{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.127138.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/2039384"}},{"@id":"https://doi.org/10.1007/JHEP09(2022)088","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"CMS Collaboration"},"creator":{"@type":"Organization","name":"CMS Collaboration"},"datePublished":"2022","description":"A search is presented for a heavy $\\mathrm{W\\prime}$ boson resonance decaying to a $\\mathrm{B}$ or $\\mathrm{T}$ vector-like quark and a $\\mathrm{t}$ or a $\\mathrm{b}$ quark, respectively.  The analysis is performed using proton-proton collisions collected with the CMS detector at the LHC. The data correspond to an integrated luminosity of 138 $\\mathrm{fb}^{-1}$ at a center-of-mass energy of 13 TeV. Both decay channels result in a signature with a $\\mathrm{t}$ quark, a Higgs or $\\mathrm{Z}$ boson, and a $\\mathrm{b}$ quark, each produced with a significant Lorentz boost.  The all-hadronic decays of the Higgs or $\\mathrm{Z}$ boson and of the $\\mathrm{t}$ quark are selected using jet substructure techniques to reduce standard model backgrounds, resulting in a distinct three-jet $\\mathrm{W\\prime}$ boson decay signature.  No significant deviation in data with respect to the standard model background prediction is observed. Upper limits are set at 95\\% confidence level on the product of the $\\mathrm{W\\prime}$ boson cross section and the final state branching fraction. A $\\mathrm{W\\prime}$ boson with a mass below 3.2 TeV is excluded, given the benchmark model assumption of democratic branching fractions.  In addition, limits are set based on generalizations of these assumptions.  These are the most sensitive limits to date for this final state.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.127138.v1/t1","@type":"Dataset","description":"Reconstructed W\u2032 boson mass distributions in the tHb signal region.","name":"tHb mass in the signal region"},{"@id":"https://doi.org/10.17182/hepdata.127138.v1/t2","@type":"Dataset","description":"Reconstructed W\u2032 boson mass distributions in the tZb signal region.","name":"tZb mass in the signal region"},{"@id":"https://doi.org/10.17182/hepdata.127138.v1/t3","@type":"Dataset","description":"The W' boson 95% CL limits on the product of cross section and branching fraction. The expected and observed limits...","name":"center VLQ mass limits"},{"@id":"https://doi.org/10.17182/hepdata.127138.v1/t4","@type":"Dataset","description":"The W' boson 95% CL limits on the product of cross section and branching fraction. The expected and observed limits...","name":"high VLQ mass limits"},{"@id":"https://doi.org/10.17182/hepdata.127138.v1/t5","@type":"Dataset","description":"The W' boson 95% CL limits on the product of cross section and branching fraction. The expected and observed limits...","name":"low VLQ mass limits"},{"@id":"https://doi.org/10.17182/hepdata.127138.v1/t6","@type":"Dataset","description":"Expected 95% CL limits for generalized hypotheses varying the fraction of tB (F(VLQ=B)) and bT (F(VLQ=T)) from the W\u2032 decay","name":"Generalized Expected tB,bT limits"},{"@id":"https://doi.org/10.17182/hepdata.127138.v1/t7","@type":"Dataset","description":"Expected 95% CL limits for generalized hypotheses varying the VLQ branching fraction to qH and qZ","name":"Generalized Expected qH,qZ limits"},{"@id":"https://doi.org/10.17182/hepdata.127138.v1/t8","@type":"Dataset","description":"Observed 95% CL limits for generalized hypotheses varying the fraction of tB (F(VLQ=B)) and bT (F(VLQ=T)) from the W\u2032 decay","name":"Generalized Observed tB,bT limits"},{"@id":"https://doi.org/10.17182/hepdata.127138.v1/t9","@type":"Dataset","description":"Observed 95% CL limits for generalized hypotheses varying the VLQ branching fraction to qH and qZ","name":"Generalized Observed qH,qZ limits"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins2039384?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/127138"}],"inLanguage":"en","name":"Search for a W' boson decaying to a vector-like quark and a top or bottom quark in the all-jets final state at $\\sqrt{s}$ = 13 TeV","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins2039384?version=1","version":1}