Ka波段同轴锁相Cherenkov振荡器模拟研究

Simulation investigation of a Ka-band coaxial phase-locked Cherenkov oscillator

  • 摘要: 为实现Ka波段高功率微波相干合成,本文提出一种Ka波段同轴锁相Cherenkov振荡器。该器件由电子束预调制区和慢波能量提取区两部分组成:电子束预调制区用于实现外部注入微波功率的高效率吸收和强流相对论电子束的预调制;慢波能量提取区用于实现强流相对论电子束的深度调制和束-波能量的高效率转化。器件输出微波的频率和相位通过预调制电子束进行牵引和调控。无外部注入微波时,电子束预调制区未工作, 器件工作在自激振荡状态,输出微波功率766 MW,自激频率29.001 GHz。在注入微波功率5 kW,注入频率29.000 GHz条件下, 器件工作在相位锁定状态,输出微波相位抖动优于±5°,输出功率为801 MW,输出频率为29.000 GHz。此外,器件注入比和锁相带宽分别为−52 dB和±30 MHz。Ka波段同轴锁相Cherenkov振荡器的设计方法可推广到其他高频段锁相HPM源,为高频段锁相HPM源的设计提供了一种可选的技术方案。

     

    Abstract:
    Background Coherent power combination technology is one of the most effective technical solutions to enhance the radiation power of high-power microwave systems, and has received widespread attention.
    Purpose To achieve high-power microwave coherent power combination in Ka-band, a coaxial phase-locked relativistic Cherenkov oscillator is proposed and investigated in this paper.
    Methods The device can be divided into two parts: an electron beam pre-modulation zone and a slow-wave energy extraction zone. The electron beam pre-modulation zone is designed for efficient absorption of externally injected microwave power and electron beam pre-modulation. The slow-wave energy extraction zone is responsible for deep modulation of the electron beam and efficient energy conversion. The frequency and phase of the microwave output are steered and regulated by the modulated electron beam.
    Results When there is no external injected microwave power, the electron beam pre-modulation zone is inactive, and the device operates in a self-oscillation state, with an output microwave power of 766 MW and a self-oscillation frequency of 29.001 GHz. Under the condition of 5 kW injected microwave power at an injection frequency of 29.000 GHz, the device operates in a phase-locked state, with an output microwave phase jitter better than ±5°, an output power of 801 MW, and an output frequency of 29.000 GHz. Furthermore, the device's injection ratio and phase-locked bandwidth are −52 dB and ±30 MHz, respectively.
    Conclusions The design methodology of the Ka band phase-locked relativistic Cherenkov oscillator can be directly extended to other high-frequency bands, establishing a viable technical framework for developing phase-locked HPM sources across millimeter-wave regimes.

     

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