利用质子-质子对撞在 $\sqrt{s}$ = 13 TeV 发生的轻子+射流事件测量极化和自旋相关性并观测顶夸克对中的纠缠现象

CMS Collaboration
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引用次数: 0

摘要

本文介绍了对顶夸克对($\mathrm{tbar\{t}}$)中极化和自旋相关性的测量,这些测量是利用在终态中有单个电子或μ介子和喷流的事件进行的。测量是基于CMS实验在$\sqrt{s}$ = 13 TeV的大型强子对撞机收集的质子-质子对撞数据,对应于138 fb$^{-1}$的综合光度。通过对数据进行分档似然拟合,同时提取了偏振矢量和自旋相关矩阵的所有系数。测量是在额外观测值的包含和分段中进行的,如$\mathrm{t\bar{t}}$系统的质量和$\mathrm{t\bar{t}}$静止帧中的顶夸克散射角。测得的偏振和自旋相关与标准模型一致。根据测量到的自旋相关性,应用佩雷斯-霍罗德茨基准则得出了$\mathrm{t\bar{t}}$自旋纠缠的结论。标准模型预测$\mathrm{t\bar{t}}$态在$\mathrm{t\bar{t}}$系统的产生阈值和高质时会产生纠缠自旋。在高$\mathrm{t\{bar{t}}$质量的事件中首次观测到了纠缠,其中很大一部分$\mathrm{t\{bar{t}}$衰变是类空间分离的,预期和观测到的显著性都超过了5个标准偏差。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Measurements of polarization and spin correlation and observation of entanglement in top quark pairs using lepton+jets events from proton-proton collisions at $\sqrt{s}$ = 13 TeV
Measurements of the polarization and spin correlation in top quark pairs ($\mathrm{t\bar{t}}$) are presented using events with a single electron or muon and jets in the final state. The measurements are based on proton-proton collision data from the LHC at $\sqrt{s}$ = 13 TeV collected by the CMS experiment, corresponding to an integrated luminosity of 138 fb$^{-1}$. All coefficients of the polarization vectors and the spin correlation matrix are extracted simultaneously by performing a binned likelihood fit to the data. The measurement is performed inclusively and in bins of additional observables, such as the mass of the $\mathrm{t\bar{t}}$ system and the top quark scattering angle in the $\mathrm{t\bar{t}}$ rest frame. The measured polarization and spin correlation are in agreement with the standard model. From the measured spin correlation, conclusions on the $\mathrm{t\bar{t}}$ spin entanglement are drawn by applying the Peres-Horodecki criterion. The standard model predicts entangled spins for $\mathrm{t\bar{t}}$ states at the production threshold and at high masses of the $\mathrm{t\bar{t}}$ system. Entanglement is observed for the first time in events at high $\mathrm{t\bar{t}}$ mass, where a large fraction of the $\mathrm{t\bar{t}}$ decays are space-like separated, with an expected and observed significance of above 5 standard deviations.
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