{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.151815.v2","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/2771257"}},{"@id":"https://doi.org/10.1140/epjc/s10052-024-13159-w","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2025","description":"This paper presents a measurement of the production cross-section of a $Z$ boson in association with $b$- and $c$-jets,     in proton-proton collisions at $\\sqrt{s} = 13$ TeV with the ATLAS experiment at the Large Hadron Collider     using data corresponding to an integrated luminosity of 140 fb$^{-1}$, i.e. full Run 2 statistics. Inclusive and differential     cross-sections are measured for events containing a $Z$ boson decaying into electrons or muons and produced in association with     at least one $b-$ or $c$-jets or at least two $b$-jets with transverse momentum $p_T > 20$ Ge and rapidity $|y|<2.5$.     Predictions from several Monte Carlo generators based on leading-order (LO) or next-to-leading-order (NLO) matrix elements     interfaced with a parton-shower simulation and testing different flavour schemes for the choice of initial-state partons are     compared with measured cross-sections alongside innovative fixed order with next-to-next-to-leading-order precision predictions     with IRC safe algorithms.     N.B.: Data correspond to average of electron and muon channel.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.151815.v2/t1","@type":"Dataset","description":"Figure 6(left) of the article. Measured fiducial cross sections for events with $Z \\left( \\rightarrow \\ell \\ell \\right) \\geq 1...","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.151815.v2/t2","@type":"Dataset","description":"Figure 6(right) of the article. Measured fiducial cross sections for events with $Z \\left( \\rightarrow \\ell \\ell \\right) \\geq 2...","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.151815.v2/t3","@type":"Dataset","description":"Figure 7 of the article. Measured fiducial cross sections for events with $Z \\left( \\rightarrow \\ell \\ell \\right) \\geq 1...","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.151815.v2/t4","@type":"Dataset","description":"Figure 8(left) of the article. Differential fiducial cross-section of the Z boson $p_T$ in events with $Z \\left( \\rightarrow \\ell\\ell...","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.151815.v2/t5","@type":"Dataset","description":"Figure 8(right) of the article. Differential fiducial cross-section of the leading $b$-jet $p_T$ in events with $Z \\left( \\rightarrow \\ell\\ell...","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.151815.v2/t6","@type":"Dataset","description":"Figure 9 of the article. Differential fiducial cross-section of the $\\Delta R$ between the $Z$ boson and the leading $b$-jet...","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.151815.v2/t7","@type":"Dataset","description":"Figure 10(left) of the article. Differential fiducial cross-section of the $\\Delta \\phi$ between the leading and sub-leading $b$-jets in events...","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.151815.v2/t8","@type":"Dataset","description":"Figure 10(right) of the article. Differential fiducial cross-section of the invariant mass of the leading and sub-leading $b$-jets in events...","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.151815.v2/t9","@type":"Dataset","description":"Figure 11(left) of the article. Differential fiducial cross-section of the Z boson $p_T$ in events with $Z \\left( \\rightarrow \\ell\\ell...","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.151815.v2/t10","@type":"Dataset","description":"Figure 11(right) of the article. Differential fiducial cross-section of the leading $c$-jet $p_T$ in events with $Z \\left( \\rightarrow \\ell\\ell...","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.151815.v2/t11","@type":"Dataset","description":"Figure 12 of the article. Differential fiducial cross-section of the leading $c$-jet $x_F$ in events with $Z \\left( \\rightarrow \\ell\\ell...","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.151815.v2/t12","@type":"Dataset","description":"Correction factors from parton level done with flavour dressing algorithms as seen in Ref. [2] of the paper to hadron...","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.151815.v2/t13","@type":"Dataset","description":"Correction factors from parton level done with flavour dressing algorithms as seen in Ref. [2] of the paper to hadron...","name":"Table 13"},{"@id":"https://doi.org/10.17182/hepdata.151815.v2/t14","@type":"Dataset","description":"Correction factors from parton level done with flavour dressing algorithms as seen in Ref. [2] of the paper to hadron...","name":"Table 14"},{"@id":"https://doi.org/10.17182/hepdata.151815.v2/t15","@type":"Dataset","description":"Correction factors from parton level done with flavour dressing algorithms as seen in Ref. [2] of the paper to hadron...","name":"Table 15"},{"@id":"https://doi.org/10.17182/hepdata.151815.v2/t16","@type":"Dataset","description":"Correction factors from parton level done with flavour dressing algorithms as seen in Ref. 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