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Measurement of the top-quark mass in $ \mathrm{t}\overline{\mathrm{t}} $ events with lepton+jets final states in pp collisions at $ \sqrt{s}=7 $ TeV

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dc.contributor.authorChatrchyan, S.
dc.contributor.authorKhachatryan, V.
dc.contributor.authorSirunyan, A. M.
dc.contributor.authorTumasyan, A.
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dc.contributor.authorSultanov, G.
dc.contributor.authorTcholakov, V.
dc.contributor.authorTrayanov, R.
dc.contributor.authorVutova, M.
dc.contributor.authorDimitrov, A.
dc.contributor.authorHadjiiska, R.
dc.contributor.authorKozhuharov, V.
dc.contributor.authorLitov, L.
dc.contributor.authorPavlov, B.
dc.contributor.authorPetkov, P.
dc.contributor.authorBian, J. G.
dc.contributor.authorChen, G. M.
dc.contributor.authorChen, H. S.
dc.contributor.authorJiang, C. H.
dc.contributor.authorLiang, D.
dc.contributor.authorLiang, S.
dc.contributor.authorMeng, X.
dc.contributor.authorTao, J.
dc.contributor.authorWang, J.
dc.contributor.authorWang, X.
dc.contributor.authorWang, Z.
dc.contributor.authorXiao, H.
dc.contributor.authorXu, M.
dc.contributor.authorZang, J.
dc.contributor.authorZhang, Z.
dc.contributor.authorAsawatangtrakuldee, C.
dc.contributor.authorBan, Y.
dc.contributor.authorGuo, Y.
dc.contributor.authorLi, W.
dc.contributor.authorLiu, S.
dc.contributor.authorMao, Y.
dc.contributor.authorQian, S. J.
dc.contributor.authorTeng, H.
dc.contributor.authorWang, D.
dc.contributor.authorZhang, L.
dc.contributor.authorZou, W.
dc.contributor.authorAvila, C.
dc.contributor.authorGomez, J. P.
dc.contributor.authorGomez Moreno, B.
dc.contributor.authorOsorio Oliveros, A. F.
dc.contributor.authorSanabria, J. C.
dc.contributor.authorGodinovic, N.
dc.contributor.authorLelas, D.
dc.contributor.authorPlestina, R.
dc.contributor.authorPolic, D.
dc.date.accessioned2026-01-26T00:11:30Z
dc.date.issued2012-12-01
dc.description.abstractAbstract The mass of the top quark is measured using a sample of $ \mathrm{t}\overline{\mathrm{t}} $ candidate events with one electron or muon and at least four jets in the final state, collected by CMS in pp collisions at $ \sqrt{s}=7 $ TeV at the LHC. A total of 5174 candidate events is selected from data corresponding to an integrated luminosity of 5.0 fb−1. For each event the mass is reconstructed from a kinematic fit of the decay products to a $ \mathrm{t}\overline{\mathrm{t}} $ hypothesis. The top-quark mass is determined simultaneously with the jet energy scale (JES), constrained by the known mass of the W boson in $ \mathrm{q}\overline{\mathrm{q}} $ decays, to be 173.49 ± 0.43 (stat. + JES) ±0.98 (syst.) GeV.
dc.description.urihttps://doi.org/10.1007/jhep12(2012)105
dc.description.urihttps://link.springer.com/content/pdf/10.1007%2FJHEP12%282012%29105.pdf
dc.description.urihttp://dx.doi.org/10.1007/jhep12(2012)105
dc.description.urihttps://hdl.handle.net/11573/530930
dc.description.urihttps://hdl.handle.net/11391/1223604
dc.description.urihttps://doi.org/10.1007/JHEP12(2012)105
dc.description.urihttps://hdl.handle.net/11585/145256
dc.description.urihttps://doi.org/https://doi.org/10.1007/JHEP12(2012)105
dc.identifier.doi10.1007/jhep12(2012)105
dc.identifier.eissn1029-8479
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dc.identifier.orcid0000-0002-4674-9450
dc.identifier.urihttps://hdl.handle.net/11527/53864
dc.identifier.volume2012
dc.language.isoeng
dc.publisherSpringer Science and Business Media LLC
dc.relation.ispartofJournal of High Energy Physics
dc.rightsOPEN
dc.subjectNuclear and High Energy Physics
dc.subjectHEP
dc.subjectCMS
dc.subjectLHC
dc.titleMeasurement of the top-quark mass in $ \mathrm{t}\overline{\mathrm{t}} $ events with lepton+jets final states in pp collisions at $ \sqrt{s}=7 $ TeV
dc.typeArticle
dspace.entity.typePublication

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