{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.132485.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/2159368"}},{"@id":"https://doi.org/10.1016/j.physletb.2023.137813","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"CMS Collaboration"},"creator":{"@type":"Organization","name":"CMS Collaboration"},"datePublished":"2022","description":"A search for new heavy resonances decaying to WW, WZ, ZZ, WH, or ZH boson pairs in the all-jets final state is presented. The analysis is based on proton-proton collision data recorded by the CMS detector in 2016-2018 at a centre-of-mass energy of 13 TeV at the CERN LHC, corresponding to an integrated luminosity of 138 fb$^{-1}$. The search is sensitive to resonances with masses between 1.3 and 6 TeV, decaying to bosons that are highly Lorentz-boosted such that each of the bosons forms a single large-radius jet. Machine learning techniques are employed to identify such jets. No significant excess over the estimated standard model background is observed. A maximum local significance of 3.6 standard deviations, corresponding to a global significance of 2.3 standard deviations, is observed at masses of 2.1 and 2.9 TeV. In a heavy vector triplet model, spin-1 Z' and W' resonances with masses below 4.8 TeV are excluded at the 95% confidence level (CL). These limits are the most stringent to date. In a bulk graviton model, spin-2 gravitons and spin-0 radions with masses below 1.4 and 2.7 TeV, respectively, are excluded at 95% CL. Production of heavy resonances through vector boson fusion is constrained with upper cross section limits at 95% CL as low as 0.1 fb.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.132485.v1/t1","@type":"Dataset","description":"Observed and expected 95% CL upper limits on the product of the production cross section ($\\sigma$) and the branching fraction,...","name":"Figure 7a"},{"@id":"https://doi.org/10.17182/hepdata.132485.v1/t2","@type":"Dataset","description":"Observed and expected 95% CL upper limits on the product of the production cross section ($\\sigma$) and the branching fraction,...","name":"Figure 7b"},{"@id":"https://doi.org/10.17182/hepdata.132485.v1/t3","@type":"Dataset","description":"Observed and expected 95% CL upper limits on the product of the production cross section ($\\sigma$) and the branching fraction,...","name":"Figure 7c"},{"@id":"https://doi.org/10.17182/hepdata.132485.v1/t4","@type":"Dataset","description":"Observed and expected 95% CL upper limits on the product of the production cross section ($\\sigma$) and the branching fraction,...","name":"Figure 7d"},{"@id":"https://doi.org/10.17182/hepdata.132485.v1/t5","@type":"Dataset","description":"Total signal efficiency including all event categories as a function of the resonance mass $M_X$ for all DY/ggF signal models...","name":"Additional Figure 1a"},{"@id":"https://doi.org/10.17182/hepdata.132485.v1/t6","@type":"Dataset","description":"Total signal efficiency including all event categories as a function of the resonance mass $M_X$ for all VBF signal models...","name":"Additional Figure 1b"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins2159368?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/132485"}],"inLanguage":"en","name":"Search for new heavy resonances decaying to WW, WZ, ZZ, WH, or ZH boson pairs in the all-jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins2159368?version=1","version":1}