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Public Preliminary figures by analysis

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ID number ALI-PREL-XXX

Figure Caption

Scope: PWG

System

Energy

Measurements of the groomed and ungroomed jet mass in pp and Pb-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV

Measurement of the groomed jet mass for $R=0.2$ charged-particle jets in $80 < p_\text{T}^\text{ch jet} < 100$ GeV/$c$ in Pb-Pb collisions at $\sqrt{s_\text{NN}}=5.02$ TeV as compared to pp baseline

Fig. Group : Measurements of the groomed and ungroomed jet mass in pp and Pb-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV
PWG : PWG-JE (Jets)
Energy: 5.02 TeV
System: p-p, Pb-Pb

Measurement of the groomed jet mass for $R=0.2$ charged-particle jets in $60 < p_\text{T}^\text{ch jet} < 80$ GeV/$c$ in Pb-Pb collisions at $\sqrt{s_\text{NN}}=5.02$ TeV as compared to pp baseline

Fig. Group : Measurements of the groomed and ungroomed jet mass in pp and Pb-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV
PWG : PWG-JE (Jets)
Energy: 5.02 TeV
System: p-p, Pb-Pb

Measurement of the groomed jet mass for $R=0.2$ charged-particle jets in $40 < p_\text{T}^\text{ch jet} < 60$ GeV/$c$ in Pb-Pb collisions at $\sqrt{s_\text{NN}}=5.02$ TeV as compared to pp baseline

Fig. Group : Measurements of the groomed and ungroomed jet mass in pp and Pb-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV
PWG : PWG-JE (Jets)
Energy: 5.02 TeV
System: p-p, Pb-Pb

Measurement of the ungroomed jet mass for $R=0.2$ charged-particle jets in $80 < p_\text{T}^\text{ch jet} < 100$ GeV/$c$ in Pb-Pb collisions at $\sqrt{s_\text{NN}}=5.02$ TeV as compared to pp baseline

Fig. Group : Measurements of the groomed and ungroomed jet mass in pp and Pb-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV
PWG : PWG-JE (Jets)
Energy: 5.02 TeV
System: p-p, Pb-Pb

Measurement of the ungroomed jet mass for $R=0.2$ charged-particle jets in $60 < p_\text{T}^\text{ch jet} < 80$ GeV/$c$ in Pb-Pb collisions at $\sqrt{s_\text{NN}}=5.02$ TeV as compared to pp baseline

Fig. Group : Measurements of the groomed and ungroomed jet mass in pp and Pb-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV
PWG : PWG-JE (Jets)
Energy: 5.02 TeV
System: p-p, Pb-Pb

Measurement of the ungroomed jet mass for $R=0.2$ charged-particle jets in $40 < p_\text{T}^\text{ch jet} < 60$ GeV/$c$ in Pb-Pb collisions at $\sqrt{s_\text{NN}}=5.02$ TeV as compared to pp baseline

Fig. Group : Measurements of the groomed and ungroomed jet mass in pp and Pb-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV
PWG : PWG-JE (Jets)
Energy: 5.02 TeV
System: p-p, Pb-Pb

Measurement of the groomed jet mass in Pb-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV from $100 < p_\mathrm{T}^\mathrm{ch\;jet} < 150$ GeV/$c$ with $R=0.2$

Fig. Group : Measurements of the groomed and ungroomed jet mass in pp and Pb-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV
PWG : PWG-JE (Jets)
Energy: 5.02 TeV
System: Pb-Pb

Measurement of the groomed jet mass in Pb-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV from $80 < p_\mathrm{T}^\mathrm{ch\;jet} < 100$ GeV/$c$ with $R=0.2$

Fig. Group : Measurements of the groomed and ungroomed jet mass in pp and Pb-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV
PWG : PWG-JE (Jets)
Energy: 5.02 TeV
System: Pb-Pb

Measurement of the groomed jet mass in Pb-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV from $60 < p_\mathrm{T}^\mathrm{ch\;jet} < 80$ GeV/$c$ with $R=0.2$

Fig. Group : Measurements of the groomed and ungroomed jet mass in pp and Pb-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV
PWG : PWG-JE (Jets)
Energy: 5.02 TeV
System: Pb-Pb

Measurement of the groomed jet mass in Pb-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV from $40 < p_\mathrm{T}^\mathrm{ch\;jet} < 60$ GeV/$c$ with $R=0.2$

Fig. Group : Measurements of the groomed and ungroomed jet mass in pp and Pb-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV
PWG : PWG-JE (Jets)
Energy: 5.02 TeV
System: Pb-Pb

Measurement of the groomed jet mass in pp collisions at $\sqrt{s} = 5.02$ TeV from $80 < p_\mathrm{T}^\mathrm{ch\;jet} < 100$ GeV/$c$ with $R=0.2$

Fig. Group : Measurements of the groomed and ungroomed jet mass in pp and Pb-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV
PWG : PWG-JE (Jets)
Energy: 5.02 TeV
System: p-p

Measurement of the groomed jet mass in pp collisions at $\sqrt{s} = 5.02$ TeV from $60 < p_\mathrm{T}^\mathrm{ch\;jet} < 80$ GeV/$c$ with $R=0.2$

Fig. Group : Measurements of the groomed and ungroomed jet mass in pp and Pb-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV
PWG : PWG-JE (Jets)
Energy: 5.02 TeV
System: p-p

Measurement of the groomed jet mass in pp collisions at $\sqrt{s} = 5.02$ TeV from $40 < p_\mathrm{T}^\mathrm{ch\;jet} < 60$ GeV/$c$ with $R=0.2$

Fig. Group : Measurements of the groomed and ungroomed jet mass in pp and Pb-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV
PWG : PWG-JE (Jets)
Energy: 5.02 TeV
System: p-p

Measurement of the ungroomed jet mass in pp collisions at $\sqrt{s} = 5.02$ TeV from $80 < p_\mathrm{T}^\mathrm{ch\;jet} < 100$ GeV/$c$ with $R=0.2$

Fig. Group : Measurements of the groomed and ungroomed jet mass in pp and Pb-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV
PWG : PWG-JE (Jets)
Energy: 5.02 TeV
System: p-p

Measurement of the ungroomed jet mass in pp collisions at $\sqrt{s} = 5.02$ TeV from $60 < p_\mathrm{T}^\mathrm{ch\;jet} < 80$ GeV/$c$ with $R=0.2$

Fig. Group : Measurements of the groomed and ungroomed jet mass in pp and Pb-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV
PWG : PWG-JE (Jets)
Energy: 5.02 TeV
System: p-p

Measurement of the ungroomed jet mass in pp collisions at $\sqrt{s} = 5.02$ TeV from $40 < p_\mathrm{T}^\mathrm{ch\;jet} < 60$ GeV/$c$ with $R=0.2$

Fig. Group : Measurements of the groomed and ungroomed jet mass in pp and Pb-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV
PWG : PWG-JE (Jets)
Energy: 5.02 TeV
System: p-p

Measurement of the ungroomed jet mass in Pb-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV from $100 < p_\mathrm{T}^\mathrm{ch\;jet} < 150$ GeV/$c$ with $R=0.2$

Fig. Group : Measurements of the groomed and ungroomed jet mass in pp and Pb-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV
PWG : PWG-JE (Jets)
Energy: 5.02 TeV
System: Pb-Pb

Measurement of the ungroomed jet mass in Pb-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV from $80 < p_\mathrm{T}^\mathrm{ch\;jet} < 100$ GeV/$c$ with $R=0.2$

Fig. Group : Measurements of the groomed and ungroomed jet mass in pp and Pb-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV
PWG : PWG-JE (Jets)
Energy: 5.02 TeV
System: Pb-Pb

Measurement of the ungroomed jet mass in Pb-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV from $60 < p_\mathrm{T}^\mathrm{ch\;jet} < 80$ GeV/$c$ with $R=0.2$

Fig. Group : Measurements of the groomed and ungroomed jet mass in pp and Pb-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV
PWG : PWG-JE (Jets)
Energy: 5.02 TeV
System: Pb-Pb

Measurement of the ungroomed jet mass in Pb-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV from $40 < p_\mathrm{T}^\mathrm{ch\;jet} < 60$ GeV/$c$ with $R=0.2$

Fig. Group : Measurements of the groomed and ungroomed jet mass in pp and Pb-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV
PWG : PWG-JE (Jets)
Energy: 5.02 TeV
System: Pb-Pb

Omega over pion ratio as a function of the pion yield in pp collisions at 9 GeV, 7 TeV and 13.6 TeV

Fig. Group :
PWG : PWG-LF (Light Flavour Spectra)
Energy: 900 GeV, 7 TeV, 13.6 TeV
System: p-p

Kaon over pion ratio as a function of pT in pp collisions at 900 GeV, 13 TeV and 13.6 TeV with Run 3 data

Fig. Group :
PWG : PWG-LF (Light Flavour Spectra)
Energy: 900 GeV
System: p-p

Physics Analysis Group: Spectra

Proton over pion ratio as a function of pT in pp collisions at 900 GeV, 13 TeV and 13.6 TeV with Run 3 data

Fig. Group : Physics Analysis Group: Spectra
PWG : PWG-LF (Light Flavour Spectra)
Energy: 900 GeV, 13 TeV, 13.6 TeV
System: p-p

$\Omega_{\rm c}^{0}$ production in semileptonic decay channel in pp collisions at $\sqrt s$ = 13 TeV

BR ratio comparisons of $\Omega_{\rm c}^{0}$

Fig. Group : $\Omega_{\rm c}^{0}$ production in semileptonic decay channel in pp collisions at $\sqrt s$ = 13 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13 TeV
System: p-p

Xic multiplicity dependence via hadronic decay in proton-proton collisions at s√=13 TeV

Xic/D0 and Xic/Lc ratio in low and high V0M multiplicity classes compared to PYTHIA

Fig. Group : Xic multiplicity dependence via hadronic decay in proton-proton collisions at s√=13 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13 TeV
System: p-p

Invariant mass distribution of Xic in high multiplicity class

Fig. Group : Xic multiplicity dependence via hadronic decay in proton-proton collisions at s√=13 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13 TeV
System: p-p

Prompt efficiency of Xic for different multiplicity classes

Fig. Group : Xic multiplicity dependence via hadronic decay in proton-proton collisions at s√=13 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13 TeV
System: p-p

Corrected yield of \Xi_c^0 in different V0M multiplicity classes

Fig. Group : Xic multiplicity dependence via hadronic decay in proton-proton collisions at s√=13 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13 TeV
System: p-p

Csic0/D0 and Csic+/D0 ratio in low and high V0M multiplicity classes

Fig. Group : Xic multiplicity dependence via hadronic decay in proton-proton collisions at s√=13 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13 TeV
System: p-p

Xic/Lc ratio in low and high V0M multiplicity classes

Fig. Group : Xic multiplicity dependence via hadronic decay in proton-proton collisions at s√=13 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13 TeV
System: p-p

Xic/D0 ratio in low and high V0M multiplicity classes

Fig. Group : Xic multiplicity dependence via hadronic decay in proton-proton collisions at s√=13 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13 TeV
System: p-p

Xic/Lc ratio measured in \pp collisions at 13TeV in different multiplicity

Fig. Group : Xic multiplicity dependence via hadronic decay in proton-proton collisions at s√=13 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13 TeV
System: p-p

Xi_c^0/D^0 ratio in different V0M multiplicity classes

Fig. Group : Xic multiplicity dependence via hadronic decay in proton-proton collisions at s√=13 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13 TeV
System: p-p

Azimuthal correlations between heavy-flavour decay electrons and charged particles in Pb-Pb collisions at 5.02 TeV

Away-Side Nuclear Modification factor ($I_{AA}$) of Pb-Pb in 0 - 10% Centrality compared to LF $I_{AA}$

Fig. Group : Azimuthal correlations between heavy-flavour decay electrons and charged particles in Pb-Pb collisions at 5.02 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV
System: Pb-Pb

Near-Side Nuclear Modification factor ($I_{AA}$) of Pb-Pb in 0 - 10% Centrality compared to LF $I_{AA}$

Fig. Group : Azimuthal correlations between heavy-flavour decay electrons and charged particles in Pb-Pb collisions at 5.02 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV
System: Pb-Pb

Delta Phi Distribution of heavy-flavor decay electrons and charged particles, Pb-Pb 30 - 50% Centrality and pp, 2 pT bins

Fig. Group : Azimuthal correlations between heavy-flavour decay electrons and charged particles in Pb-Pb collisions at 5.02 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV
System: Pb-Pb

Delta Phi Distribution of heavy-flavor decay electrons and charged particles, Pb-Pb 0 - 10% Centrality and pp, 2 pT bins

Fig. Group : Azimuthal correlations between heavy-flavour decay electrons and charged particles in Pb-Pb collisions at 5.02 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV
System: Pb-Pb

Delta Phi Distribution of heavy-flavor decay electrons and charged particles with background uncertainty, Pb-Pb 0 - 10%, 2 pT bins

Fig. Group : Azimuthal correlations between heavy-flavour decay electrons and charged particles in Pb-Pb collisions at 5.02 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV
System: Pb-Pb

Measurement of inclusive jet distributions in central Pb-Pb collisions at 5.02 TeV with a novel mixed-event approach.

Charged jet $R_{AA}$ for R = 0.3 measured in central Pb-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV: Comparison to STAR $R_{AA}$

Fig. Group : Measurement of inclusive jet distributions in central Pb-Pb collisions at 5.02 TeV with a novel mixed-event approach.
PWG : PWG-JE (Jets)
Energy: 5.02 TeV
System: Pb-Pb

Charged jet $R_{AA}$ for R = 0.3 measured in central Pb-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV: Comparison to previous ALICE $R_{AA}$ measured with 2015 Pb-Pb data

Fig. Group : Measurement of inclusive jet distributions in central Pb-Pb collisions at 5.02 TeV with a novel mixed-event approach.
PWG : PWG-JE (Jets)
Energy: 5.02 TeV
System: Pb-Pb

Charged jet $R_{AA}$ for R = 0.3 measured in central Pb-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV

Fig. Group : Measurement of inclusive jet distributions in central Pb-Pb collisions at 5.02 TeV with a novel mixed-event approach.
PWG : PWG-JE (Jets)
Energy: 5.02 TeV
System: Pb-Pb

Corrected charged jet distributions with $p_{T}^{lead} > 3$ GeV/c and $p_{T}^{lead} > 4$ GeV/c for central Pb-Pb collisions at 5.02 TeV

Fig. Group : Measurement of inclusive jet distributions in central Pb-Pb collisions at 5.02 TeV with a novel mixed-event approach.
PWG : PWG-JE (Jets)
Energy: 5.02 TeV
System: Pb-Pb

Response matrix for R=0.3 jets with $p_{T}^{lead} > 4$ GeV/c in central Pb-Pb collisions at 5.02 TeV

Fig. Group : Measurement of inclusive jet distributions in central Pb-Pb collisions at 5.02 TeV with a novel mixed-event approach.
PWG : PWG-JE (Jets)
Energy: 5.02 TeV
System: Pb-Pb

Response matrix for R=0.3 jets with $p_{T}^{lead} > 3$ GeV/c in central Pb-Pb collisions at 5.02 TeV

Fig. Group : Measurement of inclusive jet distributions in central Pb-Pb collisions at 5.02 TeV with a novel mixed-event approach.
PWG : PWG-JE (Jets)
Energy: 5.02 TeV
System: Pb-Pb

Raw correlated quasi-inclusive jet $p_{T,jet}^{reco}$ distribution with $p_{T}^{lead} > 3$ GeV/c for central Pb-Pb collisions at 5.02 TeV

Fig. Group : Measurement of inclusive jet distributions in central Pb-Pb collisions at 5.02 TeV with a novel mixed-event approach.
PWG : PWG-JE (Jets)
Energy: 5.02 TeV
System: Pb-Pb

Raw correlated quasi-inclusive jet $p_{T,jet}^{reco}$ distribution with $p_{T}^{lead} > 4$ GeV/c for central Pb-Pb collisions at 5.02 TeV

Fig. Group : Measurement of inclusive jet distributions in central Pb-Pb collisions at 5.02 TeV with a novel mixed-event approach.
PWG : PWG-JE (Jets)
Energy: 5.02 TeV
System: Pb-Pb

Raw quasi-inclusive jet $p_{T,jet}^{reco}$ distribution of the SE and ME with $p_{T}^{lead} > 3$ GeV/c for central Pb-Pb collisions at 5.02 TeV

Fig. Group : Measurement of inclusive jet distributions in central Pb-Pb collisions at 5.02 TeV with a novel mixed-event approach.
PWG : PWG-JE (Jets)
Energy: 5.02 TeV
System: Pb-Pb

Raw quasi-inclusive jet $p_{T,jet}^{reco}$ distribution of the SE and ME with $p_{T}^{lead} > 4$ GeV/c for central Pb-Pb collisions at 5.02 TeV

Fig. Group : Measurement of inclusive jet distributions in central Pb-Pb collisions at 5.02 TeV with a novel mixed-event approach.
PWG : PWG-JE (Jets)
Energy: 5.02 TeV
System: Pb-Pb

LcOverD0_pPb_5.02TeV

Lc/D0_vs_multiplcity_pt_pPb_5.02TeV

Fig. Group : LcOverD0_pPb_5.02TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV
System: p-Pb

D0_corrected_yield_pPb_5.02TeV

Fig. Group : LcOverD0_pPb_5.02TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV
System: p-Pb

Lc_corrected_yield_pPb_5.02TeV

Fig. Group : LcOverD0_pPb_5.02TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV
System: p-Pb

[poster] Measurement of the transverse momentum($j_T$) distributions of charged-particle jet fragments in pp collisions at $\sqrt{s}$ = 5.02 TeV with ALICE

Ratio of the $j_\mathrm{T}$ distributions in high $z$ to the $j_\mathrm{T}$ distributions in inclusive $z$

Fig. Group : [poster] Measurement of the transverse momentum($j_T$) distributions of charged-particle jet fragments in pp collisions at $\sqrt{s}$ = 5.02 TeV with ALICE
PWG : PWG-JE (Jets)
Energy: 5.02 TeV
System: p-p

Ratio of the $j_\mathrm{T}$ distributions in low $z$ to the $j_\mathrm{T}$ distributions in inclusive $z$

Fig. Group : [poster] Measurement of the transverse momentum($j_T$) distributions of charged-particle jet fragments in pp collisions at $\sqrt{s}$ = 5.02 TeV with ALICE
PWG : PWG-JE (Jets)
Energy: 5.02 TeV
System: p-p

$j_\mathrm{T}$ distributions in $60 < p_\mathrm{T,jet}^\mathrm{ch} < 100 \;\mathrm{ GeV}/c$ in differential $z$ compared to HERWIG7

Fig. Group : [poster] Measurement of the transverse momentum($j_T$) distributions of charged-particle jet fragments in pp collisions at $\sqrt{s}$ = 5.02 TeV with ALICE
PWG : PWG-JE (Jets)
Energy: 5.02 TeV
System: p-p

$j_\mathrm{T}$ distributions in $40 < p_\mathrm{T,jet}^\mathrm{ch} < 60 \;\mathrm{ GeV}/c$ in differential $z$ compared to HERWIG7

Fig. Group : [poster] Measurement of the transverse momentum($j_T$) distributions of charged-particle jet fragments in pp collisions at $\sqrt{s}$ = 5.02 TeV with ALICE
PWG : PWG-JE (Jets)
Energy: 5.02 TeV
System: p-p

$j_\mathrm{T}$ distributions in $20 < p_\mathrm{T,jet}^\mathrm{ch} < 40 \;\mathrm{ GeV}/c$ in differential $z$ compared to HERWIG7

Fig. Group : [poster] Measurement of the transverse momentum($j_T$) distributions of charged-particle jet fragments in pp collisions at $\sqrt{s}$ = 5.02 TeV with ALICE
PWG : PWG-JE (Jets)
Energy: 5.02 TeV
System: p-p

$j_\mathrm{T}$ distributions in $10 < p_\mathrm{T,jet}^\mathrm{ch} < 20 \;\mathrm{ GeV}/c$ in differential $z$ compared to HERWIG7

Fig. Group : [poster] Measurement of the transverse momentum($j_T$) distributions of charged-particle jet fragments in pp collisions at $\sqrt{s}$ = 5.02 TeV with ALICE
PWG : PWG-JE (Jets)
Energy: 5.02 TeV
System: p-p

$j_\mathrm{T}$ distributions in $10 < p_\mathrm{T,jet}^\mathrm{ch} < 20 \;\mathrm{ GeV}/c$ in differential $z$ compared to PYTHIA8 Monash

Fig. Group : [poster] Measurement of the transverse momentum($j_T$) distributions of charged-particle jet fragments in pp collisions at $\sqrt{s}$ = 5.02 TeV with ALICE
PWG : PWG-JE (Jets)
Energy: 5.02 TeV
System: p-p

$j_\mathrm{T}$ distributions in $20 < p_\mathrm{T,jet}^\mathrm{ch} < 40 \;\mathrm{ GeV}/c$ in differential $z$ compared to PYTHIA8 Monash

Fig. Group : [poster] Measurement of the transverse momentum($j_T$) distributions of charged-particle jet fragments in pp collisions at $\sqrt{s}$ = 5.02 TeV with ALICE
PWG : PWG-JE (Jets)
Energy: 5.02 TeV
System: p-p

$j_\mathrm{T}$ distributions in $40 < p_\mathrm{T,jet}^\mathrm{ch} < 60 \;\mathrm{ GeV}/c$ in differential $z$ compared to PYTHIA8 Monash

Fig. Group : [poster] Measurement of the transverse momentum($j_T$) distributions of charged-particle jet fragments in pp collisions at $\sqrt{s}$ = 5.02 TeV with ALICE
PWG : PWG-JE (Jets)
Energy: 5.02 TeV
System: p-p

$j_\mathrm{T}$ distributions in $60 < p_\mathrm{T,jet}^\mathrm{ch} < 100 \;\mathrm{ GeV}/c$ in differential $z$ compared to PYTHIA8 Monash

Fig. Group : [poster] Measurement of the transverse momentum($j_T$) distributions of charged-particle jet fragments in pp collisions at $\sqrt{s}$ = 5.02 TeV with ALICE
PWG : PWG-JE (Jets)
Energy: 5.02 TeV
System: p-p

Jet $p_\mathrm{T}$ dependence of $j_\mathrm{T}$ distributions in inclusive $z$

Fig. Group : [poster] Measurement of the transverse momentum($j_T$) distributions of charged-particle jet fragments in pp collisions at $\sqrt{s}$ = 5.02 TeV with ALICE
PWG : PWG-JE (Jets)
Energy: 5.02 TeV
System: p-p

Jet $p_\mathrm{T}$ dependence of $j_\mathrm{T}$ distributions in low $z$

Fig. Group : [poster] Measurement of the transverse momentum($j_T$) distributions of charged-particle jet fragments in pp collisions at $\sqrt{s}$ = 5.02 TeV with ALICE
PWG : PWG-JE (Jets)
Energy: 5.02 TeV
System: p-p

Jet $p_\mathrm{T}$ dependence of $j_\mathrm{T}$ distributions in mid $z$

Fig. Group : [poster] Measurement of the transverse momentum($j_T$) distributions of charged-particle jet fragments in pp collisions at $\sqrt{s}$ = 5.02 TeV with ALICE
PWG : PWG-JE (Jets)
Energy: 5.02 TeV
System: p-p

Jet $p_\mathrm{T}$ dependence of $j_\mathrm{T}$ distributions in high $z$

Fig. Group : [poster] Measurement of the transverse momentum($j_T$) distributions of charged-particle jet fragments in pp collisions at $\sqrt{s}$ = 5.02 TeV with ALICE
PWG : PWG-JE (Jets)
Energy: 5.02 TeV
System: p-p

Xic+ to Xi pi pi versus multiplicity in pp at 13 TeV

Invariant mass distribution of Xic+ in high multiplicity class

Fig. Group : Xic+ to Xi pi pi versus multiplicity in pp at 13 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13 TeV
System: p-p

ROC curve for high multiplicity, transverse momentum 6 to 8 GeV interval

Fig. Group : Xic+ to Xi pi pi versus multiplicity in pp at 13 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13 TeV
System: p-p

BDT output distribution in high multiplicity, transverse momentum 6 to 8 GeV interval

Fig. Group : Xic+ to Xi pi pi versus multiplicity in pp at 13 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13 TeV
System: p-p

Prompt efficiency of Xic+ for different multiplicity classes

Fig. Group : Xic+ to Xi pi pi versus multiplicity in pp at 13 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13 TeV
System: p-p

Xic+ over D0 for different multiplicity classes

Fig. Group : Xic+ to Xi pi pi versus multiplicity in pp at 13 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13 TeV
System: p-p

Corrected yield of Xic+ for different multiplicity classes with ratio to INEL>0 classes

Fig. Group : Xic+ to Xi pi pi versus multiplicity in pp at 13 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13 TeV
System: p-p

psi-to-jpsi analysis at midrapidity in pp at 13.6 TeV (QM2023)

psi and jpsi signal extraction from 13.6 TeV pp data

Fig. Group : psi-to-jpsi analysis at midrapidity in pp at 13.6 TeV (QM2023)
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 13.6 TeV
System: p-p

psi-to-jpsi ratio as function of the pT at midrapidity in pp at 13.6 TeV, compared with the similar measurements from forward rapidity

Fig. Group : psi-to-jpsi analysis at midrapidity in pp at 13.6 TeV (QM2023)
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 13.6 TeV
System: p-p

y-differential J/psi photoproduction in Pb-Pb (QM2023)

y-differential coherent J/psi photoproduction cross section at pT < 0.3 GeV/c in the centrality range (70-90)% in Pb-Pb collisions at 5.02 TeV with data points only

Fig. Group : y-differential J/psi photoproduction in Pb-Pb (QM2023)
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 5.02 TeV
System: Pb-Pb

y-differential raw J/psi yield as a function of pT in the centrality range (70-90)% in Pb-Pb collisions at 5.02 TeV

Fig. Group : y-differential J/psi photoproduction in Pb-Pb (QM2023)
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 5.02 TeV
System: Pb-Pb

y-differential J/psi production cross section at forward y as a function of pT in pp collisions at 5.02 TeV

Fig. Group : y-differential J/psi photoproduction in Pb-Pb (QM2023)
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 5.02 TeV
System: p-p

The J/psi nuclear modification factor as a function of pT in the centrality range (70-90)% in Pb-Pb collisions at 5.02 TeV for 3.75 < y < 4

Fig. Group : y-differential J/psi photoproduction in Pb-Pb (QM2023)
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 5.02 TeV
System: Pb-Pb

The J/psi nuclear modification factor as a function of pT in the centrality range (70-90)% in Pb-Pb collisions at 5.02 TeV for 3.5 < y < 3.75

Fig. Group : y-differential J/psi photoproduction in Pb-Pb (QM2023)
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 5.02 TeV
System: Pb-Pb

The J/psi nuclear modification factor as a function of pT in the centrality range (70-90)% in Pb-Pb collisions at 5.02 TeV for 3.25 < y < 3.5

Fig. Group : y-differential J/psi photoproduction in Pb-Pb (QM2023)
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 5.02 TeV
System: Pb-Pb

The J/psi nuclear modification factor as a function of pT in the centrality range (70-90)% in Pb-Pb collisions at 5.02 TeV for 3 < y < 3.25

Fig. Group : y-differential J/psi photoproduction in Pb-Pb (QM2023)
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 5.02 TeV
System: Pb-Pb

The J/psi nuclear modification factor as a function of pT in the centrality range (70-90)% in Pb-Pb collisions at 5.02 TeV for 2.75 < y < 3

Fig. Group : y-differential J/psi photoproduction in Pb-Pb (QM2023)
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 5.02 TeV
System: Pb-Pb

The J/psi nuclear modification factor as a function of pT in the centrality range (70-90)% in Pb-Pb collisions at 5.02 TeV for 2.5 < y < 2.75

Fig. Group : y-differential J/psi photoproduction in Pb-Pb (QM2023)
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 5.02 TeV
System: Pb-Pb

The J/psi nuclear modification factor for six y intervals at forward rapidity as a function of pT, pT < 3 GeV/c, in the centrality range (70-90)% in Pb-Pb collisions at 5.02 TeV

Fig. Group : y-differential J/psi photoproduction in Pb-Pb (QM2023)
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 5.02 TeV
System: Pb-Pb

The J/psi nuclear modification factor for six y intervals at forward rapidity as a function of pT in the centrality range (70-90)% in Pb-Pb collisions at 5.02 TeV

Fig. Group : y-differential J/psi photoproduction in Pb-Pb (QM2023)
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 5.02 TeV
System: Pb-Pb

y-differential coherent J/psi photoproduction cross section at pT < 0.3 GeV/c in the centrality range (70-90)% in Pb-Pb collisions at 5.02 TeV compared with one set of models of different scenarios

Fig. Group : y-differential J/psi photoproduction in Pb-Pb (QM2023)
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 5.02 TeV
System: Pb-Pb

y-differential coherent J/psi photoproduction cross section at pT < 0.3 GeV/c in the centrality range (70-90)% in Pb-Pb collisions at 5.02 TeV

Fig. Group : y-differential J/psi photoproduction in Pb-Pb (QM2023)
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 5.02 TeV
System: Pb-Pb

Mesons inside jets: Figures as function of z

Eta/Pi0 ratio as function of z for different jet pT intervals

Fig. Group : Mesons inside jets: Figures as function of z
PWG : PWG-EM (Electromagnetic probes)
Energy: 13 TeV
System: p-p

Ratio of Pi0 z spectra (Fragmentation function) for data and PYTHIA to parameterization

Fig. Group : Mesons inside jets: Figures as function of z
PWG : PWG-EM (Electromagnetic probes)
Energy: 13 TeV
System: p-p

Comparison of corrected Eta spectra inside jets from different reconstruction methods as function of z

Fig. Group : Mesons inside jets: Figures as function of z
PWG : PWG-EM (Electromagnetic probes)
Energy: 13 TeV
System: p-p

Comparison of corrected Pi0 spectra inside jets from different reconstruction methods as function of z

Fig. Group : Mesons inside jets: Figures as function of z
PWG : PWG-EM (Electromagnetic probes)
Energy: 13 TeV
System: p-p

Mesons inside jets: Figures as function of pT

Eta/Pi0 ratio inside jets as function of pT for different jet pT intervals

Fig. Group : Mesons inside jets: Figures as function of pT
PWG : PWG-EM (Electromagnetic probes)
Energy: 13 TeV
System: p-p

Ratio of fully corrected Eta pT spectra inside jets (data and PYTHIA) to parameterization

Fig. Group : Mesons inside jets: Figures as function of pT
PWG : PWG-EM (Electromagnetic probes)
Energy: 13 TeV
System: p-p

Eta pT spectra in different jet pT intervals normalized per jet

Fig. Group : Mesons inside jets: Figures as function of pT
PWG : PWG-EM (Electromagnetic probes)
Energy: 13 TeV
System: p-p

Ratio of fully corrected Pi0 pT spectra inside jets (data and PYTHIA) to parameterization

Fig. Group : Mesons inside jets: Figures as function of pT
PWG : PWG-EM (Electromagnetic probes)
Energy: 13 TeV
System: p-p

Pi0 pT spectra in different jet pT intervals normalized per jet

Fig. Group : Mesons inside jets: Figures as function of pT
PWG : PWG-EM (Electromagnetic probes)
Energy: 13 TeV
System: p-p

Ratio of Eta pT spectra in different jet pT intervals to a fit to the inclusive Eta spectrum

Fig. Group : Mesons inside jets: Figures as function of pT
PWG : PWG-EM (Electromagnetic probes)
Energy: 13 TeV
System: p-p

Eta pT spectra in different jet pT intervals normalized per event

Fig. Group : Mesons inside jets: Figures as function of pT
PWG : PWG-EM (Electromagnetic probes)
Energy: 13 TeV
System: p-p

Ratio of Pi0 pT spectra in different jet pT intervals to a fit to the inclusive Pi0 spectrum

Fig. Group : Mesons inside jets: Figures as function of pT
PWG : PWG-EM (Electromagnetic probes)
Energy: 13 TeV
System: p-p

Pi0 pT spectra in different jet pT intervals normalized per event and the inclusive Pi0 spectrum

Fig. Group : Mesons inside jets: Figures as function of pT
PWG : PWG-EM (Electromagnetic probes)
Energy: 13 TeV
System: p-p

Pi0 pT spectra in different jet pT intervals normalized per event

Fig. Group : Mesons inside jets: Figures as function of pT
PWG : PWG-EM (Electromagnetic probes)
Energy: 13 TeV
System: p-p

CERN Accelerating science

User

Public Preliminary figures by analysis

Public Preliminary figures by analysis

Measurements of the groomed and ungroomed jet mass in pp and Pb-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV

Physics Analysis Group: Spectra

$\Omega_{\rm c}^{0}$ production in semileptonic decay channel in pp collisions at $\sqrt s$ = 13 TeV

Xic multiplicity dependence via hadronic decay in proton-proton collisions at s√=13 TeV

Azimuthal correlations between heavy-flavour decay electrons and charged particles in Pb-Pb collisions at 5.02 TeV

Measurement of inclusive jet distributions in central Pb-Pb collisions at 5.02 TeV with a novel mixed-event approach.

LcOverD0_pPb_5.02TeV

[poster] Measurement of the transverse momentum($j_T$) distributions of charged-particle jet fragments in pp collisions at $\sqrt{s}$ = 5.02 TeV with ALICE

Xic+ to Xi pi pi versus multiplicity in pp at 13 TeV

psi-to-jpsi analysis at midrapidity in pp at 13.6 TeV (QM2023)

y-differential J/psi photoproduction in Pb-Pb (QM2023)

Mesons inside jets: Figures as function of z

Mesons inside jets: Figures as function of pT

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