{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.79077.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1609250"}},{"@id":"https://doi.org/10.1007/JHEP10(2017)182","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2017","description":"A search is conducted for new resonant and non-resonant high-mass phenomena in dielectron and dimuon final states. The search uses 36.1 fb$^{-1}$ of proton-proton collision data, collected at $\\sqrt{s}$ = 13 TeV by the ATLAS experiment at the LHC in 2015 and 2016. No significant deviation from the Standard Model prediction is observed. Upper limits at 95% credibility level are set on the cross-section times branching ratio for resonances decaying into dileptons, which are converted to lower limits on the resonance mass, up to 4.1 for the E$_{6}$-motivated Z'$_{\\chi}$. Lower limits on the $qq \\ell\\ell$ contact interaction scale are set between 24 TeV and 40 TeV, depending on the model.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.79077.v1/t1","@type":"Dataset","description":"Product of acceptance and efficiency for the dielectron (upper curve) and dimuon (lower curve) selections as a function of the...","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.79077.v1/t2","@type":"Dataset","description":"Distribution of dielectron reconstructed invariant mass after selection, for data and the SM background estimates.","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.79077.v1/t3","@type":"Dataset","description":"Distribution of dimuon reconstructed invariant mass after selection, for data and the SM background estimates.","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.79077.v1/t4","@type":"Dataset","description":"Upper 95% CL limits on the Z' production cross-section times branching ratio to two electrons as a function of Z'...","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.79077.v1/t5","@type":"Dataset","description":"Upper 95% CL limits on the Z' production cross-section times branching ratio to two muons as a function of Z'...","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.79077.v1/t6","@type":"Dataset","description":"Upper 95% CL limits on the Z' production cross-section times branching ratio to two leptons as a function of Z'...","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.79077.v1/t7","@type":"Dataset","description":"Upper 95% CL limits on the acceptance times Z' production cross-section times branching ratio to two leptons in the dielectron...","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.79077.v1/t8","@type":"Dataset","description":"Upper 95% CL limits on the acceptance times Z' production cross-section times branching ratio to two leptons in the dielectron...","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.79077.v1/t9","@type":"Dataset","description":"Upper 95% CL limits on the acceptance times Z' production cross-section times branching ratio to two leptons in the dimuon...","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.79077.v1/t10","@type":"Dataset","description":"Upper 95% CL limits on the acceptance times Z' production cross-section times branching ratio to two leptons in the dimuon...","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.79077.v1/t11","@type":"Dataset","description":"Upper 95% CL limits on the acceptance times Z' production cross-section times branching ratio to two leptons in the combined...","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.79077.v1/t12","@type":"Dataset","description":"Upper 95% CL limits on the acceptance times Z' production cross-section times branching ratio to two leptons in the dilepton...","name":"Table 12"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1609250?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/79077"}],"inLanguage":"en","name":"Search for new high-mass phenomena in the dilepton final state using 36.1 fb$^{-1}$ of proton-proton collision data 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/ins1609250?version=1","version":1}
