High Power Laser Science and Engineering, Volume. 12, Issue 3, 03000e26(2024)

A comprehensive diagnostic system of ultra-thin liquid sheet targets

Ziyang Peng1, Zhengxuan Cao1,2, Xuan Liu1, Yinren Shou3, Jiarui Zhao1, Shiyou Chen1, Ying Gao1, Pengjie Wang4, Zhusong Mei1, Zhuo Pan1, Defeng Kong1, Shirui Xu1, Zhipeng Liu1, Yulan Liang1, Tianqi Xu1, Tan Song1, Xun Chen1, Qingfan Wu1, Yujia Zhang1, Zihao Zhang1, Xueqin Yan1,5,6, and Wenjun Ma1,5,6、*
Author Affiliations
  • 1State Key Laboratory of Nuclear Physics and Technology, School of Physics, Peking University, Beijing, China
  • 2National Key Laboratory of Shock Wave and Detonation Physics, Institute of Fluid Physics, China Academy of Engineering Physics, Mianyang, China
  • 3Center for Relativistic Laser Science, Institute for Basic Science, Gwangju, Republic of Korea
  • 4Institute of Radiation Physics, Helmholtz-Zentrum Dresden Rossendorf, Dresden, Germany
  • 5Beijing Laser Acceleration Innovation Center, Beijing, China
  • 6Institute of Guangdong Laser Plasma Technology, Guangzhou, China
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    Figures & Tables(7)
    (a) Schematic of liquid sheet generation. (b) Top view of liquid sheet generation. (c) Overview of the main modules of the diagnostic system.
    (a) Schematic diagram of reflectance spectroscopy. (b) Side view and front view of the LST; the light source is connected to the six cores here to clearly display the measurement point. (c) A typical reflected spectrum of the LST with the theoretical fitting curve. (d) Theoretical reflectivity of films with different thicknesses at different wave numbers.
    (a) Fourier transform of a measured spectrum in wave number space. (b) Reflected spectrum of an ultra-thin liquid sheet at 238 nm with the theoretical fitting. (c) Thickness of the LST at different flow rates and positions. (d) Thickness of the LST at different misalignments of the colliding jets.
    (a) Typical interference fringes of the LST. (b) Wrapped phase in the red box of (a). (c) Thickness distribution unwrapped from (b). (d) Interference fringes corresponding to the thickness distribution of Hasson’s model. (e) The change of interference fringes with the improvement of flow symmetry.
    (a) Schematic diagram of the tilt angle measurement. (b) The tilt angle change within 1 hour. (c) The intensity integral of CCD1 and CCD3 to calculate the absolute reflectivity of the LST. (d) The change of the spot collected by CCD2 with the improvement of flow symmetry.
    (a) Schematic diagram of position measurement. (b) Time domain of the LST’s position (distance to the confocal detector). (c) Frequency domain of the LST’s vibration in (b). (d) Histogram of the LST’s relative position within 10 minutes.
    • Table 1. Parameters of each measurement module.

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      Table 1. Parameters of each measurement module.

      Module numberABCD
      Measured metricThicknessFlatnessTilt anglePosition
      Frequency~10 Hz~10 Hz~10 Hz~1 kHz
      Range0.01–50 μm0–50 nm/μm0–25 mrad0–1 mm
      Accuracy±0.5% (>200 nm) ±2 nm (<300 nm)±0.1 nm/μm±0.2 mrad±2 nm
      Spatial resolution~20 μm~5 μm~20 μm~20 μm
      Conflict$ / $$ / $DC
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    Ziyang Peng, Zhengxuan Cao, Xuan Liu, Yinren Shou, Jiarui Zhao, Shiyou Chen, Ying Gao, Pengjie Wang, Zhusong Mei, Zhuo Pan, Defeng Kong, Shirui Xu, Zhipeng Liu, Yulan Liang, Tianqi Xu, Tan Song, Xun Chen, Qingfan Wu, Yujia Zhang, Zihao Zhang, Xueqin Yan, Wenjun Ma. A comprehensive diagnostic system of ultra-thin liquid sheet targets[J]. High Power Laser Science and Engineering, 2024, 12(3): 03000e26

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    Paper Information

    Special Issue: THE 10TH ANNIVERSARY OF HIGH POWER LASER SCIENCE AND ENGINEERING 2023

    Received: Jul. 31, 2023

    Accepted: Dec. 11, 2023

    Published Online: Jul. 23, 2024

    The Author Email: Wenjun Ma (wenjun.ma@pku.edu.cn)

    DOI:10.1017/hpl.2023.101

    CSTR:32185.14.hpl.2023.101

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