用ATLAS探测器测量质子-质子对撞中$\sqrt{s}=13$ TeV的顶夸克对产生与粲夸克的关系

ATLAS Collaboration
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摘要

2015年至2018年期间,在大型强子对撞机上利用ATLAS实验收集到的质子-质子对撞数据,在13 TeV的质量中心能量下测量了顶夸克对产生的包涵截面,对应于140 fb$^{-1}$的综合光度。测量需要一个或两个带电轻子(电子和μ介子)、两个b$标记的射流,以及最终状态中至少一个额外的射流。为了同时识别b$射流和c$射流,采用了一种定制的味道标记算法。在一个复制了ATLAS探测器接受度的固定相空间中,测量到的$t\bar{t}+ {\geq} 2c$和$t\bar{t}+1c$产生的横截面分别为$1.28^{+0.27}_{-0.24}\text{pb}$和$6.4^{+1.0}_{-0.9}\text{pb}$。测量结果主要受到包容性$t\bar{t}$ 和$t\bar{t}+b\bar{b}$ 产生的建模中的不确定性、味道标记算法校准中的不确定性以及数据统计的限制。在对t/bar{t}$衰变产物和射流倍率没有要求的相空间中,$t/bar{t}+ {\geq} 2c$和$t/bar{t}+1c$的横截面与总$t/bar{t}+text{jets}$产生的比率被确定为$(1.23\pm 0.25) \%$和$(8.8\pm 1.3) \%$。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Measurement of top-quark pair production in association with charm quarks in proton-proton collisions at $\sqrt{s}=13$ TeV with the ATLAS detector
Inclusive cross-sections for top-quark pair production in association with charm quarks are measured with proton-proton collision data at a center-of-mass energy of 13 TeV corresponding to an integrated luminosity of 140 fb$^{-1}$, collected with the ATLAS experiment at the LHC between 2015 and 2018. The measurements are performed by requiring one or two charged leptons (electrons and muons), two $b$-tagged jets, and at least one additional jet in the final state. A custom flavor-tagging algorithm is employed for the simultaneous identification of $b$-jets and $c$-jets. In a fiducial phase space that replicates the acceptance of the ATLAS detector, the cross-sections for $t\bar{t}+ {\geq} 2c$ and $t\bar{t}+1c$ production are measured to be $1.28^{+0.27}_{-0.24}\;\text{pb}$ and $6.4^{+1.0}_{-0.9}\;\text{pb}$, respectively. The measurements are primarily limited by uncertainties in the modeling of inclusive $t\bar{t}$ and $t\bar{t}+b\bar{b}$ production, in the calibration of the flavor-tagging algorithm, and by data statistics. Cross-section predictions from various $t\bar{t}$ simulations are largely consistent with the measured cross-section values, though all underpredict the observed values by 0.5 to 2.0 standard deviations. In a phase-space volume without requirements on the $t\bar{t}$ decay products and the jet multiplicity, the cross-section ratios of $t\bar{t}+ {\geq} 2c$ and $t\bar{t}+1c$ to total $t\bar{t}+\text{jets}$ production are determined to be $(1.23 \pm 0.25) \%$ and $(8.8 \pm 1.3) \%$.
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