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Figure Caption

Scope: PWG

System

Energy

Differential and Integrated event-by-event analysis of mean $\it{p}_\rm{T}$ correlations in pp collisions at $\sqrt{s}$ = 13 TeV at different $\it{p}_\rm{T}$ ranges

Normalized $\it{p}_{\rm{T}}$ correlator as a function of charged particle multiplicity for fixed $\it{p}_{\rm{T}}$ window sliding from lower to higher $\it{p}_{\rm{T}}$

Fig. Group : Differential and Integrated event-by-event analysis of mean $\it{p}_\rm{T}$ correlations in pp collisions at $\sqrt{s}$ = 13 TeV at different $\it{p}_\rm{T}$ ranges
PWG : PWG-CF (Flow and Correlations)
Energy: 13 TeV
System: p-p

Normalized $\it{p}_{\rm{T}}$ correlator as a function of charged particle multiplicity with increasing upper limit of $\it{p}_{\rm{T}}$ windows

Fig. Group : Differential and Integrated event-by-event analysis of mean $\it{p}_\rm{T}$ correlations in pp collisions at $\sqrt{s}$ = 13 TeV at different $\it{p}_\rm{T}$ ranges
PWG : PWG-CF (Flow and Correlations)
Energy: 13 TeV
System: p-p

Mean $\it{p}_{\rm{T}}$ as a function of charged particle multiplicity at fixed $\it{p}_{\rm{T}}$ window sliding from lower to higher $\it{p}_{\rm{T}}$

Fig. Group : Differential and Integrated event-by-event analysis of mean $\it{p}_\rm{T}$ correlations in pp collisions at $\sqrt{s}$ = 13 TeV at different $\it{p}_\rm{T}$ ranges
PWG : PWG-CF (Flow and Correlations)
Energy: 13 TeV
System: p-p

Mean $\it{p}_{\rm{T}}$ as a function of charged particle multiplicity for increasing upper limit of $\it{p}_{\rm{T}}$ windows

Fig. Group : Differential and Integrated event-by-event analysis of mean $\it{p}_\rm{T}$ correlations in pp collisions at $\sqrt{s}$ = 13 TeV at different $\it{p}_\rm{T}$ ranges
PWG : PWG-CF (Flow and Correlations)
Energy: 13 TeV
System: p-p

Jet substructure correlation of Soft Drop Rg and Zg

Ratio of zg distribution for wide and narrow jets in pp and Pb-Pb

Fig. Group : Jet substructure correlation of Soft Drop Rg and Zg
PWG : PWG-JE (Jets)
Energy: 5.02 TeV
System: p-p, Pb-Pb

Ratio of θg distribution for balanced and unbalanced jets in pp and Pb-Pb

Fig. Group : Jet substructure correlation of Soft Drop Rg and Zg
PWG : PWG-JE (Jets)
Energy: 5.02 TeV
System: p-p, Pb-Pb

zg distribution for wide jets in pp and Pb-Pb

Fig. Group : Jet substructure correlation of Soft Drop Rg and Zg
PWG : PWG-JE (Jets)
Energy: 5.02 TeV
System: p-p, Pb-Pb

zg distribution for narrow jets in pp and Pb-Pb

Fig. Group : Jet substructure correlation of Soft Drop Rg and Zg
PWG : PWG-JE (Jets)
Energy: 5.02 TeV
System: p-p, Pb-Pb

θg distribution for balanced jets in pp and Pb-Pb

Fig. Group : Jet substructure correlation of Soft Drop Rg and Zg
PWG : PWG-JE (Jets)
Energy: 5.02 TeV
System: p-p, Pb-Pb

θg distribution for unbalanced jets in pp and Pb-Pb

Fig. Group : Jet substructure correlation of Soft Drop Rg and Zg
PWG : PWG-JE (Jets)
Energy: 5.02 TeV
System: p-p, Pb-Pb

zg distribution for wide jets in Pb-Pb

Fig. Group : Jet substructure correlation of Soft Drop Rg and Zg
PWG : PWG-JE (Jets)
Energy: 5.02 TeV
System: Pb-Pb

zg distribution for narrow jets in Pb-Pb

Fig. Group : Jet substructure correlation of Soft Drop Rg and Zg
PWG : PWG-JE (Jets)
Energy: 5.02 TeV
System: Pb-Pb

θg distribution for balanced jets in Pb-Pb

Fig. Group : Jet substructure correlation of Soft Drop Rg and Zg
PWG : PWG-JE (Jets)
Energy: 5.02 TeV
System: Pb-Pb

θg distribution for unbalanced jets in Pb-Pb

Fig. Group : Jet substructure correlation of Soft Drop Rg and Zg
PWG : PWG-JE (Jets)
Energy: 5.02 TeV
System: Pb-Pb

zg distribution for wide jets in pp

Fig. Group : Jet substructure correlation of Soft Drop Rg and Zg
PWG : PWG-JE (Jets)
Energy: 5.02 TeV
System: p-p

zg distribution for narrow jets in pp

Fig. Group : Jet substructure correlation of Soft Drop Rg and Zg
PWG : PWG-JE (Jets)
Energy: 5.02 TeV
System: p-p

θg distribution for balanced jets in pp

Fig. Group : Jet substructure correlation of Soft Drop Rg and Zg
PWG : PWG-JE (Jets)
Energy: 5.02 TeV
System: p-p

θg distribution for unbalanced jets in pp

Fig. Group : Jet substructure correlation of Soft Drop Rg and Zg
PWG : PWG-JE (Jets)
Energy: 5.02 TeV
System: p-p

Energy-energy correlator measurements for jets in p-Pb collisions at 5.02TeV

EEC distributions of charged jets in p-Pb -- x (R_{L}) axis scaled by average jet pt

Fig. Group : Energy-energy correlator measurements for jets in p-Pb collisions at 5.02TeV
PWG : PWG-JE (Jets)
Energy: 5.02 TeV
System: p-Pb

Ratio of EECs in p-Pb /pp for 20-40 GeV/c jets with CGC comparisons

Fig. Group : Energy-energy correlator measurements for jets in p-Pb collisions at 5.02TeV
PWG : PWG-JE (Jets)
Energy: 5.02 TeV
System: p-Pb

Ratio of EECs in p-Pb/pp for 20-40 GeV/c jets with varying track pT cut (150 MeV, 1 GeV, 2 GeV)

Fig. Group : Energy-energy correlator measurements for jets in p-Pb collisions at 5.02TeV
PWG : PWG-JE (Jets)
Energy: 5.02 TeV
System: p-Pb

Ratio of EECs in p-Pb and pp in different jet pT bins (20-40, 40-60, 60-80 GeV)

Fig. Group : Energy-energy correlator measurements for jets in p-Pb collisions at 5.02TeV
PWG : PWG-JE (Jets)
Energy: 5.02 TeV
System: p-Pb

EEC distribution for charged jets in p-Pb collisions -- jet pT comparison (20-40, 40-60, 60-80 GeV)

Fig. Group : Energy-energy correlator measurements for jets in p-Pb collisions at 5.02TeV
PWG : PWG-JE (Jets)
Energy: 5.02 TeV
System: p-Pb

Spin alignment of prompt and non-prompt D∗+ mesons in pp collisions at √s = 13.6 TeV

Measurement spin alignment of prompt and non-prompt D∗+ mesons for both helicity and production frame in pp collisions at √s = 13.6 TeV

Fig. Group : Spin alignment of prompt and non-prompt D∗+ mesons in pp collisions at √s = 13.6 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13.6 TeV
System: p-p

Linear fit of #rho_{00}$ as function of non-promp fraction in both helicity and production frame

Fig. Group : Spin alignment of prompt and non-prompt D∗+ mesons in pp collisions at √s = 13.6 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13.6 TeV
System: p-p

$\rho_{00}$ extraction in different cut of BDT score for non-prompt D* for helicity and production frame

Fig. Group : Spin alignment of prompt and non-prompt D∗+ mesons in pp collisions at √s = 13.6 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13.6 TeV
System: p-p

Measurement spin alignment of non-prompt D∗+ mesons compared to $J/\Psi$ meson measured by CMS

Fig. Group : Spin alignment of prompt and non-prompt D∗+ mesons in pp collisions at √s = 13.6 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13.6 TeV
System: p-p

D* mesons raw yield extraction in the 10<pT<20 GeV/c interval in pp collisions at s√=13.6 TeV

Fig. Group : Spin alignment of prompt and non-prompt D∗+ mesons in pp collisions at √s = 13.6 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13.6 TeV
System: p-p

Measurement spin alignment of prompt and non-prompt D∗+ mesons at production frame in pp collisions at √s = 13.6 TeV

Fig. Group : Spin alignment of prompt and non-prompt D∗+ mesons in pp collisions at √s = 13.6 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13.6 TeV
System: p-p

Measurement spin alignment of prompt and non-prompt D∗+ mesons at helicity frame in pp collisions at √s = 13.6 TeV

Fig. Group : Spin alignment of prompt and non-prompt D∗+ mesons in pp collisions at √s = 13.6 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13.6 TeV
System: p-p

[HP2024] low mass dileptons

$\omega$/$\pi$ ratio of ALICE and PHENIX measurements

Fig. Group : [HP2024] low mass dileptons
PWG : PWG-EM (Electromagnetic probes)
Energy: 5.02 TeV
System: p-p

$\omega$/$\pi$ ratio for pp collisions at a center-of-mass energy of 5.02TeV.

Fig. Group : [HP2024] low mass dileptons
PWG : PWG-EM (Electromagnetic probes)
Energy: 5.02 TeV
System: p-p

$\omega$/$\pi$ ratio in pp collisions at a center-of-mass energy of 5.02 TeV in comparison to measurements and model calculations

Fig. Group : [HP2024] low mass dileptons
PWG : PWG-EM (Electromagnetic probes)
Energy: 5.02 TeV
System: p-p

Spectrum of \omega yield for inelastic pp collisions at $\sqrt{s}$ = 5.02 TeV as a function of $p_{\rm T}$

Fig. Group : [HP2024] low mass dileptons
PWG : PWG-EM (Electromagnetic probes)
Energy: 5.02 TeV
System: p-p

Jpsi v2 in Pb-Pb collisions at 5.36 TeV at fwd rapidity

J/ψ v2 vs pT at forward rapidity in the dimuon channel at 5.36 TeV vs J/ψ v2 at 5.02 TeV

Fig. Group : Jpsi v2 in Pb-Pb collisions at 5.36 TeV at fwd rapidity
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 5.36 TeV
System: Pb-Pb

J/ψ v2 vs pT at forward rapidity in the dimuon channel for the centrality class 10-50% and at 5.36 TeV

Fig. Group : Jpsi v2 in Pb-Pb collisions at 5.36 TeV at fwd rapidity
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 5.36 TeV
System: Pb-Pb

Measurement of charged particle correlations in Pb--Pb collisions at Pb-P collisions at 5.36 TeV

ICP as a function of <Npart> for pT = 4-6 GeV/c in Pb-Pb collisions at 5.36 TeV and comparison with Pb-Pb collisions at 2.76 TeV

Fig. Group : Measurement of charged particle correlations in Pb--Pb collisions at Pb-P collisions at 5.36 TeV
PWG : PWG-CF (Flow and Correlations)
Energy: 5.36 TeV
System: Pb-Pb

ICP as a function of <Npart> for pT = 6-8 GeV/c in Pb-Pb collisions at 5.36 TeV

Fig. Group : Measurement of charged particle correlations in Pb--Pb collisions at Pb-P collisions at 5.36 TeV
PWG : PWG-CF (Flow and Correlations)
Energy: 5.36 TeV
System: Pb-Pb

ICP as a function of <Npart> for pT = 4-6 GeV/c in Pb-Pb collisions at 5.36 TeV

Fig. Group : Measurement of charged particle correlations in Pb--Pb collisions at Pb-P collisions at 5.36 TeV
PWG : PWG-CF (Flow and Correlations)
Energy: 5.36 TeV
System: Pb-Pb

ICP as a function of <Npart> for pT = 3-4 GeV/c in Pb-Pb collisions at 5.36 TeV

Fig. Group : Measurement of charged particle correlations in Pb--Pb collisions at Pb-P collisions at 5.36 TeV
PWG : PWG-CF (Flow and Correlations)
Energy: 5.36 TeV
System: Pb-Pb

Non-prompt D^0 fraction in pp collisions at 13.6 TeV

Invariant-mass distribution of $\mathrm{D^0}$ candidates with $12 < p_\mathrm{T} < 16$ in pp collisions at $\sqrt{s} = 13.6$ TeV

Fig. Group : Non-prompt D^0 fraction in pp collisions at 13.6 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13.6 TeV
System: p-p

Invariant-mass fit of non-prompt $\rm D^0$ in pp collisions at 13.6 TeV

Fig. Group : Non-prompt D^0 fraction in pp collisions at 13.6 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13.6 TeV
System: p-p

Non-prompt $\rm D^0$ fraction as a function of $p_{\rm T}$

Fig. Group : Non-prompt D^0 fraction in pp collisions at 13.6 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13.6 TeV
System: p-p

Contributions of the estimated prompt and non-prompt $\rm D^0$ with the cut-variation method

Fig. Group : Non-prompt D^0 fraction in pp collisions at 13.6 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13.6 TeV
System: p-p

Invariant-mass fit of non-prompt $\rm D^0$ in pp collisions at 13.6 TeV

Fig. Group : Non-prompt D^0 fraction in pp collisions at 13.6 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13.6 TeV
System: p-p

$\mathrm{D_s^+/D^+}$ production yield ratio in pp collisions at $\sqrt{s}=13.6$ TeV

$\mathrm{D_s^+/D^+}$ production yield ratio measured in pp collisions at $\sqrt{s}=13.6$ TeV compared to PYTHIA 8, Catania and POWLANG predictions

Fig. Group : $\mathrm{D_s^+/D^+}$ production yield ratio in pp collisions at $\sqrt{s}=13.6$ TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13.6 TeV
System: p-p

$\mathrm{D_s^+/D^+}$ production yield ratio measured in pp collisions at midrapidity $(\lvert y\rvert<0.5)$ at $\sqrt{s}=13.6$ TeV compared to forward-rapidity measurements by LHCb

Fig. Group : $\mathrm{D_s^+/D^+}$ production yield ratio in pp collisions at $\sqrt{s}=13.6$ TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13.6 TeV
System: p-p

$\mathrm{D_s^+/D^+}$ production yield ratio measured in pp collisions at $\sqrt{s}=13.6$ TeV compared to measurements by ALICE at different centre-of-mass energies

Fig. Group : $\mathrm{D_s^+/D^+}$ production yield ratio in pp collisions at $\sqrt{s}=13.6$ TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13.6 TeV
System: p-p

Fit to the invariant-mass distribution of $\mathrm{D_s^+}$ and $\mathrm{D^+}$ mesons in the $5< \pt <5.5$ GeV/$c$ interval in pp collisions at $\sqrt{s}=13.6$ TeV

Fig. Group : $\mathrm{D_s^+/D^+}$ production yield ratio in pp collisions at $\sqrt{s}=13.6$ TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13.6 TeV
System: p-p

Fit to the invariant-mass distribution of $\mathrm{D_s^+}$ and $\mathrm{D^+}$ mesons in the $2< \pt <2.5$ GeV/$c$ interval in pp collisions at $\sqrt{s}=13.6$ TeV

Fig. Group : $\mathrm{D_s^+/D^+}$ production yield ratio in pp collisions at $\sqrt{s}=13.6$ TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13.6 TeV
System: p-p

Three-body femtoscopy in Run 3 with apass4 of 2022 data

ppΛ correlation function in Run3

Fig. Group : Three-body femtoscopy in Run 3 with apass4 of 2022 data
PWG : PWG-CF (Flow and Correlations)
Energy: 13.6 TeV
System: p-p

ppp correlation function in Run3

Fig. Group : Three-body femtoscopy in Run 3 with apass4 of 2022 data
PWG : PWG-CF (Flow and Correlations)
Energy: 13.6 TeV
System: p-p

ppΛ correlation function in Run3 compared to Run 2

Fig. Group : Three-body femtoscopy in Run 3 with apass4 of 2022 data
PWG : PWG-CF (Flow and Correlations)
Energy: 13.6 TeV
System: p-p

ppp correlation function in Run3 compared to Run 2

Fig. Group : Three-body femtoscopy in Run 3 with apass4 of 2022 data
PWG : PWG-CF (Flow and Correlations)
Energy: 13.6 TeV
System: p-p

Sigma_c(2520) / Sigma_c(2455) in pp collisions at 13.6 TeV

$\Sigma_{\rm c}^{0,++}(2520)/\Sigma_{\rm c}^{0,++}(2455)$ ratio in pp collisions at $\sqrt{s} = 13.6$ TeV compared with PYTHIA 8 predictions with Mode2, with variations on parameter probQQ1toQQ0join_charm

Fig. Group : Sigma_c(2520) / Sigma_c(2455) in pp collisions at 13.6 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13.6 TeV
System: p-p

$M({\rm pK\pi\pi}) - M({\rm pK\pi})$ distribution in the interval $8 < p_{\rm T} < 12$ GeV/$c$ in pp collisions at $\sqrt{s} = 13.6$ TeV

Fig. Group : Sigma_c(2520) / Sigma_c(2455) in pp collisions at 13.6 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13.6 TeV
System: p-p

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

Physics Analysis Group: Spectra

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

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

E3C and EEC measurements in jets in pp collisions at 5.02 and 13TeV

EEC collision energy dependence

Fig. Group : E3C and EEC measurements in jets in pp collisions at 5.02 and 13TeV
PWG : PWG-JE (Jets)
Energy: 13 TeV
System: p-p

E3C/EEC ratio theory comparison for 60-80 GeV charged jets

Fig. Group : E3C and EEC measurements in jets in pp collisions at 5.02 and 13TeV
PWG : PWG-JE (Jets)
Energy: 13 TeV
System: p-p

E3C/EEC ratio theory comparison for 40-60 GeV charged jets

Fig. Group : E3C and EEC measurements in jets in pp collisions at 5.02 and 13TeV
PWG : PWG-JE (Jets)
Energy: 13 TeV
System: p-p

E3C/EEC ratio theory comparison for 20-40 GeV charged jets

Fig. Group : E3C and EEC measurements in jets in pp collisions at 5.02 and 13TeV
PWG : PWG-JE (Jets)
Energy: 13 TeV
System: p-p

E3C/EEC ratio model comparison for 60-80 GeV charged jets

Fig. Group : E3C and EEC measurements in jets in pp collisions at 5.02 and 13TeV
PWG : PWG-JE (Jets)
Energy: 13 TeV
System: p-p

E3C/EEC ratio model comparison for 40-60 GeV charged jets

Fig. Group : E3C and EEC measurements in jets in pp collisions at 5.02 and 13TeV
PWG : PWG-JE (Jets)
Energy: 13 TeV
System: p-p

E3C/EEC ratio model comparison for 20-40 GeV charged jets

Fig. Group : E3C and EEC measurements in jets in pp collisions at 5.02 and 13TeV
PWG : PWG-JE (Jets)
Energy: 13 TeV
System: p-p

E3C model comparison for 60-80 GeV charged jets

Fig. Group : E3C and EEC measurements in jets in pp collisions at 5.02 and 13TeV
PWG : PWG-JE (Jets)
Energy: 13 TeV
System: p-p

E3C model comparison for 40-60 GeV charged jets

Fig. Group : E3C and EEC measurements in jets in pp collisions at 5.02 and 13TeV
PWG : PWG-JE (Jets)
Energy: 13 TeV
System: p-p

E3C model comparison for 20-40 GeV charged jets

Fig. Group : E3C and EEC measurements in jets in pp collisions at 5.02 and 13TeV
PWG : PWG-JE (Jets)
Energy: 13 TeV
System: p-p

EEC model comparison for 60-80 GeV charged jets

Fig. Group : E3C and EEC measurements in jets in pp collisions at 5.02 and 13TeV
PWG : PWG-JE (Jets)
Energy: 13 TeV
System: p-p

EEC model comparison for 40-60 GeV charged jets

Fig. Group : E3C and EEC measurements in jets in pp collisions at 5.02 and 13TeV
PWG : PWG-JE (Jets)
Energy: 13 TeV
System: p-p

EEC model comparison for 20-40 GeV charged jets

Fig. Group : E3C and EEC measurements in jets in pp collisions at 5.02 and 13TeV
PWG : PWG-JE (Jets)
Energy: 13 TeV
System: p-p

E3C/EEC ratio for charged jets in pp collisions at 13 TeV

Fig. Group : E3C and EEC measurements in jets in pp collisions at 5.02 and 13TeV
PWG : PWG-JE (Jets)
Energy: 13 TeV
System: p-p

E3C distribution for charged jets in pp collisions at 13 TeV

Fig. Group : E3C and EEC measurements in jets in pp collisions at 5.02 and 13TeV
PWG : PWG-JE (Jets)
Energy: 13 TeV
System: p-p

EEC distribution for charged jets in pp collisions at 13 TeV

Fig. Group : E3C and EEC measurements in jets in pp collisions at 5.02 and 13TeV
PWG : PWG-JE (Jets)
Energy: 13 TeV
System: p-p

LcOverD0_pPb_5.02TeV

D0_corrected_yield_pPb_5.02TeV

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

Lc_corrected_yield_pPb_5.02TeV

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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