Room temperature accelerator structures for linear colliders
| dc.creator | Miller, R. H. | |
| dc.creator | Jones, R. M. | |
| dc.creator | Adolphsen, C. | |
| dc.creator | Bowden, G. | |
| dc.creator | Dolgashev, V. | |
| dc.creator | Li, N. Kroll Z. | |
| dc.creator | Loewen, R. | |
| dc.creator | Ng, C. | |
| dc.creator | Pearson, C. | |
| dc.creator | Ruth, T. Raubenheimer R. | |
| dc.creator | Tantawi, S. | |
| dc.creator | Wang, J. W. | |
| dc.date | 2001-08-29 | |
| dc.date.accessioned | 2026-07-07T11:32:49Z | |
| dc.date.available | 2026-07-07T11:32:49Z | |
| dc.description | 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 | |
| dc.description | Paper presented at PAC2001(also SLAC-PUB 8889) | |
| dc.identifier | https://arxiv.org/abs/physics/0108063 | |
| dc.identifier | http://arxiv.org/abs/physics/0108063 | |
| dc.identifier | Conf.Proc.C0106181:3819-3821,2001 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/197728 | |
| dc.subject | Accelerator Physics | |
| dc.title | Room temperature accelerator structures for linear colliders | |
| dc.type | text |