cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.165763.v1/t2
title: "Table 2" of "First measurement of D$^{*+}$ vector spin alignment in Pb-Pb collisions at $\mathbf{\sqrt{s_{\rm NN}} = 5.02}$ TeV"

description: $\rho_{00}$ of prompt D$^{*\pm}$ mesons as a function of transverse momentum ($p_{\rm T}$) in the rapidity interval $0.3 &lt; |y| &lt; 0.8$ for mid-central (30--50\%) Pb--Pb collisions at $\sqrt{s_{\rm NN}}=5.02~TeV$.
description: No data abstract available.
DOI: 10.17182/hepdata.165804.v1/t2
title: "Figure 2, right panel $\pi^{-}$–d" of "Revealing the microscopic mechanism of deuteron formation at the LHC"

description: Measured $\pi^{-}$–d$\oplus\pi^{+}$–$\overline{\mathrm{d}}$ (right panel) correlation function.
description: The formation of light (anti)nuclei with mass number A of few units (e.g., d, $^3$He, and $^4$He) in high-energy hadronic collisions presents a longstanding mystery in nuclear physics. It is not clear how nuclei bound by a few MeV can emerge in environments characterized by temperatures above 100 MeV, about 100,000 times hotter than the center of the Sun. Despite extensive studies, this question remained unanswered. The ALICE Collaboration now addresses it with a novel approach using deuteron–pion momentum correlations in proton-proton (pp) collisions at the Large Hadron Collider (LHC). Our results provide model-independent evidence that about 80% of the observed (anti)deuterons are produced in nuclear fusion reactions following the decay of short-lived resonances, such as the $\Delta (1232)$. These findings resolve a crucial gap in our understanding of nucleosynthesis in hadronic collisions. Beyond answering the fundamental question on how nuclei are formed in hadronic collisions, the results can be employed in the modeling of the production of light and heavy nuclei in cosmic rays and dark matter decays
DOI: 10.17182/hepdata.165804.v1/t3
title: "Figure 3, data for $\pi^{+}$–d" of "Revealing the microscopic mechanism of deuteron formation at the LHC"

description: The extracted kinetic decoupling temperature is derived from $\pi^{+}$–d correlation functions.
description: The formation of light (anti)nuclei with mass number A of few units (e.g., d, $^3$He, and $^4$He) in high-energy hadronic collisions presents a longstanding mystery in nuclear physics. It is not clear how nuclei bound by a few MeV can emerge in environments characterized by temperatures above 100 MeV, about 100,000 times hotter than the center of the Sun. Despite extensive studies, this question remained unanswered. The ALICE Collaboration now addresses it with a novel approach using deuteron–pion momentum correlations in proton-proton (pp) collisions at the Large Hadron Collider (LHC). Our results provide model-independent evidence that about 80% of the observed (anti)deuterons are produced in nuclear fusion reactions following the decay of short-lived resonances, such as the $\Delta (1232)$. These findings resolve a crucial gap in our understanding of nucleosynthesis in hadronic collisions. Beyond answering the fundamental question on how nuclei are formed in hadronic collisions, the results can be employed in the modeling of the production of light and heavy nuclei in cosmic rays and dark matter decays
DOI: 10.17182/hepdata.165804.v1/t4
title: "Figure 3, data for $\pi^{-}$–d" of "Revealing the microscopic mechanism of deuteron formation at the LHC"

description: The extracted kinetic decoupling temperature is derived from $\pi^{-}$–d correlation functions.
description: The formation of light (anti)nuclei with mass number A of few units (e.g., d, $^3$He, and $^4$He) in high-energy hadronic collisions presents a longstanding mystery in nuclear physics. It is not clear how nuclei bound by a few MeV can emerge in environments characterized by temperatures above 100 MeV, about 100,000 times hotter than the center of the Sun. Despite extensive studies, this question remained unanswered. The ALICE Collaboration now addresses it with a novel approach using deuteron–pion momentum correlations in proton-proton (pp) collisions at the Large Hadron Collider (LHC). Our results provide model-independent evidence that about 80% of the observed (anti)deuterons are produced in nuclear fusion reactions following the decay of short-lived resonances, such as the $\Delta (1232)$. These findings resolve a crucial gap in our understanding of nucleosynthesis in hadronic collisions. Beyond answering the fundamental question on how nuclei are formed in hadronic collisions, the results can be employed in the modeling of the production of light and heavy nuclei in cosmic rays and dark matter decays
DOI: 10.17182/hepdata.165804.v1/t5
title: "Mixed Event for $\pi^{+}$–d" of "Revealing the microscopic mechanism of deuteron formation at the LHC"

description: This is the mixed event distribution for $\pi^{+}$–d, required for the fitting
description: The formation of light (anti)nuclei with mass number A of few units (e.g., d, $^3$He, and $^4$He) in high-energy hadronic collisions presents a longstanding mystery in nuclear physics. It is not clear how nuclei bound by a few MeV can emerge in environments characterized by temperatures above 100 MeV, about 100,000 times hotter than the center of the Sun. Despite extensive studies, this question remained unanswered. The ALICE Collaboration now addresses it with a novel approach using deuteron–pion momentum correlations in proton-proton (pp) collisions at the Large Hadron Collider (LHC). Our results provide model-independent evidence that about 80% of the observed (anti)deuterons are produced in nuclear fusion reactions following the decay of short-lived resonances, such as the $\Delta (1232)$. These findings resolve a crucial gap in our understanding of nucleosynthesis in hadronic collisions. Beyond answering the fundamental question on how nuclei are formed in hadronic collisions, the results can be employed in the modeling of the production of light and heavy nuclei in cosmic rays and dark matter decays
DOI: 10.17182/hepdata.165804.v1/t6
title: "Mixed Event for $\pi^{-}$–d" of "Revealing the microscopic mechanism of deuteron formation at the LHC"

description: This is the mixed event distribution for $\pi^{-}$–d, required for the fitting
description: The formation of light (anti)nuclei with mass number A of few units (e.g., d, $^3$He, and $^4$He) in high-energy hadronic collisions presents a longstanding mystery in nuclear physics. It is not clear how nuclei bound by a few MeV can emerge in environments characterized by temperatures above 100 MeV, about 100,000 times hotter than the center of the Sun. Despite extensive studies, this question remained unanswered. The ALICE Collaboration now addresses it with a novel approach using deuteron–pion momentum correlations in proton-proton (pp) collisions at the Large Hadron Collider (LHC). Our results provide model-independent evidence that about 80% of the observed (anti)deuterons are produced in nuclear fusion reactions following the decay of short-lived resonances, such as the $\Delta (1232)$. These findings resolve a crucial gap in our understanding of nucleosynthesis in hadronic collisions. Beyond answering the fundamental question on how nuclei are formed in hadronic collisions, the results can be employed in the modeling of the production of light and heavy nuclei in cosmic rays and dark matter decays
DOI: 10.17182/hepdata.165804.v1/t7
title: "Momentum smearing matrix for $\pi$–d" of "Revealing the microscopic mechanism of deuteron formation at the LHC"

description: The momentum smearing matrix, required for the fitting, used both for $\pi^{-}$–d and $\pi^{+}$–d
description: The formation of light (anti)nuclei with mass number A of few units (e.g., d, $^3$He, and $^4$He) in high-energy hadronic collisions presents a longstanding mystery in nuclear physics. It is not clear how nuclei bound by a few MeV can emerge in environments characterized by temperatures above 100 MeV, about 100,000 times hotter than the center of the Sun. Despite extensive studies, this question remained unanswered. The ALICE Collaboration now addresses it with a novel approach using deuteron–pion momentum correlations in proton-proton (pp) collisions at the Large Hadron Collider (LHC). Our results provide model-independent evidence that about 80% of the observed (anti)deuterons are produced in nuclear fusion reactions following the decay of short-lived resonances, such as the $\Delta (1232)$. These findings resolve a crucial gap in our understanding of nucleosynthesis in hadronic collisions. Beyond answering the fundamental question on how nuclei are formed in hadronic collisions, the results can be employed in the modeling of the production of light and heavy nuclei in cosmic rays and dark matter decays
DOI: 10.17182/hepdata.165463.v1/t1
title: "$\omega$ Production in pp" of "Measurement of $\omega$ meson production in pp and p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV"

description: Differential production cross section of $\omega$ mesons in pp collisions at 5.02 TeV. In addition to the edges of the $p_{\rm T}$ intervals, the table shows the corresponding $p_{\rm T}$ position as described in the publication.
description: We present the measurement of the $p_{\rm T}$-differential production cross section of $\omega$ mesons in pp and p--Pb collisions at $\sqrt{s_{\text{\tiny NN}}}=5.02$ TeV at midrapidity by ALICE.
In addition, the first measurement of the nuclear modification factor $R_{\text{pPb}}$ for $\omega$ mesons at LHC energies is presented, complementing the existing measurements of lighter neutral mesons such as the $\pi^0$ and $\eta$.
Within the measured $p_{\rm T}$-range, the $R_{\text{pPb}}$ of $\omega$ mesons shows no cold nuclear matter effects within the uncertainties, consistent with previous measurements at lower energies.
The $\omega/\pi^{0}$ ratio is presented for both collision systems, showing no collision system dependence within the uncertainties.
The comparison to previously published $\omega/\pi^0$ ratios at lower and higher collision energies in pp collisions suggests a decreasing trend of the ratio above $p_{\rm T}$ = 4GeV/$c$ with increasing collision energy.
The data in both collision systems are compared to predictions from PYTHIA 8, EPOS LHC and DPMJET event generators, revealing significant shortcomings in these models' ability to describe the production of $\omega$ mesons.
DOI: 10.17182/hepdata.165463.v1/t2
title: "$\omega$ Production in p--Pb" of "Measurement of $\omega$ meson production in pp and p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV"

description: Differential production cross section of $\omega$ mesons in p--Pb collisions at 5.02 TeV. In addition to the edges of the $p_{\rm T}$ intervals, the table shows the corresponding $p_{\rm T}$ position as described in the publication.
description: We present the measurement of the $p_{\rm T}$-differential production cross section of $\omega$ mesons in pp and p--Pb collisions at $\sqrt{s_{\text{\tiny NN}}}=5.02$ TeV at midrapidity by ALICE.
In addition, the first measurement of the nuclear modification factor $R_{\text{pPb}}$ for $\omega$ mesons at LHC energies is presented, complementing the existing measurements of lighter neutral mesons such as the $\pi^0$ and $\eta$.
Within the measured $p_{\rm T}$-range, the $R_{\text{pPb}}$ of $\omega$ mesons shows no cold nuclear matter effects within the uncertainties, consistent with previous measurements at lower energies.
The $\omega/\pi^{0}$ ratio is presented for both collision systems, showing no collision system dependence within the uncertainties.
The comparison to previously published $\omega/\pi^0$ ratios at lower and higher collision energies in pp collisions suggests a decreasing trend of the ratio above $p_{\rm T}$ = 4GeV/$c$ with increasing collision energy.
The data in both collision systems are compared to predictions from PYTHIA 8, EPOS LHC and DPMJET event generators, revealing significant shortcomings in these models' ability to describe the production of $\omega$ mesons.
DOI: 10.17182/hepdata.165463.v1/t4
title: "$\omega/\pi^{0}$ Ratio in p--Pb" of "Measurement of $\omega$ meson production in pp and p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV"

description: Production ratio of $\omega$ to $\pi^{0}$ mesons in p--Pb collisions at 5.02 TeV.
description: We present the measurement of the $p_{\rm T}$-differential production cross section of $\omega$ mesons in pp and p--Pb collisions at $\sqrt{s_{\text{\tiny NN}}}=5.02$ TeV at midrapidity by ALICE.
In addition, the first measurement of the nuclear modification factor $R_{\text{pPb}}$ for $\omega$ mesons at LHC energies is presented, complementing the existing measurements of lighter neutral mesons such as the $\pi^0$ and $\eta$.
Within the measured $p_{\rm T}$-range, the $R_{\text{pPb}}$ of $\omega$ mesons shows no cold nuclear matter effects within the uncertainties, consistent with previous measurements at lower energies.
The $\omega/\pi^{0}$ ratio is presented for both collision systems, showing no collision system dependence within the uncertainties.
The comparison to previously published $\omega/\pi^0$ ratios at lower and higher collision energies in pp collisions suggests a decreasing trend of the ratio above $p_{\rm T}$ = 4GeV/$c$ with increasing collision energy.
The data in both collision systems are compared to predictions from PYTHIA 8, EPOS LHC and DPMJET event generators, revealing significant shortcomings in these models' ability to describe the production of $\omega$ mesons.
DOI: 10.17182/hepdata.165763.v1/t1
title: "Table 1" of "First measurement of D$^{*+}$ vector spin alignment in Pb-Pb collisions at $\mathbf{\sqrt{s_{\rm NN}} = 5.02}$ TeV"

description: $\rho_{00}$ of prompt D$^{*\pm}$ mesons as a function of transverse momentum ($p_{\rm T}$) in the rapidity interval $0.0 &lt; |y| &lt; 0.3$ for mid-central (30--50\%) Pb--Pb collisions at $\sqrt{s_{\rm NN}}=5.02~TeV$.
description: No data abstract available.
DOI: 10.17182/hepdata.165763.v1/t3
title: "Table 3" of "First measurement of D$^{*+}$ vector spin alignment in Pb-Pb collisions at $\mathbf{\sqrt{s_{\rm NN}} = 5.02}$ TeV"

description: $\rho_{00}$ of prompt D$^{*\pm}$ mesons as a function of transverse momentum ($p_{\rm T}$) in the rapidity interval $0.0 &lt; |y| &lt; 0.3$ for central (0--10\%) Pb--Pb collisions at $\sqrt{s_{\rm NN}}=5.02~TeV$.
description: No data abstract available.
DOI: 10.17182/hepdata.165463.v1/t3
title: "$\omega/\pi^{0}$ Ratio in pp" of "Measurement of $\omega$ meson production in pp and p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV"

description: Production ratio of $\omega$ to $\pi^{0}$ mesons in pp collisions at 5.02 TeV.
description: We present the measurement of the $p_{\rm T}$-differential production cross section of $\omega$ mesons in pp and p--Pb collisions at $\sqrt{s_{\text{\tiny NN}}}=5.02$ TeV at midrapidity by ALICE.
In addition, the first measurement of the nuclear modification factor $R_{\text{pPb}}$ for $\omega$ mesons at LHC energies is presented, complementing the existing measurements of lighter neutral mesons such as the $\pi^0$ and $\eta$.
Within the measured $p_{\rm T}$-range, the $R_{\text{pPb}}$ of $\omega$ mesons shows no cold nuclear matter effects within the uncertainties, consistent with previous measurements at lower energies.
The $\omega/\pi^{0}$ ratio is presented for both collision systems, showing no collision system dependence within the uncertainties.
The comparison to previously published $\omega/\pi^0$ ratios at lower and higher collision energies in pp collisions suggests a decreasing trend of the ratio above $p_{\rm T}$ = 4GeV/$c$ with increasing collision energy.
The data in both collision systems are compared to predictions from PYTHIA 8, EPOS LHC and DPMJET event generators, revealing significant shortcomings in these models' ability to describe the production of $\omega$ mesons.
DOI: 10.17182/hepdata.165463.v1/t5
title: "Nuclear Modification Factor" of "Measurement of $\omega$ meson production in pp and p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV"

description: Nuclear modification factor $R_{pPb}$ for $\omega$ meson production in p--Pb/pp collisions at 5.02 TeV.
description: We present the measurement of the $p_{\rm T}$-differential production cross section of $\omega$ mesons in pp and p--Pb collisions at $\sqrt{s_{\text{\tiny NN}}}=5.02$ TeV at midrapidity by ALICE.
In addition, the first measurement of the nuclear modification factor $R_{\text{pPb}}$ for $\omega$ mesons at LHC energies is presented, complementing the existing measurements of lighter neutral mesons such as the $\pi^0$ and $\eta$.
Within the measured $p_{\rm T}$-range, the $R_{\text{pPb}}$ of $\omega$ mesons shows no cold nuclear matter effects within the uncertainties, consistent with previous measurements at lower energies.
The $\omega/\pi^{0}$ ratio is presented for both collision systems, showing no collision system dependence within the uncertainties.
The comparison to previously published $\omega/\pi^0$ ratios at lower and higher collision energies in pp collisions suggests a decreasing trend of the ratio above $p_{\rm T}$ = 4GeV/$c$ with increasing collision energy.
The data in both collision systems are compared to predictions from PYTHIA 8, EPOS LHC and DPMJET event generators, revealing significant shortcomings in these models' ability to describe the production of $\omega$ mesons.
DOI: 10.17182/hepdata.166689.v1/t1
title: "Table 1" of "Long-range transverse momentum correlations and radial flow in Pb$-$Pb collisions at the LHC"

description: The $p_\mathrm{T}$ dependence of $v_{0}(p_\mathrm{T})$ for inclusive charged particles is measured in Pb$-$Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV within the 10$–$20% centrality interval, using a two-particle correlation method with a pseudorapidity gap of $\Delta\eta = 0.4$.
description: Measurements of $v_{0}(p_\mathrm{T})$ of inclusive charged particles and pions, kaons, and protons in Pb$-$Pb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV using the ALICE detector at the CERN LHC.
DOI: 10.17182/hepdata.166689.v1/t2
title: "Table 2" of "Long-range transverse momentum correlations and radial flow in Pb$-$Pb collisions at the LHC"

description: The $p_\mathrm{T}$ dependence of $v_{0}(p_\mathrm{T})$ for inclusive charged particles is measured in Pb$-$Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV within the 30$–$40% centrality interval, using a two-particle correlation method with a pseudorapidity gap of $\Delta\eta = 0.4$.
description: Measurements of $v_{0}(p_\mathrm{T})$ of inclusive charged particles and pions, kaons, and protons in Pb$-$Pb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV using the ALICE detector at the CERN LHC.
DOI: 10.17182/hepdata.166689.v1/t3
title: "Table 3" of "Long-range transverse momentum correlations and radial flow in Pb$-$Pb collisions at the LHC"

description: The $p_\mathrm{T}$ dependence of $v_{0}(p_\mathrm{T})$ for inclusive charged particles is measured in Pb$-$Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV within the 60$–$70% centrality interval, using a two-particle correlation method with a pseudorapidity gap of $\Delta\eta = 0.4$.
description: Measurements of $v_{0}(p_\mathrm{T})$ of inclusive charged particles and pions, kaons, and protons in Pb$-$Pb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV using the ALICE detector at the CERN LHC.
DOI: 10.17182/hepdata.166689.v1/t4
title: "Table 4" of "Long-range transverse momentum correlations and radial flow in Pb$-$Pb collisions at the LHC"

description: The $p_\mathrm{T}$ dependence of $v_{0}(p_\mathrm{T})/v_{0}$ for inclusive charged particles is measured in Pb$-$Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV within the 10$–$20% centrality interval, using a two-particle correlation method with a pseudorapidity gap of $\Delta\eta = 0.4$.
description: Measurements of $v_{0}(p_\mathrm{T})$ of inclusive charged particles and pions, kaons, and protons in Pb$-$Pb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV using the ALICE detector at the CERN LHC.
DOI: 10.17182/hepdata.166689.v1/t5
title: "Table 5" of "Long-range transverse momentum correlations and radial flow in Pb$-$Pb collisions at the LHC"

description: The $p_\mathrm{T}$ dependence of $v_{0}(p_\mathrm{T})/v_{0}$ for inclusive charged particles is measured in Pb$-$Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV within the 30$–$40% centrality interval, using a two-particle correlation method with a pseudorapidity gap of $\Delta\eta = 0.4$.
description: Measurements of $v_{0}(p_\mathrm{T})$ of inclusive charged particles and pions, kaons, and protons in Pb$-$Pb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV using the ALICE detector at the CERN LHC.
DOI: 10.17182/hepdata.166689.v1/t6
title: "Table 6" of "Long-range transverse momentum correlations and radial flow in Pb$-$Pb collisions at the LHC"

description: The $p_\mathrm{T}$ dependence of $v_{0}(p_\mathrm{T})/v_{0}$ for inclusive charged particles is measured in Pb$-$Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV within the 60$–$70% centrality interval, using a two-particle correlation method with a pseudorapidity gap of $\Delta\eta = 0.4$.
description: Measurements of $v_{0}(p_\mathrm{T})$ of inclusive charged particles and pions, kaons, and protons in Pb$-$Pb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV using the ALICE detector at the CERN LHC.
DOI: 10.17182/hepdata.166689.v1/t7
title: "Table 7" of "Long-range transverse momentum correlations and radial flow in Pb$-$Pb collisions at the LHC"

description: The $p_\mathrm{T}$ dependence of $v_{0}(p_\mathrm{T})$ for pions is measured in Pb$-$Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV within the 10$–$20% centrality interval, using a two-particle correlation method with a pseudorapidity gap of $\Delta\eta = 0.4$.
description: Measurements of $v_{0}(p_\mathrm{T})$ of inclusive charged particles and pions, kaons, and protons in Pb$-$Pb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV using the ALICE detector at the CERN LHC.
DOI: 10.17182/hepdata.166689.v1/t10
title: "Table 10" of "Long-range transverse momentum correlations and radial flow in Pb$-$Pb collisions at the LHC"

description: The $p_\mathrm{T}$ dependence of $v_{0}(p_\mathrm{T})$ for pions is measured in Pb$-$Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV within the 30$–$40% centrality interval, using a two-particle correlation method with a pseudorapidity gap of $\Delta\eta = 0.4$.
description: Measurements of $v_{0}(p_\mathrm{T})$ of inclusive charged particles and pions, kaons, and protons in Pb$-$Pb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV using the ALICE detector at the CERN LHC.
DOI: 10.17182/hepdata.166689.v1/t11
title: "Table 11" of "Long-range transverse momentum correlations and radial flow in Pb$-$Pb collisions at the LHC"

description: The $p_\mathrm{T}$ dependence of $v_{0}(p_\mathrm{T})$ for kaons is measured in Pb$-$Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV within the 30$–$40% centrality interval, using a two-particle correlation method with a pseudorapidity gap of $\Delta\eta = 0.4$.
description: Measurements of $v_{0}(p_\mathrm{T})$ of inclusive charged particles and pions, kaons, and protons in Pb$-$Pb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV using the ALICE detector at the CERN LHC.
DOI: 10.17182/hepdata.166689.v1/t13
title: "Table 13" of "Long-range transverse momentum correlations and radial flow in Pb$-$Pb collisions at the LHC"

description: The $p_\mathrm{T}$ dependence of $v_{0}(p_\mathrm{T})$ for pions is measured in Pb$-$Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV within the 60$–$70% centrality interval, using a two-particle correlation method with a pseudorapidity gap of $\Delta\eta = 0.4$.
description: Measurements of $v_{0}(p_\mathrm{T})$ of inclusive charged particles and pions, kaons, and protons in Pb$-$Pb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV using the ALICE detector at the CERN LHC.