{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.115182.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/2000816"}},{"@id":"https://doi.org/10.1103/PhysRevD.106.012002","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"CMS Collaboration"},"creator":{"@type":"Organization","name":"CMS Collaboration"},"datePublished":"2022","description":"A search for Kaluza--Klein excited vector boson resonances, $\\mathrm{W}_{\\mathrm{KK}}$, decaying in cascade to three $\\mathrm{W}$ bosons via a scalar radion $\\mathrm{R}$, $\\mathrm{W}_{\\mathrm{KK}} \\to \\mathrm{WR} \\to \\mathrm{WWW}$, with two or three massive jets is presented.The search is performed with proton-proton collision data recorded at $\\sqrt{s}$ = 13 TeV, collected by the CMS experiment at the LHC, during 2016--2018, corresponding to an integrated luminosity of 138 $\\mathrm{fb}^{-1}$.Two final states are simultaneously probed, one where the two $\\mathrm{W}$ bosons produced by the $\\mathrm{R}$ decay are reconstructed as separate, large-radius, massive jets, and one where they are merged in a single large-radius jet.The data observed are in agreement with the standard model expectations.      Limits are set on the product of the $\\mathrm{W}_{\\mathrm{KK}}$ resonance cross section and branching fraction to three W bosons in an extended warped extra-dimensional model.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.115182.v1/t1","@type":"Dataset","description":"Distribution of $m_{\\mathrm{jj}}$ for preselected events with $\\mathrm{N}_{j}$ = 2","name":"m_jj distribution at PS2"},{"@id":"https://doi.org/10.17182/hepdata.115182.v1/t2","@type":"Dataset","description":"Distribution of $m_{\\mathrm{j}}$ for preselected events with $\\mathrm{N}_{j}$ = 2","name":"m_j distribution at PS2"},{"@id":"https://doi.org/10.17182/hepdata.115182.v1/t3","@type":"Dataset","description":"Distribution of the deep-WH value of the highest-mass jet with $m_{\\mathrm{j}}$ > 100 GeV for preselected events with $\\mathrm{N}_{j}$ =...","name":"deep-WH distribution at PS2"},{"@id":"https://doi.org/10.17182/hepdata.115182.v1/t4","@type":"Dataset","description":"Distribution of $m_{\\mathrm{jjj}}$ 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of the jet with highest mass in the single-lepton sideband for LH samples.","name":"deep-W in LH of the single-lepton sideband"},{"@id":"https://doi.org/10.17182/hepdata.115182.v1/t13","@type":"Dataset","description":"The deep-WH discriminant of the jet with highest mass in the single-lepton sideband for HL samples.","name":"deep-WH in HL of the single-lepton sideband"},{"@id":"https://doi.org/10.17182/hepdata.115182.v1/t14","@type":"Dataset","description":"The deep-WH discriminant of the jet with highest mass in the single-lepton sideband for HH samples.","name":"deep-WH in HH of the single-lepton sideband"},{"@id":"https://doi.org/10.17182/hepdata.115182.v1/t15","@type":"Dataset","description":"Comparison of the distribution of data and simulated backgrounds, as a function of the deep-W discriminant value for the highest-mass...","name":"deep-W in CR1"},{"@id":"https://doi.org/10.17182/hepdata.115182.v1/t16","@type":"Dataset","description":"Comparison of the distribution of data and 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