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Relative statistical and systematic uncertainties by categories of $\rm D_{s}^{+}$-tagged jets longitudinal momentum fraction in MB pp collisions at 13 TeV Fig. Group : Ds-jet longitudinal momentum fraction in pp collisions at 13 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13 TeV System p-p
Feed-down contribution of $\rm D_{s}^{+}$ jets from POWHEG+PYTHIA6+EvtGen in MB pp collisions at 13 TeV Fig. Group : Ds-jet longitudinal momentum fraction in pp collisions at 13 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13 TeV System p-p
Invariant mass distribution of $\rm D_{s}^{+}$ candidates inside jets in MB pp collisions at 13 TeV Fig. Group : Ds-jet longitudinal momentum fraction in pp collisions at 13 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13 TeV System p-p
Energy flow distributions overview Charged jets 60-80 GeV pp 13 TeV, R=0.05 to 0.1, R=0.2 to 0.25 and R=0.35 to 0.4 Fig. Group : Energy flow within jets in pp and Pb-Pb collisions with ALICE PWG : PWG-JE (Jets) Energy: 13 TeV System p-p
Energy flow distributions overview Charged jets 40-60 GeV pp 13 TeV, R=0.05 to 0.1, R=0.2 to 0.25 and R=0.35 to 0.4 Fig. Group : Energy flow within jets in pp and Pb-Pb collisions with ALICE PWG : PWG-JE (Jets) Energy: 13 TeV System p-p
Energy flow distributions overview Charged jets 60-80 GeV pp 13 TeV, All Rjet pairs Fig. Group : Energy flow within jets in pp and Pb-Pb collisions with ALICE PWG : PWG-JE (Jets) Energy: 13 TeV System p-p
Energy flow distributions overview Charged jets 40-60 GeV pp 13 TeV, All Rjet pairs Fig. Group : Energy flow within jets in pp and Pb-Pb collisions with ALICE PWG : PWG-JE (Jets) Energy: 13 TeV System p-p
Energy flow distributions with model comparison Charged jets 60-80 GeV pp 13 TeV, R=0.35 to R=0.4 Fig. Group : Energy flow within jets in pp and Pb-Pb collisions with ALICE PWG : PWG-JE (Jets) Energy: 13 TeV System p-p
Energy flow distributions with model comparison Charged jets 40-60 GeV pp 13 TeV, R=0.35 to R=0.4 Fig. Group : Energy flow within jets in pp and Pb-Pb collisions with ALICE PWG : PWG-JE (Jets) Energy: 13 TeV System p-p
Energy flow distributions with model comparison Charged jets 60-80 GeV pp 13 TeV, R=0.2 to R=0.25 Fig. Group : Energy flow within jets in pp and Pb-Pb collisions with ALICE PWG : PWG-JE (Jets) Energy: 13 TeV System p-p
Energy flow distributions with model comparison Charged jets 40-60 GeV pp 13 TeV, R=0.2 to R=0.25 Fig. Group : Energy flow within jets in pp and Pb-Pb collisions with ALICE PWG : PWG-JE (Jets) Energy: 13 TeV System p-p
Energy flow distributions with model comparison Charged jets 60-80 GeV pp 13 TeV, R=0.05 to R=0.1 Fig. Group : Energy flow within jets in pp and Pb-Pb collisions with ALICE PWG : PWG-JE (Jets) Energy: 13 TeV System p-p
Energy flow distributions with model comparison Charged jets 40-60 GeV pp 13 TeV, R=0.05 to R=0.1 Fig. Group : Energy flow within jets in pp and Pb-Pb collisions with ALICE PWG : PWG-JE (Jets) Energy: 13 TeV System p-p
Mean energy flow versus jet radius with model comparison Charged jets 60-80 GeV pp 13 TeV Fig. Group : Energy flow within jets in pp and Pb-Pb collisions with ALICE PWG : PWG-JE (Jets) Energy: 13 TeV System p-p
Mean energy flow versus jet radius with model comparison Charged jets 40-60 GeV pp 13 TeV Fig. Group : Energy flow within jets in pp and Pb-Pb collisions with ALICE PWG : PWG-JE (Jets) Energy: 13 TeV System p-p
Mean energy flow versus jet radius with jet pt dependence Charged jets pp 13 TeV Fig. Group : Energy flow within jets in pp and Pb-Pb collisions with ALICE PWG : PWG-JE (Jets) Energy: 13 TeV System p-p
Measured $j_\mathrm{T}$ distributions in high $z$ 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 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
[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
Experimental and theoretical uncertainties of the isolated prompt photon $R_{pA}$ at $\sqrt{s_{NN}}=8.16$ TeV Fig. Group : Isolated prompt photon production in p-Pb collisions at 8.16 TeV PWG : PWG-JE (Jets) Energy: 8 TeV System p-p , System p-Pb
Isolated prompt photon purity in p-Pb collisions at 8.16 TeV Fig. Group : Isolated prompt photon production in p-Pb collisions at 8.16 TeV PWG : PWG-JE (Jets) Energy: 8 TeV System p-Pb
Data/theory ratio of isolated prompt photon production in p-Pb collisions at 8.16 TeV compared to p-Pb data at 5.02 TeV Fig. Group : Isolated prompt photon production in p-Pb collisions at 8.16 TeV PWG : PWG-JE (Jets) Energy: 5.02 TeV , Energy: 8 TeV System p-Pb
Isolated prompt photon production cross section in pp and p-Pb collisions at 8.16 TeV Fig. Group : Isolated prompt photon production in p-Pb collisions at 8.16 TeV PWG : PWG-JE (Jets) Energy: 8 TeV System p-p , System p-Pb
Nuclear modification factor of isolated prompt photon production in p-Pb collisions at 8.16 TeV (log x) Fig. Group : Isolated prompt photon production in p-Pb collisions at 8.16 TeV PWG : PWG-JE (Jets) Energy: 8 TeV System p-p , System p-Pb
Nuclear modification factor of isolated prompt photon production in p-Pb collisions at 8.16 TeV Fig. Group : Isolated prompt photon production in p-Pb collisions at 8.16 TeV PWG : PWG-JE (Jets) Energy: 8 TeV System p-p , System p-Pb
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 , Energy: 5.02 TeV , Energy: 8 TeV , Energy: 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 , Energy: 5.02 TeV , Energy: 8 TeV , Energy: 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 , Energy: 5.02 TeV , Energy: 8 TeV , Energy: 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 , 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
Isolated photon differential cross section measured in p-Pb collisions at sqrt(s) = 5.02 TeV compared with JETPHOX and NLO theory Fig. Group : Nuclear modification factor and isolated photon cross section for 5.02 TeV pp and p-Pb PWG : PWG-JE (Jets) Energy: 5.02 TeV System p-Pb
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
v2 in central p-Pb collisions with pi, K, p,Lambda using improved template fit method compared to AMPT with string melting Fig. Group : Flow of identified particles in pp and p-Pb collisions PWG : PWG-CF (Flow and Correlations) Energy: 5.02 TeV System p-Pb
v2 in central p-Pb collisions with pi, K, p,Lambda using template fit method compared to AMPT with string melting Fig. Group : Flow of identified particles in pp and p-Pb collisions PWG : PWG-CF (Flow and Correlations) Energy: 5.02 TeV System p-Pb
Ratio of eta meson invariant cross sections for 6 energies together with NLO calculations and Pythia Fig. Group : [QM2022] - Neutral meson production in MB and multiplicity dependent pp collisions at 13TeV PWG : PWG-EM (Electromagnetic probes) Energy: 13 TeV System p-p
Ratio of pi0 invariant cross sections for 6 energies together with NLO calculations and Pythia Fig. Group : [QM2022] - Neutral meson production in MB and multiplicity dependent pp collisions at 13TeV PWG : PWG-EM (Electromagnetic probes) Energy: 13 TeV System p-p
Isolated photon cross section ratios in pp collisions $\sqrt s = $ 8 to 7 TeV Fig. Group : Isolated photon cross section in different energies and systems (QM2022) PWG : PWG-JE (Jets) Energy: 7 TeV , Energy: 8 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
Ratio to JETPHOX of Isolated photon differential cross section measured in p-Pb collisions at sqrt(s) = 5.02 TeV Fig. Group : Nuclear modification factor and isolated photon cross section for 5.02 TeV pp and p-Pb PWG : PWG-JE (Jets) Energy: 5.02 TeV System p-Pb
Isolated photon differential cross section measured in p-Pb collisions at sqrt(s) = 5.02 TeV Fig. Group : Nuclear modification factor and isolated photon cross section for 5.02 TeV pp and p-Pb PWG : PWG-JE (Jets) Energy: 5.02 TeV System p-Pb
Isolated photons cross section ratio with theory prediction Fig. Group : Isolated photons cross section in pp collisions at 8 TeV PWG : PWG-JE (Jets) Energy: 8 TeV System p-p
Isolated photons cross section comparison with theory Fig. Group : Isolated photons cross section in pp collisions at 8 TeV PWG : PWG-JE (Jets) Energy: 8 TeV System p-p
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
Isolated photons cross section comparison with theory and ratio Fig. Group : Isolated photons cross section in pp collisions at 8 TeV PWG : PWG-JE (Jets) Energy: 8 TeV System p-p
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

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