• High Power Laser and Particle Beams
  • Vol. 34, Issue 6, 064008 (2022)
Dikai Li1、2, Leifeng Cao2、3、*, [in Chinese]4, Zheng Zhou5, Qiuhong Chen6, Chunhui Zhang2、3, Yanmeng Dai1、2, Jian Yu2、3, Miaomiao Yan2、3, Jialing Deng2、3, Xue Wang2、3, and [in Chinese]1、2、3
Author Affiliations
  • 1College of Engineering Physics, Shenzhen Technology University, Shenzhen 518118, China
  • 2Shenzhen Key Laboratory of Ultraintense Laser and Advanced Material Technology, Shenzhen Technology University, Shenzhen 518118, China
  • 3Center for Advanced Material Diagnostic Technology, Shenzhen Technology University, Shenzhen 518118, China
  • 4Institute of High Energy Physics, Chinese Academy of Sciences, Beijing 100049, China
  • 5Institute of Applied Electronics, CAEP, Mianyang 621900, China
  • 6ZhongkeLansheng Radiate Protection Technology Coperation Limited, Foshan 528200, China
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    DOI: 10.11884/HPLPB202234.210518 Cite this Article
    Dikai Li, Leifeng Cao, [in Chinese], Zheng Zhou, Qiuhong Chen, Chunhui Zhang, Yanmeng Dai, Jian Yu, Miaomiao Yan, Jialing Deng, Xue Wang, [in Chinese]. Radiation protection analysis of 95 MeV RF electron linac[J]. High Power Laser and Particle Beams, 2022, 34(6): 064008 Copy Citation Text show less
    Overall geometric modeling of accelerator and surrounding protective shielding wall
    Fig. 1. Overall geometric modeling of accelerator and surrounding protective shielding wall
    Engineering drawing of beam dump
    Fig. 2. Engineering drawing of beam dump
    Dose equivalent distribution produced by the beam moving from the front of the beam dump(horizontal plane)
    Fig. 3. Dose equivalent distribution produced by the beam moving from the front of the beam dump(horizontal plane)
    Dose equivalent distribution produced by the beam moving from the front of the beam dump (vertical plane)
    Fig. 4. Dose equivalent distribution produced by the beam moving from the front of the beam dump (vertical plane)
    Dose equivalent distribution, at the height where the concrete thickness of the ceiling is 0.5 m, produced by the beam moving from the front of the beam dump (horizontal plane)
    Fig. 5. Dose equivalent distribution, at the height where the concrete thickness of the ceiling is 0.5 m, produced by the beam moving from the front of the beam dump (horizontal plane)
    No.important position normalized divergence/ (mm·mrad−1) geometric divergence/ (mm·mrad−1) beam size/ mm(rms) beam size/cm (FWHM) divergence angle/ mrad divergence angle/mrad (FWHM)
    origin point0.200000.020440.250000.058880.081760.19254
    YAG10.215510.022030.237850.056010.092600.21807
    start of acceleration10.241670.024700.217360.051190.113630.26759
    end of acceleration10.311110.003180.162960.038380.019510.04595
    YAG20.334490.003420.144650.034060.023630.05566
    start of acceleration 20.342130.003500.138670.032660.025220.05938
    end of acceleration 20.411570.002210.084270.019840.026270.06187
    YAG30.423840.002280.074660.017580.030540.07192
    YAG40.440050.002370.061960.014590.038200.08996
    interaction point0.500000.002690.015000.003530.179300.42225
    YAG50.500000.002690.439290.103450.179300.42225
    start of bending magnetic field0.500000.002690.487880.114890.179300.42225
    YAG60.500000.002690.624150.146990.179300.42225
    front end of beam dump0.500000.002690.797440.187800.179300.42225
    Table 1. [in Chinese]
    No.important position remnant beam/% normalization parameter path length/cm path length after interaction point/cm beam energy/MeV γ
    origin point100.0000.000380.0059.785
    YAG199.9620.0006467.0059.785
    start of acceleration199.8980.00170180.0059.785
    end of acceleration199.7270.00057480.005097.847
    YAG299.6700.00019581.005097.847
    start of acceleration 299.6510.00170614.005097.847
    end of acceleration 299.4810.00030914.0095185.91
    YAG399.4500.00040967.0095185.91
    YAG499.4110.001471037.0095185.91
    interaction point99.2630.001391296.000.0095185.91
    YAG599.1240.000151541.00245.0095185.91
    start of bending magnetic field99.1090.000431568.10272.1095185.91
    YAG699.0660.000551644.10348.1095185.91
    front end of beam dump99.0110.990111740.75444.7595185.91
    Table 1. Parameters of beam at important positions
    Dikai Li, Leifeng Cao, [in Chinese], Zheng Zhou, Qiuhong Chen, Chunhui Zhang, Yanmeng Dai, Jian Yu, Miaomiao Yan, Jialing Deng, Xue Wang, [in Chinese]. Radiation protection analysis of 95 MeV RF electron linac[J]. High Power Laser and Particle Beams, 2022, 34(6): 064008
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