{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.99692.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1860980"}},{"@id":"https://doi.org/10.1007/JHEP12(2021)106","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"CMS Collaboration"},"creator":{"@type":"Organization","name":"CMS Collaboration"},"datePublished":"2021","description":"A search for a heavy resonance decaying to a top quark and a W boson in the fully hadronic final state is presented. The analysis is performed using data from proton-proton collisions at a center-of-mass energy of 13 TeV, corresponding to an integrated luminosity of 137 fb$^{-1}$ recorded by the CMS experiment at the LHC. The search is focused on heavy resonances, where the decay products of each top quark or W boson are expected to be reconstructed as a single, large-radius jet with a distinct substructure. The production of an excited bottom quark, b*, is used as a benchmark when setting limits on the cross section for a heavy resonance decaying to a top quark and a W boson. The hypotheses of b* quarks with left-handed, right-handed, and vector-like chiralities are excluded at 95% confidence level for masses below 2.6, 2.8, and 3.1 TeV, respectively. These are the most stringent limits on the b* quark mass to date, extending the previous best limits by almost a factor of two.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.99692.v1/t1","@type":"Dataset","description":"Upper limits on the product of the cross section and branching fraction at 95% CL for a left-handed b* quark...","name":"Figure 5 (upper)"},{"@id":"https://doi.org/10.17182/hepdata.99692.v1/t2","@type":"Dataset","description":"Upper limits on the product of the cross section and branching fraction at 95% CL for a right-handed b* quark...","name":"Figure 5 (middle)"},{"@id":"https://doi.org/10.17182/hepdata.99692.v1/t3","@type":"Dataset","description":"Upper limits on the product of the cross section and branching fraction at 95% CL for a vector-like b* quark...","name":"Figure 5 (lower)"},{"@id":"https://doi.org/10.17182/hepdata.99692.v1/t4","@type":"Dataset","description":"The distribution of Top jet $ au_{3}/ au_{2}$ for the simulation of backgrounds and a 2400 GeV (left-handed) b* signal....","name":"Figure 2 (upper left)"},{"@id":"https://doi.org/10.17182/hepdata.99692.v1/t5","@type":"Dataset","description":"The distribution of W jet $ au_{2}/ au_{1}$ for the simulation of backgrounds and a 2400 GeV (left-handed) b* signal....","name":"Figure 2 (upper right)"},{"@id":"https://doi.org/10.17182/hepdata.99692.v1/t6","@type":"Dataset","description":"The distribution of m_{W} for the simulation of backgrounds and a 2400 GeV (left-handed) b* signal. The area of the...","name":"Figure 2 (middle right)"},{"@id":"https://doi.org/10.17182/hepdata.99692.v1/t7","@type":"Dataset","description":"The distribution of Top jet DeepCSV score for the simulation of backgrounds and a 2400 GeV (left-handed) b* signal. The...","name":"Figure 2 (lower)"},{"@id":"https://doi.org/10.17182/hepdata.99692.v1/t8","@type":"Dataset","description":"The distribution of m_{t} for the simulation of backgrounds and a 2400 GeV (left-handed) b* signal. The area of the...","name":"Figure 2 (middle left)"},{"@id":"https://doi.org/10.17182/hepdata.99692.v1/t9","@type":"Dataset","description":"Distributions of $m_{tW}$ in the signal region for an interval of $m_{t}$ (65-105 GeV).","name":"Figure 4 (upper right)"},{"@id":"https://doi.org/10.17182/hepdata.99692.v1/t10","@type":"Dataset","description":"Distributions of $m_{tW}$ in the signal region for an interval of $m_{t}$ (105-225 GeV).","name":"Figure 4 (middle right)"},{"@id":"https://doi.org/10.17182/hepdata.99692.v1/t11","@type":"Dataset","description":"Distributions of $m_{tW}$ in the signal region for an interval of $m_{t}$ (225-285 GeV).","name":"Figure 4 (lower right)"},{"@id":"https://doi.org/10.17182/hepdata.99692.v1/t12","@type":"Dataset","description":"Distributions of $m_{tW}$ in themultijet control region of the signal region for an interval of $m_{t}$ (65-105 GeV).","name":"Figure 4 (upper left)"},{"@id":"https://doi.org/10.17182/hepdata.99692.v1/t13","@type":"Dataset","description":"Distributions of $m_{tW}$ in themultijet control region of the signal region for an interval of $m_{t}$ (105-225 GeV).","name":"Figure 4 (middle left)"},{"@id":"https://doi.org/10.17182/hepdata.99692.v1/t14","@type":"Dataset","description":"Distributions of $m_{tW}$ in themultijet control region of the signal region for an interval of $m_{t}$ (225-285 GeV).","name":"Figure 4 (lower left)"},{"@id":"https://doi.org/10.17182/hepdata.99692.v1/t15","@type":"Dataset","description":"Distributions of $m_{t}$ in the ttbar measurement region for an interval of $m_{t?ar{t}}$ (1200-1300 GeV).","name":"Figure 3 (upper right)"},{"@id":"https://doi.org/10.17182/hepdata.99692.v1/t16","@type":"Dataset","description":"Distributions of $m_{t}$ in the ttbar measurement region for an interval of $m_{t?ar{t}}$ (1300-1800 GeV).","name":"Figure 3 (middle right)"},{"@id":"https://doi.org/10.17182/hepdata.99692.v1/t17","@type":"Dataset","description":"Distributions of $m_{t}$ in the ttbar measurement region for an interval of $m_{t?ar{t}}$ (1800-3000 GeV).","name":"Figure 3 (lower right)"},{"@id":"https://doi.org/10.17182/hepdata.99692.v1/t18","@type":"Dataset","description":"Distributions of $m_{t}$ in themultijet control region of the ttbar measurement region for an interval of $m_{t?ar{t}}$ (1200-1300 GeV).","name":"Figure 3 (upper left)"},{"@id":"https://doi.org/10.17182/hepdata.99692.v1/t19","@type":"Dataset","description":"Distributions of $m_{t}$ in themultijet control region of the ttbar measurement region for an interval of $m_{t?ar{t}}$ (1300-1800 GeV).","name":"Figure 3 (middle left)"},{"@id":"https://doi.org/10.17182/hepdata.99692.v1/t20","@type":"Dataset","description":"Distributions of $m_{t}$ in themultijet control region of the ttbar measurement region for an interval of $m_{t?ar{t}}$ (1800-3000 GeV).","name":"Figure 3 (lower left)"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1860980?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/99692"}],"inLanguage":"en","name":"Search for a heavy resonance decaying to a top quark and a W boson at $\\sqrt{s} =$ 13 TeV in the fully hadronic final state","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1860980?version=1","version":1}