{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.129285.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/2176695"}},{"@id":"https://doi.org/10.1007/JHEP07(2023)200","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2022","description":"A search for heavy Higgs bosons decaying into a pair of vector bosons and produced in association with a vector boson is performed, using final states with two leptons of the same electric charge (electrons or muons), missing transverse momentum and jets. A data sample of proton-proton collisions at a centre-of-mass energy of 13 TeV recorded with the ATLAS detector at the Large Hadron Collider between 2015 and 2018 is used. The data correspond to a total integrated luminosity of 139 fb\u22121. The observed data are in agreement with Standard Model background expectations. The results are interpreted using higher dimensional operators in an Effective Field Theory. The upper production cross-section limits at 95\\% confidence level are calculated as a function of the heavy Higgs boson mass and coupling strengths to vector bosons. Limits are set in the Higgs boson mass region 300 to 1500 GeV, and depend upon the assumed couplings. The highest heavy Higgs boson mass excluded with the coupling combinations explored is 900 GeV. Limits on coupling strength are also provided.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.129285.v1/t1","@type":"Dataset","description":"Comparison between data and SM predictions for the meff distributions in the boosted SR. The background predictions are obtained through...","name":"Figure 3a"},{"@id":"https://doi.org/10.17182/hepdata.129285.v1/t2","@type":"Dataset","description":"Comparison between data and SM predictions for the meff distributions in the resolved SR. The background predictions are obtained through...","name":"Figure 3b"},{"@id":"https://doi.org/10.17182/hepdata.129285.v1/t3","@type":"Dataset","description":"Expected 95% CL upper limits on the production of a heavy Higgs boson as functions of fw and fww with...","name":"Figure 6a_exp"},{"@id":"https://doi.org/10.17182/hepdata.129285.v1/t4","@type":"Dataset","description":"Expected 95% CL upper limits with 1-sigma uncertainty on the production of a heavy Higgs boson as functions of fw...","name":"Figure 6a_exp_1s"},{"@id":"https://doi.org/10.17182/hepdata.129285.v1/t5","@type":"Dataset","description":"Expected 95% CL upper limits with 2-sigma uncertainty on the production of a heavy Higgs boson as functions of fw...","name":"Figure 6a_exp_2s"},{"@id":"https://doi.org/10.17182/hepdata.129285.v1/t6","@type":"Dataset","description":"Observed 95% CL upper limits on the production of a heavy Higgs boson as functions of fw and fww with...","name":"Figure 6a_obs"},{"@id":"https://doi.org/10.17182/hepdata.129285.v1/t7","@type":"Dataset","description":"Expected 95% CL upper limits on the production of a heavy Higgs boson as functions of fw and fww with...","name":"Figure 6b_exp"},{"@id":"https://doi.org/10.17182/hepdata.129285.v1/t8","@type":"Dataset","description":"Expected 95% CL upper limits with 1-sigma uncertainty on the production of a heavy Higgs boson as functions of fw...","name":"Figure 6b_exp_1s"},{"@id":"https://doi.org/10.17182/hepdata.129285.v1/t9","@type":"Dataset","description":"Expected 95% CL upper limits with 2-sigma uncertainty on the production of a heavy Higgs boson as functions of fw...","name":"Figure 6b_exp_2s"},{"@id":"https://doi.org/10.17182/hepdata.129285.v1/t10","@type":"Dataset","description":"Observed 95% CL upper limits on the production of a heavy Higgs boson as functions of fw and fww with...","name":"Figure 6b_obs"},{"@id":"https://doi.org/10.17182/hepdata.129285.v1/t11","@type":"Dataset","description":"Expected 95% CL upper limits on the production of a heavy Higgs boson as functions of fw and fww with...","name":"Figure 6c_exp"},{"@id":"https://doi.org/10.17182/hepdata.129285.v1/t12","@type":"Dataset","description":"Expected 95% CL upper limits with 1-sigma uncertainty on the production of a heavy Higgs boson as functions of fw...","name":"Figure 6c_exp_1s"},{"@id":"https://doi.org/10.17182/hepdata.129285.v1/t13","@type":"Dataset","description":"Expected 95% CL upper limits with 2-sigma uncertainty on the production of a heavy Higgs boson as functions of fw...","name":"Figure 6c_exp_2s"},{"@id":"https://doi.org/10.17182/hepdata.129285.v1/t14","@type":"Dataset","description":"Observed 95% CL upper limits on the production of a heavy Higgs boson as functions of fw and fww with...","name":"Figure 6c_obs"},{"@id":"https://doi.org/10.17182/hepdata.129285.v1/t15","@type":"Dataset","description":"Observed (black solid curve) and expected (black dashed curve) 95% CL upper limits on the production of a heavy Higgs...","name":"Figure 7a"},{"@id":"https://doi.org/10.17182/hepdata.129285.v1/t16","@type":"Dataset","description":"Observed (black solid curve) and expected (black dashed curve) 95% CL upper limits on the production of a heavy Higgs...","name":"Figure 7b"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins2176695?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/129285"}],"inLanguage":"en","name":"A search for heavy Higgs bosons decaying into vector bosons in same-sign two-lepton final states in $pp$ collisions 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/ins2176695?version=1","version":1}
