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谐波驱动自种子自由电子激光方案模拟

涂凌君 王晓凡 张未卿

涂凌君, 王晓凡, 张未卿. 谐波驱动自种子自由电子激光方案模拟[J]. 强激光与粒子束, 2024, 36: 071004. doi: 10.11884/HPLPB202436.240102
引用本文: 涂凌君, 王晓凡, 张未卿. 谐波驱动自种子自由电子激光方案模拟[J]. 强激光与粒子束, 2024, 36: 071004. doi: 10.11884/HPLPB202436.240102
Tu Lingjun, Wang Xiaofan, Zhang Weiqing. Simulation of harmonic lasing self-seeded free electron laser[J]. High Power Laser and Particle Beams, 2024, 36: 071004. doi: 10.11884/HPLPB202436.240102
Citation: Tu Lingjun, Wang Xiaofan, Zhang Weiqing. Simulation of harmonic lasing self-seeded free electron laser[J]. High Power Laser and Particle Beams, 2024, 36: 071004. doi: 10.11884/HPLPB202436.240102

谐波驱动自种子自由电子激光方案模拟

doi: 10.11884/HPLPB202436.240102
基金项目: 中国科学院科研仪器设备研制项目(GJJSTD20220001); 国家自然科学基金项目(22288201)
详细信息
    作者简介:

    涂凌君,tulingjun@mail.iasf.ac.cn

    通讯作者:

    王晓凡,wangxf@mail.iasf.ac.cn

    张未卿,weiqingzhang@dicp.ac.cn

  • 中图分类号: TN248.6

Simulation of harmonic lasing self-seeded free electron laser

  • 摘要: 在自由电子激光(FEL)中,谐波驱动自种子(HLSS)可以减小自放大自发辐射(SASE)机制的辐射带宽、提高X射线波段FEL的谱亮度,其原理已被FLASH、PAL、European XFEL等实验室验证。HLSS可改善SASE FEL的相干性,但同时相对SASE并没有提出新的硬件需求,因此可以很方便地应用于国内在建或运行在SASE机制的自由电子激光装置。本文对HLSS方案实现窄带宽效果的原理进行了归纳,给出了波荡器参数的定量条件;随后使用深圳中能高重复频率X射线自由电子激光的典型参数进行模拟,模拟结果表明在出光波长为4.5 nm与6.75 nm时,HLSS的带宽减小至SASE的1/2左右,同时谱亮度提高至2倍左右。
  • 图  1  谐波辐射与基波辐射的滑移对比。对于$ {\lambda }_{1}/3 $辐射波长,其在图1(a)的滑移长度大于图1(b)

    Figure  1.  Comparison of the slippage at $ {\lambda }_{1}/3 $ coming from harmonic generation and fundamental generation. The slippage in Fig.1 (a) is longer than that in Fig.1 (b)

    图  2  特定辐射波长分别由3次谐波辐射与基波辐射产生时,相干长度之比

    Figure  2.  Ratio of coherent lengths at a certain wavelength, for lasing at the third harmonic and at the fundamental wavelength

    图  3  HLSS与SASE对比概念图

    Figure  3.  Conceptual layout of the comparison of HLSS and SASE

    图  4  三次谐波辐射(THG)与基波辐射能量和带宽演化过程对比(10发平均)

    Figure  4.  Comparison of the pulse energy and the bandwidth of FEL (10 shots average), from the third harmonic generation (THG) and from the resonant wavelength

    图  5  HLSS 方案中,扫描第一级波荡器共振波长导致最终出光的能量和带宽(10发平均)的变化

    Figure  5.  Variation of the energy and bandwidth (10 shots average) when scanning resonance wavelength in the HLSS scheme

    图  6  在4.5 nm,HLSS与SASE的对比(10发平均)

    Figure  6.  Comparison of HLSS and SASE (10 shots average) when lasing at 4.5 nm

    图  7  在6.75 nm,HLSS与SASE在波荡器出口的光谱对比(10发平均)

    Figure  7.  Comparison of the spectrum (10 shots average) at 6.75 nm from HLSS and SASE at different distance from the undulator exit

    表  1  模拟用到的参数

    Table  1.   Parameters for simulation

    beam energy/GeVenergy spread/%current/Abeam length/$ {\text{μ}}$mnormalized emittance /$ {\text{μ}}$radperiod/cmperiod numberFODO length/m
    2.530.012800650.394.39310
    下载: 导出CSV
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出版历程
  • 收稿日期:  2024-03-20
  • 修回日期:  2024-05-11
  • 录用日期:  2024-05-11
  • 网络出版日期:  2024-05-29
  • 刊出日期:  2024-05-31

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