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Scope: PWG

System

Energy

QM2018 (poster) Factorization of two-particle distributions from (5.02 TeV Pb--Pb collisions)

Factorization ratio $f_2(\eta_a, \eta_b)$ for various centralities for $|\Delta\eta| > 2.6$ and 60-80% centrality

Fig. Group : QM2018 (poster) Factorization of two-particle distributions from (5.02 TeV Pb--Pb collisions)
PWG : PWG-CF (Flow and Correlations)
Energy: 5.02 TeV
System: Pb-Pb

Factorization ratio $f_2(\eta_a, \eta_b)$ for various centralities for $|\Delta\eta| > 2.6$ and 0-5% centrality

Fig. Group : QM2018 (poster) Factorization of two-particle distributions from (5.02 TeV Pb--Pb collisions)
PWG : PWG-CF (Flow and Correlations)
Energy: 5.02 TeV
System: Pb-Pb

Factorization ratio $f_2(\eta_a, \eta_b)$ for various centralities for $|\Delta\eta| > 3$ and 10-20% centrality

Fig. Group : QM2018 (poster) Factorization of two-particle distributions from (5.02 TeV Pb--Pb collisions)
PWG : PWG-CF (Flow and Correlations)
Energy: 5.02 TeV
System: Pb-Pb

Factorization ratio $f_2(\eta_a, \eta_b)$ for various centralities for $|\Delta\eta| > 2$ and 10-20% centrality

Fig. Group : QM2018 (poster) Factorization of two-particle distributions from (5.02 TeV Pb--Pb collisions)
PWG : PWG-CF (Flow and Correlations)
Energy: 5.02 TeV
System: Pb-Pb

Factorization ratio in the (eta_a, eta_b)-plane at 10-20% centrality for purely factorizing model $\Delta\eta > 2.6$

Fig. Group : QM2018 (poster) Factorization of two-particle distributions from (5.02 TeV Pb--Pb collisions)
PWG : PWG-CF (Flow and Correlations)
Energy: 5.02 TeV
System: Pb-Pb

Projections of the factorization ratio onto $\Delta\eta$ for various centralities for $|\Delta\eta| > 2.6$

Fig. Group : QM2018 (poster) Factorization of two-particle distributions from (5.02 TeV Pb--Pb collisions)
PWG : PWG-CF (Flow and Correlations)
Energy: 5.02 TeV
System: Pb-Pb

Heavy-flavour decay electron vs. multiplicity in p-Pb collisions at 8.16 TeV

Multiplicity distribution in p-Pb collisions at 8.16 TeV

Fig. Group : Heavy-flavour decay electron vs. multiplicity in p-Pb collisions at 8.16 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 8 TeV
System: p-Pb

Cluster energy distribution with EMCal and DCal detectors in p-Pb collisions at 8.16 TeV

Fig. Group : Heavy-flavour decay electron vs. multiplicity in p-Pb collisions at 8.16 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 8 TeV
System: p-Pb

f0(980) in pp collisions at 5.02 TeV [QM18]

Ratio p/f0(pT) in pp collisions at 5.02 TeV

Fig. Group : f0(980) in pp collisions at 5.02 TeV [QM18]
PWG : PWG-LF (Light Flavour Spectra)
Energy: 5.02 TeV
System: p-p

Ratio f0/phi(pT) in pp collisions at 5.02 TeV

Fig. Group : f0(980) in pp collisions at 5.02 TeV [QM18]
PWG : PWG-LF (Light Flavour Spectra)
Energy: 5.02 TeV
System: p-p

Ratio f0/pi(pT) in pp collisions at 5.02 TeV

Fig. Group : f0(980) in pp collisions at 5.02 TeV [QM18]
PWG : PWG-LF (Light Flavour Spectra)
Energy: 5.02 TeV
System: p-p

f0/pi vs. Energy at different energies

Fig. Group : f0(980) in pp collisions at 5.02 TeV [QM18]
PWG : PWG-LF (Light Flavour Spectra)
Energy: 5.02 TeV
System: p-p

pT spectrum of f0(980) in inelastic pp collisions at 5.02 TeV (w/o B.R. correction)

Fig. Group : f0(980) in pp collisions at 5.02 TeV [QM18]
PWG : PWG-LF (Light Flavour Spectra)
Energy: 5.02 TeV
System: p-p

pT spectrum of f0(980) in inelastic pp collisions at 5.02 TeV (w B.R. correction)

Fig. Group : f0(980) in pp collisions at 5.02 TeV [QM18]
PWG : PWG-LF (Light Flavour Spectra)
Energy: 5.02 TeV
System: p-p

f0(980) Acceptance times Efficiency correction

Fig. Group : f0(980) in pp collisions at 5.02 TeV [QM18]
PWG : PWG-LF (Light Flavour Spectra)
Energy: 5.02 TeV
System: p-p

f0(980) signal extraction: fit to the LSB-subtracted π+π- invariant mass for 5 < pT < 6 GeV/c

Fig. Group : f0(980) in pp collisions at 5.02 TeV [QM18]
PWG : PWG-LF (Light Flavour Spectra)
Energy: 5.02 TeV
System: p-p

f0(980) signal extraction: fit to the LSB-subtracted π+π- invariant mass for 1.5 < pT < 2 GeV/c

Fig. Group : f0(980) in pp collisions at 5.02 TeV [QM18]
PWG : PWG-LF (Light Flavour Spectra)
Energy: 5.02 TeV
System: p-p

f0(980) signal extraction: fit to the LSB-subtracted π+π- invariant mass for 0 < pT < 0.3 GeV/c

Fig. Group : f0(980) in pp collisions at 5.02 TeV [QM18]
PWG : PWG-LF (Light Flavour Spectra)
Energy: 5.02 TeV
System: p-p

f0(980) Invariant-Mass Distribution with Like-Sign Background, 5 < pT < 6 GeV/c

Fig. Group : f0(980) in pp collisions at 5.02 TeV [QM18]
PWG : PWG-LF (Light Flavour Spectra)
Energy: 5.02 TeV
System: p-p

f0(980) Invariant-Mass Distribution with Like-Sign Background, 1.5 < pT < 2 GeV/c

Fig. Group : f0(980) in pp collisions at 5.02 TeV [QM18]
PWG : PWG-LF (Light Flavour Spectra)
Energy: 5.02 TeV
System: p-p

f0(980) Invariant-Mass Distribution with Like-Sign Background, 0 < pT < 0.3 GeV/c

Fig. Group : f0(980) in pp collisions at 5.02 TeV [QM18]
PWG : PWG-LF (Light Flavour Spectra)
Energy: 5.02 TeV
System: p-p

Multi-differential studies of the jpsi production in PbPb collisions at sqrt(S_NN) = 5.02 TeV

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

Fig. Group : Multi-differential studies of the jpsi production in PbPb collisions at sqrt(S_NN) = 5.02 TeV
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 5.02 TeV
System: Pb-Pb

J/ψ yield in multi-differential bins in forward rapidity in Pb-Pb collisions at \sqrt{s_{NN}} = 5.02 TeV with ALICE

Fig. Group : Multi-differential studies of the jpsi production in PbPb collisions at sqrt(S_NN) = 5.02 TeV
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 5.02 TeV
System: Pb-Pb

J/ψ yield in multi-differential bins in forward rapidity in Pb-Pb collisions at \sqrt{s_{NN}} = 5.02 TeV with ALICE

Fig. Group : Multi-differential studies of the jpsi production in PbPb collisions at sqrt(S_NN) = 5.02 TeV
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 5.02 TeV
System: Pb-Pb

J/ψ yield in multi-differential bins in forward rapidity in Pb-Pb collisions at \sqrt{s_{NN}} = 5.02 TeV with ALICE

Fig. Group : Multi-differential studies of the jpsi production in PbPb collisions at sqrt(S_NN) = 5.02 TeV
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 5.02 TeV
System: Pb-Pb

D-h azimuthal correlations in p-Pb collisions @ 5.02 TeV(2016) vs ZNA centrality

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.

Fig. Group : D-h azimuthal correlations in p-Pb collisions @ 5.02 TeV(2016) vs ZNA centrality
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV
System: p-Pb

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.

Fig. Group : D-h azimuthal correlations in p-Pb collisions @ 5.02 TeV(2016) vs ZNA centrality
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV
System: p-Pb

Comparison of near-side peak observables from D-h correlations vs ZNA centrality, in p-Pb collisions @ 5.02 TeV (2016)

Fig. Group : D-h azimuthal correlations in p-Pb collisions @ 5.02 TeV(2016) vs ZNA centrality
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV
System: p-Pb

D-h azimuthal correlation distributions in 0-20%, 20-60%, 60-100% ZNA centrality

Fig. Group : D-h azimuthal correlations in p-Pb collisions @ 5.02 TeV(2016) vs ZNA centrality
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV
System: p-Pb

QM2018 (talk) Multiplicity evolution of the nearside peak in Pb-Pb 5.02 TeV

Width of the near-side peak at 5.02 TeV with large binning

Fig. Group : QM2018 (talk) Multiplicity evolution of the nearside peak in Pb-Pb 5.02 TeV
PWG : PWG-CF (Flow and Correlations)
Energy: 5.02 TeV
System: p-p, Pb-Pb

Width of the near-side peak at 5.02 TeV

Fig. Group : QM2018 (talk) Multiplicity evolution of the nearside peak in Pb-Pb 5.02 TeV
PWG : PWG-CF (Flow and Correlations)
Energy: 5.02 TeV
System: p-p, Pb-Pb

D0 jets in p-Pb at 5 TeV (Run2)

Cross Section of Charged Jets (Anti-kT, R=0.3) Tagged with a D^{0} meson with $p_{\rm T,D} > 3 GeV/c$

Fig. Group : D0 jets in p-Pb at 5 TeV (Run2)
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV
System: p-Pb

Reconstruction efficiency of D0 in charged jets, p-Pb at 5.02 TeV (Run2)

Fig. Group : D0 jets in p-Pb at 5 TeV (Run2)
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV
System: p-Pb

Raw D0- charged jets pT distributions, D0 pT intervals, p-Pb at 5.02 TeV (Run2)

Fig. Group : D0 jets in p-Pb at 5 TeV (Run2)
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV
System: p-Pb

D0 in charged jets invariant mass distributions, D0 pT intervals, p-Pb at 5.02 TeV (Run2)

Fig. Group : D0 jets in p-Pb at 5 TeV (Run2)
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV
System: p-Pb

Background fluctuations for D0-jet analysis, random cones with R=0.3, p-Pb collisions at 5.02 TeV (Run 2)

Fig. Group : D0 jets in p-Pb at 5 TeV (Run2)
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV
System: p-Pb

J/psi nuclear modification factor in Xe-Xe collisions at sqrt(sNN)=5.44 TeV

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

Fig. Group : J/psi nuclear modification factor in Xe-Xe collisions at sqrt(sNN)=5.44 TeV
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 5.44 TeV
System: Xe-Xe

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

Fig. Group : J/psi nuclear modification factor in Xe-Xe collisions at sqrt(sNN)=5.44 TeV
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 5.44 TeV
System: Xe-Xe

QM2018 (poster) Anisotropic flow of multi-strange particles in Pb--Pb collisions at sqrts = 5.02 TeV

Multi-strange particles v3 in different centrality.

Fig. Group : QM2018 (poster) Anisotropic flow of multi-strange particles in Pb--Pb collisions at sqrts = 5.02 TeV
PWG : PWG-CF (Flow and Correlations)
Energy: 5.02 TeV
System: Pb-Pb

Multi-strange particles v2 in different centrality.

Fig. Group : QM2018 (poster) Anisotropic flow of multi-strange particles in Pb--Pb collisions at sqrts = 5.02 TeV
PWG : PWG-CF (Flow and Correlations)
Energy: 5.02 TeV
System: Pb-Pb

multi-strange particles v3/nq to pT/nq compare to other identified particles

Fig. Group : QM2018 (poster) Anisotropic flow of multi-strange particles in Pb--Pb collisions at sqrts = 5.02 TeV
PWG : PWG-CF (Flow and Correlations)
Energy: 5.02 TeV
System: Pb-Pb

multi-strange particles v2/nq to pT/nq compare to other identified particles

Fig. Group : QM2018 (poster) Anisotropic flow of multi-strange particles in Pb--Pb collisions at sqrts = 5.02 TeV
PWG : PWG-CF (Flow and Correlations)
Energy: 5.02 TeV
System: Pb-Pb

multi-strange particles v3 compare to other identified particles

Fig. Group : QM2018 (poster) Anisotropic flow of multi-strange particles in Pb--Pb collisions at sqrts = 5.02 TeV
PWG : PWG-CF (Flow and Correlations)
Energy: 5.02 TeV
System: Pb-Pb

multi-strange particles v2 compare to other identified particles

Fig. Group : QM2018 (poster) Anisotropic flow of multi-strange particles in Pb--Pb collisions at sqrts = 5.02 TeV
PWG : PWG-CF (Flow and Correlations)
Energy: 5.02 TeV
System: Pb-Pb

v2 signal extract of particle xi.

Fig. Group : QM2018 (poster) Anisotropic flow of multi-strange particles in Pb--Pb collisions at sqrts = 5.02 TeV
PWG : PWG-CF (Flow and Correlations)
Energy: 5.02 TeV
System: Pb-Pb

Preliminary: Direct photons in pPb 5TeV

Direct and Inclusive Photon Production in pPb 5TeV with Theory

Fig. Group : Preliminary: Direct photons in pPb 5TeV
PWG : PWG-GA (Photons, Neutral Mesons)
Energy: 5.02 TeV
System: p-Pb

Direct and Inclusive Photon Production in pPb 5 TeV

Fig. Group : Preliminary: Direct photons in pPb 5TeV
PWG : PWG-GA (Photons, Neutral Mesons)
Energy: 5.02 TeV
System: p-Pb

Direct Photon Production in pPb 5TeV

Fig. Group : Preliminary: Direct photons in pPb 5TeV
PWG : PWG-GA (Photons, Neutral Mesons)
Energy: 5.02 TeV
System: p-Pb

Inclusive Photon Production in pPb 5 TeV

Fig. Group : Preliminary: Direct photons in pPb 5TeV
PWG : PWG-GA (Photons, Neutral Mesons)
Energy: 5.02 TeV
System: p-Pb

Direct Photon Excess in pPb 5 TeV - individual techniques

Fig. Group : Preliminary: Direct photons in pPb 5TeV
PWG : PWG-GA (Photons, Neutral Mesons)
Energy: 5.02 TeV
System: p-Pb

Direct Photon Excess in pPb 5 TeV with Theory

Fig. Group : Preliminary: Direct photons in pPb 5TeV
PWG : PWG-GA (Photons, Neutral Mesons)
Energy: 5.02 TeV
System: p-Pb

Direct Photon Excess in pPb 5 TeV

Fig. Group : Preliminary: Direct photons in pPb 5TeV
PWG : PWG-GA (Photons, Neutral Mesons)
Energy: 5.02 TeV
System: p-Pb

Electrons from beauty hadron decays in Pb-Pb 2015

DCA template fit example

Fig. Group : Electrons from beauty hadron decays in Pb-Pb 2015
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV
System: Pb-Pb

Spectrum of electrons from beauty hadron decays in Pb-Pb 5.02 TeV

Fig. Group : Electrons from beauty hadron decays in Pb-Pb 2015
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV
System: Pb-Pb

RAA of electrons from beauty hadron decays in Pb-Pb 5.02 TeV - comparison with heavy-flavour electrons measurement

Fig. Group : Electrons from beauty hadron decays in Pb-Pb 2015
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV
System: Pb-Pb

RAA of electrons from beauty hadron decays in Pb-Pb 5.02 TeV - comparison with models

Fig. Group : Electrons from beauty hadron decays in Pb-Pb 2015
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV
System: Pb-Pb

RAA of electrons from beauty hadron decays in Pb-Pb 5.02 TeV - comparison with run1 measurement

Fig. Group : Electrons from beauty hadron decays in Pb-Pb 2015
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV
System: Pb-Pb

Anti-Matter and Matter Absorption Studies

Double ratio of the matching efficiencies for (anti-)deuteron

Fig. Group : Anti-Matter and Matter Absorption Studies
PWG : PWG-LF (Light Flavour Spectra)
Energy: 5.02 TeV
System: p-Pb

Double ratio of the matching efficiencies for (anti-)proton

Fig. Group : Anti-Matter and Matter Absorption Studies
PWG : PWG-LF (Light Flavour Spectra)
Energy: 5.02 TeV
System: p-Pb

Matching efficiency for (anti-)proton

Fig. Group : Anti-Matter and Matter Absorption Studies
PWG : PWG-LF (Light Flavour Spectra)
Energy: 5.02 TeV
System: p-Pb

Matching efficiency for (anti-)deuteron

Fig. Group : Anti-Matter and Matter Absorption Studies
PWG : PWG-LF (Light Flavour Spectra)
Energy: 5.02 TeV
System: p-Pb

Deuteron mass squared vs momentum in presence of TRD

Fig. Group : Anti-Matter and Matter Absorption Studies
PWG : PWG-LF (Light Flavour Spectra)
Energy: 5.02 TeV
System: p-Pb

Phi vs transverse momentum distribution for positive particles in presence of TRD

Fig. Group : Anti-Matter and Matter Absorption Studies
PWG : PWG-LF (Light Flavour Spectra)
Energy: 5.02 TeV
System: p-Pb

TPC performance plot.

Fig. Group : Anti-Matter and Matter Absorption Studies
PWG : PWG-LF (Light Flavour Spectra)
Energy: 5.02 TeV
System: p-Pb

(Anti-)hypertriton production via 2 body decay channel in Pb-Pb at $\sqrt{s_{NN}}$ = 5.02 TeV [QM18]

Anti-hypertriton coalescence parameter B3 measured in Pb-Pb at 5.02 TeV in 10-40% centrality

Fig. Group : (Anti-)hypertriton production via 2 body decay channel in Pb-Pb at $\sqrt{s_{NN}}$ = 5.02 TeV [QM18]
PWG : PWG-LF (Light Flavour Spectra)
Energy: 5.02 TeV
System: Pb-Pb

Hypertriton coalescence parameter B3 measured in Pb-Pb at 5.02 TeV in 10-40% centrality

Fig. Group : (Anti-)hypertriton production via 2 body decay channel in Pb-Pb at $\sqrt{s_{NN}}$ = 5.02 TeV [QM18]
PWG : PWG-LF (Light Flavour Spectra)
Energy: 5.02 TeV
System: Pb-Pb

Strangeness population factor as a function of the centre-of-mass energy

Fig. Group : (Anti-)hypertriton production via 2 body decay channel in Pb-Pb at $\sqrt{s_{NN}}$ = 5.02 TeV [QM18]
PWG : PWG-LF (Light Flavour Spectra)
Energy: 5.02 TeV
System: Pb-Pb

Anti-hypertriton-to-hypertriton ratio as a function of the charged particle multiplicity in Pb-Pb at 5.02 TeV

Fig. Group : (Anti-)hypertriton production via 2 body decay channel in Pb-Pb at $\sqrt{s_{NN}}$ = 5.02 TeV [QM18]
PWG : PWG-LF (Light Flavour Spectra)
Energy: 5.02 TeV
System: Pb-Pb

Anti-hypertriton-to-hypertriton ratio as a function of the transverse momentum in 10-40% centrality

Fig. Group : (Anti-)hypertriton production via 2 body decay channel in Pb-Pb at $\sqrt{s_{NN}}$ = 5.02 TeV [QM18]
PWG : PWG-LF (Light Flavour Spectra)
Energy: 5.02 TeV
System: Pb-Pb

Hypertriton-over-light hadrons ratio in 0-10% centrality class compared with THERMUS predictions as a function of T_{chem}

Fig. Group : (Anti-)hypertriton production via 2 body decay channel in Pb-Pb at $\sqrt{s_{NN}}$ = 5.02 TeV [QM18]
PWG : PWG-LF (Light Flavour Spectra)
Energy: 5.02 TeV
System: Pb-Pb

(Anti-)hypertriton-over-(anti-)helium3 ratio as a function of the charged particle mutliplicity in Pb-Pb at 5.02 TeV

Fig. Group : (Anti-)hypertriton production via 2 body decay channel in Pb-Pb at $\sqrt{s_{NN}}$ = 5.02 TeV [QM18]
PWG : PWG-LF (Light Flavour Spectra)
Energy: 5.02 TeV
System: Pb-Pb

(Anti-)hypertriton dN/dy x B.R. compared to model predictions as a function of B.R.

Fig. Group : (Anti-)hypertriton production via 2 body decay channel in Pb-Pb at $\sqrt{s_{NN}}$ = 5.02 TeV [QM18]
PWG : PWG-LF (Light Flavour Spectra)
Energy: 5.02 TeV
System: Pb-Pb

Transverse momentum spectra of anti-hypertriton in 10-40% centrality class in Pb-Pb at 5.02 TeV

Fig. Group : (Anti-)hypertriton production via 2 body decay channel in Pb-Pb at $\sqrt{s_{NN}}$ = 5.02 TeV [QM18]
PWG : PWG-LF (Light Flavour Spectra)
Energy: 5.02 TeV
System: Pb-Pb

Transverse momentum spectra of hypertriton in 10-40% centrality class in Pb-Pb at 5.02 TeV

Fig. Group : (Anti-)hypertriton production via 2 body decay channel in Pb-Pb at $\sqrt{s_{NN}}$ = 5.02 TeV [QM18]
PWG : PWG-LF (Light Flavour Spectra)
Energy: 5.02 TeV
System: Pb-Pb

Transverse momentum spectra of (anti-)hypertriton in 10-40% centrality class in Pb-Pb at 5.02 TeV

Fig. Group : (Anti-)hypertriton production via 2 body decay channel in Pb-Pb at $\sqrt{s_{NN}}$ = 5.02 TeV [QM18]
PWG : PWG-LF (Light Flavour Spectra)
Energy: 5.02 TeV
System: Pb-Pb

(Anti-)hypertriton dN/dy x B.R. as a function of the charged particle multiplicity in Pb-Pb at 5.02 TeV

Fig. Group : (Anti-)hypertriton production via 2 body decay channel in Pb-Pb at $\sqrt{s_{NN}}$ = 5.02 TeV [QM18]
PWG : PWG-LF (Light Flavour Spectra)
Energy: 5.02 TeV
System: Pb-Pb

phi in pp collisions at 5.02 TeV vs. Multiplicity [QM18]

(dN/dy)/<dN_ch/deta> for phi mesons as a function of average charged particle multiplicity in pp collisions at 5.02 TeV

Fig. Group : phi in pp collisions at 5.02 TeV vs. Multiplicity [QM18]
PWG : PWG-LF (Light Flavour Spectra)
Energy: 5.02 TeV
System: p-p

phi Meson Invariant-Mass Distribution in pp Collisions at 5.02 TeV with Voigtian fit in V0M Multiplicity class VII

Fig. Group : phi in pp collisions at 5.02 TeV vs. Multiplicity [QM18]
PWG : PWG-LF (Light Flavour Spectra)
Energy: 5.02 TeV
System: p-p

phi Meson Invariant-Mass Distribution in pp Collisions at 5.02 TeV in V0M Multiplicity class VII

Fig. Group : phi in pp collisions at 5.02 TeV vs. Multiplicity [QM18]
PWG : PWG-LF (Light Flavour Spectra)
Energy: 5.02 TeV
System: p-p

pT Spectra of phi Mesons in pp Collisions at 5.02 TeV in V0M Multiplicity Event Classes

Fig. Group : phi in pp collisions at 5.02 TeV vs. Multiplicity [QM18]
PWG : PWG-LF (Light Flavour Spectra)
Energy: 5.02 TeV
System: p-p

K*± in pp Collisions at 8 TeV [QM18]

Model comparison of K*± yield in pp 8 TeV

Fig. Group : K*± in pp Collisions at 8 TeV [QM18]
PWG : PWG-LF (Light Flavour Spectra)
Energy: 8 TeV
System: p-p

Ratio of K*± pT spectra of 8 TeV and 13 TeV with respect to 5 TeV

Fig. Group : K*± in pp Collisions at 8 TeV [QM18]
PWG : PWG-LF (Light Flavour Spectra)
Energy: 8 TeV
System: p-p

K*± vs K*0 pT spectra in pp 8 TeV

Fig. Group : K*± in pp Collisions at 8 TeV [QM18]
PWG : PWG-LF (Light Flavour Spectra)
Energy: 8 TeV
System: p-p

K*± pT spectra in pp collisions at 8 TeV

Fig. Group : K*± in pp Collisions at 8 TeV [QM18]
PWG : PWG-LF (Light Flavour Spectra)
Energy: 8 TeV
System: p-p

K*0 in p-Pb Collisions at 8.16 TeV [QM18]

dNdy/<dNdeta> as a function of average chraged particle multiplicity of K*0 in p-Pb 8.16 TeV

Fig. Group : K*0 in p-Pb Collisions at 8.16 TeV [QM18]
PWG : PWG-LF (Light Flavour Spectra)
Energy: 8 TeV
System: p-Pb

pT spectra of K*0 for variuos V0A multiplicity classes in p-Pb Collisions at 8.16 TeV

Fig. Group : K*0 in p-Pb Collisions at 8.16 TeV [QM18]
PWG : PWG-LF (Light Flavour Spectra)
Energy: 8 TeV
System: p-Pb

pT spectrum of K*0 in p-Pb Collisions at 8.16 TeV

Fig. Group : K*0 in p-Pb Collisions at 8.16 TeV [QM18]
PWG : PWG-LF (Light Flavour Spectra)
Energy: 8 TeV
System: p-Pb

Invariant mass distribution of πK pair after background subtraction in p-Pb Collisions at 8.16 TeV

Fig. Group : K*0 in p-Pb Collisions at 8.16 TeV [QM18]
PWG : PWG-LF (Light Flavour Spectra)
Energy: 8 TeV
System: p-Pb

Invariant mass distribution of πK pair before background subtraction in p-Pb Collisions at 8.16 TeV

Fig. Group : K*0 in p-Pb Collisions at 8.16 TeV [QM18]
PWG : PWG-LF (Light Flavour Spectra)
Energy: 8 TeV
System: p-Pb

phi in p-Pb Collisions at 8.16 TeV [QM18]

Invariant mass distribution of KK pair after background subtraction in p-Pb collisions at 8.16 TeV

Fig. Group : phi in p-Pb Collisions at 8.16 TeV [QM18]
PWG : PWG-LF (Light Flavour Spectra)
Energy: 8 TeV
System: p-Pb

pT spectra of phi for various V0A multiplicity classes in p-Pb collisions 8.16 TeV

Fig. Group : phi in p-Pb Collisions at 8.16 TeV [QM18]
PWG : PWG-LF (Light Flavour Spectra)
Energy: 8 TeV
System: p-Pb

pT spectraum of phi in pPb collisions at 8.16 TeV

Fig. Group : phi in p-Pb Collisions at 8.16 TeV [QM18]
PWG : PWG-LF (Light Flavour Spectra)
Energy: 8 TeV
System: p-Pb

Invariant mass distribution of KK pair before background subtraction in pPb collisions at 8.16 TeV

Fig. Group : phi in p-Pb Collisions at 8.16 TeV [QM18]
PWG : PWG-LF (Light Flavour Spectra)
Energy: 8 TeV
System: p-Pb

Production of \pi, K and p as a function of spherocity in high multiplicity pp collisions at \sqrt{s} = 13 TeV [IS17]

pT-differential proton-to-pion ratio in V0M 0-10%, high and low spherocities with comparison to PYTHIA 8 and EPOS LHC

Fig. Group : Production of \pi, K and p as a function of spherocity in high multiplicity pp collisions at \sqrt{s} = 13 TeV [IS17]
PWG : PWG-LF (Light Flavour Spectra)
Energy: 13 TeV
System: p-p

pT-differential proton-to-pion ratio in V0M 0-10%, high and low spherocities

Fig. Group : Production of \pi, K and p as a function of spherocity in high multiplicity pp collisions at \sqrt{s} = 13 TeV [IS17]
PWG : PWG-LF (Light Flavour Spectra)
Energy: 13 TeV
System: p-p

pT-differential kaon-to-pion ratio in V0M 0-10%, high and low spherocities with comparison to PYTHIA 8 and EPOS LHC

Fig. Group : Production of \pi, K and p as a function of spherocity in high multiplicity pp collisions at \sqrt{s} = 13 TeV [IS17]
PWG : PWG-LF (Light Flavour Spectra)
Energy: 13 TeV
System: p-p

pT-differential kaon-to-pion ratio in V0M 0-10%, high and low spherocities

Fig. Group : Production of \pi, K and p as a function of spherocity in high multiplicity pp collisions at \sqrt{s} = 13 TeV [IS17]
PWG : PWG-LF (Light Flavour Spectra)
Energy: 13 TeV
System: p-p

D-meson production as a function of event spherocity

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 $30 < {\rm N}_{\rm tracklets} < 81$.

Fig. Group : D-meson production as a function of event spherocity
PWG : PWG-HF (Heavy Flavour)
Energy: 7 TeV
System: p-p

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 $20 < {\rm N}_{\rm tracklets} < 30$.

Fig. Group : D-meson production as a function of event spherocity
PWG : PWG-HF (Heavy Flavour)
Energy: 7 TeV
System: p-p

Fig. Group : D-meson production as a function of event spherocity
PWG : PWG-HF (Heavy Flavour)
Energy: 7 TeV
System: p-p

CERN Accelerating science

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Public Preliminary figures by analysis

QM2018 (poster) Factorization of two-particle distributions from (5.02 TeV Pb--Pb collisions)

Heavy-flavour decay electron vs. multiplicity in p-Pb collisions at 8.16 TeV

f0(980) in pp collisions at 5.02 TeV [QM18]

Multi-differential studies of the jpsi production in PbPb collisions at sqrt(S_NN) = 5.02 TeV

D-h azimuthal correlations in p-Pb collisions @ 5.02 TeV(2016) vs ZNA centrality

QM2018 (talk) Multiplicity evolution of the nearside peak in Pb-Pb 5.02 TeV

D0 jets in p-Pb at 5 TeV (Run2)

J/psi nuclear modification factor in Xe-Xe collisions at sqrt(sNN)=5.44 TeV

QM2018 (poster) Anisotropic flow of multi-strange particles in Pb--Pb collisions at sqrts = 5.02 TeV

Preliminary: Direct photons in pPb 5TeV

Electrons from beauty hadron decays in Pb-Pb 2015

Anti-Matter and Matter Absorption Studies

(Anti-)hypertriton production via 2 body decay channel in Pb-Pb at $\sqrt{s_{NN}}$ = 5.02 TeV [QM18]

phi in pp collisions at 5.02 TeV vs. Multiplicity [QM18]

K*± in pp Collisions at 8 TeV [QM18]

K*0 in p-Pb Collisions at 8.16 TeV [QM18]

phi in p-Pb Collisions at 8.16 TeV [QM18]

Production of \pi, K and p as a function of spherocity in high multiplicity pp collisions at \sqrt{s} = 13 TeV [IS17]

D-meson production as a function of event spherocity

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