| (dN/dy)/<dN_ch/deta> for phi mesons as a function of average charged particle multiplicity in pp collisions at 5.02 TeV
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| phi Meson Invariant-Mass Distribution in pp Collisions at 5.02 TeV with Voigtian fit in V0M Multiplicity class VII
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| phi Meson Invariant-Mass Distribution in pp Collisions at 5.02 TeV in V0M Multiplicity class VII
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| pT Spectra of phi Mesons in pp Collisions at 5.02 TeV in V0M Multiplicity Event Classes
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| Model comparison of K*± yield in pp 8 TeV
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| Ratio of K*± pT spectra of 8 TeV and 13 TeV with respect to 5 TeV
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| K*± vs K*0 pT spectra in pp 8 TeV
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| K*± pT spectra in pp collisions at 8 TeV
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| f0(980) Acceptance times Efficiency correction
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| f0(980) signal extraction: fit to the LSB-subtracted π+π- invariant mass for 5 < pT < 6 GeV/c
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| f0(980) signal extraction: fit to the LSB-subtracted π+π- invariant mass for 1.5 < pT < 2 GeV/c
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| f0(980) signal extraction: fit to the LSB-subtracted π+π- invariant mass for 0 < pT < 0.3 GeV/c
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| f0(980) Invariant-Mass Distribution with Like-Sign Background, 5 < pT < 6 GeV/c
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| f0(980) Invariant-Mass Distribution with Like-Sign Background, 1.5 < pT < 2 GeV/c
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| f0(980) Invariant-Mass Distribution with Like-Sign Background, 0 < pT < 0.3 GeV/c
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| dNdy/<dNdeta> as a function of average chraged particle multiplicity of K*0 in p-Pb 8.16 TeV
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| pT spectra of K*0 for variuos V0A multiplicity classes in p-Pb Collisions at 8.16 TeV
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| pT spectrum of K*0 in p-Pb Collisions at 8.16 TeV
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| Invariant mass distribution of πK pair after background subtraction in p-Pb Collisions at 8.16 TeV
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| Invariant mass distribution of πK pair before background subtraction in p-Pb Collisions at 8.16 TeV
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| Invariant mass distribution of KK pair after background subtraction in p-Pb collisions at 8.16 TeV
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| pT spectra of phi for various V0A multiplicity classes in p-Pb collisions 8.16 TeV
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| pT spectraum of phi in pPb collisions at 8.16 TeV
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| Invariant mass distribution of KK pair before background subtraction in pPb collisions at 8.16 TeV
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| pT-differential proton-to-pion ratio in V0M 0-10%, high and low spherocities with comparison to PYTHIA 8 and EPOS LHC
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| pT-differential proton-to-pion ratio in V0M 0-10%, high and low spherocities
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| pT-differential kaon-to-pion ratio in V0M 0-10%, high and low spherocities with comparison to PYTHIA 8 and EPOS LHC
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| pT-differential kaon-to-pion ratio in V0M 0-10%, high and low spherocities
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| Corrected D$^0$ relative yield per event as a function of spherocity, in pp collisions at $\sqrt{s} = 7$ TeV in different $p_{\rm{T}}$ intervals and multiplicity interval of $30 < {\rm N}_{\rm tracklets} < 81$.
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| Corrected D$^0$ relative yield per event as a function of spherocity, in pp collisions at $\sqrt{s} = 7$ TeV in different $p_{\rm{T}}$ intervals and multiplicity interval of $20 < {\rm N}_{\rm tracklets} < 30$.
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| Corrected D$^0$ relative yield per event as a function of spherocity, in pp collisions at $\sqrt{s} = 7$ TeV in different $p_{\rm{T}}$ intervals and multiplicity interval of $20 < {\rm N}_{\rm tracklets} < 81$.
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| True spherocity versus measured spherocity for events with at least one D$^0$ in pp collisions at $\sqrt{s} = 7$ TeV for multiplicity interval of $30 < {\rm N}_{\rm tracklets} < 81$.
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| True spherocity versus measured spherocity for events with at least one D$^0$ in pp collisions at $\sqrt{s} = 7$ TeV for multiplicity interval of $20 < {\rm N}_{\rm tracklets} < 30$.
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| True spherocity versus measured spherocity for events with at least one D$^0$ in pp collisions at $\sqrt{s} = 7$ TeV for multiplicity interval of $20 < {\rm N}_{\rm tracklets} < 81$.
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| True spherocity versus measured spherocity for events with at least one D$^0$ in pp collisions at $\sqrt{s} = 7$ TeV.
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| D$^0$ reconstruction efficiency (feed-down D$^0$) as a function of $p_{\rm{T}}$, in pp collisions at $\sqrt{s} = 7$ TeV in different spherocity intervals for multiplicity interval of $20 < {\rm N}_{\rm tracklets} < 81$.
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| D$^0$ reconstruction efficiency (prompt D$^0$) as a function of $p_{\rm{T}}$, in pp collisions at $\sqrt{s} = 7$ TeV in different spherocity intervals for multiplicity interval of $20 < {\rm N}_{\rm tracklets} < 81$.
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| D$^0$ reconstruction efficiency (prompt D$^0$) as a function of spherocity, in pp collisions at $\sqrt{s} = 7$ TeV in different $p_{\rm{T}}$ intervals for multiplicity interval of $20 < {\rm N}_{\rm tracklets} < 81$.
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| D$^0$ invariant-mass distribution in pp collisions at $sqrt{s} =$ 7 TeV for $8 < p_{\rm{T}} < 12$ GeV/$c$ and multiplicity interval of $20 < {\rm N}_{\rm tracklets} < 81$ for three spherocity intervals (0.00, 0.40, 0.55, 1.00).
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| D$^0$ invariant-mass distribution in pp collisions at $sqrt{s} =$ 7 TeV for $4 < p_{\rm{T}} < 8$ GeV/$c$ and multiplicity interval of $20 < {\rm N}_{\rm tracklets} < 81$ for four spherocity intervals (0.00, 0.40, 0.55, 0.70, 1.00).
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| D$^0$ invariant-mass distribution in pp collisions at $sqrt{s} =$ 7 TeV for $2 < p_{\rm{T}} < 4$ GeV/$c$ and multiplicity interval of $20 < {\rm N}_{\rm tracklets} < 81$ for four spherocity intervals (0.00, 0.40, 0.55, 0.70, 1.00).
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| D$^0$ invariant-mass distribution in pp collisions at $sqrt{s} =$ 7 TeV for integrated spherocity in three $p_{\rm{T}}$ intervals (2, 4, 8, 12) GeV/$c$ for multiplicity interval of $20 < {\rm N}_{\rm tracklets} < 81$.
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| Background fluctuations estimated using random cones with R=0.4 in p-Pb collisions at 5.02 TeV (Run 2)
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| Raw D* - charged jets pT distributions, D* pT intervals, p-Pb at 5.02 TeV (Run2)
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| Dstar cross section in pp collisions at 7 TeV compared to POWHEG+PYTHIA6
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| D0 cross section in pp collisions at 7 TeV compared to POWHEG+PYTHIA6
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| Dplus cross section in pp collisions at 7 TeV compared to POWHEG+PYTHIA6
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| Ds invariant mass distribution in pp collisions at 13 TeV (pT [4,6] GeV/c)
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| Mean pT in Backward window vs mean pT in Forward window (with corresponding profile) in centrality class 0-80% (by V0M) in Pb-Pb collisions at 2.76 TeV
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| Mean pT in Backward window vs mean pT in Forward window (with corresponding profile) in centrality class 0-40% (by V0M) in Pb-Pb collisions at 2.76 TeV
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| Mean pT in Backward window vs mean pT in Forward window (with corresponding profile) in centrality class 75-80% (by V0M) in Pb-Pb collisions at 2.76 TeV
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| Mean pT in Backward window vs mean pT in Forward window (with corresponding profile) in centrality class 0-5% (by V0M) in Pb-Pb collisions at 2.76 TeV
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| Mean pT in Backward window vs mean pT in Forward window (with corresponding profile) in centrality class 70-80% (by V0M) in Pb-Pb collisions at 2.76 TeV
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| Mean pT in Backward window vs mean pT in Forward window (with corresponding profile) in centrality class 50-60% (by V0M) in Pb-Pb collisions at 2.76 TeV
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| Mean pT in Backward window vs mean pT in Forward window (with corresponding profile) in centrality class 30-40% (by V0M) in Pb-Pb collisions at 2.76 TeV
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| Mean pT in Backward window vs mean pT in Forward window (with corresponding profile) in centrality class 0-10% (by V0M) in Pb-Pb collisions at 2.76 TeV
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| Average values of mean pT in Backward window as a function of mean pT in Forward window: centrality class of 80% width (by V0M) in Pb-Pb collisions at 2.76 TeV
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| Average values of mean pT in Backward window as a function of mean pT in Forward window: several centrality classes of 40% width (by V0M) in Pb-Pb collisions at 2.76 TeV
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| Average values of mean pT in Backward window as a function of mean pT in Forward window: several centrality classes of 20% width (by V0M) in Pb-Pb collisions at 2.76 TeV
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| Average values of mean pT in Backward window as a function of mean pT in Forward window: several centrality classes of 10% width (by V0M) in Pb-Pb collisions at 2.76 TeV
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| Average values of mean pT in Backward window as a function of mean pT in Forward window: several centrality classes of 5% width (by V0M) in Pb-Pb collisions at 2.76 TeV
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| Pion spectra comparison in real and measured spherocities
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| Real-measured spherocity correlation matrix in V0M 0-10% multiplicity events
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| pT-differential proton-to-pion ratio in V0M 0-10%, high and low spherocities with comparison to Monte-Carlo
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| pT-differential kaon-to-pion ratio in V0M 0-10%, high and low spherocities with comparison to Monte-Carlo
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| pT-differential proton yield in V0M 0-10%, high and low spherocities
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| pT-differential kaon yield in V0M 0-10%, high and low spherocities
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| pT-differential pion yield in V0M 0-10%, high and low spherocities
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| Ratios of pT spectra of K*± in minimum bias INEL pp collisions at 13 TeV to 5.02 TeV
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| K*± pT spectra
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| K*± vs K*0 pT spectra
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| Strength of event-mean transverse momenta correlations (bcorr) in centrality classes of 5% width in Pb-Pb collisions at 2.76 TeV at three η-gaps 0, 0.6 and 1.2 in comparison with AMPT
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| Strength of event-mean transverse momenta correlations (bcorr) in centrality classes (2% width) by V0M, ZDCvsZEM and CL1 in Pb-Pb collisions at 2.76 TeV
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| Strength of event-mean transverse momenta correlations (bcorr) in centrality classes (5% width) by V0M, ZDCvsZEM and CL1 in Pb-Pb collisions at 2.76 TeV
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| Cross Section of Charged Jets (Anti-kT, R=0.4) Tagged with a D^{*} meson with $p_{\rm T,D} > 3 GeV/c$
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| Reconstruction efficiency of D* in charged jets, p-Pb at 5.02 TeV (Run2)
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| D* in charged jets invariant mass distributions, D* pT intervals, p-Pb at 5.02 TeV (Run2)
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| D* in charged jets invariant mass distributions, jet pT intervals, p-Pb at 5.02 TeV (Run2)
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| Heavy-flavour muon yield in pt bins vs. event multiplicity in pp collisions at 8 TeV: comparison with D meson measurements at 7 TeV
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| y-differential cross section of muons from heavy flavour decays in pp collisions at 8 TeV (high pt)
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| y-differential cross section of muons from heavy flavour decays in pp collisions at 8 TeV (low pt)
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| y-differential cross section of muons from heavy flavour decays in pp collisions at 8 TeV
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| Ratio between data and FONLL calculations vs pt in different rapidity regions in pp collisions at 8 TeV
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| pt-differential cross sections of muons from heavy flavour decays in different rapidity regions in pp collisions at 8 TeV
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| pt-differential cross section of muons from heavy flavour decays in pp collisions at 8 TeV
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| Heavy-flavour muon yield in pt bins vs. event multiplicity in pp collisions at 8 TeV: comparison with EPOS predictions
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| Heavy-flavour muon yield in pt bins vs. event multiplicity in pp collisions at 8 TeV
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| Comparison of D-h away-side observables in p-Pb @ 5.02 TeV (2016) and from model predictions (higher pT ranges)
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| Comparison of D-h away-side observables in p-Pb @ 5.02 TeV (2016) and from model predictions (lower pT ranges)
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| Comparison of D-h near-side observables in p-Pb @ 5.02 TeV (2016) and from model predictions (higher pT ranges)
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| Comparison of D-h near-side observables in p-Pb @ 5.02 TeV (2016) and from model predictions (lower pT ranges)
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| Heavy-flavour muon yield vs. event multiplicity in pp collisions at 8 TeV
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| v_2 of inclusive charged hadrons, K0s, Lambda and Phi in centrality 0-20% with published pi,K,p results from Run 1
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| Comparison of D-h correlation distributions in p-Pb @ 5.02 TeV (2016) and from model predictions (2/2)
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| Comparison of D-h correlation distributions in p-Pb @ 5.02 TeV (2016) and from model predictions (1/2)
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| Fit of D-h correlation distribution, for 5 < pT(D) < 8 GeV/c and pT(assoc) > 1 GeV/c, on p-Pb @ 5.02 TeV.
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| Comparison of near-side observables from D-h correlations in pp @ 7 TeV and p-Pb @ 5.02 TeV (2016)
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| Comparison of D-h correlation distributions in pp @ 7 TeV and p-Pb @ 5.02 TeV (2016)
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| D-h correlation distribution, for 5 < pT(D) < 8 GeV/c and pT(assoc) > 1 GeV/c, on p-Pb @ 5.02 TeV.
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| phi Raa as a function of pT in Pb-Pb collisions at 5.02 TeV for 0-10% and 60-90% centrality
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