PPPS-2013:高电流无铁脉冲四极透镜

C. Tenholt, O. Kester, P. Spiller, U. Blell
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摘要

对于离子在同步加速器之间的转移或对目标的最终聚焦,脉冲无铁四极透镜是非常合适的。对于这些应用,需要极高的场梯度,这是标准磁铁无法实现的,因为它们受到铁轭饱和的限制。另一种选择是超导磁体。大电流脉冲透镜可以在短时间内产生与超导磁体相似的梯度,而无需复杂的低温系统。至少需要一个重态才能使离子束在x轴和y轴上聚焦。SIS18的典型束流能量达到磁场梯度所需的电流约为400 kA。因此,脉冲持续时间需要几个10 μ秒长。它是通过火花间隙放电电容器组来实现的。然后将脉冲施加到形成四极子的四个导体上,它们被串联开关。每个导体都是由许多独立的引线组成的,这些引线被钻孔并相互隔离。这样就补偿了集肤效应的影响。导体的形状等于一个cos(2θ)分布关于它们的尺寸和到光束的距离。为了保护近距离的光束线组件,四极杆由层压的电磁屏障屏蔽,以避免涡流。本文将介绍其概念和仿真。
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PPPS-2013: High current iron-free pulsed quadrupole lenses
For the transfer of ions between synchrotrons or for the final focus on targets, pulsed iron free quadrupole lenses are well suited. For those applications an extremely high field gradient is needed, that cannot be achieved with standard magnets as they are limited by saturation of the iron yoke. Another option would be superconducting magnets. High current pulsed lenses are able to produce a similar gradient for a short time as the superconducting magnets without the complex cryogenic systems. At least one doublet is needed to focus the ion bunches in both x- and y-axes. The current needed to reach magnetic field gradients for typical beam energies of the SIS18 is about 400 kA. Therefore the pulse duration need to be a few 10 μsec long. It is achieved by discharging a capacitor bank through a spark gap. The pulse is then applied to the four conductors forming the quardupole, which are switched in series. Each conductor is built of many separate lead strands, which are drilled and isolated against each other. By this the impacts of the skin effect are compensated. The shape of the conductor equals a cos(2θ)-distribution with respect to their dimensions and the distance to the beam. For the protection of close-by beamline components the quadrupole is shielded by an electromagnetic barrier which is laminated to avoid eddy currents. The concept and simulations will be presented.
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