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用于直线感应加速器光源焦斑测量的双锥厚针孔结构设计

王毅 李勤 刘云龙 龙全红 代志勇

王毅, 李勤, 刘云龙, 等. 用于直线感应加速器光源焦斑测量的双锥厚针孔结构设计[J]. 强激光与粒子束, 2019, 31: 065102. doi: 10.11884/HPLPB201931.180291
引用本文: 王毅, 李勤, 刘云龙, 等. 用于直线感应加速器光源焦斑测量的双锥厚针孔结构设计[J]. 强激光与粒子束, 2019, 31: 065102. doi: 10.11884/HPLPB201931.180291
Wang Yi, Li Qin, Liu Yunlong, et al. Structure design of thick pinhole with double cones for spot size measurement of the linear induction accelerator light source[J]. High Power Laser and Particle Beams, 2019, 31: 065102. doi: 10.11884/HPLPB201931.180291
Citation: Wang Yi, Li Qin, Liu Yunlong, et al. Structure design of thick pinhole with double cones for spot size measurement of the linear induction accelerator light source[J]. High Power Laser and Particle Beams, 2019, 31: 065102. doi: 10.11884/HPLPB201931.180291

用于直线感应加速器光源焦斑测量的双锥厚针孔结构设计

doi: 10.11884/HPLPB201931.180291
基金项目: 

国家自然科学基金项目 11875242

详细信息
    作者简介:

    王毅(1983-),男,博士,从事强流电子束及X光探测技术研究;wangyi_caep@163.com

  • 中图分类号: O434.1

Structure design of thick pinhole with double cones for spot size measurement of the linear induction accelerator light source

  • 摘要: 研究设计双锥厚针孔结构体,利用小孔成像测量高能强流直线感应加速器光源的焦斑。建立数值计算模型,根据实际光源特性和实验布局条件,模拟光子穿过厚针孔结构的辐射成像过程,分析光源尺寸、分布和偏轴等对焦斑测量的影响。理论计算结果显示对光源物面的空间分辨率可达5 lp/mm。
  • 图  1  双锥厚针孔结构与成像模型

    Figure  1.  Structure and imaging model of thick pinhole with double cones

    图  2  光源空间分布理论模型

    Figure  2.  Models of spatial distributions of the light source

    图  3  电子束打靶的轫致辐射能谱

    Figure  3.  Energy spectra of bremsstrahlung radiation for the electron beam striking a target

    图  4  点光源条件下的双锥厚针孔成像

    Figure  4.  Imaging of thick pinhole with double cones by point light source

    图  5  不同条件下厚针孔成像的有效孔径

    Figure  5.  Effective diameters for the pinhole imaging under different conditions

    图  6  光源偏心对分布测量影响

    Figure  6.  Effect of light source eccentric distance on the measurement of the source distribution

    图  7  厚针孔成像的空间分辨率曲线

    Figure  7.  Curves of spatial resolutions for thick pinhole imaging

    表  1  双锥厚针孔成像的焦斑FWHM计算结果

    Table  1.   Results of source FWHM by thick pinhole imaging

    distribution source FWHM / mm L2=1 m L2=2 m L2=3 m
    δFWHMcal/mm Δ δFWHMcal/mm Δ δFWHMcal/mm Δ
    KV 1.00 0.94 -6.5% 0.96 -3.6% 0.97 -3.1%
    1.10 1.04 -5.6% 1.06 -3.2% 1.07 -2.7%
    1.30 1.24 -4.4% 1.27 -2.6% 1.27 -2.3%
    1.50 1.45 -3.6% 1.47 -2.2% 1.47 -2.0%
    GS 1.00 1.06 5.6% 1.01 0.7% 1.00 0.2%
    1.10 1.15 4.2% 1.10 0.0% 1.09 -0.5%
    1.30 1.33 1.9% 1.28 -1.2% 1.28 -1.7%
    1.50 1.51 0.4% 1.47 -2.0% 1.46 -2.5%
    BNT 1.00 1.10 10.2% 1.03 2.7% 1.02 1.8%
    1.10 1.19 7.8% 1.12 2.0% 1.11 0.7%
    1.30 1.36 4.3% 1.30 -0.2% 1.29 -0.8%
    1.50 1.53 2.0% 1.48 -1.4% 1.46 -3.0%
    QBNT 1.00 1.12 11.7% 1.03 3.2% 1.02 2.5%
    1.10 1.20 9.2% 1.13 2.4% 1.11 1.2%
    1.30 1.37 5.5% 1.30 -0.1% 1.30 -0.2%
    1.50 1.54 2.8% 1.49 -1.0% 1.47 -1.9%
    下载: 导出CSV
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出版历程
  • 收稿日期:  2018-10-29
  • 修回日期:  2019-03-25
  • 刊出日期:  2019-07-15

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