{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.145997.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/2760468"}},{"@id":"https://doi.org/10.1103/PhysRevD.110.052004","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"CMS Collaboration"},"creator":{"@type":"Organization","name":"CMS Collaboration"},"datePublished":"2024","description":"A search is described for the production of a pair of bottom-type vector-like quarks (B VLQs) with mass greater than 1000 GeV. Each B VLQ decays into a b quark and a Higgs boson, a b quark and a Z boson, or a t quark and a W boson. This analysis considers both fully hadronic final states and those containing a charged lepton pair from a Z boson decay. The products of the H $\\to$ bb boson decay and of the hadronic Z or W boson decays can be resolved as two distinct jets or merged into a single jet, so the final states are classified by the number of reconstructed jets. The analysis uses data corresponding to an integrated luminosity of 138 fb$^{-1}$ collected in proton-proton collisions at $\\sqrt{s}$ = 13 TeV with the CMS detector at the LHC from 2016 to 2018. No excess over the expected background is observed. Lower limits are set on the B VLQ mass at 95% confidence level. These depend on the B VLQ branching fractions and are 1570 and 1540 GeV for 100% B $\\to$ bH and 100% B $\\to$ bZ, respectively. In most cases, the mass limits obtained exceed previous limits by at least 100 GeV.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.145997.v1/t1","@type":"Dataset","description":"Distributions of reconstructed VLQ mass for expected postfit background (blue histogram), signal plus background (colored lines), and observed data (black...","name":"Figure 14 Hadronic 4-Jet bHbH"},{"@id":"https://doi.org/10.17182/hepdata.145997.v1/t2","@type":"Dataset","description":"Distributions of reconstructed VLQ mass for expected postfit background (blue histogram), signal plus background (colored lines), and observed data (black...","name":"Figure 14 Hadronic 4-Jet bHbZ"},{"@id":"https://doi.org/10.17182/hepdata.145997.v1/t3","@type":"Dataset","description":"Distributions of reconstructed VLQ mass for expected postfit background (blue histogram), signal plus background (colored lines), and observed data (black...","name":"Figure 14 Hadronic 4-Jet 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observed data (black...","name":"Figure 17 Semileptonic 4-Jet bZbZ"},{"@id":"https://doi.org/10.17182/hepdata.145997.v1/t18","@type":"Dataset","description":"The limit at 95% CL on the cross section for VLQ pair production for the branching fraction hypothesis 0% $\\mathcal{B}(B...","name":"Figure 18 0% B$(B \\to bH)$, 100% B$(B \\to bZ)$"},{"@id":"https://doi.org/10.17182/hepdata.145997.v1/t19","@type":"Dataset","description":"The limit at 95% CL on the cross section for VLQ pair production for the branching fraction hypothesis 25% $\\mathcal{B}(B...","name":"Figure 18 25% B$(B \\to bH)$, 25% B$(B \\to bZ)$"},{"@id":"https://doi.org/10.17182/hepdata.145997.v1/t20","@type":"Dataset","description":"The limit at 95% CL on the cross section for VLQ pair production for the branching fraction hypothesis 50% $\\mathcal{B}(B...","name":"Figure 18 50% B$(B \\to bH)$, 50% B$(B \\to bZ)$"},{"@id":"https://doi.org/10.17182/hepdata.145997.v1/t21","@type":"Dataset","description":"The limit at 95% 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