{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.97159.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1820316"}},{"@id":"https://doi.org/10.1140/epjc/s10052-021-09013-y","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2021","description":"CERN-LHC. Search for heavy ZZ resonances in the 4l and 2l2nu final states using proton-proton collisions at a center-of-mass energy of 13 TeV with 139 fb^{-1} of data collected from 2015 to 2018 with the ATLAS detector. Different mass ranges for the hypothetical resonances are considered, depending on the final state and model. The different ranges span between 200 GeV and 2000 GeV. The results are interpreted as upper limits on the production cross section of a spin-0 or spin-2 resonance.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.97159.v1/t1","@type":"Dataset","description":"Distribution of the four-lepton invariant mass in the four-lepton final state for the ggF-MVA-high 4-muon category.","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.97159.v1/t2","@type":"Dataset","description":"Distribution of the four-lepton invariant mass in the four-lepton final state for the ggF-MVA-high 2e2mu category.","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.97159.v1/t3","@type":"Dataset","description":"Distribution of the four-lepton invariant mass in the four-lepton final state for the ggF-MVA-high 4-electron category.","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.97159.v1/t4","@type":"Dataset","description":"Distribution of the four-lepton invariant mass in the four-lepton final state for the ggF-MVA-low category.","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.97159.v1/t5","@type":"Dataset","description":"Distribution of the four-lepton invariant mass in the four-lepton final state for the VBF-MVA-enriched category.","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.97159.v1/t6","@type":"Dataset","description":"Distribution of the transverse mass in the llvv final state for the ggF-enriched eevv category.","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.97159.v1/t7","@type":"Dataset","description":"Distribution of the transverse mass in the llvv final state for the ggF-enriched mumuvv category.","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.97159.v1/t8","@type":"Dataset","description":"Distribution of the transverse mass in the llvv final state for the VBF-enriched eevv category.","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.97159.v1/t9","@type":"Dataset","description":"Distribution of the transverse mass in the llvv final state for the VBF-enriched mumuvv category.","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.97159.v1/t10","@type":"Dataset","description":"The upper limits at 95% CL on the cross section times branching ratio as a function of the heavy resonance...","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.97159.v1/t11","@type":"Dataset","description":"The upper limits at 95% CL on the cross section times branching ratio as a function of the heavy resonance...","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.97159.v1/t12","@type":"Dataset","description":"The upper limits at 95% CL on the cross section for the ggF production mode times branching ratio as a...","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.97159.v1/t13","@type":"Dataset","description":"The upper limits at 95% CL on the cross section for the ggF production mode times branching ratio as a...","name":"Table 13"},{"@id":"https://doi.org/10.17182/hepdata.97159.v1/t14","@type":"Dataset","description":"The upper limits at 95% CL on the cross section for the ggF production mode times branching ratio as a...","name":"Table 14"},{"@id":"https://doi.org/10.17182/hepdata.97159.v1/t15","@type":"Dataset","description":"The upper limits at 95% CL on the cross section for the ggF production mode times branching ratio as a...","name":"Table 15"},{"@id":"https://doi.org/10.17182/hepdata.97159.v1/t16","@type":"Dataset","description":"The upper limits at 95% CL on the cross section times branching ratio for a KK graviton produced with k/M_{PI}...","name":"Table 16"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1820316?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/97159"}],"inLanguage":"en","name":"Search for heavy resonances decaying into a pair of $Z$ bosons in the $\\ell^+\\ell^-\\ell'^+\\ell'^-$ and $\\ell^+\\ell^-\\nu\\bar\\nu$ final states using 139 fb$^{-1}$ of proton-proton 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/ins1820316?version=1","version":1}