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Scope: PWG

System

Energy

$\Lambda_{c}^{+}$ -- proton azimuthal correlations in pp collisions at $\sqrt{s} = 13.6$ TeV

Associated $\Delta\varphi$ integrated $\Lambda_{c}$-p yield in $p_{\mathrm{T}}^{\Lambda_{c}} 3$-$12$ GeV/$c$ and $p_{\mathrm{T}}^{p} 0.4$-$4.5$ GeV/$c$ with models

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

Associated away-side peak yield $\Lambda_{c}$-pyield in $p_{\mathrm{T}}^{\Lambda_{c}} 3$-$12$ GeV/$c$ and $p_{\mathrm{T}}^{p} 0.4$-$4.5$ GeV/$c$ with models

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

Associated near-side peak yield $\Lambda_{c}$-pyield in $p_{\mathrm{T}}^{\Lambda_{c}} 3$-$12$ GeV/$c$ and $p_{\mathrm{T}}^{p} 0.4$-$4.5$ GeV/$c$ with models

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

Unlike-sign - like-sign $\Lambda_{c}$-p Azimuthal Correlations in $p_{\mathrm{T}}^{\Lambda_{c}} 3$-$5$ GeV/$c$ and $p_{\mathrm{T}}^{p} 0.4$-$1.0$ GeV/$c$ with models

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

Unlike-sign - like-sign $\Lambda_{c}$-p Azimuthal Correlations in $p_{\mathrm{T}}^{\Lambda_{c}} 3$-$5$ GeV/$c$ and $p_{\mathrm{T}}^{p} 1.0$-$2.5$ GeV/$c$ with models

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

Unlike-sign - like-sign $\Lambda_{c}$-p Azimuthal Correlations in $p_{\mathrm{T}}^{\Lambda_{c}} 3$-$5$ GeV/$c$ and $p_{\mathrm{T}}^{p} 2.5$-$4.5$ GeV/$c$ with models

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

Unlike-sign - like-sign $\Lambda_{c}$-p Azimuthal Correlations in $p_{\mathrm{T}}^{\Lambda_{c}} 5$-$8$ GeV/$c$ and $p_{\mathrm{T}}^{p} 2.5$-$4.5$ GeV/$c$ with models

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

Unlike-sign - like-sign $\Lambda_{c}$-p Azimuthal Correlations in $p_{\mathrm{T}}^{\Lambda_{c}} 5$-$8$ GeV/$c$ and $p_{\mathrm{T}}^{p} 1.0$-$2.5$ GeV/$c$ with models

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

Unlike-sign - like-sign $\Lambda_{c}$-p Azimuthal Correlations in $p_{\mathrm{T}}^{\Lambda_{c}} 5$-$8$ GeV/$c$ and $p_{\mathrm{T}}^{p} 0.4$-$1.0$ GeV/$c$ with models

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

Unlike-sign - like-sign $\Lambda_{c}$-p Azimuthal Correlations in $p_{\mathrm{T}}^{\Lambda_{c}} 8$-$12$ GeV/$c$ and $p_{\mathrm{T}}^{p} 0.4$-$1.0$ GeV/$c$ with models

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

Unlike-sign - like-sign $\Lambda_{c}$-p Azimuthal Correlations in $p_{\mathrm{T}}^{\Lambda_{c}} 8$-$12$ GeV/$c$ and $p_{\mathrm{T}}^{p} 2.5$-$4.5$ GeV/$c$ with models

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

Unlike-sign - like-sign $\Lambda_{c}$-p Azimuthal Correlations in $p_{\mathrm{T}}^{\Lambda_{c}} 8$-$12$ GeV/$c$ and $p_{\mathrm{T}}^{p} 1.0$-$2.5$ GeV/$c$ with models

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

Unlike-sign - like-sign $\Lambda_{c}$-p Azimuthal Correlations in $p_{\mathrm{T}}^{\Lambda_{c}} 12$-$24$ GeV/$c$ and $p_{\mathrm{T}}^{p} 1.0$-$2.5$ GeV/$c$ with models

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

Unlike-sign - like-sign $\Lambda_{c}$-p Azimuthal Correlations in $p_{\mathrm{T}}^{\Lambda_{c}} 12$-$24$ GeV/$c$ and $p_{\mathrm{T}}^{p} 2.5$-$4.5$ GeV/$c$ with models

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 $p_{\mathrm{T}}^{\Lambda_{c}} 12$-$24$ GeV/$c$ and $p_{\mathrm{T}}^{p} 1.0$-$2.5$ GeV/$c$ with models

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 $p_{\mathrm{T}}^{\Lambda_{c}} 12$-$24$ GeV/$c$ and $p_{\mathrm{T}}^{p} 2.5$-$4.5$ GeV/$c$ with models

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 $p_{\mathrm{T}}^{\Lambda_{c}} 8$-$12$ GeV/$c$ and $p_{\mathrm{T}}^{p} 2.5$-$4.5$ GeV/$c$ with models

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 $p_{\mathrm{T}}^{\Lambda_{c}} 8$-$12$ GeV/$c$ and $p_{\mathrm{T}}^{p} 1.0$-$2.5$ GeV/$c$ with models

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 $p_{\mathrm{T}}^{\Lambda_{c}} 8$-$12$ GeV/$c$ and $p_{\mathrm{T}}^{p} 0.4$-$1.0$ GeV/$c$ with models

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 $p_{\mathrm{T}}^{p} 0.4$-$1.0$ GeV/$c$ with models

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 $p_{\mathrm{T}}^{p} 1.0$-$2.5$ GeV/$c$ with models

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 $p_{\mathrm{T}}^{p} 2.5$-$4.5$ GeV/$c$ with models

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 $p_{\mathrm{T}}^{p} 2.5$-$4.5$ GeV/$c$ with models

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 $p_{\mathrm{T}}^{p} 1.0$-$2.5$ GeV/$c$ with models

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/$c$ with models

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

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

Ds-K ULS-LS near-side yield

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

Ds-$\pi$ ULS-LS azimuthal correlation distribution (5 < $p_{T}$ < 8 GeV/c) comparison with models

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

Ds-K ULS-LS azimuthal correlation distribution (5 < $p_{T}$ < 8 GeV/c) comparison with models

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

Ds-K ULS and LS azimuthal correlation distribution comparison (8 < $p_{T}$ < 16 GeV/c) comparison with models

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

Ds-K ULS and LS azimuthal correlation distribution comparison (5 < $p_{T}$ < 8 GeV/c) comparison with models

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

Ds-$pi$ ULS and LS azimuthal correlation distribution comparison (5 < $p_{T}$ < 8 GeV/c) comparison with models

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

Ds-$\pi$ ULS-LS azimuthal correlation distribution (1 < $p_{T}$ < 3 GeV/c) comparison with models

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

Ds-K ULS-LS near-side yield comparison with models

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

Ds-$\pi$ ULS-LS azimuthal correlation distribution (1 < $p_{T}$ < 3 GeV/c)

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

Ds-$\pi$ ULS-LS azimuthal correlation distribution (3 < $p_{T}$ < 5 GeV/c)

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

Ds-$\pi$ ULS-LS azimuthal correlation distribution (5 < $p_{T}$ < 8 GeV/c)

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

Ds-$\pi$ ULS-LS azimuthal correlation distribution (8 < $p_{T}$ < 16 GeV/c)

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

Ds-K ULS-LS azimuthal correlation distribution (8 < $p_{T}$ < 16 GeV/c)

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

Ds-K ULS-LS azimuthal correlation distribution (5 < $p_{T}$ < 8 GeV/c)

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

Ds-K ULS-LS azimuthal correlation distribution (3 < $p_{T}$ < 5 GeV/c)

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

Ds-K ULS-LS azimuthal correlation distribution (1 < $p_{T}$ < 3 GeV/c)

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

Ds-$pi$ ULS and LS azimuthal correlation distribution comparison (1 < $p_{T}$ < 3 GeV/c)

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

Ds-$pi$ ULS and LS azimuthal correlation distribution comparison (3 < $p_{T}$ < 5 GeV/c)

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

Ds-$pi$ ULS and LS azimuthal correlation distribution comparison (5 < $p_{T}$ < 8 GeV/c)

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

Ds-$pi$ ULS and LS azimuthal correlation distribution comparison (8 < $p_{T}$ < 16 GeV/c)

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

Ds-K ULS and LS azimuthal correlation distribution comparison (8 < $p_{T}$ < 16 GeV/c)

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

Ds-K ULS and LS azimuthal correlation distribution comparison (5 < $p_{T}$ < 8 GeV/c)

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

Ds-K ULS and LS azimuthal correlation distribution comparison (3 < $p_{T}$ < 5 GeV/c)

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

Ds-K ULS and LS azimuthal correlation distribution comparison (1 < $p_{T}$ < 3 GeV/c)

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

Measurement of the prompt $\mathrm{D}^0$ cross section in pp collisions at $\sqrt{s} = 13.6\ \mathrm{TeV}$

$\mathrm{\Lambda_{c}^{+}}/\mathrm{D}^0$ 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

Preliminary measurement of prompt D-meson elliptic flow in OO collisions

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, Pb-Pb

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

D+-p femto in pp collisions at 13.6 TeV

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

$\Xi_c^+/\Lambda_c^+$ ratio in pp collisions at $\sqrt{s} = 13.6$ TeV

$\Xi_c^+/\Lambda_c^+$ 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

$\Xi_c^+/\Lambda_c^+$ 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

OmegaC production vs multiplicity in pp collisions at 13.6 TeV

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

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

$\mathrm{D_s^+/D^+}$ production yield ratio in Pb$-$Pb collisions at $\sqrt{s_\mathrm{NN}}=5.36$ TeV

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, 13.6 TeV
System: p-p, 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, 13.6 TeV
System: p-p, 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, 13.6 TeV
System: p-p, 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, 13.6 TeV
System: p-p, Pb-Pb

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, 13.6 TeV
System: p-p, Pb-Pb

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, 13.6 TeV
System: p-p, 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, 13.6 TeV
System: p-p, 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, 13.6 TeV
System: p-p, 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

$\Xi_{\mathrm{c}}^{0}\rightarrow \pi^{+}\Xi^{-}$ production in Pb–Pb collisions at $\sqrt{s_{\rm {NN}}}=5.02~TeV$

$\Xi_{\mathrm{c}}^{0}/\Lambda_{\mathrm{c}}^{+}$ 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

Lambda longitudinal polarization in Run 3 OO collisions at 5.36 TeV

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, Pb-Pb

[Light-Ion-Workshop 2025] Nuclear Modification of Neutral Pions in OO

ROO of Neutral Pions - Comparison to CMS

Fig. Group : [Light-Ion-Workshop 2025] Nuclear Modification of Neutral Pions in OO
PWG : PWG-EM (Electromagnetic probes)
Energy: 2.76 TeV, 5.36 TeV
System: O-O, Pb-Pb

ROO of Neutral Pions - Comparison to nPDF Predictions

Fig. Group : [Light-Ion-Workshop 2025] Nuclear Modification of Neutral Pions in OO
PWG : PWG-EM (Electromagnetic probes)
Energy: 5.36 TeV
System: O-O

ROO of Neutral Pions - Comparison to Energy Loss Prediction: Collisional + Radiative

Fig. Group : [Light-Ion-Workshop 2025] Nuclear Modification of Neutral Pions in OO
PWG : PWG-EM (Electromagnetic probes)
Energy: 5.36 TeV
System: O-O

ROO of Neutral Pions - Comparison to Energy Loss Prediction: Light Cone Path Integral

Fig. Group : [Light-Ion-Workshop 2025] Nuclear Modification of Neutral Pions in OO
PWG : PWG-EM (Electromagnetic probes)
Energy: 5.36 TeV
System: O-O

ROO of Neutral Pions - Comparison to Energy Loss Prediction: Simple Model

Fig. Group : [Light-Ion-Workshop 2025] Nuclear Modification of Neutral Pions in OO
PWG : PWG-EM (Electromagnetic probes)
Energy: 5.36 TeV
System: O-O

ROO of Neutral Pions - Comparison to Energy Loss Prediction: Hybrid Coupling Approach

Fig. Group : [Light-Ion-Workshop 2025] Nuclear Modification of Neutral Pions in OO
PWG : PWG-EM (Electromagnetic probes)
Energy: 5.36 TeV
System: O-O

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