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首页> 外文期刊>Nuclear Physics, A: Journal Devoted to the Experimental Study of the Fundamental Constituents of Matter and Their Actions >Centrality, rapidity and p(T) dependence of isolated prompt photon production in lead-lead collisions at root(NN)-N-S=2.76 TeV with the ATLAS detector at the LHC
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Centrality, rapidity and p(T) dependence of isolated prompt photon production in lead-lead collisions at root(NN)-N-S=2.76 TeV with the ATLAS detector at the LHC

机译:在LHC上使用ATLAS探测器在根(NN)-N-S = 2.76 TeV处的铅-铅碰撞中孤立的即时光子产生的中心性,速度和p(T)依赖性

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The ATLAS experiment at the LHC has measured prompt photon production in root(NN)-N-S = 2.76 TeV Pb + Pb collisions using data collected in 2011 with an integrated luminosity of 0.14 nb(-1). The measurement is performed with a hermetic, longitudinally segmented calorimeter, which gives excellent spatial and energy resolution, and detailed information about the shower shape of each measured photon. Using a selection based on shower shapes and an isolation criterion gives measured purities between approximately 50-90%, depending on p(T), eta and centrality. Photon yields, scaled by the mean nuclear thickness function, are determined as a function of collision centrality, pseudorapidity (in two intervals vertical bar eta vertical bar < 1.37 and 1.52 < vertical bar eta vertical bar < 2.37) and transverse momentum (22 < p(T) < 280 GeV). The scaled yields are shown compared to expectations from JETPHOX (perturbative QCD calculations at next to leading order), as are the ratios of the forward yields to those near mid-rapidity (for 22 < p(T) < 140 GeV). The observed photon yields agree well with the predictions for proton proton within statistical and systematic uncertainties, but are unable to distinguish between these calculations and others including isospin and nuclear PDF effects. (C) 2014 CERN. Published by Elsevier B.V. All rights reserved.
机译:LHC的ATLAS实验使用2011年收集的光度为0.14 nb(-1)的数据,测量了根(NN)-N-S = 2.76 TeV Pb + Pb碰撞中迅速产生的光子。使用密封的纵向分段量热计进行测量,该量热计具有出色的空间和能量分辨率,以及有关每个被测光子的簇射形状的详细信息。根据p(T),η和中心度,使用基于花洒形状和隔离标准的选择得出的测得纯度约为50-90%。光子产量由平均核厚度函数确定,取决于碰撞中心性,假快速性(在两个区间中,垂直线eta垂直线<1.37和1.52 <垂直线eta垂直线<2.37)和横向动量(22 (T)<280 GeV)。图中显示的是与JETPHOX的预期值相比的缩放收益率(领先于下一个指令时的扰动QCD计算),以及正向收益率与接近快速波动率的收益率之比(对于22 (T)<140 GeV)。在统计和系统不确定性内,观测到的光子产量与质子质子的预测非常吻合,但无法区分这些计算与其他计算(包括同位旋和核PDF效应)。 (C)2014欧洲核子研究组织。由Elsevier B.V.发布。保留所有权利。

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