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基于预群聚的回旋管注入锁相研究

马国武 卓婷婷 胡林林 孙迪敏 陈洪斌 孟凡宝

马国武, 卓婷婷, 胡林林, 等. 基于预群聚的回旋管注入锁相研究[J]. 强激光与粒子束, 2018, 30: 083004. doi: 10.11884/HPLPB201830.180025
引用本文: 马国武, 卓婷婷, 胡林林, 等. 基于预群聚的回旋管注入锁相研究[J]. 强激光与粒子束, 2018, 30: 083004. doi: 10.11884/HPLPB201830.180025
Ma Guowu, Zhuo Tingting, Hu Linlin, et al. Study on injection locked gyrotron with pre-bunched beam[J]. High Power Laser and Particle Beams, 2018, 30: 083004. doi: 10.11884/HPLPB201830.180025
Citation: Ma Guowu, Zhuo Tingting, Hu Linlin, et al. Study on injection locked gyrotron with pre-bunched beam[J]. High Power Laser and Particle Beams, 2018, 30: 083004. doi: 10.11884/HPLPB201830.180025

基于预群聚的回旋管注入锁相研究

doi: 10.11884/HPLPB201830.180025
基金项目: 国家高技术发展计划项目
详细信息
    作者简介:

    马国武(1981—),男,硕士,副研究员,主要从事微波器件研究;hunter_ma@126.com

  • 中图分类号: TN722

Study on injection locked gyrotron with pre-bunched beam

  • 摘要: 开展了40 kW预群聚注入锁相回旋管的理论与模拟设计。基于全电磁仿真方法完成了预群聚腔的设计,并采用给定场理论对电子束经过预调制腔后的群聚状态进行了计算。采用自洽理论获得了回旋管的自由振荡工作参数,并计算了振荡频率随各种参数变化的规律,由此提出了锁相带宽的要求。采用PIC粒子模拟进行了锁相状态的模拟,得到7 mm漂移距离下锁定增益可达30.5 dB,相应的锁相带宽为20 MHz。如果进一步增长漂移距离或者进一步增大输入功率,锁相带宽还会增大。理论计算和粒子模拟结果表明40 kW级回旋管注入锁相具有良好的可行性。
  • 图  1  预群聚腔结构

    Figure  1.  Structure of the pre-bunching cavity

    图  2  同轴波导截止频率与半径的关系

    Figure  2.  Cut-off frequency versus radius of the coaxial waveguide

    图  3  预群聚腔的模型及腔内场分布

    Figure  3.  Model and field distribution of the pre-bunching cavity

    图  4  归一化耦合系数与注入半径的关系

    Figure  4.  Normalized coupling coefficient vs radius of the beam

    图  5  群聚因子与漂移长度的关系

    Figure  5.  Bunching factor vs drifting length

    图  6  最佳群聚位置与输入功率的关系

    Figure  6.  Best bunching position vs input power

    图  7  末腔的腔体结构和场分布

    Figure  7.  Structure and field distribution of the last cavity

    图  8  计算所得起振电流与磁场的关系

    Figure  8.  Calculated threshold current vs magnetic intensity

    图  9  自洽理论计算得到的电子束动量变化、输出功率与效率

    Figure  9.  Variation of the electronic momentum, output power and efficiency by self-consistent theory

    图  10  给定场理论计算得到的输出功率与磁场的关系

    Figure  10.  Output power versus magnetic field by fixed-profile theory

    图  11  频率漂移与磁场波动、电流波动之间的关系

    Figure  11.  Frequency shifting vs fluctuation of the magnetic field and the beam current

    图  12  频率漂移与电压波动、腔体半径变化量之间的关系

    Figure  12.  Frequency shifting vs fluctuation of the beam voltage and radius of the cavity

    图  13  预群聚注入锁定的二维PIC模型

    Figure  13.  2-D PIC model of the injection locking with pre-bunched beam

    图  14  自由振荡时的输出功率和频谱

    Figure  14.  Output power and frequency spectrum under free oscillation state

    图  15  注入锁定后的功率频谱

    Figure  15.  Output power and frequency spectrum when injection is locked

    图  16  电子束的能量变化

    Figure  16.  Variation of the energy of the beam

    图  17  锁定带宽与输入功率的关系

    Figure  17.  Locking bandwidth vs input power

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    Tang Changjian, Yang Zhonghai, Liu Pukun. Phase-locking of high power gyrotron. High Power Laser and Particle Beams, 1995, 7(1): 49-56 https://www.cnki.com.cn/Article/CJFDTOTAL-QJGY501.006.htm
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    Liu Jianwei, Zhao Qing. Research and design of quasi-optical mode converter. High Power Laser and Particle Beams, 1995, 7(1): 49-56. doi: 10.3788/HPLPB20132510.2663
    [11] Danly B G, Temkin R J. Generalized nonlinear harmonic gyrotron theory[J]. Phys Fluids, 1986, 29(2): 561-567.
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出版历程
  • 收稿日期:  2018-01-22
  • 修回日期:  2018-04-02
  • 刊出日期:  2018-08-15

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