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Figure Caption

Scope: PWG

System

Energy

[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

Measured $j_\mathrm{T}$ distributions in mid $z$ bin compared to PYTHIA8 Tune4C

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

Measured $j_\mathrm{T}$ distributions in low $z$ bin compared to PYTHIA8 Tune4C

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

Measured $j_\mathrm{T}$ distributions in inclusive $z$ bin compared to PYTHIA8 Tune4C

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

Measured $j_\mathrm{T}$ distributions in high $z$ bin compared to Herwig

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

Measured $j_\mathrm{T}$ distributions in mid $z$ bin compared to Herwig

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

Measured $j_\mathrm{T}$ distributions in low $z$ bin compared to Herwig

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

Measured $j_\mathrm{T}$ distributions in inclusive $z$ bin compared to Herwig

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

Measurement of heavy-flavor production in the high-mass dimuon spectrum in pp collisions at sqrt{s}=13 TeV with ALICE (HP2023)

[HP 2023] Beauty cross section as a function of rapidity compared with FONLL prediction (NNPDF pdf)

Fig. Group : Measurement of heavy-flavor production in the high-mass dimuon spectrum in pp collisions at sqrt{s}=13 TeV with ALICE (HP2023)
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 13 TeV
System: p-p

[HP 2023] Beauty cross section as a function of rapidity compared with FONLL prediction (CTEQ6 pdf)

Fig. Group : Measurement of heavy-flavor production in the high-mass dimuon spectrum in pp collisions at sqrt{s}=13 TeV with ALICE (HP2023)
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 13 TeV
System: p-p

[HP 2023] Charm cross section as a function of rapidity compared with FONLL prediction (CTEQ6 pdf)

Fig. Group : Measurement of heavy-flavor production in the high-mass dimuon spectrum in pp collisions at sqrt{s}=13 TeV with ALICE (HP2023)
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 13 TeV
System: p-p

[HP 2023] Charm cross section as a function of rapidity compared with FONLL prediction (NNPDF pdf)

Fig. Group : Measurement of heavy-flavor production in the high-mass dimuon spectrum in pp collisions at sqrt{s}=13 TeV with ALICE (HP2023)
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 13 TeV
System: p-p

[HP 2023] Simultaneous unbinned fit to dimuon data distribution (transverse momentum component)

Fig. Group : Measurement of heavy-flavor production in the high-mass dimuon spectrum in pp collisions at sqrt{s}=13 TeV with ALICE (HP2023)
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 13 TeV
System: p-p

[HP 2023] Simultaneous unbinned fit to dimuon data distribution (mass component)

Fig. Group : Measurement of heavy-flavor production in the high-mass dimuon spectrum in pp collisions at sqrt{s}=13 TeV with ALICE (HP2023)
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 13 TeV
System: p-p

[HP 2023] Dimuon invariant mass distribution with m>4 Gev/c^2

Fig. Group : Measurement of heavy-flavor production in the high-mass dimuon spectrum in pp collisions at sqrt{s}=13 TeV with ALICE (HP2023)
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 13 TeV
System: p-p

Preliminary: Full Jet Spectra - pp 8 TeV, p--Pb 8.16 TeV

Comparison of the Invariant Cross-Section Ratio for R = 0.2/0.5 Full Jets in pp to PYTHIA8 Monash

Fig. Group : Preliminary: Full Jet Spectra - pp 8 TeV, p--Pb 8.16 TeV
PWG : PWG-JE (Jets)
Energy: 8 TeV
System: p-p

Comparison of the Invariant Cross-Section Ratio for R = 0.2/0.4 Full Jets in pp to PYTHIA8 Monash

Fig. Group : Preliminary: Full Jet Spectra - pp 8 TeV, p--Pb 8.16 TeV
PWG : PWG-JE (Jets)
Energy: 8 TeV
System: p-p

Comparison of the Invariant Cross-Section Ratio for R = 0.2/0.3 Full Jets in pp to PYTHIA8 Monash

Fig. Group : Preliminary: Full Jet Spectra - pp 8 TeV, p--Pb 8.16 TeV
PWG : PWG-JE (Jets)
Energy: 8 TeV
System: p-p

Comparison of the Invariant Cross-Section for R = 0.5 Full Jets in pp to PYTHIA8 Monash

Fig. Group : Preliminary: Full Jet Spectra - pp 8 TeV, p--Pb 8.16 TeV
PWG : PWG-JE (Jets)
Energy: 8 TeV
System: p-p

Comparison of the Invariant Cross-Section for R = 0.4 Full Jets in pp to PYTHIA8 Monash

Fig. Group : Preliminary: Full Jet Spectra - pp 8 TeV, p--Pb 8.16 TeV
PWG : PWG-JE (Jets)
Energy: 8 TeV
System: p-p

Comparison of the Invariant Cross-Section for R = 0.3 Full Jets in pp to PYTHIA8 Monash

Fig. Group : Preliminary: Full Jet Spectra - pp 8 TeV, p--Pb 8.16 TeV
PWG : PWG-JE (Jets)
Energy: 8 TeV
System: p-p

Comparison of the Invariant Cross-Section for R = 0.2 Full Jets in pp to PYTHIA8 Monash

Fig. Group : Preliminary: Full Jet Spectra - pp 8 TeV, p--Pb 8.16 TeV
PWG : PWG-JE (Jets)
Energy: 8 TeV
System: p-p

$\sqrt{s}$ Comparison for Several Bins in $p_{T}^{jet}$ for R = 0.5 - 2.76, 5, 8, 13 TeV

Fig. Group : Preliminary: Full Jet Spectra - pp 8 TeV, p--Pb 8.16 TeV
PWG : PWG-JE (Jets)
Energy: 2.76 TeV, 5.02 TeV, 8 TeV, 13 TeV
System: p-p

$\sqrt{s}$ Comparison for Several Bins in $p_{T}^{jet}$ for R = 0.4 - 2.76, 5, 8, 13 TeV

Fig. Group : Preliminary: Full Jet Spectra - pp 8 TeV, p--Pb 8.16 TeV
PWG : PWG-JE (Jets)
Energy: 2.76 TeV, 5.02 TeV, 8 TeV, 13 TeV
System: p-p

$\sqrt{s}$ Comparison for Several Bins in $p_{T}^{jet}$ for R = 0.3 - 2.76, 5, 8, 13 TeV

Fig. Group : Preliminary: Full Jet Spectra - pp 8 TeV, p--Pb 8.16 TeV
PWG : PWG-JE (Jets)
Energy: 2.76 TeV, 5.02 TeV, 8 TeV, 13 TeV
System: p-p

$\sqrt{s}$ Comparison for Several Bins in $p_{T}^{jet}$ for R = 0.2 - 2.76, 5, 8, 13 TeV

Fig. Group : Preliminary: Full Jet Spectra - pp 8 TeV, p--Pb 8.16 TeV
PWG : PWG-JE (Jets)
Energy: 2.76 TeV, 5.02 TeV, 8 TeV, 13 TeV
System: p-p

Compilation of Invariant Cross-Sections for R = 0.5 in pp Full Jet Spectra - 5, 8, 13 TeV

Fig. Group : Preliminary: Full Jet Spectra - pp 8 TeV, p--Pb 8.16 TeV
PWG : PWG-JE (Jets)
Energy: 5.02 TeV, 8 TeV, 13 TeV
System: p-p

Compilation of Invariant Cross-Sections for R = 0.4 in pp Full Jet Spectra - 2.76, 5, 8, 13 TeV

Fig. Group : Preliminary: Full Jet Spectra - pp 8 TeV, p--Pb 8.16 TeV
PWG : PWG-JE (Jets)
Energy: 2.76 TeV, 5.02 TeV, 8 TeV, 13 TeV
System: p-p

Compilation of Invariant Cross-Sections for R = 0.3 in pp Full Jet Spectra - 5, 8, 13 TeV

Fig. Group : Preliminary: Full Jet Spectra - pp 8 TeV, p--Pb 8.16 TeV
PWG : PWG-JE (Jets)
Energy: 5.02 TeV, 8 TeV, 13 TeV
System: p-p

Compilation of Invariant Cross-Sections for R = 0.2 in pp Full Jet Spectra - 2.76, 5, 8, 13 TeV

Fig. Group : Preliminary: Full Jet Spectra - pp 8 TeV, p--Pb 8.16 TeV
PWG : PWG-JE (Jets)
Energy: 2.76 TeV, 5.02 TeV, 8 TeV, 13 TeV
System: p-p

Compilation of Invariant Cross-Section Ratios of R = 0.2/0.5 in pp Full Jet Spectra - 5, 8, 13 TeV

Fig. Group : Preliminary: Full Jet Spectra - pp 8 TeV, p--Pb 8.16 TeV
PWG : PWG-JE (Jets)
Energy: 5.02 TeV, 8 TeV, 13 TeV
System: p-p

Compilation of Invariant Cross-Section Ratios of R = 0.2/0.4 in pp Full Jet Spectra - 2.76, 5, 8, 13 TeV

Fig. Group : Preliminary: Full Jet Spectra - pp 8 TeV, p--Pb 8.16 TeV
PWG : PWG-JE (Jets)
Energy: 2.76 TeV, 5.02 TeV, 8 TeV, 13 TeV
System: p-p

Compilation of Invariant Cross-Section Ratios of R = 0.2/0.3 in pp Full Jet Spectra - 5, 8, 13 TeV

Fig. Group : Preliminary: Full Jet Spectra - pp 8 TeV, p--Pb 8.16 TeV
PWG : PWG-JE (Jets)
Energy: 5.02 TeV, 8 TeV, 13 TeV
System: p-p

Invariant Cross-Section Ratios of Different Jet Radii for pp Full Jet Spectra 8 TeV

Fig. Group : Preliminary: Full Jet Spectra - pp 8 TeV, p--Pb 8.16 TeV
PWG : PWG-JE (Jets)
Energy: 8 TeV
System: p-p

Invariant Cross-Section pp Full Jet Spectra 8 TeV, R = 0.2 -0.5

Fig. Group : Preliminary: Full Jet Spectra - pp 8 TeV, p--Pb 8.16 TeV
PWG : PWG-JE (Jets)
Energy: 8 TeV
System: p-p

Fraction of Women in ALICE by Employment Category and Time (2014-2021, Final)

Fig. Group :
PWG : Diversity Office
Energy: none
System: none

Direct photon spectra in PbPb 5.02TeV

Direct photon spectra PbPb 5TeV ratios to model calculation, with PHENIX, 20-40%

Fig. Group : Direct photon spectra in PbPb 5.02TeV
PWG : PWG-EM (Electromagnetic probes)
Energy: 5.02 TeV
System: Pb-Pb

Direct photon spectra in PbPb 5.02TeV from PCM with comparison to all model calculations

Fig. Group : Direct photon spectra in PbPb 5.02TeV
PWG : PWG-EM (Electromagnetic probes)
Energy: 5.02 TeV
System: Pb-Pb

Longitudinal Fluctuations in Heavy-Ion Collisions with the ALICE Detector

Charge conservation effect in first longitudinal coefficient a_{1} as a function of <dNch/deta> in Xe-Xe collisions

Fig. Group : Longitudinal Fluctuations in Heavy-Ion Collisions with the ALICE Detector
PWG : PWG-CF (Flow and Correlations)
Energy: 5.44 TeV
System: Xe-Xe

Charge conservation effect in first longitudinal coefficient a_{1} as a function of <dNch/deta> in Pb-Pb collisions

Fig. Group : Longitudinal Fluctuations in Heavy-Ion Collisions with the ALICE Detector
PWG : PWG-CF (Flow and Correlations)
Energy: 5.02 TeV
System: Pb-Pb

First longitudinal coefficient a_{1} scaled with sqrt(<dNch/deta>) as a function of <dNch/deta> in Pb-Pb and Xe-Xe collisions

Fig. Group : Longitudinal Fluctuations in Heavy-Ion Collisions with the ALICE Detector
PWG : PWG-CF (Flow and Correlations)
Energy: 5.02 TeV, 5.44 TeV
System: Pb-Pb, Xe-Xe

First longitudinal coefficient a_{1} in Xe-Xe and Pb-Pb collisions as a function of <dNch/deta>

Fig. Group : Longitudinal Fluctuations in Heavy-Ion Collisions with the ALICE Detector
PWG : PWG-CF (Flow and Correlations)
Energy: 5.02 TeV, 5.44 TeV
System: Pb-Pb, Xe-Xe

$J/\psi$ $v_{2}$ in pp collisions at 13 TeV - QM2022

$p_T$ dependence of $J/\psi$ $v_2$ for various collision systems

Fig. Group : $J/\psi$ $v_{2}$ in pp collisions at 13 TeV - QM2022
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 13 TeV
System: p-p

Procedure of $V_{2,J/\psi-tracklet}$ extraction from $V_{2,dimuon-tracklet}(m_{\mu\mu})$

Fig. Group : $J/\psi$ $v_{2}$ in pp collisions at 13 TeV - QM2022
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 13 TeV
System: p-p

$p_T$ dependence of $J/\psi$ $v_2$ in pp collisions at 13 TeV - Yield subtraction method

Fig. Group : $J/\psi$ $v_{2}$ in pp collisions at 13 TeV - QM2022
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 13 TeV
System: p-p

$p_T$ dependence of $J/\psi$ $v_2$ in pp collisions at 13 TeV

Fig. Group : $J/\psi$ $v_{2}$ in pp collisions at 13 TeV - QM2022
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 13 TeV
System: p-p

Direct photon R_gamma in PbPb 5.02TeV

Direct photon double ratio in PbPb 5.02TeV from PCM with all models

Fig. Group : Direct photon R_gamma in PbPb 5.02TeV
PWG : PWG-EM (Electromagnetic probes)
Energy: 5.02 TeV
System: Pb-Pb

Double ratio 0-20% from PCM and 0-10% from Dielectrons

Fig. Group : Direct photon R_gamma in PbPb 5.02TeV
PWG : PWG-EM (Electromagnetic probes)
Energy: 5.02 TeV
System: Pb-Pb

Double ratio 60-80% with different model calculations

Fig. Group : Direct photon R_gamma in PbPb 5.02TeV
PWG : PWG-EM (Electromagnetic probes)
Energy: 5.02 TeV
System: Pb-Pb

Double ratio 40-60% with different model calculations

Fig. Group : Direct photon R_gamma in PbPb 5.02TeV
PWG : PWG-EM (Electromagnetic probes)
Energy: 5.02 TeV
System: Pb-Pb

Double ratio 20-40% with different model calculations

Fig. Group : Direct photon R_gamma in PbPb 5.02TeV
PWG : PWG-EM (Electromagnetic probes)
Energy: 5.02 TeV
System: Pb-Pb

Double ratio 0-20% with different model calculations

Fig. Group : Direct photon R_gamma in PbPb 5.02TeV
PWG : PWG-EM (Electromagnetic probes)
Energy: 5.02 TeV
System: Pb-Pb

Measurement of isolated photon-jet correlations in 5.02 TeV Pb-Pb collisions

Truncated mean of momentum imbalance between isolated photons and jets in 5.02 TeV Pb-Pb collisions with PYTHIA comparison

Fig. Group : Measurement of isolated photon-jet correlations in 5.02 TeV Pb-Pb collisions
PWG : PWG-JE (Jets)
Energy: 5.02 TeV
System: Pb-Pb

Momentum imbalance between isolated photons and jets in 5.02 TeV Pb-Pb collisions with PYTHIA comparison

Fig. Group : Measurement of isolated photon-jet correlations in 5.02 TeV Pb-Pb collisions
PWG : PWG-JE (Jets)
Energy: 5.02 TeV
System: Pb-Pb

Angular correlations between isolated photons and jets in 5.02 TeV Pb-Pb collisions with PYTHIA comparison

Fig. Group : Measurement of isolated photon-jet correlations in 5.02 TeV Pb-Pb collisions
PWG : PWG-JE (Jets)
Energy: 5.02 TeV
System: Pb-Pb

Momentum imbalance between isolated photons and jets in 5.02 TeV Pb-Pb collisions

Fig. Group : Measurement of isolated photon-jet correlations in 5.02 TeV Pb-Pb collisions
PWG : PWG-JE (Jets)
Energy: 5.02 TeV
System: Pb-Pb

Angular correlations between isolated photons and jets in 5.02 TeV Pb-Pb collisions

Fig. Group : Measurement of isolated photon-jet correlations in 5.02 TeV Pb-Pb collisions
PWG : PWG-JE (Jets)
Energy: 5.02 TeV
System: Pb-Pb

Subtraction procedure with same/mixed event for momentum imbalance between isolated photons and jets in 0-30% Pb-Pb collisions

Fig. Group : Measurement of isolated photon-jet correlations in 5.02 TeV Pb-Pb collisions
PWG : PWG-JE (Jets)
Energy: 5.02 TeV
System: Pb-Pb

Event shape and multiplicity dependence of K*(892)$^{\mathbf{\pm}}$ production at mid-rapidity in pp collisions at $\sqrt{s}$ = 13 TeV

$\it{p}_{T}$-differential K*(892)$^{\mathbf{\pm}}$-to-Proton ratio as a function of spherocity ($S_{0}^{p_{T}=1}$) in pp collisions at $\sqrt{s}$ = 13 TeV (I-III V0M multiplicity class)

Fig. Group : Event shape and multiplicity dependence of K*(892)$^{\mathbf{\pm}}$ production at mid-rapidity in pp collisions at $\sqrt{s}$ = 13 TeV
PWG : PWG-LF (Light Flavour Spectra)
Energy: 13 TeV
System: p-p

$\it{p}_{T}$-differential K*(892)$^{\mathbf{\pm}}$-to-Kaon ratio as a function of spherocity ($S_{0}^{p_{T}=1}$) in pp collisions at $\sqrt{s}$ = 13 TeV (I-III V0M multiplicity class)

Fig. Group : Event shape and multiplicity dependence of K*(892)$^{\mathbf{\pm}}$ production at mid-rapidity in pp collisions at $\sqrt{s}$ = 13 TeV
PWG : PWG-LF (Light Flavour Spectra)
Energy: 13 TeV
System: p-p

$\it{p}_{T}$-differential K*(892)$^{\mathbf{\pm}}$-to-Pion ratio as a function of spherocity ($S_{0}^{p_{T}=1}$) in pp collisions at $\sqrt{s}$ = 13 TeV (I-III V0M multiplicity class)

Fig. Group : Event shape and multiplicity dependence of K*(892)$^{\mathbf{\pm}}$ production at mid-rapidity in pp collisions at $\sqrt{s}$ = 13 TeV
PWG : PWG-LF (Light Flavour Spectra)
Energy: 13 TeV
System: p-p

Transverse Momentum spectra of K*(892)$^{\mathbf{\pm}}$ in (I-III) V0M Multiplicity class and 5% $S_{0}^{p_{T}=1}$ in pp collisions at $\sqrt{s}$ = 13 TeV

Fig. Group : Event shape and multiplicity dependence of K*(892)$^{\mathbf{\pm}}$ production at mid-rapidity in pp collisions at $\sqrt{s}$ = 13 TeV
PWG : PWG-LF (Light Flavour Spectra)
Energy: 13 TeV
System: p-p

Transverse Momentum spectra of K*(892)$^{\mathbf{\pm}}$ in (I-III) V0M Multiplicity class and 10% $S_{0}^{p_{T}=1}$ in pp collisions at $\sqrt{s}$ = 13 TeV

Fig. Group : Event shape and multiplicity dependence of K*(892)$^{\mathbf{\pm}}$ production at mid-rapidity in pp collisions at $\sqrt{s}$ = 13 TeV
PWG : PWG-LF (Light Flavour Spectra)
Energy: 13 TeV
System: p-p

Transverse Momentum spectra of K*(892)$^{\mathbf{\pm}}$ in (I-III) V0M Multiplicity class and 20% $S_{0}^{p_{T}=1}$ in pp collisions at $\sqrt{s}$ = 13 TeV

Fig. Group : Event shape and multiplicity dependence of K*(892)$^{\mathbf{\pm}}$ production at mid-rapidity in pp collisions at $\sqrt{s}$ = 13 TeV
PWG : PWG-LF (Light Flavour Spectra)
Energy: 13 TeV
System: p-p

$\phi$-meson pair measurement

Results for $\phi$ meson production characterisation in pp collisions at $\sqrt{s}$ = 7 TeV

Fig. Group : $\phi$-meson pair measurement
PWG : PWG-LF (Light Flavour Spectra)
Energy: 7 TeV
System: p-p

[QM2022] - omega meson production in pp collisions at 13 TeV

Acceptance Times Efficiency

Fig. Group : [QM2022] - omega meson production in pp collisions at 13 TeV
PWG : PWG-EM (Electromagnetic probes)
Energy: 13 TeV
System: p-p

Charged-particle jet properties in p-Pb collisions at 5.02 TeV

Underlying event (UE) subtraction procedure for $z^{\rm ch}$ distribution for leading jet $p_{\rm T,jet}^{\rm ch}$ = 40-60 GeV/$c$ in p-Pb collisions at 5.02 TeV

Fig. Group : Charged-particle jet properties in p-Pb collisions at 5.02 TeV
PWG : PWG-JE (Jets)
Energy: 5.02 TeV
System: p-Pb

Underlying event (UE) subtraction procedure for $\langle N_{\rm ch}\rangle$ distribution as a function of leading jet $p_{\rm T,jet}^{\rm ch}$ in p-Pb collisions at 5.02 TeV

Fig. Group : Charged-particle jet properties in p-Pb collisions at 5.02 TeV
PWG : PWG-JE (Jets)
Energy: 5.02 TeV
System: p-Pb

V0s in p-Pb 8.16 TeV

Nuclear Modification Factor in p-Pb 8.16 TeV for K0S and Lambda

Fig. Group : V0s in p-Pb 8.16 TeV
PWG : PWG-LF (Light Flavour Spectra)
Energy: 8 TeV
System: p-Pb

Ratio of Lambda to K0s as a function of charge particle multiplicity

Fig. Group : V0s in p-Pb 8.16 TeV
PWG : PWG-LF (Light Flavour Spectra)
Energy: 8 TeV
System: p-Pb

Ratio of Lambda to K0s as a function of transverse momentum

Fig. Group : V0s in p-Pb 8.16 TeV
PWG : PWG-LF (Light Flavour Spectra)
Energy: 8 TeV
System: p-Pb

Ratio of Lambda yield to pions yield as a function of multiplicity

Fig. Group : V0s in p-Pb 8.16 TeV
PWG : PWG-LF (Light Flavour Spectra)
Energy: 8 TeV
System: p-Pb

Ratio of K0S yield to pions yield as a function of multiplicity

Fig. Group : V0s in p-Pb 8.16 TeV
PWG : PWG-LF (Light Flavour Spectra)
Energy: 8 TeV
System: p-Pb

Average transverse momentum as a function of multiplicity for Lambda including Pb-Pb data points

Fig. Group : V0s in p-Pb 8.16 TeV
PWG : PWG-LF (Light Flavour Spectra)
Energy: 8 TeV
System: p-Pb

Average transverse momentum as a function of multiplicity for Lambda

Fig. Group : V0s in p-Pb 8.16 TeV
PWG : PWG-LF (Light Flavour Spectra)
Energy: 8 TeV
System: p-Pb

Average transverse momentum as a function of multiplicity for K0s including Pb-Pb data points

Fig. Group : V0s in p-Pb 8.16 TeV
PWG : PWG-LF (Light Flavour Spectra)
Energy: 8 TeV
System: p-Pb

Average transverse momentum as a function of multiplicity for K0s

Fig. Group : V0s in p-Pb 8.16 TeV
PWG : PWG-LF (Light Flavour Spectra)
Energy: 8 TeV
System: p-Pb

pT integrated yield of Lambda as a function of multiplicity including Pb-Pb data points

Fig. Group : V0s in p-Pb 8.16 TeV
PWG : PWG-LF (Light Flavour Spectra)
Energy: 8 TeV
System: p-Pb

pT integrated yield of Lambda as a function of multiplicity

Fig. Group : V0s in p-Pb 8.16 TeV
PWG : PWG-LF (Light Flavour Spectra)
Energy: 8 TeV
System: p-Pb

pT integrated yield of K0s as a function of multiplicity including Pb-Pb data points

Fig. Group : V0s in p-Pb 8.16 TeV
PWG : PWG-LF (Light Flavour Spectra)
Energy: 8 TeV
System: p-Pb

pT integrated yield of K0s as a function of multiplicity

Fig. Group : V0s in p-Pb 8.16 TeV
PWG : PWG-LF (Light Flavour Spectra)
Energy: 8 TeV
System: p-Pb

Transverse momentum spectra of Anti-Lambda in p-Pb 8.16 TeV and ratio to NSD

Fig. Group : V0s in p-Pb 8.16 TeV
PWG : PWG-LF (Light Flavour Spectra)
Energy: 8 TeV
System: p-Pb

Transverse momentum spectra of Anti-Lambda in p-Pb 8.16 TeV

Fig. Group : V0s in p-Pb 8.16 TeV
PWG : PWG-LF (Light Flavour Spectra)
Energy: 8 TeV
System: p-Pb

Transverse momentum spectra of Lambda in p-Pb 8.16 TeV and ratio to NSD

Fig. Group : V0s in p-Pb 8.16 TeV
PWG : PWG-LF (Light Flavour Spectra)
Energy: 8 TeV
System: p-Pb

Transverse momentum spectra of Lambda in p-Pb 8.16 TeV

Fig. Group : V0s in p-Pb 8.16 TeV
PWG : PWG-LF (Light Flavour Spectra)
Energy: 8 TeV
System: p-Pb

Transverse momentum spectra of K^{0}_{S} in p-Pb 8.16 TeV and ratio to NSD

Fig. Group : V0s in p-Pb 8.16 TeV
PWG : PWG-LF (Light Flavour Spectra)
Energy: 8 TeV
System: p-Pb

Transverse momentum spectra of K^{0}_{S} in p-Pb 8.16 TeV

Fig. Group : V0s in p-Pb 8.16 TeV
PWG : PWG-LF (Light Flavour Spectra)
Energy: 8 TeV
System: p-Pb

Average D mesons production vs unweighted spherocity S0 in pp at $\sqrt{s}$ = 13 TeV

D-mesons self normalised yield vs spherocity in [20,81] $N_{\mathrm{trk}}$

Fig. Group : Average D mesons production vs unweighted spherocity S0 in pp at $\sqrt{s}$ = 13 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13 TeV
System: p-p

D-mesons self normalised yield vs spherocity in [31,81] $N_{\mathrm{trk}}$

Fig. Group : Average D mesons production vs unweighted spherocity S0 in pp at $\sqrt{s}$ = 13 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13 TeV
System: p-p

D-mesons self normalised yield vs spherocity in [20,30] $N_{\mathrm{trk}}$

Fig. Group : Average D mesons production vs unweighted spherocity S0 in pp at $\sqrt{s}$ = 13 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13 TeV
System: p-p

Reconstruction of Beauty Jets in Proton-Proton Collisions at sqrt{s}=13\,TeV

Template fit to untagged data sample for performance estimation

Fig. Group : Reconstruction of Beauty Jets in Proton-Proton Collisions at sqrt{s}=13\,TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13 TeV
System: p-p

Template fit to b-tagged data sample for performance estimation

Fig. Group : Reconstruction of Beauty Jets in Proton-Proton Collisions at sqrt{s}=13\,TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13 TeV
System: p-p

Purity for b-jet selection in 13 TeV pp

Fig. Group : Reconstruction of Beauty Jets in Proton-Proton Collisions at sqrt{s}=13\,TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13 TeV
System: p-p

Efficiency for b-jet selection in 13 TeV pp

Fig. Group : Reconstruction of Beauty Jets in Proton-Proton Collisions at sqrt{s}=13\,TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13 TeV
System: p-p

Comparison of b-jet fractions at 5.02 TeV and 13 TeV

Fig. Group : Reconstruction of Beauty Jets in Proton-Proton Collisions at sqrt{s}=13\,TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13 TeV
System: p-p

Comparison of b-jet spectra at 5.02 and 13 TeV

Fig. Group : Reconstruction of Beauty Jets in Proton-Proton Collisions at sqrt{s}=13\,TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13 TeV
System: p-p

Investigations of anisotropic flow using multiparticle azimuthal correlations

Symmetric cumulants SC(3,2) in pp with different 3-sub configurations

Fig. Group : Investigations of anisotropic flow using multiparticle azimuthal correlations
PWG : PWG-CF (Flow and Correlations)
Energy: 13 TeV
System: p-p

Multiplicity dependence of symmetric cumulants and normalized symmetric cumulants in pp collisions

Fig. Group : Investigations of anisotropic flow using multiparticle azimuthal correlations
PWG : PWG-CF (Flow and Correlations)
Energy: 5.02 TeV, 13 TeV
System: p-p

Multiplicity dependence of nonlinear flow modes in pp and Pb--Pb collisions

Fig. Group : Investigations of anisotropic flow using multiparticle azimuthal correlations
PWG : PWG-CF (Flow and Correlations)
Energy: 5.02 TeV, 13 TeV
System: p-p, Pb-Pb

Multiplicity dependence of vn{m} in pp collisions (larger multiplicity range)

Fig. Group : Investigations of anisotropic flow using multiparticle azimuthal correlations
PWG : PWG-CF (Flow and Correlations)
Energy: 13 TeV
System: p-p

Multiplicity dependence of vn{m} in pp collisions

Fig. Group : Investigations of anisotropic flow using multiparticle azimuthal correlations
PWG : PWG-CF (Flow and Correlations)
Energy: 13 TeV
System: p-p

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