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Ku波段相对论扩展互作用速调管振荡器粒子模拟研究

蒋俊杰 阳福香 党方超 葛行军 张鹏 李家文 邓如金 李志敏

蒋俊杰, 阳福香, 党方超, 等. Ku波段相对论扩展互作用速调管振荡器粒子模拟研究[J]. 强激光与粒子束. doi: 10.11884/HPLPB202436.240190
引用本文: 蒋俊杰, 阳福香, 党方超, 等. Ku波段相对论扩展互作用速调管振荡器粒子模拟研究[J]. 强激光与粒子束. doi: 10.11884/HPLPB202436.240190
Jiang Junjie, Yang Fuxiang, Dang Fangchao, et al. Particle simulation study of Ku-band relativistic extended interaction klystron oscillator[J]. High Power Laser and Particle Beams. doi: 10.11884/HPLPB202436.240190
Citation: Jiang Junjie, Yang Fuxiang, Dang Fangchao, et al. Particle simulation study of Ku-band relativistic extended interaction klystron oscillator[J]. High Power Laser and Particle Beams. doi: 10.11884/HPLPB202436.240190

Ku波段相对论扩展互作用速调管振荡器粒子模拟研究

doi: 10.11884/HPLPB202436.240190
详细信息
    作者简介:

    蒋俊杰,229517315@qq.com

    通讯作者:

    党方超,dangfangchao@sina.com

  • 中图分类号: TN752.5

Particle simulation study of Ku-band relativistic extended interaction klystron oscillator

  • 摘要: 射频击穿、模式竞争是导致速调管振荡器(RKO)功率下降、脉冲缩短的主要原因。本文引入扩展互作用提取结构,可以有效降低提取腔射频电场,增大器件功率容量。传统的双间隙提取结构将电子能量在提取腔内转化为微波能量,共用一个通道输出。而扩展互作用提取结构采用了分布式提取腔而非集中式提取腔,增加了输出通道,可以有效提高束-波转换效率,降低提取腔的射频电场。粒子模拟结果显示:二极管电压561 kV,磁场强度0.5 T条件下,保持阴极结构、调制腔及反射器不变时,分别对传统双间隙提取腔、双间隙及三间隙扩展互作用提取腔进行仿真:输出功率分别为2.14、2.22、2.35 GW;分析其提取腔最大射频电场,分别为1.50、1.21、1.10 MV/cm;束波转换效率分别为35.7%、36.9%、39.1%;器件工作频率为12.52 GHz。在三维仿真中,通过改变阴极结构的S参数、设计新的反射器,有效抑制了调制腔TM113模带来的模式竞争,为开展后续实验奠定了基础。
  • 图  1  相对论扩展互作用速调管振荡器示意图

    Figure  1.  Schematic diagram of a relativistic extended interaction klystron oscillator

    1-dual annular cathode, 2-reflective cavity, 3-modulation cavity, 4-extended interaction extraction, 5-collector

    图  2  归一化电场分布示意图和其对应的电子束负载电导

    Figure  2.  Normalized electric field distribution and electron conductivity

    图  3  提取腔工作模式

    Figure  3.  Working mode of extraction cavity

    图  4  射频电场及输出功率对比示意图

    Figure  4.  Schematic diagram of RF electric field and output power comparison

    图  5  提取腔电子束功率下降对比示意图

    Figure  5.  Comparison of power drop of the electron beam in the extraction cavity

    图  6  输出波导耦合环参数分析

    Figure  6.  Parameter analysis of the output waveguide coupling loop

    图  7  磁场及电压的敏感性分析

    Figure  7.  Sensitivity analysis of magnetic fields and voltages

    图  8  三维电场分布

    Figure  8.  Three-dimensional electric field distribution

    图  9  TEM模与TE11模的S参数

    Figure  9.  S parameters of TEM and TE11 modes

    图  10  新反射器TEM模与TE11模的S参数

    Figure  10.  S-parameters of the new reflector TEM mode and TE11 mode

    图  11  横截面轴向电场示意图

    Figure  11.  Schematic diagram of the axial electric field of the cross-section

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出版历程
  • 收稿日期:  2024-06-06
  • 修回日期:  2024-08-19
  • 录用日期:  2024-08-19
  • 网络出版日期:  2024-08-26

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