MEG II 试验的现状

Marco Francesconi
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引用次数: 0

摘要

MEG II 实验的重点是研究μ介子衰变中的带电质子味 Violation,它在 2021 年运行前及时完成了所有子探测器的调试,目前正在保罗舍勒研究所(瑞士)收集第三年的光束时间。该实验装置专门设计用于搜索 𝜇 + → 𝑒 + 𝛾衰变,目的是提高对分支比的限制,使其从目前由前 MEG 实验设定的 90% 置信度下的 4 . 2 × 10 - 13 提高到 90% 置信度下的 4 × 10 - 13。这需要高性能和轻便的探测器,能够处理来自世界上最强烈的连续 𝜇 + 光束的堆积效应。本文简要概述了所采用的实验技术,然后重点介绍了所收集的数据集和分析策略。虽然我们在 2021 年只积累了几周的数据,但实验对 𝜇 + 的灵敏度已经达到了 8 .8 × 10 - 13,分析受到现有统计数据的很大限制。在会议结束后的几个月里,该数据集被取消了盲法,极限被设定为 7 .5 × 10 - 13 .将这一数据集与现有的极限相结合,得出了目前最佳的排除 𝜇 + → 𝑒 + 𝛾 过程,分支率极限为 3 .1 × 10 - 13,置信度为 90%。最后,MEG II 的数据采集预计将持续到 2026 年底,以达到 6 × 10 - 14 的最终灵敏度。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Status of the MEG II experiment
The MEG II experiment, which focuses on investigating Charged Lepton Flavour Violation in muon decays, completed the commissioning of all subdetectors in time for the 2021 run and it is currently collecting its third year of beam time at the Paul Scherrer Institut (CH). The experimental apparatus has been specifically designed to search for 𝜇 + → 𝑒 + 𝛾 decay, aiming at improving the limit on the branching ratio from the current 4 . 2 × 10 − 13 at 90% confidence level set by the former MEG experiment. This requires high-performance and lightweight detectors capable of handling the pileup effect from world most intense continuous 𝜇 + beam. This contribution provides a brief overview of the experimental techniques employed and then focuses on the description of the collected datasets and analysis strategy. Although we accumulated only a few weeks of data in 2021, the experiment already has a sensitivity of 8 . 8 × 10 − 13 to the 𝜇 + → 𝑒 + 𝛾 branching ratio, with analysis strongly limited by available statistics. In the months following the conference, that dataset was unblinded and the limit was set at 7 . 5 × 10 − 13 . The combination of this with the existing limit yields the current best exclusion of 𝜇 + → 𝑒 + 𝛾 process with a limit in branching ratio of 3 . 1 × 10 − 13 at 90% confidence level. Finally, MEG II data-taking is expected to continue until the end of 2026, to achieve its final sensitivity of 6 × 10 − 14 .
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