{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.97160.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1843269"}},{"@id":"https://doi.org/10.1007/JHEP06(2021)146","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2021","description":"A search for charged Higgs bosons decaying into $W^\\pm W^\\pm$ or $W^\\pm Z$ bosons is performed, involving experimental signatures with two leptons of the same charge, or three or four leptons with a variety of charge combinations, 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$^{-1}$. The search is guided by a type-II seesaw model that extends the scalar sector of the Standard Model with a scalar triplet, leading to a phenomenology that includes doubly and singly charged Higgs bosons. Two scenarios are explored, corresponding to the pair production of doubly charged $H^{\\pm\\pm}$ bosons, or the associated production of a doubly charged $H^{\\pm\\pm}$ boson and a singly charged $H^\\pm$ boson. No significant deviations from the Standard Model predictions are observed. $H^{\\pm\\pm}$ bosons are excluded at 95% confidence level up to 350 GeV and 230 GeV for the pair and associated production modes, respectively.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.97160.v1/t1","@type":"Dataset","description":"Distribution of $E_{T}^{miss}$, which is one of the discriminating variables used to define the $2\\ell^{sc}$ SRs. The events are selected...","name":"Figure 3a"},{"@id":"https://doi.org/10.17182/hepdata.97160.v1/t2","@type":"Dataset","description":"Distribution of $\\Delta R_{\\ell^{\\pm}\\ell^{\\pm}}$, which is one of the discriminating variables used to define the $2\\ell^{sc}$ SRs. The events are...","name":"Figure 3b"},{"@id":"https://doi.org/10.17182/hepdata.97160.v1/t3","@type":"Dataset","description":"Distribution of $M_{jets}$, which is one of the discriminating variables used to define the $2\\ell^{sc}$ SRs. The events are selected...","name":"Figure 3c"},{"@id":"https://doi.org/10.17182/hepdata.97160.v1/t4","@type":"Dataset","description":"Distribution of $S$, which is one of the discriminating variables used to define the $2\\ell^{sc}$ SRs. The events are selected...","name":"Figure 3d"},{"@id":"https://doi.org/10.17182/hepdata.97160.v1/t5","@type":"Dataset","description":"Distribution of $E_{T}^{miss}$, which is one of the discriminating variables used to define the $3\\ell$ SRs. 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The events are selected...","name":"Figure 5a"},{"@id":"https://doi.org/10.17182/hepdata.97160.v1/t10","@type":"Dataset","description":"Distribution of $\\Delta R_{\\ell^{\\pm}\\ell^{\\pm}}^{min}$, which is one of the discriminating variables used to define the $4\\ell$ SRs. The events are...","name":"Figure 5b"},{"@id":"https://doi.org/10.17182/hepdata.97160.v1/t11","@type":"Dataset","description":"Distribution of $m_{x\\ell}$ ($x$=4), which is one of the discriminating variables used to define the $4\\ell$ SRs. The events are...","name":"Figure 5c"},{"@id":"https://doi.org/10.17182/hepdata.97160.v1/t12","@type":"Dataset","description":"Distribution of $p_{T}^{\\ell_{1}}$, which is one of the discriminating variables used to define the $4\\ell$ SRs. The events are selected...","name":"Figure 5d"},{"@id":"https://doi.org/10.17182/hepdata.97160.v1/t13","@type":"Dataset","description":"Contributions from different categories of uncertainties relative to the expected background yields in the defined SRs, as obtained after performing...","name":"Figure 6"},{"@id":"https://doi.org/10.17182/hepdata.97160.v1/t14","@type":"Dataset","description":"Data event yields compared with the expected contributions from relevant background sources, for the combination of the individual channels of...","name":"Figure 7"},{"@id":"https://doi.org/10.17182/hepdata.97160.v1/t15","@type":"Dataset","description":"The $E_{T}^{miss}$ distribution for the SRs of the $m_{H^{\\pm\\pm}} = 300~GeV$ signal mass hypothesis, where the selection requirement on $E_{T}^{miss}$...","name":"Figure 8a"},{"@id":"https://doi.org/10.17182/hepdata.97160.v1/t16","@type":"Dataset","description":"The $E_{T}^{miss}$ distribution for the SRs of the $m_{H^{\\pm\\pm}} = 300~GeV$ signal mass hypothesis, where the selection requirement on $E_{T}^{miss}$...","name":"Figure 8b"},{"@id":"https://doi.org/10.17182/hepdata.97160.v1/t17","@type":"Dataset","description":"The $E_{T}^{miss}$ distribution for the SRs of the $m_{H^{\\pm\\pm}} = 300~GeV$ signal mass hypothesis, where the selection requirement on $E_{T}^{miss}$...","name":"Figure 8c"},{"@id":"https://doi.org/10.17182/hepdata.97160.v1/t18","@type":"Dataset","description":"Observed and expected upper limits of the $H^{\\pm\\pm}$ pair production cross section times branching fraction at 95% CL obtained from...","name":"Figure 9a"},{"@id":"https://doi.org/10.17182/hepdata.97160.v1/t19","@type":"Dataset","description":"The theoretical prediction of Figure 9(a) in the paper.","name":"Figure 9a (Theory)"},{"@id":"https://doi.org/10.17182/hepdata.97160.v1/t20","@type":"Dataset","description":"Observed and expected upper limits of the $H^{\\pm\\pm}$ and $H^{\\pm}$ production cross section times branching fraction at 95% CL obtained...","name":"Figure 9b"},{"@id":"https://doi.org/10.17182/hepdata.97160.v1/t21","@type":"Dataset","description":"The theoretical prediction of Figure 9(b) in the paper.","name":"Figure 9b (Theory)"},{"@id":"https://doi.org/10.17182/hepdata.97160.v1/t22","@type":"Dataset","description":"Data event yields compared with the estimated background in the $m_{H^{\\pm\\pm}} = 200~GeV$ or $m_{H^{\\pm\\pm}} = 220~GeV$ SRs. SFOC 0...","name":"Figure 10"},{"@id":"https://doi.org/10.17182/hepdata.97160.v1/t23","@type":"Dataset","description":"Data event yields compared with the estimated background in the $m_{H^{\\pm\\pm}} = 300~GeV$ or $m_{H^{\\pm\\pm}} = 350~GeV$ SRs. SFOC 0...","name":"Figure 11"},{"@id":"https://doi.org/10.17182/hepdata.97160.v1/t24","@type":"Dataset","description":"Data event yields compared with the estimated background in the $m_{H^{\\pm\\pm}} = 400~GeV$ or $m_{H^{\\pm\\pm}} = 450~GeV$ SRs. SFOC 0...","name":"Figure 12"},{"@id":"https://doi.org/10.17182/hepdata.97160.v1/t25","@type":"Dataset","description":"Data event yields compared with the estimated background in the $m_{H^{\\pm\\pm}} = 500~GeV$ or $m_{H^{\\pm\\pm}} = 550~GeV$ or $m_{H^{\\pm\\pm}} =...","name":"Figure 13"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1843269?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/97160"}],"inLanguage":"en","name":"Search for doubly and singly charged Higgs bosons decaying into vector bosons 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/ins1843269?version=1","version":1}