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ID number ALI-PREL-XXX

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Scope: PWG

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Compilation of All Available Non-Strange Nuclear Modification Factors ROO - Linear pT Axis Fig. Group : Preliminary/Derived Figures: Evidence for parton energy loss in oxygen$-$oxygen collisions at $\mathbf{\sqrt{s_{\rm NN}}=5.36}$ TeV PWG : PWG-EM (Electromagnetic probes) Energy: 5.36 TeV System O-O , System p-p
Compilation of All Available Nuclear Modification Factors ROO - Linear pT Axis Fig. Group : Preliminary/Derived Figures: Evidence for parton energy loss in oxygen$-$oxygen collisions at $\mathbf{\sqrt{s_{\rm NN}}=5.36}$ TeV PWG : PWG-EM (Electromagnetic probes) Energy: 5.36 TeV System O-O , System p-p
Compilation of All Available Identified Particle Nuclear Modification Factors ROO Fig. Group : Preliminary/Derived Figures: Evidence for parton energy loss in oxygen$-$oxygen collisions at $\mathbf{\sqrt{s_{\rm NN}}=5.36}$ TeV PWG : PWG-EM (Electromagnetic probes) Energy: 5.36 TeV System O-O , System p-p
Compilation of All Available Non-Strange Nuclear Modification Factors ROO Fig. Group : Preliminary/Derived Figures: Evidence for parton energy loss in oxygen$-$oxygen collisions at $\mathbf{\sqrt{s_{\rm NN}}=5.36}$ TeV PWG : PWG-EM (Electromagnetic probes) Energy: 5.36 TeV System O-O , System p-p
Compilation of All Available Nuclear Modification Factors ROO Fig. Group : Preliminary/Derived Figures: Evidence for parton energy loss in oxygen$-$oxygen collisions at $\mathbf{\sqrt{s_{\rm NN}}=5.36}$ TeV PWG : PWG-EM (Electromagnetic probes) Energy: 5.36 TeV System O-O , System p-p
Ds-h azimuthal correlation away-side IAA Fig. Group : $D^{+}_{s}$-hadron azimuthal correlations in OO collisions at $\sqrt{s}$=5.36 TeV PWG : PWG-HF (Heavy Flavour) Energy: 5.36 TeV System O-O
Ds-h azimuthal correlation near-side IAA Fig. Group : $D^{+}_{s}$-hadron azimuthal correlations in OO collisions at $\sqrt{s}$=5.36 TeV PWG : PWG-HF (Heavy Flavour) Energy: 5.36 TeV System O-O
Ds-h azimuthal correlation near-side width comparison between pp and OO collisions Fig. Group : $D^{+}_{s}$-hadron azimuthal correlations in OO collisions at $\sqrt{s}$=5.36 TeV PWG : PWG-HF (Heavy Flavour) Energy: 5.36 TeV System O-O
Ds-h azimuthal correlation away-side width comparison between pp and OO collisions Fig. Group : $D^{+}_{s}$-hadron azimuthal correlations in OO collisions at $\sqrt{s}$=5.36 TeV PWG : PWG-HF (Heavy Flavour) Energy: 5.36 TeV System O-O
Ds-h azimuthal correlation away-side yield comparison between pp and OO collisions Fig. Group : $D^{+}_{s}$-hadron azimuthal correlations in OO collisions at $\sqrt{s}$=5.36 TeV PWG : PWG-HF (Heavy Flavour) Energy: 5.36 TeV System O-O
Ds-h azimuthal correlation near-side yield comparison between pp and OO collisions Fig. Group : $D^{+}_{s}$-hadron azimuthal correlations in OO collisions at $\sqrt{s}$=5.36 TeV PWG : PWG-HF (Heavy Flavour) Energy: 5.36 TeV System O-O
Ds-h azimuthal correlation distribution comparison between pp and OO collisions (5 < $p_{T}$ < 8 GeV/c) Fig. Group : $D^{+}_{s}$-hadron azimuthal correlations in OO collisions at $\sqrt{s}$=5.36 TeV PWG : PWG-HF (Heavy Flavour) Energy: 5.36 TeV System O-O
Opposite-baryon and same-baryon $\Sigma_{\rm c}^{0}\text{--p}$ azimuthal correlations for $4 < p_{\mathrm{T}}(\Sigma_{\rm c}^{0}) < 12$ GeV/$c$ and $0.4 < p_{\mathrm{T}}(\text{p}) < 4.5$ GeV/$c$ compared with models Fig. Group : $\Sigma_{c}^{++,0}$ -- proton azimuthal correlations in pp collisions at $\sqrt{s} = 13.6$ TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
Opposite-baryon and same-baryon $\Sigma_{\rm c}^{++}\text{--p}$ azimuthal correlations for $4 < p_{\mathrm{T}}(\Sigma_{\rm c}^{++}) < 12$ GeV/$c$ and $0.4 < p_{\mathrm{T}}(\text{p}) < 4.5$ GeV/$c$ compared with models Fig. Group : $\Sigma_{c}^{++,0}$ -- proton azimuthal correlations in pp collisions at $\sqrt{s} = 13.6$ TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
Opposite-baryon$-$ same-baryon $\Sigma_{\rm c}^{++}\text{--p}$ azimuthal correlations for $4 < p_{\mathrm{T}}(\Sigma_{\rm c}^{++}) < 12$ GeV/$c$ and $0.4 < p_{\mathrm{T}}(\text{p}) < 4.5$ GeV/$c$ compared with models Fig. Group : $\Sigma_{c}^{++,0}$ -- proton azimuthal correlations in pp collisions at $\sqrt{s} = 13.6$ TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
Opposite baryon $-$ same-baryon $\Sigma_{\rm c}^{0}\text{--p}$ azimuthal correlations for $4 < p_{\mathrm{T}}(\Sigma_{\rm c}^{0}) < 12$ GeV/$c$ and $0.4 < p_{\mathrm{T}}(\text{p}) < 4.5$ GeV/$c$ compared with models Fig. Group : $\Sigma_{c}^{++,0}$ -- 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 associated $\Sigma_{\rm c}^{++}\text{--p}$ over $\Sigma_{\rm c}^{0}\text{--p}$ yield for $4 < p_{\mathrm{T}}(\Sigma_{\rm c}^{0, ++}) < 12$ GeV/$c$ and $0.4 < p_{\mathrm{T}}(\text{p}) < 4.5$ GeV/$c$ compared with models Fig. Group : $\Sigma_{c}^{++,0}$ -- 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 associated near-side $\Sigma_{\rm c}^{++}\text{--p}$ over $\Sigma_{\rm c}^{0}\text{--p}$ yield for $4 < p_{\mathrm{T}}(\Sigma_{\rm c}^{0, ++}) < 12$ GeV/$c$ and $0.4 < p_{\mathrm{T}}(\text{p}) < 4.5$ GeV/$c$ compared with models Fig. Group : $\Sigma_{c}^{++,0}$ -- 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 associated away-side $\Sigma_{\rm c}^{++}\text{--p}$ over $\Sigma_{\rm c}^{0}\text{--p}$ yield for $4 < p_{\mathrm{T}}(\Sigma_{\rm c}^{0, ++}) < 12$ GeV/$c$ and $0.4 < p_{\mathrm{T}}(\text{p}) < 4.5$ GeV/$c$ compared with models Fig. Group : $\Sigma_{c}^{++,0}$ -- 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 $\Delta\varphi$ $\Sigma_{\rm c}^{0, ++}$-p yield in $p_{\mathrm{T}}^{\Sigma_{\rm c}^{0, ++}} 4$-$12$ GeV/$c$ and $p_{\mathrm{T}}^{p} 0.4$-$4.5$ GeV/$c$ with models Fig. Group : $\Sigma_{c}^{++,0}$ -- 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 $\Delta\varphi$ $\Sigma_{\rm c}^{0, ++}$-p yield in $p_{\mathrm{T}}^{\Sigma_{\rm c}^{0, ++}} 4$-$12$ GeV/$c$ and $p_{\mathrm{T}}^{p} 0.4$-$4.5$ GeV/$c$ with models Fig. Group : $\Sigma_{c}^{++,0}$ -- 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 $\Delta\varphi$ integrated $\Sigma_{\rm c}^{0, ++}$-p yield in $p_{\mathrm{T}}^{\Sigma_{\rm c}^{0, ++}} 4$-$12$ GeV/$c$ and $p_{\mathrm{T}}^{p} 0.4$-$4.5$ GeV/$c$ with models Fig. Group : $\Sigma_{c}^{++,0}$ -- proton azimuthal correlations in pp collisions at $\sqrt{s} = 13.6$ TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
*Overlay of prompt $D^{+}$ and $D^{0}$ cross sections in pp collisions at $\sqrt{s}$ = 13.6 TeV Fig. Group :** Minimum bias production of prompt D$^{+}$ in pp collision at $\sqrt{s} = 13.6$ TeV PWG :* PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
*Fit to the invariant-mass distribution of prompt $D^{+}$ in the $1.5 < p_{T} < 2 \text{GeV}/c$ interval, in pp collisions at $\sqrt{s}$ = 13.6 TeV Fig. Group :** Minimum bias production of prompt D$^{+}$ in pp collision at $\sqrt{s} = 13.6$ TeV PWG :* PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
*$D^{+}/D^{0}$ ratio in pp collisions at $\sqrt{s}$ = 13.6 TeV Fig. Group :** Minimum bias production of prompt D$^{+}$ in pp collision at $\sqrt{s} = 13.6$ TeV PWG :* PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
*Prompt $D^{+}$ cross section in pp collisions at $\sqrt{s}$ = 13.6 TeV compared with FONLL Fig. Group :** Minimum bias production of prompt D$^{+}$ in pp collision at $\sqrt{s} = 13.6$ TeV PWG :* PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
*Prompt $D^{+}$ cross section in pp collisions at $\sqrt{s}$ = 13.6 TeV compared with Run 2 measurement Fig. Group :** Minimum bias production of prompt D$^{+}$ in pp collision at $\sqrt{s} = 13.6$ TeV PWG :* PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
Raw yield of Xic0 in pT bin [5, 6] GeV/c for the 0–100% FT0M, 0>INEL Fig. Group : Xic0 self-normalized yield in pp collisions at 13.6 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-O , System p-p
Raw yield of Xic0 in pT bin [5, 6] GeV/c for the 70–100% FT0M multiplicity class Fig. Group : Xic0 self-normalized yield in pp collisions at 13.6 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13 TeV , Energy: 13.6 TeV System p-p
Xic0 self-normalized yields in pp collisions at 13.6 TeV compare with EPOS4HQ Fig. Group : Xic0 self-normalized yield in pp collisions at 13.6 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
Xic0 self-normalized yields in pp collisions at 13.6 TeV compare with Pythia Fig. Group : Xic0 self-normalized yield in pp collisions at 13.6 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p , System p-Pb
Xic0 self-normalized yields in pp collisions at 13.6 TeV Fig. Group : Xic0 self-normalized yield in pp collisions at 13.6 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
Spectrum of omega measured in the dielectron channel Fig. Group : [HP2026] Soft omega prodution in pp collisions at 5.02 TeV PWG : PWG-EM (Electromagnetic probes) Energy: 5.02 TeV System p-p
Ratio of omega/pi as a function of pT Fig. Group : [HP2026] Soft omega prodution in pp collisions at 5.02 TeV PWG : PWG-EM (Electromagnetic probes) Energy: 5.02 TeV System p-p
mean pt of omega and other particles vs mass Fig. Group : [HP2026] Soft omega prodution in pp collisions at 5.02 TeV PWG : PWG-EM (Electromagnetic probes) Energy: 5.02 TeV System p-p
Integrated omega/pi ratio with models Fig. Group : [HP2026] Soft omega prodution in pp collisions at 5.02 TeV PWG : PWG-EM (Electromagnetic probes) Energy: 5.02 TeV System p-p
$\rho_{00}$ of prompt $\mathrm{D}^{+}$ in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.36 TeV, compared to previous measurement of $\mathrm{D}^{+}$ and inclusive $J/\psi$ at $\sqrt{s_{\mathrm{NN}}}$ = 5.02TeV Fig. Group : Measurement spin alignment of prompt $\mathrm{D}^{+}$ mesons in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.36 TeV PWG :* PWG-HF (Heavy Flavour) Energy: 5.36 TeV System Pb-Pb
*$\rho_{00}$ of prompt $\mathrm{D}^{+}$ in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.36 TeV, compared with previous measurement at $\sqrt{s_{\mathrm{NN}}}$ = 5.02TeV Fig. Group :** Measurement spin alignment of prompt $\mathrm{D}^{+}$ mesons in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.36 TeV PWG :* PWG-HF (Heavy Flavour) Energy: 5.36 TeV System Pb-Pb
*$\rho_{00}$ of prompt $\mathrm{D}^{+}$ in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.36 TeV Fig. Group :** Measurement spin alignment of prompt $\mathrm{D}^{+}$ mesons 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 of corrected $\mathrm{D}^{+}$ mesons yield as a function of $cos\theta^$ in Pb-Pb collisions with two $p_\mathrm{T}$ intervals* Fig. Group : Measurement spin alignment of prompt $\mathrm{D}^{+}$ mesons in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.36 TeV PWG :* PWG-HF (Heavy Flavour) Energy: 5.36 TeV System Pb-Pb
*Raw yield as a function of BDT selections and extracted contributions from prompt and non-prompt $\mathrm{D}^{+}$ mesons with $15<p_\mathrm{T}<30~\mathrm{GeV}/c$ Fig. Group :** Measurement spin alignment of prompt $\mathrm{D}^{+}$ mesons in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.36 TeV PWG :* PWG-HF (Heavy Flavour) Energy: 5.36 TeV System Pb-Pb
Invariant mass distribution in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.36 TeV in two intervals of $p_\mathrm{T}$ Fig. Group : Measurement spin alignment of prompt $\mathrm{D}^{+}$ mesons in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.36 TeV PWG :* PWG-HF (Heavy Flavour) Energy: 5.36 TeV System Pb-Pb
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
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
Non-prompt $\psi$(2S) and J/$\psi$ 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
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
Ds-meson invariant mass distribution (3 < $p_{T}$ < 5GeV/c) Fig. Group : $D^{+}_{s}$-hadron azimuthal correlations in OO collisions at $\sqrt{s}$=5.36 TeV PWG : PWG-HF (Heavy Flavour) Energy: 5.36 TeV System O-O
Ds-h azimuthal correlation distribution (16 < $p_{T}$ < 36 GeV/c) Fig. Group : $D^{+}_{s}$-hadron azimuthal correlations in OO collisions at $\sqrt{s}$=5.36 TeV PWG : PWG-HF (Heavy Flavour) Energy: 5.36 TeV System O-O
Ds-h azimuthal correlation distribution (8 < $p_{T}$ < 16 GeV/c) Fig. Group : $D^{+}_{s}$-hadron azimuthal correlations in OO collisions at $\sqrt{s}$=5.36 TeV PWG : PWG-HF (Heavy Flavour) Energy: 5.36 TeV System O-O
Ds-h azimuthal correlation distribution (5 < $p_{T}$ < 8 GeV/c) Fig. Group : $D^{+}_{s}$-hadron azimuthal correlations in OO collisions at $\sqrt{s}$=5.36 TeV PWG : PWG-HF (Heavy Flavour) Energy: 5.36 TeV System O-O
Ds-h azimuthal correlation distribution (3 < $p_{T}$ < 5 GeV/c) Fig. Group : $D^{+}_{s}$-hadron azimuthal correlations in OO collisions at $\sqrt{s}$=5.36 TeV PWG : PWG-HF (Heavy Flavour) Energy: 5.36 TeV System O-O
Ds-h azimuthal correlation distribution (1 < $p_{T}$ < 3 GeV/c) Fig. Group : $D^{+}_{s}$-hadron azimuthal correlations in OO collisions at $\sqrt{s}$=5.36 TeV PWG : PWG-HF (Heavy Flavour) Energy: 5.36 TeV System O-O
Ds-h ($\Delta\phi,\Delta\eta$) angular correlation distribution (8 < $p_{T}$ < 16 GeV/c) Fig. Group : $D^{+}_{s}$-hadron azimuthal correlations in OO collisions at $\sqrt{s}$=5.36 TeV PWG : PWG-HF (Heavy Flavour) Energy: 5.36 TeV System O-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 System O-O , System Pb-Pb

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