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飞秒激光产生的X射线双光谱成像

王洪建 叶雁 阳庆国 李泽仁 刘红杰

王洪建, 叶雁, 阳庆国, 等. 飞秒激光产生的X射线双光谱成像[J]. 强激光与粒子束, 2022, 34: 031015. doi: 10.11884/HPLPB202234.210287
引用本文: 王洪建, 叶雁, 阳庆国, 等. 飞秒激光产生的X射线双光谱成像[J]. 强激光与粒子束, 2022, 34: 031015. doi: 10.11884/HPLPB202234.210287
Wang Hongjian, Ye Yan, Yang Qingguo, et al. X-ray dual-spectrum imaging produced by femtosecond laser[J]. High Power Laser and Particle Beams, 2022, 34: 031015. doi: 10.11884/HPLPB202234.210287
Citation: Wang Hongjian, Ye Yan, Yang Qingguo, et al. X-ray dual-spectrum imaging produced by femtosecond laser[J]. High Power Laser and Particle Beams, 2022, 34: 031015. doi: 10.11884/HPLPB202234.210287

飞秒激光产生的X射线双光谱成像

doi: 10.11884/HPLPB202234.210287
基金项目: 国家自然科学基金委员会-中国工程物理研究院联合基金项目(U2030120);国家重点研发计划项目(2018YFB1306602);重庆市技术创新与应用发展项目(cstc2019jscx-msxmX0032);重庆工商大学科研平台项目(KFJJ2017052 、KFJJ2016031、1952038)
详细信息
    作者简介:

    王洪建,whj_cqu@163.com

  • 中图分类号: TH742.63

X-ray dual-spectrum imaging produced by femtosecond laser

  • 摘要: 在微介观诊断中往往因为空间限制,选择具有亮度高、单色性好、对比度强的特征谱线,而忽略了轫致辐射谱线。率先实验设计了特征谱线和轫致辐射谱线的双光谱诊断X射线光源的方法,在中国工程物理研究院“星光Ⅲ”激光装置飞秒激光束靶室上进行实验,激光功率密度大于1.6×1018 W/cm2,脉宽为30 fs,45°入射靶面。在入射靶前侧,设计了用于特征光谱成像的针孔成像光路,获得Cu纳米颗粒靶产生的特征X射线的焦斑图像,为76 μm,大于刃边方法测得半径为54 μm的焦斑。在靶后侧,设计了轫致辐射成像光路,利用PIX射线CCD获得2×5的圆形Ta组图像。实验表明,利用双光谱成像设计合理,适合微介观材料动态诊断,提高诊断效率。
  • 图  1  星光Ⅲ装置中双光谱成像实验布局图

    Figure  1.  Experiment setup of two spectrum imaging method on XG -Ⅲ facility

    图  2  轫致辐射背光成像(分别是原始图、半径为5,10和20 pixel的平坦型圆盘结构腐蚀)

    Figure  2.  Bremsstrahlung backlit imaging (original image, corrosion of flat disc structure with radius of 5, 10 and 20 pixel respectively)

    图  3  轫致辐射背光成像(分别是开运算、闭运算,先开后闭和先闭后开运算,3×3算子结构)

    Figure  3.  Bremsstrahlung backlit imaging (respectively open operation, close operation, open first and then close operation and close first and then open operation, 3×3 operator structure)

    图  4  针孔相机获取的图像

    Figure  4.  Image by pinhole CCD

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出版历程
  • 收稿日期:  2021-07-14
  • 修回日期:  2021-11-11
  • 网络出版日期:  2021-11-19
  • 刊出日期:  2022-01-13

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