Search for Preliminary Figures

Factorization ratio $f_2(\eta_a, \eta_b)$ for various centralities for $|\Delta\eta| > 2.6$ and 60-80% centrality
Factorization ratio $f_2(\eta_a, \eta_b)$ for various centralities for $|\Delta\eta| > 2.6$ and 0-5% centrality
Factorization ratio $f_2(\eta_a, \eta_b)$ for various centralities for $|\Delta\eta| > 3$ and 10-20% centrality
Factorization ratio $f_2(\eta_a, \eta_b)$ for various centralities for $|\Delta\eta| > 2$ and 10-20% centrality
Multiplicity distribution in p-Pb collisions at 8.16 TeV
Cluster energy distribution with EMCal and DCal detectors in p-Pb collisions at 8.16 TeV
Factorization ratio in the (eta_a, eta_b)-plane at 10-20% centrality for purely factorizing model $\Delta\eta > 2.6$
Projections of the factorization ratio onto $\Delta\eta$ for various centralities for $|\Delta\eta| > 2.6$
Ratio p/f0(pT) in pp collisions at 5.02 TeV
Ratio f0/phi(pT) in pp collisions at 5.02 TeV
Ratio f0/pi(pT) in pp collisions at 5.02 TeV
f0/pi vs. Energy at different energies
pT spectrum of f0(980) in inelastic pp collisions at 5.02 TeV (w/o B.R. correction)
pT spectrum of f0(980) in inelastic pp collisions at 5.02 TeV (w B.R. correction)
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
J/ψ yield in multi-differential bins in forward rapidity in Pb-Pb collisions at \sqrt{s_{NN}} = 5.02 TeV with ALICE
J/ψ yield in multi-differential bins in forward rapidity in Pb-Pb collisions at \sqrt{s_{NN}} = 5.02 TeV with ALICE
J/ψ yield in multi-differential bins in forward rapidity in Pb-Pb collisions at \sqrt{s_{NN}} = 5.02 TeV with ALICE
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.
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.
Width of the near-side peak at 5.02 TeV with large binning
Width of the near-side peak at 5.02 TeV
Comparison of near-side peak observables from D-h correlations vs ZNA centrality, in p-Pb collisions @ 5.02 TeV (2016)
D-h azimuthal correlation distributions in 0-20%, 20-60%, 60-100% ZNA centrality
Cross Section of Charged Jets (Anti-kT, R=0.3) Tagged with a D^{0} meson with $p_{\rm T,D} > 3 GeV/c$
Reconstruction efficiency of D0 in charged jets, p-Pb at 5.02 TeV (Run2)
Raw D0- charged jets pT distributions, D0 pT intervals, p-Pb at 5.02 TeV (Run2)
D0 in charged jets invariant mass distributions, D0 pT intervals, p-Pb at 5.02 TeV (Run2)
Background fluctuations for D0-jet analysis, random cones with R=0.3, p-Pb collisions at 5.02 TeV (Run 2)
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
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
Multi-strange particles v3 in different centrality.
Multi-strange particles v2 in different centrality.
multi-strange particles v3/nq to pT/nq compare to other identified particles
multi-strange particles v2/nq to pT/nq compare to other identified particles
multi-strange particles v3 compare to other identified particles
multi-strange particles v2 compare to other identified particles
v2 signal extract of particle xi.
Direct and Inclusive Photon Production in pPb 5TeV with Theory
Direct and Inclusive Photon Production in pPb 5 TeV
Direct Photon Production in pPb 5TeV
Inclusive Photon Production in pPb 5 TeV
DCA template fit example
Spectrum of electrons from beauty hadron decays in Pb-Pb 5.02 TeV
RAA of electrons from beauty hadron decays in Pb-Pb 5.02 TeV - comparison with heavy-flavour electrons measurement
RAA of electrons from beauty hadron decays in Pb-Pb 5.02 TeV - comparison with models
RAA of electrons from beauty hadron decays in Pb-Pb 5.02 TeV - comparison with run1 measurement
Direct Photon Excess in pPb 5 TeV - individual techniques
Direct Photon Excess in pPb 5 TeV with Theory
Direct Photon Excess in pPb 5 TeV
Double ratio of the matching efficiencies for (anti-)deuteron
Double ratio of the matching efficiencies for (anti-)proton
Matching efficiency for (anti-)proton
Matching efficiency for (anti-)deuteron
Deuteron mass squared vs momentum in presence of TRD
Phi vs transverse momentum distribution for positive particles in presence of TRD
TPC performance plot.
Anti-hypertriton coalescence parameter B3 measured in Pb-Pb at 5.02 TeV in 10-40% centrality
Hypertriton coalescence parameter B3 measured in Pb-Pb at 5.02 TeV in 10-40% centrality
Strangeness population factor as a function of the centre-of-mass energy
Anti-hypertriton-to-hypertriton ratio as a function of the charged particle multiplicity in Pb-Pb at 5.02 TeV
Anti-hypertriton-to-hypertriton ratio as a function of the transverse momentum in 10-40% centrality
Hypertriton-over-light hadrons ratio in 0-10% centrality class compared with THERMUS predictions as a function of T_{chem}
(Anti-)hypertriton-over-(anti-)helium3 ratio as a function of the charged particle mutliplicity in Pb-Pb at 5.02 TeV
(Anti-)hypertriton dN/dy x B.R. compared to model predictions as a function of B.R.
Transverse momentum spectra of anti-hypertriton in 10-40% centrality class in Pb-Pb at 5.02 TeV
Transverse momentum spectra of hypertriton in 10-40% centrality class in Pb-Pb at 5.02 TeV
Transverse momentum spectra of (anti-)hypertriton in 10-40% centrality class in Pb-Pb at 5.02 TeV
(Anti-)hypertriton dN/dy x B.R. as a function of the charged particle multiplicity in Pb-Pb at 5.02 TeV
(dN/dy)/<dN_ch/deta> for phi mesons as a function of average charged particle multiplicity in pp collisions at 5.02 TeV
phi Meson Invariant-Mass Distribution in pp Collisions at 5.02 TeV with Voigtian fit in V0M Multiplicity class VII
phi Meson Invariant-Mass Distribution in pp Collisions at 5.02 TeV in V0M Multiplicity class VII
pT Spectra of phi Mesons in pp Collisions at 5.02 TeV in V0M Multiplicity Event Classes
Model comparison of K*± yield in pp 8 TeV
Ratio of K*± pT spectra of 8 TeV and 13 TeV with respect to 5 TeV
K*± vs K*0 pT spectra in pp 8 TeV
K*± pT spectra in pp collisions at 8 TeV
f0(980) Acceptance times Efficiency correction
f0(980) signal extraction: fit to the LSB-subtracted π+π- invariant mass for 5 < pT < 6 GeV/c
f0(980) signal extraction: fit to the LSB-subtracted π+π- invariant mass for 1.5 < pT < 2 GeV/c
f0(980) signal extraction: fit to the LSB-subtracted π+π- invariant mass for 0 < pT < 0.3 GeV/c
f0(980) Invariant-Mass Distribution with Like-Sign Background, 5 < pT < 6 GeV/c
f0(980) Invariant-Mass Distribution with Like-Sign Background, 1.5 < pT < 2 GeV/c
f0(980) Invariant-Mass Distribution with Like-Sign Background, 0 < pT < 0.3 GeV/c
dNdy/<dNdeta> as a function of average chraged particle multiplicity of K*0 in p-Pb 8.16 TeV
pT spectra of K*0 for variuos V0A multiplicity classes in p-Pb Collisions at 8.16 TeV
pT spectrum of K*0 in p-Pb Collisions at 8.16 TeV
Invariant mass distribution of πK pair after background subtraction in p-Pb Collisions at 8.16 TeV
Invariant mass distribution of πK pair before background subtraction in p-Pb Collisions at 8.16 TeV
Invariant mass distribution of KK pair after background subtraction in p-Pb collisions at 8.16 TeV
pT spectra of phi for various V0A multiplicity classes in p-Pb collisions 8.16 TeV
pT spectraum of phi in pPb collisions at 8.16 TeV
Invariant mass distribution of KK pair before background subtraction in pPb collisions at 8.16 TeV
pT-differential proton-to-pion ratio in V0M 0-10%, high and low spherocities with comparison to PYTHIA 8 and EPOS LHC
pT-differential proton-to-pion ratio in V0M 0-10%, high and low spherocities
pT-differential kaon-to-pion ratio in V0M 0-10%, high and low spherocities with comparison to PYTHIA 8 and EPOS LHC
pT-differential kaon-to-pion ratio in V0M 0-10%, high and low spherocities
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 $30 < {\rm N}_{\rm tracklets} < 81$.
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 $20 < {\rm N}_{\rm tracklets} < 30$.
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 $20 < {\rm N}_{\rm tracklets} < 81$.