Please use this identifier to cite or link to this item: https://hdl.handle.net/2440/102723
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dc.contributor.authorAad, G.-
dc.contributor.authorAbbott, B.-
dc.contributor.authorAbdallah, J.-
dc.contributor.authorAbdel Khalek, S.-
dc.contributor.authorAbdinov, O.-
dc.contributor.authorAben, R.-
dc.contributor.authorAbi, B.-
dc.contributor.authorAbolins, M.-
dc.contributor.authorAbouZeid, O.-
dc.contributor.authorAbramowicz, H.-
dc.contributor.authorAbreu, H.-
dc.contributor.authorAbreu, R.-
dc.contributor.authorAbulaiti, Y.-
dc.contributor.authorAcharya, B.-
dc.contributor.authorAdamczyk, L.-
dc.contributor.authorAdams, D.-
dc.contributor.authorAdelman, J.-
dc.contributor.authorAdomeit, S.-
dc.date.issued2015-
dc.identifier.citationThe Journal of High Energy Physics, 2015; 2015(6):1-55-
dc.identifier.issn1029-8479-
dc.identifier.issn1126-6708-
dc.identifier.urihttp://hdl.handle.net/2440/102723-
dc.description.abstractAbstract: Various differential cross-sections are measured in top-quark pair (tt) events produced in proton-proton collisions at a centre-of-mass energy of √s = 7 TeV at the LHC with the ATLAS detector. These differential cross-sections are presented in a data set corresponding to an integrated luminosity of 4.6 fb−1. The differential cross-sections are presented in terms of kinematic variables, such as momentum, rapidity and invariant mass, of a top-quark proxy referred to as the pseudo-top-quark as well as the pseudo-top-quark pair system. The dependence of the measurement on theoretical models is minimal. The measurements are performed on tt events in the lepton+jets channel, requiring exactly one charged lepton and at least four jets with at least two of them tagged as originating from a b-quark. The hadronic and leptonic pseudo-top-quarks are defined via the leptonic or hadronic decay mode of the W boson produced by the top-quark decay in events with a single charged lepton. Differential cross-section measurements of the pseudo-top-quark variables are compared with several Monte Carlo models that implement next-to-leading order or leading-order multi-leg matrix-element calculations.-
dc.description.statementofresponsibilityG. Aad … P. Jackson … L. Lee … A. Petridis … N. Soni ... M. White ... et al. (The ATLAS Collaboration)-
dc.language.isoen-
dc.publisherSpringer-
dc.rightsCopyright CERN, for the benefit of the ATLAS Collaboration. Article funded by SCOAP3.This article is distributed under the terms of the Creative Commons Attribution License (CC-BY 4.0), which permits any use, distribution and reproduction in any medium, provided the original author(s) and source are credited.-
dc.source.urihttp://dx.doi.org/10.1007/jhep06(2015)100-
dc.subjectHadron-Hadron scattering; top physics-
dc.titleDifferential top-antitop cross-section measurements as a function of observables constructed from final-state particles using pp collisions at √s = 7 TeV in the ATLAS detector-
dc.title.alternativeDifferential top-antitop cross-section measurements as a function of observables constructed from final-state particles using pp collisions at root s = 7 TeV in the ATLAS detector-
dc.typeJournal article-
dc.identifier.doi10.1007/JHEP06(2015)100-
pubs.publication-statusPublished-
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