{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.114367.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1976980"}},{"@id":"https://doi.org/10.1007/JHEP04(2022)087","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"CMS Collaboration"},"creator":{"@type":"Organization","name":"CMS Collaboration"},"datePublished":"2021","description":"A search has been performed for heavy resonances decaying to ZZ or ZW and axion-like particles mediating nonresonant ZZ or ZH production in semileptonic final states, with two charged leptons (electrons or muons) produced by the decay of a Z boson, and two quarks produced by the decay of a Z, W, or Higgs boson H. The analysis is sensitive to resonances with masses in the range from 450 to 1800 GeV. Two categories are defined based on the merged or resolved reconstruction of the hadronically decaying boson. The search is based on data collected during 2016 to 2018 by the CMS experiment at the LHC in proton-proton collisions at a center-of-mass energy of 13 TeV, corresponding to an integrated luminosity of 137 $\\text{fb}^{-1}$. No significant excess is observed in the data above the standard model background expectation. Upper limits on the production cross section of heavy, narrow spin-1 and spin-2 resonances are derived as functions of the resonance mass, and exclusion limits on the production of W' bosons and bulk graviton particles are calculated in the framework of the heavy vector triplet and warped extra dimensions model, respectively. In addition, upper limits on the ALP-mediated diboson production cross section and ALP couplings to standard model particles are obtained in the framework of linear and chiral effective field theories.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.114367.v1/t1","@type":"Dataset","description":"SR1 diboson invariant mass distribution in the boosted untagged category after fitting the signal and sideband regions using a signal...","name":"SR1 diboson mass boosted untagged category"},{"@id":"https://doi.org/10.17182/hepdata.114367.v1/t2","@type":"Dataset","description":"SR1 diboson invariant mass distribution in the boosted tagged category after fitting the signal and sideband regions using a signal...","name":"SR1 diboson mass boosted tagged category"},{"@id":"https://doi.org/10.17182/hepdata.114367.v1/t3","@type":"Dataset","description":"SR1 diboson invariant mass distribution in the resolved untagged category after fitting the signal and sideband regions using a signal...","name":"SR1 diboson mass resolved untagged category"},{"@id":"https://doi.org/10.17182/hepdata.114367.v1/t4","@type":"Dataset","description":"SR1 diboson invariant mass distribution in the resolved tagged category after fitting the signal and sideband regions using a signal...","name":"SR1 diboson mass resolved tagged category"},{"@id":"https://doi.org/10.17182/hepdata.114367.v1/t5","@type":"Dataset","description":"SR2 diboson invariant mass distribution in the boosted untagged category after fitting the signal and sideband regions using a signal...","name":"SR2 diboson mass boosted untagged category"},{"@id":"https://doi.org/10.17182/hepdata.114367.v1/t6","@type":"Dataset","description":"SR2 diboson invariant mass distribution in the boosted tagged category after fitting the signal and sideband regions using a signal...","name":"SR2 diboson mass boosted tagged category"},{"@id":"https://doi.org/10.17182/hepdata.114367.v1/t7","@type":"Dataset","description":"SR2 diboson invariant mass distribution in the resolved untagged category after fitting the signal and sideband regions using a signal...","name":"SR2 diboson mass resolved untagged category"},{"@id":"https://doi.org/10.17182/hepdata.114367.v1/t8","@type":"Dataset","description":"SR2 diboson invariant mass distribution in the resolved tagged category after fitting the signal and sideband regions using a signal...","name":"SR2 diboson mass resolved tagged category"},{"@id":"https://doi.org/10.17182/hepdata.114367.v1/t9","@type":"Dataset","description":"Observed and expected 95% CL upper limit on $\\sigma \\mathcal{B}$(G -> ZZ) as a function of the resonance mass, taking...","name":"Observed 95% CL upper limits for bulk graviton signal"},{"@id":"https://doi.org/10.17182/hepdata.114367.v1/t10","@type":"Dataset","description":"Observed and expected 95% CL upper limit on $\\sigma \\mathcal{B}$(W' -> ZW) as a function of the resonance mass, taking...","name":"Observed 95% CL upper limits for Wprime signal"},{"@id":"https://doi.org/10.17182/hepdata.114367.v1/t11","@type":"Dataset","description":"Observed and expected 95% CL upper limit on the product of the ALP coupling to gluons and the coupling to...","name":"Observed 95% CL upper limits on ALP linear couplings"},{"@id":"https://doi.org/10.17182/hepdata.114367.v1/t12","@type":"Dataset","description":"Observed and expected 95% CL upper limit on the product of the ALP coupling to gluons and the chiral $a_\\widetilde{2D}$...","name":"Observed 95% CL upper limits on ALP chiral couplings"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1976980?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/114367"}],"inLanguage":"en","name":"Search for heavy resonances decaying to ZZ or ZW and axion-like particles mediating nonresonant ZZ or ZH production at $\\sqrt{s}$ = 13 TeV","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1976980?version=1","version":1}