{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.100426.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/2006491"}},{"@id":"https://doi.org/10.1007/JHEP05(2022)093","@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 single production of a vector-like T quark with charge $2e/3$, in the decay channel featuring a top quark and a Z boson, with the top quark decaying hadronically and the Z boson decaying to neutrinos. The search uses data collected by the CMS experiment in proton-proton collisions at a center-of-mass energy of 13 TeV, corresponding to an integrated luminosity of 136 $\\mathrm{fb}^{-1}$ recorded at the CERN LHC in 2016--2018. The search is sensitive to a T quark mass between 0.6 and 1.8 TeV with decay widths ranging from negligibly small up to 30$\\%$ of the T quark mass. Reconstruction strategies for the top quark are based on the degree of Lorentz boosting of its final state. At 95$\\%$ confidence level, the upper limit on the product of the cross section and branching fraction for a T quark of small decay width varies between 15 and 602 $\\mathrm{fb}$, depending on its mass. For a T quark with decay widths between 10 and 30$\\%$ of its mass, this upper limit ranges between 16 and 836 $\\mathrm{fb}$. For most of the studied range, the results provide the best limits to date. This is the first search for single T quark production based on the full Run 2 data set of the LHC.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.100426.v1/t1","@type":"Dataset","description":"Product of efficiency and acceptance of the event selection for T signal events as a function of the particle mass...","name":"Figure 2a"},{"@id":"https://doi.org/10.17182/hepdata.100426.v1/t2","@type":"Dataset","description":"Product of efficiency and acceptance of the event selection for T signal events as a function of the particle mass...","name":"Figure 2b"},{"@id":"https://doi.org/10.17182/hepdata.100426.v1/t3","@type":"Dataset","description":"Product of efficiency and acceptance of the event selection for T signal events as a function of the particle mass...","name":"Figure 2c"},{"@id":"https://doi.org/10.17182/hepdata.100426.v1/t4","@type":"Dataset","description":"Product of efficiency and acceptance of the event selection for T signal events as a function of the particle 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