cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.155473.v1/t12
title: "Table 12 - B3 vs PTA centrality 0 to 90" of "Measurement of the production and elliptic flow of (anti)nuclei in Xe-Xe collisions at $\sqrt{s_{\rm NN}}$ = 5.44 TeV"

description: Coalescence parameter B3 as a function of the transverse momentum per nucleon pT/A, in the centrality class 0 to 90 percent. The B3 is shown in Figure 7 (right panel).
description: Transverse momentum spectra of deuterons and 3He nuclei, measured in Xe--Xe collisions at centre-of-mass per nucleon-nucleon energy of 5.44 TeV, are shown in Fig. 3. The coalescence parameters B2 and B3 as a function of the transverse momentum per nucleon are reported in Fig. 7. The ratios of the integrated yields of deuterons to protons and 3He to protons are shown in Fig. 5 as a function of the average charged particle multiplicity density. The ratios of the integrated yields of deuterons to pions and 3He to pions are shown in Fig. 6 as a function of the average charged particle multiplicity density. The coalescence parameter B2 as a function of the average charged particle multiplicity density is not shown in the paper but the data are reported in Table 17. Finally, in Fig. 8 the elliptic flow v2 is shown.
DOI: 10.17182/hepdata.155473.v1/t13
title: "Table 13 - Deuteron-over-proton yields vs multiplicity" of "Measurement of the production and elliptic flow of (anti)nuclei in Xe-Xe collisions at $\sqrt{s_{\rm NN}}$ = 5.44 TeV"

description: Ratio of integrated yields of deuterons and of protons, as a function of the average charged particle multiplicity density. The d-to-p ratio is shown in Figure 5 (top panel).
description: Transverse momentum spectra of deuterons and 3He nuclei, measured in Xe--Xe collisions at centre-of-mass per nucleon-nucleon energy of 5.44 TeV, are shown in Fig. 3. The coalescence parameters B2 and B3 as a function of the transverse momentum per nucleon are reported in Fig. 7. The ratios of the integrated yields of deuterons to protons and 3He to protons are shown in Fig. 5 as a function of the average charged particle multiplicity density. The ratios of the integrated yields of deuterons to pions and 3He to pions are shown in Fig. 6 as a function of the average charged particle multiplicity density. The coalescence parameter B2 as a function of the average charged particle multiplicity density is not shown in the paper but the data are reported in Table 17. Finally, in Fig. 8 the elliptic flow v2 is shown.
DOI: 10.17182/hepdata.155473.v1/t7
title: "Table 7 - B2 vs PTA centrality 0 to 10" of "Measurement of the production and elliptic flow of (anti)nuclei in Xe-Xe collisions at $\sqrt{s_{\rm NN}}$ = 5.44 TeV"

description: Coalescence parameter B2 as a function of the transverse momentum per nucleon pT/A, in the centrality class 0 to 10 percent. The B2 is shown in Figure 7 (left panel).
description: Transverse momentum spectra of deuterons and 3He nuclei, measured in Xe--Xe collisions at centre-of-mass per nucleon-nucleon energy of 5.44 TeV, are shown in Fig. 3. The coalescence parameters B2 and B3 as a function of the transverse momentum per nucleon are reported in Fig. 7. The ratios of the integrated yields of deuterons to protons and 3He to protons are shown in Fig. 5 as a function of the average charged particle multiplicity density. The ratios of the integrated yields of deuterons to pions and 3He to pions are shown in Fig. 6 as a function of the average charged particle multiplicity density. The coalescence parameter B2 as a function of the average charged particle multiplicity density is not shown in the paper but the data are reported in Table 17. Finally, in Fig. 8 the elliptic flow v2 is shown.
DOI: 10.17182/hepdata.155473.v1/t8
title: "Table 8 - B2 vs PTA centrality 10 to 20" of "Measurement of the production and elliptic flow of (anti)nuclei in Xe-Xe collisions at $\sqrt{s_{\rm NN}}$ = 5.44 TeV"

description: Coalescence parameter B2 as a function of the transverse momentum per nucleon pT/A, in the centrality class 10 to 20 percent. The B2 is shown in Figure 7 (left panel).
description: Transverse momentum spectra of deuterons and 3He nuclei, measured in Xe--Xe collisions at centre-of-mass per nucleon-nucleon energy of 5.44 TeV, are shown in Fig. 3. The coalescence parameters B2 and B3 as a function of the transverse momentum per nucleon are reported in Fig. 7. The ratios of the integrated yields of deuterons to protons and 3He to protons are shown in Fig. 5 as a function of the average charged particle multiplicity density. The ratios of the integrated yields of deuterons to pions and 3He to pions are shown in Fig. 6 as a function of the average charged particle multiplicity density. The coalescence parameter B2 as a function of the average charged particle multiplicity density is not shown in the paper but the data are reported in Table 17. Finally, in Fig. 8 the elliptic flow v2 is shown.
DOI: 10.17182/hepdata.155473.v1/t9
title: "Table 9 - B2 vs PTA centrality 20 to 40" of "Measurement of the production and elliptic flow of (anti)nuclei in Xe-Xe collisions at $\sqrt{s_{\rm NN}}$ = 5.44 TeV"

description: Coalescence parameter B2 as a function of the transverse momentum per nucleon pT/A, in the centrality class 20 to 40 percent. The B2 is shown in Figure 7 (left panel).
description: Transverse momentum spectra of deuterons and 3He nuclei, measured in Xe--Xe collisions at centre-of-mass per nucleon-nucleon energy of 5.44 TeV, are shown in Fig. 3. The coalescence parameters B2 and B3 as a function of the transverse momentum per nucleon are reported in Fig. 7. The ratios of the integrated yields of deuterons to protons and 3He to protons are shown in Fig. 5 as a function of the average charged particle multiplicity density. The ratios of the integrated yields of deuterons to pions and 3He to pions are shown in Fig. 6 as a function of the average charged particle multiplicity density. The coalescence parameter B2 as a function of the average charged particle multiplicity density is not shown in the paper but the data are reported in Table 17. Finally, in Fig. 8 the elliptic flow v2 is shown.
DOI: 10.17182/hepdata.155473.v1/t14
title: "Table 14 - He3-over-proton yields vs multiplicity" of "Measurement of the production and elliptic flow of (anti)nuclei in Xe-Xe collisions at $\sqrt{s_{\rm NN}}$ = 5.44 TeV"

description: Ratio of integrated yields of He3 and of protons, as a function of the average charged particle multiplicity density. The He3-to-p ratio is shown in Figure 5 (bottom panel).
description: Transverse momentum spectra of deuterons and 3He nuclei, measured in Xe--Xe collisions at centre-of-mass per nucleon-nucleon energy of 5.44 TeV, are shown in Fig. 3. The coalescence parameters B2 and B3 as a function of the transverse momentum per nucleon are reported in Fig. 7. The ratios of the integrated yields of deuterons to protons and 3He to protons are shown in Fig. 5 as a function of the average charged particle multiplicity density. The ratios of the integrated yields of deuterons to pions and 3He to pions are shown in Fig. 6 as a function of the average charged particle multiplicity density. The coalescence parameter B2 as a function of the average charged particle multiplicity density is not shown in the paper but the data are reported in Table 17. Finally, in Fig. 8 the elliptic flow v2 is shown.
DOI: 10.17182/hepdata.155473.v1/t15
title: "Table 15 - Deuteron-over-pion yields vs multiplicity" of "Measurement of the production and elliptic flow of (anti)nuclei in Xe-Xe collisions at $\sqrt{s_{\rm NN}}$ = 5.44 TeV"

description: Ratio of integrated yields of deuterons and of pions, as a function of the average charged particle multiplicity density. The d-to-pi ratio is shown in Figure 6 (top panel).
description: Transverse momentum spectra of deuterons and 3He nuclei, measured in Xe--Xe collisions at centre-of-mass per nucleon-nucleon energy of 5.44 TeV, are shown in Fig. 3. The coalescence parameters B2 and B3 as a function of the transverse momentum per nucleon are reported in Fig. 7. The ratios of the integrated yields of deuterons to protons and 3He to protons are shown in Fig. 5 as a function of the average charged particle multiplicity density. The ratios of the integrated yields of deuterons to pions and 3He to pions are shown in Fig. 6 as a function of the average charged particle multiplicity density. The coalescence parameter B2 as a function of the average charged particle multiplicity density is not shown in the paper but the data are reported in Table 17. Finally, in Fig. 8 the elliptic flow v2 is shown.
DOI: 10.17182/hepdata.155473.v1/t16
title: "Table 16 - He3-over-pion yields vs multiplicity" of "Measurement of the production and elliptic flow of (anti)nuclei in Xe-Xe collisions at $\sqrt{s_{\rm NN}}$ = 5.44 TeV"

description: Ratio of integrated yields of He3 and of pions, as a function of the average charged particle multiplicity density. The He3-to-pi ratio is shown in Figure 6 (bottom panel).
description: Transverse momentum spectra of deuterons and 3He nuclei, measured in Xe--Xe collisions at centre-of-mass per nucleon-nucleon energy of 5.44 TeV, are shown in Fig. 3. The coalescence parameters B2 and B3 as a function of the transverse momentum per nucleon are reported in Fig. 7. The ratios of the integrated yields of deuterons to protons and 3He to protons are shown in Fig. 5 as a function of the average charged particle multiplicity density. The ratios of the integrated yields of deuterons to pions and 3He to pions are shown in Fig. 6 as a function of the average charged particle multiplicity density. The coalescence parameter B2 as a function of the average charged particle multiplicity density is not shown in the paper but the data are reported in Table 17. Finally, in Fig. 8 the elliptic flow v2 is shown.
DOI: 10.17182/hepdata.155473.v1/t17
title: "Table 17 - B2 vs multiplicity" of "Measurement of the production and elliptic flow of (anti)nuclei in Xe-Xe collisions at $\sqrt{s_{\rm NN}}$ = 5.44 TeV"

description: B2 as a function of the average charged particle multiplicity density for pT-over-A equal to 0.75 GEV. The B2 vs. multiplicity is not shown in the paper.
description: Transverse momentum spectra of deuterons and 3He nuclei, measured in Xe--Xe collisions at centre-of-mass per nucleon-nucleon energy of 5.44 TeV, are shown in Fig. 3. The coalescence parameters B2 and B3 as a function of the transverse momentum per nucleon are reported in Fig. 7. The ratios of the integrated yields of deuterons to protons and 3He to protons are shown in Fig. 5 as a function of the average charged particle multiplicity density. The ratios of the integrated yields of deuterons to pions and 3He to pions are shown in Fig. 6 as a function of the average charged particle multiplicity density. The coalescence parameter B2 as a function of the average charged particle multiplicity density is not shown in the paper but the data are reported in Table 17. Finally, in Fig. 8 the elliptic flow v2 is shown.
DOI: 10.17182/hepdata.155473.v1/t19
title: "Table 19 - v2 (elliptic flow) deuterons 20-40" of "Measurement of the production and elliptic flow of (anti)nuclei in Xe-Xe collisions at $\sqrt{s_{\rm NN}}$ = 5.44 TeV"

description: (Anti)deuteron $v_2$ measured at midrapidity in the 20-40 centrality class, as shown in Fig. 8 (right panel).
description: Transverse momentum spectra of deuterons and 3He nuclei, measured in Xe--Xe collisions at centre-of-mass per nucleon-nucleon energy of 5.44 TeV, are shown in Fig. 3. The coalescence parameters B2 and B3 as a function of the transverse momentum per nucleon are reported in Fig. 7. The ratios of the integrated yields of deuterons to protons and 3He to protons are shown in Fig. 5 as a function of the average charged particle multiplicity density. The ratios of the integrated yields of deuterons to pions and 3He to pions are shown in Fig. 6 as a function of the average charged particle multiplicity density. The coalescence parameter B2 as a function of the average charged particle multiplicity density is not shown in the paper but the data are reported in Table 17. Finally, in Fig. 8 the elliptic flow v2 is shown.
DOI: 10.17182/hepdata.155473.v1/t18
title: "Table 18 - v2 (elliptic flow) deuterons 0-20" of "Measurement of the production and elliptic flow of (anti)nuclei in Xe-Xe collisions at $\sqrt{s_{\rm NN}}$ = 5.44 TeV"

description: (Anti)deuteron $v_2$ measured at midrapidity in the 0-20 centrality class, as shown in Fig. 8 (left panel).
description: Transverse momentum spectra of deuterons and 3He nuclei, measured in Xe--Xe collisions at centre-of-mass per nucleon-nucleon energy of 5.44 TeV, are shown in Fig. 3. The coalescence parameters B2 and B3 as a function of the transverse momentum per nucleon are reported in Fig. 7. The ratios of the integrated yields of deuterons to protons and 3He to protons are shown in Fig. 5 as a function of the average charged particle multiplicity density. The ratios of the integrated yields of deuterons to pions and 3He to pions are shown in Fig. 6 as a function of the average charged particle multiplicity density. The coalescence parameter B2 as a function of the average charged particle multiplicity density is not shown in the paper but the data are reported in Table 17. Finally, in Fig. 8 the elliptic flow v2 is shown.
DOI: 10.17182/hepdata.156383.v1/t1
title: "Figure 3 top left" of "Investigating $\Lambda$ baryon production in p-Pb collisions in jets and the underlying event using angular correlations"

description: Azimuthal distribution of the per-trigger h-$\Lambda$ yield with trigger transverse momentum between 4 and 8 GeV/c and associated transverse momentum between 1.5 and 2.5 GeV/c for 0-20% multiplicity class p-Pb collisions
description: First measurements of hadron(h)-$\Lambda$ azimuthal angular correlations in p--Pb collisions at $\sqrt{s_{\text{NN}}}= 5.02$ TeV using the ALICE detector at the LHC are presented. These correlations are used to separate the production of associated $\Lambda$ baryons into three different kinematic regions, namely those produced in the direction of the trigger particle (near-side), those produced in the opposite direction (away-side), and those whose production is uncorrelated with the jet-axis (underlying event). The per-trigger associated $\Lambda$ yields in these regions are extracted, along with the near- and away-side azimuthal peak widths, and the results are studied as a function of associated particle $p_{\text{T}}$ and event multiplicity. Comparisons with the DPMJET event generator and previous measurements of the $\phi(1020)$ meson are also made. The final results indicate that strangeness production in the highest multiplicity p-Pb collisions is enhanced relative to low multiplicity collisions in the jet-like regions, as well as the underlying event. The production of $\Lambda$ relative to charged hadrons is also enhanced in the underlying event when compared to the jet-like regions. Additionally, the results hint that strange quark production in the away-side of the jet is modified by soft interactions with the underlying event.
DOI: 10.17182/hepdata.156383.v1/t2
title: "Figure 3 top middle" of "Investigating $\Lambda$ baryon production in p-Pb collisions in jets and the underlying event using angular correlations"

description: Azimuthal distribution of the per-trigger h-$\Lambda$ yield with trigger transverse momentum between 4 and 8 GeV/c and associated transverse momentum between 1.5 and 2.5 GeV/c for 20-50% multiplicity class p-Pb collisions
description: First measurements of hadron(h)-$\Lambda$ azimuthal angular correlations in p--Pb collisions at $\sqrt{s_{\text{NN}}}= 5.02$ TeV using the ALICE detector at the LHC are presented. These correlations are used to separate the production of associated $\Lambda$ baryons into three different kinematic regions, namely those produced in the direction of the trigger particle (near-side), those produced in the opposite direction (away-side), and those whose production is uncorrelated with the jet-axis (underlying event). The per-trigger associated $\Lambda$ yields in these regions are extracted, along with the near- and away-side azimuthal peak widths, and the results are studied as a function of associated particle $p_{\text{T}}$ and event multiplicity. Comparisons with the DPMJET event generator and previous measurements of the $\phi(1020)$ meson are also made. The final results indicate that strangeness production in the highest multiplicity p-Pb collisions is enhanced relative to low multiplicity collisions in the jet-like regions, as well as the underlying event. The production of $\Lambda$ relative to charged hadrons is also enhanced in the underlying event when compared to the jet-like regions. Additionally, the results hint that strange quark production in the away-side of the jet is modified by soft interactions with the underlying event.
DOI: 10.17182/hepdata.156383.v1/t3
title: "Figure 3 top right" of "Investigating $\Lambda$ baryon production in p-Pb collisions in jets and the underlying event using angular correlations"

description: Azimuthal distribution of the per-trigger h-$\Lambda$ yield with trigger transverse momentum between 4 and 8 GeV/c and associated transverse momentum between 1.5 and 2.5 GeV/c for 50-80% multiplicity class p-Pb collisions
description: First measurements of hadron(h)-$\Lambda$ azimuthal angular correlations in p--Pb collisions at $\sqrt{s_{\text{NN}}}= 5.02$ TeV using the ALICE detector at the LHC are presented. These correlations are used to separate the production of associated $\Lambda$ baryons into three different kinematic regions, namely those produced in the direction of the trigger particle (near-side), those produced in the opposite direction (away-side), and those whose production is uncorrelated with the jet-axis (underlying event). The per-trigger associated $\Lambda$ yields in these regions are extracted, along with the near- and away-side azimuthal peak widths, and the results are studied as a function of associated particle $p_{\text{T}}$ and event multiplicity. Comparisons with the DPMJET event generator and previous measurements of the $\phi(1020)$ meson are also made. The final results indicate that strangeness production in the highest multiplicity p-Pb collisions is enhanced relative to low multiplicity collisions in the jet-like regions, as well as the underlying event. The production of $\Lambda$ relative to charged hadrons is also enhanced in the underlying event when compared to the jet-like regions. Additionally, the results hint that strange quark production in the away-side of the jet is modified by soft interactions with the underlying event.
DOI: 10.17182/hepdata.156383.v1/t4
title: "Figure 3 bottom left" of "Investigating $\Lambda$ baryon production in p-Pb collisions in jets and the underlying event using angular correlations"

description: Azimuthal distribution of the per-trigger h-h yield with trigger transverse momentum between 4 and 8 GeV/c and associated transverse momentum between 1.5 and 2.5 GeV/c for 0-20% multiplicity class p-Pb collisions
description: First measurements of hadron(h)-$\Lambda$ azimuthal angular correlations in p--Pb collisions at $\sqrt{s_{\text{NN}}}= 5.02$ TeV using the ALICE detector at the LHC are presented. These correlations are used to separate the production of associated $\Lambda$ baryons into three different kinematic regions, namely those produced in the direction of the trigger particle (near-side), those produced in the opposite direction (away-side), and those whose production is uncorrelated with the jet-axis (underlying event). The per-trigger associated $\Lambda$ yields in these regions are extracted, along with the near- and away-side azimuthal peak widths, and the results are studied as a function of associated particle $p_{\text{T}}$ and event multiplicity. Comparisons with the DPMJET event generator and previous measurements of the $\phi(1020)$ meson are also made. The final results indicate that strangeness production in the highest multiplicity p-Pb collisions is enhanced relative to low multiplicity collisions in the jet-like regions, as well as the underlying event. The production of $\Lambda$ relative to charged hadrons is also enhanced in the underlying event when compared to the jet-like regions. Additionally, the results hint that strange quark production in the away-side of the jet is modified by soft interactions with the underlying event.
DOI: 10.17182/hepdata.156383.v1/t5
title: "Figure 3 bottom middle" of "Investigating $\Lambda$ baryon production in p-Pb collisions in jets and the underlying event using angular correlations"

description: Azimuthal distribution of the per-trigger h-h yield with trigger transverse momentum between 4 and 8 GeV/c and associated transverse momentum between 1.5 and 2.5 GeV/c for 20-50% multiplicity class p-Pb collisions
description: First measurements of hadron(h)-$\Lambda$ azimuthal angular correlations in p--Pb collisions at $\sqrt{s_{\text{NN}}}= 5.02$ TeV using the ALICE detector at the LHC are presented. These correlations are used to separate the production of associated $\Lambda$ baryons into three different kinematic regions, namely those produced in the direction of the trigger particle (near-side), those produced in the opposite direction (away-side), and those whose production is uncorrelated with the jet-axis (underlying event). The per-trigger associated $\Lambda$ yields in these regions are extracted, along with the near- and away-side azimuthal peak widths, and the results are studied as a function of associated particle $p_{\text{T}}$ and event multiplicity. Comparisons with the DPMJET event generator and previous measurements of the $\phi(1020)$ meson are also made. The final results indicate that strangeness production in the highest multiplicity p-Pb collisions is enhanced relative to low multiplicity collisions in the jet-like regions, as well as the underlying event. The production of $\Lambda$ relative to charged hadrons is also enhanced in the underlying event when compared to the jet-like regions. Additionally, the results hint that strange quark production in the away-side of the jet is modified by soft interactions with the underlying event.
DOI: 10.17182/hepdata.156383.v1/t6
title: "Figure 3 bottom right" of "Investigating $\Lambda$ baryon production in p-Pb collisions in jets and the underlying event using angular correlations"

description: Azimuthal distribution of the per-trigger h-h yield with trigger transverse momentum between 4 and 8 GeV/c and associated transverse momentum between 1.5 and 2.5 GeV/c for 50-80% multiplicity class p-Pb collisions
description: First measurements of hadron(h)-$\Lambda$ azimuthal angular correlations in p--Pb collisions at $\sqrt{s_{\text{NN}}}= 5.02$ TeV using the ALICE detector at the LHC are presented. These correlations are used to separate the production of associated $\Lambda$ baryons into three different kinematic regions, namely those produced in the direction of the trigger particle (near-side), those produced in the opposite direction (away-side), and those whose production is uncorrelated with the jet-axis (underlying event). The per-trigger associated $\Lambda$ yields in these regions are extracted, along with the near- and away-side azimuthal peak widths, and the results are studied as a function of associated particle $p_{\text{T}}$ and event multiplicity. Comparisons with the DPMJET event generator and previous measurements of the $\phi(1020)$ meson are also made. The final results indicate that strangeness production in the highest multiplicity p-Pb collisions is enhanced relative to low multiplicity collisions in the jet-like regions, as well as the underlying event. The production of $\Lambda$ relative to charged hadrons is also enhanced in the underlying event when compared to the jet-like regions. Additionally, the results hint that strange quark production in the away-side of the jet is modified by soft interactions with the underlying event.