{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.90709.v1/t1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1736895"}},{"@id":"https://doi.org/10.1016/j.physletb.2019.134811","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Dataset","author":{"@type":"Organization","name":"CMS Collaboration"},"creator":{"@type":"Organization","name":"CMS Collaboration"},"datePublished":"2019","description":"Exclusion limits at 95% CL for the branching fractions ($\\mathcal{B}$s) of the $H$ and $Z$ boson decays to $J/\\psi$ or...","distribution":[{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/466660/root","description":"ROOT file","encodingFormat":"https://root.cern"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/466660/yaml","description":"YAML file","encodingFormat":"https://yaml.org"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/466660/csv","description":"CSV file","encodingFormat":"text/csv"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/466660/yoda","description":"YODA file","encodingFormat":"https://yoda.hepforge.org"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1736895?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/90709"}],"inLanguage":"en","includedInDataCatalog":{"@id":"https://doi.org/10.17182/hepdata.90709.v1","@type":"DataCatalog","url":"https://www.hepdata.net/record/ins1736895?version=1"},"isPartOf":{"@id":"https://doi.org/10.17182/hepdata.90709.v1","@type":"Dataset","description":"A search for decays of the Higgs and $Z$ boson to pairs of $J/\\psi$ or $\\Upsilon(nS) (n = 1, 2, 3)$ mesons, with their subsequent decay to $\\mu^+$ $\\mu^\u2212$ pairs, is presented. The analysis uses data from proton-proton collisions at $\\sqrt{s} = 13$ TeV, collected with the CMS detector at the LHC in 2017 and corresponding to an integrated luminosity of 37.5 fb$^{\u22121}$ . While an observation of such a decay with this sample would indicate the presence of physics beyond the standard model, no significant excess is observed. Upper limits at 95% confidence level are placed on the branching fractions of these decays. In the $J/\\psi$ pair channel, the limits are $1.8 \\times 10^{-3}$ and $2.2 \\times 10^{-6}$ for the Higgs and Z boson, respectively, while in the combined $\\Upsilon(nS)$ pair channel, the limits are $1.8 \\times 10^{-3}$ and $1.5 \\times 10^{-6}$ , respectively, when the mesons from the Higgs and Z boson decay are assumed to be unpolarized. When fully longitudinal and transverse polarizations are considered the limits reduce by about $22\u201329$% and increase by about $10\u201313$%, respectively.","name":"Search for Higgs and Z boson decays to J/$\\psi$ or $\\Upsilon$ pairs in proton-proton collisions at $\\sqrt{s}=$ 13 TeV","url":"https://www.hepdata.net/record/ins1736895?version=1"},"keywords":"$H \\rightarrow J/\\psi J/\\psi$, $H \\rightarrow \\Upsilon \\Upsilon$, $Z \\rightarrow J/\\psi J/\\psi$, $Z \\rightarrow \\Upsilon \\Upsilon$","name":"Table 1","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/91236","version":1}