High Power Laser and Particle Beams, Volume. 33, Issue 11, 114001(2021)

Effects of bunch state on measurement of beam emittance and energy

Chaofan An1...2, Xiucui Xie1,*, and Yuehu Pu34 |Show fewer author(s)
Author Affiliations
  • 1Shanghai Institute of Applied Physics, Chinese Academy of Sciences, Shanghai 201800, China
  • 2University of Chinese Academy of Sciences, Beijing 100049, China
  • 3Shanghai APACTRON Particle Equipment Co, Ltd, Shanghai 201800, China
  • 4Shanghai Institute of Advanced Studies, Chinese Academy of Sciences , Shanghai 201210, China
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    Figures & Tables(12)
    Schematic diagram of the beam energy measurement system
    The beam measurement system design structure diagram
    The results of simulated measurement of the APF output beam
    [in Chinese]
    Relationship between the magnetic field gradient of the third magnet and the position of the screen 第3块磁铁磁场梯度变化与荧光靶处的关系
    The relation between j0−j and kinetic energy
    The relation between j0−j and j0−j和的关系
    Tracewin simulated beam current distribution using the Faraday cup
    • Table 1. Initial parameters of ideal and non-ideal bunch

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      Table 1. Initial parameters of ideal and non-ideal bunch

      particle bunch${\alpha }_{x}$$\;{\beta }_{x}$/(mm/(π·mrad)) ${\alpha }_{y}$$\;{\beta }_{y}$/(mm/(π·mrad)) ${\alpha }_{{\textit{z}} }$$\;{\beta }_{{\textit{z}} }$/(mm/(π·mrad)) xx′/(mm/(π·mrad)) yy′/(mm/(π·mrad)) ${E}_{K}$/MeV
      ideal bunch0.1150.7850.1210.760−1.8612.7810.3140.3156.98
      non-ideal bunch0.0200.6400.0270.617−3.3081.6970.3760.3776.79
    • Table 2. The results of the emittance at the entrance obtained by the two methods and their relative errors

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      Table 2. The results of the emittance at the entrance obtained by the two methods and their relative errors

      nameemittance of ideal bunch (normalized RMS)/( $\mathrm{ {\text{π} } }\cdot\mathrm{m}\mathrm{m}\cdot\mathrm{m}\mathrm{r}\mathrm{a}\mathrm{d}$) emittance of non-ideal bunch (normalized RMS)/( $\mathrm{ {\text{π} } }\cdot \mathrm{m}\mathrm{m}\cdot \mathrm{m}\mathrm{r}\mathrm{a}\mathrm{d}$)
      directionxyxy
      emittance at entrance obtained by the least square method0.3020.3020.8210.433
      calculated input emittance of the software0.2880.3020.3760.377
      relative error/%4.640118.3514.85
    • Table 3. Simulated emittance measurement results after changing phase difference

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      Table 3. Simulated emittance measurement results after changing phase difference

      j0j/(°) initial beam emittance (normalized RMS)/( $\mathrm{ {\text{π} } }\cdot\mathrm{m}\mathrm{m}\cdot\mathrm{m}\mathrm{r}\mathrm{a}\mathrm{d}$) fitting the emittance of beam (normalized RMS)/( $\mathrm{ {\text{π} } }\cdot\mathrm{m}\mathrm{m}\cdot\mathrm{m}\mathrm{r}\mathrm{a}\mathrm{d}$) relative error/%
      directionxyxyxy
      10800.3760.3770.3370.35710.375.3
      12600.3760.3770.3630.3643.463.45
      14400.3760.3770.4020.3706.911.86
      16200.3760.3770.4570.37621.540.27
      18000.3760.3770.5150.38336.971.59
      21600.3760.3770.7740.410105.853.3
      23400.3760.3770.8190.432117.8214.59
    • Table 4. Simulation results of beam energy measured by analyzing magnet

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      Table 4. Simulation results of beam energy measured by analyzing magnet

      particle bunchthe highest point where the current through slit2 deviates from point J/mm energy spread/ MeV degree of energy spread/% relative error with standard energy /%
      ideal bunch−0.3750.074441.20.09
      non-ideal bunch−7.50.07961.151.77
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    Chaofan An, Xiucui Xie, Yuehu Pu. Effects of bunch state on measurement of beam emittance and energy[J]. High Power Laser and Particle Beams, 2021, 33(11): 114001

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    Paper Information

    Category: Particle Beams and Accelerator Technology

    Received: Jul. 20, 2021

    Accepted: --

    Published Online: Dec. 1, 2021

    The Author Email: Xie Xiucui (xiexiucui@sinap.ac.cn)

    DOI:10.11884/HPLPB202133.210302

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