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Public Preliminary figures by analysis

Public Preliminary figures by analysis

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

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

$\Omega_{\rm c}^{0}$ production in semileptonic decay channel in pp collisions at $\sqrt s$ = 13 TeV

BR ratio comparisons
The measurements of the $\Omega_{\rm c}^{0}-$baryon, not corrected by the BRs, in the two different decay channels (hadronic and semileptonic), also the ratio of the branching fraction
Acceptance and efficiency of $\Omega_{\rm c}^{0} \rightarrow e^{+}\Omega^{-}\nu_{e}$
Response matrix
Invariant mass distribution of $e\Omega$

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

Rg vs pt (HM)
Rg vs pt (MB)
Photon yield vs multiplicity (pp13TeV)
Direct photon pt (HM)
Direct photon pt (MB)
r vs pt HM (updated)
r vs pt MB (updated)

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

Hardest kt splittings in pp and PbPb at 5 TeV

Hardest $k_{\mathrm{T}}$ jet splitting for R = 0.2 jets in 30-50% PbPb collisions - soft drop zcut = 0.2, comparison with models
Hardest $k_{\mathrm{T}}$ jet splitting for R = 0.2 jets in 0-10% PbPb collisions - soft drop zcut = 0.4, comparison with models
Hardest $k_{\mathrm{T}}$ jet splitting for R = 0.2 jets in 0-10% PbPb collisions - soft drop zcut = 0.2, comparison with models
Hardest $k_{\mathrm{T}}$ jet splitting for R = 0.2 jets in 0-10% PbPb collisions - Dynamical grooming a = 1.0 z > 0.2, comparison with models
Hardest $k_{\mathrm{T}}$ jet splitting for R = 0.2 jets in 0-10% PbPb collisions - Dynamical grooming a = 1.0, comparison with models
Hardest $k_{\mathrm{T}}$ jet splitting for R = 0.2 jets in pp collisions - additional grooming methods comparison with PYTHIA8
Hardest $k_{\mathrm{T}}$ jet splitting for R = 0.2 jets in pp collisions - selection of grooming methods
Hardest $k_{\mathrm{T}}$ jet splitting for R = 0.2 jets in pp collisions - additional grooming methods
Hardest $k_{\mathrm{T}}$ jet splitting for R = 0.2 jets in 0-10% PbPb collisions - selection of grooming methods
Hardest $k_{\mathrm{T}}$ jet splitting for R = 0.2 jets in 0-10% PbPb collisions - additional grooming methods
Hardest $k_{\mathrm{T}}$ jet splitting for R = 0.2 jets in 0-10% PbPb collisions - original grooming methods
Hardest $k_{\mathrm{T}}$ jet splitting for R = 0.2 jets in 30-50% PbPb collisions - selection of grooming methods
Hardest $k_{\mathrm{T}}$ jet splitting for R = 0.2 jets in 30-50% PbPb collisions - additional grooming methods
Hardest $k_{\mathrm{T}}$ jet splitting for R = 0.2 jets in 0-10% and 30-50% PbPb collisions - Soft Drop z_cut = 0.4
Hardest $k_{\mathrm{T}}$ jet splitting for R = 0.2 jets in 0-10% and 30-50% PbPb collisions - Dynamical grooming a = 2.0, z > 0.2
Hardest $k_{\mathrm{T}}$ jet splitting for R = 0.2 jets in 0-10% and 30-50% PbPb collisions - Dynamical grooming a = 1.0, z > 0.2
Hardest $k_{\mathrm{T}}$ jet splitting for R = 0.2 jets in 0-10% and 30-50% PbPb collisions - Dynamical grooming a = 0.5, z > 0.2
Hardest $k_{\mathrm{T}}$ jet splitting for R = 0.2 jets in 0-10% and 30-50% PbPb collisions - Soft Drop z_cut = 0.2
Hardest $k_{\mathrm{T}}$ jet splitting for R = 0.2 jets in 0-10% and 30-50% PbPb collisions - Dynamical grooming a = 2.0
Hardest $k_{\mathrm{T}}$ jet splitting for R = 0.2 jets in 0-10% and 30-50% PbPb collisions - Dynamical grooming a = 1.0
Hardest $k_{\mathrm{T}}$ jet splitting for R = 0.2 jets in 0-10% and 30-50% PbPb collisions - Dynamical grooming a = 0.5

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.

Energy-energy correlator measurements for jets in p+p collisions at 5.02TeV

EEC distribution for 40-60GeV charged jets in pp collision (theory comparison included)

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
Away-Side yield comparison between measured Λc-h and PYTHIA8 predictions for 0.3 < pT(assoc) < 1 GeV/c
Away-Side yields and widths comparison between measured Λc-h and PYTHIA8 predictions
Near-Side width comparison between measured Λc-h and PYTHIA8 predictions for 0.3 < pT(assoc) < 1 GeV/c
Near-Side yield comparison between measured Λc-h and PYTHIA8 predictions for 0.3 < pT(assoc) < 1 GeV/c
Near-Side yields and widths comparison between measured Λc-h and PYTHIA8 predictions
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
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
Away-Side yields and widths comparison between Λc-h and D-h
Baseline comparison between Λc-h and D-h at 3 < pT(trigger) < 5 GeV/c and 0.3 < pT(assoc) < 1 GeV/c
Near-Side width comparison between Λc-h and D-h for 0.3 < pT(assoc) < 1 GeV/c
Near-Side Yield comparison between Λc-h and D-h for 0.3 < pT(assoc) < 1 GeV/c
Near-Side yields and widths comparison between Λc-h and D-h
Comparison between measured Λc+-h and D-h azimuthal correlation distributions
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
Comparison between the measured Λc-h azimuthal correlation distributions and PYTHIA8 predictions
Comparison between Λc-h and D-h azimuthal correlation distributions measured in the transverse momentum interval 3 < pT(trigger) < 5 GeV/c and 0.3 < pT(assoc) < 1 GeV/c

Measurement of non-prompt $\Dplus$ and non-prompt $\Ds$ meson production in pp collisions at $\sqrts=13$ TeV

Non-prompt $\rm D^{+}$ production cross section in pp collisions at 13 TeV vs. models
Non-prompt $\rm D_{s}^{+}$ production cross section in pp collisions at 13 TeV vs. models
Non-prompt $\rm D^{+}$/$\rm D^{0}$ ratio in pp collisions at 13 TeV
Non-prompt $\rm D_{s}^{+}$/$\rm D^{0}$ ratio in pp collisions at 13 TeV
Non-prompt $\rm D_{s}^{+}$/$\rm D^{+}$ ratio in pp collisions at 13 TeV
Non-prompt $\rm D_{s}^{+}$/($\rm D^{+}$ + $\rm D^{0}$) ratio in pp collisions at 13 TeV
$\rm D^{+}$ efficiency times acceptance in pp collisions at 13 TeV
$\rm D_{s}^{+}$ efficiency times acceptance in pp collisions at 13 TeV
Non-prompt $\rm D^{+}$ cut variation in pp collisions at 13 TeV
Non-prompt $\rm D_{s}^{+}$ cut variation in pp collisions at 13 TeV
Non-prompt $\rm D^{0}$, $\rm D^{+}$, $\rm D_{s}^{+}$ fraction pp collisions at 13 TeV
Non-prompt $\rm D^{+}$ invariant-mass distribution in pp collisions at 13 TeV
Non-prompt $\rm D_{s}^{+}$ invariant-mass distribution in pp collisions at 13 TeV

Charm production cross section and fragmentation fractions in p-Pb

Integrated $R_\mathrm{pPb}$ of charm, D$^{0}$, $\Lambda_\mathrm{c}^{+}$ and J/$\psi$
Total charm production cross section in pp and p-Pb collisions as a function of $\sqrt{s}$
Charm-hadron fragmentation fractions in pp and p-Pb collisions including measured Xic in p-Pb (2023)

Measurement of non-prompt $\rm D^0$ production in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV with ALICE

$p_{\rm T}$-integrated non-prompt $\rm D^{0}$ $R_{\rm pPb}$ from 0-24 GeV/$\it{c}$ in pPb collisions at 5.02 TeV
Invariant-mass distribution of non-prompt $\rm D^{0}$ in pPb collisions at 5.02 TeV
Non-prompt $\rm D^{0}$ $R_{\rm pPb}$ in pPb collisions at 5.02 TeV compared with CMS measurement in log scale
Non-prompt $\rm D^{0}$ $R_{\rm pPb}$ in pPb collisions at 5.02 TeV compared with CMS measurement