| Charged particles Balance Functions RMS DeltaPhi in p-Pb at 5.02 TeV vs centrality (2016 data sample)
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| Charged particles Balance Functions RMS DeltaEta in p-Pb at 5.02 TeV vs centrality (2016 data sample)
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| Charged particles Balance Functions Away Side Yields in Pb-Pb at 5.02 TeV vs centrality
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| Charged particles Balance Functions Near Side Yields in Pb-Pb at 5.02 TeV vs centrality
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| Charged particles Balance Functions Total Yields in Pb-Pb at 5.02 TeV vs centrality
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| Charged particles Balance Functions RMS DeltaPhi in Pb-Pb at 5.02 TeV vs centrality
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| Charged particles Balance Functions RMS DeltaEta in Pb-Pb at 5.02 TeV vs centrality
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| 2D Charged particles Balance Functions at 5.02 TeV - 70-80% - 1 < pT trigger, pT ass < 2 GeV/c
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| 2D Charged particles Balance Functions at 5.02 TeV - 30-40% - 1 < pT trigger, pT ass < 2 GeV/c
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| 2D Charged particles Balance Functions at 5.02 TeV - 0-5% - 1 < pT trigger, pT ass < 2 GeV/c
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| 2D Charged particles Balance Functions at 5.02 TeV - 70-80%
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| 2D Charged particles Balance Functions at 5.02 TeV - 30-40%
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| 2D Charged particles Balance Functions at 5.02 TeV - 0-5%
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| Net-lambda moments versus DeltaEta in 30-40% central events
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| Net-lambda moments versus DeltaEta in 0-10% central events
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| Net-lambda moments versus centrality, first and second moments only
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| Net-lambda moments versus centrality, first moments only
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| Net-lambda moments versus centrality, with MC comparison
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| Net-lambda moments versus centrality
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| Example lambda minv weights for Identity Method analysis
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| Example lambda invariant mass peak for Identity Method analysis
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| K*0 signal after background subtraction in Pb-Pb collisions at 5.02 TeV in Production plane
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| Invariant mass distribution before background subtraction in Pb-Pb collisions at 5.02 TeV in Production plane
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| v_{2} \{2\} of \Lambda(\bar{\Lambda}) in 0-20\% V0A multiplicity class compared to published CMS
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| v_{2} \{2\} of K^{0}_{S} in 0-20\% V0A multiplicity class compared to published CMS
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| v_{2} \{2\} of inclusive charged hadrons in 0-20\% V0A multiplicity class compared to published CMS
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| v_{2}^{sub} \{2,|\Delta\eta| < 0.4\} / n_{q} with KE_{T} scaling in 40-60\% V0A multiplicity class
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| v_{2}^{sub} \{2,|\Delta\eta| < 0.4\} / n_{q} with KE_{T} scaling in 20-40\% V0A multiplicity class2
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| v_{2}^{sub} \{2,|\Delta\eta| < 0.4\} / n_{q} with KE_{T} scaling in 0-20\% V0A multiplicity class
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| v_{2}^{sub} \{2,|\Delta\eta| < 0.4\} / n_{q} in 40-60\% V0A multiplicity class
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| v_{2}^{sub} \{2,|\Delta\eta| < 0.4\} / n_{q} in 20-40\% V0A multiplicity class
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| v_{2}^{sub} \{2,|\Delta\eta| < 0.4\} / n_{q} in 0-20\% V0A multiplicity class
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| v_{2}^{sub} \{2,|\Delta\eta| < 0.4\} in 40-60\% V0A multiplicity class
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| v_{2}^{sub} \{2,|\Delta\eta| < 0.4\} in 20-40\% V0A multiplicity class
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| v_{2}^{sub} \{2,|\Delta\eta| < 0.4\} of inclusive and identified hadrons in 0-20\% V0A multiplicity class
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| v_{2}^{sub} \{2,|\Delta\eta| < 0.4\} of \phi in various V0A multiplicity classes
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| v_{2}^{sub} \{2,|\Delta\eta| < 0.4\} of \Lambda(\bar{\Lambda}) in various V0A multiplicity classes
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| v_{2}^{sub} \{2,|\Delta\eta| < 0.4\} of K_{S}^{0} in various V0A multiplicity classes
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| v_{2}^{sub} \{2,|\Delta\eta| < 0.4\} of charged protons in various V0A multiplicity classes
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| v_{2}^{sub} \{2,|\Delta\eta| < 0.4\} of charged kaons in various V0A multiplicity classes
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| v_{2}^{sub} \{2,|\Delta\eta| < 0.4\} of charged pions in various V0A multiplicity classes
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| Charged Jet RAA in Pb-Pb 5.02TeV (R=0.2, R=0.3)
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| Charged Jet RAA in Pb-Pb 5.02TeV for 50-80% centrality (R=0.2, R=0.3)
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| Charged Jet RAA in Pb-Pb 5.02TeV for 30-50% centrality (R=0.2, R=0.3)
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| Charged Jet RAA in Pb-Pb 5.02TeV for 10-30% centrality (R=0.2, R=0.3)
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| Charged Jet RAA in Pb-Pb 5.02TeV for 0-10% centrality (R=0.2, R=0.3)
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| Charged Jet RAA in Pb-Pb 5.02TeV (R=0.3)
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| Charged Jet RAA in Pb-Pb 5.02TeV (R=0.2)
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| Charged jet cross section ratio of R=0.2 to R=0.3 in Pb-Pb 5.02TeV
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| Charged jet cross section ratio of R=0.2 to R=0.3 in Pb-Pb 5.02TeV for 50-80% centrality
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| Charged jet cross section ratio of R=0.2 to R=0.3 in Pb-Pb 5.02TeV for 30-50% centrality
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| Charged jet cross section ratio of R=0.2 to R=0.3 in Pb-Pb 5.02TeV for 10-30% centrality
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| Charged jet cross section ratio of R=0.2 to R=0.3 in Pb-Pb 5.02TeV for 0-10% centrality
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| Charged Jet RAA in Pb-Pb 5.02TeV for 50-80% centrality (R=0.3)
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| Charged Jet RAA in Pb-Pb 5.02TeV for 30-50% centrality (R=0.3)
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| Charged Jet RAA in Pb-Pb 5.02TeV for 10-30% centrality (R=0.3)
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| Charged Jet RAA in Pb-Pb 5.02TeV for 0-10% centrality (R=0.3)
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| Charged Jet RAA in Pb-Pb 5.02TeV for 50-80% centrality (R=0.2)
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| Charged Jet RAA in Pb-Pb 5.02TeV for 30-50% centrality (R=0.2)
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| Charged Jet RAA in Pb-Pb 5.02TeV for 10-30% centrality (R=0.2)
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| Charged Jet RAA in Pb-Pb 5.02TeV for 0-10% centrality (R=0.2)
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| TAA scaled charged Jet spectra in Pb-Pb 5.02TeV (R=0.3)
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| TAA scaled charged Jet spectra in Pb-Pb 5.02TeV (R=0.2)
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| rho_00 vs <Npart> for pT range 0.8 - 5.0 GeV/c w.r.t. Production plane for K*0 in Pb-Pb collisions at 2.76 and 5.02 TeV
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| rho_00 vs <Npart> for pT range 0.8 - 1.2 GeV/c w.r.t. Production plane for K*0 in Pb-Pb collisions at 2.76 and 5.02 TeV
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| rho_00 vs pT w.r.t. Production plane for K*0 in pp collisions at 13 TeV, Pb-Pb collisions at 2.76 and 5.02 TeV and K0s in Pb-Pb collisions at 2.76 TeV
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| rho_00 vs pT w.r.t. Production plane for K*0 in pp collisions at 13 TeV and Pb-Pb collisions at 2.76 and 5.02 TeV
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| cos(theta*) distribution for K*0 yields in Pb-Pb collisions at 5.02 TeV w.r.t. Production plane
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| Charged particle multiplicity as function of corrected SPD tracklets with linear fit to the total distribution and in different multiplicity intervals.
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| Corrected and uncorrected mean SPD tracklets within |η| < 1 as a function of Z vertex in p-Pb collisions at 8.16 TeV.
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| Self-normalized yield of electrons from heavy-flavour hadron decays in p-Pb collisions at 8.16 TeV with TPC+EMCal+DCal. -with D-mesons self-normalize yield in p-Pb collisions at 5.02 TeV
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| Self-normalized yield of electrons from heavy-flavour hadron decays in p-Pb collisions at 8.16 TeV with TPC+EMCal+DCal. -with HFE self-normalize in p-Pb collisions at 5.02 TeV
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| Pb--Pb 5.02 TeV $v_{2,2}(\eta_a, \eta_b)$ for 10--20% centrality
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| Empirical decorrelation parameter $F_2^\eta$ as a function of multiplicity for various $\Delta\eta$-gaps
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| Self-normalized yield of electrons from heavy-flavour hadron decays in p-Pb collisions at 8.16 TeV with TPC+EMCal+DCal.
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| Factorization ratio $f_2(\eta_a, \eta_b)$ for various centralities for $|\Delta\eta| > 2.6$ and 60-80% centrality
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| Factorization ratio $f_2(\eta_a, \eta_b)$ for various centralities for $|\Delta\eta| > 2.6$ and 0-5% centrality
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| Factorization ratio $f_2(\eta_a, \eta_b)$ for various centralities for $|\Delta\eta| > 3$ and 10-20% centrality
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| Factorization ratio $f_2(\eta_a, \eta_b)$ for various centralities for $|\Delta\eta| > 2$ and 10-20% centrality
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| Multiplicity distribution in p-Pb collisions at 8.16 TeV
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| Cluster energy distribution with EMCal and DCal detectors in p-Pb collisions at 8.16 TeV
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| Factorization ratio in the (eta_a, eta_b)-plane at 10-20% centrality for purely factorizing model $\Delta\eta > 2.6$
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| Projections of the factorization ratio onto $\Delta\eta$ for various centralities for $|\Delta\eta| > 2.6$
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| Ratio p/f0(pT) in pp collisions at 5.02 TeV
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| Ratio f0/phi(pT) in pp collisions at 5.02 TeV
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| Ratio f0/pi(pT) in pp collisions at 5.02 TeV
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| f0/pi vs. Energy at different energies
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| pT spectrum of f0(980) in inelastic pp collisions at 5.02 TeV (w/o B.R. correction)
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| pT spectrum of f0(980) in inelastic pp collisions at 5.02 TeV (w B.R. correction)
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| Rapidity slope of the J/ψ yield as a function of p_T in various centrality bins in Pb-Pb collisions at \sqrt{s_{NN}} = 5.02 TeV with ALICE
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| J/ψ yield in multi-differential bins in forward rapidity in Pb-Pb collisions at \sqrt{s_{NN}} = 5.02 TeV with ALICE
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| J/ψ yield in multi-differential bins in forward rapidity in Pb-Pb collisions at \sqrt{s_{NN}} = 5.02 TeV with ALICE
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| J/ψ yield in multi-differential bins in forward rapidity in Pb-Pb collisions at \sqrt{s_{NN}} = 5.02 TeV with ALICE
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| D-h azimuthal correlation distributions in 0-20%, 20-60%, 60-100% ZNA centrality for 8<pT(D)<16 GeV/c and pT(assoc)>0.3GeV/c.
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| D-h azimuthal correlation distributions in 0-20%, 20-60%, 60-100% ZNA centrality for 5<pT(D)<8 GeV/c and pT(assoc)>1GeV/c.
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| Width of the near-side peak at 5.02 TeV with large binning
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| Width of the near-side peak at 5.02 TeV
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| Comparison of near-side peak observables from D-h correlations vs ZNA centrality, in p-Pb collisions @ 5.02 TeV (2016)
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| D-h azimuthal correlation distributions in 0-20%, 20-60%, 60-100% ZNA centrality
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| Cross Section of Charged Jets (Anti-kT, R=0.3) Tagged with a D^{0} meson with $p_{\rm T,D} > 3 GeV/c$
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