C. Adolphsen, J. Frisch, R. Jobe, D. McCormick, W. Nelson, T. Raubenheimer, S. Rokni, M. Ross, P. Tenenbaum, D. Walz
{"title":"The Next Linear Collider machine protection system","authors":"C. Adolphsen, J. Frisch, R. Jobe, D. McCormick, W. Nelson, T. Raubenheimer, S. Rokni, M. Ross, P. Tenenbaum, D. Walz","doi":"10.1109/PAC.1999.795677","DOIUrl":null,"url":null,"abstract":"The Next Linear Collider (NLC) electron and positron beams are capable of damaging the linac accelerating structure and beamline vacuum chambers during an individual aberrant accelerator pulse. Machine protection system (MPS) considerations, outlined in this paper for the 1 TeV NLC design, have an impact on the engineering and design of most machine components downstream of the damping ring injector complex. The MPS consists of two functional levels. The first level provides a benign, single bunch, low intensity, high emittance pilot beam that will be used for commissioning and also whenever the integrity or the settings of the downstream components are in doubt. This level also provides for the smooth transition back and forth between high power operation and the benign diagnostic pilot bunch operation. The pilot bunch parameters in the main linac are estimated on the basis of the expected stress in the accelerator structure copper. Beam tests have been done at the SLAC linac to examine the behavior of the copper at the damage stress threshold. Typical pilot beam parameters (compared with nominal) are: 10 times reduced intensity, 10 times increased horizontal emittance and 1000 times increased vertical emittance, resulting in a reduction in charge density of 10/sup 5/. The second level is the primary protection against a single aberrant pulse. Its goal is to reduce the possibility that a substantial transverse field changes the trajectory of the high power beam from one pulse to the next. All devices that could produce such a field are (1) monitored by a fast response network and where possible have (2) deliberately slowed response times. A 'maximum allowable interpulse difference' is evaluated for each such device as well as the beam trajectory monitors in each interpulse period.","PeriodicalId":20453,"journal":{"name":"Proceedings of the 1999 Particle Accelerator Conference (Cat. No.99CH36366)","volume":"42 1","pages":"253-255 vol.1"},"PeriodicalIF":0.0000,"publicationDate":"1999-04-19","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"8","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Proceedings of the 1999 Particle Accelerator Conference (Cat. No.99CH36366)","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/PAC.1999.795677","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 8
Abstract
The Next Linear Collider (NLC) electron and positron beams are capable of damaging the linac accelerating structure and beamline vacuum chambers during an individual aberrant accelerator pulse. Machine protection system (MPS) considerations, outlined in this paper for the 1 TeV NLC design, have an impact on the engineering and design of most machine components downstream of the damping ring injector complex. The MPS consists of two functional levels. The first level provides a benign, single bunch, low intensity, high emittance pilot beam that will be used for commissioning and also whenever the integrity or the settings of the downstream components are in doubt. This level also provides for the smooth transition back and forth between high power operation and the benign diagnostic pilot bunch operation. The pilot bunch parameters in the main linac are estimated on the basis of the expected stress in the accelerator structure copper. Beam tests have been done at the SLAC linac to examine the behavior of the copper at the damage stress threshold. Typical pilot beam parameters (compared with nominal) are: 10 times reduced intensity, 10 times increased horizontal emittance and 1000 times increased vertical emittance, resulting in a reduction in charge density of 10/sup 5/. The second level is the primary protection against a single aberrant pulse. Its goal is to reduce the possibility that a substantial transverse field changes the trajectory of the high power beam from one pulse to the next. All devices that could produce such a field are (1) monitored by a fast response network and where possible have (2) deliberately slowed response times. A 'maximum allowable interpulse difference' is evaluated for each such device as well as the beam trajectory monitors in each interpulse period.
下一代直线对撞机(NLC)的电子和正电子光束能够在单个异常加速器脉冲中破坏直线加速结构和束线真空室。本文为1 TeV NLC设计概述的机器保护系统(MPS)考虑因素对阻尼环喷油器综合体下游大多数机器部件的工程和设计产生了影响。MPS由两个功能级别组成。第一层提供良性、单束、低强度、高发射度的导束,用于调试,也用于下游组件的完整性或设置有疑问的时候。该级别还提供了高功率操作和良性诊断导束操作之间的平稳转换。根据加速器结构铜的预期应力,估计了主直线加速器中的导束参数。在SLAC直线加速器上进行了梁试验,以检查铜在损伤应力阈值下的行为。典型的导束参数(与标称相比)是:强度降低10倍,水平发射度增加10倍,垂直发射度增加1000倍,导致电荷密度降低10/sup 5/。第二层是对单个异常脉冲的主要保护。它的目标是减少一个巨大的横向场改变高功率光束从一个脉冲到下一个脉冲的轨迹的可能性。所有可能产生这种场的设备都(1)由快速响应网络监控,并在可能的情况下(2)故意减慢响应时间。对每个这样的设备以及每个脉冲间周期的波束轨迹监视器进行了“最大允许脉冲间差”评估。