• High Power Laser and Particle Beams
  • Vol. 36, Issue 8, 083007 (2024)
Qiong Zheng1, Liangjie Bi1,*, Dagui Shen2, Hailong Li1..., Yu Qin1, Bin Wang1, Lin Meng1 and Yong Yin1|Show fewer author(s)
Author Affiliations
  • 1School of Electronic Science and Engineering, University of Electronic Science and Technology of China, Chengdu 611731, China
  • 2Guoguang Electric Co., Ltd., Chengdu 610100, China
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    DOI: 10.11884/HPLPB202436.240109 Cite this Article
    Qiong Zheng, Liangjie Bi, Dagui Shen, Hailong Li, Yu Qin, Bin Wang, Lin Meng, Yong Yin. Mode distribution control of S-band MW-level high-efficiency mutual coupling magnetron[J]. High Power Laser and Particle Beams, 2024, 36(8): 083007 Copy Citation Text show less
    Locked phase difference of the mutual coupling oscillator varies with the bridge length
    Fig. 1. Locked phase difference of the mutual coupling oscillator varies with the bridge length
    Simplified model of high-efficiency mutual coupling phase-locked magnetron
    Fig. 2. Simplified model of high-efficiency mutual coupling phase-locked magnetron
    Equivalent circuit model
    Fig. 3. Equivalent circuit model
    Schematic diagram of double-tube high-efficiency mutual coupling phase-locked structure
    Fig. 4. Schematic diagram of double-tube high-efficiency mutual coupling phase-locked structure
    Electric field distributions of π phase difference mode at /2 and 0 phase difference mode, π- mode, π+ mode at /2时的π相位差模场分布图和 时的0相位差模、π-模、π+模场分布图
    Fig. 5. Electric field distributions of π phase difference mode at /2 and 0 phase difference mode, π- mode, π+ mode at /2时的π相位差模场分布图和 时的0相位差模、π-模、π+模场分布图
    Mode frequency varies with the bridge length, where the solid line represents the theoretical curve and the scattered points represent the simulation results , and the shadow part is the overlapping area
    Fig. 6. Mode frequency varies with the bridge length, where the solid line represents the theoretical curve and the scattered points represent the simulation results , and the shadow part is the overlapping area
    Electronic phase space
    Fig. 7. Electronic phase space
    PIC results at 时的粒子模拟结果
    Fig. 8. PIC results at 时的粒子模拟结果
    Output signal corresponding to different α不同对应的输出信号
    Fig. 9. Output signal corresponding to different α不同对应的输出信号
    Fourier transform spectrum of the output signal corresponding to different α不同对应的输出信号傅里叶变换频谱
    Fig. 10. Fourier transform spectrum of the output signal corresponding to different α不同对应的输出信号傅里叶变换频谱
    Field distribution at each frequency peak in the spectrums corresponding to different 不同对应的频谱中各频率峰处的场分布
    Fig. 11. Field distribution at each frequency peak in the spectrums corresponding to different 不同对应的频谱中各频率峰处的场分布
    PIC results at 时的粒子模拟结果
    Fig. 12. PIC results at 时的粒子模拟结果
    αflow/GHzflocking/GHzfhigh/GHz|flockingflow|/GHz|flockingfhigh|/GHz
    0.72.4432.5730.130
    1.02.3402.5452.7550.2050.210
    1.12.3152.5422.7310.2270.189
    1.32.5152.6300.115
    Table 1. Frequency separation corresponding to different α
    Qiong Zheng, Liangjie Bi, Dagui Shen, Hailong Li, Yu Qin, Bin Wang, Lin Meng, Yong Yin. Mode distribution control of S-band MW-level high-efficiency mutual coupling magnetron[J]. High Power Laser and Particle Beams, 2024, 36(8): 083007
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