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dc.contributor.authorCMS Collaborationen_US
dc.contributor.authorTumasyan, A.en_US
dc.contributor.authorALPANA, A.en_US
dc.contributor.authorDUBE, SOURABHen_US
dc.contributor.authorKANSAL, B.en_US
dc.contributor.authorLAHA, A.en_US
dc.contributor.authorPANDEY, S.en_US
dc.contributor.authorRASTOGI, A.en_US
dc.contributor.authorSHARMA, SEEMA et al.en_US
dc.date.accessioned2023-12-19T11:03:17Z-
dc.date.available2023-12-19T11:03:17Z-
dc.date.issued2023-10en_US
dc.identifier.citationEuropean Physical Journal C, 83(10), 963.en_US
dc.identifier.issn1434-6044en_US
dc.identifier.issn1434-6052en_US
dc.identifier.urihttps://doi.org/10.1140/epjc/s10052-023-12050-4en_US
dc.identifier.urihttp://dr.iiserpune.ac.in:8080/xmlui/handle/123456789/8355-
dc.description.abstractThe mass of the top quark is measured in 36.3 fb(-1) of LHC proton-proton collision data collected with the CMS detector at root s = 13 TeV. 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 +/- 0.37 GeV. This approach significantly improves the precision over previous measurements.en_US
dc.language.isoenen_US
dc.publisherSpringer Natureen_US
dc.subjectPhysicsen_US
dc.subjectParticles & Fieldsen_US
dc.subject2023-DEC-WEEK3en_US
dc.subjectTOC-DEC-2023en_US
dc.subject2023en_US
dc.titleMeasurement of the top quark mass using a profile likelihood approach with the lepton + jets final states in proton–proton collisions at √s = 13TeVen_US
dc.typeArticleen_US
dc.contributor.departmentDept. of Physicsen_US
dc.identifier.sourcetitleEuropean Physical Journal Cen_US
dc.publication.originofpublisherForeignen_US
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