利用高辐度低温常导射频光枪改进阴极测试

G. Lawler, Fabio Bosco, Martina Carillo, Atsushi Fukasawa, Zenghai Li, N. Majernik, Yusuke Sakai, Sami Tantawi, Oliver Williams, M. Yadav, James Rosenzweig
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摘要

未来的电子加速器应用(如 X 射线自由电子激光器和对撞机)依赖于大幅提高光束亮度。据观察,直列加速器光束操作的最佳最大亮度保持在阴极,因此我们有动力创造一种环境,研究如何实现尽可能高的光枪亮度。为此,我们打算从高亮度光电阴极中提取光束,并利用我们能够管理的最高加速梯度,在一个以速调管为动力的射频(RF)光枪中实现。在这里,我们利用低温正常导电腔,通过限制击穿率(BDR)来实现超高梯度。低温还能降低光发射阈值附近电子的平均横向能量(MTE),从而减少阴极发射率。为此,我们设计并生产了一种新型的原生亮度优化射频枪(CYBORG),用于加州大学洛杉矶分校的一条新光束线。我们将介绍射频和光发射物理学,作为我们打算进入的高场低温阴极新领域的入门知识。我们将进一步报告光束线的调试现状,包括将光枪冷却到 100 K,并产生 0.5 MW 的射频馈电功率,这相当于 80-90 MV/m 范围内的阴极加速场。我们计划进一步迭代改进,使其达到 77 K 和 1 MW,从而实现 >120 MV/m 的最终目标。我们的讨论将包括未来的光束线测试和超高梯度光注入器概念的初步实现。
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Improving Cathode Testing with a High-Gradient Cryogenic Normal Conducting RF Photogun
Future electron accelerator applications such as X-ray free electron lasers and colliders are dependent on significantly increasing beam brightness. With the observation that linac beam manipulation’s best preservation of max brightness is at the cathode, we are incentivized to create an environment where we can study how to achieve the highest possible photogun brightness. In order to do so, we intend to extract beams from high-brightness photocathodes with the highest achievable accelerating gradients we can manage in a klystron-powered radiofrequency (RF) photogun. We utilize here cryogenic normal conducting cavities to achieve ultra-high gradients via limitation of breakdown rates (BDR). The low temperatures should also reduce cathode emittance by reducing the mean transverse energy (MTE) of electrons near the photoemission threshold. To this end, we have designed and produced a new CrYogenic Brightness-Optimized Radiofrequency Gun (CYBORG) for use in a new beamline at UCLA. We will introduce the enabling RF and photoemission physics as a primer for the new regime of high field low temperature cathodes we intend to enter. We further report the current status of the beamline commissioning, including the cooling of the photogun to 100 K, and producing 0.5 MW of RF feed power, which corresponds to cathode accelerating fields in the range of 80–90 MV/m. We further plan iterative improvements to both to 77 K and 1 MW corresponding to our ultimate goal >120 MV/m. Our discussion will include future beamline tests and the consideration of the initial realization of an ultra-high-gradient photoinjector concept.
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