{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.82124.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1635891"}},{"@id":"https://doi.org/10.1007/JHEP03(2018)003","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"CMS Collaboration"},"creator":{"@type":"Organization","name":"CMS Collaboration"},"datePublished":"2018","description":"A search for heavy resonances decaying to a pair of Z bosons is performed using data collected with the CMS detector at the LHC. Events are selected by requiring two oppositely charged leptons (electrons or muons), consistent with the decay of a Z boson, and large missing transverse momentum, which is interpreted as arising from the decay of a second Z boson to two neutrinos. The analysis uses data from proton-proton collisions at a center-of-mass energy of 13 TeV, corresponding to an integrated luminosity of 35.9 fb$^{\u22121}$. The hypothesis of a spin-2 bulk graviton (X) decaying to a pair of Z bosons is examined and upper limits at 95% confidence level are set on the product of the production cross section and branching fraction of X $\\rightarrow$ ZZ ranging from 100 to 4 fb. For bulk graviton models characterized by a curvature scale parameter $\\tilde{k}=0.5$ in the extra dimension, the region $m_X < 800 GeV$ is excluded, providing the most stringent limit reported to date. Variations of the model considering the possibility of a wide resonance produced exclusively via gluon-gluon fusion or qq annihilation are also examined.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.82124.v1/t1","@type":"Dataset","description":"The $p_T^Z$ distributions for electron channel comparing the data and background model with systematic uncertainty.","name":"Z $p_T$ distributions in the electron channel"},{"@id":"https://doi.org/10.17182/hepdata.82124.v1/t2","@type":"Dataset","description":"The $p_T^Z$ distributions for muon channel comparing the data and background model with systematic uncertainty.","name":"Z $p_T$ distributions in the muon channel"},{"@id":"https://doi.org/10.17182/hepdata.82124.v1/t3","@type":"Dataset","description":"The $p_T ^{miss}$ distributions for electron channel comparing the data and background model with systematic uncertainty.","name":"$p_T ^{miss}$ distributions in the electron channel"},{"@id":"https://doi.org/10.17182/hepdata.82124.v1/t4","@type":"Dataset","description":"The $p_T ^{miss}$ distributions for muon channel comparing the data and background model with systematic uncertainty.","name":"$p_T ^{miss}$ distributions in the muon channel"},{"@id":"https://doi.org/10.17182/hepdata.82124.v1/t5","@type":"Dataset","description":"The $m_T$ distributions for electron channel comparing the data and background model with systematic uncertainty, after fitting the background-only model...","name":"post-fit $m_T$ distributions in the electron channel"},{"@id":"https://doi.org/10.17182/hepdata.82124.v1/t6","@type":"Dataset","description":"The $m_T$ distributions for muon channel comparing the data and background model with systematic uncertainty, after fitting the background-only model...","name":"post-fit $m_T$ distributions in the muon channel"},{"@id":"https://doi.org/10.17182/hepdata.82124.v1/t7","@type":"Dataset","description":"Expected and observed limits on the product of cross section and branching fraction of a new spin-2 heavy resonance X$\\rightarrow$ZZ,...","name":"Expected and observed limits."},{"@id":"https://doi.org/10.17182/hepdata.82124.v1/t8","@type":"Dataset","description":"Expected and observed limits on the product of cross section and branching fraction of a new spin-2 heavy resonance X$\\rightarrow$ZZ,...","name":"Expected and observed limits for electron channel."},{"@id":"https://doi.org/10.17182/hepdata.82124.v1/t9","@type":"Dataset","description":"Expected and observed limits on the product of cross section and branching fraction of a new spin-2 heavy resonance X$\\rightarrow$ZZ,...","name":"Expected and observed limits for muon channel."},{"@id":"https://doi.org/10.17182/hepdata.82124.v1/t10","@type":"Dataset","description":"Expected and observed limits on the product of cross section and branching fraction of a new spin-2 heavy resonance X$\\rightarrow$ZZ...","name":"Expected and observed limits for gg fusion production"},{"@id":"https://doi.org/10.17182/hepdata.82124.v1/t11","@type":"Dataset","description":"Expected and observed limits on the product of cross section and branching fraction of a new spin-2 heavy resonance X$\\rightarrow$ZZ...","name":"Expected and observed limits for qq annihilation production"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1635891?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/82124"}],"inLanguage":"en","name":"Search for diboson resonances in the 2$\\ell$2$\\nu$ final state","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1635891?version=1","version":1}