{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.131626.v2/t3","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/2164067"}},{"@id":"https://doi.org/10.1140/epjc/s10052-023-11559-y","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Dataset","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2023","description":"Acceptance times efficiency as a function of resonant mass for each event selection step in the search for a neutral...","distribution":[{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/1492676/root","description":"ROOT file","encodingFormat":"https://root.cern"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/1492676/yaml","description":"YAML file","encodingFormat":"https://yaml.org"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/1492676/csv","description":"CSV file","encodingFormat":"text/csv"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/1492676/yoda","description":"YODA file","encodingFormat":"https://yoda.hepforge.org"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/1492676/yoda.h5","description":"YODA.H5 file","encodingFormat":"https://yoda.hepforge.org"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins2164067?version=2"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/131626"}],"inLanguage":"en","includedInDataCatalog":{"@id":"https://doi.org/10.17182/hepdata.131626.v2","@type":"DataCatalog","url":"https://www.hepdata.net/record/ins2164067?version=2"},"isPartOf":{"@id":"https://doi.org/10.17182/hepdata.131626.v2","@type":"Dataset","description":"CERN-LHC. A search for Higgs boson pair ($hh$) production in association with a vector boson ($W\\; {\\textrm or}\\; Z$) is presented, using 139 $fb^{-1}$ of proton--proton collision data at $\\sqrt{s}=13\\,\\text{TeV}$ recorded with the ATLAS detector at the Large Hadron Collider. The search is performed in final states in which the vector boson decays leptonically ($W\\to\\ell\\nu,\\, Z\\to\\ell\\ell,\\nu\\nu$ with $\\ell=e, \\mu$) and the Higgs bosons each decay into a pair of $b$-quarks. It targets $Vhh$ signals from both non-resonant $hh$ production, present in the Standard Model (SM), and resonant $hh$ production, as predicted in some SM extensions. For the resonant search, upper limits on the production cross-sections are derived for two specific models: one is the production of a vector boson along with a neutral heavy scalar resonance $H$, in the mass range 260--1000 GeV, that decays into $hh$, and the other is the production of a heavier neutral pseudoscalar resonance $A$ that decays into a $Z$ boson and $H$ boson, where the $A$ boson mass is 360--800 GeV and the $H$ boson mass is 260--400 GeV. Constraints are also derived in the parameter space of two-Higgs-doublet models.","name":"Search for Higgs boson pair production in association with a vector boson in $pp$ collisions at $\\sqrt{s}=$ 13 TeV with the ATLAS detector","url":"https://www.hepdata.net/record/ins2164067?version=2"},"keywords":"P P --> Z0 HIGGS HIGGS --> LEPTON+ LEPTON- BQ BQBAR BQ BQBAR, N, Events, Proton-Proton, Events, resonance, BSM, Higgs boson, Higgs boson pair, bbbb, 4b, 13000.0","name":"Table 3","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/140267","version":2}