User


Roles
Anonymous

This Group is not Public

Search for Preliminary Figures

Title

ID number ALI-PREL-XXX

Figure Caption

Scope: PWG

System

Energy

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
$\Sigma_{\rm c}^{0,++}(2520)/\Sigma_{\rm c}^{0,++}(2455)$ 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
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
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
Omega over pion ratio as a function of the pion yield in pp collisions at 9 GeV, 7 TeV and 13.6 TeV PWG : PWG-LF (Light Flavour Spectra) Energy: 900 GeV , Energy: 7 TeV , Energy: 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 PWG : PWG-LF (Light Flavour Spectra) Energy: 900 GeV System p-p
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 , Energy: 13 TeV , Energy: 13.6 TeV System p-p
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
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
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
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 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 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
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
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
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
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
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
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

CERN Accelerating science

User

Warning message

Search for Preliminary Figures

< June >