cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.82624.v1/t3
title: "Table 3" of "Measurement of quarkonium production in proton--lead and proton--proton collisions at $5.02$ $\mathrm{TeV}$ with the ATLAS detector"

description: Summary of results for cross-section of prompt J/psi decaying to a muon pair in pp collisions at 5.02 TeV in nb/GeV. Uncertainties are statistical and systematic, respectively.
description: CERN-LHC. The modification of the production of J/psi psi(2S), and Upsilon(nS) (n = 1, 2, 3) in p+Pb collisions with respect to their production in pp collisions has been studied. The p+Pb and pp datasets used in this paper correspond to integrated luminosities of 28 nb^-1 and 25 pb^-1 respectively, collected in 2013 and 2015 by the ATLAS detector at the LHC, both at a centre-of-mass energy per nucleon pair of 5.02 TeV. .
DOI: 10.17182/hepdata.82624.v1/t4
title: "Table 4" of "Measurement of quarkonium production in proton--lead and proton--proton collisions at $5.02$ $\mathrm{TeV}$ with the ATLAS detector"

description: Summary of results for cross-section of prompt psi(2S) decaying to a muon pair in pp collisions at 5.02 TeV in nb/GeV. Uncertainties are statistical and systematic, respectively.
description: CERN-LHC. The modification of the production of J/psi psi(2S), and Upsilon(nS) (n = 1, 2, 3) in p+Pb collisions with respect to their production in pp collisions has been studied. The p+Pb and pp datasets used in this paper correspond to integrated luminosities of 28 nb^-1 and 25 pb^-1 respectively, collected in 2013 and 2015 by the ATLAS detector at the LHC, both at a centre-of-mass energy per nucleon pair of 5.02 TeV. .
DOI: 10.17182/hepdata.82624.v1/t5
title: "Table 5" of "Measurement of quarkonium production in proton--lead and proton--proton collisions at $5.02$ $\mathrm{TeV}$ with the ATLAS detector"

description: Summary of results for cross-section of Upsilon(1S) decaying to a muon pair in pp collisions at 5.02 TeV in nb/GeV. Uncertainties are statistical and systematic, respectively.
description: CERN-LHC. The modification of the production of J/psi psi(2S), and Upsilon(nS) (n = 1, 2, 3) in p+Pb collisions with respect to their production in pp collisions has been studied. The p+Pb and pp datasets used in this paper correspond to integrated luminosities of 28 nb^-1 and 25 pb^-1 respectively, collected in 2013 and 2015 by the ATLAS detector at the LHC, both at a centre-of-mass energy per nucleon pair of 5.02 TeV. .
DOI: 10.17182/hepdata.82624.v1/t6
title: "Table 6" of "Measurement of quarkonium production in proton--lead and proton--proton collisions at $5.02$ $\mathrm{TeV}$ with the ATLAS detector"

description: Summary of results for cross-section of Upsilon(2S) decaying to a muon pair in pp collisions at 5.02 TeV in nb/GeV. Uncertainties are statistical and systematic, respectively.
description: CERN-LHC. The modification of the production of J/psi psi(2S), and Upsilon(nS) (n = 1, 2, 3) in p+Pb collisions with respect to their production in pp collisions has been studied. The p+Pb and pp datasets used in this paper correspond to integrated luminosities of 28 nb^-1 and 25 pb^-1 respectively, collected in 2013 and 2015 by the ATLAS detector at the LHC, both at a centre-of-mass energy per nucleon pair of 5.02 TeV. .
DOI: 10.17182/hepdata.82624.v1/t7
title: "Table 7" of "Measurement of quarkonium production in proton--lead and proton--proton collisions at $5.02$ $\mathrm{TeV}$ with the ATLAS detector"

description: Summary of results for cross-section of Upsilon(3S) decaying to a muon pair in pp collisions at 5.02 TeV in nb/GeV. Uncertainties are statistical and systematic, respectively.
description: CERN-LHC. The modification of the production of J/psi psi(2S), and Upsilon(nS) (n = 1, 2, 3) in p+Pb collisions with respect to their production in pp collisions has been studied. The p+Pb and pp datasets used in this paper correspond to integrated luminosities of 28 nb^-1 and 25 pb^-1 respectively, collected in 2013 and 2015 by the ATLAS detector at the LHC, both at a centre-of-mass energy per nucleon pair of 5.02 TeV. .
DOI: 10.17182/hepdata.85369.v1/t4
title: "Table 4" of "Measurement of photon-jet transverse momentum correlations in 5.02 TeV Pb+Pb and $pp$ collisions with ATLAS"

description: Photon-jet pT balance distributions (1/Ng)(dN/dxJg) in pp events (blue, reproduced on all panels) and Pb+Pb events (red) with each panel denoting a different centrality selection. These panels show results with pTg = 158-200 GeV. Total systematic uncertainties are shown as boxes, while statistical uncertainties are shown with vertical bars.
description: CERN-LHC. Measurements of the transverse momentum balance between isolated photons and inclusive jets are presented using 0.49 nb^{-1} of Pb+Pb collision data at 5.02 TeV and 25 pb^{-1} of pp collision data at 5.02 TeV recorded with the ATLAS detector at the LHC. Photons with pT(γ)&gt;63.1 GeV and |eta(γ)|&lt;2.37 are paired inclusively with all jets that have pT&gt;31.6GeV and |eta|&lt;2.8 in the event. The transverse momentum balance given by the jet-to-photon pT ratio, xJγ, are measured for pairs with azimuthal opening angl dphi &gt; 7pi/8. Distributions of the per-photon jet yield (1/Nγ)(dN/dxJγ) are corrected via a two-dimensional unfolding procedure for detector effects and reported at the particle level for the first time. In pp collisions, the distributions are well described by Monte Carlo event generators. In Pb+Pb collisions, the xJγ distribution is modified with increasing centrality, consistent with the picture of parton-energy loss in the hot nuclear medium. The data are compared to a suite of energy loss models and calculations.
DOI: 10.17182/hepdata.82624.v1/t10
title: "Table 10" of "Measurement of quarkonium production in proton--lead and proton--proton collisions at $5.02$ $\mathrm{TeV}$ with the ATLAS detector"

description: Summary of results for cross-section of J/psi decaying to a muon pair in p+Pb collisions at 5.02 TeV as a function of center-of-mass rapdiity in nb/GeV. Uncertainties are statistical and systematic, respectively.
description: CERN-LHC. The modification of the production of J/psi psi(2S), and Upsilon(nS) (n = 1, 2, 3) in p+Pb collisions with respect to their production in pp collisions has been studied. The p+Pb and pp datasets used in this paper correspond to integrated luminosities of 28 nb^-1 and 25 pb^-1 respectively, collected in 2013 and 2015 by the ATLAS detector at the LHC, both at a centre-of-mass energy per nucleon pair of 5.02 TeV. .
DOI: 10.17182/hepdata.82624.v1/t8
title: "Table 8" of "Measurement of quarkonium production in proton--lead and proton--proton collisions at $5.02$ $\mathrm{TeV}$ with the ATLAS detector"

description: Summary of results for cross-section of J/psi decaying to a muon pair in p+Pb collisions at 5.02 TeV in nb/GeV. Uncertainties are statistical and systematic, respectively.
description: CERN-LHC. The modification of the production of J/psi psi(2S), and Upsilon(nS) (n = 1, 2, 3) in p+Pb collisions with respect to their production in pp collisions has been studied. The p+Pb and pp datasets used in this paper correspond to integrated luminosities of 28 nb^-1 and 25 pb^-1 respectively, collected in 2013 and 2015 by the ATLAS detector at the LHC, both at a centre-of-mass energy per nucleon pair of 5.02 TeV. .
DOI: 10.17182/hepdata.82624.v1/t9
title: "Table 9" of "Measurement of quarkonium production in proton--lead and proton--proton collisions at $5.02$ $\mathrm{TeV}$ with the ATLAS detector"

description: Summary of results for cross-section of psi(2S) decaying to a muon pair in p+Pb collisions at 5.02 TeV in nb/GeV. Uncertainties are statistical and systematic, respectively.
description: CERN-LHC. The modification of the production of J/psi psi(2S), and Upsilon(nS) (n = 1, 2, 3) in p+Pb collisions with respect to their production in pp collisions has been studied. The p+Pb and pp datasets used in this paper correspond to integrated luminosities of 28 nb^-1 and 25 pb^-1 respectively, collected in 2013 and 2015 by the ATLAS detector at the LHC, both at a centre-of-mass energy per nucleon pair of 5.02 TeV. .
DOI: 10.17182/hepdata.72848.v1/t1
title: "Table 1" of "Measurement of Parity-Violating Asymmetry in Electron-Deuteron Inelastic Scattering"

description: Asymmetry results on $\vec e-^2$H parity-violating scattering from the PVDIS experiment at JLab.
description: Jefferson Lab-CEBAF. The parity-violating asymmetries between a longitudinally-polarized electron beam and an unpolarized deuterium target have been measured recently. The measurement covered two kinematic points in the deep inelastic scattering region and five in the nucleon resonance region.
DOI: 10.17182/hepdata.72848.v1/t2
title: "Table 2" of "Measurement of Parity-Violating Asymmetry in Electron-Deuteron Inelastic Scattering"

description: Asymmetry results on $\vec e-^2$H parity-violating scattering from the PVDIS experiment at JLab, for RES I settings.
description: Jefferson Lab-CEBAF. The parity-violating asymmetries between a longitudinally-polarized electron beam and an unpolarized deuterium target have been measured recently. The measurement covered two kinematic points in the deep inelastic scattering region and five in the nucleon resonance region.
DOI: 10.17182/hepdata.82624.v1/t11
title: "Table 11" of "Measurement of quarkonium production in proton--lead and proton--proton collisions at $5.02$ $\mathrm{TeV}$ with the ATLAS detector"

description: Summary of results for cross-section of psi(2S) decaying to a muon pair in p+Pb collisions at 5.02 TeV as a function of center-of-mass rapdiity in nb/GeV. Uncertainties are statistical and systematic, respectively.
description: CERN-LHC. The modification of the production of J/psi psi(2S), and Upsilon(nS) (n = 1, 2, 3) in p+Pb collisions with respect to their production in pp collisions has been studied. The p+Pb and pp datasets used in this paper correspond to integrated luminosities of 28 nb^-1 and 25 pb^-1 respectively, collected in 2013 and 2015 by the ATLAS detector at the LHC, both at a centre-of-mass energy per nucleon pair of 5.02 TeV. .
DOI: 10.17182/hepdata.82624.v1/t12
title: "Table 12" of "Measurement of quarkonium production in proton--lead and proton--proton collisions at $5.02$ $\mathrm{TeV}$ with the ATLAS detector"

description: Summary of results for cross-section of Upsilon(nS) decaying to a muon pair in p+Pb collisions at 5.02 TeV in nb/GeV. Uncertainties are statistical and systematic, respectively.
description: CERN-LHC. The modification of the production of J/psi psi(2S), and Upsilon(nS) (n = 1, 2, 3) in p+Pb collisions with respect to their production in pp collisions has been studied. The p+Pb and pp datasets used in this paper correspond to integrated luminosities of 28 nb^-1 and 25 pb^-1 respectively, collected in 2013 and 2015 by the ATLAS detector at the LHC, both at a centre-of-mass energy per nucleon pair of 5.02 TeV. .
DOI: 10.17182/hepdata.82624.v1/t13
title: "Table 13" of "Measurement of quarkonium production in proton--lead and proton--proton collisions at $5.02$ $\mathrm{TeV}$ with the ATLAS detector"

description: Summary of results for cross-section of Upsilon(nS) decaying to a muon pair in p+Pb collisions at 5.02 TeV in nb/GeV. Uncertainties are statistical and systematic, respectively.
description: CERN-LHC. The modification of the production of J/psi psi(2S), and Upsilon(nS) (n = 1, 2, 3) in p+Pb collisions with respect to their production in pp collisions has been studied. The p+Pb and pp datasets used in this paper correspond to integrated luminosities of 28 nb^-1 and 25 pb^-1 respectively, collected in 2013 and 2015 by the ATLAS detector at the LHC, both at a centre-of-mass energy per nucleon pair of 5.02 TeV. .
DOI: 10.17182/hepdata.82624.v1/t14
title: "Table 14" of "Measurement of quarkonium production in proton--lead and proton--proton collisions at $5.02$ $\mathrm{TeV}$ with the ATLAS detector"

description: Summary of results for RpPb of prompt J/psi in p+Pb collisions at 5.02 TeV as a function of pT. Uncertainties are statistical and local systematic and global systematic, respectively.
description: CERN-LHC. The modification of the production of J/psi psi(2S), and Upsilon(nS) (n = 1, 2, 3) in p+Pb collisions with respect to their production in pp collisions has been studied. The p+Pb and pp datasets used in this paper correspond to integrated luminosities of 28 nb^-1 and 25 pb^-1 respectively, collected in 2013 and 2015 by the ATLAS detector at the LHC, both at a centre-of-mass energy per nucleon pair of 5.02 TeV. .
DOI: 10.17182/hepdata.82624.v1/t15
title: "Table 15" of "Measurement of quarkonium production in proton--lead and proton--proton collisions at $5.02$ $\mathrm{TeV}$ with the ATLAS detector"

description: Summary of results for RpPb of non-prompt J/psi in p+Pb collisions at 5.02 TeV as a function of pT. Uncertainties are statistical and local systematic and global systematic, respectively.
description: CERN-LHC. The modification of the production of J/psi psi(2S), and Upsilon(nS) (n = 1, 2, 3) in p+Pb collisions with respect to their production in pp collisions has been studied. The p+Pb and pp datasets used in this paper correspond to integrated luminosities of 28 nb^-1 and 25 pb^-1 respectively, collected in 2013 and 2015 by the ATLAS detector at the LHC, both at a centre-of-mass energy per nucleon pair of 5.02 TeV. .
DOI: 10.17182/hepdata.82624.v1/t16
title: "Table 16" of "Measurement of quarkonium production in proton--lead and proton--proton collisions at $5.02$ $\mathrm{TeV}$ with the ATLAS detector"

description: Summary of results for RpPb of prompt J/psi in p+Pb collisions at 5.02 TeV as a function of ystar. Uncertainties are statistical and local systematic and global systematic, respectively.
description: CERN-LHC. The modification of the production of J/psi psi(2S), and Upsilon(nS) (n = 1, 2, 3) in p+Pb collisions with respect to their production in pp collisions has been studied. The p+Pb and pp datasets used in this paper correspond to integrated luminosities of 28 nb^-1 and 25 pb^-1 respectively, collected in 2013 and 2015 by the ATLAS detector at the LHC, both at a centre-of-mass energy per nucleon pair of 5.02 TeV. .
DOI: 10.17182/hepdata.72848.v1/t3
title: "Table 3" of "Measurement of Parity-Violating Asymmetry in Electron-Deuteron Inelastic Scattering"

description: Asymmetry results on $\vec e-^2$H parity-violating scattering from the PVDIS experiment at JLab, for RES II settings.
description: Jefferson Lab-CEBAF. The parity-violating asymmetries between a longitudinally-polarized electron beam and an unpolarized deuterium target have been measured recently. The measurement covered two kinematic points in the deep inelastic scattering region and five in the nucleon resonance region.
DOI: 10.17182/hepdata.72848.v1/t4
title: "Table 4" of "Measurement of Parity-Violating Asymmetry in Electron-Deuteron Inelastic Scattering"

description: Asymmetry results on $\vec e-^2$H parity-violating scattering from the PVDIS experiment at JLab, for RES IV settings.
description: Jefferson Lab-CEBAF. The parity-violating asymmetries between a longitudinally-polarized electron beam and an unpolarized deuterium target have been measured recently. The measurement covered two kinematic points in the deep inelastic scattering region and five in the nucleon resonance region.
DOI: 10.17182/hepdata.72848.v1/t5
title: "Table 5" of "Measurement of Parity-Violating Asymmetry in Electron-Deuteron Inelastic Scattering"

description: Asymmetry results on $\vec e-^2$H parity-violating scattering from the PVDIS experiment at JLab, for RES III settings.
description: Jefferson Lab-CEBAF. The parity-violating asymmetries between a longitudinally-polarized electron beam and an unpolarized deuterium target have been measured recently. The measurement covered two kinematic points in the deep inelastic scattering region and five in the nucleon resonance region.
DOI: 10.17182/hepdata.82624.v1/t17
title: "Table 17" of "Measurement of quarkonium production in proton--lead and proton--proton collisions at $5.02$ $\mathrm{TeV}$ with the ATLAS detector"

description: Summary of results for RpPb of non-prompt J/psi in p+Pb collisions at 5.02 TeV as a function of ystar. Uncertainties are statistical and local systematic and global systematic, respectively.
description: CERN-LHC. The modification of the production of J/psi psi(2S), and Upsilon(nS) (n = 1, 2, 3) in p+Pb collisions with respect to their production in pp collisions has been studied. The p+Pb and pp datasets used in this paper correspond to integrated luminosities of 28 nb^-1 and 25 pb^-1 respectively, collected in 2013 and 2015 by the ATLAS detector at the LHC, both at a centre-of-mass energy per nucleon pair of 5.02 TeV. .
DOI: 10.17182/hepdata.82624.v1/t18
title: "Table 18" of "Measurement of quarkonium production in proton--lead and proton--proton collisions at $5.02$ $\mathrm{TeV}$ with the ATLAS detector"

description: Summary of results for RpPb of Upsilon(1S) in p+Pb collisions at 5.02 TeV as a function of pT. Uncertainties are statistical and local systematic and global systematic, respectively.
description: CERN-LHC. The modification of the production of J/psi psi(2S), and Upsilon(nS) (n = 1, 2, 3) in p+Pb collisions with respect to their production in pp collisions has been studied. The p+Pb and pp datasets used in this paper correspond to integrated luminosities of 28 nb^-1 and 25 pb^-1 respectively, collected in 2013 and 2015 by the ATLAS detector at the LHC, both at a centre-of-mass energy per nucleon pair of 5.02 TeV. .
DOI: 10.17182/hepdata.82624.v1/t19
title: "Table 19" of "Measurement of quarkonium production in proton--lead and proton--proton collisions at $5.02$ $\mathrm{TeV}$ with the ATLAS detector"

description: Summary of results for RpPb of Upsilon(1S) in p+Pb collisions at 5.02 TeV as a function of ystar. Uncertainties are statistical and local systematic and global systematic, respectively.
description: CERN-LHC. The modification of the production of J/psi psi(2S), and Upsilon(nS) (n = 1, 2, 3) in p+Pb collisions with respect to their production in pp collisions has been studied. The p+Pb and pp datasets used in this paper correspond to integrated luminosities of 28 nb^-1 and 25 pb^-1 respectively, collected in 2013 and 2015 by the ATLAS detector at the LHC, both at a centre-of-mass energy per nucleon pair of 5.02 TeV. .
DOI: 10.17182/hepdata.82624.v1/t20
title: "Table 20" of "Measurement of quarkonium production in proton--lead and proton--proton collisions at $5.02$ $\mathrm{TeV}$ with the ATLAS detector"

description: Summary of results for RpPb of quarkonia (prompt J/psi, non-prompt J/psi, prompt psi(2S), Upsilon(1S)) to RpPb of Z ratio in p+Pb collisions at 5.02 TeV as a function of centrality. Uncertainties are statistical and local systematic and global systematic, respectively.
description: CERN-LHC. The modification of the production of J/psi psi(2S), and Upsilon(nS) (n = 1, 2, 3) in p+Pb collisions with respect to their production in pp collisions has been studied. The p+Pb and pp datasets used in this paper correspond to integrated luminosities of 28 nb^-1 and 25 pb^-1 respectively, collected in 2013 and 2015 by the ATLAS detector at the LHC, both at a centre-of-mass energy per nucleon pair of 5.02 TeV. .
DOI: 10.17182/hepdata.82624.v1/t21
title: "Table 21" of "Measurement of quarkonium production in proton--lead and proton--proton collisions at $5.02$ $\mathrm{TeV}$ with the ATLAS detector"

description: Summary of results for quarkonia self-normalized yields in p+Pb collisions at 5.02 TeV as a function of self-normalized event activity. Uncertainties are statistical and systematic, respectively.
description: CERN-LHC. The modification of the production of J/psi psi(2S), and Upsilon(nS) (n = 1, 2, 3) in p+Pb collisions with respect to their production in pp collisions has been studied. The p+Pb and pp datasets used in this paper correspond to integrated luminosities of 28 nb^-1 and 25 pb^-1 respectively, collected in 2013 and 2015 by the ATLAS detector at the LHC, both at a centre-of-mass energy per nucleon pair of 5.02 TeV. .
DOI: 10.17182/hepdata.82624.v1/t22
title: "Table 22" of "Measurement of quarkonium production in proton--lead and proton--proton collisions at $5.02$ $\mathrm{TeV}$ with the ATLAS detector"

description: Summary of results for prompt Psi(2S) to J/psi double ratio in p+Pb collisions at 5.02 TeV as a function of center-of-mass rapidity. Uncertainties are statistical and systematic, respectively.
description: CERN-LHC. The modification of the production of J/psi psi(2S), and Upsilon(nS) (n = 1, 2, 3) in p+Pb collisions with respect to their production in pp collisions has been studied. The p+Pb and pp datasets used in this paper correspond to integrated luminosities of 28 nb^-1 and 25 pb^-1 respectively, collected in 2013 and 2015 by the ATLAS detector at the LHC, both at a centre-of-mass energy per nucleon pair of 5.02 TeV. .
DOI: 10.17182/hepdata.82624.v1/t23
title: "Table 23" of "Measurement of quarkonium production in proton--lead and proton--proton collisions at $5.02$ $\mathrm{TeV}$ with the ATLAS detector"

description: Summary of results for Upsilon(2S) and Upsilon(3S) to Upsilon(1S) double ratio in p+Pb collisions at 5.02 TeV. Uncertainties are statistical and systematic, respectively.
description: CERN-LHC. The modification of the production of J/psi psi(2S), and Upsilon(nS) (n = 1, 2, 3) in p+Pb collisions with respect to their production in pp collisions has been studied. The p+Pb and pp datasets used in this paper correspond to integrated luminosities of 28 nb^-1 and 25 pb^-1 respectively, collected in 2013 and 2015 by the ATLAS detector at the LHC, both at a centre-of-mass energy per nucleon pair of 5.02 TeV. .
DOI: 10.17182/hepdata.82624.v1/t24
title: "Table 24" of "Measurement of quarkonium production in proton--lead and proton--proton collisions at $5.02$ $\mathrm{TeV}$ with the ATLAS detector"

description: Summary of results for prompt Psi(2S) and J/psi double ratio in p+Pb collisions at 5.02 TeV as a function of centrality. Uncertainties are statistical and local systematic and global systematic, respectively.
description: CERN-LHC. The modification of the production of J/psi psi(2S), and Upsilon(nS) (n = 1, 2, 3) in p+Pb collisions with respect to their production in pp collisions has been studied. The p+Pb and pp datasets used in this paper correspond to integrated luminosities of 28 nb^-1 and 25 pb^-1 respectively, collected in 2013 and 2015 by the ATLAS detector at the LHC, both at a centre-of-mass energy per nucleon pair of 5.02 TeV. .
DOI: 10.17182/hepdata.82624.v1/t25
title: "Table 25" of "Measurement of quarkonium production in proton--lead and proton--proton collisions at $5.02$ $\mathrm{TeV}$ with the ATLAS detector"

description: Summary of results for Upsilon(2S) and Upsilon(3S) to Upsilon(1S) double ratio in p+Pb collisions at 5.02 TeV as a function of centrality. Uncertainties are statistical and local systematic and global systematic, respectively.
description: CERN-LHC. The modification of the production of J/psi psi(2S), and Upsilon(nS) (n = 1, 2, 3) in p+Pb collisions with respect to their production in pp collisions has been studied. The p+Pb and pp datasets used in this paper correspond to integrated luminosities of 28 nb^-1 and 25 pb^-1 respectively, collected in 2013 and 2015 by the ATLAS detector at the LHC, both at a centre-of-mass energy per nucleon pair of 5.02 TeV. .
DOI: 10.17182/hepdata.83969.v1/t1
title: "Table 1" of "Correlated long-range mixed-harmonic fluctuations measured in $pp$, $p$+Pb and low-multiplicity Pb+Pb collisions with the ATLAS detector"

description: The symmetric cumulant $sc_{2,3}\{4\}$ results as a function of multiplicity ($N_{ch}$) in pp collisions at $\sqrt{s_{NN}}$ = 13 TeV
description: No data abstract available.
DOI: 10.17182/hepdata.83969.v1/t2
title: "Table 2" of "Correlated long-range mixed-harmonic fluctuations measured in $pp$, $p$+Pb and low-multiplicity Pb+Pb collisions with the ATLAS detector"

description: The symmetric cumulant $sc_{2\,3}\{4\}$ results as a function of multiplicity ($N_{ch}$) in pp collisions at $\sqrt{s_{NN}}$ = 13 TeV
description: No data abstract available.