{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.129151.v2","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/2107940"}},{"@id":"https://doi.org/10.1140/epjc/s10052-023-11437-7","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2022","description":"A search for a WZ resonance, in the fully  leptonic final state  (electrons and muons), is performed using 139 fb^-1 of data collected at a center-of-mass energy of 13 TeV by the ATLAS detector at the Large Hadron Collider.  The results are interpreted in terms of a singly-charged Higgs boson of the Georgi-Machacek model, produced by WZ-fusion, and of a Heavy Vector Triplet, with the resonance produced by WZ-fusion or the Drell-Yan process.  No significant excess is observed over the Standard Model predictions and limits are set on the production cross-section times branching ratio as a function of the resonance mass for these processes.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.129151.v2/t1","@type":"Dataset","description":"Comparisons of the data and the expected background distributions of the WZ invariant mass in the Drell-Yan signal region. The...","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.129151.v2/t2","@type":"Dataset","description":"Comparisons of the data and the expected background distributions of the WZ invariant mass in the ANN-based VBF signal region....","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.129151.v2/t3","@type":"Dataset","description":"Comparisons of the observed data and the expected background distributions of the WZ invariant mass using the cut-based VBF selection....","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.129151.v2/t4","@type":"Dataset","description":"Drell-Yan signal region selection cutflow for a simulated W' in the HVT model A with m_W' = 1 TeV. The...","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.129151.v2/t5","@type":"Dataset","description":"VBF signal region selection cutflow for a simulated W' in the HVT model C with m_W' = 500 GeV. The...","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.129151.v2/t6","@type":"Dataset","description":"VBF signal region selection cutflow for a simulated H5+ in the GM model with m_H5+ = 450 GeV. The unweighted...","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.129151.v2/t7","@type":"Dataset","description":"The acceptancetimes efficiencyof the HVT W' in the Drell-Yan signal region for different mass points and for the individual channels...","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.129151.v2/t8","@type":"Dataset","description":"The acceptancetimes efficiencyof VBF H5+ selection after the ANN-based VBF selection at different mass points for the individual channels and...","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.129151.v2/t9","@type":"Dataset","description":"The acceptancetimes efficiencyof VBF HVT W' selection after the ANN-based VBF selection at different mass points for the individual channels...","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.129151.v2/t10","@type":"Dataset","description":"The acceptancetimes efficiencyof VBF H5+ selection after the cut-based VBF selection at different mass points for the individual channels and...","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.129151.v2/t11","@type":"Dataset","description":"The acceptancetimes efficiencyof VBF HVT W' selection after the cut-based VBF selection at different mass points for the individual channels...","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.129151.v2/t12","@type":"Dataset","description":"Observed and expected 95% CL exclusion upper limits on sigma * B(W' -> WZ) for the Drell-Yan production of a...","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.129151.v2/t13","@type":"Dataset","description":"Using the ANN VBF selection, observed and expected 95% CL upper limits on sigma * B(W' -> WZ) for the...","name":"Table 13"},{"@id":"https://doi.org/10.17182/hepdata.129151.v2/t14","@type":"Dataset","description":"Using the ANN VBF selection, observed and expected 95% CL upper limits on sigma * B(W' -> WZ) of the...","name":"Table 14"},{"@id":"https://doi.org/10.17182/hepdata.129151.v2/t15","@type":"Dataset","description":"Using the ANN VBF selection, observed and expected 95% CL upper limits on sin(thetaH) of the GM model as a...","name":"Table 15"},{"@id":"https://doi.org/10.17182/hepdata.129151.v2/t16","@type":"Dataset","description":"Using the cut-based VBF selection, observed and expected 95% CL upper limits on sigma * B(W' -> WZ) for the...","name":"Table 16"},{"@id":"https://doi.org/10.17182/hepdata.129151.v2/t17","@type":"Dataset","description":"Using the cut-based VBF selection, observed and expected 95% CL upper limits on sigma * B(W' -> WZ) of the...","name":"Table 17"},{"@id":"https://doi.org/10.17182/hepdata.129151.v2/t18","@type":"Dataset","description":"Using the cut-based VBF selection, observed and expected 95% CL upper limits on sin(thetaH) of the GM model as a...","name":"Table 18"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins2107940?version=2"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/129151"}],"inLanguage":"en","name":"Search for resonant $WZ \\rightarrow \\ell\\nu \\ell^{\\prime}\\ell^{\\prime}$ production in proton$-$proton collisions at $\\mathbf{\\sqrt{s} = 13}$ TeV with the ATLAS detector","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins2107940?version=2","version":2}