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ID number ALI-PREL-XXX

Figure Caption

Scope: PWG

System

Energy

Xic multiplicity dependence via hadronic decay in proton-proton collisions at s√=13 TeV

Xic/Lc ratio measured in \pp collisions at 13TeV in different multiplicity

Fig. Group : Xic multiplicity dependence via hadronic decay in proton-proton collisions at s√=13 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13 TeV
System: p-p

Xi_c^0/D^0 ratio in different V0M multiplicity classes

Fig. Group : Xic multiplicity dependence via hadronic decay in proton-proton collisions at s√=13 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13 TeV
System: p-p

psi-to-jpsi analysis at midrapidity in pp at 13.6 TeV (QM2023)

psi and jpsi signal extraction from 13.6 TeV pp data

Fig. Group : psi-to-jpsi analysis at midrapidity in pp at 13.6 TeV (QM2023)
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 13.6 TeV
System: p-p

psi-to-jpsi ratio as function of the pT at midrapidity in pp at 13.6 TeV, compared with the similar measurements from forward rapidity

Fig. Group : psi-to-jpsi analysis at midrapidity in pp at 13.6 TeV (QM2023)
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 13.6 TeV
System: p-p

y-differential J/psi photoproduction in Pb-Pb (QM2023)

y-differential coherent J/psi photoproduction cross section at pT < 0.3 GeV/c in the centrality range (70-90)% in Pb-Pb collisions at 5.02 TeV with data points only

Fig. Group : y-differential J/psi photoproduction in Pb-Pb (QM2023)
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 5.02 TeV
System: Pb-Pb

y-differential raw J/psi yield as a function of pT in the centrality range (70-90)% in Pb-Pb collisions at 5.02 TeV

Fig. Group : y-differential J/psi photoproduction in Pb-Pb (QM2023)
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 5.02 TeV
System: Pb-Pb

y-differential J/psi production cross section at forward y as a function of pT in pp collisions at 5.02 TeV

Fig. Group : y-differential J/psi photoproduction in Pb-Pb (QM2023)
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 5.02 TeV
System: p-p

The J/psi nuclear modification factor as a function of pT in the centrality range (70-90)% in Pb-Pb collisions at 5.02 TeV for 3.75 < y < 4

Fig. Group : y-differential J/psi photoproduction in Pb-Pb (QM2023)
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 5.02 TeV
System: Pb-Pb

The J/psi nuclear modification factor as a function of pT in the centrality range (70-90)% in Pb-Pb collisions at 5.02 TeV for 3.5 < y < 3.75

Fig. Group : y-differential J/psi photoproduction in Pb-Pb (QM2023)
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 5.02 TeV
System: Pb-Pb

The J/psi nuclear modification factor as a function of pT in the centrality range (70-90)% in Pb-Pb collisions at 5.02 TeV for 3.25 < y < 3.5

Fig. Group : y-differential J/psi photoproduction in Pb-Pb (QM2023)
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 5.02 TeV
System: Pb-Pb

The J/psi nuclear modification factor as a function of pT in the centrality range (70-90)% in Pb-Pb collisions at 5.02 TeV for 3 < y < 3.25

Fig. Group : y-differential J/psi photoproduction in Pb-Pb (QM2023)
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 5.02 TeV
System: Pb-Pb

The J/psi nuclear modification factor as a function of pT in the centrality range (70-90)% in Pb-Pb collisions at 5.02 TeV for 2.75 < y < 3

Fig. Group : y-differential J/psi photoproduction in Pb-Pb (QM2023)
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 5.02 TeV
System: Pb-Pb

The J/psi nuclear modification factor as a function of pT in the centrality range (70-90)% in Pb-Pb collisions at 5.02 TeV for 2.5 < y < 2.75

Fig. Group : y-differential J/psi photoproduction in Pb-Pb (QM2023)
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 5.02 TeV
System: Pb-Pb

The J/psi nuclear modification factor for six y intervals at forward rapidity as a function of pT, pT < 3 GeV/c, in the centrality range (70-90)% in Pb-Pb collisions at 5.02 TeV

Fig. Group : y-differential J/psi photoproduction in Pb-Pb (QM2023)
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 5.02 TeV
System: Pb-Pb

The J/psi nuclear modification factor for six y intervals at forward rapidity as a function of pT in the centrality range (70-90)% in Pb-Pb collisions at 5.02 TeV

Fig. Group : y-differential J/psi photoproduction in Pb-Pb (QM2023)
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 5.02 TeV
System: Pb-Pb

y-differential coherent J/psi photoproduction cross section at pT < 0.3 GeV/c in the centrality range (70-90)% in Pb-Pb collisions at 5.02 TeV compared with one set of models of different scenarios

Fig. Group : y-differential J/psi photoproduction in Pb-Pb (QM2023)
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 5.02 TeV
System: Pb-Pb

y-differential coherent J/psi photoproduction cross section at pT < 0.3 GeV/c in the centrality range (70-90)% in Pb-Pb collisions at 5.02 TeV

Fig. Group : y-differential J/psi photoproduction in Pb-Pb (QM2023)
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 5.02 TeV
System: Pb-Pb

Mesons inside jets: Figures as function of z

Eta/Pi0 ratio as function of z for different jet pT intervals

Fig. Group : Mesons inside jets: Figures as function of z
PWG : PWG-EM (Electromagnetic probes)
Energy: 13 TeV
System: p-p

Ratio of Pi0 z spectra (Fragmentation function) for data and PYTHIA to parameterization

Fig. Group : Mesons inside jets: Figures as function of z
PWG : PWG-EM (Electromagnetic probes)
Energy: 13 TeV
System: p-p

Comparison of corrected Eta spectra inside jets from different reconstruction methods as function of z

Fig. Group : Mesons inside jets: Figures as function of z
PWG : PWG-EM (Electromagnetic probes)
Energy: 13 TeV
System: p-p

Comparison of corrected Pi0 spectra inside jets from different reconstruction methods as function of z

Fig. Group : Mesons inside jets: Figures as function of z
PWG : PWG-EM (Electromagnetic probes)
Energy: 13 TeV
System: p-p

Mesons inside jets: Figures as function of pT

Eta/Pi0 ratio inside jets as function of pT for different jet pT intervals

Fig. Group : Mesons inside jets: Figures as function of pT
PWG : PWG-EM (Electromagnetic probes)
Energy: 13 TeV
System: p-p

Ratio of fully corrected Eta pT spectra inside jets (data and PYTHIA) to parameterization

Fig. Group : Mesons inside jets: Figures as function of pT
PWG : PWG-EM (Electromagnetic probes)
Energy: 13 TeV
System: p-p

Eta pT spectra in different jet pT intervals normalized per jet

Fig. Group : Mesons inside jets: Figures as function of pT
PWG : PWG-EM (Electromagnetic probes)
Energy: 13 TeV
System: p-p

Ratio of fully corrected Pi0 pT spectra inside jets (data and PYTHIA) to parameterization

Fig. Group : Mesons inside jets: Figures as function of pT
PWG : PWG-EM (Electromagnetic probes)
Energy: 13 TeV
System: p-p

Pi0 pT spectra in different jet pT intervals normalized per jet

Fig. Group : Mesons inside jets: Figures as function of pT
PWG : PWG-EM (Electromagnetic probes)
Energy: 13 TeV
System: p-p

Ratio of Eta pT spectra in different jet pT intervals to a fit to the inclusive Eta spectrum

Fig. Group : Mesons inside jets: Figures as function of pT
PWG : PWG-EM (Electromagnetic probes)
Energy: 13 TeV
System: p-p

Eta pT spectra in different jet pT intervals normalized per event

Fig. Group : Mesons inside jets: Figures as function of pT
PWG : PWG-EM (Electromagnetic probes)
Energy: 13 TeV
System: p-p

Ratio of Pi0 pT spectra in different jet pT intervals to a fit to the inclusive Pi0 spectrum

Fig. Group : Mesons inside jets: Figures as function of pT
PWG : PWG-EM (Electromagnetic probes)
Energy: 13 TeV
System: p-p

Pi0 pT spectra in different jet pT intervals normalized per event and the inclusive Pi0 spectrum

Fig. Group : Mesons inside jets: Figures as function of pT
PWG : PWG-EM (Electromagnetic probes)
Energy: 13 TeV
System: p-p

Pi0 pT spectra in different jet pT intervals normalized per event

Fig. Group : Mesons inside jets: Figures as function of pT
PWG : PWG-EM (Electromagnetic probes)
Energy: 13 TeV
System: p-p

$\mathrm{D}^{*+}$ spin alignment in Pb-Pb collisions at $\sqrt{s}_\mathrm{NN}=5.02$ TeV

$\rho_{00}$ parameter of prompt $\mathrm{D}^{*+}$ mesons in $0.3<|y|<0.8$ with respect to the reaction plane and a random axis in 30-50% Pb-Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV

Fig. Group : $\mathrm{D}^{*+}$ spin alignment in Pb-Pb collisions at $\sqrt{s}_\mathrm{NN}=5.02$ TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV
System: Pb-Pb

$\rho_{00}$ parameter of prompt $\mathrm{D}^{*+}$ mesons with $15<p_\mathrm{T}<30$ GeV$/c$ with respect to the reaction and production planes in 30-50% Pb-Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV

Fig. Group : $\mathrm{D}^{*+}$ spin alignment in Pb-Pb collisions at $\sqrt{s}_\mathrm{NN}=5.02$ TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV
System: Pb-Pb

$\rho_{00}$ parameter of prompt $\mathrm{D}^{*+}$ mesons with $15<p_\mathrm{T}<30$ GeV$/c$ as a function of $|y|$ with respect to the reaction plane in 30-50% Pb-Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV

Fig. Group : $\mathrm{D}^{*+}$ spin alignment in Pb-Pb collisions at $\sqrt{s}_\mathrm{NN}=5.02$ TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV
System: Pb-Pb

$\rho_{00}$ parameter of prompt $\mathrm{D}^{*+}$ mesons in $0.3<|y|<0.8$ with respect to the reaction plane in 0-10% and 30-50% Pb-Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV

Fig. Group : $\mathrm{D}^{*+}$ spin alignment in Pb-Pb collisions at $\sqrt{s}_\mathrm{NN}=5.02$ TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV
System: Pb-Pb

Non-prompt fraction of $\mathrm{D}^{*+}$ candidates in 0-10% and 30-50% Pb-Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV

Fig. Group : $\mathrm{D}^{*+}$ spin alignment in Pb-Pb collisions at $\sqrt{s}_\mathrm{NN}=5.02$ TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV
System: Pb-Pb

$|\cos{\vartheta^*}|$ differential corrected yields of $\mathrm{D}^{*+}$ candidates in two $p_\mathrm{T}$ intervals, for $0.3<|y|<0.8$ in 30-50% Pb-Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV

Fig. Group : $\mathrm{D}^{*+}$ spin alignment in Pb-Pb collisions at $\sqrt{s}_\mathrm{NN}=5.02$ TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV
System: Pb-Pb

Invariant-mass distributions of $\mathrm{D}^{*+}$ candidates in two $p_\mathrm{T}$ and $|\cos{\vartheta^*}|$ intervals, for $0.3<|y|<0.8$ in 30-50% Pb-Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV

Fig. Group : $\mathrm{D}^{*+}$ spin alignment in Pb-Pb collisions at $\sqrt{s}_\mathrm{NN}=5.02$ TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV
System: Pb-Pb

[EPS&QM2023] - Virtual photon production in MB and high multiplicity pp collisions at 13TeV

Direct photon pt (MB and HM)

Fig. Group : [EPS&QM2023] - Virtual photon production in MB and high multiplicity pp collisions at 13TeV
PWG : PWG-EM (Electromagnetic probes)
Energy: 13 TeV
System: p-p

Rg vs pt (HM)

Fig. Group : [EPS&QM2023] - Virtual photon production in MB and high multiplicity pp collisions at 13TeV
PWG : PWG-EM (Electromagnetic probes)
Energy: 13 TeV
System: p-p

Rg vs pt (MB)

Fig. Group : [EPS&QM2023] - Virtual photon production in MB and high multiplicity pp collisions at 13TeV
PWG : PWG-EM (Electromagnetic probes)
Energy: 13 TeV
System: p-p

Photon yield vs multiplicity (pp13TeV)

Fig. Group : [EPS&QM2023] - Virtual photon production in MB and high multiplicity pp collisions at 13TeV
PWG : PWG-EM (Electromagnetic probes)
Energy: 13 TeV
System: p-p

Direct photon pt (HM)

Fig. Group : [EPS&QM2023] - Virtual photon production in MB and high multiplicity pp collisions at 13TeV
PWG : PWG-EM (Electromagnetic probes)
Energy: 13 TeV
System: p-p

Direct photon pt (MB)

Fig. Group : [EPS&QM2023] - Virtual photon production in MB and high multiplicity pp collisions at 13TeV
PWG : PWG-EM (Electromagnetic probes)
Energy: 13 TeV
System: p-p

r vs pt HM (updated)

Fig. Group : [EPS&QM2023] - Virtual photon production in MB and high multiplicity pp collisions at 13TeV
PWG : PWG-EM (Electromagnetic probes)
Energy: 13 TeV
System: p-p

r vs pt MB (updated)

Fig. Group : [EPS&QM2023] - Virtual photon production in MB and high multiplicity pp collisions at 13TeV
PWG : PWG-EM (Electromagnetic probes)
Energy: 13 TeV
System: p-p

D0-tagged jet axes difference measurement in pp collisions at √s = 5.02 TeV

$\rm D^{0}$-tagged raw jet axis distribution, $\Delta R_{\rm STD,D}$, for $R = 0.4$ in $10 < p_{\rm T,ch~ jet} < 20 {\rm ~ GeV}/c$

Fig. Group : D0-tagged jet axes difference measurement in pp collisions at √s = 5.02 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV
System: p-p

Fully corrected $\rm D^{0}$-tagged jet axis distribution, $\Delta R_{\rm STD,D}$, compared to PYTHIA 8 for $R = 0.4$ in $10 < p_{\rm T,ch~ jet} < 20 {\rm ~ GeV}/c$

Fig. Group : D0-tagged jet axes difference measurement in pp collisions at √s = 5.02 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV
System: p-p

Feed-down fraction in $\rm D^{0}$-tagged jet axis difference, $\Delta R_{\rm STD,D}$, in $10 < p_{\rm T, ch ~ jet} < 20 ~ {\rm GeV}/c$ and $5 < p_{\rm T, D^{0}} < 20 ~ {\rm GeV}/c$ for $R=0.4$.

Fig. Group : D0-tagged jet axes difference measurement in pp collisions at √s = 5.02 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV
System: p-p

Azimuthal correlations between heavy-flavour decay electrons and charged particles in Pb-Pb collisions at 5.02 TeV

Delta Phi Distribution of heavy-flavor decay electrons and charged particles, Pb-Pb 30 - 50% Centrality and pp

Fig. Group : Azimuthal correlations between heavy-flavour decay electrons and charged particles in Pb-Pb collisions at 5.02 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV
System: Pb-Pb

Delta Phi Distribution of heavy-flavor decay electrons and charged particles, Pb-Pb 0 - 10% Centrality and pp

Fig. Group : Azimuthal correlations between heavy-flavour decay electrons and charged particles in Pb-Pb collisions at 5.02 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV
System: Pb-Pb

Delta Phi Distribution of heavy-flavor decay electrons and charged particles with background uncertainty, Pb-Pb 30 - 50% Centrality

Fig. Group : Azimuthal correlations between heavy-flavour decay electrons and charged particles in Pb-Pb collisions at 5.02 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV
System: Pb-Pb

Delta Phi Distribution of heavy-flavor decay electrons and charged particles with background uncertainty, Pb-Pb 0 - 10% Centrality

Fig. Group : Azimuthal correlations between heavy-flavour decay electrons and charged particles in Pb-Pb collisions at 5.02 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV
System: Pb-Pb

Away-Side Nuclear Modification factor ($I_{AA}$) of Pb-Pb in 30 - 50% Centrality

Fig. Group : Azimuthal correlations between heavy-flavour decay electrons and charged particles in Pb-Pb collisions at 5.02 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV
System: Pb-Pb

Away-Side Nuclear Modification factor ($I_{AA}$) of Pb-Pb in 0 - 10% Centrality

Fig. Group : Azimuthal correlations between heavy-flavour decay electrons and charged particles in Pb-Pb collisions at 5.02 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV
System: Pb-Pb

Near-Side Nuclear Modification factor ($I_{AA}$) of Pb-Pb in 30 - 50% Centrality

Fig. Group : Azimuthal correlations between heavy-flavour decay electrons and charged particles in Pb-Pb collisions at 5.02 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV
System: Pb-Pb

Near-Side Nuclear Modification factor ($I_{AA}$) of Pb-Pb in 0 - 10% Centrality

Fig. Group : Azimuthal correlations between heavy-flavour decay electrons and charged particles in Pb-Pb collisions at 5.02 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV
System: Pb-Pb

Comparison of Per-Trigger Associated Away-Side Yield in Pb-Pb 30 - 50% Centrality and pp

Fig. Group : Azimuthal correlations between heavy-flavour decay electrons and charged particles in Pb-Pb collisions at 5.02 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV
System: Pb-Pb

Comparison of Per-Trigger Associated Away-Side Yield in Pb-Pb 0 - 10% Centrality and pp

Fig. Group : Azimuthal correlations between heavy-flavour decay electrons and charged particles in Pb-Pb collisions at 5.02 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV
System: Pb-Pb

Comparison of Per-Trigger Associated Near-Side Yield in Pb-Pb 30 - 50% Centrality and pp

Fig. Group : Azimuthal correlations between heavy-flavour decay electrons and charged particles in Pb-Pb collisions at 5.02 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV
System: Pb-Pb

Comparison of Per-Trigger Associated Near-Side Yield in Pb-Pb 0 - 10% Centrality and pp

Fig. Group : Azimuthal correlations between heavy-flavour decay electrons and charged particles in Pb-Pb collisions at 5.02 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV
System: Pb-Pb

Polarization of photoproduced J/psi in Pb-Pb (QM2023)

Comparison of $\lambda_{\theta}$ with UPC measurement

Fig. Group : Polarization of photoproduced J/psi in Pb-Pb (QM2023)
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 5.02 TeV
System: Pb-Pb

dNdcostheta vs costheta in Pb--Pb collisions at 5.02 TeV using Helicity Frame

Fig. Group : Polarization of photoproduced J/psi in Pb-Pb (QM2023)
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 5.02 TeV
System: Pb-Pb

Invariant mass distribution of dimuon pairs for 0.5 < |cos\theta| < 0.6 in Pb-Pb collsions at 5.02 TeV

Fig. Group : Polarization of photoproduced J/psi in Pb-Pb (QM2023)
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 5.02 TeV
System: Pb-Pb

Invariant mass distribution of dimuon pairs for 0.2 < |cos\theta| < 0.3 in Pb-Pb collsions at 5.02 TeV

Fig. Group : Polarization of photoproduced J/psi in Pb-Pb (QM2023)
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 5.02 TeV
System: Pb-Pb

Invariant mass distribution of dimuon pairs for 0.0 < |cos\theta| < 0.1 in Pb-Pb collsions at 5.02 TeV

Fig. Group : Polarization of photoproduced J/psi in Pb-Pb (QM2023)
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 5.02 TeV
System: Pb-Pb

Upsilon cross section in pp collisions at 13 TeV (HP2023)

y-differential upsilon(1S) and upsilon(2S) pp cross section at 13 TeV compared to ICEM+FONLL

Fig. Group : Upsilon cross section in pp collisions at 13 TeV (HP2023)
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 13 TeV
System: p-p

pT differential Upsilon(1S) and upsilon(2S) cross section in pp collisions at 13 TeV compared to ICEM+FONLL

Fig. Group : Upsilon cross section in pp collisions at 13 TeV (HP2023)
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 13 TeV
System: p-p

Integrated Upsilon(1S) and Upsilon(2S) cross section as a function of energy compared to ICEM+FONLL model calculations

Fig. Group : Upsilon cross section in pp collisions at 13 TeV (HP2023)
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 13 TeV
System: p-p

pT differential Upsilon(1S) and upsilon(2S) cross section in pp collisions at 13 TeV compared to LHCb

Fig. Group : Upsilon cross section in pp collisions at 13 TeV (HP2023)
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 13 TeV
System: p-p

y-differential upsilon(1S) pp cross section at 13 TeV compared to lower energy ALICE data

Fig. Group : Upsilon cross section in pp collisions at 13 TeV (HP2023)
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 13 TeV
System: p-p

y-differential upsilon(1S) and upsilon(2S) pp cross section at 13 TeV compared to LHCb

Fig. Group : Upsilon cross section in pp collisions at 13 TeV (HP2023)
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 13 TeV
System: p-p

y-differential upsilon(1S) and upsilon(2S) pp cross section at 13 TeV

Fig. Group : Upsilon cross section in pp collisions at 13 TeV (HP2023)
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 13 TeV
System: p-p

pT differential Upsilon(1S) and Upsilon(2S) cross section in pp collisions at 13 TeV

Fig. Group : Upsilon cross section in pp collisions at 13 TeV (HP2023)
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 13 TeV
System: p-p

pT differential Upsilon(1S) cross section in pp collisions at 13 TeV compared to lower energy ALICE data

Fig. Group : Upsilon cross section in pp collisions at 13 TeV (HP2023)
PWG : PWG-DQ (Dileptons and Quarkonia)
Energy: 13 TeV
System: p-p

D0-tagged jet angularity measurement in pp collisions at $\sqrt{s}$ = 5.02 TeV

D0-tagged jets compared to semi-inclusive jets and to PYTHIA 8 on left and to their ratio on right for $\alpha=3$, $R=0.4$ in 10 < $p_{\rm T, ch. jet}$ < 20 GeV/c.

Fig. Group : D0-tagged jet angularity measurement in pp collisions at $\sqrt{s}$ = 5.02 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV
System: p-p

D0-tagged jets compared to semi-inclusive jets and to PYTHIA 8 on left and to their ratio on right for $\alpha=2$, $R=0.4$ in 10 < $p_{\rm T, ch. jet}$ < 20 GeV/c.

Fig. Group : D0-tagged jet angularity measurement in pp collisions at $\sqrt{s}$ = 5.02 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV
System: p-p

D0-tagged jets compared to semi-inclusive jets and to PYTHIA 8 on left and to their ratio on right for $\alpha=1.5$, $R=0.4$ in 10 < $p_{\rm T, ch. jet}$ < 20 GeV/c.

Fig. Group : D0-tagged jet angularity measurement in pp collisions at $\sqrt{s}$ = 5.02 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV
System: p-p

D0-tagged jets compared to semi-inclusive jets and to PYTHIA 8 on left and to their ratio on right for $\alpha=1$, $R=0.4$ in 10 < $p_{\rm T, ch. jet}$ < 20 GeV/c.

Fig. Group : D0-tagged jet angularity measurement in pp collisions at $\sqrt{s}$ = 5.02 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV
System: p-p

Feed-down fraction in D$^{0}$-tagged jet angularity in 10 < $p_{\rm T, ch. jet}$ < 20 GeV/c and 5 < $p_{\rm T,D^{0}}$ < 20 GeV/c for R = 0.4, $\alpha=1$.

Fig. Group : D0-tagged jet angularity measurement in pp collisions at $\sqrt{s}$ = 5.02 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV
System: p-p

Fully corrected jet angularity distributions of D0-tagged jet compared to semi-inclusive jets and to PYTHIA 8 for $\alpha=3$, $R=0.4$ in 10 < $p_{\rm T, ch. jet}$ < 20 GeV/c.

Fig. Group : D0-tagged jet angularity measurement in pp collisions at $\sqrt{s}$ = 5.02 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV
System: p-p

Fully corrected jet angularity distributions of D0-tagged jet compared to semi-inclusive jets and to PYTHIA 8 for $\alpha=2$, $R=0.4$ in 10 < $p_{\rm T, ch. jet}$ < 20 GeV/c.

Fig. Group : D0-tagged jet angularity measurement in pp collisions at $\sqrt{s}$ = 5.02 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV
System: p-p

Fully corrected jet angularity distributions of D0-tagged jet compared to semi-inclusive jets and to PYTHIA 8 for $\alpha=1.5$, $R=0.4$ in 10 < $p_{\rm T, ch. jet}$ < 20 GeV/c.

Fig. Group : D0-tagged jet angularity measurement in pp collisions at $\sqrt{s}$ = 5.02 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV
System: p-p

D0-tagged jet raw angularity distributions for $\alpha=1$ in 10 < $p_{\rm T, ch. jet}$ < 20 GeV/c and 8 < $p_{\rm T,D^{0}}$ < 12 GeV/c.

Fig. Group : D0-tagged jet angularity measurement in pp collisions at $\sqrt{s}$ = 5.02 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV
System: p-p

Invariant mass distribution of D$^{0}$-tagged jet candidates with 10 < $p_{\rm T, ch. jet}$ < 20 GeV/c and 8 < $p_{\rm T,D^{0}}$ < 12 GeV/c for R = 0.4.

Fig. Group : D0-tagged jet angularity measurement in pp collisions at $\sqrt{s}$ = 5.02 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 5.02 TeV
System: p-p

Azimuthal correlations between Λc+ baryons and charged particles in pp collisions at √s=13 TeV

Away-Side width comparison between measured Λc-h and PYTHIA8 predictions for 0.3 < pT(assoc) < 1 GeV/c

Fig. Group : Azimuthal correlations between Λc+ baryons and charged particles in pp collisions at √s=13 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13 TeV
System: p-p

Away-Side yield comparison between measured Λc-h and PYTHIA8 predictions for 0.3 < pT(assoc) < 1 GeV/c

Fig. Group : Azimuthal correlations between Λc+ baryons and charged particles in pp collisions at √s=13 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13 TeV
System: p-p

Away-Side yields and widths comparison between measured Λc-h and PYTHIA8 predictions

Fig. Group : Azimuthal correlations between Λc+ baryons and charged particles in pp collisions at √s=13 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13 TeV
System: p-p

Near-Side width comparison between measured Λc-h and PYTHIA8 predictions for 0.3 < pT(assoc) < 1 GeV/c

Fig. Group : Azimuthal correlations between Λc+ baryons and charged particles in pp collisions at √s=13 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13 TeV
System: p-p

Near-Side yield comparison between measured Λc-h and PYTHIA8 predictions for 0.3 < pT(assoc) < 1 GeV/c

Fig. Group : Azimuthal correlations between Λc+ baryons and charged particles in pp collisions at √s=13 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13 TeV
System: p-p

Near-Side yields and widths comparison between measured Λc-h and PYTHIA8 predictions

Fig. Group : Azimuthal correlations between Λc+ baryons and charged particles in pp collisions at √s=13 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13 TeV
System: p-p

Away-Side Width comparison between Λc-h and D-h at 3 < pT(trigger) < 5 GeV/c and 0.3 < pT(assoc) < 1 GeV/c

Fig. Group : Azimuthal correlations between Λc+ baryons and charged particles in pp collisions at √s=13 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13 TeV
System: p-p

Away-Side Yield comparison between Λc-h and D-h at 3 < pT(trigger) < 5 GeV/c and 0.3 < pT(assoc) < 1 GeV/c

Fig. Group : Azimuthal correlations between Λc+ baryons and charged particles in pp collisions at √s=13 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13 TeV
System: p-p

Away-Side yields and widths comparison between Λc-h and D-h

Fig. Group : Azimuthal correlations between Λc+ baryons and charged particles in pp collisions at √s=13 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13 TeV
System: p-p

Baseline comparison between Λc-h and D-h at 3 < pT(trigger) < 5 GeV/c and 0.3 < pT(assoc) < 1 GeV/c

Fig. Group : Azimuthal correlations between Λc+ baryons and charged particles in pp collisions at √s=13 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13 TeV
System: p-p

Near-Side width comparison between Λc-h and D-h for 0.3 < pT(assoc) < 1 GeV/c

Fig. Group : Azimuthal correlations between Λc+ baryons and charged particles in pp collisions at √s=13 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13 TeV
System: p-p

Near-Side Yield comparison between Λc-h and D-h for 0.3 < pT(assoc) < 1 GeV/c

Fig. Group : Azimuthal correlations between Λc+ baryons and charged particles in pp collisions at √s=13 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13 TeV
System: p-p

Near-Side yields and widths comparison between Λc-h and D-h

Fig. Group : Azimuthal correlations between Λc+ baryons and charged particles in pp collisions at √s=13 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13 TeV
System: p-p

Comparison between measured Λc+-h and D-h azimuthal correlation distributions

Fig. Group : Azimuthal correlations between Λc+ baryons and charged particles in pp collisions at √s=13 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13 TeV
System: p-p

Comparison between the measured Λc-h azimuthal correlation distributions and PYTHIA8 predictions at 3 < pT(trigger) < 5 GeV/c and 0.3 < pT(assoc) < 1 GeV/c

Fig. Group : Azimuthal correlations between Λc+ baryons and charged particles in pp collisions at √s=13 TeV
PWG : PWG-HF (Heavy Flavour)
Energy: 13 TeV
System: p-p

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