论文标题

使用$ \ sqrt {s} = 13 $ tev使用Atlas实验的DiLepton事件在Top-Quark衰减中产生的$ W $玻色子的两极分化的测量

Measurement of the polarisation of $W$ bosons produced in top-quark decays using dilepton events at $\sqrt{s} = 13$ TeV with the ATLAS experiment

论文作者

ATLAS Collaboration

论文摘要

提出了质子 - 普罗顿碰撞数据在$ \ sqrt {s} = 13 $ tev的质量中,对$ w $ boson的极化的测量进行了测量。数据是由Atlas检测器在大型强子对撞机上收集的,对应于139 fb $^{ - 1} $的集成光度。进行测量,以选择$ t \ bar {t} $事件,并用两个带电的瘦素(电子或MUON)和至少两个$ b $标记的喷气机腐烂到最终状态。 The polarisation is extracted from the differential cross-section distribution of the $\cos{θ^{*}}$ variable, where $θ^{*}$ is the angle between the momentum direction of the charged lepton from the $W$ boson decay and the reversed momentum direction of the $b$-quark from the top-quark decay, both calculated in the $W$ boson rest frame.针对检测器的接受和分辨率校正了Parton级别的结果,以$ \ cos {θ^{*}} $ angle提出。发现纵向,左和右极化状态的测量分数为$ f_ {0} = 0.684 \ pm 0.005 \,\ Mathrm {(stat。 0.003 \,\ Mathrm {(stat。)} \ pm 0.008 \,\ Mathrm {(syst。)} $和$ f _ {\ Mathrm {\ Mathrm {r}} = -0.002 \ 0.002 \ pm 0.002 \ pm pm 0.002 \,,\ Mathrm {(stat。与标准模型预测。

A measurement of the polarisation of $W$ bosons produced in top-quark decays is presented, using proton-proton collision data at a centre-of-mass energy of $\sqrt{s} = 13$ TeV. The data were collected by the ATLAS detector at the Large Hadron Collider and correspond to an integrated luminosity of 139 fb$^{-1}$. The measurement is performed selecting $t\bar{t}$ events decaying into final states with two charged leptons (electrons or muons) and at least two $b$-tagged jets. The polarisation is extracted from the differential cross-section distribution of the $\cos{θ^{*}}$ variable, where $θ^{*}$ is the angle between the momentum direction of the charged lepton from the $W$ boson decay and the reversed momentum direction of the $b$-quark from the top-quark decay, both calculated in the $W$ boson rest frame. Parton-level results, corrected for the detector acceptance and resolution, are presented for the $\cos{θ^{*}}$ angle. The measured fractions of longitudinal, left- and right-handed polarisation states are found to be $f_{0} = 0.684 \pm 0.005\,\mathrm{(stat.)} \pm 0.014\,\mathrm{(syst.)}$, $f_{\mathrm{L}} = 0.318 \pm 0.003\,\mathrm{(stat.)} \pm 0.008\,\mathrm{(syst.)}$ and $f_{\mathrm{R}} = -0.002 \pm 0.002\,\mathrm{(stat.)} \pm 0.014\,\mathrm{(syst.)}$, in agreement with the Standard Model prediction.

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