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Scope: PWG

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J/$\psi$ ROO vs pT (Model Comparison) in OO collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.36 TeV in the dimuon channel at forward rapidity [SQM26] Fig. Group : J/$\psi$ Nuclear Modification factor in OO collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.36 TeV in the dimuon channel at forward rapidity [SQM26] PWG : PWG-DQ (Dileptons and Quarkonia) Energy: 5.02 TeV , Energy: 5.36 TeV , Energy: 9.61 TeV System O-O , System p-O , System Pb-Pb
J/$\psi$ ROO vs pT (Model Comparison) in OO collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.36 TeV in the dimuon channel at forward rapidity [SQM26] Fig. Group : J/$\psi$ Nuclear Modification factor in OO collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.36 TeV in the dimuon channel at forward rapidity [SQM26] PWG : PWG-DQ (Dileptons and Quarkonia) Energy: 5.36 TeV , Energy: 9.61 TeV System O-O , System p-O
J/$\psi$ ROO vs pT (Model Comparison) in OO collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.36 TeV in the dimuon channel at forward rapidity [SQM26] Fig. Group : J/$\psi$ Nuclear Modification factor in OO collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.36 TeV in the dimuon channel at forward rapidity [SQM26] PWG : PWG-DQ (Dileptons and Quarkonia) Energy: 5.02 TeV , Energy: 5.36 TeV , Energy: 8 TeV , Energy: 9.61 TeV System O-O , System p-O , System Pb-Pb
J/$\psi$ ROO vs pT (Model Comparison) in OO collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.36 TeV in the dimuon channel at forward rapidity [SQM26] Fig. Group : J/$\psi$ Nuclear Modification factor in OO collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.36 TeV in the dimuon channel at forward rapidity [SQM26] PWG : PWG-DQ (Dileptons and Quarkonia) Energy: 5.36 TeV System O-O
J/$\psi$ ROO vs pT in OO collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.36 TeV in the dimuon channel at forward rapidity [SQM26] Fig. Group : J/$\psi$ Nuclear Modification factor in OO collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.36 TeV in the dimuon channel at forward rapidity [SQM26] PWG : PWG-DQ (Dileptons and Quarkonia) Energy: 5.36 TeV System O-O
Non-prompt $\psi$(2S) fraction compare with EPOS4 Fig. Group : Non-prompt $\psi$(2S) fraction in pp collisions at 13.6 TeV [SQM2026] PWG : PWG-DQ (Dileptons and Quarkonia) Energy: 13.6 TeV System p-p
$\mathrm{\Lambda_{c}^{+}}/\mathrm{D}^0$ ratio in pp collisions at $\sqrt{s} = 13.6\ \mathrm{TeV}$ Fig. Group : Measurement of the prompt $\mathrm{D}^0$ cross section in pp collisions at $\sqrt{s} = 13.6\ \mathrm{TeV}$ PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
Fit to the invariant-mass distribution of prompt $\mathrm{D}^{0}$ in the $3.5 < p_{\mathrm{T}} < 4 \mathrm{GeV}/c$ interval, in pp collisions at $\sqrt{s} = 13.6 \ \mathrm{TeV}$ Fig. Group : Measurement of the prompt $\mathrm{D}^0$ cross section in pp collisions at $\sqrt{s} = 13.6\ \mathrm{TeV}$ PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
Prompt $\mathrm{D}^0$ cross section in pp collisions at $\sqrt{s} = 13.6\ \mathrm{TeV}$ compared with FONLL Fig. Group : Measurement of the prompt $\mathrm{D}^0$ cross section in pp collisions at $\sqrt{s} = 13.6\ \mathrm{TeV}$ PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
Prompt $\mathrm{D}^0$ cross section in pp collisions at $\sqrt{s} = 13.6\ \mathrm{TeV}$ compared with Run 2 measurement Fig. Group : Measurement of the prompt $\mathrm{D}^0$ cross section in pp collisions at $\sqrt{s} = 13.6\ \mathrm{TeV}$ PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
fB in mid rapidities compared with PYTHIA comparisons Fig. Group : Prompt and non-prompt J/$\psi$ separation at mid-rapidity in pp collisions at $\sqrt{s} = $ 13.6 TeV PWG : PWG-DQ (Dileptons and Quarkonia) Energy: 13.6 TeV System p-p
The model comparison of differential cross section of inclusive J/psi at midrapidity in pp collisions at 5.36 TeV Fig. Group : Inclusive J/psi production in midrapidity at 5.36TeV in pp collisions PWG : PWG-DQ (Dileptons and Quarkonia) Energy: 5.36 TeV System p-p
Differential cross section of inclusive J/psi at midrapidity in pp collisions at 5.36 TeV Fig. Group : Inclusive J/psi production in midrapidity at 5.36TeV in pp collisions PWG : PWG-DQ (Dileptons and Quarkonia) Energy: 5.36 TeV System p-p
Prompt $D^0$ elliptic flow comparison from semicentral Pb--Pb to central OO collisions Fig. Group : Preliminary measurement of prompt D-meson elliptic flow in OO collisions PWG : PWG-HF (Heavy Flavour) Energy: 5.36 TeV System O-O , System Pb-Pb
J/ψ v2 as a function of centrality at high pT in OO collisions, compared with results in Pb-Pb collisions Fig. Group : J/ψ v2 at midrapidity in OO collisions at 5.36 TeV [SQM2026] PWG : PWG-DQ (Dileptons and Quarkonia) Energy: 5.36 TeV System O-O
J/ψ v2 as a function of centrality at low pT in OO collisions, compared with results in Pb-Pb collisions Fig. Group : J/ψ v2 at midrapidity in OO collisions at 5.36 TeV [SQM2026] PWG : PWG-DQ (Dileptons and Quarkonia) Energy: 5.36 TeV System O-O
J/ψ v2 as a function of pT in semi-central OO collisions, compared with results in p-Pb and Pb-Pb collisions Fig. Group : J/ψ v2 at midrapidity in OO collisions at 5.36 TeV [SQM2026] PWG : PWG-DQ (Dileptons and Quarkonia) Energy: 5.36 TeV System O-O
J/ψ v2 as a function of pT in central OO collisions, compared with results in p-Pb and Pb-Pb collisions Fig. Group : J/ψ v2 at midrapidity in OO collisions at 5.36 TeV [SQM2026] PWG : PWG-DQ (Dileptons and Quarkonia) Energy: 5.36 TeV System O-O
J/ψ v2 as a function of pT in semi-central OO collisions compared with model calculations Fig. Group : J/ψ v2 at midrapidity in OO collisions at 5.36 TeV [SQM2026] PWG : PWG-DQ (Dileptons and Quarkonia) Energy: 5.36 TeV System O-O
J/ψ v2 as a function of pT in central OO collisions compared with model calculations Fig. Group : J/ψ v2 at midrapidity in OO collisions at 5.36 TeV [SQM2026] PWG : PWG-DQ (Dileptons and Quarkonia) Energy: 5.36 TeV System O-O
Nuclear modification factor of J/psi in pO collisions as a function of pT, compared with p-Pb data and with FCEL model Fig. Group : J/$\psi$ production at forward rapidity in pO collisions at $\sqrt{s_{NN}}$ = 9.62 TeV PWG : PWG-DQ (Dileptons and Quarkonia) Energy: 9.61 TeV System p-O
Nuclear modification factor of J/psi in pO collisions as a function of pT, compared with p-Pb data Fig. Group : J/$\psi$ production at forward rapidity in pO collisions at $\sqrt{s_{NN}}$ = 9.62 TeV PWG : PWG-DQ (Dileptons and Quarkonia) Energy: 9.61 TeV System p-O
Nuclear modification factor of J/psi in pO collisions as a function of pT, compared with FCEL model Fig. Group : J/$\psi$ production at forward rapidity in pO collisions at $\sqrt{s_{NN}}$ = 9.62 TeV PWG : PWG-DQ (Dileptons and Quarkonia) Energy: 9.61 TeV System p-O
Nuclear modification factor of J/psi in pO collisions as a function of pT Fig. Group : J/$\psi$ production at forward rapidity in pO collisions at $\sqrt{s_{NN}}$ = 9.62 TeV PWG : PWG-DQ (Dileptons and Quarkonia) Energy: 9.61 TeV System p-O
Non-prompt $\psi$(2S) fraction compare with measurements from other LHC experiments Fig. Group : Non-prompt $\psi$(2S) fraction in pp collisions at 13.6 TeV [SQM2026] PWG : PWG-DQ (Dileptons and Quarkonia) Energy: 13.6 TeV System p-p
Non-prompt $\psi$(2S) fraction compare with non-prompt J/$\psi$ fraction Fig. Group : Non-prompt $\psi$(2S) fraction in pp collisions at 13.6 TeV [SQM2026] PWG : PWG-DQ (Dileptons and Quarkonia) Energy: 13.6 TeV System p-p
Non-prompt $\psi$(2S) fraction in pp at 13.6 TeV Fig. Group : Non-prompt $\psi$(2S) fraction in pp collisions at 13.6 TeV [SQM2026] PWG : PWG-DQ (Dileptons and Quarkonia) Energy: 13.6 TeV System p-p
Prompt $D^0$ elliptic flow comparison with light flavour hadrons Fig. Group : Preliminary measurement of prompt D-meson elliptic flow in OO collisions PWG : PWG-HF (Heavy Flavour) Energy: 5.36 TeV System O-O
Charm meson elliptic flow in central OO collisions Fig. Group : Preliminary measurement of prompt D-meson elliptic flow in OO collisions PWG : PWG-HF (Heavy Flavour) Energy: 5.36 TeV System O-O
$D^0$ meson simultaneous fit Fig. Group : Preliminary measurement of prompt D-meson elliptic flow in OO collisions PWG : PWG-HF (Heavy Flavour) Energy: 5.36 TeV System O-O
$D^+$ meson simultaneous fit Fig. Group : Preliminary measurement of prompt D-meson elliptic flow in OO collisions PWG : PWG-HF (Heavy Flavour) Energy: 5.36 TeV System O-O
$D_s^+$ meson simultaneous fit Fig. Group : Preliminary measurement of prompt D-meson elliptic flow in OO collisions PWG : PWG-HF (Heavy Flavour) Energy: 5.36 TeV System O-O
Fit to the raw-yield distribution of $D^{+}$ mesons for different BDT non-prompt scores performed to extract the $D^{+}$ $f_{\mathrm{non-prompt}}$ fraction in the 1<pT<2 GeV/c in pp collisions at 13.6 TeV Fig. Group : D+-p femto in pp collisions at 13.6 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
Comparison of p$D^{-}$ momentum correlation function with model predictions in proton–proton collisions at 13.6 TeV Fig. Group : D+-p femto in pp collisions at 13.6 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
Comparison of p$D^{+}$ momentum correlation function with model predictions in proton–proton collisions at 13.6 TeV Fig. Group : D+-p femto in pp collisions at 13.6 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
Raw correlation function of p$D^{\pm}$ and simulation of non-femtosocpy background of p$D^{\pm}$ in proton–proton collisions at 13.6 TeV Fig. Group : D+-p femto in pp collisions at 13.6 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
*Fit to the invariant-mass distribution of $D^{+}$ mesons in mixed events in the 0.06 < $k^{}$ <0.10 GeV/c in proton–proton collisions at 13.6 TeV Fig. Group : D+-p femto in pp collisions at 13.6 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System** p-p
*Fit to the invariant-mass distribution of $D^{+}$ mesons in same events in the 0.06 < $k^{}$ <0.10 GeV/c in proton–proton collisions at 13.6 TeV Fig. Group : D+-p femto in pp collisions at 13.6 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System** p-p
Highest and lowest multiplicity nonprompt \jpsi~fB at mid-rapidity in pp collisions at $\sqrt{s} = $ 13.6 TeV [SQM2026] Fig. Group : Multiplicity dependence of prompt and non-prompt \jpsi~at mid-rapidity in pp collisions at $\sqrt{s} = $ 13.6 TeV [SQM2026] PWG : PWG-DQ (Dileptons and Quarkonia) Energy: 13.6 TeV System p-p
Multiplicity dependence fB of \jpsi~at mid-rapidity in pp collisions at $\sqrt{s} = $ 13.6 TeV [SQM2026] Fig. Group : Multiplicity dependence of prompt and non-prompt \jpsi~at mid-rapidity in pp collisions at $\sqrt{s} = $ 13.6 TeV [SQM2026] PWG : PWG-DQ (Dileptons and Quarkonia) Energy: 13.6 TeV System p-p
$\Xi_c^+/\Lambda_c^+$ ratio compared with $\Xi_c^0/\Lambda_c^+$ by ALICE and $\Xi_c^+/\Lambda_c^+$ by LHCb Fig. Group : $\Xi_c^+/\Lambda_c^+$ ratio in pp collisions at $\sqrt{s} = 13.6$ TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
$\Xi_c^+/\Lambda_c^+$ ratio compared with LHCb results Fig. Group : $\Xi_c^+/\Lambda_c^+$ ratio in pp collisions at $\sqrt{s} = 13.6$ TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
BDT score for Omegac to Omega pi analysis in 4 < pT< 6 GeV/c in pp collisions at 13.6 TeV Fig. Group : OmegaC production vs multiplicity in pp collisions at 13.6 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
ROC curve for Omegac to Omega pi analysis in 4 < pT< 6 GeV/c in pp collisions at 13.6 TeV Fig. Group : OmegaC production vs multiplicity in pp collisions at 13.6 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
B meson production cross section, comparison to kT factorization Fig. Group : Measurement of charged B meson production in pp collisions in Run 3 PWG : PWG-DQ (Dileptons and Quarkonia) Energy: 13.6 TeV System p-p
B meson production cross section, comparison phenomenological models, ratio Fig. Group : Measurement of charged B meson production in pp collisions in Run 3 PWG : PWG-DQ (Dileptons and Quarkonia) Energy: 13.6 TeV System p-p
B meson production cross section, comparison phenomenological models Fig. Group : Measurement of charged B meson production in pp collisions in Run 3 PWG : PWG-DQ (Dileptons and Quarkonia) Energy: 13.6 TeV System p-p
B meson production cross section, comparison FONLL, NNLO+NNL, ratio Fig. Group : Measurement of charged B meson production in pp collisions in Run 3 PWG : PWG-DQ (Dileptons and Quarkonia) Energy: 13.6 TeV System p-p
B meson production cross section, comparison FONLL, NNLO+NNL Fig. Group : Measurement of charged B meson production in pp collisions in Run 3 PWG : PWG-DQ (Dileptons and Quarkonia) Energy: 13.6 TeV System p-p
OmegaC self normalized yields in pp collisions at 13.6 TeV Fig. Group : OmegaC production vs multiplicity in pp collisions at 13.6 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
OmegaC raw yield in 4_pT_6 and 10-50% FT0M Fig. Group : OmegaC production vs multiplicity in pp collisions at 13.6 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
OmegaC raw yield in 4_pT_6 and 0-10% FT0M Fig. Group : OmegaC production vs multiplicity in pp collisions at 13.6 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
$\Xi_c^+/\Lambda_c^+$ ratio compared with Run 2 results including $\Xi_c^+\rightarrow \Xi^- \pi^+ \pi^+$ and model predictions Fig. Group : $\Xi_c^+/\Lambda_c^+$ ratio in pp collisions at $\sqrt{s} = 13.6$ TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
$\Xi_c^+/\Lambda_c^+$ ratio compared with Run 2 results and model predictions Fig. Group : $\Xi_c^+/\Lambda_c^+$ ratio in pp collisions at $\sqrt{s} = 13.6$ TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
$\Xi_c^+/\Lambda_c^+$ ratio compared with Run 2 results Fig. Group : $\Xi_c^+/\Lambda_c^+$ ratio in pp collisions at $\sqrt{s} = 13.6$ TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
B meson production cross section, comparison to pQCD-based models, ratios Fig. Group : Measurement of charged B meson production in pp collisions in Run 3 PWG : PWG-DQ (Dileptons and Quarkonia) Energy: 13.6 TeV System p-p
B meson production cross section, comparison to pQCD-based models Fig. Group : Measurement of charged B meson production in pp collisions in Run 3 PWG : PWG-DQ (Dileptons and Quarkonia) Energy: 13.6 TeV System p-p
B meson production cross section, comparison to data Fig. Group : Measurement of charged B meson production in pp collisions in Run 3 PWG : PWG-DQ (Dileptons and Quarkonia) Energy: 13.6 TeV System p-p , System p-Pb
Ratio of $\pt$-integrated $\mathrm{D_s^+/D^+}$ production yield ratio measured in pp collisions at $\sqrt{s}=13.6$ TeV and $\mathrm{Pb-Pb}$ collisions at $\sqrt{s_\mathrm{NN}}=5.36$ TeV to low-multiplicity pp collisions, compared to $\mathrm{K}^+/\pi^+$ Fig. Group : $\mathrm{D_s^+/D^+}$ production yield ratio in Pb$-$Pb collisions at $\sqrt{s_\mathrm{NN}}=5.36$ TeV PWG : PWG-HF (Heavy Flavour) Energy: 5.36 TeV , Energy: 13.6 TeV System p-p , System Pb-Pb
$\pt$-integrated $\mathrm{D_s^+/D^+}$ production yield ratio measured in pp collisions at $\sqrt{s}=13.6$ TeV and $\mathrm{Pb-Pb}$ collisions at $\sqrt{s_\mathrm{NN}}=5.36$ TeV, compared to theoretical predictions Fig. Group : $\mathrm{D_s^+/D^+}$ production yield ratio in Pb$-$Pb collisions at $\sqrt{s_\mathrm{NN}}=5.36$ TeV PWG : PWG-HF (Heavy Flavour) Energy: 5.36 TeV , Energy: 13.6 TeV System p-p , System Pb-Pb
$\mathrm{D_s^+/D^+}$ production yield ratio measured in pp collisions at $\sqrt{s}=13.6$ TeV and $\mathrm{Pb-Pb}$ collisions at $\sqrt{s_\mathrm{NN}}=5.36$ TeV as a function of $\pt$ Fig. Group : $\mathrm{D_s^+/D^+}$ production yield ratio in Pb$-$Pb collisions at $\sqrt{s_\mathrm{NN}}=5.36$ TeV PWG : PWG-HF (Heavy Flavour) Energy: 5.36 TeV , Energy: 13.6 TeV System p-p , System Pb-Pb
$\mathrm{D_s^+/D^+}$ production yield ratio measured in pp collisions at $\sqrt{s}=13.6$ TeV and $\mathrm{Pb-Pb}$ collisions at $\sqrt{s_\mathrm{NN}}=5.36$ TeV compared to PYTHIA 8 and EPOS4HQ predictions (EPOS4HQ highlight) Fig. Group : $\mathrm{D_s^+/D^+}$ production yield ratio in Pb$-$Pb collisions at $\sqrt{s_\mathrm{NN}}=5.36$ TeV PWG : PWG-HF (Heavy Flavour) Energy: 5.36 TeV , Energy: 13.6 TeV System p-p , System Pb-Pb
$\mathrm{D_s^+/D^+}$ production yield ratio measured in pp collisions at $\sqrt{s}=13.6$ TeV and $\mathrm{Pb-Pb}$ collisions at $\sqrt{s_\mathrm{NN}}=5.36$ TeV compared to PYTHIA 8 and EPOS4HQ predictions (PYTHIA highlight) Fig. Group : $\mathrm{D_s^+/D^+}$ production yield ratio in Pb$-$Pb collisions at $\sqrt{s_\mathrm{NN}}=5.36$ TeV PWG : PWG-HF (Heavy Flavour) Energy: 5.36 TeV , Energy: 13.6 TeV System p-p , System Pb-Pb
$\mathrm{D_s^+/D^+}$ production yield ratio measured in pp collisions at $\sqrt{s}=13.6$ TeV and $\mathrm{Pb-Pb}$ collisions at $\sqrt{s_\mathrm{NN}}=5.36$ TeV compared to PYTHIA 8 and EPOS4HQ predictions Fig. Group : $\mathrm{D_s^+/D^+}$ production yield ratio in Pb$-$Pb collisions at $\sqrt{s_\mathrm{NN}}=5.36$ TeV PWG : PWG-HF (Heavy Flavour) Energy: 5.36 TeV , Energy: 13.6 TeV System p-p , System Pb-Pb
$\mathrm{D_s^+/D^+}$ production yield ratio measured in pp collisions at $\sqrt{s}=13.6$ TeV and $\mathrm{Pb-Pb}$ collisions compared at $\sqrt{s_\mathrm{NN}}=5.36$ TeV compared to LHCb measurement in p$-$Pb collisions Fig. Group : $\mathrm{D_s^+/D^+}$ production yield ratio in Pb$-$Pb collisions at $\sqrt{s_\mathrm{NN}}=5.36$ TeV PWG : PWG-HF (Heavy Flavour) Energy: 5.36 TeV , Energy: 13.6 TeV System p-p , System Pb-Pb
$\mathrm{D_s^+/D^+}$ production yield ratio measured in pp collisions at $\sqrt{s}=13.6$ TeV and $\mathrm{Pb-Pb}$ collisions at $\sqrt{s_\mathrm{NN}}=5.36$ TeV Fig. Group : $\mathrm{D_s^+/D^+}$ production yield ratio in Pb$-$Pb collisions at $\sqrt{s_\mathrm{NN}}=5.36$ TeV PWG : PWG-HF (Heavy Flavour) Energy: 5.36 TeV , Energy: 13.6 TeV System p-p , System Pb-Pb
Fit to the raw-yield distribution of $\mathrm{D^+}$ mesons for different BDT non-prompt scores performed to extract the $\mathrm{D^+}$ $f_\mathrm{prompt}$ fraction in the $2< \pt <4$ GeV/$c$ and $50-60\%$ FT0C interval Fig. Group : $\mathrm{D_s^+/D^+}$ production yield ratio in Pb$-$Pb collisions at $\sqrt{s_\mathrm{NN}}=5.36$ TeV PWG : PWG-HF (Heavy Flavour) Energy: 5.36 TeV System Pb-Pb
Fit to the raw-yield distribution of $\mathrm{D_s^+}$ mesons for different BDT non-prompt scores performed to extract the $\mathrm{D_s^+}$ $f_\mathrm{prompt}$ fraction in the $2< \pt <4$ GeV/$c$ and $50-60\%$ FT0C interval Fig. Group : $\mathrm{D_s^+/D^+}$ production yield ratio in Pb$-$Pb collisions at $\sqrt{s_\mathrm{NN}}=5.36$ TeV PWG : PWG-HF (Heavy Flavour) Energy: 5.36 TeV System Pb-Pb
Fit to the invariant-mass distribution of $\mathrm{D_s^+}$ and $\mathrm{D^+}$ mesons in the $2< \pt <4$ GeV/$c$ interval and the $80-90\%$ FT0C percentile in Pb$-$Pb collisions at $\sqrt{s_\mathrm{NN}}=5.36$ TeV Fig. Group : $\mathrm{D_s^+/D^+}$ production yield ratio in Pb$-$Pb collisions at $\sqrt{s_\mathrm{NN}}=5.36$ TeV PWG : PWG-HF (Heavy Flavour) Energy: 5.36 TeV System Pb-Pb
Fit to the invariant-mass distribution of $\mathrm{D_s^+}$ and $\mathrm{D^+}$ mesons in the $2< \pt <4$ GeV/$c$ interval and the $0-10\%$ FT0C percentile in Pb$-$Pb collisions at $\sqrt{s_\mathrm{NN}}=5.36$ TeV Fig. Group : $\mathrm{D_s^+/D^+}$ production yield ratio in Pb$-$Pb collisions at $\sqrt{s_\mathrm{NN}}=5.36$ TeV PWG : PWG-HF (Heavy Flavour) Energy: 5.36 TeV System Pb-Pb
$\Xi_{\mathrm{c}}^{0}/\Lambda_{\mathrm{c}}^{+}$ compared to model predictions in 0–10% and 30–50% centrality intervals. Fig. Group : $\Xi_{\mathrm{c}}^{0}\rightarrow \pi^{+}\Xi^{-}$ production in Pb–Pb collisions at $\sqrt{s_{\rm {NN}}}=5.02~TeV$ PWG : PWG-HF (Heavy Flavour) Energy: 5.02 TeV System Pb-Pb
$\Xi_{\mathrm{c}}^{0}/D_{\mathrm{s}}^{+}$ compared to model predictions in 0–10% and 30–50% centrality intervals. Fig. Group : $\Xi_{\mathrm{c}}^{0}\rightarrow \pi^{+}\Xi^{-}$ production in Pb–Pb collisions at $\sqrt{s_{\rm {NN}}}=5.02~TeV$ PWG : PWG-HF (Heavy Flavour) Energy: 5.02 TeV System Pb-Pb
$\Xi_{\mathrm{c}}^{0}/D^{0}$ compared to model predictions in 0–10% and 30–50% centrality intervals. Fig. Group : $\Xi_{\mathrm{c}}^{0}\rightarrow \pi^{+}\Xi^{-}$ production in Pb–Pb collisions at $\sqrt{s_{\rm {NN}}}=5.02~TeV$ PWG : PWG-HF (Heavy Flavour) Energy: 5.02 TeV System Pb-Pb
$\mathrm{\Xi_c^0}$ $R_{\mathrm{AA}}$ compared to EPOS4HQ and POWLANG model predictions in 0–10% and 30–50% centrality intervals. Fig. Group : $\Xi_{\mathrm{c}}^{0}\rightarrow \pi^{+}\Xi^{-}$ production in Pb–Pb collisions at $\sqrt{s_{\rm {NN}}}=5.02~TeV$ PWG : PWG-HF (Heavy Flavour) Energy: 5.02 TeV System Pb-Pb
$\mathrm{\Xi_c^0}$ $R_{\mathrm{AA}}$ compared to QCM and TAMU model predictions in 0–10% and 30–50% centrality intervals. Fig. Group : $\Xi_{\mathrm{c}}^{0}\rightarrow \pi^{+}\Xi^{-}$ production in Pb–Pb collisions at $\sqrt{s_{\rm {NN}}}=5.02~TeV$ PWG : PWG-HF (Heavy Flavour) Energy: 5.02 TeV System Pb-Pb
$\mathrm{\Xi_c^0}$ corrected $p_{\mathrm{T}}$ spectrum w.r.t. model predictions in 0-10% and 30-50%. Fig. Group : $\Xi_{\mathrm{c}}^{0}\rightarrow \pi^{+}\Xi^{-}$ production in Pb–Pb collisions at $\sqrt{s_{\rm {NN}}}=5.02~TeV$ PWG : PWG-HF (Heavy Flavour) Energy: 5.02 TeV System Pb-Pb
Longitudinal polarization Pz,s2 of Lambda + AntiLambda vs charged-particle multiplicity in OO and Pb-Pb collisions at 5.36 TeV Fig. Group : Lambda longitudinal polarization in Run 3 OO collisions at 5.36 TeV PWG : PWG-LF (Light Flavour Spectra) Energy: 5.36 TeV System O-O , System Pb-Pb
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

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