cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.151815.v1/t14
title: "Table 14" of "Measurements of the production cross-section for a $Z$ boson in association with $b$- or $c$-jets in proton-proton collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Correction factors from parton level done with flavour dressing algorithms as seen in Ref. [2] of the paper to hadron level with R 0.3 cone labelling (see Tables 20 & 26) for the differential cross-section of the leading $b$-jet $p_T$ in events with $Z (\rightarrow ll) \ge 1 $ b-jets. Systematic errors include Sherpa 2.2.11 and MGaMC+Py8 FxFx uncertainties for what concerns the passage from hadron level flavour dressing to hadron level cone labelling, plus statistical uncertainty of Pythia8 simulations used for parton to hadron corrections. See Table 5.
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 $p_T &gt; 20$ Ge and rapidity $|y|&lt;2.5$. 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.
DOI: 10.17182/hepdata.151815.v1/t15
title: "Table 15" of "Measurements of the production cross-section for a $Z$ boson in association with $b$- or $c$-jets in proton-proton collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Correction factors from parton level done with flavour dressing algorithms as seen in Ref. [2] of the paper to hadron level with R 0.3 cone labelling (see Tables 21 & 27) for the differential cross-section of the leading $c$-jet $p_T$ in events with $Z (\rightarrow ll) \ge 1 $ c-jets. Systematic errors include Sherpa 2.2.11 and MGaMC+Py8 FxFx uncertainties for what concerns the passage from hadron level flavour dressing to hadron level cone labelling, plus statistical uncertainty of Pythia8 simulations used for parton to hadron corrections. See Table 10.
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 $p_T &gt; 20$ Ge and rapidity $|y|&lt;2.5$. 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.
DOI: 10.17182/hepdata.151815.v1/t17
title: "Table 17" of "Measurements of the production cross-section for a $Z$ boson in association with $b$- or $c$-jets in proton-proton collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Correction factors from parton level done with flavour dressing algorithms as seen in Ref. [2] of the paper of the paper to hadron level with R 0.3 cone labelling (see Tables 23 & 29) for the differential cross-section of $\Delta R$ between the $Z$ boson and the leading $b$-jet in events with $Z (\rightarrow ll) \ge 1 $ b-jets. Systematic errors include Sherpa 2.2.11 and MGaMC+Py8 FxFx uncertainties for what concerns the passage from hadron level flavour dressing to hadron level cone labelling, plus statistical uncertainty of Pythia8 simulations used for parton to hadron corrections. See Table 6.
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 $p_T &gt; 20$ Ge and rapidity $|y|&lt;2.5$. 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.
DOI: 10.17182/hepdata.151815.v1/t18
title: "Table 18" of "Measurements of the production cross-section for a $Z$ boson in association with $b$- or $c$-jets in proton-proton collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Correction factors from hadron level done with flavour dressing algorithms as seen in Ref. [2] of the paper to hadron level R 0.3 cone labelling for the differential cross-section of the Z boson $p_T$ in events with $Z (\rightarrow ll) \ge 1 $ b-jets. Systematic errors include Sherpa 2.2.11 and MGaMC+Py8 FxFx uncertainties. See Table 12.
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 $p_T &gt; 20$ Ge and rapidity $|y|&lt;2.5$. 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.
DOI: 10.17182/hepdata.151815.v1/t16
title: "Table 16" of "Measurements of the production cross-section for a $Z$ boson in association with $b$- or $c$-jets in proton-proton collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Correction factors from parton level done with flavour dressing algorithms as seen in Ref. [2] of the paper to hadron level with R 0.3 cone labelling (see Tables 22 & 28) for the differential cross-section of the leading $c$-jet $x_F$ in events with $Z (\rightarrow ll) \ge 1 $ c-jets. Systematic errors include Sherpa 2.2.11 and MGaMC+Py8 FxFx uncertainties for what concerns the passage from hadron level flavour dressing to hadron level cone labelling, plus statistical uncertainty of Pythia8 simulations used for parton to hadron corrections. See Table 11.
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 $p_T &gt; 20$ Ge and rapidity $|y|&lt;2.5$. 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.
DOI: 10.17182/hepdata.151815.v1/t19
title: "Table 19" of "Measurements of the production cross-section for a $Z$ boson in association with $b$- or $c$-jets in proton-proton collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Correction factors from hadron level done with flavour dressing algorithms as seen in Ref. [2] of the paper to hadron level with R 0.3 cone labelling for the differential cross-section of the Z boson $p_T$ in events with $Z (\rightarrow ll) \ge 1 $ c-jets. Systematic errors include Sherpa 2.2.11 and MGaMC+Py8 FxFx uncertainties. See Table 13.
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 $p_T &gt; 20$ Ge and rapidity $|y|&lt;2.5$. 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.
DOI: 10.17182/hepdata.151815.v1/t20
title: "Table 20" of "Measurements of the production cross-section for a $Z$ boson in association with $b$- or $c$-jets in proton-proton collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Correction factors from hadron level done with flavour dressing algorithms as seen in Ref. [2] of the paper to hadron level with R 0.3 cone labelling for the differential cross-section of the leading $b$-jet $p_T$ in events with $Z (\rightarrow ll) \ge 1 $ b-jets. Systematic errors include Sherpa 2.2.11 and MGaMC+Py8 FxFx uncertainties. See Table 14.
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 $p_T &gt; 20$ Ge and rapidity $|y|&lt;2.5$. 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.
DOI: 10.17182/hepdata.151815.v1/t21
title: "Table 21" of "Measurements of the production cross-section for a $Z$ boson in association with $b$- or $c$-jets in proton-proton collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Correction factors from hadron level done with flavour dressing algorithms as seen in Ref. [2] of the paper to hadron level with R 0.3 cone labelling for the differential cross-section of the leading $c$-jet $p_T$ in events with $Z (\rightarrow ll) \ge 1 $ c-jets. Systematic errors include Sherpa 2.2.11 and MGaMC+Py8 FxFx uncertainties. See Table 15.
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 $p_T &gt; 20$ Ge and rapidity $|y|&lt;2.5$. 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.
DOI: 10.17182/hepdata.151815.v1/t22
title: "Table 22" of "Measurements of the production cross-section for a $Z$ boson in association with $b$- or $c$-jets in proton-proton collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Correction factors from hadron level done with flavour dressing algorithms as seen in Ref. [2] of the paper to hadron level with R 0.3 cone labelling for the differential cross-section of the leading $c$-jet $x_F$ in events with $Z (\rightarrow ll) \ge 1 $ c-jets. Systematic errors include Sherpa 2.2.11 and MGaMC+Py8 FxFx uncertainties. See Table 16.
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 $p_T &gt; 20$ Ge and rapidity $|y|&lt;2.5$. 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.
DOI: 10.17182/hepdata.151815.v1/t23
title: "Table 23" of "Measurements of the production cross-section for a $Z$ boson in association with $b$- or $c$-jets in proton-proton collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Correction factors from hadron level done with flavour dressing algorithms as seen in Ref. [2] of the paper of the paper to hadron level with R 0.3 cone labelling for the differential cross-section of $\Delta R$ between the $Z$ boson and the leading $b$-jet in events with $Z (\rightarrow ll) \ge 1 $ b-jets. Systematic errors include Sherpa 2.2.11 and MGaMC+Py8 FxFx uncertainties. See Table 17.
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 $p_T &gt; 20$ Ge and rapidity $|y|&lt;2.5$. 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.
DOI: 10.17182/hepdata.151815.v1/t24
title: "Table 24" of "Measurements of the production cross-section for a $Z$ boson in association with $b$- or $c$-jets in proton-proton collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Correction factors from parton level to hadron level for the differential cross-section of the Z boson $p_T$ in events with $Z (\rightarrow ll) \ge 1 $ b-jets. Systematic errors statistical uncertainty of Pythia8 simulations. See Table 12.
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 $p_T &gt; 20$ Ge and rapidity $|y|&lt;2.5$. 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.
DOI: 10.17182/hepdata.151815.v1/t25
title: "Table 25" of "Measurements of the production cross-section for a $Z$ boson in association with $b$- or $c$-jets in proton-proton collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Correction factors from parton level to hadron level for the differential cross-section of the Z boson $p_T$ in events with $Z (\rightarrow ll) \ge 1 $ c-jets. Systematic errors include statistical uncertainty of Pythia8 simulations. See Table 13.
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 $p_T &gt; 20$ Ge and rapidity $|y|&lt;2.5$. 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.
DOI: 10.17182/hepdata.151815.v1/t26
title: "Table 26" of "Measurements of the production cross-section for a $Z$ boson in association with $b$- or $c$-jets in proton-proton collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Correction factors from parton level to hadron level for the differential cross-section of the leading $b$-jet $p_T$ in events with $Z (\rightarrow ll) \ge 1 $ b-jets. Systematic errors include statistical uncertainty of Pythia8 simulations. See Table 14.
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 $p_T &gt; 20$ Ge and rapidity $|y|&lt;2.5$. 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.
DOI: 10.17182/hepdata.151815.v1/t27
title: "Table 27" of "Measurements of the production cross-section for a $Z$ boson in association with $b$- or $c$-jets in proton-proton collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Correction factors from parton level to hadron level for the differential cross-section of the leading $c$-jet $p_T$ in events with $Z (\rightarrow ll) \ge 1 $ c-jets. Systematic errors include statistical uncertainty of Pythia8 simulations. See Table 15.
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 $p_T &gt; 20$ Ge and rapidity $|y|&lt;2.5$. 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.