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Influence of SXFEL resistive wall wakefield on beam phase space distortion

Gong Youwei Cheng Wencai Zhao Minghua Li Xuan Gu Duan Zhang Meng

龚有为, 程文才, 赵明华, 等. SXFEL阻抗壁尾场对束流相空间畸变的影响[J]. 强激光与粒子束, 2022, 34: 064007. doi: 10.11884/HPLPB202234.210491
引用本文: 龚有为, 程文才, 赵明华, 等. SXFEL阻抗壁尾场对束流相空间畸变的影响[J]. 强激光与粒子束, 2022, 34: 064007. doi: 10.11884/HPLPB202234.210491
Gong Youwei, Cheng Wencai, Zhao Minghua, et al. Influence of SXFEL resistive wall wakefield on beam phase space distortion[J]. High Power Laser and Particle Beams, 2022, 34: 064007. doi: 10.11884/HPLPB202234.210491
Citation: Gong Youwei, Cheng Wencai, Zhao Minghua, et al. Influence of SXFEL resistive wall wakefield on beam phase space distortion[J]. High Power Laser and Particle Beams, 2022, 34: 064007. doi: 10.11884/HPLPB202234.210491

SXFEL阻抗壁尾场对束流相空间畸变的影响

doi: 10.11884/HPLPB202234.210491
详细信息
  • 中图分类号: TL53

Influence of SXFEL resistive wall wakefield on beam phase space distortion

More Information
  • 摘要:

    X射线自由电子激光器(FEL)由于其超高亮度、超短脉冲等特点,在世界范围内得到广泛应用。 基于尾流场理论,我们计算了上海X射线自由电子激光器(SXFEL)中从直线加速器出口到波荡器末端,束流在245 m不锈钢传输线和波荡器中的阻抗壁尾场。通过对两种不同的阻抗壁尾场的叠加,发现将导致束流纵向相空间的畸变。在SXFEL上进行束流物理的实验,并得到与理论预测非常吻合的实验结果。 结合之前对主要直线加速器部分的详细模拟和实验研究,为后续FEL整体束流优化提供了参考。

  • Figure  1.  Layout of the SXFEL

    Figure  2.  Total wakefield in the bypass-line 1 and bypass-line 2. $ {\sigma }_{z} $= 0 represents the head of the bunch, and the y-axis represents wakefield in MeV unit

    Figure  3.  Wakefield in the copper flat-plate pipe. The $ {\sigma }_{z} $= 0 represents the head of the bunch, and the y-axis represents wakefield in MeV unit

    Figure  4.  Total wakefield for bypass-line 1, bypass-line 2 and the copper flat-plate pipe. $ {\sigma }_{z} $= 0 represents the head of the bunch, and y-axis represents wakefield in MeV unit

    Figure  5.  Experimental layout of SXFEL

    Figure  6.  (a) Distribution for bunch A, and (b) measured and calculated wakefields in bypass-line 1

    Figure  7.  Measured longitudinal phase space in position 1 and position 2. The figure is separated in 500×500 pixels, and x axis stands for bunch length (left is beam head), y stands for the energy (top is higher energy)

    Figure  8.  The energy distribution in position 1 and position 3

    Figure  9.  (a) Distribution for bunch B and (b) measured and calculated wakefields for all the pipes

    Table  1.   Parameters of three different types of pipes

    materialtypelength/mradius/mm
    bypass-line 1 stainless-steel round 125 17.50
    bypass-line 2 stainless-steel round 120 8.00
    undulator copper flat plate 40 2.15
    下载: 导出CSV

    Table  2.   Initial bunch parameters in SXFEL

    length/µmenergy /GeVcharge/pC
    bunch A 250 1.35 500
    bunch B 120 1.35 500
    下载: 导出CSV
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出版历程
  • 收稿日期:  2021-11-16
  • 修回日期:  2022-03-23
  • 网络出版日期:  2022-03-28
  • 刊出日期:  2022-06-15

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