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Public Preliminary figures by analysis

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

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
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
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
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
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

Mesons inside jets: Figures as function of z

Eta/Pi0 ratio as function of z for different jet pT intervals
Ratio of Pi0 z spectra (Fragmentation function) for data and PYTHIA to parameterization
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

Mesons inside jets: Figures as function of pT

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

$\mathrm{D}^{*+}$ 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
$\rho_{00}$ 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
$\rho_{00}$ 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
$\rho_{00}$ 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
Non-prompt fraction of $\mathrm{D}^{*+}$ candidates in 0-10% and 30-50% Pb-Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV
$|\cos{\vartheta^*}|$ 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
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

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

Direct photon pt (MB and HM)
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)

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

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

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.

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