Y. Ji, R. Dhuley, C. Edward, J. Thangaraj, D. Mihalcea, P. P. O. Mohsen, I. Salehinia, V. Korampally
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引用次数: 0
摘要
为了实现安培级电子束加速器,脉冲传输速率需要比典型的光注入器重复速率高出几千赫兹。我们在此提出一种注入器,原则上能以与工作射频频率相同的速率产生电子束。在连续波模式下工作并在其高轴向电场区域放置场发射元件的传导冷却超导射频腔是产生高重复率电子束的可行方法。本文报道了用铌棒作为场发射极支撑的传导冷却Nb3Sn腔体的研制和实验。初始实验显示平均加速梯度为0.4 MV/m,相当于峰值梯度为3.2 MV/m。测量到的射频腔质量因子为1.4 x 108,略高于我们的目标。获得的场梯度受到相对较低的射频输入功率和外部电源与射频腔之间较差耦合的限制。在理想耦合情况下,场梯度可高达0.6 MV/m,仍低于我们的目标约1 MV/m。
Experiments on a conduction cooled superconducting radio frequency cavity with field emission cathode
To achieve Ampere-class electron beam accelerators the pulse delivery rate need to be much higher than the typical photo injector repetition rate of the order of a few kilohertz. We propose here an injector which can, in principle, generate electron bunches at the same rate as the operating RF frequency. A conduction-cooled superconducting radio frequency (SRF) cavity operating in the CW mode and housing a field emission element at its region of high axial electric field can be a viable method of generating high repetition-rate electron bunches. In this paper, we report the development and experiments on a conduction-cooled Nb3Sn cavity with a niobium rod intended as a field emitter support. The initial experiments demonstrate 0.4 MV/m average accelerating gradient, which is equivalent of peak gradient of 3.2 MV/m. The measured RF cavity quality factor is 1.4 x 108 slightly above our goal. The achieved field gradient is limited by the relatively low input RF power and by the poor coupling between the external power supply and the RF cavity. With ideal coupling the field gradient can be as high as 0.6 MV/m still below our goal of about 1 MV/m.