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J/ψ, D0 and J/ψ-D0 cross sections vs HELAC-onia & PYTHIA (CharmoniumShower:all) Fig. Group : D0-J/ψ associated production in pp collisions at 13.6 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
J/ψ & D0 ratios vs PYTHIA (CharmoniumShower:all) Fig. Group : D0-J/ψ associated production in pp collisions at 13.6 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
dσ(J/ψ-D0) / dΔy vs HELAC-onia & PYTHIA (CharmoniumShower:all) (fwd-Δy only) Fig. Group : D0-J/ψ associated production in pp collisions at 13.6 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
dσ(J/ψ-D0) / dΔy vs HELAC-onia & PYTHIA (CharmoniumShower:all) Fig. Group : D0-J/ψ associated production in pp collisions at 13.6 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
dσ(J/ψ-D0) / dΔy vs HELAC-onia Fig. Group : D0-J/ψ associated production in pp collisions at 13.6 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
dσ(J/ψ-D0) / dΔy vs HELAC-onia (fwd-Δy only) Fig. Group : D0-J/ψ associated production in pp collisions at 13.6 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
χ2 distribution for σ effective extraction Fig. Group : D0-J/ψ associated production in pp collisions at 13.6 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
Projection along D0 axis of the 2D-fit to the D0-J/ψ(→μμ) mass distribution Axε weights applied Fig. Group : D0-J/ψ associated production in pp collisions at 13.6 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
Projection along J/ψ axis of the 2D-fit to the D0-J/ψ(→μμ) mass distribution Axε weights applied Fig. Group : D0-J/ψ associated production in pp collisions at 13.6 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
Projection along D0 axis of the 2D-fit to the D0-J/ψ(→μμ) mass distribution Fig. Group : D0-J/ψ associated production in pp collisions at 13.6 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
Projection along J/ψ axis of the 2D-fit to the D0-J/ψ(→μμ) mass distribution Fig. Group : D0-J/ψ associated production in pp collisions at 13.6 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
2D-fit to the D0-J/ψ(→μμ) mass distribution with Axε weights applied Fig. Group : D0-J/ψ associated production in pp collisions at 13.6 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
2D-fit to the D0-J/ψ(→μμ) mass distribution Fig. Group : D0-J/ψ associated production in pp collisions at 13.6 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
J/ψ v2 vs pT for the centrality class 30-50% and at 5.36 TeV compared to Upsilon(1S) 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 and ψ(2S) invariant mass Run 3 in dimuon channel at forward rapidity in 0-20% centrality bin, opposite sign mixed events Fig. Group : Charmonium production Run 3 in Pb-Pb collisions at √sNN = 5.36 TeV at forward rapidity PWG : PWG-DQ (Dileptons and Quarkonia) Energy: 5.36 TeV System Pb-Pb
J/ψ and ψ(2S) invariant mass Run 3 in dimuon channel at forward rapidity in 0-20% centrality bin, same-event opposite sign dimuons Fig. Group : Charmonium production Run 3 in Pb-Pb collisions at √sNN = 5.36 TeV at forward rapidity PWG : PWG-DQ (Dileptons and Quarkonia) Energy: 5.36 TeV System Pb-Pb
ψ(2S)-to-J/ψ ratio vs pT in Run 3 Pb-Pb collisions in the dimuon channel at forward rapidity with TAMU model Fig. Group : Charmonium production Run 3 in Pb-Pb collisions at √sNN = 5.36 TeV at forward rapidity PWG : PWG-DQ (Dileptons and Quarkonia) Energy: 5.36 TeV System Pb-Pb
Pb-Pb and smeared pp p/pi comparison - without inclusive comparison Fig. Group : pi, K, p in jets in 0-10% Pb-Pb and pp 5.02 TeV Preliminary PWG : PWG-JE (Jets) Energy: 5.02 TeV System p-p , System Pb-Pb
Pb-Pb and smeared pp K/pi comparison - without inclusive comparison Fig. Group : pi, K, p in jets in 0-10% Pb-Pb and pp 5.02 TeV Preliminary PWG : PWG-JE (Jets) Energy: 5.02 TeV System p-p , System Pb-Pb
Pb-Pb and smeared pp p/pi comparison - with inclusive comparison Fig. Group : pi, K, p in jets in 0-10% Pb-Pb and pp 5.02 TeV Preliminary PWG : PWG-JE (Jets) Energy: 5.02 TeV System p-p , System Pb-Pb
Pb-Pb and smeared pp K/pi comparison - with inclusive comparison Fig. Group : pi, K, p in jets in 0-10% Pb-Pb and pp 5.02 TeV Preliminary PWG : PWG-JE (Jets) Energy: 5.02 TeV System p-p , System Pb-Pb
Pb-Pb and smeared pp p spectra comparison Fig. Group : pi, K, p in jets in 0-10% Pb-Pb and pp 5.02 TeV Preliminary PWG : PWG-JE (Jets) Energy: 5.02 TeV System p-p , System Pb-Pb
Pb-Pb and smeared pp K spectra comparison Fig. Group : pi, K, p in jets in 0-10% Pb-Pb and pp 5.02 TeV Preliminary PWG : PWG-JE (Jets) Energy: 5.02 TeV System p-p , System Pb-Pb
Pb-Pb and smeared pp pi spectra comparison Fig. Group : pi, K, p in jets in 0-10% Pb-Pb and pp 5.02 TeV Preliminary PWG : PWG-JE (Jets) Energy: 5.02 TeV System p-p , System Pb-Pb
Standalone pp p/pi in jets - 3 curves Fig. Group : pi, K, p in jets in 0-10% Pb-Pb and pp 5.02 TeV Preliminary PWG : PWG-JE (Jets) Energy: 5.02 TeV System p-p
Standalone pp K/pi in jets - 3 curves Fig. Group : pi, K, p in jets in 0-10% Pb-Pb and pp 5.02 TeV Preliminary PWG : PWG-JE (Jets) Energy: 5.02 TeV System p-p
Standalone pp p/pi in jets - all curves Fig. Group : pi, K, p in jets in 0-10% Pb-Pb and pp 5.02 TeV Preliminary PWG : PWG-JE (Jets) Energy: 5.02 TeV System p-p
Standalone pp K/pi in jets - all curves Fig. Group : pi, K, p in jets in 0-10% Pb-Pb and pp 5.02 TeV Preliminary PWG : PWG-JE (Jets) Energy: 5.02 TeV System p-p
Standalone pp pi in jets spectra - inclusive, jet+UE, and UE curves Fig. Group : pi, K, p in jets in 0-10% Pb-Pb and pp 5.02 TeV Preliminary PWG : PWG-JE (Jets) Energy: 5.02 TeV System p-p
Standalone pp pi in jets spectra - inclusive and jet+UE Fig. Group : pi, K, p in jets in 0-10% Pb-Pb and pp 5.02 TeV Preliminary PWG : PWG-JE (Jets) Energy: 5.02 TeV System p-p
Standalone pp pi in jets spectra - inclusive only Fig. Group : pi, K, p in jets in 0-10% Pb-Pb and pp 5.02 TeV Preliminary PWG : PWG-JE (Jets) Energy: 5.02 TeV System p-p
Standalone pp p in jets spectra Fig. Group : pi, K, p in jets in 0-10% Pb-Pb and pp 5.02 TeV Preliminary PWG : PWG-JE (Jets) Energy: 5.02 TeV System p-p
Standalone pp K in jets spectra Fig. Group : pi, K, p in jets in 0-10% Pb-Pb and pp 5.02 TeV Preliminary PWG : PWG-JE (Jets) Energy: 5.02 TeV System p-p , System Pb-Pb
Standalone pp pi in jets spectra - all curves Fig. Group : pi, K, p in jets in 0-10% Pb-Pb and pp 5.02 TeV Preliminary PWG : PWG-JE (Jets) Energy: 5.02 TeV System p-p
Charged jet EEC in PbPb and pp (compared with models) in 40-60 GeV Fig. Group : Charged jet EEC measurements in PbPb at 5.02 TeV PWG : PWG-JE (Jets) Energy: 5.02 TeV System Pb-Pb
Charged jet EEC in PbPb and pp (compared with models) in 60-80 GeV Fig. Group : Charged jet EEC measurements in PbPb at 5.02 TeV PWG : PWG-JE (Jets) Energy: 5.02 TeV System Pb-Pb
Charged jet EEC in PbPb and pp (compared with models) in 80-100 GeV Fig. Group : Charged jet EEC measurements in PbPb at 5.02 TeV PWG : PWG-JE (Jets) Energy: 5.02 TeV System Pb-Pb
Charged jet EEC in PbPb and pp (compared with Hybrid) in 40-60 GeV Fig. Group : Charged jet EEC measurements in PbPb at 5.02 TeV PWG : PWG-JE (Jets) Energy: 5.02 TeV System Pb-Pb
Charged jet EEC in PbPb Fig. Group : Charged jet EEC measurements in PbPb at 5.02 TeV PWG : PWG-JE (Jets) Energy: 5.02 TeV System Pb-Pb
Charged jet EEC in PbPb (pT scaled) Fig. Group : Charged jet EEC measurements in PbPb at 5.02 TeV PWG : PWG-JE (Jets) Energy: 5.02 TeV System Pb-Pb
Charged jet EEC in PbPb and pp (compared with models) in 100-120 GeV Fig. Group : Charged jet EEC measurements in PbPb at 5.02 TeV PWG : PWG-JE (Jets) Energy: 5.02 TeV System Pb-Pb
Charged jet EEC in PbPb and pp (including Pythia and Herwig) in 80-100 GeV Fig. Group : Charged jet EEC measurements in PbPb at 5.02 TeV PWG : PWG-JE (Jets) Energy: 5.02 TeV System Pb-Pb
Charged jet EEC in PbPb and pp (including Pythia and Herwig) in 100-120 GeV Fig. Group : Charged jet EEC measurements in PbPb at 5.02 TeV PWG : PWG-JE (Jets) Energy: 5.02 TeV System Pb-Pb
Charged jet EEC in PbPb and pp in 60-80 GeV Fig. Group : Charged jet EEC measurements in PbPb at 5.02 TeV PWG : PWG-JE (Jets) Energy: 5.02 TeV System Pb-Pb
Charged jet EEC in PbPb and pp (including Pythia and Herwig) in 40-60 GeV Fig. Group : Charged jet EEC measurements in PbPb at 5.02 TeV PWG : PWG-JE (Jets) Energy: 5.02 TeV System Pb-Pb
Charged jet EEC in PbPb and pp (including Pythia and Herwig) in 60-80 GeV Fig. Group : Charged jet EEC measurements in PbPb at 5.02 TeV PWG : PWG-JE (Jets) Energy: 5.02 TeV System Pb-Pb
Charged jet EEC in PbPb and pp (compared with Hybrid) in 100-120 GeV Fig. Group : Charged jet EEC measurements in PbPb at 5.02 TeV PWG : PWG-JE (Jets) Energy: 5.02 TeV System Pb-Pb
Charged jet EEC in PbPb and pp (compared with Hybrid) in 80-100 GeV Fig. Group : Charged jet EEC measurements in PbPb at 5.02 TeV PWG : PWG-JE (Jets) Energy: 5.02 TeV System Pb-Pb
Charged jet EEC in PbPb and pp (compared with Hybrid) in 60-80 GeV Fig. Group : Charged jet EEC measurements in PbPb at 5.02 TeV PWG : PWG-JE (Jets) Energy: 5.02 TeV System Pb-Pb
Charged jet EEC in PbPb and pp in 100-120 GeV Fig. Group : Charged jet EEC measurements in PbPb at 5.02 TeV PWG : PWG-JE (Jets) Energy: 5.02 TeV System Pb-Pb
Charged jet EEC in PbPb and pp in 80-100 GeV Fig. Group : Charged jet EEC measurements in PbPb at 5.02 TeV PWG : PWG-JE (Jets) Energy: 5.02 TeV System Pb-Pb
Charged jet EEC in PbPb and pp in 40-60 GeV Fig. Group : Charged jet EEC measurements in PbPb at 5.02 TeV PWG : PWG-JE (Jets) Energy: 5.02 TeV System Pb-Pb
E3C/EEC at 5.02 TeV Fig. Group : E3C and EEC measurements in jets in pp collisions at 5.02 and 13TeV PWG : PWG-JE (Jets) Energy: 5.02 TeV System p-p
E3C (per jet normalized) at 5.02 TeV Fig. Group : E3C and EEC measurements in jets in pp collisions at 5.02 and 13TeV PWG : PWG-JE (Jets) Energy: 5.02 TeV System p-p
EEC (per jet normalized) at 5.02 TeV Fig. Group : E3C and EEC measurements in jets in pp collisions at 5.02 and 13TeV PWG : PWG-JE (Jets) Energy: 5.02 TeV System p-p
$\mathrm{D_s^+/D^+}$ production yield ratio measured in pp collisions at $\sqrt{s}=13.6$ TeV compared to ALICE measurements in $\mathrm{Pb-Pb}$ collisions and PYTHIA 8 and EPOS4HQ 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
Comparison with model calculation in pp collision in CS frame (CSM,NRQCD) Fig. Group : J/ψ polarization at midrapidity in pp collisions at 13.6 TeV (QM2025) PWG : PWG-DQ (Dileptons and Quarkonia) Energy: 13.6 TeV System p-p
Comparison with model calculation in pp collision in CS frame (ICEM,CSM,NRQCD) Fig. Group : J/ψ polarization at midrapidity in pp collisions at 13.6 TeV (QM2025) PWG : PWG-DQ (Dileptons and Quarkonia) Energy: 13.6 TeV System p-p
J/ψ v2{SP} vs pT at forward rapidity in the dimuon channel for the centrality class 10-30% and at 5.36 TeV compared to Run 2 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{2}, v2{SP} and v2{4} vs pT at forward rapidity in the dimuon channel for the centrality class 10-30% 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
Ratios of prompt $\Lambda_\text{c}$ corrected yields between different multiplicity intervals and the multiplicity integrated class, pp collisions at $\sqrt s = 13.6 \text{TeV}$ Fig. Group : Measurement of the Lc cross section (integrated and vs multiplicity) in pp collisions at 13.6 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
Like-sign and Unlike-sign $\Lambda_{c}$-p Azimuthal Correlations in $p_{\mathrm{T}}^{\Lambda_{c}} 3$-$5$ GeV/$c$ and $p_{\mathrm{T}}^{p} 1$-$2.5$ GeV/$c$ Fig. Group : $\Lambda_{c}^{+}$ -- proton azimuthal correlations in pp collisions at $\sqrt{s} = 13.6$ TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
Like-sign and Unlike-sign $\Lambda_{c}$-p Azimuthal Correlations in $p_{\mathrm{T}}^{\Lambda_{c}} 5$-$8$ GeV/$c$ and $p_{\mathrm{T}}^{p} 1$-$2.5$ GeV/$c$ Fig. Group : $\Lambda_{c}^{+}$ -- proton azimuthal correlations in pp collisions at $\sqrt{s} = 13.6$ TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
Like-sign and Unlike-sign $\Lambda_{c}$-p Azimuthal Correlations in $p_{\mathrm{T}}^{\Lambda_{c}} 5$-$8$ GeV/$c$ and $p_{\mathrm{T}}^{p} 0.4$-$1$ GeV/$c$ Fig. Group : $\Lambda_{c}^{+}$ -- proton azimuthal correlations in pp collisions at $\sqrt{s} = 13.6$ TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
Like-sign and Unlike-sign $\Lambda_{c}$-p Azimuthal Correlations in $p_{\mathrm{T}}^{\Lambda_{c}} 3$-$5$ GeV/$c$ and $p_{\mathrm{T}}^{p} 0.4$-$1$ GeV/$c$ Fig. Group : $\Lambda_{c}^{+}$ -- proton azimuthal correlations in pp collisions at $\sqrt{s} = 13.6$ TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
$\Lambda_{c}^{+}$ -- proton azimuthal correlations in pp collisions at $\sqrt{s} = 13.6$ TeV Fig. Group : $\Lambda_{c}^{+}$ -- proton azimuthal correlations in pp collisions at $\sqrt{s} = 13.6$ TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
Ratio of the integrated cross section of single D⁰ mesons over D⁰D⁰ and D⁰D⁰bar pairs Fig. Group : Associated production of D⁰D⁰ and D⁰D⁰bar pairs 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 ALICE measurements in $\mathrm{Pb-Pb}$ collisions 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
integrated cross section of D⁰D⁰ and D⁰D⁰bar pairs Fig. Group : Associated production of D⁰D⁰ and D⁰D⁰bar pairs in pp collisions at 13.6 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
Distribution of the $\|\Delta\varphi\|$ of D⁰D⁰ pairs Fig. Group : Associated production of D⁰D⁰ and D⁰D⁰bar pairs in pp collisions at 13.6 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
2D distribution of the $p_\rm{T}$ of D⁰D⁰ pairs vs. $\Delta \varphi$ Fig. Group : Associated production of D⁰D⁰ and D⁰D⁰bar pairs in pp collisions at 13.6 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
Acceptance multiplied by the efficiency vs. $p_\rm{T}$ vs. $y$ Fig. Group : Associated production of D⁰D⁰ and D⁰D⁰bar pairs in pp collisions at 13.6 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
Projection of the fit to the 2D invariant-mass distribution of D⁰D⁰bar pairs Fig. Group : Associated production of D⁰D⁰ and D⁰D⁰bar pairs in pp collisions at 13.6 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
Projection of the fit to the 2D invariant-mass distribution of D⁰D⁰ pairs Fig. Group : Associated production of D⁰D⁰ and D⁰D⁰bar pairs in pp collisions at 13.6 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
Fit to the 2D invariant-mass distribution of D⁰D⁰ pairs Fig. Group : Associated production of D⁰D⁰ and D⁰D⁰bar pairs in pp collisions at 13.6 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
Fit to the 2D invariant-mass distribution of D⁰D⁰bar pairs Fig. Group : Associated production of D⁰D⁰ and D⁰D⁰bar pairs in pp collisions at 13.6 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
J/ψ and ψ(2S) invariant mass Run 3 in dimuon channel at forward rapidity with ψ(2S) rescaled in pp Fig. Group : Charmonium production Run 3 in Pb-Pb collisions at √sNN = 5.36 TeV at forward rapidity PWG : PWG-DQ (Dileptons and Quarkonia) Energy: 5.36 TeV System Pb-Pb
Raw quasi-inclusive jet $p_\mathrm{T,jet}^\mathrm{reco}$ distribution for $R = 0.5$ of the SE and ME with $p_\mathrm{T}^\mathrm{lead} > 5$ 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 quasi-inclusive jet $p_\mathrm{T,jet}^\mathrm{reco}$ distribution for $R = 0.5$ with $p_\mathrm{T}^\mathrm{lead} > 5$ 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
Corrected charged particle jet distributions for $R = 0.5$ with $p_\mathrm{T}^\mathrm{lead} > 4$ GeV/c and $p_\mathrm{T}^\mathrm{lead} > 5$ 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
Charged particle jet $R_{AA}$ for R = 0.5 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
Comparison with publiced results in PbPb collision in Production frame Fig. Group : J/ψ polarization at midrapidity in pp collisions at 13.6 TeV (QM2025) PWG : PWG-DQ (Dileptons and Quarkonia) Energy: 13.6 TeV System p-p
Comparison with publiced results in pp collision in Production frame Fig. Group : J/ψ polarization at midrapidity in pp collisions at 13.6 TeV (QM2025) PWG : PWG-DQ (Dileptons and Quarkonia) Energy: 13.6 TeV System p-p
J/ψ and ψ(2S) invariant mass Run 3 in dimuon channel at forward rapidity vs pT Fig. Group : Charmonium production Run 3 in Pb-Pb collisions at √sNN = 5.36 TeV at forward rapidity PWG : PWG-DQ (Dileptons and Quarkonia) Energy: 5.36 TeV System Pb-Pb
J/ψ and ψ(2S) invariant mass Run 3 in dimuon channel at forward rapidity in 6 < pT < 12 GeV/c bin Fig. Group : Charmonium production Run 3 in Pb-Pb collisions at √sNN = 5.36 TeV at forward rapidity PWG : PWG-DQ (Dileptons and Quarkonia) Energy: 5.36 TeV System Pb-Pb
J/ψ and ψ(2S) invariant mass Run 3 in dimuon channel at forward rapidity in 4 < pT < 6 GeV/c bin Fig. Group : Charmonium production Run 3 in Pb-Pb collisions at √sNN = 5.36 TeV at forward rapidity PWG : PWG-DQ (Dileptons and Quarkonia) Energy: 5.36 TeV System Pb-Pb
J/ψ and ψ(2S) invariant mass Run 3 in dimuon channel at forward rapidity in 2 < pT < 4 GeV/c bin Fig. Group : Charmonium production Run 3 in Pb-Pb collisions at √sNN = 5.36 TeV at forward rapidity PWG : PWG-DQ (Dileptons and Quarkonia) Energy: 5.36 TeV System Pb-Pb
J/ψ and ψ(2S) invariant mass Run 3 in dimuon channel at forward rapidity in 0 < pT < 2 GeV/c bin Fig. Group : Charmonium production Run 3 in Pb-Pb collisions at √sNN = 5.36 TeV at forward rapidity PWG : PWG-DQ (Dileptons and Quarkonia) Energy: 5.36 TeV System Pb-Pb
J/ψ and ψ(2S) invariant mass Run 3 in dimuon channel at forward rapidity in 60-90% centrality bin Fig. Group : Charmonium production Run 3 in Pb-Pb collisions at √sNN = 5.36 TeV at forward rapidity PWG : PWG-DQ (Dileptons and Quarkonia) Energy: 5.36 TeV System Pb-Pb
J/ψ and ψ(2S) invariant mass Run 3 in dimuon channel at forward rapidity in 40-60% centrality bin Fig. Group : Charmonium production Run 3 in Pb-Pb collisions at √sNN = 5.36 TeV at forward rapidity PWG : PWG-DQ (Dileptons and Quarkonia) Energy: 5.36 TeV System Pb-Pb
J/ψ and ψ(2S) invariant mass Run 3 in dimuon channel at forward rapidity in 20-40% centrality bin Fig. Group : Charmonium production Run 3 in Pb-Pb collisions at √sNN = 5.36 TeV at forward rapidity PWG : PWG-DQ (Dileptons and Quarkonia) Energy: 5.36 TeV System Pb-Pb
J/ψ and ψ(2S) invariant mass Run 3 in dimuon channel at forward rapidity in 0-20% centrality bin Fig. Group : Charmonium production Run 3 in Pb-Pb collisions at √sNN = 5.36 TeV at forward rapidity PWG : PWG-DQ (Dileptons and Quarkonia) Energy: 5.36 TeV System Pb-Pb
J/ψ and ψ(2S) invariant mass Run 3 in dimuon channel at forward rapidity vs centrality Fig. Group : Charmonium production Run 3 in Pb-Pb collisions at √sNN = 5.36 TeV at forward rapidity PWG : PWG-DQ (Dileptons and Quarkonia) Energy: 5.36 TeV System Pb-Pb
ψ(2S)-to-J/ψ ratio vs Npart in Run 3 Pb-Pb collisions in the dimuon channel at forward rapidity Fig. Group : Charmonium production Run 3 in Pb-Pb collisions at √sNN = 5.36 TeV at forward rapidity PWG : PWG-DQ (Dileptons and Quarkonia) Energy: 5.36 TeV System Pb-Pb
ψ(2S)-to-J/ψ ratio vs pT in Run 3 Pb-Pb collisions in the dimuon channel at forward rapidity Fig. Group : Charmonium production Run 3 in Pb-Pb collisions at √sNN = 5.36 TeV at forward rapidity PWG : PWG-DQ (Dileptons and Quarkonia) Energy: 5.36 TeV System Pb-Pb
ψ(2S)-to-J/ψ ratio vs centrality in Run 3 Pb-Pb collisions in the dimuon channel at forward rapidity Fig. Group : Charmonium production Run 3 in Pb-Pb collisions at √sNN = 5.36 TeV at forward rapidity PWG : PWG-DQ (Dileptons and Quarkonia) Energy: 5.36 TeV System Pb-Pb
Comparison with model calculation in pp collision in CS frame Fig. Group : J/ψ polarization at midrapidity in pp collisions at 13.6 TeV (QM2025) PWG : PWG-DQ (Dileptons and Quarkonia) Energy: 13.6 TeV System p-p
Inclusive Jpsi signal extraction by using 22+23+24 pp data (except for 24ao) Fig. Group : J/ψ polarization at midrapidity in pp collisions at 13.6 TeV (QM2025) PWG : PWG-DQ (Dileptons and Quarkonia) Energy: 13.6 TeV System p-p
Distribution of rho background in signal and reference events Fig. Group : Measurement of the semi-inclusive hadron+jet distributions in pp collisions at √s = 13.6 TeV using Run 3 data PWG : PWG-JE (Jets) Energy: 5.36 TeV System Pb-Pb
Raw spectra of signal, reference and delta recoil vs pT for R=0.4 jets in Pb-Pb collisions Fig. Group : Measurement of the semi-inclusive hadron+jet distributions in pp collisions at √s = 13.6 TeV using Run 3 data PWG : PWG-JE (Jets) Energy: 5.36 TeV System Pb-Pb

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