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$\sqrt{s}$ 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 , Energy: 5.02 TeV , Energy: 8 TeV , Energy: 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 , Energy: 8 TeV , Energy: 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 , Energy: 5.02 TeV , Energy: 8 TeV , Energy: 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 , Energy: 8 TeV , Energy: 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 , Energy: 5.02 TeV , Energy: 8 TeV , Energy: 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 , Energy: 8 TeV , Energy: 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 , Energy: 5.02 TeV , Energy: 8 TeV , Energy: 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 , Energy: 8 TeV , Energy: 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) PWG : Diversity Office Energy: none System none
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
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
$p_T$ 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
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 , Energy: 5.44 TeV System Pb-Pb , System Xe-Xe
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
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 , Energy: 5.44 TeV System Pb-Pb , System Xe-Xe
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
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
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
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
*$\it{p}_{T}$-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
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
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
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
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
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
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
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
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
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 , Energy: 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 , Energy: 13 TeV System p-p , System 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
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
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
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
Multiplicity dependence of electrons from W boson and associate hadron production with W boson in pp collisions at 13 TeV with PYTHIA predictions Fig. Group : W production at midrapidity via single electrons in pp @ 13 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13 TeV System p-p
Multiplicity dependence of associate hadron production with W boson in pp collisions at 13 TeV with PYTHIA prediction Fig. Group : W production at midrapidity via single electrons in pp @ 13 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13 TeV System p-p
Multiplicity dependence of electrons from W boson and associate hadron production with W boson in pp collisions at 13 TeV Fig. Group : W production at midrapidity via single electrons in pp @ 13 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13 TeV System p-p
Multiplicity dependence of W boson production via electrons in pp collisions at 13 TeV with PYTHIA8 production Fig. Group : W production at midrapidity via single electrons in pp @ 13 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13 TeV System p-p
Multiplicity dependence of W boson production via electrons in pp collisions at 13 TeV Fig. Group : W production at midrapidity via single electrons in pp @ 13 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13 TeV System p-p
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

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