"Table 18" of "Differential $t\bar{t}$ cross-section measurements using boosted top quarks in the all-hadronic final state with 139 fb$^{-1}$ of ATLAS data"

Measurements of single-, double-, and triple-differential cross-sections are presented for boosted top-quark pair-production in 13 TeV proton--proton collisions recorded by the ATLAS detector at the LHC. The top quarks are observed through their hadronic decay and reconstructed as large-radius jets with the leading jet having transverse momentum ($p_{\rm T}$) greater than 500 GeV. The observed data are unfolded to remove detector effects. The particle-level cross-section, multiplied by the $t\bar{t}\rightarrow WWb\bar{b}$ branching fraction and measured in a fiducial phase space defined by requiring the leading and second-leading jets to have $p_{\rm T}$ > 500 GeV and $p_{\rm T}$ > 350 GeV, respectively, is $331 \pm 3 \rm{(stat.)} \pm 39 \rm{(syst.)}$ fb. This is approximately 20% lower than the prediction of $398^{+48}_{-49}$ fb by POWHEG+PYTHIA8 with next-to-leading-order (NLO) accuracy but consistent within the theoretical uncertainties. Results are also presented at the parton level, where the effects of top-quark decay, parton showering, and hadronization are removed such that they can be compared with fixed-order next-to-next-to-leading-order (NNLO) calculations. The parton-level cross-section, measured in a fiducial phase space similar to that at particle level, is $1.94 \pm 0.02 \rm{(stat.)} \pm 0.25 \rm{(syst.)}$ pb. This agrees with the NNLO prediction of $1.96^{+0.02}_{-0.17}$ pb. Reasonable agreement with the differential cross-sections is found for most NLO models, while the NNLO calculations are generally in better agreement with the data. The differential cross-sections are interpreted using a Standard Model effective field-theory formalism and limits are set on Wilson coefficients of several four-fermion operators.

针对大型强子对撞机（LHC）ATLAS探测器采集的13 TeV质子-质子碰撞数据，本文报道了大横动量顶夸克对产生过程的单微分、双微分及三微分截面测量结果。顶夸克通过强子衰变被观测，并重建为大半径喷注，其中领头喷注的横向动量（transverse momentum, $p_{
m T}$）大于500 GeV。对观测数据进行解卷处理以扣除探测器效应的影响。在由领头喷注与次领头喷注的横向动量分别大于500 GeV、350 GeV所定义的fiducial相空间（fiducial phase space）中，粒子级截面乘以$tar{t}
ightarrow WWbar{b}$分支比后的测量结果为$331 pm 3
m{(统计误差)} pm 39
m{(系统误差)}$ fb。该结果较POWHEG+PYTHIA8给出的次领头阶（next-to-leading-order, NLO）精度下的理论预言$398^{+48}_{-49}$ fb低约20%，但与考虑理论不确定性后的预言结果一致。本文还给出了部分子级的测量结果：通过移除顶夸克衰变、部分子簇射（parton showering）与强子化效应，使得该结果可与固定阶次的次次领头阶（next-to-next-to-leading-order, NNLO）计算结果进行对比。在与粒子级相似的fiducial相空间（fiducial phase space）中测量得到的部分子级截面为$1.94 pm 0.02
m{(统计误差)} pm 0.25
m{(系统误差)}$ pb。该结果与次次领头阶（NNLO）的理论预言$1.96^{+0.02}_{-0.17}$ pb相符。多数次领头阶（NLO）模型与微分截面结果存在合理的符合程度，而次次领头阶（NNLO）计算结果与实验数据的符合程度总体更优。本文采用标准模型有效场论（Standard Model effective field theory）形式对微分截面进行诠释，并对若干四费米子算符的威尔逊系数（Wilson coefficients）设定了取值限制。