{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.82571.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1664330"}},{"@id":"https://doi.org/10.1007/JHEP09(2018)101","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"CMS Collaboration"},"creator":{"@type":"Organization","name":"CMS Collaboration"},"datePublished":"2018","description":"A search has been performed for heavy resonances decaying to ZZ or ZW in 2$\\ell$2q final states, with two charged leptons ($\\ell$=e,$\\mu$) produced by the decay of a Z boson, and two quarks produced by the decay of a W or Z boson.The analysis is sensitive to resonances with masses in the range from 400 to 4500 GeV. Two categories are defined based on the merged or resolved reconstruction of the hadronically decaying vector boson, optimized for high- and low-mass resonances, respectively.The search is based on data collected during 2016 by the CMS experiment at the LHC in proton-proton collisions with a center-of-mass energy of $\\sqrt{s}$ = 13 TeV, corresponding to an integrated luminosity of 35.9 fb$^{-1}$.No excess is observed in the data above the standard model background expectation.Upper limits on the production cross section of heavy, narrow spin-1 and spin-2 resonances are derived as a function of the resonance mass, and exclusion limits on the production of W' bosons and bulk graviton particles are calculated in the framework of the heavy vector triplet model and warped extra dimensions, respectively.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.82571.v1/t1","@type":"Dataset","description":"Distribution of the merged V candidate $\\tau_{21}$, where the $\\tau_{21}<$ 0.4 requirement has been removed, in data and simulation for...","name":"Figure 1-a"},{"@id":"https://doi.org/10.17182/hepdata.82571.v1/t2","@type":"Dataset","description":"Distribution of the jet $p_{T}$ in data and simulation for events in the signal region of the low-mass analysis. The...","name":"Figure 1-b"},{"@id":"https://doi.org/10.17182/hepdata.82571.v1/t3","@type":"Dataset","description":"Distribution of V candidate $m_{j}$ in data and simulation for events in the signal regions of the low-mass search. The...","name":"Figure 1-c"},{"@id":"https://doi.org/10.17182/hepdata.82571.v1/t4","@type":"Dataset","description":"Distribution of $m_{jj}$ in data and simulation for events in the signal regions of the low-mass search. The points show...","name":"Figure 1-d"},{"@id":"https://doi.org/10.17182/hepdata.82571.v1/t5","@type":"Dataset","description":"The m$_{j}$ distributions of the events in data, compared to the expected background shape, for the high-mass analysis in the...","name":"Figure 2-a"},{"@id":"https://doi.org/10.17182/hepdata.82571.v1/t6","@type":"Dataset","description":"The m$_{j}$ distributions of the events in data, compared to the expected background shape, for the high-mass analysis in the...","name":"Figure 2-b"},{"@id":"https://doi.org/10.17182/hepdata.82571.v1/t7","@type":"Dataset","description":"The m$_{j}$ distributions of the events in data, compared to the expected background shape, for the high-mass analysis in the...","name":"Figure 2-c"},{"@id":"https://doi.org/10.17182/hepdata.82571.v1/t8","@type":"Dataset","description":"The m$_{j}$ distributions of the events in data, compared to the expected background shape, for the high-mass analysis in the...","name":"Figure 2-d"},{"@id":"https://doi.org/10.17182/hepdata.82571.v1/t9","@type":"Dataset","description":"Expected and observed distributions of the resonance candidate mass $m_{\\text{VZ}}$ in the high-mass analysis, in the electron channel, high-purity category....","name":"Figure 3-a"},{"@id":"https://doi.org/10.17182/hepdata.82571.v1/t10","@type":"Dataset","description":"Expected and observed distributions of the resonance candidate mass $m_{\\text{VZ}}$ in the high-mass analysis, in the electron channel, low-purity category....","name":"Figure 3-b"},{"@id":"https://doi.org/10.17182/hepdata.82571.v1/t11","@type":"Dataset","description":"Expected and observed distributions of the resonance candidate mass $m_{\\text{VZ}}$ in the high-mass analysis, in the muon channel, high-purity category....","name":"Figure 3-c"},{"@id":"https://doi.org/10.17182/hepdata.82571.v1/t12","@type":"Dataset","description":"Expected and observed distributions of the resonance candidate mass $m_{\\text{VZ}}$ in the high-mass analysis, in the muon channel, low-purity category....","name":"Figure 3-d"},{"@id":"https://doi.org/10.17182/hepdata.82571.v1/t13","@type":"Dataset","description":"Sideband $m_{ZV}$ distribution for the low-mass search in the merged V, untagged category, after fitting the sideband data alone. The...","name":"Figure 4-a"},{"@id":"https://doi.org/10.17182/hepdata.82571.v1/t14","@type":"Dataset","description":"Sideband $m_{ZV}$ distribution for the low-mass search in the merged V, tagged category, after fitting the sideband data alone. The...","name":"Figure 4-b"},{"@id":"https://doi.org/10.17182/hepdata.82571.v1/t15","@type":"Dataset","description":"Sideband $m_{ZV}$ distribution for the low-mass search in the resolved V, untagged category, after fitting the sideband data alone. The...","name":"Figure 4-c"},{"@id":"https://doi.org/10.17182/hepdata.82571.v1/t16","@type":"Dataset","description":"Sideband $m_{ZV}$ distribution for the low-mass search in the resolved V, tagged category, after fitting the sideband data alone. The...","name":"Figure 4-d"},{"@id":"https://doi.org/10.17182/hepdata.82571.v1/t17","@type":"Dataset","description":"The signal region $m_{VZ}$ distribution for the low-mass search, in the the merged V, untagged category, after fitting the signal...","name":"Figure 5-a"},{"@id":"https://doi.org/10.17182/hepdata.82571.v1/t18","@type":"Dataset","description":"The signal region $m_{VZ}$ distribution for the low-mass search, in the the merged V, tagged category, after fitting the signal...","name":"Figure 5-b"},{"@id":"https://doi.org/10.17182/hepdata.82571.v1/t19","@type":"Dataset","description":"The signal region $m_{VZ}$ distribution for the low-mass search, in the the resolved V, untagged category, after fitting the signal...","name":"Figure 5-c"},{"@id":"https://doi.org/10.17182/hepdata.82571.v1/t20","@type":"Dataset","description":"The signal region $m_{VZ}$ distribution for the low-mass search, in the the resolved V, tagged category, after fitting the signal...","name":"Figure 5-d"},{"@id":"https://doi.org/10.17182/hepdata.82571.v1/t21","@type":"Dataset","description":"Observed and expected 95% CL upper limit on $\\sigma_{W'} Br(W' \\to ZW)$ as a function of the resonance mass, taking...","name":"Figure 6-a"},{"@id":"https://doi.org/10.17182/hepdata.82571.v1/t22","@type":"Dataset","description":"Observed and expected 95% CL upper limit on $\\sigma_{G} Br(G \\to ZZ)$ as a function of the resonance mass, taking...","name":"Figure 6-b"},{"@id":"https://doi.org/10.17182/hepdata.82571.v1/t23","@type":"Dataset","description":"Observed local p-values for W' narrow resonances as a function of the resonance mass.","name":"Figure 7-a"},{"@id":"https://doi.org/10.17182/hepdata.82571.v1/t24","@type":"Dataset","description":"Observed local p-values for G narrow resonances as a function of the resonance mass.","name":"Figure 7-b"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1664330?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/82571"}],"inLanguage":"en","name":"Search for a new heavy resonance decaying into a Z boson and a Z or W boson in 2$\\ell$2q final states at $\\sqrt{s}=$ 13 TeV","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1664330?version=1","version":1}