{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.80462.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1632760"}},{"@id":"https://doi.org/10.1140/epjc/s10052-018-5661-z","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2017","description":"A search for doubly-charged Higgs bosons with pairs of prompt, isolated, highly energetic leptons with the same electric charge is presented. The search uses proton-proton collision data at the center-of-mass energy of 13 TeV data sample corresponding to 36.1 $\\mathrm{fb}^{-1}$ of integrated luminosity recorded in 2015 and 2016 by the ATLAS detector at the LHC. This analysis focuses on the decays $H^{\\pm\\pm}\\to e^{\\pm}e^{\\pm}$, $H^{\\pm\\pm}\\to e^{\\pm}\\mu^{\\pm}$ and $H^{\\pm\\pm}\\to \\mu^{\\pm}\\mu^{\\pm}$, fitting the dilepton mass spectra in several exclusive signal regions. No significant evidence of a signal was observed and corresponding limits on the production cross-section and consequently the lower limit on $m(H^{\\pm \\pm})$ were derived at $95\\%$ confidence level. With $\\ell={e,\\mu}$, the observed lower limit on the mass of a doubly-charged Higgs only coupling to left-handed leptons varies from 770 GeV to 870 GeV (850 GeV expected) for $Br(H^{\\pm\\pm}\\to \\ell^{\\pm}\\ell^{\\pm})=100\\%$ and both the expected and observed mass limits are still above 450 GeV for $Br(H^{\\pm\\pm}\\to \\ell^{\\pm}\\ell^{\\pm})=10\\%$ for any combination of partial branching ratios.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.80462.v1/t1","@type":"Dataset","description":"Observed and expected upper limit on the cross-section for $pp \\to H^{++}H^{--}$ for a combination of partial branching ratios of...","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.80462.v1/t2","@type":"Dataset","description":"Observed and expected upper limit on the cross-section for $pp \\to H^{++}H^{--}$ for a combination of partial branching ratios of...","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.80462.v1/t3","@type":"Dataset","description":"Observed and expected upper limit on the cross-section for $pp \\to H^{++}H^{--}$ for a combination of partial branching ratios of...","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.80462.v1/t4","@type":"Dataset","description":"Observed and expected upper limit on the cross-section for $pp \\to H^{++}H^{--}$ for a combination of partial branching ratios of...","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.80462.v1/t5","@type":"Dataset","description":"Observed and expected lower limit on the $H_{L}^{\\pm\\pm}$ boson mass as a function of the branching ratio $B(H_{L}^{\\pm\\pm} \\to e^{\\pm}e^{\\pm})$...","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.80462.v1/t6","@type":"Dataset","description":"Observed and expected lower limit on the $H_{L}^{\\pm\\pm}$ boson mass as a function of the branching ratio $B(H_{L}^{\\pm\\pm} \\to \\mu^{\\pm}\\mu^{\\pm})$...","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.80462.v1/t7","@type":"Dataset","description":"Observed and expected lower limit on the $H_{L}^{\\pm\\pm}$ boson mass as a function of the branching ratio $B(H_{L}^{\\pm\\pm} \\to e^{\\pm}\\mu^{\\pm})$...","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.80462.v1/t8","@type":"Dataset","description":"Minimum observed and expected lower limit (among all partial branching ratio combinations) on the $H_{L}^{\\pm\\pm}$ boson mass as a function...","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.80462.v1/t9","@type":"Dataset","description":"Observed and expected lower limit on the $H_{R}^{\\pm\\pm}$ boson mass as a function of the branching ratio $B(H_{R}^{\\pm\\pm} \\to e^{\\pm}e^{\\pm})$...","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.80462.v1/t10","@type":"Dataset","description":"Observed and expected lower limit on the $H_{R}^{\\pm\\pm}$ boson mass as a function of the branching ratio $B(H_{R}^{\\pm\\pm} \\to \\mu^{\\pm}\\mu^{\\pm})$...","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.80462.v1/t11","@type":"Dataset","description":"Observed and expected lower limit on the $H_{R}^{\\pm\\pm}$ boson mass as a function of the branching ratio $B(H_{R}^{\\pm\\pm} \\to e^{\\pm}\\mu^{\\pm})$...","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.80462.v1/t12","@type":"Dataset","description":"Minimum observed and expected lower limit (among all partial branching ratio combinations) on the $H_{R}^{\\pm\\pm}$ boson mass as a function...","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.80462.v1/t13","@type":"Dataset","description":"Observed and expected lower limit on the $H_{L}^{\\pm\\pm}$ boson mass for all branching ratio combinations ($B(ee)$,$B(e\\mu)$,$B(\\mu\\mu)$) that sum to 100%.","name":"Table 13"},{"@id":"https://doi.org/10.17182/hepdata.80462.v1/t14","@type":"Dataset","description":"Observed and expected lower limit on the $H_{R}^{\\pm\\pm}$ boson mass for all branching ratio combinations ($B(ee)$,$B(e\\mu)$,$B(\\mu\\mu)$) that sum to 100%.","name":"Table 14"},{"@id":"https://doi.org/10.17182/hepdata.80462.v1/t15","@type":"Dataset","description":"Observed and expected lower limit on the $H_{L}^{\\pm\\pm}$ boson mass for all branching ratio combinations ($B(ee)$,$B(e\\mu)$,$B(\\mu\\mu)$) that sum to 90%.","name":"Table 15"},{"@id":"https://doi.org/10.17182/hepdata.80462.v1/t16","@type":"Dataset","description":"Observed and expected lower limit on the $H_{R}^{\\pm\\pm}$ boson mass for all branching ratio combinations ($B(ee)$,$B(e\\mu)$,$B(\\mu\\mu)$) that sum to 90%.","name":"Table 16"},{"@id":"https://doi.org/10.17182/hepdata.80462.v1/t17","@type":"Dataset","description":"Observed and expected lower limit on the $H_{L}^{\\pm\\pm}$ boson mass for all branching ratio combinations ($B(ee)$,$B(e\\mu)$,$B(\\mu\\mu)$) that sum to 80%.","name":"Table 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combinations ($B(ee)$,$B(e\\mu)$,$B(\\mu\\mu)$) that sum to 60%.","name":"Table 21"},{"@id":"https://doi.org/10.17182/hepdata.80462.v1/t22","@type":"Dataset","description":"Observed and expected lower limit on the $H_{R}^{\\pm\\pm}$ boson mass for all branching ratio combinations ($B(ee)$,$B(e\\mu)$,$B(\\mu\\mu)$) that sum to 60%.","name":"Table 22"},{"@id":"https://doi.org/10.17182/hepdata.80462.v1/t23","@type":"Dataset","description":"Observed and expected lower limit on the $H_{L}^{\\pm\\pm}$ boson mass for all branching ratio combinations ($B(ee)$,$B(e\\mu)$,$B(\\mu\\mu)$) that sum to 50%.","name":"Table 23"},{"@id":"https://doi.org/10.17182/hepdata.80462.v1/t24","@type":"Dataset","description":"Observed and expected lower limit on the $H_{R}^{\\pm\\pm}$ boson mass for all branching ratio combinations ($B(ee)$,$B(e\\mu)$,$B(\\mu\\mu)$) that sum to 50%.","name":"Table 24"},{"@id":"https://doi.org/10.17182/hepdata.80462.v1/t25","@type":"Dataset","description":"Observed and expected lower limit on the $H_{L}^{\\pm\\pm}$ boson mass for all branching ratio combinations ($B(ee)$,$B(e\\mu)$,$B(\\mu\\mu)$) that sum to 40%.","name":"Table 25"},{"@id":"https://doi.org/10.17182/hepdata.80462.v1/t26","@type":"Dataset","description":"Observed and expected lower limit on the $H_{R}^{\\pm\\pm}$ boson mass for all branching ratio combinations ($B(ee)$,$B(e\\mu)$,$B(\\mu\\mu)$) that sum to 40%.","name":"Table 26"},{"@id":"https://doi.org/10.17182/hepdata.80462.v1/t27","@type":"Dataset","description":"Observed and expected lower limit on the $H_{L}^{\\pm\\pm}$ boson mass for all branching ratio combinations ($B(ee)$,$B(e\\mu)$,$B(\\mu\\mu)$) that sum to 30%.","name":"Table 27"},{"@id":"https://doi.org/10.17182/hepdata.80462.v1/t28","@type":"Dataset","description":"Observed and expected lower limit on the $H_{R}^{\\pm\\pm}$ boson mass for all branching ratio combinations ($B(ee)$,$B(e\\mu)$,$B(\\mu\\mu)$) that sum to 30%.","name":"Table 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combinations ($B(ee)$,$B(e\\mu)$,$B(\\mu\\mu)$) that sum to 10%.","name":"Table 32"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1632760?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/80462"}],"inLanguage":"en","name":"Search for doubly charged Higgs boson production in multi-lepton final states with the ATLAS detector using proton-proton collisions at $\\sqrt{s}$ = 13 TeV","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1632760?version=1","version":1}