{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.83661.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1685207"}},{"@id":"https://doi.org/10.1103/PhysRevD.98.092005","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2018","description":"CERN-LHC, ATLAS.  Results from a search for the pair production of heavy vector-like quarks, $T\\bar T$ or $B\\bar B$, that decay into final states with jets and no reconstructed leptons. Jets in the final state are classified using a deep neural network as arising from hadronically decaying $W/Z$ bosons, Higgs bosons, top quarks, or background. The analysis uses data from the ATLAS experiment corresponding to 36.1 fb$^{-1}$ of proton--proton collisions with a center-of-mass energy of $\\sqrt{s}$ = 13 TeV delivered by the Large Hadron Collider in 2015 and 2016. No significant deviation from the Standard Model expectation is observed. Results are interpreted assuming the vector-like quarks decay into a Standard Model boson and a third-generation-quark, $T\\rightarrow Wb,Ht,Zt$ or $B\\rightarrow Wt,Hb,Zb$, for a variety of branching ratios.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.83661.v1/t1","@type":"Dataset","description":"Expected and observed upper limits at the 95% CL on the $T\\bar T$ cross section as a function of $T$...","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.83661.v1/t2","@type":"Dataset","description":"Expected and observed upper limits at the 95% CL on the $B\\bar B$ cross section as a function of $B$...","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.83661.v1/t3","@type":"Dataset","description":"Expected and observed upper limits at the 95% CL on the $B\\bar B$ cross section as a function of $B$...","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.83661.v1/t4","@type":"Dataset","description":"Expected and observed 95% CL lower limits on the mass of a vector-like $T$ quark in the branching-ratio plane.","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.83661.v1/t5","@type":"Dataset","description":"Expected and observed 95% CL lower limits on the mass of a vector-like $B$ quark in the branching-ratio plane.","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.83661.v1/t6","@type":"Dataset","description":"Expected and observed upper limits at the 95% CL on the $T\\bar T$ cross section as a function of $T$...","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.83661.v1/t7","@type":"Dataset","description":"Expected and observed upper limits at the 95% CL on the $B\\bar B$ cross section as a function of $B$...","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.83661.v1/t8","@type":"Dataset","description":"Expected and observed upper limits at the 95% CL on the $B\\bar B$ cross section as a function of $B$...","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.83661.v1/t9","@type":"Dataset","description":"Expected and observed upper limits at the 95% CL on the $B\\bar B$ cross section as a function of $B$...","name":"Table 9"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1685207?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/83661"}],"inLanguage":"en","name":"Search for pair production of heavy vector-like quarks decaying into hadronic final states in $pp$ collisions at $\\sqrt{s} = 13$ TeV with the ATLAS detector","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1685207?version=1","version":1}