• Acta Physica Sinica
  • Vol. 69, Issue 17, 175202-1 (2020)
Bo Han1 and Ya-Qiong Liang2、*
Author Affiliations
  • 1Department of Astronomy, Beijing Normal University, Beijing 100875, China
  • 2School of Logistic, Beijing Wuzi University, Beijing 101149, China
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    DOI: 10.7498/aps.69.20200215 Cite this Article
    Bo Han, Ya-Qiong Liang. Measurement of magnetic field of capacitor-coil target using proton radiography[J]. Acta Physica Sinica, 2020, 69(17): 175202-1 Copy Citation Text show less
    (a) Configuration of capacitor-coil target; (b) schematic of magnetic field of capacitor-coil target. Pink-semitransparent is the coil, white arrows indicate the current direction, and colorful arrows indicate the magnetic field in X-Y plane; (c) experimental setup of proton radiography.
    Fig. 1. (a) Configuration of capacitor-coil target; (b) schematic of magnetic field of capacitor-coil target. Pink-semitransparent is the coil, white arrows indicate the current direction, and colorful arrows indicate the magnetic field in X-Y plane; (c) experimental setup of proton radiography.
    Simulation results of Geant4, the coordinates are adjusted at the position of detector: (a) Coil current I = 0; (b) coil current I = 10 kA; (c) coil current I = 50 kA. The red dash regions are the position of the shadow of the coils
    Fig. 2. Simulation results of Geant4, the coordinates are adjusted at the position of detector: (a) Coil current I = 0; (b) coil current I = 10 kA; (c) coil current I = 50 kA. The red dash regions are the position of the shadow of the coils
    (a) Theoretical magnetic strength for I = 10 kA; (b) theoretical magnetic strength for I = 50 kA; (c) theoretical magnetic configuration for I = 10 kA; (d) theoretical magnetic configuration for I = 50 kA. The black dash regions are the position of the shadow of the coils. The coordinates are adjusted at the position of detector
    Fig. 3. (a) Theoretical magnetic strength for I = 10 kA; (b) theoretical magnetic strength for I = 50 kA; (c) theoretical magnetic configuration for I = 10 kA; (d) theoretical magnetic configuration for I = 50 kA. The black dash regions are the position of the shadow of the coils. The coordinates are adjusted at the position of detector
    (a) Reconstructed magnetic strength for I = 10 kA; (b) reconstructed magnetic strength for I = 50 kA; (c) reconstructed magnetic configuration for I = 10 kA; (d) reconstructed magnetic configuration for I = 50 kA. The black dash regions are the position of the shadow of the coils. The coordinates are adjusted at the position of detector
    Fig. 4. (a) Reconstructed magnetic strength for I = 10 kA; (b) reconstructed magnetic strength for I = 50 kA; (c) reconstructed magnetic configuration for I = 10 kA; (d) reconstructed magnetic configuration for I = 50 kA. The black dash regions are the position of the shadow of the coils. The coordinates are adjusted at the position of detector
    (a) Comparison between the mean theoretical and the mean reconstructed magnetic field for the I = 10 kA case in the region of –0.15 cm X I = 50 kA case in the region of –0.15 cm X Y direction. The black solid lines are the theoretical results. The red solid lines are the reconstructed line. The black dash lines are the position of the tips of the coils; (c) comparison of μ value along the Y direction between the I = 10 kA and I = 50 kA cases
    Fig. 5. (a) Comparison between the mean theoretical and the mean reconstructed magnetic field for the I = 10 kA case in the region of –0.15 cm < X < 0.15 cm along Y direction; (b) comparison between the mean theoretical and the mean reconstructed magnetic field for the I = 50 kA case in the region of –0.15 cm < X < 0.15 cm along Y direction. The black solid lines are the theoretical results. The red solid lines are the reconstructed line. The black dash lines are the position of the tips of the coils; (c) comparison of μ value along the Y direction between the I = 10 kA and I = 50 kA cases
    Black solid line and scatters are the relation between current strength and the magnetic flux density at the top of the nickel coil. The colorful solid line and scatters are the corresponding μ values when proton energy is 1, 4, 7.5 and 10 MeV, respectively
    Fig. 6. Black solid line and scatters are the relation between current strength and the magnetic flux density at the top of the nickel coil. The colorful solid line and scatters are the corresponding μ values when proton energy is 1, 4, 7.5 and 10 MeV, respectively
    Bo Han, Ya-Qiong Liang. Measurement of magnetic field of capacitor-coil target using proton radiography[J]. Acta Physica Sinica, 2020, 69(17): 175202-1
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