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dc.contributor.authorTonon, N.
dc.contributor.authorAarup Petersen, H.
dc.contributor.authorAldaya Martin, M.
dc.contributor.authorAsmuss, P.
dc.contributor.authorBaxter, S.
dc.contributor.authorBayatmakou, M.
dc.contributor.authorBehnke, O.
dc.contributor.authorBermúdez Martínez, A.
dc.contributor.authorBhattacharya, S.
dc.contributor.authorBin Anuar, A. A.
dc.contributor.authorBorras, K.
dc.contributor.authorBrunner, D.
dc.contributor.authorCampbell, A.
dc.contributor.authorCardini, A.
dc.contributor.authorCheng, C.
dc.contributor.authorColombina, F.
dc.contributor.authorConsuegra Rodríguez, S.
dc.contributor.authorCorreia Silva, G.
dc.date.accessioned2021-12-20T13:10:15Z
dc.date.available2021-12-20T13:10:15Z
dc.date.issued2021-12-13
dc.identifier.urihttps://hdl.handle.net/1721.1/138729
dc.description.abstractAbstract A search for new top quark interactions is performed within the framework of an effective field theory using the associated production of either one or two top quarks with a Z boson in multilepton final states. The data sample corresponds to an integrated luminosity of 138 fb−1 of proton-proton collisions at s $$ \sqrt{s} $$ = 13 TeV collected by the CMS experiment at the LHC. Five dimension-six operators modifying the electroweak interactions of the top quark are considered. Novel machine-learning techniques are used to enhance the sensitivity to effects arising from these operators. Distributions used for the signal extraction are parameterized in terms of Wilson coefficients describing the interaction strengths of the operators. All five Wilson coefficients are simultaneously fit to data and 95% confidence level intervals are computed. All results are consistent with the SM expectations.en_US
dc.publisherSpringer Berlin Heidelbergen_US
dc.relation.isversionofhttps://doi.org/10.1007/JHEP12(2021)083en_US
dc.rightsCreative Commons Attributionen_US
dc.rights.urihttps://creativecommons.org/licenses/by/4.0/en_US
dc.sourceSpringer Berlin Heidelbergen_US
dc.titleProbing effective field theory operators in the associated production of top quarks with a Z boson in multilepton final states at s $$ \sqrt{s} $$ = 13 TeVen_US
dc.typeArticleen_US
dc.identifier.citationJournal of High Energy Physics. 2021 Dec 13;2021(12):83en_US
dc.contributor.departmentMassachusetts Institute of Technology. Department of Physics
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.updated2021-12-19T04:11:59Z
dc.language.rfc3066en
dc.rights.holderThe Author(s)
dspace.embargo.termsN
dspace.date.submission2021-12-19T04:11:59Z
mit.licensePUBLISHER_CC
mit.metadata.statusAuthority Work and Publication Information Neededen_US


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