ATLAS Forward Proton DetectorsStatus and Plans

P. Erland
{"title":"ATLAS Forward Proton DetectorsStatus and Plans","authors":"P. Erland","doi":"10.22323/1.348.0007","DOIUrl":null,"url":null,"abstract":"Located at Large Hadron Collider (LHC), ATLAS experiment has been designed with the goal of measuring the products of proton--proton collisions. Although it has full azimuthal angle coverage and large acceptance in pseudorapidity, it is insufficient for some of interactions which can take place in interaction point. Such interactions are for example Central Exlusive Productions. It's product is a central system, which can be measured in ATLAS and two protons scattered at small angles into beam pipe beyond the reach of ATLAS. To fully measure such processes another detector is needed. Therefore ATLAS Forward Proton (AFP) detector was installed. \n \nAFP consists of two stations on both sides of ATLAS, located further than 200 m from interaction point. It is practical to move out stations if they are no longer needed (e.g. in runs with special optics) that is why Roman Pot technology was used for installation allowing to move detectors horizontally. Each Roman Pot station is designed to house Silicon Tracker (SiT) and Time of Flight (ToF) detectors. SiT consists of 4 silicon sensor planes to determine proton kinematics by reconstructing it's trajectory from one station to the other. While ToF detector, created from of 16 L-shaped quartz bars, allows us to reduce pile-up by determining the primary vertex of the two protons by measuring the time of theirs arrival. \n \nThis talk is focusing on main features of AFP detector. Roman Pot technology will be explained as well as SiT and ToF structure. In addition performance of SiT planes will be presented and discussed.","PeriodicalId":267466,"journal":{"name":"Proceedings of The 27th International Workshop on Vertex Detectors — PoS(VERTEX2018)","volume":"97 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2019-09-03","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"1","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Proceedings of The 27th International Workshop on Vertex Detectors — PoS(VERTEX2018)","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.22323/1.348.0007","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 1

Abstract

Located at Large Hadron Collider (LHC), ATLAS experiment has been designed with the goal of measuring the products of proton--proton collisions. Although it has full azimuthal angle coverage and large acceptance in pseudorapidity, it is insufficient for some of interactions which can take place in interaction point. Such interactions are for example Central Exlusive Productions. It's product is a central system, which can be measured in ATLAS and two protons scattered at small angles into beam pipe beyond the reach of ATLAS. To fully measure such processes another detector is needed. Therefore ATLAS Forward Proton (AFP) detector was installed. AFP consists of two stations on both sides of ATLAS, located further than 200 m from interaction point. It is practical to move out stations if they are no longer needed (e.g. in runs with special optics) that is why Roman Pot technology was used for installation allowing to move detectors horizontally. Each Roman Pot station is designed to house Silicon Tracker (SiT) and Time of Flight (ToF) detectors. SiT consists of 4 silicon sensor planes to determine proton kinematics by reconstructing it's trajectory from one station to the other. While ToF detector, created from of 16 L-shaped quartz bars, allows us to reduce pile-up by determining the primary vertex of the two protons by measuring the time of theirs arrival. This talk is focusing on main features of AFP detector. Roman Pot technology will be explained as well as SiT and ToF structure. In addition performance of SiT planes will be presented and discussed.
ATLAS正向质子探测器的现状和计划
位于大型强子对撞机(LHC)的ATLAS实验旨在测量质子-质子碰撞的产物。虽然它具有完全的方位角覆盖范围和伪快度接受度,但对于在相互作用点发生的一些相互作用,它是不够的。例如Central exclusive Productions就是这样的互动。它的产物是一个可以在ATLAS中测量的中心系统,两个质子以小角度散射到ATLAS无法到达的束流管中。为了充分测量这些过程,需要另一个探测器。为此,我们安装了ATLAS正向质子(AFP)探测器。AFP由ATLAS两侧的两个站点组成,位于距离交互点200米以上的地方。如果不再需要监测站(例如,在运行中使用特殊光学),则将其移出是可行的,这就是为什么使用罗马锅技术进行安装,允许水平移动探测器。每个罗马锅站设计容纳硅跟踪器(SiT)和飞行时间(ToF)探测器。它由4个硅传感器平面组成,通过重建质子从一个站到另一个站的轨迹来确定质子的运动学。而由16根l形石英棒制成的ToF探测器,通过测量两个质子到达的时间来确定它们的主顶点,使我们能够减少堆积。本讲座主要介绍AFP检测器的主要特点。罗马锅技术以及SiT和ToF结构将被解释。此外,还将介绍和讨论SiT飞机的性能。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
求助全文
约1分钟内获得全文 求助全文
来源期刊
自引率
0.00%
发文量
0
×
引用
GB/T 7714-2015
复制
MLA
复制
APA
复制
导出至
BibTeX EndNote RefMan NoteFirst NoteExpress
×
提示
您的信息不完整,为了账户安全,请先补充。
现在去补充
×
提示
您因"违规操作"
具体请查看互助需知
我知道了
×
提示
确定
请完成安全验证×
copy
已复制链接
快去分享给好友吧!
我知道了
右上角分享
点击右上角分享
0
联系我们:info@booksci.cn Book学术提供免费学术资源搜索服务,方便国内外学者检索中英文文献。致力于提供最便捷和优质的服务体验。 Copyright © 2023 布克学术 All rights reserved.
京ICP备2023020795号-1
ghs 京公网安备 11010802042870号
Book学术文献互助
Book学术文献互助群
群 号:604180095
Book学术官方微信