{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.83541.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1685421"}},{"@id":"https://doi.org/10.1103/PhysRevLett.121.211801","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2018","description":"CERN-LHC.  A combination of the searches for pair-produced vector-like partners of the top and bottom quarks in various decay channels ($T$$\\rightarrow$$Zt/Wb/Ht$, $B$$\\rightarrow$$Zb/Wt/Hb$) is performed using 36.1 fb$^{-1}$ of $pp$ collision data at $\\sqrt{s}$ = 13 TeV with the ATLAS detector at the Large Hadron Collider. The observed data are found to be in good agreement with the Standard Model background prediction in all individual searches. Therefore, combined 95% confidence level upper limits are set on the production cross-section for a range of vector-like quark scenarios, significantly extending the reach of the individual searches.  A singlet $T$ is excluded for masses below 1.31 TeV and a singlet $B$ is excluded for masses below 1.22 TeV.  Assuming a weak isospin $(T,B)$ doublet, $T$ and $B$ masses below 1.37 TeV are excluded.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.83541.v1/t1","@type":"Dataset","description":"Expected and observed 95% lower limits on the vector-like top quark mass as a function of the branching ratio, asumming...","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.83541.v1/t2","@type":"Dataset","description":"Expected and observed 95% lower limits on the vector-like bottom quark mass as a function of the branching ratio, asumming...","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.83541.v1/t3","@type":"Dataset","description":"Expected and observed 95% upper limits on the vector-like top quark pair-production signal strength (i.e. the ratio sigma_exclusion/sigma_VLQ) as a...","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.83541.v1/t4","@type":"Dataset","description":"Expected and observed 95% upper limits on the vector-like top quark pair-production signal 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upper limits on the vector-like top quark pair-production signal strength (i.e. the ratio sigma_exclusion/sigma_VLQ) as a...","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.83541.v1/t13","@type":"Dataset","description":"Expected and observed 95% upper limits on the vector-like bottom quark pair-production signal strength (i.e. the ratio sigma_exclusion/sigma_VLQ) as a...","name":"Table 13"},{"@id":"https://doi.org/10.17182/hepdata.83541.v1/t14","@type":"Dataset","description":"Expected and observed 95% upper limits on the vector-like bottom quark pair-production signal strength (i.e. the ratio sigma_exclusion/sigma_VLQ) as a...","name":"Table 14"},{"@id":"https://doi.org/10.17182/hepdata.83541.v1/t15","@type":"Dataset","description":"Expected and observed 95% upper limits on the vector-like bottom quark pair-production signal strength (i.e. the ratio sigma_exclusion/sigma_VLQ) as a...","name":"Table 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