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ID number ALI-PREL-XXX

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Scope: PWG

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Fit to the invariant-mass distribution of prompt $\Lambda_\text{c}$ in the $8<p_\text{T}<10 \text{GeV}/c$ interval and $<\text{d}N_\text{ch}/\text{d}\eta> = 4.34$ in pp collisions at $\sqrt s = 13.6 \text{TeV}$ Fig. Group : Measurement of the Lc cross section (integrated and vs multiplicity) in pp collisions at 13.6 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
Fit to the invariant-mass distribution of prompt $\Lambda_\text{c}$ in the $4<p_\text{T}<5 \text{GeV}/c$ interval and $<\text{d}N_\text{ch}/\text{d}\eta> = 20.07$ in pp collisions at $\sqrt s = 13.6 \text{TeV}$ Fig. Group : Measurement of the Lc cross section (integrated and vs multiplicity) in pp collisions at 13.6 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
Ratio of $\Lambda_\text{c}$-to-$\text{D}^0$ cross section, pp collisions at $\sqrt s = 13.6 \text{TeV}$ Fig. Group : Measurement of the Lc cross section (integrated and vs multiplicity) in pp collisions at 13.6 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
Prompt $\Lambda_\text{c}$ cross section, pp collisions at $\sqrt s = 13.6 \text{TeV}$ Fig. Group : Measurement of the Lc cross section (integrated and vs multiplicity) in pp collisions at 13.6 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
$\mathrm{D_s^+/D^+}$ production yield ratio measured in pp collisions at $\sqrt{s}=13.6$ TeV compared to forward-rapidity measurements by LHCb in $\mathrm{p-Pb}$ collisions and ALICE measurements in $\mathrm{Pb-Pb}$ collisions Fig. Group : $\mathrm{D_s^+/D^+}$ production yield ratio in pp collisions at $\sqrt{s}=13.6$ TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
Acceptance$\times$Efficiency correction for prompt $\mathrm{D_s^+}$ and $\mathrm{D^+}$ mesons as a function of FT0M percentile and $\pt$ in pp collisions at $\sqrt{s}=13.6$ TeV Fig. Group : $\mathrm{D_s^+/D^+}$ production yield ratio in pp collisions at $\sqrt{s}=13.6$ TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
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 with the cut-variation method Fig. Group : $\mathrm{D_s^+/D^+}$ production yield ratio in pp collisions at $\sqrt{s}=13.6$ TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
Fit to the invariant-mass distribution of $\mathrm{D_s^+}$ and $\mathrm{D^+}$ mesons in the $8< \pt <12$ GeV/$c$ interval and the $70-100\%$ FT0M percentile in pp collisions at $\sqrt{s}=13.6$ TeV Fig. Group : $\mathrm{D_s^+/D^+}$ production yield ratio in pp collisions at $\sqrt{s}=13.6$ TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
Fit to the invariant-mass distribution of $\mathrm{D_s^+}$ and $\mathrm{D^+}$ mesons in the $8< \pt <12$ GeV/$c$ interval and the $0-1\%$ FT0M percentile in pp collisions at $\sqrt{s}=13.6$ TeV Fig. Group : $\mathrm{D_s^+/D^+}$ production yield ratio in pp collisions at $\sqrt{s}=13.6$ TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
Fit to the invariant-mass distribution of $\mathrm{D_s^+}$ and $\mathrm{D^+}$ mesons in the $2< \pt <4$ GeV/$c$ interval and the $70-100\%$ FT0M percentile in pp collisions at $\sqrt{s}=13.6$ TeV Fig. Group : $\mathrm{D_s^+/D^+}$ production yield ratio in pp collisions at $\sqrt{s}=13.6$ TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
Fit to the invariant-mass distribution of $\mathrm{D_s^+}$ and $\mathrm{D^+}$ mesons in the $2< \pt <4$ GeV/$c$ interval and the $0-1\%$ FT0M percentile in pp collisions at $\sqrt{s}=13.6$ TeV Fig. Group : $\mathrm{D_s^+/D^+}$ production yield ratio in pp collisions at $\sqrt{s}=13.6$ TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
Comparison of the $\Omega^{-}$ baryons DCA_{z} distribution with and without the strangeness tracking Fig. Group : Measurement of the non-prompt $\Omega^{-}$ in pp collisions at $\sqrt{s}$ = 13.6 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
Comparison of the $\Omega^{-}$ baryons DCA_{xy} distribution with and without the strangeness tracking Fig. Group : Measurement of the non-prompt $\Omega^{-}$ in pp collisions at $\sqrt{s}$ = 13.6 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
DCA_{z} resolution of $\Omega^{-}$ baryons with and without the strangeness tracking Fig. Group : Measurement of the non-prompt $\Omega^{-}$ in pp collisions at $\sqrt{s}$ = 13.6 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
DCA_{xy} resolution of $\Omega^{-}$ baryons with and without the strangeness tracking Fig. Group : Measurement of the non-prompt $\Omega^{-}$ 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 strangeness tracked $\Omega^{-}$ baryons Fig. Group : Measurement of the non-prompt $\Omega^{-}$ in pp collisions at $\sqrt{s}$ = 13.6 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
$\Omega^{-}$ DCA$_{z}$ fit with MC model in the interval 1.6 $\leq$ $p_{\mathrm{T}}$ < 2.0 GeV/c Fig. Group : Measurement of the non-prompt $\Omega^{-}$ in pp collisions at $\sqrt{s}$ = 13.6 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
$\Omega^{-}$ DCA$_{xy}$ fit with MC model in the interval 1.6 $\leq$ $p_{\mathrm{T}}$ < 2.0 GeV/c Fig. Group : Measurement of the non-prompt $\Omega^{-}$ in pp collisions at $\sqrt{s}$ = 13.6 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
Prompt $\Omega^{-}$ fraction as a function of $p_\mathrm{T}$ Fig. Group : Measurement of the non-prompt $\Omega^{-}$ in pp collisions at $\sqrt{s}$ = 13.6 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
Comparison between of Ds+-h and D+h measurement away-side observables in differential pT bins of D meson and associated particles 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 of Ds+-h and D+h measurement near-side observables in differential pT bins of D meson and associated particles 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 of near-side observables with PYTHIA 8 predictions in differential pT bins of Ds+ meson and associated particles 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 of away-side observables with PYTHIA 8 predictions in differential pT bins of Ds+ meson and associated particles 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 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
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+/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
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
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
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 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
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
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
pi spectra inclusive, jet+UE, UE Fig. Group : pi, K, p in jets in 0-10% Pb-Pb and pp 5.02 TeV Preliminary PWG : PWG-JE (Jets) Energy: 5.02 TeV System Pb-Pb
pi spectra inclusive and jet+UE Fig. Group : pi, K, p in jets in 0-10% Pb-Pb and pp 5.02 TeV Preliminary PWG : PWG-JE (Jets) Energy: 5.02 TeV System Pb-Pb
pi spectra inclusive only Fig. Group : pi, K, p in jets in 0-10% Pb-Pb and pp 5.02 TeV Preliminary PWG : PWG-JE (Jets) Energy: 5.02 TeV System Pb-Pb
p/pi in jets all 5 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 all 5 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
p in jets spectra Fig. Group : pi, K, p in jets in 0-10% Pb-Pb and pp 5.02 TeV Preliminary PWG : PWG-JE (Jets) Energy: 5.02 TeV System Pb-Pb
K in jets spectra Fig. Group : pi, K, p in jets in 0-10% Pb-Pb and pp 5.02 TeV Preliminary PWG : PWG-JE (Jets) Energy: 5.02 TeV System Pb-Pb
pi in jets spectra - all four 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
nSD of D0-tagged jets in pp at 13.6 TeV for jet pT 15-30 GeV/c compared with Run 2 results Fig. Group : Substructure of charm-tagged jets in pp collisions at 13.6 TeV PWG : PWG-JE (Jets) Energy: 13.6 TeV System p-p
Rg of D0-tagged jets in pp at 13.6 TeV for jet pT 15-30 GeV/c compared with Run 2 results Fig. Group : Substructure of charm-tagged jets in pp collisions at 13.6 TeV PWG : PWG-JE (Jets) Energy: 13.6 TeV System p-p
nSD of D0-tagged jets in pp at 13.6 TeV for jet pT 30-50 GeV/c Fig. Group : Substructure of charm-tagged jets in pp collisions at 13.6 TeV PWG : PWG-JE (Jets) Energy: 13.6 TeV System p-p
nSD of D0-tagged jets in pp at 13.6 TeV for jet pT 15-30 GeV/c Fig. Group : Substructure of charm-tagged jets in pp collisions at 13.6 TeV PWG : PWG-JE (Jets) Energy: 13.6 TeV System p-p
Rg of D0-tagged jets in pp at 13.6 TeV for jet pT 30-50 GeV/c Fig. Group : Substructure of charm-tagged jets in pp collisions at 13.6 TeV PWG : PWG-JE (Jets) Energy: 13.6 TeV System p-p
Rg of D0-tagged jets in pp at 13.6 TeV for jet pT 15-30 GeV/c Fig. Group : Substructure of charm-tagged jets in pp collisions at 13.6 TeV PWG : PWG-JE (Jets) Energy: 13.6 TeV System p-p
nSD of D0-tagged jets in pp at 13.6 TeV compared with Run 2 results Fig. Group : Substructure of charm-tagged jets in pp collisions at 13.6 TeV PWG : PWG-JE (Jets) Energy: 13.6 TeV System p-p
nSD of D0-tagged jets in pp at 13.6 TeV Fig. Group : Substructure of charm-tagged jets in pp collisions at 13.6 TeV PWG : PWG-JE (Jets) Energy: 13.6 TeV System p-p
Rg of D0-tagged jets in pp at 13.6 TeV compared with Run 2 results Fig. Group : Substructure of charm-tagged jets in pp collisions at 13.6 TeV PWG : PWG-JE (Jets) Energy: 13.6 TeV System p-p
Rg of D0-tagged jets in pp at 13.6 TeV Fig. Group : Substructure of charm-tagged jets in pp collisions at 13.6 TeV PWG : PWG-JE (Jets) Energy: 13.6 TeV System p-p
Ratio of EEC distributions for charged jets in pp and p-Pb collisions -- 20-40 GeV/c with HT calculation 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 model+nPDF bands 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
zg of D0-tagged jets in pp at 13.6 TeV for jet pT 15-30 GeV/c compared with Run 2 results Fig. Group : Substructure of charm-tagged jets in pp collisions at 13.6 TeV PWG : PWG-JE (Jets) Energy: 13.6 TeV System p-p
$\Lambda_{\text{c}}^{+}$ fragmentation function in pp at 13.6 TeV compared with Run 2 results Fig. Group : Substructure of charm-tagged jets in pp collisions at 13.6 TeV PWG : PWG-JE (Jets) Energy: 13.6 TeV System p-p
zg of D0-tagged jets in pp at 13.6 TeV for jet pT 30-50 GeV/c Fig. Group : Substructure of charm-tagged jets in pp collisions at 13.6 TeV PWG : PWG-JE (Jets) Energy: 13.6 TeV System p-p
zg of D0-tagged jets in pp at 13.6 TeV for jet pT 15-30 GeV/c Fig. Group : Substructure of charm-tagged jets in pp collisions at 13.6 TeV PWG : PWG-JE (Jets) Energy: 13.6 TeV System p-p
zg of D0-tagged jets in pp at 13.6 TeV compared with Run 2 results Fig. Group : Substructure of charm-tagged jets in pp collisions at 13.6 TeV PWG : PWG-JE (Jets) Energy: 13.6 TeV System p-p

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