• High Power Laser Science and Engineering
  • Vol. 8, Issue 1, 010000e6 (2020)
Duanyang Chen1、2, Bin Wang1, Hu Wang1, Xiangyu Zhu3, Ziyuan Xu1, Yuanan Zhao1, Shenghao Wang1, Kaizao Ni1, Lili Zheng3, Hui Zhang4, Hongji Qi1, and Jianda Shao1
Author Affiliations
  • 1Key Laboratory of Materials for High Power Laser, Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Shanghai201800, China
  • 2Center of Materials Science and Optoelectronics Engineering, University of Chinese Academy of Sciences, Beijing100049, China
  • 3School of Aerospace Engineering, Tsinghua University, Beijing100084, China
  • 4Department of Engineering Physics, Tsinghua University, Beijing100084, China
  • show less
    DOI: 10.1017/hpl.2019.54 Cite this Article Set citation alerts
    Duanyang Chen, Bin Wang, Hu Wang, Xiangyu Zhu, Ziyuan Xu, Yuanan Zhao, Shenghao Wang, Kaizao Ni, Lili Zheng, Hui Zhang, Hongji Qi, Jianda Shao. Rapid growth of a long-seed KDP crystal[J]. High Power Laser Science and Engineering, 2020, 8(1): 010000e6 Copy Citation Text show less

    Abstract

    To reduce the seed length while maintaining the advantages of the cuboid KDP-type crystal, a long-seed KDP crystal with size $471~\text{mm}\times 480~\text{mm}\times 400~\text{mm}$ is rapidly grown. With almost the same high cutting efficiency to obtain third harmonic generation oriented samples, this long-seed KDP-type crystal can be grown with a shorter seed than that of the cuboid KDP-type crystal. The full width at half maximum of the high-resolution X-ray diffraction of the (200) crystalline face is 28.8 arc seconds, indicating that the long-seed KDP crystal has good crystalline quality. In the wavelength range of 377–1022 nm, the transmittance of the long-seed KDP crystal is higher than 90%. The fluence for the 50% probability of laser-induced damage (LID) is $18.5~\text{J}/\text{cm}^{2}$ (3 ns, 355 nm). Several test points survive when the laser fluence exceeds $30~\text{J}/\text{cm}^{2}$ (3 ns, 355 nm), indicating the good LID performance of the long-seed KDP crystal. At present, the growth of a long-seed DKDP crystal is under way.
    $$\begin{eqnarray}\displaystyle (T\sin \unicode[STIX]{x1D6FC}+V)\times 2+s=L, & & \displaystyle\end{eqnarray}$$(1)

    View in Article

    $$\begin{eqnarray}\displaystyle W\sin \unicode[STIX]{x1D6FC}+T\cos \unicode[STIX]{x1D6FC}+IN/2=H, & & \displaystyle\end{eqnarray}$$(2)

    View in Article

    $$\begin{eqnarray}\displaystyle (0.886T+0.5W)\times 2+15=L, & & \displaystyle\end{eqnarray}$$(3)

    View in Article

    $$\begin{eqnarray}\displaystyle 0.886W+0.5T+NT=H. & & \displaystyle\end{eqnarray}$$(4)

    View in Article

    $$\begin{eqnarray}\displaystyle W\sin \unicode[STIX]{x1D6FC}+T\cos \unicode[STIX]{x1D6FC}+IN/2+T=H. & & \displaystyle\end{eqnarray}$$(5)

    View in Article

    Duanyang Chen, Bin Wang, Hu Wang, Xiangyu Zhu, Ziyuan Xu, Yuanan Zhao, Shenghao Wang, Kaizao Ni, Lili Zheng, Hui Zhang, Hongji Qi, Jianda Shao. Rapid growth of a long-seed KDP crystal[J]. High Power Laser Science and Engineering, 2020, 8(1): 010000e6
    Download Citation