| Reconstruction efficiency of D0 in charged jets, p-Pb at 5.02 TeV (Run2)
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| Raw D0- charged jets pT distributions, D0 pT intervals, p-Pb at 5.02 TeV (Run2)
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| D0 in charged jets invariant mass distributions, D0 pT intervals, p-Pb at 5.02 TeV (Run2)
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| Background fluctuations for D0-jet analysis, random cones with R=0.3, p-Pb collisions at 5.02 TeV (Run 2)
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| J/psi Raa in 0-90% Xe-Xe collisions at sqrt(s_NN)=5.44 TeV at mid-rapidity compared to the Xe-Xe results at fwd-y
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| J/psi Raa in 0-90% Xe-Xe collisions at sqrt(s_NN)=5.44 TeV at mid-rapidity compared to the Pb-Pb results
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| Multi-strange particles v3 in different centrality.
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| Multi-strange particles v2 in different centrality.
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| multi-strange particles v3/nq to pT/nq compare to other identified particles
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| multi-strange particles v2/nq to pT/nq compare to other identified particles
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| multi-strange particles v3 compare to other identified particles
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| multi-strange particles v2 compare to other identified particles
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| v2 signal extract of particle xi.
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| Direct and Inclusive Photon Production in pPb 5TeV with Theory
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| Direct and Inclusive Photon Production in pPb 5 TeV
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| Direct Photon Production in pPb 5TeV
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| Inclusive Photon Production in pPb 5 TeV
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| DCA template fit example
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| Spectrum of electrons from beauty hadron decays in Pb-Pb 5.02 TeV
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| RAA of electrons from beauty hadron decays in Pb-Pb 5.02 TeV - comparison with heavy-flavour electrons measurement
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| RAA of electrons from beauty hadron decays in Pb-Pb 5.02 TeV - comparison with models
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| RAA of electrons from beauty hadron decays in Pb-Pb 5.02 TeV - comparison with run1 measurement
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| Direct Photon Excess in pPb 5 TeV - individual techniques
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| Direct Photon Excess in pPb 5 TeV with Theory
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| Direct Photon Excess in pPb 5 TeV
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| Double ratio of the matching efficiencies for (anti-)deuteron
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| Double ratio of the matching efficiencies for (anti-)proton
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| Matching efficiency for (anti-)proton
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| Matching efficiency for (anti-)deuteron
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| Deuteron mass squared vs momentum in presence of TRD
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| Phi vs transverse momentum distribution for positive particles in presence of TRD
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| TPC performance plot.
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| Anti-hypertriton coalescence parameter B3 measured in Pb-Pb at 5.02 TeV in 10-40% centrality
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| Hypertriton coalescence parameter B3 measured in Pb-Pb at 5.02 TeV in 10-40% centrality
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| Strangeness population factor as a function of the centre-of-mass energy
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| Anti-hypertriton-to-hypertriton ratio as a function of the charged particle multiplicity in Pb-Pb at 5.02 TeV
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| Anti-hypertriton-to-hypertriton ratio as a function of the transverse momentum in 10-40% centrality
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| Hypertriton-over-light hadrons ratio in 0-10% centrality class compared with THERMUS predictions as a function of T_{chem}
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| (Anti-)hypertriton-over-(anti-)helium3 ratio as a function of the charged particle mutliplicity in Pb-Pb at 5.02 TeV
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| (Anti-)hypertriton dN/dy x B.R. compared to model predictions as a function of B.R.
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| Transverse momentum spectra of anti-hypertriton in 10-40% centrality class in Pb-Pb at 5.02 TeV
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| Transverse momentum spectra of hypertriton in 10-40% centrality class in Pb-Pb at 5.02 TeV
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| Transverse momentum spectra of (anti-)hypertriton in 10-40% centrality class in Pb-Pb at 5.02 TeV
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| (Anti-)hypertriton dN/dy x B.R. as a function of the charged particle multiplicity in Pb-Pb at 5.02 TeV
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| (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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