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ID number ALI-PREL-XXX

Figure Caption

Scope: PWG

System

Energy

$D^{+}_{s}$-hadron azimuthal correlations in pp collisions at $\sqrt{s}$=13.6 TeV

Baseline of Ds-h measurement in the different $p_{T}^{assoc}$ intervals considered

Fig. Group : $D^{+}_{s}$-hadron azimuthal correlations in pp collisions at $\sqrt{s}$=13.6 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13.6 TeV
System: p-p

Near-side width of Ds-h measurement in the different $p_{T}^{assoc}$ intervals considered

Fig. Group : $D^{+}_{s}$-hadron azimuthal correlations in pp collisions at $\sqrt{s}$=13.6 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13.6 TeV
System: p-p

Away-side width of Ds-h measurement in the different $p_{T}^{assoc}$ intervals considered

Fig. Group : $D^{+}_{s}$-hadron azimuthal correlations in pp collisions at $\sqrt{s}$=13.6 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13.6 TeV
System: p-p

Away-side yield of Ds-h measurement in the different $p_{T}^{assoc}$ intervals considered

Fig. Group : $D^{+}_{s}$-hadron azimuthal correlations in pp collisions at $\sqrt{s}$=13.6 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13.6 TeV
System: p-p

Near-side yield of Ds-h measurement in the different $p_{T}^{assoc}$ intervals considered

Fig. Group : $D^{+}_{s}$-hadron azimuthal correlations in pp collisions at $\sqrt{s}$=13.6 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13.6 TeV
System: p-p

Baseline comparison between Ds-h and D+-h ($p_{T}^{assoc}$ > 0.3 GeV/c)

Fig. Group : $D^{+}_{s}$-hadron azimuthal correlations in pp collisions at $\sqrt{s}$=13.6 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13.6 TeV
System: p-p

Near-side yield comparison between Ds-h and D+-h ($p_{T}^{assoc}$ > 0.3 GeV/c)

Fig. Group : $D^{+}_{s}$-hadron azimuthal correlations in pp collisions at $\sqrt{s}$=13.6 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13.6 TeV
System: p-p

Away-side yield comparison between Ds-h and D+-h ($p_{T}^{assoc}$ > 0.3 GeV/c)

Fig. Group : $D^{+}_{s}$-hadron azimuthal correlations in pp collisions at $\sqrt{s}$=13.6 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13.6 TeV
System: p-p

Away-side widths comparison between Ds-h and D+-h ($p_{T}^{assoc}$ > 0.3 GeV/c)

Fig. Group : $D^{+}_{s}$-hadron azimuthal correlations in pp collisions at $\sqrt{s}$=13.6 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13.6 TeV
System: p-p

Near-side widths comparison between Ds-h and D+-h ($p_{T}^{assoc}$ > 0.3 GeV/c)

Fig. Group : $D^{+}_{s}$-hadron azimuthal correlations in pp collisions at $\sqrt{s}$=13.6 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13.6 TeV
System: p-p

Near-side yield comparison between measured Ds-h and PYTHIA8 predictions ($p_{T}^{assoc}$ > 0.3 GeV/c)

Fig. Group : $D^{+}_{s}$-hadron azimuthal correlations in pp collisions at $\sqrt{s}$=13.6 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13.6 TeV
System: p-p

Away-side yield comparison between measured Ds-h and PYTHIA8 predictions ($p_{T}^{assoc}$ > 0.3 GeV/c)

Fig. Group : $D^{+}_{s}$-hadron azimuthal correlations in pp collisions at $\sqrt{s}$=13.6 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13.6 TeV
System: p-p

Away-side width comparison between measured Ds-h and PYTHIA8 predictions ($p_{T}^{assoc}$ > 0.3 GeV/c)

Fig. Group : $D^{+}_{s}$-hadron azimuthal correlations in pp collisions at $\sqrt{s}$=13.6 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13.6 TeV
System: p-p

Near-side width comparison between measured Ds-h and PYTHIA8 predictions ($p_{T}^{assoc}$ > 0.3 GeV/c)

Fig. Group : $D^{+}_{s}$-hadron azimuthal correlations in pp collisions at $\sqrt{s}$=13.6 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13.6 TeV
System: p-p

Comparison between measured Ds-h and D+-h azimuthal correlation distributions (5 < $p_{T}$ < 8 GeV/c)

Fig. Group : $D^{+}_{s}$-hadron azimuthal correlations in pp collisions at $\sqrt{s}$=13.6 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13.6 TeV
System: p-p

Comparison between measured Ds-h and D+-h azimuthal correlation distributions (3 < $p_{T}$ < 5 GeV/c)

Fig. Group : $D^{+}_{s}$-hadron azimuthal correlations in pp collisions at $\sqrt{s}$=13.6 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13.6 TeV
System: p-p

Comparison between measured Ds-h azimuthal correlation distribution and PYTHIA8 predictions (1 < $p_{T}$ < 3 GeV/c)

Fig. Group : $D^{+}_{s}$-hadron azimuthal correlations in pp collisions at $\sqrt{s}$=13.6 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13.6 TeV
System: p-p

Comparison between measured Ds-h azimuthal correlation distribution and PYTHIA8 predictions (3 < $p_{T}$ < 5 GeV/c)

Fig. Group : $D^{+}_{s}$-hadron azimuthal correlations in pp collisions at $\sqrt{s}$=13.6 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13.6 TeV
System: p-p

Comparison between measured Ds-h azimuthal correlation distribution and PYTHIA8 predictions (5 < $p_{T}$ < 8 GeV/c)

Fig. Group : $D^{+}_{s}$-hadron azimuthal correlations in pp collisions at $\sqrt{s}$=13.6 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13.6 TeV
System: p-p

Comparison between measured Ds-h azimuthal correlation distribution and PYTHIA8 predictions (8 < $p_{T}$ < 16 GeV/c)

Fig. Group : $D^{+}_{s}$-hadron azimuthal correlations in pp collisions at $\sqrt{s}$=13.6 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13.6 TeV
System: p-p

Comparison between measured Ds-h azimuthal correlation distribution and PYTHIA8 predictions (16 < $p_{T}$ < 36 GeV/c)

Fig. Group : $D^{+}_{s}$-hadron azimuthal correlations in pp collisions at $\sqrt{s}$=13.6 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13.6 TeV
System: p-p

Elliptic flow of $\Lambda_c^+$ in Pb--Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.36 TeV in 30--50% centrality in Run 3

$\Lambda_c^+$ raw yield distribution as a function of the selection applied on the BDT output score in 4 < $p_T$ < 5 GeV/c interval.

Fig. Group : Elliptic flow of $\Lambda_c^+$ in Pb--Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.36 TeV in 30--50% centrality in Run 3
PWG : PWG-HF (Heavy Flavour)
Energy: 5.36 TeV
System: Pb-Pb

Observed elliptic flow as a function of non-prompt fraction for $\Lambda_c^+$ in 4 < $p_T$ < 5 GeV/c interval.

Fig. Group : Elliptic flow of $\Lambda_c^+$ in Pb--Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.36 TeV in 30--50% centrality in Run 3
PWG : PWG-HF (Heavy Flavour)
Energy: 5.36 TeV
System: Pb-Pb

Simultaneous fit of the invariant-mass distribution and $v_2$ versus invariant mass of $\Lambda_c^+$ candidates in the 4 < $p_T$< 5 GeV/c interval (0.8 < BDT score to be prompt < 1).

Fig. Group : Elliptic flow of $\Lambda_c^+$ in Pb--Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.36 TeV in 30--50% centrality in Run 3
PWG : PWG-HF (Heavy Flavour)
Energy: 5.36 TeV
System: Pb-Pb

Simultaneous fit of the invariant-mass distribution and $v_2$ versus invariant mass of $\Lambda_c^+$ candidates in the 4 < $p_T$< 5 GeV/c interval (0.03 < BDT score to be prompt < 0.8).

Fig. Group : Elliptic flow of $\Lambda_c^+$ in Pb--Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.36 TeV in 30--50% centrality in Run 3
PWG : PWG-HF (Heavy Flavour)
Energy: 5.36 TeV
System: Pb-Pb

Simultaneous fit of the invariant-mass distribution and $v_2$ versus invariant mass of $\Lambda_c^+$ candidates in the 4 < $p_T$< 5 GeV/c interval (0 < BDT score to be prompt < 0.03).

Fig. Group : Elliptic flow of $\Lambda_c^+$ in Pb--Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.36 TeV in 30--50% centrality in Run 3
PWG : PWG-HF (Heavy Flavour)
Energy: 5.36 TeV
System: Pb-Pb

$v_2$ of Prompt $\Lambda_c^+$ and Prompt $D^0$ in Pb--Pb collisions at 5.36 TeV compared with models and light flavor from published data with $KE_T$ NCQ scaling ($KE_T$<3.3 version)

Fig. Group : Elliptic flow of $\Lambda_c^+$ in Pb--Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.36 TeV in 30--50% centrality in Run 3
PWG : PWG-HF (Heavy Flavour)
Energy: 5.36 TeV
System: Pb-Pb

$v_2$ of Prompt $\Lambda_c^+$ and Prompt $D^0$ in Pb--Pb collisions at 5.36 TeV compared with models and light flavor from published data with $p_T$ NCQ scaling

Fig. Group : Elliptic flow of $\Lambda_c^+$ in Pb--Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.36 TeV in 30--50% centrality in Run 3
PWG : PWG-HF (Heavy Flavour)
Energy: 5.36 TeV
System: Pb-Pb

$v_2$ of Prompt $\Lambda_c^+$ and Prompt $D^0$ in Pb--Pb collisions at 5.36 TeV compared with models and light flavor from published data with $p_T$ NCQ scaling (logx version)

Fig. Group : Elliptic flow of $\Lambda_c^+$ in Pb--Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.36 TeV in 30--50% centrality in Run 3
PWG : PWG-HF (Heavy Flavour)
Energy: 5.36 TeV
System: Pb-Pb

$v_2$ of Prompt $\Lambda_c^+$ and Prompt $D^0$ in Pb--Pb collisions at 5.36 TeV compared with models and light flavor from published data with $KE_T$ NCQ scaling (logx version)

Fig. Group : Elliptic flow of $\Lambda_c^+$ in Pb--Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.36 TeV in 30--50% centrality in Run 3
PWG : PWG-HF (Heavy Flavour)
Energy: 5.36 TeV
System: Pb-Pb

$v_2$ of Prompt $\Lambda_c^+$ and Prompt $D^0$ in Pb--Pb collisions at 5.36 TeV compared with models and light flavor from published data with $KE_T$ NCQ scaling

Fig. Group : Elliptic flow of $\Lambda_c^+$ in Pb--Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.36 TeV in 30--50% centrality in Run 3
PWG : PWG-HF (Heavy Flavour)
Energy: 5.36 TeV
System: Pb-Pb

$v_2$ of Prompt $\Lambda_c^+$ and Prompt $D^0$ in Pb--Pb collisions at 5.36 TeV compared with light flavor from published data

Fig. Group : Elliptic flow of $\Lambda_c^+$ in Pb--Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.36 TeV in 30--50% centrality in Run 3
PWG : PWG-HF (Heavy Flavour)
Energy: 5.36 TeV
System: Pb-Pb

$v_2$ of Prompt $\Lambda_c^+$ and Prompt $D^0$ in Pb--Pb collisions at 5.36 TeV compared with tamu model

Fig. Group : Elliptic flow of $\Lambda_c^+$ in Pb--Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.36 TeV in 30--50% centrality in Run 3
PWG : PWG-HF (Heavy Flavour)
Energy: 5.36 TeV
System: Pb-Pb

$v_2$ of Prompt $\Lambda_c^+$ and Prompt $D^0$ in Pb--Pb collisions at 5.36 TeV compared with models

Fig. Group : Elliptic flow of $\Lambda_c^+$ in Pb--Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.36 TeV in 30--50% centrality in Run 3
PWG : PWG-HF (Heavy Flavour)
Energy: 5.36 TeV
System: Pb-Pb

$v_2$ of Prompt $\Lambda_c^+$ compared with Prompt $D^0$ in Pb--Pb collisions at 5.36 TeV

Fig. Group : Elliptic flow of $\Lambda_c^+$ in Pb--Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.36 TeV in 30--50% centrality in Run 3
PWG : PWG-HF (Heavy Flavour)
Energy: 5.36 TeV
System: Pb-Pb

$v_2$ of $\Lambda_c^+$ compared with $D^0$ in Pb--Pb collisions at 5.36 TeV

Fig. Group : Elliptic flow of $\Lambda_c^+$ in Pb--Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.36 TeV in 30--50% centrality in Run 3
PWG : PWG-HF (Heavy Flavour)
Energy: 5.36 TeV
System: Pb-Pb

Elliptic flow of D mesons in Pb--Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.36$ TeV in 30--50% centrality in Run 3

$\it{v}_{\rm 2}$ of prompt and non-prompt $\rm {D^{0}}$ in Pb--Pb collisions at 5.36 TeV compared to TAMU model predictions

Fig. Group : Elliptic flow of D mesons in Pb--Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.36$ TeV in 30--50% centrality in Run 3
PWG : PWG-HF (Heavy Flavour)
Energy: 5.36 TeV
System: Pb-Pb

$\it{v}_{\rm 2}$ of non-prompt $\rm {D^{0}}$ in Pb--Pb collisions at 5.36 TeV compared to transport model predictions

Fig. Group : Elliptic flow of D mesons in Pb--Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.36$ TeV in 30--50% centrality in Run 3
PWG : PWG-HF (Heavy Flavour)
Energy: 5.36 TeV
System: Pb-Pb

$\it{v}_{\rm 2}$ of non-prompt $\rm {D^{0}}$ in Pb--Pb collisions at 5.36 TeV versus Run 2 results

Fig. Group : Elliptic flow of D mesons in Pb--Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.36$ TeV in 30--50% centrality in Run 3
PWG : PWG-HF (Heavy Flavour)
Energy: 5.36 TeV
System: Pb-Pb

$\it{v}_{\rm 2}$ of $\rm {D^{0}}$, $\rm {D^{+}}$, $\rm {D_{s}^{+}}$, and $\rm {J/\psi}$ in Pb--Pb collisions at 5.36 TeV for one pT bin verus centrality

Fig. Group : Elliptic flow of D mesons in Pb--Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.36$ TeV in 30--50% centrality in Run 3
PWG : PWG-HF (Heavy Flavour)
Energy: 5.36 TeV
System: Pb-Pb

$\it{v}_{\rm 2}$ of $\rm {D^{0}}$ and $\rm {\Lambda_{c}^{+}}$ in Pb--Pb collisions at 5.36 TeV (log scale)

Fig. Group : Elliptic flow of D mesons in Pb--Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.36$ TeV in 30--50% centrality in Run 3
PWG : PWG-HF (Heavy Flavour)
Energy: 5.36 TeV
System: Pb-Pb

$\it{v}_{\rm 2}$ of $\rm {D^{0}}$ and $\rm {\Lambda_{c}^{+}}$ in Pb--Pb collisions at 5.36 TeV (no log scale)

Fig. Group : Elliptic flow of D mesons in Pb--Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.36$ TeV in 30--50% centrality in Run 3
PWG : PWG-HF (Heavy Flavour)
Energy: 5.36 TeV
System: Pb-Pb

$\it{v}_{\rm 2}$ of $\rm {D^{0}}$, $\rm {D^{+}}$, $\rm {D_{s}^{+}}$, $\rm {J/\psi}$, and $\rm {\Lambda_{c}^{+}}$ in Pb--Pb collisions at 5.36 TeV compared to TAMU predictions (no log scale)

Fig. Group : Elliptic flow of D mesons in Pb--Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.36$ TeV in 30--50% centrality in Run 3
PWG : PWG-HF (Heavy Flavour)
Energy: 5.36 TeV
System: Pb-Pb

$\it{v}_{\rm 2}$ of $\rm {D^{0}}$, $\rm {D^{+}}$, $\rm {D_{s}^{+}}$, $\rm {J/\psi}$, and $\rm {\Lambda_{c}^{+}}$ in Pb--Pb collisions at 5.36 TeV compared to TAMU predictions (log scale)

Fig. Group : Elliptic flow of D mesons in Pb--Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.36$ TeV in 30--50% centrality in Run 3
PWG : PWG-HF (Heavy Flavour)
Energy: 5.36 TeV
System: Pb-Pb

$\it{v}_{\rm 2}$ of $\rm {D^{0, +}}$ in Pb--Pb collisions at 5.36 TeV in 60-80% centrality versus Langevin model predictions

Fig. Group : Elliptic flow of D mesons in Pb--Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.36$ TeV in 30--50% centrality in Run 3
PWG : PWG-HF (Heavy Flavour)
Energy: 5.36 TeV
System: Pb-Pb

Observed elliptic flow as a function of non-prompt fraction for $\rm{D^{0}}$, $\rm{D^{+}}$, and $\rm{D_{s}^{+}}$ in one pT and centrality interval

Fig. Group : Elliptic flow of D mesons in Pb--Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.36$ TeV in 30--50% centrality in Run 3
PWG : PWG-HF (Heavy Flavour)
Energy: 5.36 TeV
System: Pb-Pb

$\mathrm{D}^{0}$ raw yield distribution as a function of the selection applied on the BDT output score

Fig. Group : Elliptic flow of D mesons in Pb--Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.36$ TeV in 30--50% centrality in Run 3
PWG : PWG-HF (Heavy Flavour)
Energy: 5.36 TeV
System: Pb-Pb

$\it{v}_{\rm 2}$ of $\rm {D^{0}}$ in Pb--Pb collisions at 5.36 TeV compared with pions and deuterons from Run 2 in different centrality bins

Fig. Group : Elliptic flow of D mesons in Pb--Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.36$ TeV in 30--50% centrality in Run 3
PWG : PWG-HF (Heavy Flavour)
Energy: 5.36 TeV
System: Pb-Pb

$\it{v}_{\rm 2}$ of $\rm {D^{0}}$, $\rm {D^{+}}$, and $\rm {D_{s}^{+}}$ in Pb--Pb collisions at 5.36 TeV compared with PHSD in different centrality bins

Fig. Group : Elliptic flow of D mesons in Pb--Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.36$ TeV in 30--50% centrality in Run 3
PWG : PWG-HF (Heavy Flavour)
Energy: 5.36 TeV
System: Pb-Pb

$\it{v}_{\rm 2}$ of $\rm {D^{0}}$, $\rm {D^{+}}$, and $\rm {D_{s}^{+}}$ in Pb--Pb collisions at 5.36 TeV verus pions from Run 2 in different centrality bins

Fig. Group : Elliptic flow of D mesons in Pb--Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.36$ TeV in 30--50% centrality in Run 3
PWG : PWG-HF (Heavy Flavour)
Energy: 5.36 TeV
System: Pb-Pb

$\it{v}_{\rm 2}$ of $\rm {D^{0}}$, $\rm {D^{+}}$, $\rm {D_{s}^{+}}$, and $\rm {J/\psi}$ in Pb--Pb collisions at 5.36 TeV verus pions from Run 2

Fig. Group : Elliptic flow of D mesons in Pb--Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.36$ TeV in 30--50% centrality in Run 3
PWG : PWG-HF (Heavy Flavour)
Energy: 5.36 TeV
System: Pb-Pb

$\it{v}_{\rm 2}$ of $\rm {D^{0}}$ and $\rm {D_{s}^{+}}$ in Pb--Pb collisions at 5.36 TeV versus TAMU

Fig. Group : Elliptic flow of D mesons in Pb--Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.36$ TeV in 30--50% centrality in Run 3
PWG : PWG-HF (Heavy Flavour)
Energy: 5.36 TeV
System: Pb-Pb

$\it{v}_{\rm 2}$ of $\rm {D^{0, +}}$ in Pb--Pb collisions at 5.36 TeV versus Run 2 results

Fig. Group : Elliptic flow of D mesons in Pb--Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.36$ TeV in 30--50% centrality in Run 3
PWG : PWG-HF (Heavy Flavour)
Energy: 5.36 TeV
System: Pb-Pb

$\it{v}_{\rm 2}$ of $\rm {D_{s}^+}$ in Pb--Pb collisions at 5.36 TeV versus Run 2 results

Fig. Group : Elliptic flow of D mesons in Pb--Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.36$ TeV in 30--50% centrality in Run 3
PWG : PWG-HF (Heavy Flavour)
Energy: 5.36 TeV
System: Pb-Pb

$\it{v}_{\rm 2}$ of $\rm {D_{s}^+}$ in Pb--Pb collisions at 5.36 TeV versus models

Fig. Group : Elliptic flow of D mesons in Pb--Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.36$ TeV in 30--50% centrality in Run 3
PWG : PWG-HF (Heavy Flavour)
Energy: 5.36 TeV
System: Pb-Pb

Simultaneous fit to invariant-mass distribution and $\it{v}_{\rm 2}$ of $\rm {D^0}$ in Pb--Pb collisions at 5.36 TeV

Fig. Group : Elliptic flow of D mesons in Pb--Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.36$ TeV in 30--50% centrality in Run 3
PWG : PWG-HF (Heavy Flavour)
Energy: 5.36 TeV
System: Pb-Pb

Simultaneous fit to invariant-mass distribution and $\it{v}_{\rm 2}$ of $\rm {D^+}$ in Pb--Pb collisions at 5.68 TeV

Fig. Group : Elliptic flow of D mesons in Pb--Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.36$ TeV in 30--50% centrality in Run 3
PWG : PWG-HF (Heavy Flavour)
Energy: 5.36 TeV
System: Pb-Pb

Simultaneous fit to invariant-mass distribution and $\it{v}_{\rm 2}$ of $\rm {D_{s}^+}$ in Pb--Pb collisions at 5.36 TeV

Fig. Group : Elliptic flow of D mesons in Pb--Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.36$ TeV in 30--50% centrality in Run 3
PWG : PWG-HF (Heavy Flavour)
Energy: 5.36 TeV
System: Pb-Pb

p-$\Lambda_c$ femtoscopy in pp collisions at 13.6 TeV

Cut variation of $\Lambda_c$ in pt 2 to 3 geV/c in pp collisions at 13.6 TeV

Fig. Group : p-$\Lambda_c$ femtoscopy in pp collisions at 13.6 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13.6 TeV
System: p-p

p-$\Lambda_c$ inv.mass in mixed-event in pp collisions at 13.6 TeV

Fig. Group : p-$\Lambda_c$ femtoscopy in pp collisions at 13.6 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13.6 TeV
System: p-p

p-$\Lambda_c$ inv.mass in same-event in pp collisions at 13.6 TeV

Fig. Group : p-$\Lambda_c$ femtoscopy in pp collisions at 13.6 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13.6 TeV
System: p-p

p-$\Lambda_c$ raw correlation function compare with models included strong interaction in pp collisions at 13.6 TeV

Fig. Group : p-$\Lambda_c$ femtoscopy in pp collisions at 13.6 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13.6 TeV
System: p-p

p-$\Lambda_c$ raw correlation function fit decomposition in pp collisions at 13.6 TeV

Fig. Group : p-$\Lambda_c$ femtoscopy in pp collisions at 13.6 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13.6 TeV
System: p-p

p-$\Lambda_c$ raw correlation function fit with coulomb only and background in pp collisions at 13.6 TeV

Fig. Group : p-$\Lambda_c$ femtoscopy in pp collisions at 13.6 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13.6 TeV
System: p-p

Ds1+and Ds2*+ production in pp collisions at 13.6 TeV

Ds1+/Ds ratio, (BR factorized)

Fig. Group : Ds1+and Ds2*+ production in pp collisions at 13.6 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13.6 TeV
System: p-p

Ds2*/Ds ratio, (BR factorized)

Fig. Group : Ds1+and Ds2*+ production in pp collisions at 13.6 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13.6 TeV
System: p-p

Ds2*/Ds ratio

Fig. Group : Ds1+and Ds2*+ production in pp collisions at 13.6 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13.6 TeV
System: p-p

Ds1+/Ds ratio

Fig. Group : Ds1+and Ds2*+ production in pp collisions at 13.6 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13.6 TeV
System: p-p

Ds, Ds1+ and Ds2* cross section

Fig. Group : Ds1+and Ds2*+ production in pp collisions at 13.6 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13.6 TeV
System: p-p

Ds1+ Invariant Mass 2<pT<3 GeV/c

Fig. Group : Ds1+and Ds2*+ production in pp collisions at 13.6 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13.6 TeV
System: p-p

Ds1+ Invariant Mass 6<pT<8 GeV/c

Fig. Group : Ds1+and Ds2*+ production in pp collisions at 13.6 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13.6 TeV
System: p-p

Ds1+ Invariant Mass 12<pT<24 GeV/c

Fig. Group : Ds1+and Ds2*+ production in pp collisions at 13.6 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13.6 TeV
System: p-p

Ds2* Invariant Mass 12<pT<24 GeV/c

Fig. Group : Ds1+and Ds2*+ production in pp collisions at 13.6 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13.6 TeV
System: p-p

Ds2* Invariant Mass 6<pT<8 GeV/c

Fig. Group : Ds1+and Ds2*+ production in pp collisions at 13.6 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13.6 TeV
System: p-p

Ds2* Invariant Mass 2<pT<4 GeV/c

Fig. Group : Ds1+and Ds2*+ production in pp collisions at 13.6 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13.6 TeV
System: p-p

Energy-energy correlator measurements for jets in p-Pb collisions at 5.02TeV

Ratio of EECs in p-Pb and pp in different jet pT bins (20-27, 27-40, 40-80 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

Ratio of EEC distributions for charged jets in pp and p-Pb collisions -- 20-40 GeV/c with fit

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

$\mathrm{B^0}$-meson production cross section in pp collisions at $\sqrt{s}=13.6~\mathrm{TeV}$

Beauty production cross section per rapidity unit at midrapidity as a function of $\sqrt{s}$

Fig. Group : $\mathrm{B^0}$-meson production cross section in pp collisions at $\sqrt{s}=13.6~\mathrm{TeV}$
PWG : PWG-HF (Heavy Flavour)
Energy: 13.6 TeV
System: p-p

Mid-over-forward rapidity ratio of $\mathrm{B}$ meson production yields in pp collisions compared to $\mathrm{D^0}$ meson measurement

Fig. Group : $\mathrm{B^0}$-meson production cross section in pp collisions at $\sqrt{s}=13.6~\mathrm{TeV}$
PWG : PWG-HF (Heavy Flavour)
Energy: 13.6 TeV
System: p-p

Mid-over-forward rapidity ratio of $\mathrm{B}$ meson production yields in pp collisions compared to FONLL predictions

Fig. Group : $\mathrm{B^0}$-meson production cross section in pp collisions at $\sqrt{s}=13.6~\mathrm{TeV}$
PWG : PWG-HF (Heavy Flavour)
Energy: 13.6 TeV
System: p-p

Production cross section of $\mathrm{B^0}$ mesons in pp collisions at $\sqrt{s}=13.6~\mathrm{TeV}$ compared to $k_\mathrm{T}$ factorisation predictions

Fig. Group : $\mathrm{B^0}$-meson production cross section in pp collisions at $\sqrt{s}=13.6~\mathrm{TeV}$
PWG : PWG-HF (Heavy Flavour)
Energy: 13.6 TeV
System: p-p

Production cross section of $\mathrm{B^0}$ mesons in pp collisions at $\sqrt{s}=13.6~\mathrm{TeV}$ compared to theoretical predictions

Fig. Group : $\mathrm{B^0}$-meson production cross section in pp collisions at $\sqrt{s}=13.6~\mathrm{TeV}$
PWG : PWG-HF (Heavy Flavour)
Energy: 13.6 TeV
System: p-p

Production cross section of $\mathrm{B^0}$ mesons in pp collisions at $\sqrt{s}=13.6~\mathrm{TeV}$ compared to CMS measurement and FONLL predictions

Fig. Group : $\mathrm{B^0}$-meson production cross section in pp collisions at $\sqrt{s}=13.6~\mathrm{TeV}$
PWG : PWG-HF (Heavy Flavour)
Energy: 13.6 TeV
System: p-p

Recall efficiency for non-prompt $\mathrm{D^\pm}$ mesons in pp collisions at $\sqrt{s}=13.6~\mathrm{TeV}$

Fig. Group : $\mathrm{B^0}$-meson production cross section in pp collisions at $\sqrt{s}=13.6~\mathrm{TeV}$
PWG : PWG-HF (Heavy Flavour)
Energy: 13.6 TeV
System: p-p

Acceptance$\times$Efficiency correction for $\mathrm{B^0}$ mesons in pp collisions at $\sqrt{s}=13.6~\mathrm{TeV}$

Fig. Group : $\mathrm{B^0}$-meson production cross section in pp collisions at $\sqrt{s}=13.6~\mathrm{TeV}$
PWG : PWG-HF (Heavy Flavour)
Energy: 13.6 TeV
System: p-p

Invariant mass distribution of $\mathrm{D^-}\pi^+$pairs in the $10<\pt<14~\mathrm{GeV}/c$ interval in pp collisions at $\sqrt{s}=13.6~\mathrm{TeV}$

Fig. Group : $\mathrm{B^0}$-meson production cross section in pp collisions at $\sqrt{s}=13.6~\mathrm{TeV}$
PWG : PWG-HF (Heavy Flavour)
Energy: 13.6 TeV
System: p-p

Invariant mass distribution of $\mathrm{D^-}\pi^+$pairs in the $2<\pt<4~\mathrm{GeV}/c$ interval in pp collisions at $\sqrt{s}=13.6~\mathrm{TeV}$

Fig. Group : $\mathrm{B^0}$-meson production cross section in pp collisions at $\sqrt{s}=13.6~\mathrm{TeV}$
PWG : PWG-HF (Heavy Flavour)
Energy: 13.6 TeV
System: p-p

Invariant mass distribution of $\mathrm{D^-}\pi^+$pairs in the $1<\pt<23.5~\mathrm{GeV}/c$ interval in pp collisions at $\sqrt{s}=13.6~\mathrm{TeV}$

Fig. Group : $\mathrm{B^0}$-meson production cross section in pp collisions at $\sqrt{s}=13.6~\mathrm{TeV}$
PWG : PWG-HF (Heavy Flavour)
Energy: 13.6 TeV
System: p-p

$\Lambda_{\rm c}^{+}$ polarization in pp collisions at $\sqrt{s} = 13.6$ TeV

Longitudinal polarization ($P_{\rm z}$) of prompt and non-prompt $\Lambda_{\rm c}^+$ and $\bar{\Lambda}_{\rm c}^-$ in pp collisions at $\sqrt{s} = 13.6$ TeV (production frame)

Fig. Group : $\Lambda_{\rm c}^{+}$ polarization in pp collisions at $\sqrt{s} = 13.6$ TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13.6 TeV
System: p-p

Longitudinal polarization as a function of non-prompt fraction for $\Lambda_{\rm c}^+$ and $\bar{\Lambda}_{\rm c}^-$ in pp collisions at $\sqrt{s} = 13.6$ TeV (production frame)

Fig. Group : $\Lambda_{\rm c}^{+}$ polarization in pp collisions at $\sqrt{s} = 13.6$ TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13.6 TeV
System: p-p

Simultaneous fit of $\Lambda_{\rm c}^+$ and $\bar{\Lambda}_{\rm c}^-$ corrected yield as a function of $\cos(\theta^*)$ in pp collisions at $\sqrt{s} = 13.6$ TeV (production frame)

Fig. Group : $\Lambda_{\rm c}^{+}$ polarization in pp collisions at $\sqrt{s} = 13.6$ TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13.6 TeV
System: p-p

Invariant mass distribution of ${\rm pK}\pi$ triplets in pp collisions at $\sqrt{s} = 13.6$ TeV in two intervals of $\cos(\theta^*)$ (production frame)

Fig. Group : $\Lambda_{\rm c}^{+}$ polarization in pp collisions at $\sqrt{s} = 13.6$ TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13.6 TeV
System: p-p

D$^{0}$ meson yields as a function of the underlying event activity in pp collisions at $\sqrt{s}$=13 TeV

Ratio of the $R_{\rm T}$-dependent per-event D$^0$ meson yields to the $R_{\rm T}$-integrated yield in the toward region

Fig. Group : D$^{0}$ meson yields as a function of the underlying event activity in pp collisions at $\sqrt{s}$=13 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13 TeV
System: p-p

Acceptance-times-efficiency correction of D$^0$ mesons as a function of the $R_{\rm T}$

Fig. Group : D$^{0}$ meson yields as a function of the underlying event activity in pp collisions at $\sqrt{s}$=13 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13 TeV
System: p-p

Invariant mass distribution of D$^0$ candidates with 12 < $p_{\rm T}^{\rm D^0}$ < 18 GeV/$c$ in $R_{\rm T}$ > 1 events

Fig. Group : D$^{0}$ meson yields as a function of the underlying event activity in pp collisions at $\sqrt{s}$=13 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13 TeV
System: p-p

Invariant mass distribution of D$^0$ candidates with 5 < $p_{\rm T}^{\rm D^0}$ < 8 GeV/$c$ in $R_{\rm T}$ < 1 events

Fig. Group : D$^{0}$ meson yields as a function of the underlying event activity in pp collisions at $\sqrt{s}$=13 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13 TeV
System: p-p

Inclusive charged-particle jet cross section in pp collisions at \sqrt{s} = 13.6 TeV

Inclusive charged-particle jet invariant yield in pp collisions at \sqrt{s} = 13.6 TeV

Fig. Group : Inclusive charged-particle jet cross section in pp collisions at \sqrt{s} = 13.6 TeV
PWG : PWG-JE (Jets)
Energy: 13.6 TeV
System: p-p

Inclusive charged-particle jet cross section in pp collisions at \sqrt{s} = 13.6 TeV

Fig. Group : Inclusive charged-particle jet cross section in pp collisions at \sqrt{s} = 13.6 TeV
PWG : PWG-JE (Jets)
Energy: 13.6 TeV
System: p-p

pi, K, p in jets in 0-10% Pb-Pb and pp 5.02 TeV Preliminary

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: Pb-Pb

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: Pb-Pb

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