{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.88425.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1725190"}},{"@id":"https://doi.org/10.1016/j.physletb.2019.07.016","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2019","description":"A search for high-mass dielectron and dimuon resonances in the mass range of 250 GeV to 6 TeV is presented. The data were recorded by the ATLAS experiment in proton-proton collisions at a centre-of-mass energy of $\\sqrt{s}$=13 TeV during Run 2 of the Large Hadron Collider and correspond to an integrated luminosity of 139 fb$^{-1}$. Limits are set on the fiducial cross-section times branching ratio to dielectrons and dimuons for generic resonances with a relative natural width in the range of zero to 10%. Limits on the Heavy Vector Triplet model couplings and on the masses of vector resonances are inferred.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.88425.v1/t1","@type":"Dataset","description":"Distribution of the dielectron invariant mass for events passing the full selection.","name":"Dielectron invariant mass spectrum"},{"@id":"https://doi.org/10.17182/hepdata.88425.v1/t2","@type":"Dataset","description":"Distribution of the dimuon invariant mass for events passing the full selection.","name":"Dimuon invariant mass spectrum"},{"@id":"https://doi.org/10.17182/hepdata.88425.v1/t3","@type":"Dataset","description":"Expected upper limits at 95% CL on the fiducial cross-section times branching ratio as a function of pole mass for...","name":"Expected dilepton cross-section limits"},{"@id":"https://doi.org/10.17182/hepdata.88425.v1/t4","@type":"Dataset","description":"Observed upper limits at 95% CL on the fiducial cross-section times branching ratio as a function of pole mass for...","name":"Observed dilepton cross-section limits"},{"@id":"https://doi.org/10.17182/hepdata.88425.v1/t5","@type":"Dataset","description":"Expected upper limits at 95% CL on the fiducial cross-section times branching ratio as a function of pole mass for...","name":"Expected dielectron cross-section limits"},{"@id":"https://doi.org/10.17182/hepdata.88425.v1/t6","@type":"Dataset","description":"Observed upper limits at 95% CL on the fiducial cross-section times branching ratio as a function of pole mass for...","name":"Observed dielectron cross-section limits"},{"@id":"https://doi.org/10.17182/hepdata.88425.v1/t7","@type":"Dataset","description":"Expected upper limits at 95% CL on the fiducial cross-section times branching ratio as a function of pole mass for...","name":"Expected dimuon cross-section limits"},{"@id":"https://doi.org/10.17182/hepdata.88425.v1/t8","@type":"Dataset","description":"Observed upper limits at 95% CL on the fiducial cross-section times branching ratio as a function of pole mass for...","name":"Observed dimuon cross-section limits"},{"@id":"https://doi.org/10.17182/hepdata.88425.v1/t9","@type":"Dataset","description":"Ratio of the observed limit to the Z'$_\\mathrm{SSM}$ cross-section for the combination of the dielectron and dimuon channels. A number...","name":"Ratio of observed limits to SSM cross section"},{"@id":"https://doi.org/10.17182/hepdata.88425.v1/t10","@type":"Dataset","description":"Observed 95% exclusion contours in the HVT parameter space $\\{g_h,g_f\\}$ with $g_f\\equiv g_l=g_q$ for a resonance mass of 3 TeV...","name":"Observed exclusion contours on HVT $\\{g_h,g_f\\}$ at 3 TeV"},{"@id":"https://doi.org/10.17182/hepdata.88425.v1/t11","@type":"Dataset","description":"Observed 95% exclusion contours in the HVT parameter space $\\{g_h,g_f\\}$ with $g_f\\equiv g_l=g_q$ for a resonance mass of 4 TeV...","name":"Observed exclusion contours on HVT $\\{g_h,g_f\\}$ at 4 TeV"},{"@id":"https://doi.org/10.17182/hepdata.88425.v1/t12","@type":"Dataset","description":"Observed 95% exclusion contours in the HVT parameter space $\\{g_h,g_f\\}$ with $g_f\\equiv g_l=g_q$ for a resonance mass of 5 TeV...","name":"Observed exclusion contours on HVT $\\{g_h,g_f\\}$ at 5 TeV"},{"@id":"https://doi.org/10.17182/hepdata.88425.v1/t13","@type":"Dataset","description":"Observed 95% exclusion contours in the HVT parameter space $\\{g_q,g_l\\}$ with $g_h$ set to zero for a resonance mass of...","name":"Observed exclusion contours on HVT $\\{g_q,g_l\\}$ at 3 TeV"},{"@id":"https://doi.org/10.17182/hepdata.88425.v1/t14","@type":"Dataset","description":"Observed 95% exclusion contours in the HVT parameter space $\\{g_q,g_l\\}$ with $g_h$ set to zero for a resonance mass of...","name":"Observed exclusion contours on HVT $\\{g_q,g_l\\}$ at 4 TeV"},{"@id":"https://doi.org/10.17182/hepdata.88425.v1/t15","@type":"Dataset","description":"Observed 95% exclusion contours in the HVT parameter space $\\{g_q,g_l\\}$ with $g_h$ set to zero for a resonance mass of...","name":"Observed exclusion contours on HVT $\\{g_q,g_l\\}$ at 5 TeV"},{"@id":"https://doi.org/10.17182/hepdata.88425.v1/t16","@type":"Dataset","description":"Expected 95% exclusion contours in the HVT parameter space $\\{g_h,g_f\\}$ with $g_f\\equiv g_l=g_q$ for a resonance mass of 3 TeV...","name":"Expected exclusion contours on HVT $\\{g_h,g_f\\}$ at 3 TeV"},{"@id":"https://doi.org/10.17182/hepdata.88425.v1/t17","@type":"Dataset","description":"Expected 95% exclusion contours in the HVT parameter space $\\{g_h,g_f\\}$ with $g_f\\equiv g_l=g_q$ for a resonance mass of 4 TeV...","name":"Expected exclusion contours on HVT $\\{g_h,g_f\\}$ at 4 TeV"},{"@id":"https://doi.org/10.17182/hepdata.88425.v1/t18","@type":"Dataset","description":"Expected 95% exclusion contours in the HVT parameter space $\\{g_h,g_f\\}$ with $g_f\\equiv g_l=g_q$ for a resonance mass of 5 TeV...","name":"Expected exclusion contours on HVT $\\{g_h,g_f\\}$ at 5 TeV"},{"@id":"https://doi.org/10.17182/hepdata.88425.v1/t19","@type":"Dataset","description":"Expected 95% exclusion contours in the HVT parameter space $\\{g_q,g_l\\}$ with $g_h$ set to zero for a resonance masses of...","name":"Expected exclusion contours on HVT $\\{g_q,g_l\\}$ at 3 TeV"},{"@id":"https://doi.org/10.17182/hepdata.88425.v1/t20","@type":"Dataset","description":"Expected 95% exclusion contours in the HVT parameter space $\\{g_q,g_l\\}$ with $g_h$ set to zero for a resonance masses of...","name":"Expected exclusion contours on HVT $\\{g_q,g_l\\}$ at 4 TeV"},{"@id":"https://doi.org/10.17182/hepdata.88425.v1/t21","@type":"Dataset","description":"Expected 95% exclusion contours in the HVT parameter space $\\{g_q,g_l\\}$ with $g_h$ set to zero for a resonance masses of...","name":"Expected exclusion contours on HVT $\\{g_q,g_l\\}$ at 5 TeV"},{"@id":"https://doi.org/10.17182/hepdata.88425.v1/t22","@type":"Dataset","description":"Dielectron and dimuon selection efficiency as a function of pole mass for spin-0, spin-1 and spin-2 resonances. 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