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dc.contributor.authorTumasyan, A.
dc.contributor.authorAdam, W.
dc.contributor.authorAndrejkovic, J. W.
dc.contributor.authorBergauer, T.
dc.contributor.authorChatterjee, S.
dc.contributor.authorDamanakis, K.
dc.contributor.authorDragicevic, M.
dc.contributor.authorDel Valle, A. E.
dc.contributor.authorHussain, P. S.
dc.contributor.authorJeitler, M.
dc.contributor.authorKrammer, N.
dc.contributor.authorLechner, L.
dc.contributor.authorLiko, D.
dc.contributor.authorMikulec, I.
dc.contributor.authorPaulitsch, P.
dc.contributor.authorPitters, F. M.
dc.contributor.authorSchieck, J.
dc.contributor.authorSchöfbeck, R.
dc.contributor.authorSchwarz, D.
dc.contributor.authorSonawane, M.
dc.date.accessioned2024-04-08T18:00:41Z
dc.date.available2024-04-08T18:00:41Z
dc.date.issued2023-10-25
dc.identifier.issn1434-6052
dc.identifier.urihttps://hdl.handle.net/1721.1/154096
dc.description.abstractThe mass of the top quark is measured in 36.3 $$\,\text {fb}^{-1}$$ fb - 1 of LHC proton–proton collision data collected with the CMS detector at $$\sqrt{s}=13\,\text {Te}\hspace{-.08em}\text {V} $$ s = 13 Te V . The measurement uses a sample of top quark pair candidate events containing one isolated electron or muon and at least four jets in the final state. For each event, the mass is reconstructed from a kinematic fit of the decay products to a top quark pair hypothesis. A profile likelihood method is applied using up to four observables per event to extract the top quark mass. The top quark mass is measured to be $$171.77\pm 0.37\,\text {Ge}\hspace{-.08em}\text {V} $$ 171.77 ± 0.37 Ge V . This approach significantly improves the precision over previous measurements.en_US
dc.publisherSpringer Science and Business Media LLCen_US
dc.relation.isversionof10.1140/epjc/s10052-023-12050-4en_US
dc.rightsCreative Commons Attributionen_US
dc.rights.urihttps://creativecommons.org/licenses/by/4.0/en_US
dc.sourceSpringer Berlin Heidelbergen_US
dc.subjectPhysics and Astronomy (miscellaneous)en_US
dc.subjectEngineering (miscellaneous)en_US
dc.titleMeasurement of the top quark mass using a profile likelihood approach with the lepton + jets final states in proton–proton collisions at $$\sqrt{s}=13\,\text {Te}\hspace{-.08em}\text {V} $$ s = 13 Te Ven_US
dc.typeArticleen_US
dc.identifier.citationThe European Physical Journal C. 2023 Oct 25;83(10):963en_US
dc.contributor.departmentMassachusetts Institute of Technology. Department of Physics
dc.relation.journalThe European Physical Journal Cen_US
dc.identifier.mitlicensePUBLISHER_CC
dc.eprint.versionFinal published versionen_US
dc.type.urihttp://purl.org/eprint/type/JournalArticleen_US
eprint.statushttp://purl.org/eprint/status/PeerRevieweden_US
dc.date.updated2023-11-19T04:53:59Z
dc.language.rfc3066en
dc.rights.holderThe Author(s)
dspace.embargo.termsN
dspace.date.submission2023-11-19T04:53:59Z
mit.journal.volume83en_US
mit.journal.issue10en_US
mit.licensePUBLISHER_CC
mit.metadata.statusAuthority Work and Publication Information Neededen_US


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