align}$$ ((2))

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    Ning Wen, Nan Wang, Nan Zong, Xue-Chun Lin, Hong-Wei Gao, Yong Bo, Qin-Jun Peng, Da-Fu Cui, Zu-Yan Xu. High-energy, hundred-picosecond pulsed 266 nm mid-ultraviolet generation by a barium borate crystal[J]. High Power Laser Science and Engineering, 2023, 11(2): 02000e31
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