ATLAS实验中的触发

J. Berlingen
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引用次数: 0

摘要

大型强子对撞机上的ATLAS实验可以记录大约1 kHz的物理碰撞,而大型强子对撞机设计的束交叉速率为40MHz。为了实现稀有物理事件(如超出标准模型物理)的高选择效率,同时降低大背景率,使用了两级触发系统。事件选择是基于物理特征,如高能轻子、光子、喷流或缺失能量的存在。此外,触发系统利用拓扑信息和多元方法的算法对ATLAS合作所追求的许多物理分析进行过滤。在Run 2中,触发器菜单中包含大约1500个单独的选择,即触发器链,指定用于数据获取的选择算法。触发菜单必须反映给定数据采集周期的物理目标,考虑到LHC的瞬时亮度和ATLAS探测器读出和离线处理农场的限制。概述了2015-2018触发器系统及其性能。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Triggering in the ATLAS Experiment
The ATLAS experiment at the LHC can record about 1 kHz of physics collisions, out of an LHC design bunch crossing rate of 40MHz. To achieve a high selection efficiency for rare physics events (such as beyond the StandardModel physics) while reducing the large background rate, a two-level trigger system is used. The event selection is based on physics signatures, such as the presence of energetic leptons, photons, jets or missing energy. In addition, the trigger system exploits algorithms using topological information and multivariate methods to carry out the filtering for the many physics analyses pursued by the ATLAS collaboration. In Run 2, around 1500 individual selections, the trigger chains, are included in the trigger menu specifying the selection algorithms to be used for data taking. Trigger menus must reflect the physics goals for a given data-taking period, taking the instantaneous luminosity of the LHC and limitations from the ATLAS detector readout and offline processing farm into account. An overview of the 2015–2018 trigger system and its performance is presented.
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