cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.151815.v2/t1
title: "Table 1" 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: Figure 6(left) of the article. Measured fiducial cross sections for events with $Z \left( \rightarrow \ell \ell \right) \geq 1 b$-jet. The thin inner band corresponds to the statistical uncertainty of the data, and the outer band to statistical and systematic uncertainties of the data, added in quadrature.
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.v2/t2
title: "Table 2" 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: Figure 6(right) of the article. Measured fiducial cross sections for events with $Z \left( \rightarrow \ell \ell \right) \geq 2 b$-jets. The thin inner band corresponds to the statistical uncertainty of the data, and the outer band to statistical and systematic uncertainties of the data, added in quadrature.
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.v2/t3
title: "Table 3" 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: Figure 7 of the article. Measured fiducial cross sections for events with $Z \left( \rightarrow \ell \ell \right) \geq 1 c$-jet. The thin inner band corresponds to the statistical uncertainty of the data, and the outer band to statistical and systematic uncertainties of the data, added in quadrature.
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.v2/t4
title: "Table 4" 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: Figure 8(left) of the article. Differential fiducial cross-section of the Z boson $p_T$ in events with $Z \left( \rightarrow \ell\ell \right) + 1 b$-jet. The thin inner band corresponds to the statistical uncertainty of the data, and the outer band to statistical and systematic uncertainties of the data, added in quadrature.
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.v2/t5
title: "Table 5" 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: Figure 8(right) of the article. Differential fiducial cross-section of the leading $b$-jet $p_T$ in events with $Z \left( \rightarrow \ell\ell \right) + 1 b$-jet. The thin inner band corresponds to the statistical uncertainty of the data, and the outer band to statistical and systematic uncertainties of the data, added in quadrature.
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.v2/t6
title: "Table 6" 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: Figure 9 of the article. Differential fiducial cross-section of the $\Delta R$ between the $Z$ boson and the leading $b$-jet in events with $Z \left( \rightarrow \ell\ell \right) + 1 b$-jet. The thin inner band corresponds to the statistical uncertainty of the data, and the outer band to statistical and systematic uncertainties of the data, added in quadrature.
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.v2/t7
title: "Table 7" 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: Figure 10(left) of the article. Differential fiducial cross-section of the $\Delta \phi$ between the leading and sub-leading $b$-jets in events with $Z \left( \rightarrow \ell\ell \right) + 2 b$-jets. The thin inner band corresponds to the statistical uncertainty of the data, and the outer band to statistical and systematic uncertainties of the data, added in quadrature.
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.v2/t8
title: "Table 8" 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: Figure 10(right) of the article. Differential fiducial cross-section of the invariant mass of the leading and sub-leading $b$-jets in events with $Z \left( \rightarrow \ell\ell \right) + 2 b$-jets. The thin inner band corresponds to the statistical uncertainty of the data, and the outer band to statistical and systematic uncertainties of the data, added in quadrature.
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.v2/t9
title: "Table 9" 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: Figure 11(left) of the article. Differential fiducial cross-section of the Z boson $p_T$ in events with $Z \left( \rightarrow \ell\ell \right) + 1 c$-jet. The thin inner band corresponds to the statistical uncertainty of the data, and the outer band to statistical and systematic uncertainties of the data, added in quadrature.
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.v2/t10
title: "Table 10" 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: Figure 11(right) of the article. Differential fiducial cross-section of the leading $c$-jet $p_T$ in events with $Z \left( \rightarrow \ell\ell 
ight) + 1 c$-jet. The thin inner band corresponds to the statistical uncertainty of the data, and the outer band to statistical and systematic uncertainties of the data, added in quadrature.
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.v2/t11
title: "Table 11" 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: Figure 12 of the article. Differential fiducial cross-section of the leading $c$-jet $x_F$ in events with $Z \left( \rightarrow \ell\ell \right) + 1 c$-jet. The thin inner band corresponds to the statistical uncertainty of the data, and the outer band to statistical and systematic uncertainties of the data, added in quadrature.
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.v2/t12
title: "Table 12" 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 18 & 24) 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 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 4.
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.v2/t13
title: "Table 13" 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 19 & 25) 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 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 9.
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.v2/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.