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dc.contributor.authorCMS Collaborationen_US
dc.contributor.authorSirunyan, A. M.en_US
dc.contributor.authorCHAUHAN, S.en_US
dc.contributor.authorDUBE, SOURABHen_US
dc.contributor.authorHEGDE, V.en_US
dc.contributor.authorKAPOOR, A.en_US
dc.contributor.authorKOTHEKAR, K.en_US
dc.contributor.authorPANDEY, S.en_US
dc.contributor.authorRANE, A.en_US
dc.contributor.authorSHARMA, SEEMA et al.en_US
dc.date.accessioned2019-09-09T11:27:45Z
dc.date.available2019-09-09T11:27:45Z
dc.date.issued2018-01en_US
dc.identifier.citationPhysics Letters B, 776, 355-378.en_US
dc.identifier.issn0370-2693en_US
dc.identifier.issn1873-2445en_US
dc.identifier.urihttp://dr.iiserpune.ac.in:8080/xmlui/handle/123456789/3905-
dc.identifier.urihttps://doi.org/10.1016/j.physletb.2017.11.043en_US
dc.description.abstractThe cross sections for the production of t¯tb¯b and t¯tjj events and their ratio σt¯tb¯b/σt¯tjj are measured using data corresponding to an integrated luminosity of 2.3 fb−1collected in pp collisions at √s=13TeV with the CMS detector at the LHC. Events with two leptons (e or μ) and at least four reconstructed jets, including at least two identified as b quark jets, in the final state are selected. In the full phase space, the measured ratio is 0.022±0.003(stat)±0.006(syst), the cross section σt¯tb¯b is 4.0±0.6(stat)±1.3(syst)pb and σt¯tjj is 184±6(stat)±33(syst)pb. The measurements are compared with the standard model expectations obtained from a powheg simulation at next-to-leading-order interfaced with pythia.en_US
dc.language.isoenen_US
dc.publisherElsevier B.V.en_US
dc.subjectCMSen_US
dc.subjectPhysicsen_US
dc.subjectTop quarken_US
dc.subjectInterfaced with pythiaen_US
dc.subject2018en_US
dc.titleMeasurements of t¯t cross sections in association with b jets and inclusive jets and their ratio using dilepton final states in pp collisions at √s=13TeVen_US
dc.typeArticleen_US
dc.contributor.departmentDept. of Physicsen_US
dc.identifier.sourcetitlePhysics Letters Ben_US
dc.publication.originofpublisherForeignen_US
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