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Scope: PWG

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Delta recoil distributions for 15<pT,jet<20 GeV jet as measured by ALICE compated to PYTHIA events embedded to MB and HM pp 13 TeV Fig. Group : QM2019 h+jet correlations pp 13 TeV PWG : PWG-JE (Jets) Energy: 13 TeV System Pb-Pb
Delta recoil distributions as measured by ALICE compated to PYTHIA events embedded to MB and HM pp 13 TeV Fig. Group : QM2019 h+jet correlations pp 13 TeV PWG : PWG-JE (Jets) Energy: 13 TeV System Pb-Pb
Delta recoil distributions as measured by ALICE and simulated by PYTHIA8 particle level in MB and HM pp 13 TeV Fig. Group : QM2019 h+jet correlations pp 13 TeV PWG : PWG-JE (Jets) Energy: 13 TeV System Pb-Pb
Per trigger normalized yield of 15<pT,jet<20 GeV recoil jets in MB and HM events for TT{20,30} in pp 13 TeV Fig. Group : QM2019 h+jet correlations pp 13 TeV PWG : PWG-JE (Jets) Energy: 13 TeV System Pb-Pb
Delta_recoil distribution as a function of azimuth for charged akt R=0.4 jets with 40< pT,jet<60 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
Delta_recoil distribution as a function of azimuth for charged akt R=0.4 jets with 20< pT,jet<30 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
Delta_recoil distribution as a function of azimuth for charged akt R=0.4 jets with 15< pT,jet<20 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
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
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
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
$p_\textrm{T}$-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
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
$p_\textrm{T}$-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
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 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
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
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
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
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
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
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
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
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 , System p-Pb
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
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 , Energy: 5.02 TeV , Energy: 7 TeV , Energy: 13 TeV System p-p , System Pb-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 , System Pb-Pb , System p-Pb
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
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
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 , System 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 , System 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 , System Pb-Pb , System 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
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
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
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

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