• Matter and Radiation at Extremes
  • Vol. 5, Issue 1, 014401 (2020)
Qiang Xu1, Shaotong Zhou1, Kun-lun Wang1, Siqun Zhang1, Hongchun Cai1, Xiao Ren1, Pan Liu1, Xian bin Huang1、a), Li Zhao2, and Wenkang Zou1
Author Affiliations
  • 1Key Laboratory of Pulsed Power, Institute of Fluid Physics, China Academy of Engineering Physics, P.O. Box 919-108, Mianyang 621999, China
  • 2Southwest University of Science and Technology, Mianyang City, Sichuan Province 621010, China
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    DOI: 10.1063/1.5120256 Cite this Article
    Qiang Xu, Shaotong Zhou, Kun-lun Wang, Siqun Zhang, Hongchun Cai, Xiao Ren, Pan Liu, Xian bin Huang, Li Zhao, Wenkang Zou. X-ray emission characteristics in magnetically driven plasma jet experiments on PTS facility[J]. Matter and Radiation at Extremes, 2020, 5(1): 014401 Copy Citation Text show less
    Schematic of the load, showing the electrical current path, the magnetic field, and the structure of the electrodes.
    Fig. 1. Schematic of the load, showing the electrical current path, the magnetic field, and the structure of the electrodes.
    Photograph of the actual load, with the foil, the cubic holder, the anode plate, and the B-dot probes.
    Fig. 2. Photograph of the actual load, with the foil, the cubic holder, the anode plate, and the B-dot probes.
    Schematic of the discharge chamber of PTS and the surrounding diagnostic instruments.
    Fig. 3. Schematic of the discharge chamber of PTS and the surrounding diagnostic instruments.
    Setup of the laser shadow imaging system.
    Fig. 4. Setup of the laser shadow imaging system.
    Dynamics and radiation characteristics of soft x-rays in shot 345 driven by a single post and aluminum foil. (a) Result from the laser shadow imaging system, which shows the foil behavior in the early stage. (b) Wave forms of electric current and x-ray power. The red region is the cathode post, the yellow dashed line indicates the initial foil position, and the red dashed line shows the result from the 0-D model.
    Fig. 5. Dynamics and radiation characteristics of soft x-rays in shot 345 driven by a single post and aluminum foil. (a) Result from the laser shadow imaging system, which shows the foil behavior in the early stage. (b) Wave forms of electric current and x-ray power. The red region is the cathode post, the yellow dashed line indicates the initial foil position, and the red dashed line shows the result from the 0-D model.
    Dynamics and radiation characteristics of soft x-rays in shot 387 driven by a single post and copper foil. (a) Result from the laser shadow imaging system, which shows the foil behavior in the late stage. (b) Wave forms of electric current and x-ray power. (c) X-ray self-emission image. The red region is the cathode post, and the yellow dashed line indicates the initial foil position.
    Fig. 6. Dynamics and radiation characteristics of soft x-rays in shot 387 driven by a single post and copper foil. (a) Result from the laser shadow imaging system, which shows the foil behavior in the late stage. (b) Wave forms of electric current and x-ray power. (c) X-ray self-emission image. The red region is the cathode post, and the yellow dashed line indicates the initial foil position.
    Dynamics and radiation characteristics of soft x-rays in shot 390 driven by a single post and copper foil. (a) Result from the laser shadow imaging system, which shows the foil behavior in the late stage. (b) Wave forms of electric current and x-ray power. (c) X-ray self-emission image. Note that the bright area on the magnetic cavity in (a) may be caused by disturbance from another frame and can be ignored.
    Fig. 7. Dynamics and radiation characteristics of soft x-rays in shot 390 driven by a single post and copper foil. (a) Result from the laser shadow imaging system, which shows the foil behavior in the late stage. (b) Wave forms of electric current and x-ray power. (c) X-ray self-emission image. Note that the bright area on the magnetic cavity in (a) may be caused by disturbance from another frame and can be ignored.
    Boundary positions and expansion velocities of magnetic cavities in shots 387 and 390. The filled and hollow circles denote axial and radial positions, respectively, in shot 387, and the solid and hollow squares denote axial and radial positions, respectively, in shot 390. The red and green symbols correspond to results from the x-ray framing pinhole camera and the laser shadow camera, respectively.
    Fig. 8. Boundary positions and expansion velocities of magnetic cavities in shots 387 and 390. The filled and hollow circles denote axial and radial positions, respectively, in shot 387, and the solid and hollow squares denote axial and radial positions, respectively, in shot 390. The red and green symbols correspond to results from the x-ray framing pinhole camera and the laser shadow camera, respectively.
    Dose rates in shot 387 detected by each channel compared with the soft x-ray power. Note that the wave form of the soft x-ray here is the same as in Fig. 6(b).
    Fig. 9. Dose rates in shot 387 detected by each channel compared with the soft x-ray power. Note that the wave form of the soft x-ray here is the same as in Fig. 6(b).
    Unfolded spectrum of hard x-rays in shot 387.
    Fig. 10. Unfolded spectrum of hard x-rays in shot 387.
    Schematic of a possible radiation mechanism.
    Fig. 11. Schematic of a possible radiation mechanism.
    Channel123456
    Filter materialAlAlAlAlCuFe
    Thickness (mm)12481.120
    Spectral response (keV)>10>15>20>25>40>150
    Table 1. Parameters of the filters in the Si-PIN array.
    Qiang Xu, Shaotong Zhou, Kun-lun Wang, Siqun Zhang, Hongchun Cai, Xiao Ren, Pan Liu, Xian bin Huang, Li Zhao, Wenkang Zou. X-ray emission characteristics in magnetically driven plasma jet experiments on PTS facility[J]. Matter and Radiation at Extremes, 2020, 5(1): 014401
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