{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.137888.v3","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/2648096"}},{"@id":"https://doi.org/10.1007/JHEP07(2023)141","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2023","description":"Inclusive and differential cross-sections for dilepton $t\\bar{t}$ production measured in $\\sqrt{s}=13\\;$TeV $pp$ collisions with the ATLAS detector\n\nThe analysis uses data collected in $pp$ collisions at $\\sqrt{s} = 13$~TeV during the LHC Run 2 corresponding to an integrated luminosity of 140~fb$^{-1}$.\nThe final state consists of a $e\\mu$ pair with opposite sign leptons and one or two $b$-tagged jets.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.137888.v3/t1","@type":"Dataset","description":"Definition of the fiducial phase space with the lepton candidate, electron $e$ and muon $\\mu$, and jets.","name":"Fiducial phase space"},{"@id":"https://doi.org/10.17182/hepdata.137888.v3/t2","@type":"Dataset","description":"Breakdown of systematic uncertainties in the measured fiducial cross-section. The impact of the top-quark mass on the cross-section is included...","name":"Table 1 - Fiducial cross Sections"},{"@id":"https://doi.org/10.17182/hepdata.137888.v3/t3","@type":"Dataset","description":"Data bootstrap post unfolding for the fiducial cross-section. The replicas are obtained by reweighting each observed data event by a...","name":"Table 2 - Fiducial cross Sections (bootstrap)"},{"@id":"https://doi.org/10.17182/hepdata.137888.v3/t4","@type":"Dataset","description":"Breakdown of systematic uncertainties in the measured inclusive cross-section. The impact of the top-quark mass on the cross-section is included...","name":"Table 3 - Inclusive cross Sections"},{"@id":"https://doi.org/10.17182/hepdata.137888.v3/t5","@type":"Dataset","description":"Data bootstrap post unfolding for the inclusive cross-section. The replicas are obtained by reweighting each observed data event by a...","name":"Table 4 - Inclusive cross Sections (bootstrap)"},{"@id":"https://doi.org/10.17182/hepdata.137888.v3/t6","@type":"Dataset","description":"Differential absolute cross-section for $\\textrm{p}_{\\textrm{T}}^{l}$. The impact of the top-quark mass on the cross-section is included in the table and...","name":"Table 5 - Diff. XS $p_T^{l}$"},{"@id":"https://doi.org/10.17182/hepdata.137888.v3/t7","@type":"Dataset","description":"Covariance Matrix (statistical uncertainties only) for the differential absolute cross-section for $\\textrm{p}_{\\textrm{T}}^{l}$. The last bin of the distribution contains the...","name":"Table 6 - Cov. Matrix Diff. XS $p_T^{l}$"},{"@id":"https://doi.org/10.17182/hepdata.137888.v3/t8","@type":"Dataset","description":"Data bootstrap post unfolding for the differential absolute cross-section for $\\textrm{p}_{\\textrm{T}}^{l}$. The replicas are obtained by reweighting each observed data...","name":"Table 7 - Bootstrap Diff. XS $p_T^{l}$"},{"@id":"https://doi.org/10.17182/hepdata.137888.v3/t9","@type":"Dataset","description":"Differential absolute cross-section for $|\\eta^{l}|$. The impact of the top-quark mass on the cross-section is included in the table and...","name":"Table 8 - Diff. XS $|\\eta^{l}|$"},{"@id":"https://doi.org/10.17182/hepdata.137888.v3/t10","@type":"Dataset","description":"Covariance Matrix (statistical uncertainties only) for the differential absolute cross-section for $|\\eta^{l}|$.","name":"Table 9 - Cov. Matrix Diff. XS $|\\eta^{l}|$"},{"@id":"https://doi.org/10.17182/hepdata.137888.v3/t11","@type":"Dataset","description":"Data bootstrap post unfolding for the differential absolute cross-section for $|\\eta^{l}|$. The replicas are obtained by reweighting each observed data...","name":"Table 10 - Bootstrap Diff. 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The replicas are obtained by reweighting each...","name":"Table 19 - Bootstrap Diff. XS $p_T^{e} + p_T^{\\mu}$"},{"@id":"https://doi.org/10.17182/hepdata.137888.v3/t21","@type":"Dataset","description":"Differential absolute cross-section for $\\textrm{p}_{\\textrm{T}}^{e\\mu}$. The impact of the top-quark mass on the cross-section is included in the table and...","name":"Table 20 - Diff. XS $p_T^{e\\mu}$"},{"@id":"https://doi.org/10.17182/hepdata.137888.v3/t22","@type":"Dataset","description":"Covariance Matrix (statistical uncertainties only) for the differential absolute cross-section for $\\textrm{p}_{\\textrm{T}}^{e\\mu}$. The last bin of the distribution contains the...","name":"Table 21 - Cov. Matrix Diff. XS $p_T^{e\\mu}$"},{"@id":"https://doi.org/10.17182/hepdata.137888.v3/t23","@type":"Dataset","description":"Data bootstrap post unfolding for the differential absolute cross-section for $\\textrm{p}_{\\textrm{T}}^{e\\mu}$. The replicas are obtained by reweighting each observed data...","name":"Table 22 - Bootstrap Diff. XS $p_T^{e\\mu}$"},{"@id":"https://doi.org/10.17182/hepdata.137888.v3/t24","@type":"Dataset","description":"Differential absolute cross-section for $|\\Delta\\phi^{e\\mu}|$. The impact of the top-quark mass on the cross-section is included in the table and...","name":"Table 23 - Diff. XS $|\\Delta\\phi^{e\\mu}|$"},{"@id":"https://doi.org/10.17182/hepdata.137888.v3/t25","@type":"Dataset","description":"Covariance Matrix (statistical uncertainties only) for the differential absolute cross-section for $|\\Delta\\phi^{e\\mu}|$.","name":"Table 24 - Cov. Matrix Diff. XS $|\\Delta\\phi^{e\\mu}|$"},{"@id":"https://doi.org/10.17182/hepdata.137888.v3/t26","@type":"Dataset","description":"Data bootstrap post unfolding for the differential absolute cross-section for $|\\Delta\\phi^{e\\mu}|$. The replicas are obtained by reweighting each observed data...","name":"Table 25 - Bootstrap Diff. XS $|\\Delta\\phi^{e\\mu}|$"},{"@id":"https://doi.org/10.17182/hepdata.137888.v3/t27","@type":"Dataset","description":"Differential absolute cross-section for $|y^{e\\mu}|$. The impact of the top-quark mass on the cross-section is included in the table and...","name":"Table 26 - Diff. XS $|y^{e\\mu}|$"},{"@id":"https://doi.org/10.17182/hepdata.137888.v3/t28","@type":"Dataset","description":"Covariance Matrix (statistical uncertainties only) for the differential absolute cross-section for $|y^{e\\mu}|$.","name":"Table 27 - Cov. Matrix Diff. XS $|y^{e\\mu}|$"},{"@id":"https://doi.org/10.17182/hepdata.137888.v3/t29","@type":"Dataset","description":"Data bootstrap post unfolding for the differential absolute cross-section for $|y^{e\\mu}|$. The replicas are obtained by reweighting each observed data...","name":"Table 28 - Bootstrap Diff. XS $|y^{e\\mu}|$"},{"@id":"https://doi.org/10.17182/hepdata.137888.v3/t30","@type":"Dataset","description":"Double differential absolute cross-section for $|y^{e\\mu}|$ x $m^{e\\mu}$. The impact of the top-quark mass on the cross-section is included in...","name":"Table 29 - Diff. XS $|y^{e\\mu}|$ x $m^{e\\mu}$"},{"@id":"https://doi.org/10.17182/hepdata.137888.v3/t31","@type":"Dataset","description":"Covariance Matrix (statistical uncertainties only) for the double differential absolute cross-section for $|y^{e\\mu}|$ x $m^{e\\mu}$. The highest invariant mass bin...","name":"Table 30 - Cov. Matrix Diff. XS $|y^{e\\mu}|$ x $m^{e\\mu}$"},{"@id":"https://doi.org/10.17182/hepdata.137888.v3/t32","@type":"Dataset","description":"Data bootstrap post unfolding for the double differential absolute cross-section for $|y^{e\\mu}|$ x $m^{e\\mu}$. The replicas are obtained by reweighting...","name":"Table 31 - Bootstrap Diff. XS $|y^{e\\mu}|$ x $m^{e\\mu}$"},{"@id":"https://doi.org/10.17182/hepdata.137888.v3/t33","@type":"Dataset","description":"Double differential absolute cross-section for $|\\Delta\\phi^{e\\mu}|$ x $m^{e\\mu}$. The impact of the top-quark mass on the cross-section is included in...","name":"Table 32 - Diff. XS $|\\Delta\\phi^{e\\mu}|$ x $m^{e\\mu}$"},{"@id":"https://doi.org/10.17182/hepdata.137888.v3/t34","@type":"Dataset","description":"Covariance Matrix (statistical uncertainties only) for the double differential absolute cross-section for $|\\Delta\\phi^{e\\mu}|$ x $m^{e\\mu}$. The highest invariant mass bin...","name":"Table 33 - Cov. Matrix $|\\Delta\\phi^{e\\mu}|$ x $m^{e\\mu}$"},{"@id":"https://doi.org/10.17182/hepdata.137888.v3/t35","@type":"Dataset","description":"Data bootstrap post unfolding for the double differential absolute cross-section for $|\\Delta\\phi^{e\\mu}|$ x $m^{e\\mu}$. The replicas are obtained by reweighting...","name":"Table 34 - Bootstrap $|\\Delta\\phi^{e\\mu}|$ x $m^{e\\mu}$"},{"@id":"https://doi.org/10.17182/hepdata.137888.v3/t36","@type":"Dataset","description":"Double differential absolute cross-section for $|\\Delta\\phi^{e\\mu}|$ x $\\textrm{p}_{\\textrm{T}}^{e\\mu}$. The impact of the top-quark mass on the cross-section is included in...","name":"Table 35 - Diff. XS $|\\Delta\\phi^{e\\mu}|$ x $p_T^{e\\mu}$"},{"@id":"https://doi.org/10.17182/hepdata.137888.v3/t37","@type":"Dataset","description":"Covariance Matrix (statistical uncertainties only) for the double differential absolute cross-section for $|\\Delta\\phi^{e\\mu}|$ x $\\textrm{p}_{\\textrm{T}}^{e\\mu}$. The highest $\\textrm{p}_{\\textrm{T}}^{e\\mu}$ bin contains...","name":"Table 36 - Cov. Matrix $|\\Delta\\phi^{e\\mu}|$ x $p_T^{e\\mu}$"},{"@id":"https://doi.org/10.17182/hepdata.137888.v3/t38","@type":"Dataset","description":"Data bootstrap post unfolding for the double differential absolute cross-section for $|\\Delta\\phi^{e\\mu}|$ x $\\textrm{p}_{\\textrm{T}}^{e\\mu}$. The replicas are obtained by reweighting...","name":"Table 37 - Bootstrap $|\\Delta\\phi^{e\\mu}|$ x $p_T^{e\\mu}$"},{"@id":"https://doi.org/10.17182/hepdata.137888.v3/t39","@type":"Dataset","description":"Double differential absolute cross-section for $|\\Delta\\phi^{e\\mu}|$ x $\\textrm{E}^{e} + \\textrm{E}^{\\mu}$. The impact of the top-quark mass on the cross-section is...","name":"Table 38 - Diff. XS $|\\Delta\\phi^{e\\mu}|$ x $E^e + E^{\\mu}$"},{"@id":"https://doi.org/10.17182/hepdata.137888.v3/t40","@type":"Dataset","description":"Covariance Matrix (statistical uncertainties only) for the double differential absolute cross-section for $|\\Delta\\phi^{e\\mu}|$ x $\\textrm{E}^{e} + \\textrm{E}^{\\mu}$. The highest $\\textrm{E}^{e}...","name":"Table 39 - Cov. Matrix $|\\Delta\\phi^{e\\mu}|$ x $E^e + E^{\\mu}$"},{"@id":"https://doi.org/10.17182/hepdata.137888.v3/t41","@type":"Dataset","description":"Data bootstrap post unfolding for the double differential absolute cross-section for $|\\Delta\\phi^{e\\mu}|$ x $\\textrm{E}^{e} + \\textrm{E}^{\\mu}$. The replicas are obtained...","name":"Table 40 - Bootstrap $|\\Delta\\phi^{e\\mu}|$ x $E^e + E^{\\mu}$"},{"@id":"https://doi.org/10.17182/hepdata.137888.v3/t42","@type":"Dataset","description":"Differential normalised cross-section for $\\textrm{p}_{\\textrm{T}}^{l}$. The impact of the top-quark mass on the cross-section is included in the table and...","name":"Table 41 - Norm. $p_T^{l}$"},{"@id":"https://doi.org/10.17182/hepdata.137888.v3/t43","@type":"Dataset","description":"Covariance Matrix (statistical uncertainties only) for the differential normalised cross-section for $\\textrm{p}_{\\textrm{T}}^{l}$. The last bin of the distribution contains the...","name":"Table 42 - Cov. Matrix norm. $p_T^{l}$"},{"@id":"https://doi.org/10.17182/hepdata.137888.v3/t44","@type":"Dataset","description":"Data bootstrap post unfolding for the differential normalised cross-section for $\\textrm{p}_{\\textrm{T}}^{l}$. The replicas are obtained by reweighting each observed data...","name":"Table 43 - Bootstrap norm. $p_T^{l}$"},{"@id":"https://doi.org/10.17182/hepdata.137888.v3/t45","@type":"Dataset","description":"Differential normalised cross-section for $|\\eta^{l}|$. The impact of the top-quark mass on the cross-section is included in the table and...","name":"Table 44 - Norm. $|\\eta^{l}|$"},{"@id":"https://doi.org/10.17182/hepdata.137888.v3/t46","@type":"Dataset","description":"Covariance Matrix (statistical uncertainties only) for the differential normalised cross-section for $|\\eta^{l}|$.","name":"Table 45 - Cov. Matrix norm. $|\\eta^{l}|$"},{"@id":"https://doi.org/10.17182/hepdata.137888.v3/t47","@type":"Dataset","description":"Data bootstrap post unfolding for the differential normalised cross-section for $|\\eta^{l}|$. The replicas are obtained by reweighting each observed data...","name":"Table 46 - Bootstrap norm. $|\\eta^{l}|$"},{"@id":"https://doi.org/10.17182/hepdata.137888.v3/t48","@type":"Dataset","description":"Differential normalised cross-section for $\\textrm{E}^{e} + \\textrm{E}^{\\mu}$. The impact of the top-quark mass on the cross-section is included in the...","name":"Table 47 - Norm. $E^e + E^{\\mu}$"},{"@id":"https://doi.org/10.17182/hepdata.137888.v3/t49","@type":"Dataset","description":"Covariance Matrix (statistical uncertainties only) for the differential normalised cross-section for $\\textrm{E}^{e} + \\textrm{E}^{\\mu}$. The last bin of the distribution...","name":"Table 48 - Cov. Matrix norm. $E^e + E^{\\mu}$"},{"@id":"https://doi.org/10.17182/hepdata.137888.v3/t50","@type":"Dataset","description":"Data bootstrap post unfolding for the differential normalised cross-section for $\\textrm{E}^{e} + \\textrm{E}^{\\mu}$. The replicas are obtained by reweighting each...","name":"Table 49 - Bootstrap norm. $E^e + E^{\\mu}$"},{"@id":"https://doi.org/10.17182/hepdata.137888.v3/t51","@type":"Dataset","description":"Differential normalised cross-section for $m^{e\\mu}$. The impact of the top-quark mass on the cross-section is included in the table and...","name":"Table 50 - Norm. $m^{e\\mu}$"},{"@id":"https://doi.org/10.17182/hepdata.137888.v3/t52","@type":"Dataset","description":"Covariance Matrix (statistical uncertainties only) for the differential normalised cross-section for $m^{e\\mu}$. The last bin of the distribution contains the...","name":"Table 51 - Cov. Matrix norm. $m^{e\\mu}$"},{"@id":"https://doi.org/10.17182/hepdata.137888.v3/t53","@type":"Dataset","description":"Data bootstrap post unfolding for the differential normalised cross-section for $m^{e\\mu}$. The replicas are obtained by reweighting each observed data...","name":"Table 52 - Bootstrap norm. $m^{e\\mu}$"},{"@id":"https://doi.org/10.17182/hepdata.137888.v3/t54","@type":"Dataset","description":"Differential normalised cross-section for $\\textrm{p}_{\\textrm{T}}^{e} + \\textrm{p}_{\\textrm{T}}^{\\mu}$. The impact of the top-quark mass on the cross-section is included in the...","name":"Table 53 - Norm. $p_T^{e} + p_T^{\\mu}$"},{"@id":"https://doi.org/10.17182/hepdata.137888.v3/t55","@type":"Dataset","description":"Covariance Matrix (statistical uncertainties only) for the differential normalised cross-section for $\\textrm{p}_{\\textrm{T}}^{e} + \\textrm{p}_{\\textrm{T}}^{\\mu}$. The last bin of the distribution...","name":"Table 54 - Cov. Matrix norm. $p_T^{e} + p_T^{\\mu}$"},{"@id":"https://doi.org/10.17182/hepdata.137888.v3/t56","@type":"Dataset","description":"Data bootstrap post unfolding for the differential normalised cross-section for $\\textrm{p}_{\\textrm{T}}^{e} + \\textrm{p}_{\\textrm{T}}^{\\mu}$. The replicas are obtained by reweighting each...","name":"Table 55 - Bootstrap norm. $p_T^{e} + p_T^{\\mu}$"},{"@id":"https://doi.org/10.17182/hepdata.137888.v3/t57","@type":"Dataset","description":"Differential normalised cross-section for $\\textrm{p}_{\\textrm{T}}^{e\\mu}$. The impact of the top-quark mass on the cross-section is included in the table and...","name":"Table 56 - Norm. $p_T^{e\\mu}$"},{"@id":"https://doi.org/10.17182/hepdata.137888.v3/t58","@type":"Dataset","description":"Covariance Matrix (statistical uncertainties only) for the differential normalised cross-section for $\\textrm{p}_{\\textrm{T}}^{e\\mu}$. The last bin of the distribution contains the...","name":"Table 57 - Cov. Matrix norm. $p_T^{e\\mu}$"},{"@id":"https://doi.org/10.17182/hepdata.137888.v3/t59","@type":"Dataset","description":"Data bootstrap post unfolding for the differential normalised cross-section for $\\textrm{p}_{\\textrm{T}}^{e\\mu}$. The replicas are obtained by reweighting each observed data...","name":"Table 58 - Bootstrap norm. $p_T^{e\\mu}$"},{"@id":"https://doi.org/10.17182/hepdata.137888.v3/t60","@type":"Dataset","description":"Differential normalised cross-section for $|\\Delta\\phi^{e\\mu}|$. The impact of the top-quark mass on the cross-section is included in the table and...","name":"Table 59 - Norm. $|\\Delta\\phi^{e\\mu}|$"},{"@id":"https://doi.org/10.17182/hepdata.137888.v3/t61","@type":"Dataset","description":"Covariance Matrix (statistical uncertainties only) for the differential normalised cross-section for $|\\Delta\\phi^{e\\mu}|$.","name":"Table 60 - Cov. Matrix norm. $|\\Delta\\phi^{e\\mu}|$"},{"@id":"https://doi.org/10.17182/hepdata.137888.v3/t62","@type":"Dataset","description":"Data bootstrap post unfolding for the differential normalised cross-section for $|\\Delta\\phi^{e\\mu}|$. The replicas are obtained by reweighting each observed data...","name":"Table 61 - Bootstrap norm. $|\\Delta\\phi^{e\\mu}|$"},{"@id":"https://doi.org/10.17182/hepdata.137888.v3/t63","@type":"Dataset","description":"Differential normalised cross-section for $|y^{e\\mu}|$. The impact of the top-quark mass on the cross-section is included in the table and...","name":"Table 62 - Norm. $|y^{e\\mu}|$"},{"@id":"https://doi.org/10.17182/hepdata.137888.v3/t64","@type":"Dataset","description":"Covariance Matrix (statistical uncertainties only) for the differential normalised cross-section for $|y^{e\\mu}|$.","name":"Table 63 - Cov. Matrix norm. $|y^{e\\mu}|$"},{"@id":"https://doi.org/10.17182/hepdata.137888.v3/t65","@type":"Dataset","description":"Data bootstrap post unfolding for the differential normalised cross-section for $|y^{e\\mu}|$. The replicas are obtained by reweighting each observed data...","name":"Table 64 - Bootstrap norm. $|y^{e\\mu}|$"},{"@id":"https://doi.org/10.17182/hepdata.137888.v3/t66","@type":"Dataset","description":"Double differential normalised cross-section for $|y^{e\\mu}|$ x $m^{e\\mu}$. The impact of the top-quark mass on the cross-section is included in...","name":"Table 65 - Norm. $|y^{e\\mu}|$ x $m^{e\\mu}$"},{"@id":"https://doi.org/10.17182/hepdata.137888.v3/t67","@type":"Dataset","description":"Covariance Matrix (statistical uncertainties only) for the double differential normalised cross-section for $|y^{e\\mu}|$ x $m^{e\\mu}$. The highest invariant mass bin...","name":"Table 66 - Cov. Matrix norm. $|y^{e\\mu}|$ x $m^{e\\mu}$"},{"@id":"https://doi.org/10.17182/hepdata.137888.v3/t68","@type":"Dataset","description":"Data bootstrap post unfolding for the double differential normalised cross-section for $|y^{e\\mu}|$ x $m^{e\\mu}$. The replicas are obtained by reweighting...","name":"Table 67 - Bootstrap norm. $|y^{e\\mu}|$ x $m^{e\\mu}$"},{"@id":"https://doi.org/10.17182/hepdata.137888.v3/t69","@type":"Dataset","description":"Double differential normalised cross-section for $|\\Delta\\phi^{e\\mu}|$ x $m^{e\\mu}$. The impact of the top-quark mass on the cross-section is included in...","name":"Table 68 - Norm. $|\\Delta\\phi^{e\\mu}|$ x $m^{e\\mu}$"},{"@id":"https://doi.org/10.17182/hepdata.137888.v3/t70","@type":"Dataset","description":"Covariance Matrix (statistical uncertainties only) for the double differential normalised cross-section for $|\\Delta\\phi^{e\\mu}|$ x $m^{e\\mu}$. The highest invariant mass bin...","name":"Table 69 - Cov.Mat. norm. $|\\Delta\\phi^{e\\mu}|$ x $m^{e\\mu}$"},{"@id":"https://doi.org/10.17182/hepdata.137888.v3/t71","@type":"Dataset","description":"Data bootstrap post unfolding for the double differential normalised cross-section for $|\\Delta\\phi^{e\\mu}|$ x $m^{e\\mu}$. The replicas are obtained by reweighting...","name":"Table 70 - Bootstrap norm. $|\\Delta\\phi^{e\\mu}|$ x $m^{e\\mu}$"},{"@id":"https://doi.org/10.17182/hepdata.137888.v3/t72","@type":"Dataset","description":"Double differential normalised cross-section for $|\\Delta\\phi^{e\\mu}|$ x $\\textrm{p}_{\\textrm{T}}^{e\\mu}$. The impact of the top-quark mass on the cross-section is included in...","name":"Table 71 - Norm. $|\\Delta\\phi^{e\\mu}|$ x $p_T^{e\\mu}$"},{"@id":"https://doi.org/10.17182/hepdata.137888.v3/t73","@type":"Dataset","description":"Covariance Matrix (statistical uncertainties only) for the double differential normalised cross-section for $|\\Delta\\phi^{e\\mu}|$ x $\\textrm{p}_{\\textrm{T}}^{e\\mu}$. The highest $\\textrm{p}_{\\textrm{T}}^{e\\mu}$ bin contains...","name":"Table 72 - Cov.Mat. norm. $|\\Delta\\phi^{e\\mu}|$ x $p_T^{e\\mu}$"},{"@id":"https://doi.org/10.17182/hepdata.137888.v3/t74","@type":"Dataset","description":"Data bootstrap post unfolding for the double differential normalised cross-section for $|\\Delta\\phi^{e\\mu}|$ x $\\textrm{p}_{\\textrm{T}}^{e\\mu}$. The replicas are obtained by reweighting...","name":"Table 73 - Boots. norm. $|\\Delta\\phi^{e\\mu}|$ x $p_T^{e\\mu}$"},{"@id":"https://doi.org/10.17182/hepdata.137888.v3/t75","@type":"Dataset","description":"Double differential normalised cross-section for $|\\Delta\\phi^{e\\mu}|$ x $\\textrm{E}^{e} + \\textrm{E}^{\\mu}$. The impact of the top-quark mass on the cross-section is...","name":"Table 74 - Norm. $|\\Delta\\phi^{e\\mu}|$ x $E^e + E^{\\mu}$"},{"@id":"https://doi.org/10.17182/hepdata.137888.v3/t76","@type":"Dataset","description":"Covariance Matrix (statistical uncertainties only) for the double differential normalised cross-section for $|\\Delta\\phi^{e\\mu}|$ x $\\textrm{E}^{e} + \\textrm{E}^{\\mu}$. The highest $\\textrm{E}^{e}...","name":"Table 75 - Cov.M. norm $|\\Delta\\phi^{e\\mu}|$ x $E^{e}+E^{\\mu}$"},{"@id":"https://doi.org/10.17182/hepdata.137888.v3/t77","@type":"Dataset","description":"Data bootstrap post unfolding for the double differential normalised cross-section for $|\\Delta\\phi^{e\\mu}|$ x $\\textrm{E}^{e} + \\textrm{E}^{\\mu}$. 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