cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.86140.v1/t38
title: "Table 38" of "Azimuthal correlations for inclusive 2-jet, 3-jet, and 4-jet events in pp collisions at $\sqrt{s}= $ 13 TeV"

description: Normalized inclusive 4-jet cross section differential in $\Delta\phi_{2j}^{min}$ for $600 &lt; p_{T}^{max} &lt; 700$ GeV
description: CERN-LHC. CMS. Azimuthal correlations between the two jets with the largest transverse momenta $p_{T}$ in inclusive 2-, 3-, and 4-jet events are presented for several regions of the leading jet $p_{T}$ up to 4 TeV. For 3- and 4-jet scenarios, measurements of the minimum azimuthal angles between any two of the three or four leading $p_{T}$ jets are also presented. Jets are reconstructed using the infrared- and collinear-safe anti-$k_{T}$ clustering algorithm with a distance parameter $R=0.4$.
DOI: 10.17182/hepdata.86140.v1/t39
title: "Table 39" of "Azimuthal correlations for inclusive 2-jet, 3-jet, and 4-jet events in pp collisions at $\sqrt{s}= $ 13 TeV"

description: Normalized inclusive 4-jet cross section differential in $\Delta\phi_{2j}^{min}$ for $700 &lt; p_{T}^{max} &lt; 800$ GeV
description: CERN-LHC. CMS. Azimuthal correlations between the two jets with the largest transverse momenta $p_{T}$ in inclusive 2-, 3-, and 4-jet events are presented for several regions of the leading jet $p_{T}$ up to 4 TeV. For 3- and 4-jet scenarios, measurements of the minimum azimuthal angles between any two of the three or four leading $p_{T}$ jets are also presented. Jets are reconstructed using the infrared- and collinear-safe anti-$k_{T}$ clustering algorithm with a distance parameter $R=0.4$.
DOI: 10.17182/hepdata.86140.v1/t40
title: "Table 40" of "Azimuthal correlations for inclusive 2-jet, 3-jet, and 4-jet events in pp collisions at $\sqrt{s}= $ 13 TeV"

description: Normalized inclusive 4-jet cross section differential in $\Delta\phi_{2j}^{min}$ for $800 &lt; p_{T}^{max} &lt; 1000$ GeV
description: CERN-LHC. CMS. Azimuthal correlations between the two jets with the largest transverse momenta $p_{T}$ in inclusive 2-, 3-, and 4-jet events are presented for several regions of the leading jet $p_{T}$ up to 4 TeV. For 3- and 4-jet scenarios, measurements of the minimum azimuthal angles between any two of the three or four leading $p_{T}$ jets are also presented. Jets are reconstructed using the infrared- and collinear-safe anti-$k_{T}$ clustering algorithm with a distance parameter $R=0.4$.
DOI: 10.17182/hepdata.86140.v1/t41
title: "Table 41" of "Azimuthal correlations for inclusive 2-jet, 3-jet, and 4-jet events in pp collisions at $\sqrt{s}= $ 13 TeV"

description: Normalized inclusive 4-jet cross section differential in $\Delta\phi_{2j}^{min}$ for $p_{T}^{max} &gt; 1000$ GeV
description: CERN-LHC. CMS. Azimuthal correlations between the two jets with the largest transverse momenta $p_{T}$ in inclusive 2-, 3-, and 4-jet events are presented for several regions of the leading jet $p_{T}$ up to 4 TeV. For 3- and 4-jet scenarios, measurements of the minimum azimuthal angles between any two of the three or four leading $p_{T}$ jets are also presented. Jets are reconstructed using the infrared- and collinear-safe anti-$k_{T}$ clustering algorithm with a distance parameter $R=0.4$.
DOI: 10.17182/hepdata.86210.v1/t1
title: "Table 1" of "Transverse momentum spectra and nuclear modification factors of charged particles in pp, p-Pb and Pb-Pb collisions at the LHC"

description: Transverse momentum spectra of charged particles in PbPb collisions in nine centrality classes.
description: No data abstract available.
DOI: 10.17182/hepdata.86210.v1/t2
title: "Table 2" of "Transverse momentum spectra and nuclear modification factors of charged particles in pp, p-Pb and Pb-Pb collisions at the LHC"

description: Transverse momentum spectra of charged particles in PbPb collisions in nine centrality classes.
description: No data abstract available.
DOI: 10.17182/hepdata.86210.v1/t3
title: "Table 3" of "Transverse momentum spectra and nuclear modification factors of charged particles in pp, p-Pb and Pb-Pb collisions at the LHC"

description: Transverse momentum spectra of charged particles in pPb collisions.
description: No data abstract available.
DOI: 10.17182/hepdata.86210.v1/t4
title: "Table 4" of "Transverse momentum spectra and nuclear modification factors of charged particles in pp, p-Pb and Pb-Pb collisions at the LHC"

description: Transverse momentum spectra of charged particles in pp collisions.
description: No data abstract available.
DOI: 10.17182/hepdata.86210.v1/t5
title: "Table 5" of "Transverse momentum spectra and nuclear modification factors of charged particles in pp, p-Pb and Pb-Pb collisions at the LHC"

description: Ratio Data/MC
description: No data abstract available.
DOI: 10.17182/hepdata.86210.v1/t6
title: "Table 6" of "Transverse momentum spectra and nuclear modification factors of charged particles in pp, p-Pb and Pb-Pb collisions at the LHC"

description: Additional systematic error for pp data: +3.0 pct -3.0 pct
Additional systematic error for PBPB 0-5 pct data: +0.08 pct -0.08 pct
Additional systematic error for PBPB 5-10 pct data: +0.24 pct -0.24 pct
Additional systematic error for PBPB 10-20 pct data: +0.46 pct -0.46 pct
Additional systematic error for PBPB 20-30 pct data: +0.81 pct -0.81 pct
Additional systematic error for PBPB 30-40 pct data: +1.26 pct -1.26 pct
Additional systematic error for PBPB 40-50 pct data: +1.86 pct -1.86 pct
Additional systematic error for PBPB 50-60 pct data: +2.64 pct -2.64 pct
Additional systematic error for PBPB 60-70 pct data: +3.67 pct -3.67 pct
Additional systematic error for PBPB 70-80 pct data: +5.01 pct -5.01 pct.
description: No data abstract available.
DOI: 10.17182/hepdata.86210.v1/t7
title: "Table 7" of "Transverse momentum spectra and nuclear modification factors of charged particles in pp, p-Pb and Pb-Pb collisions at the LHC"

description: Additional systematic error for PBPB 0-5 pct data: +2.2 pct -2.2 pct
Additional systematic error for PBPB 5-10 pct data: +2.2 pct -2.2 pct
Additional systematic error for PBPB 10-20 pct data: +2.4 pct -2.4 pct
Additional systematic error for PBPB 20-30 pct data: +2.7 pct -2.7 pct
Additional systematic error for PBPB 30-40 pct data: +3.4 pct -3.4 pct
Additional systematic error for PBPB 40-50 pct data: +3.7 pct -3.7 pct
Additional systematic error for PBPB 50-60 pct data: +4.9 pct -4.9 pct
Additional systematic error for PBPB 60-70 pct data: +6.7 pct -6.7 pct
Additional systematic error for PBPB 70-80 pct data: +7.1 pct -7.1 pct.
description: No data abstract available.
DOI: 10.17182/hepdata.86210.v1/t8
title: "Table 8" of "Transverse momentum spectra and nuclear modification factors of charged particles in pp, p-Pb and Pb-Pb collisions at the LHC"

description: Additional systematic error for PBPB 0-5 pct data: +2.7 pct -2.7 pct
Additional systematic error for PBPB 5-10 pct data: +3.5 pct -3.5 pct
Additional systematic error for PBPB 10-20 pct data: +3.5 pct -3.5 pct
Additional systematic error for PBPB 20-30 pct data: +4.1 pct -4.1 pct
Additional systematic error for PBPB 30-40 pct data: +3.7 pct -3.7 pct
Additional systematic error for PBPB 40-50 pct data: +3.9 pct -3.9 pct
Additional systematic error for PBPB 50-60 pct data: +3.6 pct -3.6 pct
Additional systematic error for PBPB 60-70 pct data: +4.6 pct -4.6 pct
Additional systematic error for PBPB 70-80 pct data: +5.9 pct -5.9 pct.
description: No data abstract available.
DOI: 10.17182/hepdata.86210.v1/t9
title: "Table 9" of "Transverse momentum spectra and nuclear modification factors of charged particles in pp, p-Pb and Pb-Pb collisions at the LHC"

description: Additional systematic error for P-PB NSD data: +4.6 pct -4.6 pct.
description: No data abstract available.
DOI: 10.17182/hepdata.86211.v1/t1
title: "Figure 8a" of "Measurement of electroweak production of a W boson in association with two jets in proton-proton collisions at $\sqrt{s}=$ 13 TeV"

description: Transformed BDT output distribution after the event preselection, in the muon channel.
description: No data abstract available.
DOI: 10.17182/hepdata.86211.v1/t2
title: "Figure 8b" of "Measurement of electroweak production of a W boson in association with two jets in proton-proton collisions at $\sqrt{s}=$ 13 TeV"

description: Transformed BDT output distribution after the event preselection, in the electron channel.
description: No data abstract available.
DOI: 10.15468/dl.3b2w78
title: Occurrence Download

description: A dataset containing 27 species occurrences available in GBIF matching the query:
{
 "and" : [
 {
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 "PublishingCountry is Colombia",
 {
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 "Country is Colombia",
 {
 "not" : {
 "Issue" : [
 "is Country coordinate mismatch"
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 },
 "DatasetKey is one of (Registros biológicos de Amaryllidaceae y otras especies del proyecto Farma sostenible 22-211)"
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}

 The dataset includes 27 records from 1 constituent datasets; see https://api.gbif.org/v1/occurrence/download/0015474-251025141854904/datasets/export for details.
 
Data from some individual datasets included in this download may be licensed under less restrictive terms.
DOI: 10.17182/hepdata.86211.v1/t10
title: "Figure 19a" of "Measurement of electroweak production of a W boson in association with two jets in proton-proton collisions at $\sqrt{s}=$ 13 TeV"

description: Hadronic activity veto efficiencies in the signal-enriched BDT&gt; 0.95 region for the muon and electron channels combined, as a function of the leading additional jet $p_T$. The data are compared with the background-only prediction as well as background+signal with PYTHIA parton showering and background+signal with HERWIG++ parton showering. In addition, the background+signal prediction from POWHEG plus HERWIG++ parton showering is included. The uncertainty bands include only the statistical uncertainty in the prediction from simulation.
description: No data abstract available.
DOI: 10.17182/hepdata.86211.v1/t3
title: "Figure 10a" of "Measurement of electroweak production of a W boson in association with two jets in proton-proton collisions at $\sqrt{s}=$ 13 TeV"

description: Muon pT in data and SM backgrounds, and various aTGC scenarios after the event preselection, in the muon channel.
description: No data abstract available.
DOI: 10.17182/hepdata.86211.v1/t4
title: "Figure 10b" of "Measurement of electroweak production of a W boson in association with two jets in proton-proton collisions at $\sqrt{s}=$ 13 TeV"

description: Electron pT in data and SM backgrounds, and various aTGC scenarios after the event preselection, in the electron channel.
description: No data abstract available.
DOI: 10.17182/hepdata.86211.v1/t5
title: "Measured cross sections" of "Measurement of electroweak production of a W boson in association with two jets in proton-proton collisions at $\sqrt{s}=$ 13 TeV"

description: Measured cross section and signal strength, relative to the standard model expectation.
description: No data abstract available.
DOI: 10.17182/hepdata.86211.v1/t6
title: "Table 3" of "Measurement of electroweak production of a W boson in association with two jets in proton-proton collisions at $\sqrt{s}=$ 13 TeV"

description: One-dimensional limits on the ATGC EFT parameters at 95% CL.
description: No data abstract available.
DOI: 10.17182/hepdata.86211.v1/t7
title: "Table 4" of "Measurement of electroweak production of a W boson in association with two jets in proton-proton collisions at $\sqrt{s}=$ 13 TeV"

description: One-dimensional limits on the ATGC effective Lagrangian (LEP parametrization) parameters at 95% CL.
description: No data abstract available.
DOI: 10.17182/hepdata.86211.v1/t8
title: "Table 5" of "Measurement of electroweak production of a W boson in association with two jets in proton-proton collisions at $\sqrt{s}=$ 13 TeV"

description: One-dimensional limits on the ATGC EFT parameters at 95% CL from the combination of EW Wjj and EW Zjj analyses.
description: No data abstract available.
DOI: 10.17182/hepdata.86211.v1/t9
title: "Table 6" of "Measurement of electroweak production of a W boson in association with two jets in proton-proton collisions at $\sqrt{s}=$ 13 TeV"

description: One-dimensional limits on the ATGC effective Lagrangian (LEP parametrization) parameters at 95% CL from the combination of EW Wjj and EW Zjj analyses.
description: No data abstract available.
DOI: 10.17182/hepdata.86211.v1/t11
title: "Figure 19b" of "Measurement of electroweak production of a W boson in association with two jets in proton-proton collisions at $\sqrt{s}=$ 13 TeV"

description: Hadronic activity veto efficiencies in the signal-enriched BDT&gt; 0.95 region for the muon and electron channels combined, as a function of additional jet $H_T$. The data are compared with the background-only prediction as well as background+signal with PYTHIA parton showering and background+signal with HERWIG++ parton showering. In addition, the background+signal prediction from POWHEG plus HERWIG++ parton showering is included. The uncertainty bands include only the statistical uncertainty in the prediction from simulation.
description: No data abstract available.
DOI: 10.17182/hepdata.86211.v1/t12
title: "Figure 19c" of "Measurement of electroweak production of a W boson in association with two jets in proton-proton collisions at $\sqrt{s}=$ 13 TeV"

description: Hadronic activity veto efficiencies in the signal-enriched BDT&gt; 0.95 region for the muon and electron channels combined, as a function of leading soft-activity jet $p_T$. The data are compared with the background-only prediction as well as background+signal with PYTHIA parton showering and background+signal with HERWIG++ parton showering. In addition, the background+signal prediction from POWHEG plus HERWIG++ parton showering is included. The uncertainty bands include only the statistical uncertainty in the prediction from simulation.
description: No data abstract available.
DOI: 10.17182/hepdata.86211.v1/t13
title: "Figure 19d" of "Measurement of electroweak production of a W boson in association with two jets in proton-proton collisions at $\sqrt{s}=$ 13 TeV"

description: Hadronic activity veto efficiencies in the signal-enriched BDT&gt; 0.95 region for the muon and electron channels combined, as a function of soft-activity jet $H_T$. The data are compared with the background-only prediction as well as background+signal with PYTHIA parton showering and background+signal with HERWIG++ parton showering. In addition, the background+signal prediction from POWHEG plus HERWIG++ parton showering is included. The uncertainty bands include only the statistical uncertainty in the prediction from simulation.
description: No data abstract available.
DOI: 10.17182/hepdata.86228.v1/t1
title: "Table 1" of "Search for an exotic decay of the Higgs boson to a pair of light pseudoscalars in the final state with two b quarks and two $\tau$ leptons in proton-proton collisions at $\sqrt{s}=$ 13 TeV"

description: Expected and observed 95% CL upper limits on (sigma(pp-&gt;h)/sigma(pp-&gt;hSM)) * B(h -&gt; aa -&gt; bbtautau) as a function of m(a), where h(SM) is the Higgs boson of the standard model, h is the observed particle with mass of 125 GeV, and a denotes a light Higgs-like state, as obtained from the 13 TeV data.
description: CERN-LHC. The analysis searches for exotic Higgs boson decays to two light pseudoscalars, in the final state of two b quarks and two tau leptons. This signature is sensitive to the Higgs sector of the next to minimal supersymmetric standard model (NMSSM) as well as two Higgs doublet models extended with a scalar singlet (2HDM+S). The analysis is based on data from proton-proton collisions at a center-of-mass energy of 13 TeV collected with the CMS detector at the LHC, in 2016 corresponding to an integrated luminosity of 35.9 fb-1. No signal above the standard model background expectation is observed. The tables give upper limits on the cross section times branching fraction for Higgs bosons with masses between 15 and 60 GeV.
DOI: 10.17182/hepdata.86229.v1/t1
title: "Table 1" of "Charged jet cross section and fragmentation in proton-proton collisions at $\sqrt{s}$ = 7 TeV"

description: Measured charged jet differential cross sections for INEL proton-proton collisions at $\sqrt{s}$ = 7 TeV.
description: No data abstract available.
DOI: 10.17182/hepdata.86229.v1/t2
title: "Table 2" of "Charged jet cross section and fragmentation in proton-proton collisions at $\sqrt{s}$ = 7 TeV"

description: Measured charged jet differential cross section ratios for INEL proton-proton collisions at $\sqrt{s}$ = 7 TeV for $5
description: No data abstract available.
DOI: 10.17182/hepdata.86229.v1/t3
title: "Table 3" of "Charged jet cross section and fragmentation in proton-proton collisions at $\sqrt{s}$ = 7 TeV"

description: Measured charged jet differential cross section ratios for INEL proton-proton collisions at $\sqrt{s}$ = 7 TeV for $10
description: No data abstract available.
DOI: 10.17182/hepdata.86229.v1/t4
title: "Table 4" of "Charged jet cross section and fragmentation in proton-proton collisions at $\sqrt{s}$ = 7 TeV"

description: Measured charged jet differential cross section ratios for INEL proton-proton collisions at $\sqrt{s}$ = 7 TeV for $15
description: No data abstract available.
DOI: 10.17182/hepdata.86390.v1/t1
title: "Inclusive jets for $Q^2$ = 5.5-8.0 GeV$^2$" of "Measurement of Jet Production Cross Sections in Deep-inelastic $ep$ Scattering at HERA"

description: Inclusive jet cross sections measured as a function of $P_T^{\rm jet}$ for $Q^2$ = 5.5-8.0 GeV$^2$. The correction factors on the theoretical cross sections $c^{\rm had}$ are listed together with their uncertainties. The radiative correction factors $c^{\rm rad}$ are already included in the quoted cross sections. Note that the uncertainties labelled $\delta^{E_{e^\prime}}$ and $\delta^{\theta_{e^\prime}}$ in Table 6 of the paper (arXiv:1611.03421v3) should be swapped. See Table 5 of arXiv:1406.4709v2 for details of the correlation model.
description: No data abstract available.
DOI: 10.17182/hepdata.86390.v1/t2
title: "Inclusive jets for $Q^2$ = 8.0-11.0 GeV$^2$" of "Measurement of Jet Production Cross Sections in Deep-inelastic $ep$ Scattering at HERA"

description: Inclusive jet cross sections measured as a function of $P_T^{\rm jet}$ for $Q^2$ = 8.0-11.0 GeV$^2$. The correction factors on the theoretical cross sections $c^{\rm had}$ are listed together with their uncertainties. The radiative correction factors $c^{\rm rad}$ are already included in the quoted cross sections. Note that the uncertainties labelled $\delta^{E_{e^\prime}}$ and $\delta^{\theta_{e^\prime}}$ in Table 6 of the paper (arXiv:1611.03421v3) should be swapped. See Table 5 of arXiv:1406.4709v2 for details of the correlation model.
description: No data abstract available.
DOI: 10.17182/hepdata.86390.v1/t3
title: "Inclusive jets for $Q^2$ = 11.0-16.0 GeV$^2$" of "Measurement of Jet Production Cross Sections in Deep-inelastic $ep$ Scattering at HERA"

description: Inclusive jet cross sections measured as a function of $P_T^{\rm jet}$ for $Q^2$ = 11.0-16.0 GeV$^2$. The correction factors on the theoretical cross sections $c^{\rm had}$ are listed together with their uncertainties. The radiative correction factors $c^{\rm rad}$ are already included in the quoted cross sections. Note that the uncertainties labelled $\delta^{E_{e^\prime}}$ and $\delta^{\theta_{e^\prime}}$ in Table 6 of the paper (arXiv:1611.03421v3) should be swapped. See Table 5 of arXiv:1406.4709v2 for details of the correlation model.
description: No data abstract available.
DOI: 10.17182/hepdata.86390.v1/t4
title: "Inclusive jets for $Q^2$ = 16.0-22.0 GeV$^2$" of "Measurement of Jet Production Cross Sections in Deep-inelastic $ep$ Scattering at HERA"

description: Inclusive jet cross sections measured as a function of $P_T^{\rm jet}$ for $Q^2$ = 16.0-22.0 GeV$^2$. The correction factors on the theoretical cross sections $c^{\rm had}$ are listed together with their uncertainties. The radiative correction factors $c^{\rm rad}$ are already included in the quoted cross sections. Note that the uncertainties labelled $\delta^{E_{e^\prime}}$ and $\delta^{\theta_{e^\prime}}$ in Table 6 of the paper (arXiv:1611.03421v3) should be swapped. See Table 5 of arXiv:1406.4709v2 for details of the correlation model.
description: No data abstract available.
DOI: 10.17182/hepdata.86390.v1/t5
title: "Inclusive jets for $Q^2$ = 22.0-30.0 GeV$^2$" of "Measurement of Jet Production Cross Sections in Deep-inelastic $ep$ Scattering at HERA"

description: Inclusive jet cross sections measured as a function of $P_T^{\rm jet}$ for $Q^2$ = 22.0-30.0 GeV$^2$. The correction factors on the theoretical cross sections $c^{\rm had}$ are listed together with their uncertainties. The radiative correction factors $c^{\rm rad}$ are already included in the quoted cross sections. Note that the uncertainties labelled $\delta^{E_{e^\prime}}$ and $\delta^{\theta_{e^\prime}}$ in Table 6 of the paper (arXiv:1611.03421v3) should be swapped. See Table 5 of arXiv:1406.4709v2 for details of the correlation model.
description: No data abstract available.
DOI: 10.17182/hepdata.86390.v1/t6
title: "Inclusive jets for $Q^2$ = 30.0-42.0 GeV$^2$" of "Measurement of Jet Production Cross Sections in Deep-inelastic $ep$ Scattering at HERA"

description: Inclusive jet cross sections measured as a function of $P_T^{\rm jet}$ for $Q^2$ = 30.0-42.0 GeV$^2$. The correction factors on the theoretical cross sections $c^{\rm had}$ are listed together with their uncertainties. The radiative correction factors $c^{\rm rad}$ are already included in the quoted cross sections. Note that the uncertainties labelled $\delta^{E_{e^\prime}}$ and $\delta^{\theta_{e^\prime}}$ in Table 6 of the paper (arXiv:1611.03421v3) should be swapped. See Table 5 of arXiv:1406.4709v2 for details of the correlation model.
description: No data abstract available.
DOI: 10.17182/hepdata.86390.v1/t7
title: "Inclusive jets for $Q^2$ = 42.0-60.0 GeV$^2$" of "Measurement of Jet Production Cross Sections in Deep-inelastic $ep$ Scattering at HERA"

description: Inclusive jet cross sections measured as a function of $P_T^{\rm jet}$ for $Q^2$ = 42.0-60.0 GeV$^2$. The correction factors on the theoretical cross sections $c^{\rm had}$ are listed together with their uncertainties. The radiative correction factors $c^{\rm rad}$ are already included in the quoted cross sections. Note that the uncertainties labelled $\delta^{E_{e^\prime}}$ and $\delta^{\theta_{e^\prime}}$ in Table 6 of the paper (arXiv:1611.03421v3) should be swapped. See Table 5 of arXiv:1406.4709v2 for details of the correlation model.
description: No data abstract available.
DOI: 10.17182/hepdata.86390.v1/t8
title: "Inclusive jets for $Q^2$ = 60.0-80.0 GeV$^2$" of "Measurement of Jet Production Cross Sections in Deep-inelastic $ep$ Scattering at HERA"

description: Inclusive jet cross sections measured as a function of $P_T^{\rm jet}$ for $Q^2$ = 60.0-80.0 GeV$^2$. The correction factors on the theoretical cross sections $c^{\rm had}$ are listed together with their uncertainties. The radiative correction factors $c^{\rm rad}$ are already included in the quoted cross sections. Note that the uncertainties labelled $\delta^{E_{e^\prime}}$ and $\delta^{\theta_{e^\prime}}$ in Table 6 of the paper (arXiv:1611.03421v3) should be swapped. See Table 5 of arXiv:1406.4709v2 for details of the correlation model.
description: No data abstract available.
DOI: 10.17182/hepdata.86390.v1/t9
title: "Dijets for $Q^2$ = 5.5-8.0 GeV$^2$" of "Measurement of Jet Production Cross Sections in Deep-inelastic $ep$ Scattering at HERA"

description: Dijet cross sections measured as a function of $\langle P_T \rangle_2$ for $Q^2$ = 5.5-8.0 GeV$^2$. The correction factors on the theoretical cross sections $c^{\rm had}$ are listed together with their uncertainties. The radiative correction factors $c^{\rm rad}$ are already included in the quoted cross sections. Note that the uncertainties labelled $\delta^{E_{e^\prime}}$ and $\delta^{\theta_{e^\prime}}$ in Table 7 of the paper (arXiv:1611.03421v3) should be swapped. See Table 5 of arXiv:1406.4709v2 for details of the correlation model.
description: No data abstract available.