{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.134011.v2","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/2037744"}},{"@id":"https://doi.org/10.1007/JHEP06(2022)063","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2023","description":"Cross-section measurements of top-quark pair production where the hadronically decaying top quark has transverse momentum greater than $355$ GeV and the other top quark decays into $\\ell \\nu b$ are presented using 139 fb$^{-1}$ of data collected by the ATLAS experiment during proton--proton collisions at the LHC. The fiducial cross-section at $\\sqrt{s}=13$ TeV is measured to be $\\sigma = 1.267 \\pm 0.005 \\pm 0.053$ pb, where the uncertainties reflect the limited number of data events and the systematic uncertainties, giving a total uncertainty of $4.2\\%$. The cross-section is measured differentially as a function of variables characterising the $t\\bar{t}$ system and additional radiation in the events. The results are compared with various Monte Carlo generators, including comparisons where the generators are reweighted to match a parton-level calculation at next-to-next-to-leading order. The reweighting improves the agreement between data and theory. The measured distribution of the top-quark transverse momentum is used to search for new physics in the context of the effective field theory framework. No significant deviation from the Standard Model is observed and limits are set on the Wilson coefficients of the dimension-six operators $O_{tG}$ and $O_{tq}^{(8)}$, where the limits on the latter are the most stringent to date.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.134011.v2/t1","@type":"Dataset","description":"- - - - - - - - Overview of HEPData Record - - - - - - - -...","name":"Table of contents"},{"@id":"https://doi.org/10.17182/hepdata.134011.v2/t2","@type":"Dataset","description":"Total cross-section at particle level in the boosted topology. Note that the values shown here are obtained by propagating the...","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.134011.v2/t3","@type":"Dataset","description":"Absolute differential cross-section as a function of $p_T^{t,h}$ at particle level in the boosted topology. The measured differential cross-section is...","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.134011.v2/t4","@type":"Dataset","description":"Covariance matrix of the Absolute differential cross-section as function of $p_T^{t,h}$ at particle level in the boosted topology, accounting for...","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.134011.v2/t5","@type":"Dataset","description":"Relative differential cross-section as a function of $p_T^{t,h}$ at particle level in the boosted topology. The measured differential cross-section is...","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.134011.v2/t6","@type":"Dataset","description":"Absolute differential cross-section as a function of $p_T^{t,l}$ at particle level in the boosted topology. The measured differential cross-section is...","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.134011.v2/t7","@type":"Dataset","description":"Covariance matrix of the Absolute differential cross-section as function of $p_T^{t,l}$ at particle level in the boosted topology, accounting for...","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.134011.v2/t8","@type":"Dataset","description":"Relative differential cross-section as a function of $p_T^{t,l}$ at particle level in the boosted topology. The measured differential cross-section is...","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.134011.v2/t9","@type":"Dataset","description":"Absolute differential cross-section as a function of $m^{t\\bar{t}}$ at particle level in the boosted topology. 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117"},{"@id":"https://doi.org/10.17182/hepdata.134011.v2/t119","@type":"Dataset","description":"Statistical covariance matrix between the absolute differential cross-section as function of $y^{t,l}$ and the absolute differential cross-section as function of...","name":"Table 118"},{"@id":"https://doi.org/10.17182/hepdata.134011.v2/t120","@type":"Dataset","description":"Statistical covariance matrix between the absolute differential cross-section as function of $y^{t\\bar{t}}$ and the absolute differential cross-section as function of...","name":"Table 119"},{"@id":"https://doi.org/10.17182/hepdata.134011.v2/t121","@type":"Dataset","description":"Statistical covariance matrix between the absolute differential cross-section as function of $y^{t\\bar{t}}$ and the absolute differential cross-section as function of...","name":"Table 120"},{"@id":"https://doi.org/10.17182/hepdata.134011.v2/t122","@type":"Dataset","description":"Statistical covariance matrix between the absolute differential 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156"},{"@id":"https://doi.org/10.17182/hepdata.134011.v2/t158","@type":"Dataset","description":"Statistical covariance matrix between the absolute differential cross-section as function of $\\frac{\\Delta\\phi}{\\pi}(t_{h},t_{l})$ and the absolute differential cross-section as function of...","name":"Table 157"},{"@id":"https://doi.org/10.17182/hepdata.134011.v2/t159","@type":"Dataset","description":"Statistical covariance matrix between the absolute differential cross-section as function of $\\frac{\\Delta\\phi}{\\pi}(t_{h},t_{l})$ and the absolute differential cross-section as function of...","name":"Table 158"},{"@id":"https://doi.org/10.17182/hepdata.134011.v2/t160","@type":"Dataset","description":"Statistical covariance matrix between the absolute differential cross-section as function of $H_T^{t\\bar{t}+jets}$ and the absolute differential cross-section as function of...","name":"Table 159"},{"@id":"https://doi.org/10.17182/hepdata.134011.v2/t161","@type":"Dataset","description":"Statistical covariance matrix between the absolute differential cross-section as function of $H_T^{t\\bar{t}+jets}$ and the absolute differential cross-section as function of...","name":"Table 160"},{"@id":"https://doi.org/10.17182/hepdata.134011.v2/t162","@type":"Dataset","description":"Statistical covariance matrix between the absolute differential cross-section as function of $H_T^{t\\bar{t}+jets}$ and the absolute differential cross-section as function of...","name":"Table 161"},{"@id":"https://doi.org/10.17182/hepdata.134011.v2/t163","@type":"Dataset","description":"Statistical covariance matrix between the absolute differential cross-section as function of $H_T^{t\\bar{t}+jets}$ and the absolute differential cross-section as function of...","name":"Table 162"},{"@id":"https://doi.org/10.17182/hepdata.134011.v2/t164","@type":"Dataset","description":"Statistical covariance matrix between the absolute differential cross-section as function of $H_T^{t\\bar{t}+jets}$ and the absolute differential cross-section as function of...","name":"Table 163"},{"@id":"https://doi.org/10.17182/hepdata.134011.v2/t165","@type":"Dataset","description":"Statistical covariance matrix between the absolute differential cross-section as function of $H_T^{t\\bar{t}+jets}$ and the absolute differential cross-section as function of...","name":"Table 164"},{"@id":"https://doi.org/10.17182/hepdata.134011.v2/t166","@type":"Dataset","description":"Statistical covariance matrix between the absolute differential cross-section as function of $H_T^{t\\bar{t}+jets}$ and the absolute differential cross-section as function of...","name":"Table 165"},{"@id":"https://doi.org/10.17182/hepdata.134011.v2/t167","@type":"Dataset","description":"Statistical covariance matrix between the absolute differential cross-section as function of $H_T^{t\\bar{t}+jets}$ and the absolute differential cross-section as function of...","name":"Table 166"},{"@id":"https://doi.org/10.17182/hepdata.134011.v2/t168","@type":"Dataset","description":"Statistical covariance matrix between the absolute differential cross-section as function of $H_T^{t\\bar{t}+jets}$ and the absolute differential cross-section as function of...","name":"Table 167"},{"@id":"https://doi.org/10.17182/hepdata.134011.v2/t169","@type":"Dataset","description":"Statistical covariance matrix between the absolute differential cross-section as function of $H_T^{t\\bar{t}+jets}$ and the absolute differential cross-section as function of...","name":"Table 168"},{"@id":"https://doi.org/10.17182/hepdata.134011.v2/t170","@type":"Dataset","description":"Statistical covariance matrix between the absolute differential cross-section as function of $H_T^{t\\bar{t}+jets}$ and the absolute differential cross-section as function of...","name":"Table 169"},{"@id":"https://doi.org/10.17182/hepdata.134011.v2/t171","@type":"Dataset","description":"Statistical covariance matrix between the absolute differential cross-section as function of $N^j$ and the absolute differential cross-section as function of...","name":"Table 170"},{"@id":"https://doi.org/10.17182/hepdata.134011.v2/t172","@type":"Dataset","description":"Statistical covariance matrix between the absolute differential cross-section as function of $N^j$ and the absolute differential cross-section as function of...","name":"Table 171"},{"@id":"https://doi.org/10.17182/hepdata.134011.v2/t173","@type":"Dataset","description":"Statistical covariance matrix between the absolute differential cross-section as function of $N^j$ and the absolute differential cross-section as function of...","name":"Table 172"},{"@id":"https://doi.org/10.17182/hepdata.134011.v2/t174","@type":"Dataset","description":"Statistical covariance matrix between the absolute differential cross-section as function of $N^j$ and the absolute differential cross-section as function of...","name":"Table 173"},{"@id":"https://doi.org/10.17182/hepdata.134011.v2/t175","@type":"Dataset","description":"Statistical covariance matrix between the absolute differential cross-section as function of $N^j$ and the absolute differential cross-section as function of...","name":"Table 174"},{"@id":"https://doi.org/10.17182/hepdata.134011.v2/t176","@type":"Dataset","description":"Statistical covariance matrix between the absolute differential cross-section as function of $N^j$ and the absolute differential cross-section as function of...","name":"Table 175"},{"@id":"https://doi.org/10.17182/hepdata.134011.v2/t177","@type":"Dataset","description":"Statistical covariance matrix between the absolute differential cross-section as function of $N^j$ and the absolute differential cross-section as function of...","name":"Table 176"},{"@id":"https://doi.org/10.17182/hepdata.134011.v2/t178","@type":"Dataset","description":"Statistical covariance matrix between the absolute differential cross-section as 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cross-section as function of $p_T^{j,2}$ and the absolute differential cross-section as function of...","name":"Table 274"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins2037744?version=2"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/134011"}],"inLanguage":"en","name":"Measurements of differential cross-sections in top-quark pair events with a high transverse momentum top quark and limits on beyond the Standard Model contributions to top-quark pair production with the ATLAS detector at $\\sqrt{s}=13$ TeV","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins2037744?version=2","version":2}