{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.114361.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1972089"}},{"@id":"https://doi.org/10.1007/JHEP04(2022)048","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"CMS Collaboration"},"creator":{"@type":"Organization","name":"CMS Collaboration"},"datePublished":"2022","description":"A search for a heavy resonance decaying into a top quark and a W boson in proton-protoncollisions at $\\sqrt{s}=13$ TeV is presented. The data analyzed were recorded with the CMS detector at theLHC and correspond to an integrated luminosity of 137 fb$^{-1}$.The search is performed in the lepton+jets final state, where the lepton is either an electron or a muon.The top quark is reconstructed as a single jet and the W boson from its decay into a charged leptonand a neutrino. A top quark tagging technique based on a jet clusteringwith variable distance parameter and inherent jet grooming is used to identify jets from the collimated top quark decay.The results are interpreted in the context of a benchmark model where an excited bottom quark b* is the heavy resonance.A statistical combination with a search in the all-hadronic final state is performed in order to derive limits on this model.The range of probed b* masses was extended from 1.4 TeV down to 0.7 TeV.At a 95% confidence level, b*masses up to 3.0, 3.0, and 3.2 TeV are excluded for left-handed, right-handed, and vector-like couplings,respectively.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.114361.v1/t1","@type":"Dataset","description":"Distributions of MtW in the 1b category. The data are shown by filled markers, where the horizontal bars indicate the...","name":"Figure 1 a"},{"@id":"https://doi.org/10.17182/hepdata.114361.v1/t2","@type":"Dataset","description":"Distributions of MtW in the 2b category. The data are shown by filled markers, where the horizontal bars indicate the...","name":"Figure 1 b"},{"@id":"https://doi.org/10.17182/hepdata.114361.v1/t3","@type":"Dataset","description":"Upper limits on the production cross section times branching fraction of the b* LH hypothesis at a 95% CL. Dashed...","name":"Figure 2 a"},{"@id":"https://doi.org/10.17182/hepdata.114361.v1/t4","@type":"Dataset","description":"Upper limits on the production cross section times branching fraction of the b* RH hypothesis at a 95% CL. Dashed...","name":"Figure 2 b"},{"@id":"https://doi.org/10.17182/hepdata.114361.v1/t5","@type":"Dataset","description":"Upper limits on the production cross section times branching fraction of the b* VL hypothesis at a 95% CL. Dashed...","name":"Figure 2 c"},{"@id":"https://doi.org/10.17182/hepdata.114361.v1/t6","@type":"Dataset","description":"Upper limits on the production cross section times branching fraction of the B+b hypothesis at a 95% CL. Dashed colored...","name":"Figure 3 a"},{"@id":"https://doi.org/10.17182/hepdata.114361.v1/t7","@type":"Dataset","description":"Upper limits on the production cross section times branching fraction of the B+t hypothesis at a 95% CL. Dashed colored...","name":"Figure 3 b"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1972089?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/114361"}],"inLanguage":"en","name":"Search for a heavy resonance decaying into a top quark and a W boson in the lepton+jets final state at $\\sqrt{s}$= 13 TeV","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1972089?version=1","version":1}