{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.83967.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1683431"}},{"@id":"https://doi.org/10.1140/epjc/s10052-018-6457-x","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2018","description":"CERN-LHC, ATLAS.\nLimits on pair production of Higgs bosons in the final state where one Higgs boson (H) decays to two photons and the other to a b-quark together with its antiparticle.\nThe search is based on 36.1 +/- 1.2 fb^{-1} of pp collisions at sqrt{s} = 13 TeV recorded in 2015 and 2016 with the ATLAS detector at the CERN Large Hadron Collider.\nData include at least one lepton (electron or muon), at least two central jets (no $b$-jet) and two well-identified isolated photons.\nThe search is sensitive to both resonant and non-resonant production of Higgs boson pairs.\nPreselection:\n- Among isolated photons take the two with highest pT and require ET > 0.35 * m_gammagamma and ET > 0.25 * m_gammagamma respectively;\n- 105 < m_gammagamma < 160 GeV. \nAfter this preselection, further three selections are applied.\n- At least one lepton, pT > 10 GeV, 1.37 < |eta| < 1.52 for electrons or < |eta| < for muons;\n- At least two central jets, |eta| < 2.5, pT > 25 GeV; \n- no $b$-jet tagged by 70% b-tagging woking point.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.83967.v1/t1","@type":"Dataset","description":"Number of data events without pTyy selection for $m_X$ = 260 GeV.","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.83967.v1/t2","@type":"Dataset","description":"Number of data events witht pTyy selection for non-resonant.","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.83967.v1/t3","@type":"Dataset","description":"Observed and expected 95% CL upper limits on the cross-section of gluon-fusion initialted resonant production of the mass of the...","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.83967.v1/t4","@type":"Dataset","description":"Observed and expected 95% CL upper limits on the cross-section of gluon-fusion initialted resonant production of the mass of the...","name":"Table 4"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1683431?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/83967"}],"inLanguage":"en","name":"Search for Higgs boson pair production in the $\\gamma\\gamma WW^{*}$ channel using $pp$ collision data recorded at $\\sqrt{s} = 13$ TeV with the ATLAS detector","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1683431?version=1","version":1}