cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.66683.v2/t95
title: "Table 95" of "Measurements of the W production cross sections in association with jets with the ATLAS detector"

description: Breakdown of systematic uncertainties in percent in ST [GeV] with exactly three jets in the event in the electron channel.Uncertainties have been symmetrised and the sign denotes the sign of the original up-variation.
description: CERN-LHC.

This paper presents cross sections for the production of a W boson in association with jets, measured in proton--proton collisions at sqrt(s)=7 TeV with the ATLAS experiment at the Large Hadron Collider. With an integrated luminosity of 4.6 fb^{-1}, this data set allows for an exploration of a large kinematic range, including jet production up to a transverse momentum of 1 TeV and multiplicities up to seven associated jets. The production cross sections for W bosons are measured in both the electron and muon decay channels. Differential cross sections for many observables are also presented including measurements of the jet observables such as the rapidities and the transverse momenta as well as measurements of event observables such as the scalar sums of the transverse momenta of the jets. The measurements are compared to numerous QCD predictions including next-to-leading-order perturbative calculations, resummation calculations and Monte Carlo generators

Note added (27 OCT 2015): 
The bin ranges in the DeltaPhi table were incorrectly rounded. This has been fixed.
DOI: 10.17182/hepdata.66683.v2/t96
title: "Table 96" of "Measurements of the W production cross sections in association with jets with the ATLAS detector"

description: Breakdown of systematic uncertainties in percent in ST [GeV] with exactly three jets in the event in the muon channel.Uncertainties have been symmetrised and the sign denotes the sign of the original up-variation.
description: CERN-LHC.

This paper presents cross sections for the production of a W boson in association with jets, measured in proton--proton collisions at sqrt(s)=7 TeV with the ATLAS experiment at the Large Hadron Collider. With an integrated luminosity of 4.6 fb^{-1}, this data set allows for an exploration of a large kinematic range, including jet production up to a transverse momentum of 1 TeV and multiplicities up to seven associated jets. The production cross sections for W bosons are measured in both the electron and muon decay channels. Differential cross sections for many observables are also presented including measurements of the jet observables such as the rapidities and the transverse momenta as well as measurements of event observables such as the scalar sums of the transverse momenta of the jets. The measurements are compared to numerous QCD predictions including next-to-leading-order perturbative calculations, resummation calculations and Monte Carlo generators

Note added (27 OCT 2015): 
The bin ranges in the DeltaPhi table were incorrectly rounded. This has been fixed.
DOI: 10.17182/hepdata.66683.v2/t97
title: "Table 97" of "Measurements of the W production cross sections in association with jets with the ATLAS detector"

description: Distribution of ST [GeV] with at least four jets in the event.
description: CERN-LHC.

This paper presents cross sections for the production of a W boson in association with jets, measured in proton--proton collisions at sqrt(s)=7 TeV with the ATLAS experiment at the Large Hadron Collider. With an integrated luminosity of 4.6 fb^{-1}, this data set allows for an exploration of a large kinematic range, including jet production up to a transverse momentum of 1 TeV and multiplicities up to seven associated jets. The production cross sections for W bosons are measured in both the electron and muon decay channels. Differential cross sections for many observables are also presented including measurements of the jet observables such as the rapidities and the transverse momenta as well as measurements of event observables such as the scalar sums of the transverse momenta of the jets. The measurements are compared to numerous QCD predictions including next-to-leading-order perturbative calculations, resummation calculations and Monte Carlo generators

Note added (27 OCT 2015): 
The bin ranges in the DeltaPhi table were incorrectly rounded. This has been fixed.
DOI: 10.17182/hepdata.66683.v2/t98
title: "Table 98" of "Measurements of the W production cross sections in association with jets with the ATLAS detector"

description: Breakdown of systematic uncertainties in percent in ST [GeV] with at least four jets in the event in the electron channel.Uncertainties have been symmetrised and the sign denotes the sign of the original up-variation.
description: CERN-LHC.

This paper presents cross sections for the production of a W boson in association with jets, measured in proton--proton collisions at sqrt(s)=7 TeV with the ATLAS experiment at the Large Hadron Collider. With an integrated luminosity of 4.6 fb^{-1}, this data set allows for an exploration of a large kinematic range, including jet production up to a transverse momentum of 1 TeV and multiplicities up to seven associated jets. The production cross sections for W bosons are measured in both the electron and muon decay channels. Differential cross sections for many observables are also presented including measurements of the jet observables such as the rapidities and the transverse momenta as well as measurements of event observables such as the scalar sums of the transverse momenta of the jets. The measurements are compared to numerous QCD predictions including next-to-leading-order perturbative calculations, resummation calculations and Monte Carlo generators

Note added (27 OCT 2015): 
The bin ranges in the DeltaPhi table were incorrectly rounded. This has been fixed.
DOI: 10.17182/hepdata.66683.v2/t99
title: "Table 99" of "Measurements of the W production cross sections in association with jets with the ATLAS detector"

description: Breakdown of systematic uncertainties in percent in ST [GeV] with at least four jets in the event in the muon channel.Uncertainties have been symmetrised and the sign denotes the sign of the original up-variation.
description: CERN-LHC.

This paper presents cross sections for the production of a W boson in association with jets, measured in proton--proton collisions at sqrt(s)=7 TeV with the ATLAS experiment at the Large Hadron Collider. With an integrated luminosity of 4.6 fb^{-1}, this data set allows for an exploration of a large kinematic range, including jet production up to a transverse momentum of 1 TeV and multiplicities up to seven associated jets. The production cross sections for W bosons are measured in both the electron and muon decay channels. Differential cross sections for many observables are also presented including measurements of the jet observables such as the rapidities and the transverse momenta as well as measurements of event observables such as the scalar sums of the transverse momenta of the jets. The measurements are compared to numerous QCD predictions including next-to-leading-order perturbative calculations, resummation calculations and Monte Carlo generators

Note added (27 OCT 2015): 
The bin ranges in the DeltaPhi table were incorrectly rounded. This has been fixed.
DOI: 10.17182/hepdata.66683.v2/t101
title: "Table 101" of "Measurements of the W production cross sections in association with jets with the ATLAS detector"

description: Breakdown of systematic uncertainties in percent in ST [GeV] with at least five jets in the event in the electron channel.Uncertainties have been symmetrised and the sign denotes the sign of the original up-variation.
description: CERN-LHC.

This paper presents cross sections for the production of a W boson in association with jets, measured in proton--proton collisions at sqrt(s)=7 TeV with the ATLAS experiment at the Large Hadron Collider. With an integrated luminosity of 4.6 fb^{-1}, this data set allows for an exploration of a large kinematic range, including jet production up to a transverse momentum of 1 TeV and multiplicities up to seven associated jets. The production cross sections for W bosons are measured in both the electron and muon decay channels. Differential cross sections for many observables are also presented including measurements of the jet observables such as the rapidities and the transverse momenta as well as measurements of event observables such as the scalar sums of the transverse momenta of the jets. The measurements are compared to numerous QCD predictions including next-to-leading-order perturbative calculations, resummation calculations and Monte Carlo generators

Note added (27 OCT 2015): 
The bin ranges in the DeltaPhi table were incorrectly rounded. This has been fixed.
DOI: 10.17182/hepdata.66683.v2/t102
title: "Table 102" of "Measurements of the W production cross sections in association with jets with the ATLAS detector"

description: Breakdown of systematic uncertainties in percent in ST [GeV] with at least five jets in the event in the muon channel.Uncertainties have been symmetrised and the sign denotes the sign of the original up-variation.
description: CERN-LHC.

This paper presents cross sections for the production of a W boson in association with jets, measured in proton--proton collisions at sqrt(s)=7 TeV with the ATLAS experiment at the Large Hadron Collider. With an integrated luminosity of 4.6 fb^{-1}, this data set allows for an exploration of a large kinematic range, including jet production up to a transverse momentum of 1 TeV and multiplicities up to seven associated jets. The production cross sections for W bosons are measured in both the electron and muon decay channels. Differential cross sections for many observables are also presented including measurements of the jet observables such as the rapidities and the transverse momenta as well as measurements of event observables such as the scalar sums of the transverse momenta of the jets. The measurements are compared to numerous QCD predictions including next-to-leading-order perturbative calculations, resummation calculations and Monte Carlo generators

Note added (27 OCT 2015): 
The bin ranges in the DeltaPhi table were incorrectly rounded. This has been fixed.
DOI: 10.17182/hepdata.66704.v1/t1
title: "Table 1" of "Measurement of the $WW+WZ$ cross section and limits on anomalous triple gauge couplings using final states with one lepton, missing transverse momentum, and two jets with the ATLAS detector at $\sqrt{\rm{s}} = 7$ TeV"

description: The total and fiducial cross sections for the production of W(LEPTON NU) W(JET JET)
or W(LEPTON NU) Z(JET JET). The cross sections are the sum of the WW and WZ processes.
description: CERN-LHC. The production of a W boson decaying to (e nu) or (mu nu) in association with a W or Z boson decaying to two jets is studied using 4.6 fb-1 of proton-proton collision data at sqrt(s) = 7 TeV recorded with the ATLAS detector at the LHC. The combined WW+WZ cross section is measured with a significance of 3.4 sigma. Two cross sections are measured, a fiducial and a total cross section. The cross sections are measured assuming the SM ratio between the WW and WZ cross sections.

The fiducial cross section is measured for the combined WW+WZ process, with the di-bosons decaying to 
(lepton nu jet jet), summed over the (e nu) and (mu nu) channels, in the following fiducial region:
pT of lepton &gt; 25 GeV
eta of lepton: |eta|&lt;2.47
Transverse mass of leptonically-decaying W: mT&gt;40 GeV
Two jets with pT&gt;25 GeV and |eta|&lt;2.0, with |DeltaR(jet,lepton)|&gt;0.5. Leading-pT jet must have pT&gt;30 GeV. 
Veto events with more than 2 jets having pT&gt;25 GeV and |eta|&lt;2.8.
MET&gt;30 GeV
The two selected jets must have |eta(j1,j2)|&lt;1.5
Dijet-mass must satisify: 250.7
Azimuthal angle between MET direction and leading-pT jet: |DeltaPhi(MET,j1)|&gt;0.8

In the fiducial region definition, the jets are generator-level jets, reconstructed from all stable particles excluding the decay products from leptonically-decaying W/Z bosons, using the anti-kT algorithm with R=0.4. The MET is defined as the momentum of the neutrino from the leptonically-decaying W.

A total WW+WZ cross section measurement is also quoted, which is extrapolated from the fiducial region to the full WW+WZ phase-space.
DOI: 10.17182/hepdata.66742.v1/t1
title: "Table 1" of "Charged particle nuclear modification factor and pseudorapidity asymmetry in pPb collisions at sqrt(sNN)=5.02 TeV with CMS"

description: Invariant charged particle differential yield.
description: CERN-LHC. Transverse momentum spectra of charged particles are measured by the CMS experiment at the CERN LHC in pPb collisions at sqrt(s[NN]) =5.02 TeV, in the range 0.4 &lt; pt &lt; 120 GeVc and pseudorapidity abs(eta[CM]) &lt; 1.8 in the proton-nucleon center-of-mass frame, with the convention that the incoming proton travels in the positive eta[CM] direction.

The charged particle yields reported in the tables are given as per double-sided event yields, where double-sided events are defined as a collision producing at least one particle in the pseudorapidity range -5 &lt; eta[LAB] &lt; -3 and another in the range 3 &lt; eta[LAB] &lt; 5, each with proper lifetime tau &gt; 10^-18 s and energy E &gt; 3 GeV (see See Eur.Phys.J. C74 (2014) 2847). The data are corrected for the finite bin-width effect. 

A pp reference spectrum at sqrt(s) = 5.02 TeV is obtained by interpolation from previous measurements at higher and lower center-of-mass energies, and is used to determine the nuclear modification factor for abs(eta[CM]) &lt; 1.0. Note that the uncertainty of 4.8 percent in the Glauber calculation of the nuclear thickness function, T_pPb, is not included in the total systematic uncertainty quoted in the table. 

The forward-backward asymmetry of the yields for A &lt; abs(eta[CM]) &lt; B is defined as the ratio of the differential charged particle yield integrated over the range -B &lt; eta[CM] &lt; -A (Pb-going side) to the differential charged particle yield integrated over the range A &lt; eta[CM] &lt; B (p-going side). This quantity is measured for three ranges: 0.3 &lt; abs(eta[CM]) &lt; 0.8, 0.8 &lt; abs(eta[CM]) &lt; 1.3, and 1.3 &lt; abs(eta[CM]) &lt; 1.8.
DOI: 10.17182/hepdata.66742.v1/t2
title: "Table 2" of "Charged particle nuclear modification factor and pseudorapidity asymmetry in pPb collisions at sqrt(sNN)=5.02 TeV with CMS"

description: Invariant charged particle differential yield.
description: CERN-LHC. Transverse momentum spectra of charged particles are measured by the CMS experiment at the CERN LHC in pPb collisions at sqrt(s[NN]) =5.02 TeV, in the range 0.4 &lt; pt &lt; 120 GeVc and pseudorapidity abs(eta[CM]) &lt; 1.8 in the proton-nucleon center-of-mass frame, with the convention that the incoming proton travels in the positive eta[CM] direction.

The charged particle yields reported in the tables are given as per double-sided event yields, where double-sided events are defined as a collision producing at least one particle in the pseudorapidity range -5 &lt; eta[LAB] &lt; -3 and another in the range 3 &lt; eta[LAB] &lt; 5, each with proper lifetime tau &gt; 10^-18 s and energy E &gt; 3 GeV (see See Eur.Phys.J. C74 (2014) 2847). The data are corrected for the finite bin-width effect. 

A pp reference spectrum at sqrt(s) = 5.02 TeV is obtained by interpolation from previous measurements at higher and lower center-of-mass energies, and is used to determine the nuclear modification factor for abs(eta[CM]) &lt; 1.0. Note that the uncertainty of 4.8 percent in the Glauber calculation of the nuclear thickness function, T_pPb, is not included in the total systematic uncertainty quoted in the table. 

The forward-backward asymmetry of the yields for A &lt; abs(eta[CM]) &lt; B is defined as the ratio of the differential charged particle yield integrated over the range -B &lt; eta[CM] &lt; -A (Pb-going side) to the differential charged particle yield integrated over the range A &lt; eta[CM] &lt; B (p-going side). This quantity is measured for three ranges: 0.3 &lt; abs(eta[CM]) &lt; 0.8, 0.8 &lt; abs(eta[CM]) &lt; 1.3, and 1.3 &lt; abs(eta[CM]) &lt; 1.8.
DOI: 10.17182/hepdata.66742.v1/t3
title: "Table 3" of "Charged particle nuclear modification factor and pseudorapidity asymmetry in pPb collisions at sqrt(sNN)=5.02 TeV with CMS"

description: Invariant charged particle differential yield.
description: CERN-LHC. Transverse momentum spectra of charged particles are measured by the CMS experiment at the CERN LHC in pPb collisions at sqrt(s[NN]) =5.02 TeV, in the range 0.4 &lt; pt &lt; 120 GeVc and pseudorapidity abs(eta[CM]) &lt; 1.8 in the proton-nucleon center-of-mass frame, with the convention that the incoming proton travels in the positive eta[CM] direction.

The charged particle yields reported in the tables are given as per double-sided event yields, where double-sided events are defined as a collision producing at least one particle in the pseudorapidity range -5 &lt; eta[LAB] &lt; -3 and another in the range 3 &lt; eta[LAB] &lt; 5, each with proper lifetime tau &gt; 10^-18 s and energy E &gt; 3 GeV (see See Eur.Phys.J. C74 (2014) 2847). The data are corrected for the finite bin-width effect. 

A pp reference spectrum at sqrt(s) = 5.02 TeV is obtained by interpolation from previous measurements at higher and lower center-of-mass energies, and is used to determine the nuclear modification factor for abs(eta[CM]) &lt; 1.0. Note that the uncertainty of 4.8 percent in the Glauber calculation of the nuclear thickness function, T_pPb, is not included in the total systematic uncertainty quoted in the table. 

The forward-backward asymmetry of the yields for A &lt; abs(eta[CM]) &lt; B is defined as the ratio of the differential charged particle yield integrated over the range -B &lt; eta[CM] &lt; -A (Pb-going side) to the differential charged particle yield integrated over the range A &lt; eta[CM] &lt; B (p-going side). This quantity is measured for three ranges: 0.3 &lt; abs(eta[CM]) &lt; 0.8, 0.8 &lt; abs(eta[CM]) &lt; 1.3, and 1.3 &lt; abs(eta[CM]) &lt; 1.8.
DOI: 10.17182/hepdata.66742.v1/t4
title: "Table 4" of "Charged particle nuclear modification factor and pseudorapidity asymmetry in pPb collisions at sqrt(sNN)=5.02 TeV with CMS"

description: Invariant charged particle differential yield.
description: CERN-LHC. Transverse momentum spectra of charged particles are measured by the CMS experiment at the CERN LHC in pPb collisions at sqrt(s[NN]) =5.02 TeV, in the range 0.4 &lt; pt &lt; 120 GeVc and pseudorapidity abs(eta[CM]) &lt; 1.8 in the proton-nucleon center-of-mass frame, with the convention that the incoming proton travels in the positive eta[CM] direction.

The charged particle yields reported in the tables are given as per double-sided event yields, where double-sided events are defined as a collision producing at least one particle in the pseudorapidity range -5 &lt; eta[LAB] &lt; -3 and another in the range 3 &lt; eta[LAB] &lt; 5, each with proper lifetime tau &gt; 10^-18 s and energy E &gt; 3 GeV (see See Eur.Phys.J. C74 (2014) 2847). The data are corrected for the finite bin-width effect. 

A pp reference spectrum at sqrt(s) = 5.02 TeV is obtained by interpolation from previous measurements at higher and lower center-of-mass energies, and is used to determine the nuclear modification factor for abs(eta[CM]) &lt; 1.0. Note that the uncertainty of 4.8 percent in the Glauber calculation of the nuclear thickness function, T_pPb, is not included in the total systematic uncertainty quoted in the table. 

The forward-backward asymmetry of the yields for A &lt; abs(eta[CM]) &lt; B is defined as the ratio of the differential charged particle yield integrated over the range -B &lt; eta[CM] &lt; -A (Pb-going side) to the differential charged particle yield integrated over the range A &lt; eta[CM] &lt; B (p-going side). This quantity is measured for three ranges: 0.3 &lt; abs(eta[CM]) &lt; 0.8, 0.8 &lt; abs(eta[CM]) &lt; 1.3, and 1.3 &lt; abs(eta[CM]) &lt; 1.8.
DOI: 10.17182/hepdata.66742.v1/t5
title: "Table 5" of "Charged particle nuclear modification factor and pseudorapidity asymmetry in pPb collisions at sqrt(sNN)=5.02 TeV with CMS"

description: Invariant charged particle differential yield.
description: CERN-LHC. Transverse momentum spectra of charged particles are measured by the CMS experiment at the CERN LHC in pPb collisions at sqrt(s[NN]) =5.02 TeV, in the range 0.4 &lt; pt &lt; 120 GeVc and pseudorapidity abs(eta[CM]) &lt; 1.8 in the proton-nucleon center-of-mass frame, with the convention that the incoming proton travels in the positive eta[CM] direction.

The charged particle yields reported in the tables are given as per double-sided event yields, where double-sided events are defined as a collision producing at least one particle in the pseudorapidity range -5 &lt; eta[LAB] &lt; -3 and another in the range 3 &lt; eta[LAB] &lt; 5, each with proper lifetime tau &gt; 10^-18 s and energy E &gt; 3 GeV (see See Eur.Phys.J. C74 (2014) 2847). The data are corrected for the finite bin-width effect. 

A pp reference spectrum at sqrt(s) = 5.02 TeV is obtained by interpolation from previous measurements at higher and lower center-of-mass energies, and is used to determine the nuclear modification factor for abs(eta[CM]) &lt; 1.0. Note that the uncertainty of 4.8 percent in the Glauber calculation of the nuclear thickness function, T_pPb, is not included in the total systematic uncertainty quoted in the table. 

The forward-backward asymmetry of the yields for A &lt; abs(eta[CM]) &lt; B is defined as the ratio of the differential charged particle yield integrated over the range -B &lt; eta[CM] &lt; -A (Pb-going side) to the differential charged particle yield integrated over the range A &lt; eta[CM] &lt; B (p-going side). This quantity is measured for three ranges: 0.3 &lt; abs(eta[CM]) &lt; 0.8, 0.8 &lt; abs(eta[CM]) &lt; 1.3, and 1.3 &lt; abs(eta[CM]) &lt; 1.8.
DOI: 10.17182/hepdata.66742.v1/t6
title: "Table 6" of "Charged particle nuclear modification factor and pseudorapidity asymmetry in pPb collisions at sqrt(sNN)=5.02 TeV with CMS"

description: Invariant charged particle differential yield.
description: CERN-LHC. Transverse momentum spectra of charged particles are measured by the CMS experiment at the CERN LHC in pPb collisions at sqrt(s[NN]) =5.02 TeV, in the range 0.4 &lt; pt &lt; 120 GeVc and pseudorapidity abs(eta[CM]) &lt; 1.8 in the proton-nucleon center-of-mass frame, with the convention that the incoming proton travels in the positive eta[CM] direction.

The charged particle yields reported in the tables are given as per double-sided event yields, where double-sided events are defined as a collision producing at least one particle in the pseudorapidity range -5 &lt; eta[LAB] &lt; -3 and another in the range 3 &lt; eta[LAB] &lt; 5, each with proper lifetime tau &gt; 10^-18 s and energy E &gt; 3 GeV (see See Eur.Phys.J. C74 (2014) 2847). The data are corrected for the finite bin-width effect. 

A pp reference spectrum at sqrt(s) = 5.02 TeV is obtained by interpolation from previous measurements at higher and lower center-of-mass energies, and is used to determine the nuclear modification factor for abs(eta[CM]) &lt; 1.0. Note that the uncertainty of 4.8 percent in the Glauber calculation of the nuclear thickness function, T_pPb, is not included in the total systematic uncertainty quoted in the table. 

The forward-backward asymmetry of the yields for A &lt; abs(eta[CM]) &lt; B is defined as the ratio of the differential charged particle yield integrated over the range -B &lt; eta[CM] &lt; -A (Pb-going side) to the differential charged particle yield integrated over the range A &lt; eta[CM] &lt; B (p-going side). This quantity is measured for three ranges: 0.3 &lt; abs(eta[CM]) &lt; 0.8, 0.8 &lt; abs(eta[CM]) &lt; 1.3, and 1.3 &lt; abs(eta[CM]) &lt; 1.8.