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Public Preliminary figures by analysis

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ID number ALI-PREL-XXX

Figure Caption

Scope: PWG

System

Energy

QM2019 h+jet correlations pp 13 TeV

Delta_recoil distribution as a function of azimuth for charged akt R=0.4 jets with 10< pT,jet<15 GeV/c in pp 13 TeV

Fig. Group : QM2019 h+jet correlations pp 13 TeV
PWG : PWG-JE (Jets)
Energy: 13 TeV
System: Pb-Pb

DEta-DPhi correlation functions in 13 TeV

Angular correlation functions for unlike-sign pairs of pions, kaons and protons

Fig. Group : DEta-DPhi correlation functions in 13 TeV
PWG : PWG-CF (Flow and Correlations)
Energy: 13 TeV
System: p-p

Angular correlations of like-sign particles (pions, kaons, protons) in pp collisions at 13 TeV

Fig. Group : DEta-DPhi correlation functions in 13 TeV
PWG : PWG-CF (Flow and Correlations)
Energy: 13 TeV
System: p-p

Projections of angular correlation functions for unlike-sign pairs of pions, kaons and protons

Fig. Group : DEta-DPhi correlation functions in 13 TeV
PWG : PWG-CF (Flow and Correlations)
Energy: 13 TeV
System: p-p

Projections of angular correlation functions for like-sign pairs of pions, kaons and protons

Fig. Group : DEta-DPhi correlation functions in 13 TeV
PWG : PWG-CF (Flow and Correlations)
Energy: 13 TeV
System: p-p

Preliminary - Neutral mesons in pp 5TeV and PbPb 5TeV

Eta - Ratio of individual measurements to combined - 0-10% centrality - PbPb 5TeV

Fig. Group : Preliminary - Neutral mesons in pp 5TeV and PbPb 5TeV
PWG : PWG-GA (Photons, Neutral Mesons)
Energy: 5.02 TeV
System: Pb-Pb

Eta to pi0 ratio - in-jet and MB - pp 5TeV

Fig. Group : Preliminary - Neutral mesons in pp 5TeV and PbPb 5TeV
PWG : PWG-GA (Photons, Neutral Mesons)
Energy: 5.02 TeV
System: p-p

Eta - in-jet and MB production - pp 5TeV

Fig. Group : Preliminary - Neutral mesons in pp 5TeV and PbPb 5TeV
PWG : PWG-GA (Photons, Neutral Mesons)
Energy: 5.02 TeV
System: p-p

Pi0 - in-jet and MB production - pp 5TeV

Fig. Group : Preliminary - Neutral mesons in pp 5TeV and PbPb 5TeV
PWG : PWG-GA (Photons, Neutral Mesons)
Energy: 5.02 TeV
System: p-p

Light-Flavour Hadron Production in pp Collisions at $\sqrt{s}$ = 13 TeV as a Function of $R_\textrm{T}$

$p_\textrm{T}$-differential model comparison of xi-to-pion ratio as a function of $R_\textrm{T}$ in the Away region for pp collisions at $\sqrt{s}$ = 13 TeV .

Fig. Group : Light-Flavour Hadron Production in pp Collisions at $\sqrt{s}$ = 13 TeV as a Function of $R_\textrm{T}$
PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
Energy: 13 TeV
System: p-p

$p_\textrm{T}$-differential model comparison of xi-to-pion ratio as a function of $R_\textrm{T}$ in the Transverse region for pp collisions at $\sqrt{s}$ = 13 TeV .

Fig. Group : Light-Flavour Hadron Production in pp Collisions at $\sqrt{s}$ = 13 TeV as a Function of $R_\textrm{T}$
PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
Energy: 13 TeV
System: p-p

$p_\textrm{T}$-differential model comparison of xi-to-pion ratio as a function of $R_\textrm{T}$ in the Toward region for pp collisions at $\sqrt{s}$ = 13 TeV .

Fig. Group : Light-Flavour Hadron Production in pp Collisions at $\sqrt{s}$ = 13 TeV as a Function of $R_\textrm{T}$
PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
Energy: 13 TeV
System: p-p

$p_\textrm{T}$-differential model comparison of kaon-to-pion ratio as a function of $R_\textrm{T}$ in the Away region for pp collisions at $\sqrt{s}$ = 13 TeV .

Fig. Group : Light-Flavour Hadron Production in pp Collisions at $\sqrt{s}$ = 13 TeV as a Function of $R_\textrm{T}$
PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
Energy: 13 TeV
System: p-p

$p_\textrm{T}$-differential model comparison of kaon-to-pion ratio as a function of $R_\textrm{T}$ in the Transverse region for pp collisions at $\sqrt{s}$ = 13 TeV .

Fig. Group : Light-Flavour Hadron Production in pp Collisions at $\sqrt{s}$ = 13 TeV as a Function of $R_\textrm{T}$
PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
Energy: 13 TeV
System: p-p

$p_\textrm{T}$-differential model comparison of kaon-to-pion ratio as a function of $R_\textrm{T}$ in the Toward region for pp collisions at $\sqrt{s}$ = 13 TeV .

Fig. Group : Light-Flavour Hadron Production in pp Collisions at $\sqrt{s}$ = 13 TeV as a Function of $R_\textrm{T}$
PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
Energy: 13 TeV
System: p-p

$p_\textrm{T}$-differential model comparison of proton-to-pion ratio as a function of $R_\textrm{T}$ in the Away region for pp collisions at $\sqrt{s}$ = 13 TeV .

Fig. Group : Light-Flavour Hadron Production in pp Collisions at $\sqrt{s}$ = 13 TeV as a Function of $R_\textrm{T}$
PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
Energy: 13 TeV
System: p-p

$p_\textrm{T}$-differential model comparison of proton-to-pion ratio as a function of $R_\textrm{T}$ in the Transverse region for pp collisions at $\sqrt{s}$ = 13 TeV .

Fig. Group : Light-Flavour Hadron Production in pp Collisions at $\sqrt{s}$ = 13 TeV as a Function of $R_\textrm{T}$
PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
Energy: 13 TeV
System: p-p

$p_\textrm{T}$-differential model comparison of proton-to-pion ratio as a function of $R_\textrm{T}$ in the Toward region for pp collisions at $\sqrt{s}$ = 13 TeV .

Fig. Group : Light-Flavour Hadron Production in pp Collisions at $\sqrt{s}$ = 13 TeV as a Function of $R_\textrm{T}$
PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
Energy: 13 TeV
System: p-p

$p_\textrm{T}$-differential model comparison of phi-to-pion ratio as a function of $R_\textrm{T}$ in the Away region for pp collisions at $\sqrt{s}$ = 13 TeV .

Fig. Group : Light-Flavour Hadron Production in pp Collisions at $\sqrt{s}$ = 13 TeV as a Function of $R_\textrm{T}$
PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
Energy: 13 TeV
System: p-p

$p_\textrm{T}$-differential model comparison of phi-to-pion ratio as a function of $R_\textrm{T}$ in the Transverse region for pp collisions at $\sqrt{s}$ = 13 TeV .

Fig. Group : Light-Flavour Hadron Production in pp Collisions at $\sqrt{s}$ = 13 TeV as a Function of $R_\textrm{T}$
PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
Energy: 13 TeV
System: p-p

$p_\textrm{T}$-differential model comparison of phi-to-pion ratio as a function of $R_\textrm{T}$ in the Toward region for pp collisions at $\sqrt{s}$ = 13 TeV .

Fig. Group : Light-Flavour Hadron Production in pp Collisions at $\sqrt{s}$ = 13 TeV as a Function of $R_\textrm{T}$
PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
Energy: 13 TeV
System: p-p

$p_\textrm{T}$-differential xi-to-pion ratio as a function of $R_\textrm{T}$ in the Away region for pp collisions at $\sqrt{s}$ = 13 TeV .

Fig. Group : Light-Flavour Hadron Production in pp Collisions at $\sqrt{s}$ = 13 TeV as a Function of $R_\textrm{T}$
PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
Energy: 13 TeV
System: p-p

$p_\textrm{T}$-differential xi-to-pion ratio as a function of $R_\textrm{T}$ in the Transverse region for pp collisions at $\sqrt{s}$ = 13 TeV .

Fig. Group : Light-Flavour Hadron Production in pp Collisions at $\sqrt{s}$ = 13 TeV as a Function of $R_\textrm{T}$
PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
Energy: 13 TeV
System: p-p

$p_\textrm{T}$-differential xi-to-pion ratio as a function of $R_\textrm{T}$ in the Toward region for pp collisions at $\sqrt{s}$ = 13 TeV .

Fig. Group : Light-Flavour Hadron Production in pp Collisions at $\sqrt{s}$ = 13 TeV as a Function of $R_\textrm{T}$
PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
Energy: 13 TeV
System: p-p

$p_\textrm{T}$-differential kaon-to-pion ratio as a function of $R_\textrm{T}$ in the Away region for pp collisions at $\sqrt{s}$ = 13 TeV .

Fig. Group : Light-Flavour Hadron Production in pp Collisions at $\sqrt{s}$ = 13 TeV as a Function of $R_\textrm{T}$
PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
Energy: 13 TeV
System: p-p

$p_\textrm{T}$-differential kaon-to-pion ratio as a function of $R_\textrm{T}$ in the Transverse region for pp collisions at $\sqrt{s}$ = 13 TeV .

Fig. Group : Light-Flavour Hadron Production in pp Collisions at $\sqrt{s}$ = 13 TeV as a Function of $R_\textrm{T}$
PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
Energy: 13 TeV
System: p-p

$p_\textrm{T}$-differential kaon-to-pion ratio as a function of $R_\textrm{T}$ in the Toward region for pp collisions at $\sqrt{s}$ = 13 TeV .

Fig. Group : Light-Flavour Hadron Production in pp Collisions at $\sqrt{s}$ = 13 TeV as a Function of $R_\textrm{T}$
PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
Energy: 13 TeV
System: p-p

$p_\textrm{T}$-differential proton-to-pion ratio as a function of $R_\textrm{T}$ in the Transverse region for pp collisions at $\sqrt{s}$ = 13 TeV .

Fig. Group : Light-Flavour Hadron Production in pp Collisions at $\sqrt{s}$ = 13 TeV as a Function of $R_\textrm{T}$
PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
Energy: 13 TeV
System: p-p

$p_\textrm{T}$-differential proton-to-pion ratio as a function of $R_\textrm{T}$ in the Toward region for pp collisions at $\sqrt{s}$ = 13 TeV .

Fig. Group : Light-Flavour Hadron Production in pp Collisions at $\sqrt{s}$ = 13 TeV as a Function of $R_\textrm{T}$
PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
Energy: 13 TeV
System: p-p

$p_\textrm{T}$-differential phi-to-pion ratio as a function of $R_\textrm{T}$ in the Away region for pp collisions at $\sqrt{s}$ = 13 TeV .

Fig. Group : Light-Flavour Hadron Production in pp Collisions at $\sqrt{s}$ = 13 TeV as a Function of $R_\textrm{T}$
PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
Energy: 13 TeV
System: p-p

$p_\textrm{T}$-differential phi-to-pion ratio as a function of $R_\textrm{T}$ in the Transverse region for pp collisions at $\sqrt{s}$ = 13 TeV .

Fig. Group : Light-Flavour Hadron Production in pp Collisions at $\sqrt{s}$ = 13 TeV as a Function of $R_\textrm{T}$
PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
Energy: 13 TeV
System: p-p

$p_\textrm{T}$-differential phi-to-pion ratio as a function of $R_\textrm{T}$ in the Toward region for pp collisions at $\sqrt{s}$ = 13 TeV .

Fig. Group : Light-Flavour Hadron Production in pp Collisions at $\sqrt{s}$ = 13 TeV as a Function of $R_\textrm{T}$
PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
Energy: 13 TeV
System: p-p

Low-mass Dielectrons in p-Pb collisions at sqrt(sNN) = 5.02 TeV with ALICE

Low-mass dielectron pT,ee (PYTHIA+EPS09, 1.04 < mee < 2.4, pt > 0.2)

Fig. Group : Low-mass Dielectrons in p-Pb collisions at sqrt(sNN) = 5.02 TeV with ALICE
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 5.02 TeV
System: p-Pb

Heavy-flavour jets with electrons in pp at 5.02 TeV

Cross section of heavy-flvaour jets with electrons in pp at 5.02 TeV with POWHEG (R=0.6)

Fig. Group : Heavy-flavour jets with electrons in pp at 5.02 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV
System: p-p

low pTee spectra

Low pT,ee spectrum in 0-40% centrality with calculations for thermal and photo-production dielectrons.

Fig. Group : low pTee spectra
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 5.02 TeV
System: Pb-Pb

Low pT,ee spectrum in 70-90% centrality with calculations for thermal and photo-production dielectrons.

Fig. Group : low pTee spectra
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 5.02 TeV
System: Pb-Pb

Low pT,ee spectrum in 0-40% centrality with Rapp prediction

Fig. Group : low pTee spectra
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 5.02 TeV
System: Pb-Pb

Low pT,ee spectrum in 70-90% centrality with Rapp prediction

Fig. Group : low pTee spectra
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 5.02 TeV
System: Pb-Pb

Low pT,ee spectrum in 0-40% centrality

Fig. Group : low pTee spectra
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 5.02 TeV
System: Pb-Pb

Low pT,ee spectrum in 70-90% centrality

Fig. Group : low pTee spectra
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 5.02 TeV
System: Pb-Pb

Transverse momentum spectra of charged particles as a function of Underlying Event activity in pp collisions at 13 TeV

Toward pT spectra

Fig. Group : Transverse momentum spectra of charged particles as a function of Underlying Event activity in pp collisions at 13 TeV
PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
Energy: 13 TeV
System: p-p

p-Pb 8 TeV min bias

RpPb jpsi at mid-rapidity in comparison with preliminary result at 5 TeV (min bias data)

Fig. Group : p-Pb 8 TeV min bias
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 8 TeV
System: p-Pb

pt differential RpPb jpsi at mid-rapidity (min bias data) at 8TeV in comparison with theory calculations

Fig. Group : p-Pb 8 TeV min bias
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 8 TeV
System: p-Pb

pt differential RpPb jpsi at mid-rapidity (min bias data) at 8TeV

Fig. Group : p-Pb 8 TeV min bias
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 8 TeV
System: p-Pb

RpPb jpsi at mid-rapidity in comparison with muon result at 8 TeV (min bias data) and theory calculations

Fig. Group : p-Pb 8 TeV min bias
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 8 TeV
System: p-Pb

RpPb jpsi at mid-rapidity in comparison with muon result at 8 TeV (min bias data)

Fig. Group : p-Pb 8 TeV min bias
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 8 TeV
System: p-Pb

Anti-matter interaction cross-sections with ALICE material

Anti-deuteron inelastic interaction cross-section with ALICE material

Fig. Group : Anti-matter interaction cross-sections with ALICE material
PWG : PWG-LF (Light Flavour Spectra)
Energy: 5.02 TeV
System: p-Pb

Anti-proton inelastic interaction cross-section with ALICE material

Fig. Group : Anti-matter interaction cross-sections with ALICE material
PWG : PWG-LF (Light Flavour Spectra)
Energy: 5.02 TeV
System: p-Pb

J/psi->mu+mu-

Comparison of J/ψ yield at mid and forward rapidity, as a function of the charged particle multiplicity densities at mid-rapidity

Fig. Group : J/psi->mu+mu-
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 13 TeV
System: p-p

J/ψ yield at forward-rapidity as a function of the charged particle multiplicity densities at mid-rapidity with the deviation from linearity

Fig. Group : J/psi->mu+mu-
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 13 TeV
System: p-p

J/ψ yield at forward-rapidity as a function of the charged particle multiplicity densities at mid-rapidity

Fig. Group : J/psi->mu+mu-
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 13 TeV
System: p-p

D0-tagged jets in pp collisions at 5.02 TeV (Run 2)

RpPb for D0-tagged jets at 5.02 TeV, linear scale on x-axis (for comparison with RAA, part 1)

Fig. Group : D0-tagged jets in pp collisions at 5.02 TeV (Run 2)
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV
System: p-p, p-Pb

RpPb and RAA for D0-tagged jets at 5.02 TeV, linear scale on x-axis

Fig. Group : D0-tagged jets in pp collisions at 5.02 TeV (Run 2)
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV
System: p-p, Pb-Pb, p-Pb

Reconstruction efficiency of D0-tagged charged jets, pp at 5.02 TeV (Run2)

Fig. Group : D0-tagged jets in pp collisions at 5.02 TeV (Run 2)
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV
System: p-p

Raw D0-tagged charged jets pT distributions, D0 pT intervals, pp at 5.02 TeV (Run2)

Fig. Group : D0-tagged jets in pp collisions at 5.02 TeV (Run 2)
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV
System: p-p

D0-tagged charged jets: invariant mass distributions in 3 D0 pT intervals, pp at 5.02 TeV (Run 2)

Fig. Group : D0-tagged jets in pp collisions at 5.02 TeV (Run 2)
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV
System: p-p

RpPb for D0-tagged jets at 5.02 TeV

Fig. Group : D0-tagged jets in pp collisions at 5.02 TeV (Run 2)
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV
System: p-p, p-Pb

Cross section of D0-tagged charged jets (anti-kT, R=0.3) with pT,D > 3 GeV/c, in pp and p-Pb at 5.02 TeV

Fig. Group : D0-tagged jets in pp collisions at 5.02 TeV (Run 2)
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV
System: p-p, p-Pb

RpPb and RAA for D0-tagged jets at 5.02 TeV

Fig. Group : D0-tagged jets in pp collisions at 5.02 TeV (Run 2)
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV
System: p-p, Pb-Pb, p-Pb

Cross section of D0-tagged jets in pp at 5.02 TeV

Fig. Group : D0-tagged jets in pp collisions at 5.02 TeV (Run 2)
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV
System: p-p

Production of V$^{0}$s and cascades in jets and the underlying event in pp collision at $\sqrt{s}=13$ TeV with ALICE

Xi to Lambda Ratio in jet within pp with jet R=0.4 Matching R=0.4

Fig. Group : Production of V$^{0}$s and cascades in jets and the underlying event in pp collision at $\sqrt{s}=13$ TeV with ALICE
PWG : PWG-JE (Jets)
Energy: 13 TeV
System: p-p

Scope: PAG Lambda to Kshort Ratio in jet within pp with jet R=0.4 Matching R=0.4

Fig. Group : Production of V$^{0}$s and cascades in jets and the underlying event in pp collision at $\sqrt{s}=13$ TeV with ALICE
PWG : PWG-JE (Jets)
Energy: 13 TeV
System: p-p

Low Mass -> e+e-

Dielectron mass spectra in pp (7 and 13 TeV) and PbPb (2.76 and 5.02 TeV) collisions

Fig. Group : Low Mass -> e+e-
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 2.76 TeV, 5.02 TeV, 7 TeV, 13 TeV
System: p-p, Pb-Pb

Upsilon -> mu+mu-

Comparison of Υ(1S) and Y(2S) yields at forward rapidity, as a function of the charged particle multiplicity at mid-rapidity

Fig. Group : Upsilon -> mu+mu-
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 13 TeV
System: p-p

Bottomonium production rate as a function of charged particle multiplicity

Fig. Group : Upsilon -> mu+mu-
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 13 TeV
System: p-p

Υ(2S) yield at forward-rapidity as a function of the charged particle multiplicity at mid-rapidity with the deviation from linearity

Fig. Group : Upsilon -> mu+mu-
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 13 TeV
System: p-p

Y(2S) yield at forward-rapidity as a function of the charged particle multiplicity densities at mid-rapidity

Fig. Group : Upsilon -> mu+mu-
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 13 TeV
System: p-p

Comparison of Υ(1S) and J/ψ yields at forward rapidity, as a function of the charged particle multiplicity at mid-rapidity

Fig. Group : Upsilon -> mu+mu-
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 13 TeV
System: p-p

Υ(1S) yield at forward-rapidity as a function of the charged particle multiplicity at mid-rapidity with the deviation from linearity

Fig. Group : Upsilon -> mu+mu-
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 13 TeV
System: p-p

Υ(1S) yield at forward-rapidity as a function of the charged particle multiplicity densities at mid-rapidity

Fig. Group : Upsilon -> mu+mu-
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 13 TeV
System: p-p

Pb-Pb 5.02 TeV Run 2015

Dielectron spectrum with Rapp predictions

Fig. Group : Pb-Pb 5.02 TeV Run 2015
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 5.02 TeV
System: Pb-Pb

Dielectron spectrum with PHSD predictions

Fig. Group : Pb-Pb 5.02 TeV Run 2015
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 5.02 TeV
System: Pb-Pb

Dielectron spectrum with cocktail incl EPS09-modified charm

Fig. Group : Pb-Pb 5.02 TeV Run 2015
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 5.02 TeV
System: Pb-Pb

Dielectron spectrum with cocktail incl EPPS16-modified charm

Fig. Group : Pb-Pb 5.02 TeV Run 2015
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 5.02 TeV
System: Pb-Pb

Dielectron spectrum with cocktail incl binary scaled charm

Fig. Group : Pb-Pb 5.02 TeV Run 2015
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 5.02 TeV
System: Pb-Pb

Preliminary: Neutral meson measurements in pPb collisions at $\sqrt{s}$ = 5.023 TeV as function of multiplicity (HP2018)

Eta/Pi0 in pPb collisions at 5TeV with K/pi - 0-20 & 60-100% V0A

Fig. Group : Preliminary: Neutral meson measurements in pPb collisions at $\sqrt{s}$ = 5.023 TeV as function of multiplicity (HP2018)
PWG : PWG-GA (Photons, Neutral Mesons)
Energy: 5.02 TeV
System: p-Pb

Eta/Pi0 in pPb collisions at 5TeV - ZNA sliced

Fig. Group : Preliminary: Neutral meson measurements in pPb collisions at $\sqrt{s}$ = 5.023 TeV as function of multiplicity (HP2018)
PWG : PWG-GA (Photons, Neutral Mesons)
Energy: 5.02 TeV
System: p-Pb

Eta/Pi0 in pPb collisions at 5TeV - CL1 sliced

Fig. Group : Preliminary: Neutral meson measurements in pPb collisions at $\sqrt{s}$ = 5.023 TeV as function of multiplicity (HP2018)
PWG : PWG-GA (Photons, Neutral Mesons)
Energy: 5.02 TeV
System: p-Pb

Eta/Pi0 in pPb collisions at 5TeV - V0A sliced

Fig. Group : Preliminary: Neutral meson measurements in pPb collisions at $\sqrt{s}$ = 5.023 TeV as function of multiplicity (HP2018)
PWG : PWG-GA (Photons, Neutral Mesons)
Energy: 5.02 TeV
System: p-Pb

Neutral Meson QpPb in pPb collisions at 5TeV together with other particles - 60-100 % V0A

Fig. Group : Preliminary: Neutral meson measurements in pPb collisions at $\sqrt{s}$ = 5.023 TeV as function of multiplicity (HP2018)
PWG : PWG-GA (Photons, Neutral Mesons)
Energy: 5.02 TeV
System: p-Pb

Neutral Meson QpPb in pPb collisions at 5TeV together with other particles - 60-100 % CL1

Fig. Group : Preliminary: Neutral meson measurements in pPb collisions at $\sqrt{s}$ = 5.023 TeV as function of multiplicity (HP2018)
PWG : PWG-GA (Photons, Neutral Mesons)
Energy: 5.02 TeV
System: p-Pb

Neutral Meson QpPb in pPb collisions at 5TeV together with other particles - 60-100 % ZNA - Hybrid Ncoll

Fig. Group : Preliminary: Neutral meson measurements in pPb collisions at $\sqrt{s}$ = 5.023 TeV as function of multiplicity (HP2018)
PWG : PWG-GA (Photons, Neutral Mesons)
Energy: 5.02 TeV
System: p-Pb

Neutral Meson QpPb in pPb collisions at 5TeV together with other particles - 0-20 % ZNA - Hybrid Ncoll

Fig. Group : Preliminary: Neutral meson measurements in pPb collisions at $\sqrt{s}$ = 5.023 TeV as function of multiplicity (HP2018)
PWG : PWG-GA (Photons, Neutral Mesons)
Energy: 5.02 TeV
System: p-Pb

Neutral Meson QpPb in pPb collisions at 5TeV together with other particles - 0-20 % V0A

Fig. Group : Preliminary: Neutral meson measurements in pPb collisions at $\sqrt{s}$ = 5.023 TeV as function of multiplicity (HP2018)
PWG : PWG-GA (Photons, Neutral Mesons)
Energy: 5.02 TeV
System: p-Pb

Neutral Meson QpPb in pPb collisions at 5TeV together with other particles - 0-20 % CL1

Fig. Group : Preliminary: Neutral meson measurements in pPb collisions at $\sqrt{s}$ = 5.023 TeV as function of multiplicity (HP2018)
PWG : PWG-GA (Photons, Neutral Mesons)
Energy: 5.02 TeV
System: p-Pb

Eta Meson QpPb in pPb collisions at 5TeV - ZNA sliced - Hybrid Ncoll

Fig. Group : Preliminary: Neutral meson measurements in pPb collisions at $\sqrt{s}$ = 5.023 TeV as function of multiplicity (HP2018)
PWG : PWG-GA (Photons, Neutral Mesons)
Energy: 5.02 TeV
System: p-Pb

Eta Meson QpPb in pPb collisions at 5TeV - V0A sliced

Fig. Group : Preliminary: Neutral meson measurements in pPb collisions at $\sqrt{s}$ = 5.023 TeV as function of multiplicity (HP2018)
PWG : PWG-GA (Photons, Neutral Mesons)
Energy: 5.02 TeV
System: p-Pb

Eta Meson QpPb in pPb collisions at 5TeV - CL1 sliced

Fig. Group : Preliminary: Neutral meson measurements in pPb collisions at $\sqrt{s}$ = 5.023 TeV as function of multiplicity (HP2018)
PWG : PWG-GA (Photons, Neutral Mesons)
Energy: 5.02 TeV
System: p-Pb

Neutral Pion QpPb in pPb collisions at 5TeV - ZNA sliced - Hybrid Ncoll

Fig. Group : Preliminary: Neutral meson measurements in pPb collisions at $\sqrt{s}$ = 5.023 TeV as function of multiplicity (HP2018)
PWG : PWG-GA (Photons, Neutral Mesons)
Energy: 5.02 TeV
System: p-Pb

Neutral Pion QpPb in pPb collisions at 5TeV - CL1 sliced

Fig. Group : Preliminary: Neutral meson measurements in pPb collisions at $\sqrt{s}$ = 5.023 TeV as function of multiplicity (HP2018)
PWG : PWG-GA (Photons, Neutral Mesons)
Energy: 5.02 TeV
System: p-Pb

Neutral Pion and Eta Meson Invariant Yield in pPb collisions at 5TeV compared to generators - 40-60% V0A

Fig. Group : Preliminary: Neutral meson measurements in pPb collisions at $\sqrt{s}$ = 5.023 TeV as function of multiplicity (HP2018)
PWG : PWG-GA (Photons, Neutral Mesons)
Energy: 5.02 TeV
System: p-Pb

Neutral Pion and Eta Meson Invariant Yield in pPb collisions at 5TeV compared to generators - 20-40% V0A

Fig. Group : Preliminary: Neutral meson measurements in pPb collisions at $\sqrt{s}$ = 5.023 TeV as function of multiplicity (HP2018)
PWG : PWG-GA (Photons, Neutral Mesons)
Energy: 5.02 TeV
System: p-Pb

Neutral Pion and Eta Meson Invariant Yield in pPb collisions at 5TeV compared to generators - 60-100% V0A

Fig. Group : Preliminary: Neutral meson measurements in pPb collisions at $\sqrt{s}$ = 5.023 TeV as function of multiplicity (HP2018)
PWG : PWG-GA (Photons, Neutral Mesons)
Energy: 5.02 TeV
System: p-Pb

Neutral Pion and Eta Meson Invariant Yield in pPb collisions at 5TeV compared to generators - 0-20% V0A

Fig. Group : Preliminary: Neutral meson measurements in pPb collisions at $\sqrt{s}$ = 5.023 TeV as function of multiplicity (HP2018)
PWG : PWG-GA (Photons, Neutral Mesons)
Energy: 5.02 TeV
System: p-Pb

Eta Meson Invariant Yield in pPb collisions at 5TeV - V0A sliced

Fig. Group : Preliminary: Neutral meson measurements in pPb collisions at $\sqrt{s}$ = 5.023 TeV as function of multiplicity (HP2018)
PWG : PWG-GA (Photons, Neutral Mesons)
Energy: 5.02 TeV
System: p-Pb

Eta Meson Invariant Yield in pPb collisions at 5TeV - CL1 sliced

Fig. Group : Preliminary: Neutral meson measurements in pPb collisions at $\sqrt{s}$ = 5.023 TeV as function of multiplicity (HP2018)
PWG : PWG-GA (Photons, Neutral Mesons)
Energy: 5.02 TeV
System: p-Pb

Eta Meson Invariant Yield in pPb collisions at 5TeV - ZNA sliced

Fig. Group : Preliminary: Neutral meson measurements in pPb collisions at $\sqrt{s}$ = 5.023 TeV as function of multiplicity (HP2018)
PWG : PWG-GA (Photons, Neutral Mesons)
Energy: 5.02 TeV
System: p-Pb

Neutral Pion Invariant Yield in pPb collisions at 5TeV - ZNA sliced

Fig. Group : Preliminary: Neutral meson measurements in pPb collisions at $\sqrt{s}$ = 5.023 TeV as function of multiplicity (HP2018)
PWG : PWG-GA (Photons, Neutral Mesons)
Energy: 5.02 TeV
System: p-Pb

Neutral Pion Invariant Yield in pPb collisions at 5TeV - CL1 sliced

Fig. Group : Preliminary: Neutral meson measurements in pPb collisions at $\sqrt{s}$ = 5.023 TeV as function of multiplicity (HP2018)
PWG : PWG-GA (Photons, Neutral Mesons)
Energy: 5.02 TeV
System: p-Pb

Neutral Pion Invariant Yield in pPb collisions at 5TeV - V0A sliced

Fig. Group : Preliminary: Neutral meson measurements in pPb collisions at $\sqrt{s}$ = 5.023 TeV as function of multiplicity (HP2018)
PWG : PWG-GA (Photons, Neutral Mesons)
Energy: 5.02 TeV
System: p-Pb

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