Chinese Optics Letters, Volume. 13, Issue 3, 031001(2015)

Radiography of a Kα X-ray source generated through ultrahigh picosecond laser–nanostructure target interaction

剑 王1,2, 宗清 赵2、*, 卫华 何2, 斌 朱2, 克攻 董2, 玉迟 吴2, 天奎 张2, 牛 高2, 凯南 周2, 娜 谢2, 维民 周2, and 渝秋 谷2
Author Affiliations
  • 1Department of Physics, Fudan University, Shanghai 210433, China
  • 2Research Center of Laser Fusion, China Academy of Engineering Physics, Mianyang 621900, China
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    Figures & Tables(5)
    (a) Schematic overview of the experiment setup. L–N means the laser is interacting with the nanowire structure directly. L–S means the laser is interacting with the substrate; (b) scanning electron microscopy image of the nanowire array target.
    (a) Spectrum of K-shell lines obtained for 94.8 J laser incidence on the target with 20 μm nanowires; (b) dependence of the total count of Kα on the laser energy for the target with 20 μm nanowires.
    (a) Original Kα image for a nanowire array target with 10 μm long nanowires and a 5 μm thick substrate. Corresponding laser peak intensity is 1×1019 W/cm2; (b) restored image from (a).
    (a) Stack of 1D slits (50, 100, 200, and 300 μm) on a 50 μm thick Ta substrate; (b) horizontal line-outs for the point projection radiography.
    • Table 1. Laser Energy versus FWHM of the PSF and CE

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      Table 1. Laser Energy versus FWHM of the PSF and CE

      Laser Energy (J)FWHM of the Point Spread Function (μm)CE
      1943.82.4×104
      7548.91.2×104
      9446.41.6×104
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    剑 王, 宗清 赵, 卫华 何, 斌 朱, 克攻 董, 玉迟 吴, 天奎 张, 牛 高, 凯南 周, 娜 谢, 维民 周, 渝秋 谷, "Radiography of a Kα X-ray source generated through ultrahigh picosecond laser–nanostructure target interaction," Chin. Opt. Lett. 13, 031001 (2015)

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    Paper Information

    Category: Image processing

    Received: Oct. 8, 2014

    Accepted: Dec. 22, 2014

    Published Online: Sep. 25, 2018

    The Author Email: 宗清 赵 (498427431@qq.com)

    DOI:10.3788/COL201513.031001

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