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arXiv physics/0108063physics.acc-ph
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直线对撞机的室温加速器结构

Room temperature accelerator structures for linear colliders

R. H. Miller, R. M. Jones, C. Adolphsen, G. Bowden, V. Dolgashev, N. Kroll Z. Li, R. Loewen, C. Ng, C. Pearson, T. Raubenheimer R. Ruth, S. Tantawi, J. W. Wang

摘要:

早期对短的低群速和驻波结构的测试表明,X波段直线加速器的加速梯度超过100 MeV/m。传统的行波行波直线加速器随频率的缩放使单元尺寸随l缩放。因为Q按l1/2缩放,所以结构的长度不是线性缩放,而是按l3/2缩放,以便保持通过每个结构的衰减。对于NLC,我们选择不遵循从SLAC S波段直线加速器到X波段四次谐波的这种缩放。我们希望增加结构的长度,以减少耦合器和波导驱动器的数量,这可能是微波直线加速器成本的重要组成部分。此外,缩放的虹膜大小的磁盘加载的结构给出了不可接受的高短程偶极尾场。因此,我们选择将结构的平均群速度和长度增加约5倍,这将以相同的因子增加馈送到每个结构的功率,并以类似的因子减少短程偶极尾流。不幸的是,这些较长(1.8米)的结构没有表现得几乎以及在高梯度测试的短结构。我们相信我们至少对原因有部分了解,并将在下面讨论。我们现在正在研究两种类型的具有大孔径的短结构,其具有中等良好的效率,包括:1)行波结构,其群速度通过在虹膜上具有凸起的每周期进行大相位超前而降低,2)π模式驻波结构

英文摘要:

Early tests of short low group velocity and standing wave structures indicated the viability of operating X-band linacs with accelerating gradients in excess of 100 MeV/m. Conventional scaling of traveling wave traveling wave linacs with frequency scales the cell dimensions with l. Because Q scales as l1/2, the length of the structures scale not linearly but as l3/2 in order to preserve the attenuation through each structure. For NLC we chose not to follow this scaling from the SLAC S-band linac to its fourth harmonic at X-band. We wanted to increase the length of the structures to reduce the number of couplers and waveguide drives which can be a significant part of the cost of a microwave linac. Furthermore, scaling the iris size of the disk-loaded structures gave unacceptably high short range dipole wakefields. Consequently, we chose to go up a factor of about 5 in average group velocity and length of the structures, which increases the power fed to each structure by the same factor and decreases the short range dipole wakes by a similar factor. Unfortunately, these longer (1.8 m) structures have not performed nearly as well in high gradient tests as the short structures. We believe we have at least a partial understanding of the reason and will discuss it below. We are now studying two types of short structures with large apertures with moderately good efficiency including: 1) traveling wave structures with the group velocity lowered by going to large phase advance per period with bulges on the iris, 2) pi mode standing wave structures

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