User


Roles
Anonymous

Public Preliminary figures by analysis

Title

ID number ALI-PREL-XXX

Figure Caption

Scope: PWG

System

Energy

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

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

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: 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

Response matrix for R=0.3 jets 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

Corrected jet $p_{T,jet}$ distribution with $p_{T}^{lead} > 5$ 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 inclusive jet $p_{T,jet}^{reco}$ distribution 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 $p_{T}^{lead} > 5$ 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 inclusive jet $p_{T,jet}^{reco}$ distribution of the SE and ME 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 $p_{T}^{lead} > 5$ 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

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

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

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 high $z$

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

psi-to-jpsi analysis at midrapidity in pp at 13.6 TeV (QM2023)

psi and jpsi signal extraction from 13.6 TeV pp data

Fig. Group : psi-to-jpsi analysis at midrapidity in pp at 13.6 TeV (QM2023)
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 13.6 TeV
System: p-p

psi-to-jpsi ratio as function of the pT at midrapidity in pp at 13.6 TeV, compared with the similar measurements from forward rapidity

Fig. Group : psi-to-jpsi analysis at midrapidity in pp at 13.6 TeV (QM2023)
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 13.6 TeV
System: p-p

y-differential J/psi photoproduction in Pb-Pb (QM2023)

y-differential coherent J/psi photoproduction cross section at pT < 0.3 GeV/c in the centrality range (70-90)% in Pb-Pb collisions at 5.02 TeV with data points only

Fig. Group : y-differential J/psi photoproduction in Pb-Pb (QM2023)
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 5.02 TeV
System: Pb-Pb

y-differential raw J/psi yield as a function of pT in the centrality range (70-90)% in Pb-Pb collisions at 5.02 TeV

Fig. Group : y-differential J/psi photoproduction in Pb-Pb (QM2023)
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 5.02 TeV
System: Pb-Pb

y-differential J/psi production cross section at forward y as a function of pT in pp collisions at 5.02 TeV

Fig. Group : y-differential J/psi photoproduction in Pb-Pb (QM2023)
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 5.02 TeV
System: p-p

The J/psi nuclear modification factor as a function of pT in the centrality range (70-90)% in Pb-Pb collisions at 5.02 TeV for 3.75 < y < 4

Fig. Group : y-differential J/psi photoproduction in Pb-Pb (QM2023)
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 5.02 TeV
System: Pb-Pb

The J/psi nuclear modification factor as a function of pT in the centrality range (70-90)% in Pb-Pb collisions at 5.02 TeV for 3.5 < y < 3.75

Fig. Group : y-differential J/psi photoproduction in Pb-Pb (QM2023)
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 5.02 TeV
System: Pb-Pb

The J/psi nuclear modification factor as a function of pT in the centrality range (70-90)% in Pb-Pb collisions at 5.02 TeV for 3.25 < y < 3.5

Fig. Group : y-differential J/psi photoproduction in Pb-Pb (QM2023)
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 5.02 TeV
System: Pb-Pb

The J/psi nuclear modification factor as a function of pT in the centrality range (70-90)% in Pb-Pb collisions at 5.02 TeV for 3 < y < 3.25

Fig. Group : y-differential J/psi photoproduction in Pb-Pb (QM2023)
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 5.02 TeV
System: Pb-Pb

The J/psi nuclear modification factor as a function of pT in the centrality range (70-90)% in Pb-Pb collisions at 5.02 TeV for 2.75 < y < 3

Fig. Group : y-differential J/psi photoproduction in Pb-Pb (QM2023)
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 5.02 TeV
System: Pb-Pb

The J/psi nuclear modification factor as a function of pT in the centrality range (70-90)% in Pb-Pb collisions at 5.02 TeV for 2.5 < y < 2.75

Fig. Group : y-differential J/psi photoproduction in Pb-Pb (QM2023)
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 5.02 TeV
System: Pb-Pb

The J/psi nuclear modification factor for six y intervals at forward rapidity as a function of pT, pT < 3 GeV/c, in the centrality range (70-90)% in Pb-Pb collisions at 5.02 TeV

Fig. Group : y-differential J/psi photoproduction in Pb-Pb (QM2023)
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 5.02 TeV
System: Pb-Pb

The J/psi nuclear modification factor for six y intervals at forward rapidity as a function of pT in the centrality range (70-90)% in Pb-Pb collisions at 5.02 TeV

Fig. Group : y-differential J/psi photoproduction in Pb-Pb (QM2023)
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 5.02 TeV
System: Pb-Pb

y-differential coherent J/psi photoproduction cross section at pT < 0.3 GeV/c in the centrality range (70-90)% in Pb-Pb collisions at 5.02 TeV compared with one set of models of different scenarios

Fig. Group : y-differential J/psi photoproduction in Pb-Pb (QM2023)
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 5.02 TeV
System: Pb-Pb

y-differential coherent J/psi photoproduction cross section at pT < 0.3 GeV/c in the centrality range (70-90)% in Pb-Pb collisions at 5.02 TeV

Fig. Group : y-differential J/psi photoproduction in Pb-Pb (QM2023)
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 5.02 TeV
System: Pb-Pb

Mesons inside jets: Figures as function of z

Eta/Pi0 ratio as function of z for different jet pT intervals

Fig. Group : Mesons inside jets: Figures as function of z
PWG : PWG-EM (Electromagnetic probes)
Energy: 13 TeV
System: p-p

Ratio of Pi0 z spectra (Fragmentation function) for data and PYTHIA to parameterization

Fig. Group : Mesons inside jets: Figures as function of z
PWG : PWG-EM (Electromagnetic probes)
Energy: 13 TeV
System: p-p

Comparison of corrected Eta spectra inside jets from different reconstruction methods as function of z

Fig. Group : Mesons inside jets: Figures as function of z
PWG : PWG-EM (Electromagnetic probes)
Energy: 13 TeV
System: p-p

Comparison of corrected Pi0 spectra inside jets from different reconstruction methods as function of z

Fig. Group : Mesons inside jets: Figures as function of z
PWG : PWG-EM (Electromagnetic probes)
Energy: 13 TeV
System: p-p

Mesons inside jets: Figures as function of pT

Eta/Pi0 ratio inside jets as function of pT for different jet pT intervals

Fig. Group : Mesons inside jets: Figures as function of pT
PWG : PWG-EM (Electromagnetic probes)
Energy: 13 TeV
System: p-p

Ratio of fully corrected Eta pT spectra inside jets (data and PYTHIA) to parameterization

Fig. Group : Mesons inside jets: Figures as function of pT
PWG : PWG-EM (Electromagnetic probes)
Energy: 13 TeV
System: p-p

Eta pT spectra in different jet pT intervals normalized per jet

Fig. Group : Mesons inside jets: Figures as function of pT
PWG : PWG-EM (Electromagnetic probes)
Energy: 13 TeV
System: p-p

Ratio of fully corrected Pi0 pT spectra inside jets (data and PYTHIA) to parameterization

Fig. Group : Mesons inside jets: Figures as function of pT
PWG : PWG-EM (Electromagnetic probes)
Energy: 13 TeV
System: p-p

Pi0 pT spectra in different jet pT intervals normalized per jet

Fig. Group : Mesons inside jets: Figures as function of pT
PWG : PWG-EM (Electromagnetic probes)
Energy: 13 TeV
System: p-p

Ratio of Eta pT spectra in different jet pT intervals to a fit to the inclusive Eta spectrum

Fig. Group : Mesons inside jets: Figures as function of pT
PWG : PWG-EM (Electromagnetic probes)
Energy: 13 TeV
System: p-p

Eta pT spectra in different jet pT intervals normalized per event

Fig. Group : Mesons inside jets: Figures as function of pT
PWG : PWG-EM (Electromagnetic probes)
Energy: 13 TeV
System: p-p

Ratio of Pi0 pT spectra in different jet pT intervals to a fit to the inclusive Pi0 spectrum

Fig. Group : Mesons inside jets: Figures as function of pT
PWG : PWG-EM (Electromagnetic probes)
Energy: 13 TeV
System: p-p

Pi0 pT spectra in different jet pT intervals normalized per event and the inclusive Pi0 spectrum

Fig. Group : Mesons inside jets: Figures as function of pT
PWG : PWG-EM (Electromagnetic probes)
Energy: 13 TeV
System: p-p

Pi0 pT spectra in different jet pT intervals normalized per event

Fig. Group : Mesons inside jets: Figures as function of pT
PWG : PWG-EM (Electromagnetic probes)
Energy: 13 TeV
System: p-p

Polarization of photoproduced J/psi in Pb-Pb (QM2023)

Comparison of $\lambda_{\theta}$ with UPC measurement

Fig. Group : Polarization of photoproduced J/psi in Pb-Pb (QM2023)
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 5.02 TeV
System: Pb-Pb

dNdcostheta vs costheta in Pb--Pb collisions at 5.02 TeV using Helicity Frame

Fig. Group : Polarization of photoproduced J/psi in Pb-Pb (QM2023)
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 5.02 TeV
System: Pb-Pb

Invariant mass distribution of dimuon pairs for 0.5 < |cos\theta| < 0.6 in Pb-Pb collsions at 5.02 TeV

Fig. Group : Polarization of photoproduced J/psi in Pb-Pb (QM2023)
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 5.02 TeV
System: Pb-Pb

Invariant mass distribution of dimuon pairs for 0.2 < |cos\theta| < 0.3 in Pb-Pb collsions at 5.02 TeV

Fig. Group : Polarization of photoproduced J/psi in Pb-Pb (QM2023)
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 5.02 TeV
System: Pb-Pb

Invariant mass distribution of dimuon pairs for 0.0 < |cos\theta| < 0.1 in Pb-Pb collsions at 5.02 TeV

Fig. Group : Polarization of photoproduced J/psi in Pb-Pb (QM2023)
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 5.02 TeV
System: Pb-Pb

Upsilon cross section in pp collisions at 13 TeV (HP2023)

y-differential upsilon(1S) and upsilon(2S) pp cross section at 13 TeV compared to ICEM+FONLL

Fig. Group : Upsilon cross section in pp collisions at 13 TeV (HP2023)
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 13 TeV
System: p-p

pT differential Upsilon(1S) and upsilon(2S) cross section in pp collisions at 13 TeV compared to ICEM+FONLL

Fig. Group : Upsilon cross section in pp collisions at 13 TeV (HP2023)
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 13 TeV
System: p-p

Integrated Upsilon(1S) and Upsilon(2S) cross section as a function of energy compared to ICEM+FONLL model calculations

Fig. Group : Upsilon cross section in pp collisions at 13 TeV (HP2023)
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 13 TeV
System: p-p

pT differential Upsilon(1S) and upsilon(2S) cross section in pp collisions at 13 TeV compared to LHCb

Fig. Group : Upsilon cross section in pp collisions at 13 TeV (HP2023)
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 13 TeV
System: p-p

y-differential upsilon(1S) pp cross section at 13 TeV compared to lower energy ALICE data

Fig. Group : Upsilon cross section in pp collisions at 13 TeV (HP2023)
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 13 TeV
System: p-p

y-differential upsilon(1S) and upsilon(2S) pp cross section at 13 TeV compared to LHCb

Fig. Group : Upsilon cross section in pp collisions at 13 TeV (HP2023)
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 13 TeV
System: p-p

y-differential upsilon(1S) and upsilon(2S) pp cross section at 13 TeV

Fig. Group : Upsilon cross section in pp collisions at 13 TeV (HP2023)
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 13 TeV
System: p-p

pT differential Upsilon(1S) and Upsilon(2S) cross section in pp collisions at 13 TeV

Fig. Group : Upsilon cross section in pp collisions at 13 TeV (HP2023)
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 13 TeV
System: p-p

pT differential Upsilon(1S) cross section in pp collisions at 13 TeV compared to lower energy ALICE data

Fig. Group : Upsilon cross section in pp collisions at 13 TeV (HP2023)
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 13 TeV
System: p-p

D0-tagged jet angularity measurement in pp collisions at $\sqrt{s}$ = 5.02 TeV

D0-tagged jets compared to semi-inclusive jets and to PYTHIA 8 on left and to their ratio on right for $\alpha=3$, $R=0.4$ in 10 < $p_{\rm T, ch. jet}$ < 20 GeV/c.

Fig. Group : D0-tagged jet angularity measurement in pp collisions at $\sqrt{s}$ = 5.02 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV
System: p-p

D0-tagged jets compared to semi-inclusive jets and to PYTHIA 8 on left and to their ratio on right for $\alpha=2$, $R=0.4$ in 10 < $p_{\rm T, ch. jet}$ < 20 GeV/c.

Fig. Group : D0-tagged jet angularity measurement in pp collisions at $\sqrt{s}$ = 5.02 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV
System: p-p

D0-tagged jets compared to semi-inclusive jets and to PYTHIA 8 on left and to their ratio on right for $\alpha=1.5$, $R=0.4$ in 10 < $p_{\rm T, ch. jet}$ < 20 GeV/c.

Fig. Group : D0-tagged jet angularity measurement in pp collisions at $\sqrt{s}$ = 5.02 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV
System: p-p

D0-tagged jets compared to semi-inclusive jets and to PYTHIA 8 on left and to their ratio on right for $\alpha=1$, $R=0.4$ in 10 < $p_{\rm T, ch. jet}$ < 20 GeV/c.

Fig. Group : D0-tagged jet angularity measurement in pp collisions at $\sqrt{s}$ = 5.02 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV
System: p-p

Feed-down fraction in D$^{0}$-tagged jet angularity in 10 < $p_{\rm T, ch. jet}$ < 20 GeV/c and 5 < $p_{\rm T,D^{0}}$ < 20 GeV/c for R = 0.4, $\alpha=1$.

Fig. Group : D0-tagged jet angularity measurement in pp collisions at $\sqrt{s}$ = 5.02 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV
System: p-p

Fully corrected jet angularity distributions of D0-tagged jet compared to semi-inclusive jets and to PYTHIA 8 for $\alpha=3$, $R=0.4$ in 10 < $p_{\rm T, ch. jet}$ < 20 GeV/c.

Fig. Group : D0-tagged jet angularity measurement in pp collisions at $\sqrt{s}$ = 5.02 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV
System: p-p

Fully corrected jet angularity distributions of D0-tagged jet compared to semi-inclusive jets and to PYTHIA 8 for $\alpha=2$, $R=0.4$ in 10 < $p_{\rm T, ch. jet}$ < 20 GeV/c.

Fig. Group : D0-tagged jet angularity measurement in pp collisions at $\sqrt{s}$ = 5.02 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV
System: p-p

Fully corrected jet angularity distributions of D0-tagged jet compared to semi-inclusive jets and to PYTHIA 8 for $\alpha=1.5$, $R=0.4$ in 10 < $p_{\rm T, ch. jet}$ < 20 GeV/c.

Fig. Group : D0-tagged jet angularity measurement in pp collisions at $\sqrt{s}$ = 5.02 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV
System: p-p

D0-tagged jet raw angularity distributions for $\alpha=1$ in 10 < $p_{\rm T, ch. jet}$ < 20 GeV/c and 8 < $p_{\rm T,D^{0}}$ < 12 GeV/c.

Fig. Group : D0-tagged jet angularity measurement in pp collisions at $\sqrt{s}$ = 5.02 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV
System: p-p

Invariant mass distribution of D$^{0}$-tagged jet candidates with 10 < $p_{\rm T, ch. jet}$ < 20 GeV/c and 8 < $p_{\rm T,D^{0}}$ < 12 GeV/c for R = 0.4.

Fig. Group : D0-tagged jet angularity measurement in pp collisions at $\sqrt{s}$ = 5.02 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV
System: p-p

Fully corrected jet angularity distributions of D0-tagged jet compared to semi-inclusive jets and to PYTHIA 8 for $\alpha=1$, $R=0.4$ in 10 < $p_{\rm T, ch. jet}$ < 20 GeV/c.

Fig. Group : D0-tagged jet angularity measurement in pp collisions at $\sqrt{s}$ = 5.02 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV
System: p-p

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

Invariant Cross-Section Ratios of Different Jet Radii for pp Full Jet Spectra 8 TeV with Comparison to PYTHIA8

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

Ds-jet longitudinal momentum fraction in pp collisions at 13 TeV

The comparison of longitudinal momentum fraction of $\rm D_{s}^{+}$ and $\rm D^{0}$ -tagged 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

Longitudinal momentum fraction of $\rm D_{s}^{+}$-tagged 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

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

CERN Accelerating science