pT Measurement of the transverse momentum and ... formula ... distributions of Drell–Yan lepton pairs in proton–proton collisions at ... formula ... TeV with the ATLAS detector
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Measurement of the transverse momentum and ... formula ... distributions of Drell–Yan lepton pairs in proton–proton collisions at ... formula ... TeV with the ATLAS detector

机译:使用ATLAS探测器在公式... TeV的质子-质子碰撞中测量Drell-Yan轻子对的横向动量和...分布

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摘要

Distributions of transverse momentum pT and the related angular variable ϕη of DrellΓÇôYan lepton pairs are measured in 20.3┬áfb-1 of protonΓÇôproton collisions at s=8┬áTeV with the ATLAS detector at the LHC. Measurements in electron-pair and muon-pair final states are corrected for detector effects and combined. Compared to previous measurements in protonΓÇôproton collisions at s=7┬áTeV, these new measurements benefit from a larger data sample and improved control of systematic uncertainties. Measurements are performed in bins of lepton-pair mass above, around and below the Z-boson mass peak. The data are compared to predictions from perturbative and resummed QCD calculations. For values of ϕη<1 the predictions from the Monte Carlo generator ResBos are generally consistent with the data within the theoretical uncertainties. However, at larger values of ϕη this is not the case. Monte Carlo generators based on the parton-shower approach are unable to describe the data over the full range of pT while the fixed-order prediction of Dynnlo falls below the data at high values of pT. ResBos and the parton-shower Monte Carlo generators provide a much better description of the evolution of the ϕη and pT distributions as a function of lepton-pair mass and rapidity than the basic shape of the data.
机译:横向动量分布 p < mi> T 和相关的角度变量 ϕ η 在20.3┬áfb -1 质子Γ质子碰撞中在 s = 8 ┬áTeV,位于LHC的ATLAS检测器上。电子对和μ对最终状态下的测量值会因检测器效应而校正并合并。与先前在 s = 7 ┬áTeV,这些新的测量得益于更大的数据样本和更好的控制系统的不确定性。测量是在Z玻色子质量峰的上方,周围和下方的轻子对质量的仓中进行的。将数据与微扰和恢复QCD计算的预测进行比较。对于 ϕ η / mo> 1 蒙特卡洛发生器ResBos的预测通常与理论不确定性内的数据一致。但是,如果 ϕ η 并非如此。基于parton-shower方法的Monte Carlo生成器无法描述 p T ,而Dynnlo的固定顺序预测低于 p T 。 ResBos和Parton-Shower蒙特卡洛发生器生成器对 ϕ η 和<数学xmlns:mml =“ http://www.w3.org/1998/Math/MathML” id =“ M26”溢出=“ scroll”> p T 分布是轻子对质量和速度的函数,而不是基本形状数据。

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