High-power test of a C-band linear accelerating structure with an RFSoC-based LLRF system.

IF 1.3 4区 工程技术 Q3 INSTRUMENTS & INSTRUMENTATION
C Liu, L Ruckman, R Herbst, D Palmer, V Borzenets, A Dhar, D Amirari, R Agustsson, R Berry, E Nanni
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Abstract

Normal conducting linear particle accelerators consist of multiple rf stations with accelerating structure cavities. Low-level rf (LLRF) systems are employed to set the phase and amplitude of the field in the accelerating structure and to compensate for the pulse-to-pulse fluctuation of the rf field in the accelerating structures with a feedback loop. The LLRF systems are typically implemented with analog rf mixers, heterodyne-based architectures, and discrete data converters. There are multiple rf signals from each of the rf stations, so the number of rf channels required increases rapidly with multiple rf stations. With a large number of rf channels, the footprint, component cost, and system complexity of the LLRF hardware will increase significantly. To meet the design goals of being compact and affordable for future accelerators, we have designed the next-generation LLRF (NG-LLRF) with a higher integration level based on RFSoC technology. The NG-LLRF system samples rf signals directly and performs rf mixing digitally. The NG-LLRF has been characterized in loopback mode to evaluate the performance of the system and has also been tested with a standing-wave accelerating structure, a prototype for the Cool Copper Collider (C3) with a peak rf power level up to 16.45 MW. The loopback test demonstrated amplitude fluctuation below 0.15% and phase fluctuation below 0.15°, which are considerably better than the requirements of C3. The rf signals from the different stages of the accelerating structure at different power levels are measured by the NG-LLRF, which will be critical references for the control algorithm designs. The NG-LLRF also offers flexibility in waveform modulation, so we have used rf pulses with various modulation schemes, which could be useful for controlling some of the rf stations in accelerators. In this paper, the high-power test results at different stages of the test setup will be summarized, analyzed, and discussed.

基于rfsoc的LLRF系统的c波段线性加速结构的大功率测试。
普通导电直线粒子加速器由多个带加速结构腔的射频站组成。低电平射频(LLRF)系统用于设置加速结构中场的相位和幅值,并通过反馈回路补偿加速结构中射频场的脉冲间波动。LLRF系统通常采用模拟射频混频器、基于外差的架构和离散数据转换器来实现。每个射频站都有多个射频信号,因此需要的射频通道数量随着多个射频站的增加而迅速增加。由于有大量射频通道,LLRF硬件的占地面积、组件成本和系统复杂性将显著增加。为了满足未来加速器的紧凑和经济的设计目标,我们设计了基于RFSoC技术的具有更高集成度的下一代LLRF (NG-LLRF)。NG-LLRF系统直接对射频信号进行采样,并以数字方式进行射频混频。NG-LLRF在环回模式下进行了表征,以评估系统的性能,并在驻波加速结构上进行了测试,该驻波加速结构是酷铜对撞机(C3)的原型,峰值射频功率水平高达16.45 MW。环回测试显示幅值波动小于0.15%,相位波动小于0.15°,明显优于C3的要求。利用NG-LLRF测量不同功率水平下加速结构不同阶段的射频信号,为控制算法设计提供重要参考。NG-LLRF还提供了波形调制的灵活性,因此我们使用了具有各种调制方案的rf脉冲,这对于控制加速器中的一些rf站可能很有用。本文将对测试设置不同阶段的大功率测试结果进行总结、分析和讨论。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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来源期刊
Review of Scientific Instruments
Review of Scientific Instruments 工程技术-物理:应用
CiteScore
3.00
自引率
12.50%
发文量
758
审稿时长
2.6 months
期刊介绍: Review of Scientific Instruments, is committed to the publication of advances in scientific instruments, apparatuses, and techniques. RSI seeks to meet the needs of engineers and scientists in physics, chemistry, and the life sciences.
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