{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.83012.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1643838"}},{"@id":"https://doi.org/10.1140/epjc/s10052-018-5686-3","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2018","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 36.1 fb^{-1} of data collected during 2015 and 2016 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.83012.v1/t1","@type":"Dataset","description":"Distribution of the four-lepton invariant mass (m4l) in the four-lepton search for the ggF-enriched category.","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.83012.v1/t2","@type":"Dataset","description":"Distribution of the four-lepton invariant mass (m4l) in the four-lepton search for the VBF-enriched category.","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.83012.v1/t3","@type":"Dataset","description":"Transverse mass mT in the llnunu search for the electron channel.","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.83012.v1/t4","@type":"Dataset","description":"Transverse mass mT in the llnunu search for the muon channel.","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.83012.v1/t5","@type":"Dataset","description":"Upper limits at 95% CL on the cross section times branching ratio as a function of the heavy resonance mass...","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.83012.v1/t6","@type":"Dataset","description":"Upper limits at 95% CL on the cross section times branching ratio as a function of the heavy resonance mass...","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.83012.v1/t7","@type":"Dataset","description":"Upper limits at 95% CL on the cross section for the ggF production model times branching ratio as a function...","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.83012.v1/t8","@type":"Dataset","description":"Upper limits at 95% CL on the cross section for the ggF production model times branching ratio as a function...","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.83012.v1/t9","@type":"Dataset","description":"Upper limits at 95% CL on the cross section for the ggF production model times branching ratio as a function...","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.83012.v1/t10","@type":"Dataset","description":"Upper limits at 95% CL on the cross section times branching ratio for a KK graviton produced with k/M_{PI} =...","name":"Table 10"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1643838?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/83012"}],"inLanguage":"en","name":"Search for heavy $ZZ$ resonances in the $\\ell^+\\ell^-\\ell^+\\ell^-$ and $\\ell^+\\ell^-\\nu\\bar\\nu$ final states using 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/ins1643838?version=1","version":1}