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Figure Caption

Scope: PWG

System

Energy

Direct photon R_gamma in PbPb 5.02TeV

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

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

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

Direct photon double ratio in PbPb 5.02TeV from PCM with pQCD

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

Direct photon double ratio in PbPb 5.02TeV from PCM

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

Unfolded and UE subtracted $z^{\rm ch}$ distributions for different 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

$z^{\rm ch}$ 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

$z^{\rm ch}$ distribution for leading jet $p_{\rm T,jet}^{\rm ch}$ = 20-30 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

$\langle N_{\rm ch}\rangle$ 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

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

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

Subtraction procedure with total background 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

Subtraction procedure with same/mixed event for angular correlations 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

Subtraction procedure with total background for angular correlations 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

Systematic uncertainties for momentum imbalance between isolated photons and jets in 50-90% 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

Systematic uncertainties for momentum imbalance between isolated photons and jets in 30-50% 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

Systematic uncertainties 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

Systematic uncertainties for angular correlations between isolated photons and jets in 50-90% 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

Systematic uncertainties for angular correlations between isolated photons and jets in 30-50% 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

Systematic uncertainties for angular correlations 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

Photon purity 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

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

LcOverD0_pPb_5.02TeV

LcOverD0_pPb_pp

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

LcOverD0_pPb_PbPb

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

LcOverD0_pPb_3mult

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

LcOverD0_pPb_2mult

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

Measurement of Jet Constituent Yields in 5.02 TeV Pb-Pb Collisions with the ALICE Detector

Acceptance Corrected Jet-Hadron Correlation for In-Plane ch. + ne. jets, pT^jet = 20-40 GeV, pT^assoc. = 2-3 GeV, 5.02 TeV PbPb, 30-50 %

Fig. Group : Measurement of Jet Constituent Yields in 5.02 TeV Pb-Pb Collisions with the ALICE Detector
PWG : PWG-JE (Jets)
Energy: 5.02 TeV
System: Pb-Pb

Mixed Event Acceptance Correction for In-Plane ch. + ne. jets, pT^jet = 20-40 GeV, pT^assoc. = 2-3 GeV, 5.02 TeV PbPb, 30-50 %

Fig. Group : Measurement of Jet Constituent Yields in 5.02 TeV Pb-Pb Collisions with the ALICE Detector
PWG : PWG-JE (Jets)
Energy: 5.02 TeV
System: Pb-Pb

Raw Jet-Hadron Correlation for In-Plane ch. + ne. jets, pT^jet = 20-40 GeV, pT^assoc. = 2-3 GeV, 5.02 TeV PbPb, 30-50 %

Fig. Group : Measurement of Jet Constituent Yields in 5.02 TeV Pb-Pb Collisions with the ALICE Detector
PWG : PWG-JE (Jets)
Energy: 5.02 TeV
System: Pb-Pb

Mid/In Away Side Constituent Yield Ratio compared to JEWEL with no recoils, pT^jet = 20-40 GeV, pT^assoc. > 2 GeV, 5.02 TeV PbPb, 30-50 %

Fig. Group : Measurement of Jet Constituent Yields in 5.02 TeV Pb-Pb Collisions with the ALICE Detector
PWG : PWG-JE (Jets)
Energy: 5.02 TeV
System: Pb-Pb

Mid/In Near Side Constituent Yield Ratio compared to JEWEL with no recoils, pT^jet = 20-40 GeV, pT^assoc. > 2 GeV, 5.02 TeV PbPb, 30-50 %

Fig. Group : Measurement of Jet Constituent Yields in 5.02 TeV Pb-Pb Collisions with the ALICE Detector
PWG : PWG-JE (Jets)
Energy: 5.02 TeV
System: Pb-Pb

Out/In Away Side Constituent Yield Ratio compared to JEWEL with no recoils, pT^jet = 20-40 GeV, pT^assoc. > 2 GeV, 5.02 TeV PbPb, 30-50 %

Fig. Group : Measurement of Jet Constituent Yields in 5.02 TeV Pb-Pb Collisions with the ALICE Detector
PWG : PWG-JE (Jets)
Energy: 5.02 TeV
System: Pb-Pb

Out/In Near Side Constituent Yield Ratio compared to JEWEL with no recoils, pT^jet = 20-40 GeV, pT^assoc. > 2 GeV, 5.02 TeV PbPb, 30-50 %

Fig. Group : Measurement of Jet Constituent Yields in 5.02 TeV Pb-Pb Collisions with the ALICE Detector
PWG : PWG-JE (Jets)
Energy: 5.02 TeV
System: Pb-Pb

Mid/In Away Side Constituent Yield Ratio, pT^jet = 20-40 GeV, pT^assoc. > 2 GeV, 5.02 TeV PbPb, 30-50 %

Fig. Group : Measurement of Jet Constituent Yields in 5.02 TeV Pb-Pb Collisions with the ALICE Detector
PWG : PWG-JE (Jets)
Energy: 5.02 TeV
System: Pb-Pb

Mid/In Near Side Constituent Yield Ratio, pT^jet = 20-40 GeV, pT^assoc. > 2 GeV, 5.02 TeV PbPb, 30-50 %

Fig. Group : Measurement of Jet Constituent Yields in 5.02 TeV Pb-Pb Collisions with the ALICE Detector
PWG : PWG-JE (Jets)
Energy: 5.02 TeV
System: Pb-Pb

Out/In Away Side Constituent Yield Ratio, pT^jet = 20-40 GeV, pT^assoc. > 2 GeV, 5.02 TeV PbPb, 30-50 %

Fig. Group : Measurement of Jet Constituent Yields in 5.02 TeV Pb-Pb Collisions with the ALICE Detector
PWG : PWG-JE (Jets)
Energy: 5.02 TeV
System: Pb-Pb

Out/In Near Side Constituent Yield Ratio, pT^jet = 20-40 GeV, pT^assoc. > 2 GeV, 5.02 TeV PbPb, 30-50 %

Fig. Group : Measurement of Jet Constituent Yields in 5.02 TeV Pb-Pb Collisions with the ALICE Detector
PWG : PWG-JE (Jets)
Energy: 5.02 TeV
System: Pb-Pb

Away Side Constituent Yields, pT^jet = 20-40 GeV, pT^assoc. > 2 GeV, 5.02 TeV PbPb, 30-50 %

Fig. Group : Measurement of Jet Constituent Yields in 5.02 TeV Pb-Pb Collisions with the ALICE Detector
PWG : PWG-JE (Jets)
Energy: 5.02 TeV
System: Pb-Pb

Near Side Constituent Yields, pT^jet = 20-40 GeV, pT^assoc. > 2 GeV, 5.02 TeV PbPb, 30-50 %

Fig. Group : Measurement of Jet Constituent Yields in 5.02 TeV Pb-Pb Collisions with the ALICE Detector
PWG : PWG-JE (Jets)
Energy: 5.02 TeV
System: Pb-Pb

$\Upsilon$(1S) polarization in pp collisions at $\sqrt{s}$ = 13 TeV with ALICE (QM2022)

$\Upsilon$(1S) polarization as a function of transverse momentum

Fig. Group : $\Upsilon$(1S) polarization in pp collisions at $\sqrt{s}$ = 13 TeV with ALICE (QM2022)
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 13 TeV
System: p-p

$\Upsilon$(1S) polarization: simultaneous fit to the corrected angular spectra in Helicity and Collins-Soper frames

Fig. Group : $\Upsilon$(1S) polarization in pp collisions at $\sqrt{s}$ = 13 TeV with ALICE (QM2022)
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 13 TeV
System: p-p

$\Upsilon$(1S) polarization: Signal extraction

Fig. Group : $\Upsilon$(1S) polarization in pp collisions at $\sqrt{s}$ = 13 TeV with ALICE (QM2022)
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 13 TeV
System: p-p

Direct photon spectra in PbPb 5.02TeV

Direct photon spectra PbPb 5TeV ratios to model calculation, LHC

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

Direct photon spectra PbPb 5TeV ratios to model calculation, with those from dielectrons and RHIC

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

Direct photon spectra ratios to model calculation

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 pQCD

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

[QM2022] - Direct photon HBT correlations in pp and PbPb collisions at 5 TeV

Lambda invariant for PbPb collisions at 5 TeV

Fig. Group : [QM2022] - Direct photon HBT correlations in pp and PbPb collisions at 5 TeV
PWG : PWG-EM (Electromagnetic probes)
Energy: 5.02 TeV
System: Pb-Pb

Gamma-Gamma correlations in 30-50% PbPb collisions at 5 TeV, 0.35<kT<0.5 GeV/c

Fig. Group : [QM2022] - Direct photon HBT correlations in pp and PbPb collisions at 5 TeV
PWG : PWG-EM (Electromagnetic probes)
Energy: 5.02 TeV
System: Pb-Pb

Gamma-Gamma correlations in 30-50% PbPb collisions at 5 TeV, 0.25<kT<0.35 GeV/c

Fig. Group : [QM2022] - Direct photon HBT correlations in pp and PbPb collisions at 5 TeV
PWG : PWG-EM (Electromagnetic probes)
Energy: 5.02 TeV
System: Pb-Pb

Gamma-Gamma correlations in 0-10% PbPb collisions at 5 TeV, 0.35<kT<0.5 GeV/c

Fig. Group : [QM2022] - Direct photon HBT correlations in pp and PbPb collisions at 5 TeV
PWG : PWG-EM (Electromagnetic probes)
Energy: 5.02 TeV
System: Pb-Pb

Gamma-Gamma correlations in 0-10% PbPb collisions at 5 TeV, 0.25<kT<0.35 GeV/c

Fig. Group : [QM2022] - Direct photon HBT correlations in pp and PbPb collisions at 5 TeV
PWG : PWG-EM (Electromagnetic probes)
Energy: 5.02 TeV
System: Pb-Pb

Gamma-Gamma correlations in pp collisions at 5 TeV, 0.5<kT<1.0 GeV/c

Fig. Group : [QM2022] - Direct photon HBT correlations in pp and PbPb collisions at 5 TeV
PWG : PWG-EM (Electromagnetic probes)
Energy: 5.02 TeV
System: p-p

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