注入锁相磁控管作为超导射频加速器替代源的系统研究

Haipeng Wang, T. Plawski, R. Rimmer, A. Dexter, I. Tahir, M. Neubauer, A. Dudas
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引用次数: 5

摘要

作为连续电子束加速器设施(CEBAF) 5kW连续速调管系统的替代方案,采用注入锁相[1]和磁场微调和阳极电压调制慢幅变化的1497MHz高效率磁控管进行了系统的MatLab/Simulink仿真研究。该磁控管模型是根据2.45GHz电磁炉型连续磁控管的实验特点和制造工艺流程图建立的。为了实现电子束负载下超导射频加速腔的高性能,研究了磁控管在两个锁环中的低电平射频控制。在频率锁定环中,模拟了阳极的特征V-I曲线、输出功率(电子管电子效率)和频率对阳极电流(Vaughan模型推动)的依赖关系以及Rieke图(无功负载的频率拉动)。满足哈特里条件下的磁场B和阳极电压V,并考虑了丝加热器功率对频率锁定的影响。在锁相环中,引入了控制注入相稳定性的Adler方程。本文还对磁铁微调线圈电源和阳极电压调制开关电源的控制进行了仿真,以实现调幅。本文将给出SRF腔幅值和相位的线性响应结果。该结果给出了对低电平射频控制的要求。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
System study using injection phase locked magnetron as an alternative source for superconducting radio frequency accelerator
As a drop-in replacement of Continuous Electron Beam Accelerator Facility (CEBAF) 5kW CW klystron system, a 1497MHz, high efficiency magnetron using injection phase lock [1] and slow amplitude variation using magnetic field trimming and anode voltage modulation has been studied systematically using MatLab/Simulink simulations. The magnetron model is based the characteristics of experiment and manufacture chart on a 2.45GHz cooker type CW magnetron. To achieve high performance of a superconducting radio frequency (SRF) acceleration cavity with an electron beam loading, the magnetron's low level radio frequency (LLRF) control has been studied in two lock loops. In the frequency lock loop, the characterized anode V-I curve, output power (the tube electronic efficiency) and frequency dependence to the anode current (pushing by Vaughan model) and the Rieke diagram (frequency pulling by the reactive load) are simulated. The magnetic field B and anode voltage V in Hartree condition are satisfied and the effect of filament heater power to the frequency lock is also included. In the phase lock loop, the Adler equation governing injection phase stability is included in this study. The control of the magnet trim-coil power-supply and of the anode voltage modulation-switching power-supply has been also simulated to achieve the amplitude modulation. The result of linear responses to the amplitude and phase of SRF cavity will be presented in this paper. The requirement of LLRF control will be given by this result.
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