High Power Laser and Particle Beams, Volume. 34, Issue 6, 064008(2022)

Radiation protection analysis of 95 MeV RF electron linac

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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    Figures & Tables(7)
    Overall geometric modeling of accelerator and surrounding protective shielding wall
    Engineering drawing of beam dump
    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)
    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)
    • Table 1. [in Chinese]

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      Table 1. [in Chinese]

      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. Parameters of beam at important positions

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      Table 1. Parameters of beam at important positions

      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
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    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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    Paper Information

    Category: Particle Beams and Accelerator Technology

    Received: Nov. 25, 2021

    Accepted: --

    Published Online: Jun. 2, 2022

    The Author Email: Leifeng Cao (caoleifeng@sztu.edu.cn)

    DOI:10.11884/HPLPB202234.210518

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