cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.158827.v1/t1
title: "Figure 3" of "Measurement of elliptic flow of J$/\psi$ in $\sqrt{s_{_{NN}}}=200$ GeV Au$+$Au collisions at forward rapidity"

description: JPSI v2 in Au+Au collisions as a function of pT (GeV/c) for 10%--60% centrality with pT binned by [0, 1], [1, 2], [2, 3], and [3, 5] GeV/c.
description: BNL-RHIC. We report the first measurement of the azimuthal anisotropy of J$/\psi$ at forward rapidity ($1.2&lt;|\eta|&lt;2.2$) in Au$+$Au collisions at $\sqrt{s_{_{NN}}}=200$ GeV at the Relativistic Heavy Ion Collider. The data were collected by the PHENIX experiment in 2014 and 2016 with integrated luminosity of 14.5~nb$^{-1}$. The second Fourier coefficient ($v_2$) of the azimuthal distribution of $J/\psi$ is determined as a function of the transverse momentum ($p_T$) using the event-plane method. The measurements were performed for several selections of collision centrality: 0\%--50\%, 10\%--60\%, and 10\%--40\%. We find that in all cases the values of $v_2(p_T)$, which quantify the elliptic flow of J$/\psi$, are consistent with zero. The results are consistent with measurements at midrapidity, indicating no significant elliptic flow of the J$/\psi$ within the quark-gluon-plasma medium at collision energies of $\sqrt{s_{_{NN}}}=200$ GeV.
DOI: 10.17182/hepdata.158827.v1/t2
title: "Figure 4" of "Measurement of elliptic flow of J$/\psi$ in $\sqrt{s_{_{NN}}}=200$ GeV Au$+$Au collisions at forward rapidity"

description: JPSI v2 in Au+Au collisions as a function of pT (GeV/c) for 10%--60% centrality with pT binned by [0, 0.5], [0.5, 1], [1, 5], and [0, 5] GeV/c.
description: BNL-RHIC. We report the first measurement of the azimuthal anisotropy of J$/\psi$ at forward rapidity ($1.2&lt;|\eta|&lt;2.2$) in Au$+$Au collisions at $\sqrt{s_{_{NN}}}=200$ GeV at the Relativistic Heavy Ion Collider. The data were collected by the PHENIX experiment in 2014 and 2016 with integrated luminosity of 14.5~nb$^{-1}$. The second Fourier coefficient ($v_2$) of the azimuthal distribution of $J/\psi$ is determined as a function of the transverse momentum ($p_T$) using the event-plane method. The measurements were performed for several selections of collision centrality: 0\%--50\%, 10\%--60\%, and 10\%--40\%. We find that in all cases the values of $v_2(p_T)$, which quantify the elliptic flow of J$/\psi$, are consistent with zero. The results are consistent with measurements at midrapidity, indicating no significant elliptic flow of the J$/\psi$ within the quark-gluon-plasma medium at collision energies of $\sqrt{s_{_{NN}}}=200$ GeV.
DOI: 10.17182/hepdata.158827.v1/t3
title: "Figure 6" of "Measurement of elliptic flow of J$/\psi$ in $\sqrt{s_{_{NN}}}=200$ GeV Au$+$Au collisions at forward rapidity"

description: JPSI v2 in Au+Au collisions as a function of pT (GeV/c) for 10%--40% centrality with pT binned by [0, 2], [2, 5], and [5, 10] GeV/c.
description: BNL-RHIC. We report the first measurement of the azimuthal anisotropy of J$/\psi$ at forward rapidity ($1.2&lt;|\eta|&lt;2.2$) in Au$+$Au collisions at $\sqrt{s_{_{NN}}}=200$ GeV at the Relativistic Heavy Ion Collider. The data were collected by the PHENIX experiment in 2014 and 2016 with integrated luminosity of 14.5~nb$^{-1}$. The second Fourier coefficient ($v_2$) of the azimuthal distribution of $J/\psi$ is determined as a function of the transverse momentum ($p_T$) using the event-plane method. The measurements were performed for several selections of collision centrality: 0\%--50\%, 10\%--60\%, and 10\%--40\%. We find that in all cases the values of $v_2(p_T)$, which quantify the elliptic flow of J$/\psi$, are consistent with zero. The results are consistent with measurements at midrapidity, indicating no significant elliptic flow of the J$/\psi$ within the quark-gluon-plasma medium at collision energies of $\sqrt{s_{_{NN}}}=200$ GeV.
DOI: 10.17182/hepdata.158827.v1/t4
title: "Figure 7" of "Measurement of elliptic flow of J$/\psi$ in $\sqrt{s_{_{NN}}}=200$ GeV Au$+$Au collisions at forward rapidity"

description: JPSI v2 in Au+Au collisions as a function of pT (GeV/c) for 10%--40% centrality with pT binned by [0, 2], [2, 5], and [5, 10] GeV/c.
description: BNL-RHIC. We report the first measurement of the azimuthal anisotropy of J$/\psi$ at forward rapidity ($1.2&lt;|\eta|&lt;2.2$) in Au$+$Au collisions at $\sqrt{s_{_{NN}}}=200$ GeV at the Relativistic Heavy Ion Collider. The data were collected by the PHENIX experiment in 2014 and 2016 with integrated luminosity of 14.5~nb$^{-1}$. The second Fourier coefficient ($v_2$) of the azimuthal distribution of $J/\psi$ is determined as a function of the transverse momentum ($p_T$) using the event-plane method. The measurements were performed for several selections of collision centrality: 0\%--50\%, 10\%--60\%, and 10\%--40\%. We find that in all cases the values of $v_2(p_T)$, which quantify the elliptic flow of J$/\psi$, are consistent with zero. The results are consistent with measurements at midrapidity, indicating no significant elliptic flow of the J$/\psi$ within the quark-gluon-plasma medium at collision energies of $\sqrt{s_{_{NN}}}=200$ GeV.
DOI: 10.17182/hepdata.159243.v1/t1
title: "Figure 02a" of "Cross-section measurements for the production of a $W$-boson in association with high-transverse-momentum jets in $pp$ collisions at $\sqrt{s}$= 13 TeV with the ATLAS detector"

description: Differential distributions at reconstruction level in the (a, c) electron or (b, d) muon channel for (a, b) inclusive and (c, d) collinear signal regions
after the application of the background normalisation factors.
The signal process is stacked above all background predictions.
The bottom panel shows the ratio of the data to the total signal plus background prediction.
The shaded band includes statistical and systematic uncertainties from signal and background processes added in quadrature.
description: A set of measurements for the production of a $W$-boson in association with high-transverse-momentum jets is presented using 140 fb$^{-1}$ of proton-proton collision data at a centre-of-mass energy of $\sqrt{s}=13$ TeV collected by the ATLAS detector at the LHC. The measurements are performed in final states in which the $W$-boson decays into an electron or muon plus a neutrino and is produced in association with jets with $p_{\text{T}}&gt;30$ GeV, where the leading jet has $p_{\text{T}}&gt;500$ GeV. The angular separation between the lepton and the closest jet with $p_{\text{T}}&gt;100$ GeV is measured and used to define a collinear phase space, wherein measurements of kinematic properties of the $W$-boson and the associated jet are performed. The collinear phase space is populated by dijet events radiating a $W$-boson and events with a $W$-boson produced in association with several jets and it serves as an excellent data sample to probe higher-order theoretical predictions. Measured differential distributions are compared with predictions from state-of-the-art next-to-leading order multi-leg merged Monte Carlo event generators and a fixed-order calculation of the $W$+1-jet process computed at next-to-next-to-leading order in the strong coupling constant.
DOI: 10.17182/hepdata.159243.v1/t2
title: "Figure 02b" of "Cross-section measurements for the production of a $W$-boson in association with high-transverse-momentum jets in $pp$ collisions at $\sqrt{s}$= 13 TeV with the ATLAS detector"

description: Differential distributions at reconstruction level in the (a, c) electron or (b, d) muon channel for (a, b) inclusive and (c, d) collinear signal regions
after the application of the background normalisation factors.
The signal process is stacked above all background predictions.
The bottom panel shows the ratio of the data to the total signal plus background prediction.
The shaded band includes statistical and systematic uncertainties from signal and background processes added in quadrature.
description: A set of measurements for the production of a $W$-boson in association with high-transverse-momentum jets is presented using 140 fb$^{-1}$ of proton-proton collision data at a centre-of-mass energy of $\sqrt{s}=13$ TeV collected by the ATLAS detector at the LHC. The measurements are performed in final states in which the $W$-boson decays into an electron or muon plus a neutrino and is produced in association with jets with $p_{\text{T}}&gt;30$ GeV, where the leading jet has $p_{\text{T}}&gt;500$ GeV. The angular separation between the lepton and the closest jet with $p_{\text{T}}&gt;100$ GeV is measured and used to define a collinear phase space, wherein measurements of kinematic properties of the $W$-boson and the associated jet are performed. The collinear phase space is populated by dijet events radiating a $W$-boson and events with a $W$-boson produced in association with several jets and it serves as an excellent data sample to probe higher-order theoretical predictions. Measured differential distributions are compared with predictions from state-of-the-art next-to-leading order multi-leg merged Monte Carlo event generators and a fixed-order calculation of the $W$+1-jet process computed at next-to-next-to-leading order in the strong coupling constant.
DOI: 10.17182/hepdata.159243.v1/t3
title: "Figure 03b" of "Cross-section measurements for the production of a $W$-boson in association with high-transverse-momentum jets in $pp$ collisions at $\sqrt{s}$= 13 TeV with the ATLAS detector"

description: Relative systematic uncertainties in the averaged cross-section for various differential distributions in the (a, b) inclusive and (c, d) collinear phase spaces.
The upper solid line shows the total uncertainty in the measured cross-section in data,
and includes correlations between the systematic components.
The 'Others' category contains sub-dominant uncertainties arising from missing transverse momentum reconstruction and the jet-to-vertex fraction uncertainties.
description: A set of measurements for the production of a $W$-boson in association with high-transverse-momentum jets is presented using 140 fb$^{-1}$ of proton-proton collision data at a centre-of-mass energy of $\sqrt{s}=13$ TeV collected by the ATLAS detector at the LHC. The measurements are performed in final states in which the $W$-boson decays into an electron or muon plus a neutrino and is produced in association with jets with $p_{\text{T}}&gt;30$ GeV, where the leading jet has $p_{\text{T}}&gt;500$ GeV. The angular separation between the lepton and the closest jet with $p_{\text{T}}&gt;100$ GeV is measured and used to define a collinear phase space, wherein measurements of kinematic properties of the $W$-boson and the associated jet are performed. The collinear phase space is populated by dijet events radiating a $W$-boson and events with a $W$-boson produced in association with several jets and it serves as an excellent data sample to probe higher-order theoretical predictions. Measured differential distributions are compared with predictions from state-of-the-art next-to-leading order multi-leg merged Monte Carlo event generators and a fixed-order calculation of the $W$+1-jet process computed at next-to-next-to-leading order in the strong coupling constant.
DOI: 10.17182/hepdata.159243.v1/t4
title: "Figure 03a" of "Cross-section measurements for the production of a $W$-boson in association with high-transverse-momentum jets in $pp$ collisions at $\sqrt{s}$= 13 TeV with the ATLAS detector"

description: Relative systematic uncertainties in the averaged cross-section for various differential distributions in the (a, b) inclusive and (c, d) collinear phase spaces.
The upper solid line shows the total uncertainty in the measured cross-section in data,
and includes correlations between the systematic components.
The 'Others' category contains sub-dominant uncertainties arising from missing transverse momentum reconstruction and the jet-to-vertex fraction uncertainties.
description: A set of measurements for the production of a $W$-boson in association with high-transverse-momentum jets is presented using 140 fb$^{-1}$ of proton-proton collision data at a centre-of-mass energy of $\sqrt{s}=13$ TeV collected by the ATLAS detector at the LHC. The measurements are performed in final states in which the $W$-boson decays into an electron or muon plus a neutrino and is produced in association with jets with $p_{\text{T}}&gt;30$ GeV, where the leading jet has $p_{\text{T}}&gt;500$ GeV. The angular separation between the lepton and the closest jet with $p_{\text{T}}&gt;100$ GeV is measured and used to define a collinear phase space, wherein measurements of kinematic properties of the $W$-boson and the associated jet are performed. The collinear phase space is populated by dijet events radiating a $W$-boson and events with a $W$-boson produced in association with several jets and it serves as an excellent data sample to probe higher-order theoretical predictions. Measured differential distributions are compared with predictions from state-of-the-art next-to-leading order multi-leg merged Monte Carlo event generators and a fixed-order calculation of the $W$+1-jet process computed at next-to-next-to-leading order in the strong coupling constant.
DOI: 10.17182/hepdata.159243.v1/t5
title: "Figure 05b" of "Cross-section measurements for the production of a $W$-boson in association with high-transverse-momentum jets in $pp$ collisions at $\sqrt{s}$= 13 TeV with the ATLAS detector"

description: Differential cross-section measurement in the inclusive phase space as function of (a) the
minimum angular separation between the lepton and any jet with transverse momentum greater than 100 GeV (ΔR <sub>min</sub>(ℓ,jet<sup>100</sup><sub>i</sub>)), and
(b) the ratio of W p<sub>T</sub> to the closest-jet p<sub>T</sub> (p<sub>T</sub><sup>ℓν</sup> / p<sub>T</sub><sup>closest jet</sup>).
The measured cross-sections in data and their statistical uncertainty are shown by the solid dots and error bars,
while the shaded band shows the systematic and statistical uncertainties added in quadrature.
Errors bars on the theory prediction include theoretical uncertainties as discussed in the text.
The bins around p<sub>T</sub><sup>ℓν</sup> / p<sub>T</sub><sup>closest jet</sup> equal to 1 are merged to be insensitive to the singularity that exists
in the fixed-order MCFM calculation.
Additionally, in (b), the central two bins from the MCFM prediction are merged due to a singularity in fixed-order calculations, which requires p<sub>T</sub> resummation of the W + jets system.
The two lower panels show the effect of NLO EW<sub>virt</sub> as computed from Sherpa 2.2.11.
description: A set of measurements for the production of a $W$-boson in association with high-transverse-momentum jets is presented using 140 fb$^{-1}$ of proton-proton collision data at a centre-of-mass energy of $\sqrt{s}=13$ TeV collected by the ATLAS detector at the LHC. The measurements are performed in final states in which the $W$-boson decays into an electron or muon plus a neutrino and is produced in association with jets with $p_{\text{T}}&gt;30$ GeV, where the leading jet has $p_{\text{T}}&gt;500$ GeV. The angular separation between the lepton and the closest jet with $p_{\text{T}}&gt;100$ GeV is measured and used to define a collinear phase space, wherein measurements of kinematic properties of the $W$-boson and the associated jet are performed. The collinear phase space is populated by dijet events radiating a $W$-boson and events with a $W$-boson produced in association with several jets and it serves as an excellent data sample to probe higher-order theoretical predictions. Measured differential distributions are compared with predictions from state-of-the-art next-to-leading order multi-leg merged Monte Carlo event generators and a fixed-order calculation of the $W$+1-jet process computed at next-to-next-to-leading order in the strong coupling constant.
DOI: 10.17182/hepdata.159243.v1/t6
title: "Figure 05a" of "Cross-section measurements for the production of a $W$-boson in association with high-transverse-momentum jets in $pp$ collisions at $\sqrt{s}$= 13 TeV with the ATLAS detector"

description: Differential cross-section measurement in the inclusive phase space as function of (a) the
minimum angular separation between the lepton and any jet with transverse momentum greater than 100 GeV (ΔR <sub>min</sub>(ℓ,jet<sup>100</sup><sub>i</sub>)), and
(b) the ratio of W p<sub>T</sub> to the closest-jet p<sub>T</sub> (p<sub>T</sub><sup>ℓν</sup> / p<sub>T</sub><sup>closest jet</sup>).
The measured cross-sections in data and their statistical uncertainty are shown by the solid dots and error bars,
while the shaded band shows the systematic and statistical uncertainties added in quadrature.
Errors bars on the theory prediction include theoretical uncertainties as discussed in the text.
The bins around p<sub>T</sub><sup>ℓν</sup> / p<sub>T</sub><sup>closest jet</sup> equal to 1 are merged to be insensitive to the singularity that exists
in the fixed-order MCFM calculation.
Additionally, in (b), the central two bins from the MCFM prediction are merged due to a singularity in fixed-order calculations, which requires p<sub>T</sub> resummation of the W + jets system.
The two lower panels show the effect of NLO EW<sub>virt</sub> as computed from Sherpa 2.2.11.
description: A set of measurements for the production of a $W$-boson in association with high-transverse-momentum jets is presented using 140 fb$^{-1}$ of proton-proton collision data at a centre-of-mass energy of $\sqrt{s}=13$ TeV collected by the ATLAS detector at the LHC. The measurements are performed in final states in which the $W$-boson decays into an electron or muon plus a neutrino and is produced in association with jets with $p_{\text{T}}&gt;30$ GeV, where the leading jet has $p_{\text{T}}&gt;500$ GeV. The angular separation between the lepton and the closest jet with $p_{\text{T}}&gt;100$ GeV is measured and used to define a collinear phase space, wherein measurements of kinematic properties of the $W$-boson and the associated jet are performed. The collinear phase space is populated by dijet events radiating a $W$-boson and events with a $W$-boson produced in association with several jets and it serves as an excellent data sample to probe higher-order theoretical predictions. Measured differential distributions are compared with predictions from state-of-the-art next-to-leading order multi-leg merged Monte Carlo event generators and a fixed-order calculation of the $W$+1-jet process computed at next-to-next-to-leading order in the strong coupling constant.
DOI: 10.17182/hepdata.159243.v1/t7
title: "Figure 06" of "Cross-section measurements for the production of a $W$-boson in association with high-transverse-momentum jets in $pp$ collisions at $\sqrt{s}$= 13 TeV with the ATLAS detector"

description: Differential cross-section as a function of the invariant mass of the leading two jets (m<sub>jj</sub>) in the inclusive, 2-jet phase space.
The measured cross-sections in data and their statistical uncertainty are shown by the solid dots and error bars,
while the shaded band shows the systematic and statistical uncertainties added in quadrature.
Errors bars on the theory prediction include theoretical uncertainties as discussed in the text.
The two lower panels show the effect of NLO EW<sub>virt</sub> as computed from Sherpa 2.2.11.
description: A set of measurements for the production of a $W$-boson in association with high-transverse-momentum jets is presented using 140 fb$^{-1}$ of proton-proton collision data at a centre-of-mass energy of $\sqrt{s}=13$ TeV collected by the ATLAS detector at the LHC. The measurements are performed in final states in which the $W$-boson decays into an electron or muon plus a neutrino and is produced in association with jets with $p_{\text{T}}&gt;30$ GeV, where the leading jet has $p_{\text{T}}&gt;500$ GeV. The angular separation between the lepton and the closest jet with $p_{\text{T}}&gt;100$ GeV is measured and used to define a collinear phase space, wherein measurements of kinematic properties of the $W$-boson and the associated jet are performed. The collinear phase space is populated by dijet events radiating a $W$-boson and events with a $W$-boson produced in association with several jets and it serves as an excellent data sample to probe higher-order theoretical predictions. Measured differential distributions are compared with predictions from state-of-the-art next-to-leading order multi-leg merged Monte Carlo event generators and a fixed-order calculation of the $W$+1-jet process computed at next-to-next-to-leading order in the strong coupling constant.
DOI: 10.17182/hepdata.159243.v1/t8
title: "Figure 02c" of "Cross-section measurements for the production of a $W$-boson in association with high-transverse-momentum jets in $pp$ collisions at $\sqrt{s}$= 13 TeV with the ATLAS detector"

description: Differential distributions at reconstruction level in the (a, c) electron or (b, d) muon channel for (a, b) inclusive and (c, d) collinear signal regions
after the application of the background normalisation factors.
The signal process is stacked above all background predictions.
The bottom panel shows the ratio of the data to the total signal plus background prediction.
The shaded band includes statistical and systematic uncertainties from signal and background processes added in quadrature.
description: A set of measurements for the production of a $W$-boson in association with high-transverse-momentum jets is presented using 140 fb$^{-1}$ of proton-proton collision data at a centre-of-mass energy of $\sqrt{s}=13$ TeV collected by the ATLAS detector at the LHC. The measurements are performed in final states in which the $W$-boson decays into an electron or muon plus a neutrino and is produced in association with jets with $p_{\text{T}}&gt;30$ GeV, where the leading jet has $p_{\text{T}}&gt;500$ GeV. The angular separation between the lepton and the closest jet with $p_{\text{T}}&gt;100$ GeV is measured and used to define a collinear phase space, wherein measurements of kinematic properties of the $W$-boson and the associated jet are performed. The collinear phase space is populated by dijet events radiating a $W$-boson and events with a $W$-boson produced in association with several jets and it serves as an excellent data sample to probe higher-order theoretical predictions. Measured differential distributions are compared with predictions from state-of-the-art next-to-leading order multi-leg merged Monte Carlo event generators and a fixed-order calculation of the $W$+1-jet process computed at next-to-next-to-leading order in the strong coupling constant.