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ID number ALI-PREL-XXX

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Scope: PWG

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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
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
$\omega$/$\pi$ 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
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
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
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
$\mathrm{D_s^+/D^+}$ 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
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

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