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Public Preliminary figures by analysis

Mesons inside jets: Figures as function of pT

Ratio of fully corrected Eta pT spectra inside jets (data and PYTHIA) to parameterization
Eta pT spectra in different jet pT intervals normalized per jet
Ratio of fully corrected Pi0 pT spectra inside jets (data and PYTHIA) to parameterization
Pi0 pT spectra in different jet pT intervals normalized per jet
Ratio of Eta pT spectra in different jet pT intervals to a fit to the inclusive Eta spectrum
Eta pT spectra in different jet pT intervals normalized per event
Ratio of Pi0 pT spectra in different jet pT intervals to a fit to the inclusive Pi0 spectrum
Pi0 pT spectra in different jet pT intervals normalized per event and the inclusive Pi0 spectrum
Pi0 pT spectra in different jet pT intervals normalized per event

Mesons inside jets: Figures as function of z

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

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
Delta Phi Distribution of heavy-flavor decay electrons and charged particles, Pb-Pb 0 - 10% Centrality and pp
Delta Phi Distribution of heavy-flavor decay electrons and charged particles with background uncertainty, Pb-Pb 30 - 50% Centrality
Delta Phi Distribution of heavy-flavor decay electrons and charged particles with background uncertainty, Pb-Pb 0 - 10% Centrality
Away-Side Nuclear Modification factor ($I_{AA}$) of Pb-Pb in 30 - 50% Centrality
Away-Side Nuclear Modification factor ($I_{AA}$) of Pb-Pb in 0 - 10% Centrality
Near-Side Nuclear Modification factor ($I_{AA}$) of Pb-Pb in 30 - 50% Centrality
Near-Side Nuclear Modification factor ($I_{AA}$) of Pb-Pb in 0 - 10% Centrality
Comparison of Per-Trigger Associated Away-Side Yield in Pb-Pb 30 - 50% Centrality and pp
Comparison of Per-Trigger Associated Away-Side Yield in Pb-Pb 0 - 10% Centrality and pp
Comparison of Per-Trigger Associated Near-Side Yield in Pb-Pb 30 - 50% Centrality and pp
Comparison of Per-Trigger Associated Near-Side Yield in Pb-Pb 0 - 10% Centrality and pp

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

Comparison of $\lambda_{\theta}$ with UPC measurement
dNdcostheta vs costheta in Pb--Pb collisions at 5.02 TeV using Helicity Frame
Invariant mass distribution of dimuon pairs for 0.5 < |cos\theta| < 0.6 in Pb-Pb collsions at 5.02 TeV
Invariant mass distribution of dimuon pairs for 0.2 < |cos\theta| < 0.3 in Pb-Pb collsions at 5.02 TeV
Invariant mass distribution of dimuon pairs for 0.0 < |cos\theta| < 0.1 in Pb-Pb collsions at 5.02 TeV

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
pT differential Upsilon(1S) and upsilon(2S) cross section in pp collisions at 13 TeV compared to ICEM+FONLL
Integrated Upsilon(1S) and Upsilon(2S) cross section as a function of energy compared to ICEM+FONLL model calculations
pT differential Upsilon(1S) and upsilon(2S) cross section in pp collisions at 13 TeV compared to LHCb
y-differential upsilon(1S) pp cross section at 13 TeV compared to lower energy ALICE data
y-differential upsilon(1S) and upsilon(2S) pp cross section at 13 TeV compared to LHCb
y-differential upsilon(1S) and upsilon(2S) pp cross section at 13 TeV
pT differential Upsilon(1S) and Upsilon(2S) cross section in pp collisions at 13 TeV
pT differential Upsilon(1S) cross section in pp collisions at 13 TeV compared to lower energy ALICE data

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.
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.
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.
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.
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, $\alpha=1$.
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.
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.
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.
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.
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.
Fully corrected jet angularity distributions of D0-tagged jet compared to semi-inclusive jets and to PYTHIA 8 for $\alpha=1$, $R=0.4$ in 10 < $p_{\rm T, ch. jet}$ < 20 GeV/c.

Preliminary: Full Jet Spectra - pp 8 TeV, p--Pb 8.16 TeV

Invariant Cross-Section Ratios of Different Jet Radii for pp Full Jet Spectra 8 TeV with Comparison to PYTHIA8
Comparison of the Invariant Cross-Section Ratio for R = 0.2/0.5 Full Jets in pp to PYTHIA8 Monash
Comparison of the Invariant Cross-Section Ratio for R = 0.2/0.4 Full Jets in pp to PYTHIA8 Monash
Comparison of the Invariant Cross-Section Ratio for R = 0.2/0.3 Full Jets in pp to PYTHIA8 Monash
Comparison of the Invariant Cross-Section for R = 0.5 Full Jets in pp to PYTHIA8 Monash
Comparison of the Invariant Cross-Section for R = 0.4 Full Jets in pp to PYTHIA8 Monash
Comparison of the Invariant Cross-Section for R = 0.3 Full Jets in pp to PYTHIA8 Monash
Comparison of the Invariant Cross-Section for R = 0.2 Full Jets in pp to PYTHIA8 Monash
$\sqrt{s}$ Comparison for Several Bins in $p_{T}^{jet}$ for R = 0.5 - 2.76, 5, 8, 13 TeV
$\sqrt{s}$ Comparison for Several Bins in $p_{T}^{jet}$ for R = 0.4 - 2.76, 5, 8, 13 TeV
$\sqrt{s}$ Comparison for Several Bins in $p_{T}^{jet}$ for R = 0.3 - 2.76, 5, 8, 13 TeV

J/psi production in jets at midrapidity in pp collisions at 13 TeV (HP2023)

Fragmentation function of J/psi-tagged charged jets
Fragmentation function of non-prompt J/psi-tagged charged jets
Fragmentation function of prompt J/psi-tagged charged jets
f_B signal extraction 0.7 < z < 0.8
Inclusive jpsi signal extraction, 0.7 < z < 0.8

Z→e+e− in pp collisions at 13 TeV

Fiducial cross section of Z->ee at mirapidity in pp collisions at 13 TeV
Invariant mass of Z->ee (ULS and LS pairs) at midrapidity in pp collisions at 13 TeV
Invariant mass of Z->ee at midrapidity in pp collisions at 13 TeV

Ds-jet longitudinal momentum fraction in pp collisions at 13 TeV

The comparison of longitudinal momentum fraction of $\rm D_{s}^{+}$ and $\rm D^{0}$ -tagged jets in MB pp collisions at 13 TeV
Longitudinal momentum fraction of $\rm D_{s}^{+}$-tagged jets in MB pp collisions at 13 TeV
Relative statistical and systematic uncertainties by categories of $\rm D_{s}^{+}$-tagged jets longitudinal momentum fraction in MB pp collisions at 13 TeV
Feed-down contribution of $\rm D_{s}^{+}$ jets from POWHEG+PYTHIA6+EvtGen in MB pp collisions at 13 TeV
Invariant mass distribution of $\rm D_{s}^{+}$ candidates inside jets in MB pp collisions at 13 TeV

Energy flow within jets in pp and Pb-Pb collisions with ALICE

Energy flow distributions overview Charged jets 60-80 GeV pp 13 TeV, R=0.05 to 0.1, R=0.2 to 0.25 and R=0.35 to 0.4
Energy flow distributions overview Charged jets 40-60 GeV pp 13 TeV, R=0.05 to 0.1, R=0.2 to 0.25 and R=0.35 to 0.4
Energy flow distributions overview Charged jets 60-80 GeV pp 13 TeV, All Rjet pairs
Energy flow distributions overview Charged jets 40-60 GeV pp 13 TeV, All Rjet pairs
Energy flow distributions with model comparison Charged jets 60-80 GeV pp 13 TeV, R=0.35 to R=0.4
Energy flow distributions with model comparison Charged jets 40-60 GeV pp 13 TeV, R=0.35 to R=0.4
Energy flow distributions with model comparison Charged jets 60-80 GeV pp 13 TeV, R=0.2 to R=0.25
Energy flow distributions with model comparison Charged jets 40-60 GeV pp 13 TeV, R=0.2 to R=0.25
Energy flow distributions with model comparison Charged jets 60-80 GeV pp 13 TeV, R=0.05 to R=0.1
Energy flow distributions with model comparison Charged jets 40-60 GeV pp 13 TeV, R=0.05 to R=0.1
Mean energy flow versus jet radius with model comparison Charged jets 60-80 GeV pp 13 TeV
Mean energy flow versus jet radius with model comparison Charged jets 40-60 GeV pp 13 TeV
Mean energy flow versus jet radius with jet pt dependence Charged jets pp 13 TeV

[poster] Measurement of the transverse momentum($j_T$) distributions of charged-particle jet fragments in pp collisions at $\sqrt{s}$ = 5.02 TeV with ALICE

Measured $j_\mathrm{T}$ distributions in high $z$ bin compared to PYTHIA8 Tune4C
Measured $j_\mathrm{T}$ distributions in mid $z$ bin compared to PYTHIA8 Tune4C
Measured $j_\mathrm{T}$ distributions in low $z$ bin compared to PYTHIA8 Tune4C
Measured $j_\mathrm{T}$ distributions in inclusive $z$ bin compared to PYTHIA8 Tune4C
Measured $j_\mathrm{T}$ distributions in high $z$ bin compared to Herwig
Measured $j_\mathrm{T}$ distributions in mid $z$ bin compared to Herwig
Measured $j_\mathrm{T}$ distributions in low $z$ bin compared to Herwig
Measured $j_\mathrm{T}$ distributions in inclusive $z$ bin compared to Herwig

Measurement of heavy-flavor production in the high-mass dimuon spectrum in pp collisions at sqrt{s}=13 TeV with ALICE (HP2023)

[HP 2023] Beauty cross section as a function of rapidity compared with FONLL prediction (NNPDF pdf)
[HP 2023] Beauty cross section as a function of rapidity compared with FONLL prediction (CTEQ6 pdf)
[HP 2023] Charm cross section as a function of rapidity compared with FONLL prediction (CTEQ6 pdf)
[HP 2023] Charm cross section as a function of rapidity compared with FONLL prediction (NNPDF pdf)
[HP 2023] Simultaneous unbinned fit to dimuon data distribution (transverse momentum component)
[HP 2023] Simultaneous unbinned fit to dimuon data distribution (mass component)
[HP 2023] Dimuon invariant mass distribution with m>4 Gev/c^2