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Pb-Pb and smeared pp p/pi comparison - without inclusive comparison Fig. Group : pi, K, p in jets in 0-10% Pb-Pb and pp 5.02 TeV Preliminary PWG : PWG-JE (Jets) Energy: 5.02 TeV System p-p , System Pb-Pb
Pb-Pb and smeared pp K/pi comparison - without inclusive comparison Fig. Group : pi, K, p in jets in 0-10% Pb-Pb and pp 5.02 TeV Preliminary PWG : PWG-JE (Jets) Energy: 5.02 TeV System p-p , System Pb-Pb
Pb-Pb and smeared pp p/pi comparison - with inclusive comparison Fig. Group : pi, K, p in jets in 0-10% Pb-Pb and pp 5.02 TeV Preliminary PWG : PWG-JE (Jets) Energy: 5.02 TeV System p-p , System Pb-Pb
Pb-Pb and smeared pp K/pi comparison - with inclusive comparison Fig. Group : pi, K, p in jets in 0-10% Pb-Pb and pp 5.02 TeV Preliminary PWG : PWG-JE (Jets) Energy: 5.02 TeV System p-p , System Pb-Pb
Pb-Pb and smeared pp p spectra comparison Fig. Group : pi, K, p in jets in 0-10% Pb-Pb and pp 5.02 TeV Preliminary PWG : PWG-JE (Jets) Energy: 5.02 TeV System p-p , System Pb-Pb
Pb-Pb and smeared pp K spectra comparison Fig. Group : pi, K, p in jets in 0-10% Pb-Pb and pp 5.02 TeV Preliminary PWG : PWG-JE (Jets) Energy: 5.02 TeV System p-p , System Pb-Pb
Pb-Pb and smeared pp pi spectra comparison Fig. Group : pi, K, p in jets in 0-10% Pb-Pb and pp 5.02 TeV Preliminary PWG : PWG-JE (Jets) Energy: 5.02 TeV System p-p , System Pb-Pb
Standalone pp 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 p-p
Standalone pp 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 p-p
Standalone pp p/pi in jets - all 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 p-p
Standalone pp K/pi in jets - all 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 p-p
Standalone pp pi in jets spectra - inclusive, jet+UE, and UE 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 p-p
Standalone pp pi in jets 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 p-p
Standalone pp pi in jets 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 p-p
Standalone pp 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 p-p
Standalone pp 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 p-p , System Pb-Pb
Standalone pp pi in jets spectra - all 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 p-p
Charged jet EEC in PbPb and pp (compared with models) in 40-60 GeV Fig. Group : Charged jet EEC measurements in PbPb at 5.02 TeV PWG : PWG-JE (Jets) Energy: 5.02 TeV System Pb-Pb
Charged jet EEC in PbPb and pp (compared with models) in 60-80 GeV Fig. Group : Charged jet EEC measurements in PbPb at 5.02 TeV PWG : PWG-JE (Jets) Energy: 5.02 TeV System Pb-Pb
Charged jet EEC in PbPb and pp (compared with models) in 80-100 GeV Fig. Group : Charged jet EEC measurements in PbPb at 5.02 TeV PWG : PWG-JE (Jets) Energy: 5.02 TeV System Pb-Pb
Charged jet EEC in PbPb and pp (compared with Hybrid) in 40-60 GeV Fig. Group : Charged jet EEC measurements in PbPb at 5.02 TeV PWG : PWG-JE (Jets) Energy: 5.02 TeV System Pb-Pb
Charged jet EEC in PbPb Fig. Group : Charged jet EEC measurements in PbPb at 5.02 TeV PWG : PWG-JE (Jets) Energy: 5.02 TeV System Pb-Pb
Charged jet EEC in PbPb (pT scaled) Fig. Group : Charged jet EEC measurements in PbPb at 5.02 TeV PWG : PWG-JE (Jets) Energy: 5.02 TeV System Pb-Pb
Charged jet EEC in PbPb and pp (compared with models) in 100-120 GeV Fig. Group : Charged jet EEC measurements in PbPb at 5.02 TeV PWG : PWG-JE (Jets) Energy: 5.02 TeV System Pb-Pb
Charged jet EEC in PbPb and pp (including Pythia and Herwig) in 80-100 GeV Fig. Group : Charged jet EEC measurements in PbPb at 5.02 TeV PWG : PWG-JE (Jets) Energy: 5.02 TeV System Pb-Pb
Charged jet EEC in PbPb and pp (including Pythia and Herwig) in 100-120 GeV Fig. Group : Charged jet EEC measurements in PbPb at 5.02 TeV PWG : PWG-JE (Jets) Energy: 5.02 TeV System Pb-Pb
Charged jet EEC in PbPb and pp in 60-80 GeV Fig. Group : Charged jet EEC measurements in PbPb at 5.02 TeV PWG : PWG-JE (Jets) Energy: 5.02 TeV System Pb-Pb
Charged jet EEC in PbPb and pp (including Pythia and Herwig) in 40-60 GeV Fig. Group : Charged jet EEC measurements in PbPb at 5.02 TeV PWG : PWG-JE (Jets) Energy: 5.02 TeV System Pb-Pb
Charged jet EEC in PbPb and pp (including Pythia and Herwig) in 60-80 GeV Fig. Group : Charged jet EEC measurements in PbPb at 5.02 TeV PWG : PWG-JE (Jets) Energy: 5.02 TeV System Pb-Pb
Charged jet EEC in PbPb and pp (compared with Hybrid) in 100-120 GeV Fig. Group : Charged jet EEC measurements in PbPb at 5.02 TeV PWG : PWG-JE (Jets) Energy: 5.02 TeV System Pb-Pb
Charged jet EEC in PbPb and pp (compared with Hybrid) in 80-100 GeV Fig. Group : Charged jet EEC measurements in PbPb at 5.02 TeV PWG : PWG-JE (Jets) Energy: 5.02 TeV System Pb-Pb
Charged jet EEC in PbPb and pp (compared with Hybrid) in 60-80 GeV Fig. Group : Charged jet EEC measurements in PbPb at 5.02 TeV PWG : PWG-JE (Jets) Energy: 5.02 TeV System Pb-Pb
Charged jet EEC in PbPb and pp in 100-120 GeV Fig. Group : Charged jet EEC measurements in PbPb at 5.02 TeV PWG : PWG-JE (Jets) Energy: 5.02 TeV System Pb-Pb
Charged jet EEC in PbPb and pp in 80-100 GeV Fig. Group : Charged jet EEC measurements in PbPb at 5.02 TeV PWG : PWG-JE (Jets) Energy: 5.02 TeV System Pb-Pb
Charged jet EEC in PbPb and pp in 40-60 GeV Fig. Group : Charged jet EEC measurements in PbPb at 5.02 TeV PWG : PWG-JE (Jets) Energy: 5.02 TeV System Pb-Pb
E3C/EEC at 5.02 TeV Fig. Group : E3C and EEC measurements in jets in pp collisions at 5.02 and 13TeV PWG : PWG-JE (Jets) Energy: 5.02 TeV System p-p
E3C (per jet normalized) at 5.02 TeV Fig. Group : E3C and EEC measurements in jets in pp collisions at 5.02 and 13TeV PWG : PWG-JE (Jets) Energy: 5.02 TeV System p-p
EEC (per jet normalized) at 5.02 TeV Fig. Group : E3C and EEC measurements in jets in pp collisions at 5.02 and 13TeV PWG : PWG-JE (Jets) Energy: 5.02 TeV System p-p
$\mathrm{D_s^+/D^+}$ production yield ratio measured in pp collisions at $\sqrt{s}=13.6$ TeV compared to ALICE measurements in $\mathrm{Pb-Pb}$ collisions and PYTHIA 8 and EPOS4HQ predictions 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
Dijet invariant mass spectrum for pp and p-Pb including R_{pA} at 5.02 TeV with PYTHIA and POWHEG+PYTHIA comparisons Fig. Group : Dijet Invariant mass analysis PWG : PWG-JE (Jets) Energy: 5.02 TeV System p-p , System p-Pb
Dijet invariant mass spectrum for pp and p-Pb including R_{pA} at 5.02 TeV Fig. Group : Dijet Invariant mass analysis PWG : PWG-JE (Jets) Energy: 5.02 TeV System p-p , System p-Pb
J/ψ v2{SP} vs pT at forward rapidity in the dimuon channel for the centrality class 10-30% and at 5.36 TeV compared to Run 2 Fig. Group : Jpsi v2 in Pb-Pb collisions at 5.36 TeV at fwd rapidity PWG : PWG-DQ (Dileptons and Quarkonia) Energy: 5.36 TeV System Pb-Pb
Ratio of high-mult/low-mult EECs in p-Pb (20-40 GeV/c) 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 backward/forward EECs in p-Pb (20-40 GeV/c) 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
Ratios of prompt $\Lambda_\text{c}$ corrected yields between different multiplicity intervals and the multiplicity integrated class, 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
Like-sign and Unlike-sign $\Lambda_{c}$-p Azimuthal Correlations in $p_{\mathrm{T}}^{\Lambda_{c}} 3$-$5$ GeV/$c$ and $p_{\mathrm{T}}^{p} 1$-$2.5$ GeV/$c$ 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 $p_{\mathrm{T}}^{p} 1$-$2.5$ GeV/$c$ 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 $p_{\mathrm{T}}^{p} 0.4$-$1$ GeV/$c$ 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/$c$ 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
$\Lambda_{c}^{+}$ -- proton azimuthal correlations in pp collisions at $\sqrt{s} = 13.6$ TeV 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
Ratio of the integrated cross section of single D⁰ mesons over D⁰D⁰ and D⁰D⁰bar pairs Fig. Group : Associated production of D⁰D⁰ and D⁰D⁰bar pairs 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 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
integrated cross section of D⁰D⁰ and D⁰D⁰bar pairs Fig. Group : Associated production of D⁰D⁰ and D⁰D⁰bar pairs in pp collisions at 13.6 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
Distribution of the $\|\Delta\varphi\|$ of D⁰D⁰ pairs Fig. Group : Associated production of D⁰D⁰ and D⁰D⁰bar pairs in pp collisions at 13.6 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
2D distribution of the $p_\rm{T}$ of D⁰D⁰ pairs vs. $\Delta \varphi$ Fig. Group : Associated production of D⁰D⁰ and D⁰D⁰bar pairs in pp collisions at 13.6 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
Acceptance multiplied by the efficiency vs. $p_\rm{T}$ vs. $y$ Fig. Group : Associated production of D⁰D⁰ and D⁰D⁰bar pairs in pp collisions at 13.6 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
Projection of the fit to the 2D invariant-mass distribution of D⁰D⁰bar pairs Fig. Group : Associated production of D⁰D⁰ and D⁰D⁰bar pairs in pp collisions at 13.6 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
Projection of the fit to the 2D invariant-mass distribution of D⁰D⁰ pairs Fig. Group : Associated production of D⁰D⁰ and D⁰D⁰bar pairs in pp collisions at 13.6 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
Fit to the 2D invariant-mass distribution of D⁰D⁰ pairs Fig. Group : Associated production of D⁰D⁰ and D⁰D⁰bar pairs in pp collisions at 13.6 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
Fit to the 2D invariant-mass distribution of D⁰D⁰bar pairs Fig. Group : Associated production of D⁰D⁰ and D⁰D⁰bar pairs in pp collisions at 13.6 TeV PWG : PWG-HF (Heavy Flavour) Energy: 13.6 TeV System p-p
Raw quasi-inclusive jet $p_\mathrm{T,jet}^\mathrm{reco}$ distribution for $R = 0.5$ of the SE and ME with $p_\mathrm{T}^\mathrm{lead} > 5$ GeV/c for central Pb-Pb collisions at 5.02 TeV Fig. Group : Measurement of inclusive jet distributions in central Pb-Pb collisions at 5.02 TeV with a novel mixed-event approach. PWG : PWG-JE (Jets) Energy: 5.02 TeV System Pb-Pb
Raw correlated quasi-inclusive jet $p_\mathrm{T,jet}^\mathrm{reco}$ distribution for $R = 0.5$ with $p_\mathrm{T}^\mathrm{lead} > 5$ GeV/c for central Pb-Pb collisions at 5.02 TeV Fig. Group : Measurement of inclusive jet distributions in central Pb-Pb collisions at 5.02 TeV with a novel mixed-event approach. PWG : PWG-JE (Jets) Energy: 5.02 TeV System Pb-Pb
Corrected charged particle jet distributions for $R = 0.5$ with $p_\mathrm{T}^\mathrm{lead} > 4$ GeV/c and $p_\mathrm{T}^\mathrm{lead} > 5$ GeV/c for central Pb-Pb collisions at 5.02 TeV Fig. Group : Measurement of inclusive jet distributions in central Pb-Pb collisions at 5.02 TeV with a novel mixed-event approach. PWG : PWG-JE (Jets) Energy: 5.02 TeV System Pb-Pb
Charged particle jet $R_{AA}$ for R = 0.5 measured in central Pb-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV Fig. Group : Measurement of inclusive jet distributions in central Pb-Pb collisions at 5.02 TeV with a novel mixed-event approach. PWG : PWG-JE (Jets) Energy: 5.02 TeV System Pb-Pb
Charged EECs in pp and p-Pb (ratio, 20-40 GeV) Fig. Group : Charged energy correlators in pp and p-Pb collisions at 5.02 TeV PWG : PWG-JE (Jets) Energy: 5.02 TeV System p-p , System p-Pb
Charged EECs in pp collisions (MC comparison, 60-80 GeV) Fig. Group : Charged energy correlators in pp and p-Pb collisions at 5.02 TeV PWG : PWG-JE (Jets) Energy: 5.02 TeV System p-p
Charged EECs in pp collisions (MC comparison, 40-60 GeV) Fig. Group : Charged energy correlators in pp and p-Pb collisions at 5.02 TeV PWG : PWG-JE (Jets) Energy: 5.02 TeV System p-p
Charged EECs in pp collisions (MC comparison, 20-40 GeV) Fig. Group : Charged energy correlators in pp and p-Pb collisions at 5.02 TeV PWG : PWG-JE (Jets) Energy: 5.02 TeV System p-p
Charged EECs in pPb collisions (jet pT comparison) Fig. Group : Charged energy correlators in pp and p-Pb collisions at 5.02 TeV PWG : PWG-JE (Jets) Energy: 5.02 TeV System p-Pb
Charged EECs in pp collisions (jet pT comparison) Fig. Group : Charged energy correlators in pp and p-Pb collisions at 5.02 TeV PWG : PWG-JE (Jets) Energy: 5.02 TeV System p-p
Distribution of rho background in signal and reference events Fig. Group : Measurement of the semi-inclusive hadron+jet distributions in pp collisions at √s = 13.6 TeV using Run 3 data PWG : PWG-JE (Jets) Energy: 5.36 TeV System Pb-Pb
Raw spectra of signal, reference and delta recoil vs pT for R=0.4 jets in Pb-Pb collisions Fig. Group : Measurement of the semi-inclusive hadron+jet distributions in pp collisions at √s = 13.6 TeV using Run 3 data PWG : PWG-JE (Jets) Energy: 5.36 TeV System Pb-Pb
Raw spectra of signal, reference and delta recoil vs delta phi for R=0.4 jets in Pb-Pb collisions Fig. Group : Measurement of the semi-inclusive hadron+jet distributions in pp collisions at √s = 13.6 TeV using Run 3 data PWG : PWG-JE (Jets) Energy: 5.36 TeV System Pb-Pb
Raw spectra of signal, reference and delta recoil vs delta r for R=0.4 jets in Pb-Pb collisions Fig. Group : Measurement of the semi-inclusive hadron+jet distributions in pp collisions at √s = 13.6 TeV using Run 3 data PWG : PWG-JE (Jets) Energy: 5.36 TeV System Pb-Pb
Raw spectra of signal, reference and delta recoil vs delta r for R=0.4 jets in pp collisions Fig. Group : Measurement of the semi-inclusive hadron+jet distributions in pp collisions at √s = 13.6 TeV using Run 3 data PWG : PWG-JE (Jets) Energy: 13.6 TeV System p-p
Raw spectra of signal, reference and delta recoil vs delta phi for R=0.4 jets in pp collisions Fig. Group : Measurement of the semi-inclusive hadron+jet distributions in pp collisions at √s = 13.6 TeV using Run 3 data PWG : PWG-JE (Jets) Energy: 13.6 TeV System p-p
Fit to the invariant-mass distribution of prompt $\Lambda_\text{c}$ in the $1<p_\text{T}<2\text{GeV}/c$ interval, multiplicity-integrated, 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 $8<p_\text{T}<10 \text{GeV}/c$ 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

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