cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.159243.v1/t20
title: "Aux. Figure 01b" 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 reconstructed-level comparing data with the background model in the
(a) tt̄ muon, (b) Z + jets muon, and (c) multijet electron control selections.
All backgrounds and signal samples are stacked to produce the figures.
The data points are shown as solid dots with their corresponding statistical uncertainty,
while the total background model uncertainty is shown by the shaded band.
Errors bars on the theory prediction include theoretical uncertainties as discussed in the text.
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/t21
title: "Aux. Figure 01c" 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 reconstructed-level comparing data with the background model in the
(a) tt̄ muon, (b) Z + jets muon, and (c) multijet electron control selections.
All backgrounds and signal samples are stacked to produce the figures.
The data points are shown as solid dots with their corresponding statistical uncertainty,
while the total background model uncertainty is shown by the shaded band.
Errors bars on the theory prediction include theoretical uncertainties as discussed in the text.
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/t22
title: "Aux. 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: Response matrices from the Sherpa 2.2.11 event generator for (a) ΔR <sub>min</sub>(ℓ,jet<sup>100</sup><sub>i</sub>) in the inclusive electron selection,
and (b) transverse momentum of the leading jet in the collinear muon selection. The sum of the entries in each reconstructed bin (column) are normalised to unity.
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/t23
title: "Aux. 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: Response matrices from the Sherpa 2.2.11 event generator for (a) ΔR <sub>min</sub>(ℓ,jet<sup>100</sup><sub>i</sub>) in the inclusive electron selection,
and (b) transverse momentum of the leading jet in the collinear muon selection. The sum of the entries in each reconstructed bin (column) are normalised to unity.
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.159277.v1/t1
title: "Table 1" of "System size and energy dependence of the mean transverse momentum fluctuations at the LHC"

description: Normalized transverse momentum correlator, $\sqrt{ \langle\langle \Delta p_{{\rm T}1}\Delta p_{{\rm T}2} \rangle\rangle }$$/\langle\langle p_{\rm T} \rangle\rangle $, as a function of the charged-particle multiplicity density, $\langle{\rm d}N_{\rm ch}/{\rm d}\eta \rangle$, in pp collisions at $\sqrt{s}$ = 5.02 TeV.
description: Event-by-event fluctuations of the event-wise mean transverse momentum, of charged particles produced in proton--proton (pp) collisions at $\sqrt{s}$ = 5.02 TeV, Xe--Xe collisions at $\sqrt{s_{\rm NN}}$ = 5.44 TeV, and Pb--Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV are studied using the ALICE detector based on the integral correlator. The correlator strength is found to decrease monotonically with increasing produced charged-particle multiplicity measured at mid-rapidity in all three systems. In Xe--Xe and Pb--Pb collisions, the multiplicity dependence of the correlator deviates significantly from a simple power-law scaling as well as from the predictions of the HIJING and AMPT models. The observed deviation from power-law scaling is expected from transverse radial flow in semicentral to central Xe--Xe and Pb--Pb collisions. In pp collisions, the correlation strength is also studied by classifying the events based on the transverse spherocity, $S_0$, of the particle production at midrapidity, used as a proxy for the presence of a pronounced back-to-back jet topology. Low-spherocity (jetty) events feature a larger correlation strength than those with high spherocity (isotropic). The strength and multiplicity dependence of jetty and isotropic events are well reproduced by calculations with the PYTHIA 8 and EPOS LHC models.
DOI: 10.17182/hepdata.159277.v1/t2
title: "Table 2" of "System size and energy dependence of the mean transverse momentum fluctuations at the LHC"

description: Normalized transverse momentum correlator, $\sqrt{ \langle\langle \Delta p_{{\rm T}1}\Delta p_{{\rm T}2} \rangle\rangle }$$/\langle\langle p_{\rm T} \rangle\rangle $, as a function of the charged-particle multiplicity density, $\langle{\rm d}N_{\rm ch}/{\rm d}\eta \rangle$, in Pb--Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV.
description: Event-by-event fluctuations of the event-wise mean transverse momentum, of charged particles produced in proton--proton (pp) collisions at $\sqrt{s}$ = 5.02 TeV, Xe--Xe collisions at $\sqrt{s_{\rm NN}}$ = 5.44 TeV, and Pb--Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV are studied using the ALICE detector based on the integral correlator. The correlator strength is found to decrease monotonically with increasing produced charged-particle multiplicity measured at mid-rapidity in all three systems. In Xe--Xe and Pb--Pb collisions, the multiplicity dependence of the correlator deviates significantly from a simple power-law scaling as well as from the predictions of the HIJING and AMPT models. The observed deviation from power-law scaling is expected from transverse radial flow in semicentral to central Xe--Xe and Pb--Pb collisions. In pp collisions, the correlation strength is also studied by classifying the events based on the transverse spherocity, $S_0$, of the particle production at midrapidity, used as a proxy for the presence of a pronounced back-to-back jet topology. Low-spherocity (jetty) events feature a larger correlation strength than those with high spherocity (isotropic). The strength and multiplicity dependence of jetty and isotropic events are well reproduced by calculations with the PYTHIA 8 and EPOS LHC models.
DOI: 10.17182/hepdata.159277.v1/t3
title: "Table 3" of "System size and energy dependence of the mean transverse momentum fluctuations at the LHC"

description: Normalized transverse momentum correlator, $\sqrt{ \langle\langle \Delta p_{{\rm T}1}\Delta p_{{\rm T}2} \rangle\rangle }$$/\langle\langle p_{\rm T} \rangle\rangle $, as a function of the charged-particle multiplicity density, $\langle{\rm d}N_{\rm ch}/{\rm d}\eta \rangle$, in Xe--Xe collisions at $\sqrt{s_{\rm NN}}$ = 5.44 TeV.
description: Event-by-event fluctuations of the event-wise mean transverse momentum, of charged particles produced in proton--proton (pp) collisions at $\sqrt{s}$ = 5.02 TeV, Xe--Xe collisions at $\sqrt{s_{\rm NN}}$ = 5.44 TeV, and Pb--Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV are studied using the ALICE detector based on the integral correlator. The correlator strength is found to decrease monotonically with increasing produced charged-particle multiplicity measured at mid-rapidity in all three systems. In Xe--Xe and Pb--Pb collisions, the multiplicity dependence of the correlator deviates significantly from a simple power-law scaling as well as from the predictions of the HIJING and AMPT models. The observed deviation from power-law scaling is expected from transverse radial flow in semicentral to central Xe--Xe and Pb--Pb collisions. In pp collisions, the correlation strength is also studied by classifying the events based on the transverse spherocity, $S_0$, of the particle production at midrapidity, used as a proxy for the presence of a pronounced back-to-back jet topology. Low-spherocity (jetty) events feature a larger correlation strength than those with high spherocity (isotropic). The strength and multiplicity dependence of jetty and isotropic events are well reproduced by calculations with the PYTHIA 8 and EPOS LHC models.
DOI: 10.17182/hepdata.159277.v1/t4
title: "Table 4" of "System size and energy dependence of the mean transverse momentum fluctuations at the LHC"

description: Normalized transverse momentum correlator, $\sqrt{ \langle\langle \Delta p_{{\rm T}1}\Delta p_{{\rm T}2} \rangle\rangle }/\langle\langle p_{\rm T} \rangle\rangle $, as a function of the average number of participant nucleons, $\langle{ N_{\rm part}}\rangle$, in Pb--Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV
description: Event-by-event fluctuations of the event-wise mean transverse momentum, of charged particles produced in proton--proton (pp) collisions at $\sqrt{s}$ = 5.02 TeV, Xe--Xe collisions at $\sqrt{s_{\rm NN}}$ = 5.44 TeV, and Pb--Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV are studied using the ALICE detector based on the integral correlator. The correlator strength is found to decrease monotonically with increasing produced charged-particle multiplicity measured at mid-rapidity in all three systems. In Xe--Xe and Pb--Pb collisions, the multiplicity dependence of the correlator deviates significantly from a simple power-law scaling as well as from the predictions of the HIJING and AMPT models. The observed deviation from power-law scaling is expected from transverse radial flow in semicentral to central Xe--Xe and Pb--Pb collisions. In pp collisions, the correlation strength is also studied by classifying the events based on the transverse spherocity, $S_0$, of the particle production at midrapidity, used as a proxy for the presence of a pronounced back-to-back jet topology. Low-spherocity (jetty) events feature a larger correlation strength than those with high spherocity (isotropic). The strength and multiplicity dependence of jetty and isotropic events are well reproduced by calculations with the PYTHIA 8 and EPOS LHC models.
DOI: 10.17182/hepdata.159277.v1/t10
title: "Table 10" of "System size and energy dependence of the mean transverse momentum fluctuations at the LHC"

description: Normalized transverse momentum correlator, $\sqrt{ \langle\langle \Delta p_{{\rm T}1}\Delta p_{{\rm T}2} \rangle\rangle }/\langle\langle p_{\rm T} \rangle\rangle $ as a function of the charged-particle multiplicity density for spherocity-integrated events in pp collisions at $\sqrt{s}=13$ TeV
description: Event-by-event fluctuations of the event-wise mean transverse momentum, of charged particles produced in proton--proton (pp) collisions at $\sqrt{s}$ = 5.02 TeV, Xe--Xe collisions at $\sqrt{s_{\rm NN}}$ = 5.44 TeV, and Pb--Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV are studied using the ALICE detector based on the integral correlator. The correlator strength is found to decrease monotonically with increasing produced charged-particle multiplicity measured at mid-rapidity in all three systems. In Xe--Xe and Pb--Pb collisions, the multiplicity dependence of the correlator deviates significantly from a simple power-law scaling as well as from the predictions of the HIJING and AMPT models. The observed deviation from power-law scaling is expected from transverse radial flow in semicentral to central Xe--Xe and Pb--Pb collisions. In pp collisions, the correlation strength is also studied by classifying the events based on the transverse spherocity, $S_0$, of the particle production at midrapidity, used as a proxy for the presence of a pronounced back-to-back jet topology. Low-spherocity (jetty) events feature a larger correlation strength than those with high spherocity (isotropic). The strength and multiplicity dependence of jetty and isotropic events are well reproduced by calculations with the PYTHIA 8 and EPOS LHC models.
DOI: 10.17182/hepdata.159277.v1/t5
title: "Table 5" of "System size and energy dependence of the mean transverse momentum fluctuations at the LHC"

description: Normalized transverse momentum correlator, $\sqrt{ \langle\langle \Delta p_{{\rm T}1}\Delta p_{{\rm T}2} \rangle\rangle }/\langle\langle p_{\rm T} \rangle\rangle $, as a function of the average number of participant nucleons, $\langle{ N_{\rm part}}\rangle$, in Xe--Xe collisions at $\sqrt{s_{\rm NN}}$ = 5.44 TeV
description: Event-by-event fluctuations of the event-wise mean transverse momentum, of charged particles produced in proton--proton (pp) collisions at $\sqrt{s}$ = 5.02 TeV, Xe--Xe collisions at $\sqrt{s_{\rm NN}}$ = 5.44 TeV, and Pb--Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV are studied using the ALICE detector based on the integral correlator. The correlator strength is found to decrease monotonically with increasing produced charged-particle multiplicity measured at mid-rapidity in all three systems. In Xe--Xe and Pb--Pb collisions, the multiplicity dependence of the correlator deviates significantly from a simple power-law scaling as well as from the predictions of the HIJING and AMPT models. The observed deviation from power-law scaling is expected from transverse radial flow in semicentral to central Xe--Xe and Pb--Pb collisions. In pp collisions, the correlation strength is also studied by classifying the events based on the transverse spherocity, $S_0$, of the particle production at midrapidity, used as a proxy for the presence of a pronounced back-to-back jet topology. Low-spherocity (jetty) events feature a larger correlation strength than those with high spherocity (isotropic). The strength and multiplicity dependence of jetty and isotropic events are well reproduced by calculations with the PYTHIA 8 and EPOS LHC models.
DOI: 10.17182/hepdata.159277.v1/t6
title: "Table 6" of "System size and energy dependence of the mean transverse momentum fluctuations at the LHC"

description: Normalized transverse momentum correlator, $\sqrt{ \langle\langle \Delta p_{{\rm T}1}\Delta p_{{\rm T}2} \rangle\rangle }/\langle\langle p_{\rm T} \rangle\rangle $, as a function of the average number of participant nucleons, $\langle{ N_{\rm part}}\rangle$, in Pb--Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV
description: Event-by-event fluctuations of the event-wise mean transverse momentum, of charged particles produced in proton--proton (pp) collisions at $\sqrt{s}$ = 5.02 TeV, Xe--Xe collisions at $\sqrt{s_{\rm NN}}$ = 5.44 TeV, and Pb--Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV are studied using the ALICE detector based on the integral correlator. The correlator strength is found to decrease monotonically with increasing produced charged-particle multiplicity measured at mid-rapidity in all three systems. In Xe--Xe and Pb--Pb collisions, the multiplicity dependence of the correlator deviates significantly from a simple power-law scaling as well as from the predictions of the HIJING and AMPT models. The observed deviation from power-law scaling is expected from transverse radial flow in semicentral to central Xe--Xe and Pb--Pb collisions. In pp collisions, the correlation strength is also studied by classifying the events based on the transverse spherocity, $S_0$, of the particle production at midrapidity, used as a proxy for the presence of a pronounced back-to-back jet topology. Low-spherocity (jetty) events feature a larger correlation strength than those with high spherocity (isotropic). The strength and multiplicity dependence of jetty and isotropic events are well reproduced by calculations with the PYTHIA 8 and EPOS LHC models.
DOI: 10.17182/hepdata.159277.v1/t7
title: "Table 7" of "System size and energy dependence of the mean transverse momentum fluctuations at the LHC"

description: Normalized transverse momentum correlator, $\sqrt{ \langle\langle \Delta p_{{\rm T}1}\Delta p_{{\rm T}2} \rangle\rangle }/\langle\langle p_{\rm T} \rangle\rangle $ as a function of the charged-particle multiplicity density for spherocity-integrated events in pp collisions at $\sqrt{s}=5.02$ TeV
description: Event-by-event fluctuations of the event-wise mean transverse momentum, of charged particles produced in proton--proton (pp) collisions at $\sqrt{s}$ = 5.02 TeV, Xe--Xe collisions at $\sqrt{s_{\rm NN}}$ = 5.44 TeV, and Pb--Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV are studied using the ALICE detector based on the integral correlator. The correlator strength is found to decrease monotonically with increasing produced charged-particle multiplicity measured at mid-rapidity in all three systems. In Xe--Xe and Pb--Pb collisions, the multiplicity dependence of the correlator deviates significantly from a simple power-law scaling as well as from the predictions of the HIJING and AMPT models. The observed deviation from power-law scaling is expected from transverse radial flow in semicentral to central Xe--Xe and Pb--Pb collisions. In pp collisions, the correlation strength is also studied by classifying the events based on the transverse spherocity, $S_0$, of the particle production at midrapidity, used as a proxy for the presence of a pronounced back-to-back jet topology. Low-spherocity (jetty) events feature a larger correlation strength than those with high spherocity (isotropic). The strength and multiplicity dependence of jetty and isotropic events are well reproduced by calculations with the PYTHIA 8 and EPOS LHC models.
DOI: 10.17182/hepdata.159277.v1/t8
title: "Table 8" of "System size and energy dependence of the mean transverse momentum fluctuations at the LHC"

description: Normalized transverse momentum correlator, $\sqrt{ \langle\langle \Delta p_{{\rm T}1}\Delta p_{{\rm T}2} \rangle\rangle }/\langle\langle p_{\rm T} \rangle\rangle $ as a function of the charged-particle multiplicity density for jetty events in pp collisions at $\sqrt{s}=5.02$ TeV
description: Event-by-event fluctuations of the event-wise mean transverse momentum, of charged particles produced in proton--proton (pp) collisions at $\sqrt{s}$ = 5.02 TeV, Xe--Xe collisions at $\sqrt{s_{\rm NN}}$ = 5.44 TeV, and Pb--Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV are studied using the ALICE detector based on the integral correlator. The correlator strength is found to decrease monotonically with increasing produced charged-particle multiplicity measured at mid-rapidity in all three systems. In Xe--Xe and Pb--Pb collisions, the multiplicity dependence of the correlator deviates significantly from a simple power-law scaling as well as from the predictions of the HIJING and AMPT models. The observed deviation from power-law scaling is expected from transverse radial flow in semicentral to central Xe--Xe and Pb--Pb collisions. In pp collisions, the correlation strength is also studied by classifying the events based on the transverse spherocity, $S_0$, of the particle production at midrapidity, used as a proxy for the presence of a pronounced back-to-back jet topology. Low-spherocity (jetty) events feature a larger correlation strength than those with high spherocity (isotropic). The strength and multiplicity dependence of jetty and isotropic events are well reproduced by calculations with the PYTHIA 8 and EPOS LHC models.