Measurement of the groomed jet mass for $R=0.2$ charged-particle jets in $80 < p_\text{T}^\text{ch jet} < 100$ GeV/$c$ in Pb-Pb collisions at $\sqrt{s_\text{NN}}=5.02$ TeV as compared to pp baseline
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Measurement of the groomed jet mass for $R=0.2$ charged-particle jets in $60 < p_\text{T}^\text{ch jet} < 80$ GeV/$c$ in Pb-Pb collisions at $\sqrt{s_\text{NN}}=5.02$ TeV as compared to pp baseline
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Measurement of the groomed jet mass for $R=0.2$ charged-particle jets in $40 < p_\text{T}^\text{ch jet} < 60$ GeV/$c$ in Pb-Pb collisions at $\sqrt{s_\text{NN}}=5.02$ TeV as compared to pp baseline
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Measurement of the ungroomed jet mass for $R=0.2$ charged-particle jets in $80 < p_\text{T}^\text{ch jet} < 100$ GeV/$c$ in Pb-Pb collisions at $\sqrt{s_\text{NN}}=5.02$ TeV as compared to pp baseline
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Measurement of the ungroomed jet mass for $R=0.2$ charged-particle jets in $60 < p_\text{T}^\text{ch jet} < 80$ GeV/$c$ in Pb-Pb collisions at $\sqrt{s_\text{NN}}=5.02$ TeV as compared to pp baseline
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Measurement of the ungroomed jet mass for $R=0.2$ charged-particle jets in $40 < p_\text{T}^\text{ch jet} < 60$ GeV/$c$ in Pb-Pb collisions at $\sqrt{s_\text{NN}}=5.02$ TeV as compared to pp baseline
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Measurement of the groomed jet mass in Pb-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV from $100 < p_\mathrm{T}^\mathrm{ch\;jet} < 150$ GeV/$c$ with $R=0.2$
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Measurement of the groomed jet mass in Pb-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV from $80 < p_\mathrm{T}^\mathrm{ch\;jet} < 100$ GeV/$c$ with $R=0.2$
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Measurement of the groomed jet mass in Pb-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV from $60 < p_\mathrm{T}^\mathrm{ch\;jet} < 80$ GeV/$c$ with $R=0.2$
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Measurement of the groomed jet mass in Pb-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV from $40 < p_\mathrm{T}^\mathrm{ch\;jet} < 60$ GeV/$c$ with $R=0.2$
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Measurement of the groomed jet mass in pp collisions at $\sqrt{s} = 5.02$ TeV from $80 < p_\mathrm{T}^\mathrm{ch\;jet} < 100$ GeV/$c$ with $R=0.2$
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Measurement of the groomed jet mass in pp collisions at $\sqrt{s} = 5.02$ TeV from $60 < p_\mathrm{T}^\mathrm{ch\;jet} < 80$ GeV/$c$ with $R=0.2$
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Measurement of the groomed jet mass in pp collisions at $\sqrt{s} = 5.02$ TeV from $40 < p_\mathrm{T}^\mathrm{ch\;jet} < 60$ GeV/$c$ with $R=0.2$
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Measurement of the ungroomed jet mass in pp collisions at $\sqrt{s} = 5.02$ TeV from $80 < p_\mathrm{T}^\mathrm{ch\;jet} < 100$ GeV/$c$ with $R=0.2$
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Measurement of the ungroomed jet mass in pp collisions at $\sqrt{s} = 5.02$ TeV from $60 < p_\mathrm{T}^\mathrm{ch\;jet} < 80$ GeV/$c$ with $R=0.2$
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Measurement of the ungroomed jet mass in pp collisions at $\sqrt{s} = 5.02$ TeV from $40 < p_\mathrm{T}^\mathrm{ch\;jet} < 60$ GeV/$c$ with $R=0.2$
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Measurement of the ungroomed jet mass in Pb-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV from $100 < p_\mathrm{T}^\mathrm{ch\;jet} < 150$ GeV/$c$ with $R=0.2$
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Measurement of the ungroomed jet mass in Pb-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV from $80 < p_\mathrm{T}^\mathrm{ch\;jet} < 100$ GeV/$c$ with $R=0.2$
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Measurement of the ungroomed jet mass in Pb-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV from $60 < p_\mathrm{T}^\mathrm{ch\;jet} < 80$ GeV/$c$ with $R=0.2$
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Measurement of the ungroomed jet mass in Pb-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV from $40 < p_\mathrm{T}^\mathrm{ch\;jet} < 60$ GeV/$c$ with $R=0.2$
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Omega over pion ratio as a function of the pion yield in pp collisions at 9 GeV, 7 TeV and 13.6 TeV
- PWG : PWG-LF (Light Flavour Spectra)
- Energy: 900 GeV
, - Energy: 7 TeV
, - Energy: 13.6 TeV
- System p-p
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Kaon over pion ratio as a function of pT in pp collisions at 900 GeV, 13 TeV and 13.6 TeV with Run 3 data
- PWG : PWG-LF (Light Flavour Spectra)
- Energy: 900 GeV
- System p-p
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Proton over pion ratio as a function of pT in pp collisions at 900 GeV, 13 TeV and 13.6 TeV with Run 3 data
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Xic/D0 and Xic/Lc ratio in low and high V0M multiplicity classes compared to PYTHIA
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Invariant mass distribution of Xic in high multiplicity class
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Prompt efficiency of Xic for different multiplicity classes
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Away-Side Nuclear Modification factor ($I_{AA}$) of Pb-Pb in 0 - 10% Centrality compared to LF $I_{AA}$
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Near-Side Nuclear Modification factor ($I_{AA}$) of Pb-Pb in 0 - 10% Centrality compared to LF $I_{AA}$
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Charged jet $R_{AA}$ for R = 0.3 measured in central Pb-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV: Comparison to STAR $R_{AA}$
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Charged jet $R_{AA}$ for R = 0.3 measured in central Pb-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV: Comparison to previous ALICE $R_{AA}$ measured with 2015 Pb-Pb data
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Charged jet $R_{AA}$ for R = 0.3 measured in central Pb-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV
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Corrected charged jet distributions with $p_{T}^{lead} > 3$ GeV/c and $p_{T}^{lead} > 4$ GeV/c for central Pb-Pb collisions at 5.02 TeV
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Response matrix for R=0.3 jets with $p_{T}^{lead} > 4$ GeV/c in central Pb-Pb collisions at 5.02 TeV
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Response matrix for R=0.3 jets with $p_{T}^{lead} > 3$ GeV/c in central Pb-Pb collisions at 5.02 TeV
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Raw correlated quasi-inclusive jet $p_{T,jet}^{reco}$ distribution with $p_{T}^{lead} > 3$ GeV/c for central Pb-Pb collisions at 5.02 TeV
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Raw correlated quasi-inclusive jet $p_{T,jet}^{reco}$ distribution with $p_{T}^{lead} > 4$ GeV/c for central Pb-Pb collisions at 5.02 TeV
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Raw quasi-inclusive jet $p_{T,jet}^{reco}$ distribution of the SE and ME with $p_{T}^{lead} > 3$ GeV/c for central Pb-Pb collisions at 5.02 TeV
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Raw quasi-inclusive jet $p_{T,jet}^{reco}$ distribution of the SE and ME with $p_{T}^{lead} > 4$ GeV/c for central Pb-Pb collisions at 5.02 TeV
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Lc/D0_vs_multiplcity_pt_pPb_5.02TeV
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D0_corrected_yield_pPb_5.02TeV
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Lc_corrected_yield_pPb_5.02TeV
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Delta Phi Distribution of heavy-flavor decay electrons and charged particles, Pb-Pb 30 - 50% Centrality and pp, 2 pT bins
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Delta Phi Distribution of heavy-flavor decay electrons and charged particles, Pb-Pb 0 - 10% Centrality and pp, 2 pT bins
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Delta Phi Distribution of heavy-flavor decay electrons and charged particles with background uncertainty, Pb-Pb 0 - 10%, 2 pT bins
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Ratio of the $j_\mathrm{T}$ distributions in high $z$ to the $j_\mathrm{T}$ distributions in inclusive $z$
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Ratio of the $j_\mathrm{T}$ distributions in low $z$ to the $j_\mathrm{T}$ distributions in inclusive $z$
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$j_\mathrm{T}$ distributions in $60 < p_\mathrm{T,jet}^\mathrm{ch} < 100 \;\mathrm{ GeV}/c$ in differential $z$ compared to HERWIG7
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$j_\mathrm{T}$ distributions in $40 < p_\mathrm{T,jet}^\mathrm{ch} < 60 \;\mathrm{ GeV}/c$ in differential $z$ compared to HERWIG7
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$j_\mathrm{T}$ distributions in $20 < p_\mathrm{T,jet}^\mathrm{ch} < 40 \;\mathrm{ GeV}/c$ in differential $z$ compared to HERWIG7
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$j_\mathrm{T}$ distributions in $10 < p_\mathrm{T,jet}^\mathrm{ch} < 20 \;\mathrm{ GeV}/c$ in differential $z$ compared to HERWIG7
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$j_\mathrm{T}$ distributions in $10 < p_\mathrm{T,jet}^\mathrm{ch} < 20 \;\mathrm{ GeV}/c$ in differential $z$ compared to PYTHIA8 Monash
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$j_\mathrm{T}$ distributions in $20 < p_\mathrm{T,jet}^\mathrm{ch} < 40 \;\mathrm{ GeV}/c$ in differential $z$ compared to PYTHIA8 Monash
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$j_\mathrm{T}$ distributions in $40 < p_\mathrm{T,jet}^\mathrm{ch} < 60 \;\mathrm{ GeV}/c$ in differential $z$ compared to PYTHIA8 Monash
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$j_\mathrm{T}$ distributions in $60 < p_\mathrm{T,jet}^\mathrm{ch} < 100 \;\mathrm{ GeV}/c$ in differential $z$ compared to PYTHIA8 Monash
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Jet $p_\mathrm{T}$ dependence of $j_\mathrm{T}$ distributions in inclusive $z$
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Jet $p_\mathrm{T}$ dependence of $j_\mathrm{T}$ distributions in low $z$
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Jet $p_\mathrm{T}$ dependence of $j_\mathrm{T}$ distributions in mid $z$
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Jet $p_\mathrm{T}$ dependence of $j_\mathrm{T}$ distributions in high $z$
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Invariant mass distribution of Xic+ in high multiplicity class
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ROC curve for high multiplicity, transverse momentum 6 to 8 GeV interval
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BDT output distribution in high multiplicity, transverse momentum 6 to 8 GeV interval
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Prompt efficiency of Xic+ for different multiplicity classes
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Xic+ over D0 for different multiplicity classes
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Corrected yield of Xic+ for different multiplicity classes with ratio to INEL>0 classes
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Corrected yield of \Xi_c^0 in different V0M multiplicity classes
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Csic0/D0 and Csic+/D0 ratio in low and high V0M multiplicity classes
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Xic/Lc ratio in low and high V0M multiplicity classes
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Xic/D0 ratio in low and high V0M multiplicity classes
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Xic/Lc ratio measured in \pp collisions at 13TeV in different multiplicity
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Xi_c^0/D^0 ratio in different V0M multiplicity classes
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psi and jpsi signal extraction from 13.6 TeV pp data
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psi-to-jpsi ratio as function of the pT at midrapidity in pp at 13.6 TeV, compared with the similar measurements from forward rapidity
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y-differential coherent J/psi photoproduction cross section at pT < 0.3 GeV/c in the centrality range (70-90)% in Pb-Pb collisions at 5.02 TeV with data points only
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y-differential raw J/psi yield as a function of pT in the centrality range (70-90)% in Pb-Pb collisions at 5.02 TeV
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y-differential J/psi production cross section at forward y as a function of pT in pp collisions at 5.02 TeV
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The J/psi nuclear modification factor as a function of pT in the centrality range (70-90)% in Pb-Pb collisions at 5.02 TeV for 3.75 < y < 4
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The J/psi nuclear modification factor as a function of pT in the centrality range (70-90)% in Pb-Pb collisions at 5.02 TeV for 3.5 < y < 3.75
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The J/psi nuclear modification factor as a function of pT in the centrality range (70-90)% in Pb-Pb collisions at 5.02 TeV for 3.25 < y < 3.5
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The J/psi nuclear modification factor as a function of pT in the centrality range (70-90)% in Pb-Pb collisions at 5.02 TeV for 3 < y < 3.25
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The J/psi nuclear modification factor as a function of pT in the centrality range (70-90)% in Pb-Pb collisions at 5.02 TeV for 2.75 < y < 3
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The J/psi nuclear modification factor as a function of pT in the centrality range (70-90)% in Pb-Pb collisions at 5.02 TeV for 2.5 < y < 2.75
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The J/psi nuclear modification factor for six y intervals at forward rapidity as a function of pT, pT < 3 GeV/c, in the centrality range (70-90)% in Pb-Pb collisions at 5.02 TeV
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The J/psi nuclear modification factor for six y intervals at forward rapidity as a function of pT in the centrality range (70-90)% in Pb-Pb collisions at 5.02 TeV
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y-differential coherent J/psi photoproduction cross section at pT < 0.3 GeV/c in the centrality range (70-90)% in Pb-Pb collisions at 5.02 TeV compared with one set of models of different scenarios
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y-differential coherent J/psi photoproduction cross section at pT < 0.3 GeV/c in the centrality range (70-90)% in Pb-Pb collisions at 5.02 TeV
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Eta/Pi0 ratio as function of z for different jet pT intervals
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Ratio of Pi0 z spectra (Fragmentation function) for data and PYTHIA to parameterization
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Eta/Pi0 ratio inside jets as function of pT for different jet pT intervals
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Ratio of fully corrected Eta pT spectra inside jets (data and PYTHIA) to parameterization
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Eta pT spectra in different jet pT intervals normalized per jet
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Ratio of fully corrected Pi0 pT spectra inside jets (data and PYTHIA) to parameterization
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Pi0 pT spectra in different jet pT intervals normalized per jet
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Ratio of Eta pT spectra in different jet pT intervals to a fit to the inclusive Eta spectrum
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Eta pT spectra in different jet pT intervals normalized per event
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Ratio of Pi0 pT spectra in different jet pT intervals to a fit to the inclusive Pi0 spectrum
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Pi0 pT spectra in different jet pT intervals normalized per event and the inclusive Pi0 spectrum
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Pi0 pT spectra in different jet pT intervals normalized per event
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Comparison of corrected Eta spectra inside jets from different reconstruction methods as function of z
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Comparison of corrected Pi0 spectra inside jets from different reconstruction methods as function of z
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$\rho_{00}$ parameter of prompt $\mathrm{D}^{*+}$ mesons in $0.3<|y|<0.8$ with respect to the reaction plane and a random axis in 30-50% Pb-Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV
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