{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.138419.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/2738533"}},{"@id":"https://doi.org/10.1016/j.physletb.2024.138815","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"CMS Collaboration"},"creator":{"@type":"Organization","name":"CMS Collaboration"},"datePublished":"2023","description":"The first evidence for the standard model production of a top quark in association with a W boson and a Z boson is reported. The measurement is performed in multilepton final states, where the Z boson is reconstructed via its decays to electron or muon pairs and the W boson decays either to leptons or hadrons. The analysed data were recorded by the CMS experiment at the CERN LHC in 2016-2018 in proton-proton collisions at $\\sqrt{s}$ = 13 TeV, and correspond to an integrated luminosity of 138 fb$^{-1}$. The measured cross section is 354 $\\pm$ 54 (stat) $\\pm$ 95 (syst) fb, and corresponds to a statistical significance of 3.4 standard deviations.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.138419.v1/t1","@type":"Dataset","description":"Expected yields for signal and background processes and observed number of events in the signal and control regions","name":"Tables 1 and 2"},{"@id":"https://doi.org/10.17182/hepdata.138419.v1/t2","@type":"Dataset","description":"Postfit b jet multiplicity distribution in the $\\text{SR}_\\text{4l}$","name":"Figure 3 (lower right)"},{"@id":"https://doi.org/10.17182/hepdata.138419.v1/t3","@type":"Dataset","description":"Postfit score of the tWZ output node from the multiclass classifier in $\\text{SR}_\\text{3l,3j}$ for events with exactly 1 b jet","name":"Figure 3 (upper left)"},{"@id":"https://doi.org/10.17182/hepdata.138419.v1/t4","@type":"Dataset","description":"Postfit score of the $\\text{t}\\bar{\\text{t}}\\text{Z}$ output node from the multiclass classifier in $\\text{SR}_\\text{3l,3j}$ for events with at least 2 b...","name":"Figure 3 (upper right)"},{"@id":"https://doi.org/10.17182/hepdata.138419.v1/t5","@type":"Dataset","description":"Postfit score of the tWZ output node from the binary classifier in $\\text{SR}_\\text{3l,2j}$","name":"Figure 3 (lower left)"},{"@id":"https://doi.org/10.17182/hepdata.138419.v1/t6","@type":"Dataset","description":"$\\text{p}_\\text{T}$ of the leading jet in the $\\text{SR}_\\text{3l,2j}$","name":"Figure 2 (lower right)"},{"@id":"https://doi.org/10.17182/hepdata.138419.v1/t7","@type":"Dataset","description":"$\\text{p}_\\text{T}$ of the leading lepton in the $\\text{SR}_\\text{3l,2j}$","name":"Figure 2 (lower left)"},{"@id":"https://doi.org/10.17182/hepdata.138419.v1/t8","@type":"Dataset","description":"Max $\\text{p}_\\text{T}$ of the lepton-jet in the $\\text{SR}_\\text{3l,3j}$","name":"Figure 2 (upper left)"},{"@id":"https://doi.org/10.17182/hepdata.138419.v1/t9","@type":"Dataset","description":"Invariant mass of the system of leptons, jets, and $\\vec{\\text{p}}^\\text{miss}_\\text{T}$ in the $\\text{SR}_\\text{3l,3j}$","name":"Figure 2 (upper right)"},{"@id":"https://doi.org/10.17182/hepdata.138419.v1/t10","@type":"Dataset","description":"Two-dimensional likelihood scan of the signal strenghts of tWZ ($\\mu_\\text{tWZ}$) vs. $\\text{t}\\bar{\\text{t}}\\text{Z}$ ($\\mu_{\\text{t}\\bar{\\text{t}}\\text{Z}}$). The blue lines show the 68%, 95%,...","name":"Figure 4"},{"@id":"https://doi.org/10.17182/hepdata.138419.v1/t11","@type":"Dataset","description":"Two-dimensional likelihood scan of the signal strenghts of tWZ ($\\mu_\\text{tWZ}$) vs. $\\text{t}\\bar{\\text{t}}\\text{Z}$ ($\\mu_{\\text{t}\\bar{\\text{t}}\\text{Z}}$). The blue lines show the 68%, 95%,...","name":"Figure 4 limits"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins2738533?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/138419"}],"inLanguage":"en","name":"Evidence for tWZ production in proton-proton collisions at $\\sqrt{s}$ = 13 TeV in multilepton final states","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins2738533?version=1","version":1}