• High Power Laser Science and Engineering
  • Vol. 6, Issue 2, 02000e31 (2018)
Bo Han1, Feilu Wang2, Jiayong Zhong1、3、*, Guiyun Liang2, Huigang Wei2, Dawei Yuan2, Baojun Zhu4, Fang Li4, Chang Liu1, Yanfei Li4, Jiarui Zhao4, Zhe Zhang4, Chen Wang5, Jun Xiong5, Guo Jia5, Neng Hua6, Jianqiang Zhu6, Yutong Li3、4, Gang Zhao2, and Jie Zhang3、7
Author Affiliations
  • 1Department of Astronomy, Beijing Normal University, Beijing 100875, China
  • 2Key Laboratory of Optical Astronomy, National Astronomical Observatories, Chinese Academy of Sciences, Beijing 100012, China
  • 3IFSA Collaborative Innovation Center, Shanghai Jiao Tong University, Shanghai 200240, China
  • 4National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China
  • 5Research Center for Laser Fusion, China Academy of Engineering Physics, Mianyang 621900, China
  • 6National Laboratory on High Power Laser and Physics, Chinese Academy of Sciences, Shanghai 201800, China
  • 7Key Laboratory for Laser Plasmas (MoE) and Department of Physics and Astronomy, Shanghai Jiao Tong University, Shanghai 200240, China
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    DOI: 10.1017/hpl.2018.25 Cite this Article Set citation alerts
    Bo Han, Feilu Wang, Jiayong Zhong, Guiyun Liang, Huigang Wei, Dawei Yuan, Baojun Zhu, Fang Li, Chang Liu, Yanfei Li, Jiarui Zhao, Zhe Zhang, Chen Wang, Jun Xiong, Guo Jia, Neng Hua, Jianqiang Zhu, Yutong Li, Gang Zhao, Jie Zhang. Measurement and analysis of K-shell lines of silicon ions in laser plasmas[J]. High Power Laser Science and Engineering, 2018, 6(2): 02000e31 Copy Citation Text show less
    Two types of targets and schematic diagram of the experimental setups. (a) The Type I target. (b) The Type II shot and the schematic diagram of the experimental setups. The silicon plate is set at the target chamber center (TCC), and two driven laser beams are focused on it. A crystal spectrometer is used to record the spectrum of plasma.
    Fig. 1. Two types of targets and schematic diagram of the experimental setups. (a) The Type I target. (b) The Type II shot and the schematic diagram of the experimental setups. The silicon plate is set at the target chamber center (TCC), and two driven laser beams are focused on it. A crystal spectrometer is used to record the spectrum of plasma.
    Black and gray lines are the experimental spectra of two Type I shots. Red line is the simulation results (Case A), where and . Blue line is the unbroadened theoretical line.
    Fig. 2. Black and gray lines are the experimental spectra of two Type I shots. Red line is the simulation results (Case A), where and . Blue line is the unbroadened theoretical line.
    Black and gray lines are the experimental spectra of two Type II shots. Red line is the simulation results (Case B), where and .
    Fig. 3. Black and gray lines are the experimental spectra of two Type II shots. Red line is the simulation results (Case B), where and .
    Black line is the experimental spectrum of repeated Type II targets in 2017. Red line is the simulation results (Case C), where and .
    Fig. 4. Black line is the experimental spectrum of repeated Type II targets in 2017. Red line is the simulation results (Case C), where and .
    (a) and (b) are the interferograms of Type I and Type II shots. (c) and (d) are the electron density distribution deduced by Abel inversing of (a) and (b).
    Fig. 5. (a) and (b) are the interferograms of Type I and Type II shots. (c) and (d) are the electron density distribution deduced by Abel inversing of (a) and (b).
    The and values. Every line has same electron density, which spans from to exponentially, and the line ratios are plotted as a function of electron temperature.
    Fig. 6. The and values. Every line has same electron density, which spans from to exponentially, and the line ratios are plotted as a function of electron temperature.
    The (red) and (black) values. Every line has same electron temperature, which spans from 100 eV to 500 eV incrementally, and the line ratios are plotted as a function of electron density.
    Fig. 7. The (red) and (black) values. Every line has same electron temperature, which spans from 100 eV to 500 eV incrementally, and the line ratios are plotted as a function of electron density.
    The solid scatters are the experimental and values. The open scatters are the and values of the three theoretical cases.
    Fig. 8. The solid scatters are the experimental and values. The open scatters are the and values of the three theoretical cases.
    IonTransitionCase
    (Å)(Å)(Å)UpperLower
    Li6.6457A
    Li6.6462A
    Li6.6479A
    He6.64866.648A
    Li6.6491A
    Li6.6491A
    Li6.6503A
    Li6.6504A
    Li6.6506A
    Li6.6523A
    Li6.6527A
    Li6.6527A
    Li6.6539A
    Li6.6544A
    Li6.6549A
    Li6.6551A
    Li6.6552A
    Li6.6562A
    6.65650.0001Li6.6565A
    Li6.6568A
    Li6.6592A
    Li6.6593A
    Li6.6612A
    Li6.6618A
    Li6.6622A
    Li6.663A
    Li6.6635A
    Li6.6635A
    Li6.6646A
    Li6.6764A
    Li6.67996.6776A
    Li6.68726.6854A
    Li6.68786.6866A
    Li6.72076.7176A
    Li6.72286.7196A
    Li6.7242A
    Li6.7277A
    Li6.72786.7293A
    6.73330.0001Li6.73746.7365A
    Li6.74156.7398A
    Table 1. Experimental peak centroids with statistical errors of Shot 26, and the present and theoretical wavelength of intense lines in Case A.
    IonTransitionCase
    (Å)(Å)(Å)UpperLower
    6.6270.0006
    6.648 0.0002He6.64866.648B
    Li6.6523B
    Li6.6539B
    Li6.6592B
    Li6.6593B
    Li6.6612B
    Li6.6618B
    Li6.663B
    Li6.6635B
    Li6.6635B
    Li6.6646B
    6.68290.0003Li6.67996.6776B
    Li6.68726.6854B
    Li6.68786.6866B
    6.688 0.0003He6.69116.6899B
    Li6.72076.7176B
    6.71360.0005Li6.72286.7196B
    Li6.72786.7293B
    6.73720.0006Li6.73746.7365B
    Li6.74156.7398B
    Be6.79716.7992B
    6.79520.0003Be6.79876.7995B
    Be6.79896.8008B
    Be6.79916.7999B
    Be6.79956.8016B
    Be6.82116.8046B
    Be6.82516.8239B
    Be6.82546.8249B
    Table 2. Experimental peak centroids with statistical errors from 6.6 Å to 6.85 Å of Shot 32 and the present and theoretical wavelength of intense lines in Case B.
    Bo Han, Feilu Wang, Jiayong Zhong, Guiyun Liang, Huigang Wei, Dawei Yuan, Baojun Zhu, Fang Li, Chang Liu, Yanfei Li, Jiarui Zhao, Zhe Zhang, Chen Wang, Jun Xiong, Guo Jia, Neng Hua, Jianqiang Zhu, Yutong Li, Gang Zhao, Jie Zhang. Measurement and analysis of K-shell lines of silicon ions in laser plasmas[J]. High Power Laser Science and Engineering, 2018, 6(2): 02000e31
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