tt¯) production cro'/> Measurement of the ... formula ... production cross-section using ... formula ... events with ... formula ...-tagged jets in ... formula ... collisions at ... formula ... and 8 TeV with the ATLAS detector
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Measurement of the ... formula ... production cross-section using ... formula ... events with ... formula ...-tagged jets in ... formula ... collisions at ... formula ... and 8 TeV with the ATLAS detector

机译:使用带有公式标记的喷嘴的公式事件测量公式的生产横截面ATLAS检测器在...公式...和8 TeV处发生碰撞

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摘要

The inclusive top quark pair (tt¯) production cross-section σtt¯ has been measured in proton–proton collisions at s=7TeV and s=8TeV with the ATLAS experiment at the LHC, using tt¯ events with an opposite-charge eμ pair in the final state. The measurement was performed with the 2011 7 TeV dataset corresponding to an integrated luminosity of 4.6 fb-1 and the 2012 8 TeV dataset of 20.3 fb-1. The numbers of events with exactly one and exactly two b-tagged jets were counted and used to simultaneously determine σtt¯ and the efficiency to reconstruct and b-tag a jet from a top quark decay, thereby minimising the associated systematic uncertainties. The cross-section was measured to be: σtt¯=182.9±3.1±4.2±3.6±3.3pb(s=7TeV)andσtt¯=242.4±1.7±5.5±7.5±4.2pb(s=8TeV),where the four uncertainties arise from data statistics, experimental and theoretical systematic effects, knowledge of the integrated luminosity and of the LHC beam energy. The results are consistent with recent theoretical QCD calculations at next-to-next-to-leading order. Fiducial measurements corresponding to the experimental acceptance of the leptons are also reported, together with the ratio of cross-sections measured at the two centre-of-mass energies. The inclusive cross-section results were used to determine the top quark pole mass via the dependence of the theoretically predicted cross-section on mtpole giving a result of mtpole=172.9-2.6+2.5 GeV. By looking for an excess of tt¯ production with respect to the QCD prediction, the results were also used to place limits on the pair-production of supersymmetric top squarks t~1 with masses close to the top quark mass, decaying via id="IEq27">t~1tχ~10 to predominantly right-handed top quarks and a light neutralino id="IEq28">χ~10, the lightest supersymmetric particle. Top squarks with masses between the top quark mass and 177 GeV are excluded at the 95 % confidence level.
机译:包含性最强的夸克对( t t )生产横截面 σ t t ¯ 已在 s = 7 TeV s = 8 TeV 与ATLAS在LHC上使用 t t 事件,其中带有相反电荷的eμ对最终状态。使用与集成光度4.6 fb -1 相对应的2011 7 TeV数据集和20.3 fb -1 的2012 8 TeV数据集进行测量。计算具有正好一个和正好两个带有b标签的喷射器的事件数,并用于同时确定 σ t t 以及从顶夸克衰变中重建和b-标记喷气机的效率,从而最大程度地减少了相关的系统不确定性。测量横截面为: σ t <移动器> t = 182.9 ± 3.1 ± 4.2 ± 3.6 ± 3.3 pb s = 7 TeV σ t t ¯ = 242.4 ± 1.7 ± 5.5 < mo>± 7.5 ± 4.2 pb s = 8 TeV 其中四个不确定性来自数据统计,实验和理论上的系统效果,综合光度和LHC光束能量的知识。结果与最新的理论QCD计算结果相近(次之)。还报道了与轻子的实验接受相对应的基准测量,以及在两个质心能量处测得的横截面之比。包含性的横截面结果用于通过理论上预测的横截面与 m t 极点 < / msubsup> 给出 m t 极点 <数学xmlns:mml =“ http ://www.w3.org/1998/Math/MathML“ id =” M40“溢出=” scroll“> = 172 。< /mo>9-2.6+ 2.5 GeV。通过查找多余的 t t 生产,结果还用于限制超对称顶夸克的成对生成 t 1 的质量接近顶夸克质量,通过 id =“ IEq27”> t 1 t χ< / mi> 1 0 主要是右撇子顶夸克和浅中性的 id =“ IEq28”> χ < / mover> 1 < mn> 0 ,最轻的超对称粒子。在95%置信度水平下排除质量在顶夸克质量与177 GeV之间的顶夸克。

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