{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.83971.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1662926"}},{"@id":"https://doi.org/10.1007/JHEP06(2018)120","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"CMS Collaboration"},"creator":{"@type":"Organization","name":"CMS Collaboration"},"datePublished":"2018","description":"A search is presented for new high-mass resonances decaying into electron or muon pairs. The search uses proton-proton collision data at a centre-of-mass energy of 13 TeV collected by the CMS experiment at the LHC in 2016, corresponding to an integrated luminosity of $36\\mathrm{fb}^{-1}$. Observations are in agreement with standard model expectations. Upper limits on the product of a new resonance production cross section and branching fraction to dileptons are calculated in a model-independent manner. This permits the interpretation of the limits in models predicting a narrow dielectron or dimuon resonance. A scan of different intrinsic width hypotheses is performed. Limits are set on the masses of various hypothetical particles. For the $Z'_{\\mathrm{SSM}}$ ($Z'_{\\mathrm{\\Psi}}$) particle, which arises in the sequential standard model (superstring-inspired model), a lower mass limit of 4.50 (3.90) TeV is set at 95% confidence level. The lightest Kaluza--Klein graviton arising in the Randall--Sundrum model of extra dimensions, with coupling parameters $k/\\overline{M}_\\mathrm{Pl}$  of 0.01, 0.05, and 0.10, is excluded at 95% confidence level below 2.10, 3.65, and 4.25 TeV, respectively. In a simplified model of dark matter production via a vector or axial vector mediator, limits at 95% confidence level are obtained on the masses of the dark matter particle and its mediator.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.83971.v1/t1","@type":"Dataset","description":"The number of dielectron events in various invariant mass ranges. The total back- ground is the sum of the events...","name":"Data and estimated background yields in the dielectron channel"},{"@id":"https://doi.org/10.17182/hepdata.83971.v1/t2","@type":"Dataset","description":"The number of dimuon events in various invariant mass ranges. The total back- ground is the sum of the events...","name":"Data and estimated background yields in the dimuon channel"},{"@id":"https://doi.org/10.17182/hepdata.83971.v1/t3","@type":"Dataset","description":"The invariant mass spectra of dielectron events. The points with error bars represent the observed yield. The histogram represents the...","name":"Dielectron mass distribution"},{"@id":"https://doi.org/10.17182/hepdata.83971.v1/t4","@type":"Dataset","description":"The invariant mass spectra of dimuon events. The points with error bars represent the observed yield. The histogram represents the...","name":"Dimuon mass distribution"},{"@id":"https://doi.org/10.17182/hepdata.83971.v1/t5","@type":"Dataset","description":"The cumulative distributions, where all events above the specified mass on the x axis are summed, of the invariant mass...","name":"Cumulative dielectron mass distribution"},{"@id":"https://doi.org/10.17182/hepdata.83971.v1/t6","@type":"Dataset","description":"The cumulative distributions, where all events above the specified mass on the x axis are summed, of the invariant mass...","name":"Cumulative dimuon mass distribution"},{"@id":"https://doi.org/10.17182/hepdata.83971.v1/t7","@type":"Dataset","description":"The observed upper limits at 95% CL on the product of production cross section and branching fraction for a spin-1...","name":"Observed limit in narrow width, spin 1"},{"@id":"https://doi.org/10.17182/hepdata.83971.v1/t8","@type":"Dataset","description":"The expected upper limits together with the 68 and 95% quantiles at 95% 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