{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.170081.v1/t31","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/3148721"}}]},"@type":"Dataset","additionalType":"Dataset","author":{"@type":"Organization","name":"CMS Collaboration"},"creator":{"@type":"Organization","name":"CMS Collaboration"},"datePublished":"2026","description":"Selection efficiency as a function of the Z$^\\prime$, dark Higgs boson and dark matter particle masses, for 2018 conditions.","distribution":[{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/1937983/root","description":"ROOT file","encodingFormat":"https://root.cern"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/1937983/yaml","description":"YAML file","encodingFormat":"https://yaml.org"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/1937983/csv","description":"CSV file","encodingFormat":"text/csv"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/1937983/yoda","description":"YODA file","encodingFormat":"https://yoda.hepforge.org"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/1937983/yoda.h5","description":"YODA.H5 file","encodingFormat":"https://yoda.hepforge.org"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins3148721?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/170081"}],"inLanguage":"en","includedInDataCatalog":{"@id":"https://doi.org/10.17182/hepdata.170081.v1","@type":"DataCatalog","url":"https://www.hepdata.net/record/ins3148721?version=1"},"isPartOf":{"@id":"https://doi.org/10.17182/hepdata.170081.v1","@type":"Dataset","description":"A search for dark matter produced in association with a dark Higgs boson decaying into a bottom quark-antiquark pair has been performed in proton-proton collisions at a center-of-mass energy of 13 TeV. The search uses data collected with the CMS detector at the CERN LHC during the 2016-2018 data-taking period, corresponding to an integrated luminosity of 138 fb$^{-1}$ The results are interpreted in terms of a theoretical model of dark matter production that, together with a spin-1 gauge boson mediator, predicts the existence of a Higgs-boson-like particle in the dark sector (i.e., a dark Higgs boson). This search focuses on an experimental signature with large missing transverse momentum from dark matter production and a resonant structure in the invariant mass of the bottom quark-antiquark pair from the dark Higgs boson decay. Upper limits at 95% confidence level on the signal strength for dark Higgs boson mass hypotheses below 160 GeV are set. Values of the mediator mass up to 4.5 (2.5) TeV are excluded at 95% confidence level for a dark Higgs boson mass of 50 (150) GeV. This represents the best limits set to date for the dark Higgs boson masses considered in this study.","name":"Search for dark matter produced in association with a dark Higgs boson decaying into a bottom quark-antiquark pair in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","url":"https://www.hepdata.net/record/ins3148721?version=1"},"keywords":"13000, Selection efficiency, dark Higgs, Proton-Proton Scattering, P P --> INVISIBLE BQ BQ","name":"Additional Table - Efficiency - 2018","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/172814","version":1}