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

Fig. 1. (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.

Fig. 2. (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 K α on the laser energy for the target with 20 μm nanowires.

Fig. 3. (a) Original K α image for a nanowire array target with 10 μm long nanowires and a 5 μm thick substrate. Corresponding laser peak intensity is 1 × 10 19 W / cm 2 ; (b) restored image from (a).

Fig. 4. (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.
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Table 1. Laser Energy versus FWHM of the PSF and CE

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