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Jet energy measurement and its systematic uncertainty in proton–proton collisions at ... formula ... TeV with the ATLAS detector

机译:使用ATLAS探测器在公式... TeV时质子-质子碰撞的射流能量测量及其系统不确定性

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摘要

The jet energy scale (JES) and its systematic uncertainty are determined for jets measured with the ATLAS detector using proton–proton collision data with a centre-of-mass energy of s=7 TeV corresponding to an integrated luminosity of 4.7 fb -1. Jets are reconstructed from energy deposits forming topological clusters of calorimeter cells using the anti-kt algorithm with distance parameters R = 0.4 or R = 0.6, and are calibrated using MC simulations. A residual JES correction is applied to account for differences between data and MC simulations. This correction and its systematic uncertainty are estimated using a combination of in situ techniques exploiting the transverse momentum balance between a jet and a reference object such as a photon or a Z boson, for 20pTjet<1000GeV and pseudorapidities |η|  4.5. The effect of multiple proton–proton interactions is corrected for, and an uncertainty is evaluated using in situ techniques. The smallest JES uncertainty of less than 1 % is found in the central calorimeter region (|η|  1.2) for jets with 55pTjet<500GeV. For central jets at lower pT, the uncertainty is about 3 %. A consistent JES estimate is found using measurements of the calorimeter response of single hadrons in proton–proton collisions and test-beam data, which also provide the estimate for pTjet>1 TeV. The calibration of forward jets is derived from dijet pT balance measurements. The resulting uncertainty reaches its largest value of 6 % for low-pT jets at |η| = 4.5. Additional JES uncertainties due to specific event topologies, such as close-by jets or selections of event samples with an enhanced content of jets originating from light quarks or gluons, are also discussed. The magnitude of these uncertainties depends on the event sample used in a given physics analysis, but typically amounts to 0.5–3 %.
机译:对于ATLAS探测器测量的射流,其质子-质子碰撞数据的质心能量为 s = 7 < / mn> TeV,对应的综合亮度为4.7 fb -1 。使用距离参数R = 0.4或R = 0.6的anti-kt算法,从形成热量计单元拓扑簇的能量沉积中重建喷气机,并使用MC模拟对其进行校准。残余的JES校正用于解决数据和MC模拟之间的差异。对于 20 p T jet / mo> 1000 GeV 和伪快速度|η| <4.5。校正了多个质子-质子相互作用的影响,并使用原位技术评估了不确定性。在具有 55 p T jet / mo> 500 GeV 。对于较低pT的中央射流,不确定度约为3%。通过测量质子-质子碰撞中单个强子的量热计响应和测试束数据发现了一致的JES估计,这也提供了 p T jet 1 TeV。前向喷嘴的校准来自dijet pT平衡测量。对于低pT射流,在|η|处所产生的不确定性达到6%的最大值。 = 4.5。还讨论了由于特定事件拓扑结构(如近距离喷射或选择事件样本而产生的其他JES不确定性),这些事件样本具有源自轻夸克或胶子的增强的喷射量。这些不确定性的大小取决于给定物理分析中使用的事件样本,但通常为0.5–3%。

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