CMS介子触发系统在13tev质子-质子碰撞中的性能

C. Villalba
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引用次数: 16

摘要

在运行2(涵盖2015-2018)期间,LHC实现了2 × 1034cm−2s−1的最大瞬时亮度,同时以√B = 13 TeV的速度进行质子-质子碰撞。CMS实验的触发系统面临的挑战是将事件速率从约40 MHz降低到约1 kHz。本文介绍了在Run 2中使用的μ子重建和识别算法及其改进。尽管在每次LHC束交叉中额外质子-质子相互作用的数量不断增加,但新的算法在整个数据采集周期内保持了相同甚至更低的介子触发器的接受率。我们将重点关注CMS使用的具有最低可持续横向动量阈值的单和双μ子触发器。效率测量在横向动量范围从8到几百GeV。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Performance of the CMS muon trigger system in proton-proton collisions at 13 TeV
During Run 2 (covering 2015–2018) the LHC achieved a maximum instantaneous luminosity of 2 × 1034cm−2s−1 while delivering proton-proton collisions at √ B = 13 TeV. The challenge for the trigger system of the CMS experiment is to reduce the event rate from about 40 MHz to about 1 kHz. In this document, muon reconstruction and identification algorithms used during Run 2 and their improvements are presented. The new algorithms maintain the acceptance of the muon triggers at the same or even lower rate throughout the data-taking period despite the increasing number of additional proton-proton interactions in each LHC bunch crossing. We will focus on the single and double muon triggers with the lowest sustainable transverse momentum thresholds used by CMS. The efficiency is measured in a transverse momentum range from 8 to several hundred GeV.
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