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Public Preliminary figures by analysis

Jpsi v2 in Pb-Pb collisions at 5.36 TeV at fwd rapidity

Fit to the dimuon mass and v2 distribution for 5 < pT < 6 GeV at fwd rapidity for the centality class 10-50% and at 5.36 TeV
Fit to the dimuon mass and v2 distributions for 2 < pT < 3 GeV at fwd rapidity in Pb-Pb
Fit to the dimuon mass and v2 distributions for 0 < pT < 1 GeV at fwd rapidity in Pb-Pb
Fit to the dimuon mass and v2 distributions for 5 < pT < 6 GeV at fwd rapidity in Pb-Pb with event mixing background
Fit to the dimuon mass and v2 distributions for 0 < pT < 1 GeV at fwd rapidity in Pb-Pb with event mixing background
Fit to the dimuon mass and v2 distributions for 2 < pT < 3 GeV at fwd rapidity in Pb-Pb with event mixing background
J/ψ v2 vs pT at forward rapidity in the dimuon channel at 5.36 TeV vs J/ψ v2 at 5.02 TeV
J/ψ v2 vs pT at forward rapidity in the dimuon channel for the centrality class 10-50% and at 5.36 TeV

Measurement of charged particle correlations in Pb--Pb collisions at Pb-P collisions at 5.36 TeV

ICP as a function of <Npart> for pT = 4-6 GeV/c in Pb-Pb collisions at 5.36 TeV and comparison with Pb-Pb collisions at 2.76 TeV
ICP as a function of <Npart> for pT = 6-8 GeV/c in Pb-Pb collisions at 5.36 TeV
ICP as a function of <Npart> for pT = 4-6 GeV/c in Pb-Pb collisions at 5.36 TeV
ICP as a function of <Npart> for pT = 3-4 GeV/c in Pb-Pb collisions at 5.36 TeV

Non-prompt D^0 fraction in pp collisions at 13.6 TeV

Invariant-mass distribution of $\mathrm{D^0}$ candidates with $12 < p_\mathrm{T} < 16$ in pp collisions at $\sqrt{s} = 13.6$ TeV
Invariant-mass fit of non-prompt $\rm D^0$ in pp collisions at 13.6 TeV
Non-prompt $\rm D^0$ fraction as a function of $p_{\rm T}$
Contributions of the estimated prompt and non-prompt $\rm D^0$ with the cut-variation method
Invariant-mass fit of non-prompt $\rm D^0$ in pp collisions at 13.6 TeV

$\mathrm{D_s^+/D^+}$ production yield ratio in pp collisions at $\sqrt{s}=13.6$ TeV

$\mathrm{D_s^+/D^+}$ production yield ratio measured in pp collisions at $\sqrt{s}=13.6$ TeV compared to PYTHIA 8, Catania and POWLANG predictions
$\mathrm{D_s^+/D^+}$ production yield ratio measured in pp collisions at midrapidity $(\lvert y\rvert<0.5)$ at $\sqrt{s}=13.6$ TeV compared to forward-rapidity measurements by LHCb
$\mathrm{D_s^+/D^+}$ production yield ratio measured in pp collisions at $\sqrt{s}=13.6$ TeV compared to measurements by ALICE at different centre-of-mass energies
Fit to the invariant-mass distribution of $\mathrm{D_s^+}$ and $\mathrm{D^+}$ mesons in the $5< \pt <5.5$ GeV/$c$ interval in pp collisions at $\sqrt{s}=13.6$ TeV
Fit to the invariant-mass distribution of $\mathrm{D_s^+}$ and $\mathrm{D^+}$ mesons in the $2< \pt <2.5$ GeV/$c$ interval in pp collisions at $\sqrt{s}=13.6$ TeV

Three-body femtoscopy in Run 3 with apass4 of 2022 data

ppΛ correlation function in Run3
ppp correlation function in Run3
ppΛ correlation function in Run3 compared to Run 2
ppp correlation function in Run3 compared to Run 2

Sigma_c(2520) / Sigma_c(2455) in pp collisions at 13.6 TeV

$\Sigma_{\rm c}^{0,++}(2520)/\Sigma_{\rm c}^{0,++}(2455)$ ratio in pp collisions at $\sqrt{s} = 13.6$ TeV compared with PYTHIA 8 predictions with Mode2, with variations on parameter probQQ1toQQ0join_charm
$M({\rm pK\pi\pi}) - M({\rm pK\pi})$ distribution in the interval $8 < p_{\rm T} < 12$ GeV/$c$ in pp collisions at $\sqrt{s} = 13.6$ TeV

Measurements of the groomed and ungroomed jet mass in pp and Pb-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV

Measurement of the groomed jet mass for $R=0.2$ charged-particle jets in $80 < p_\text{T}^\text{ch jet} < 100$ GeV/$c$ in Pb-Pb collisions at $\sqrt{s_\text{NN}}=5.02$ TeV as compared to pp baseline
Measurement of the groomed jet mass for $R=0.2$ charged-particle jets in $60 < p_\text{T}^\text{ch jet} < 80$ GeV/$c$ in Pb-Pb collisions at $\sqrt{s_\text{NN}}=5.02$ TeV as compared to pp baseline
Measurement of the groomed jet mass for $R=0.2$ charged-particle jets in $40 < p_\text{T}^\text{ch jet} < 60$ GeV/$c$ in Pb-Pb collisions at $\sqrt{s_\text{NN}}=5.02$ TeV as compared to pp baseline
Measurement of the ungroomed jet mass for $R=0.2$ charged-particle jets in $80 < p_\text{T}^\text{ch jet} < 100$ GeV/$c$ in Pb-Pb collisions at $\sqrt{s_\text{NN}}=5.02$ TeV as compared to pp baseline
Measurement of the ungroomed jet mass for $R=0.2$ charged-particle jets in $60 < p_\text{T}^\text{ch jet} < 80$ GeV/$c$ in Pb-Pb collisions at $\sqrt{s_\text{NN}}=5.02$ TeV as compared to pp baseline
Measurement of the ungroomed jet mass for $R=0.2$ charged-particle jets in $40 < p_\text{T}^\text{ch jet} < 60$ GeV/$c$ in Pb-Pb collisions at $\sqrt{s_\text{NN}}=5.02$ TeV as compared to pp baseline
Measurement of the groomed jet mass in Pb-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV from $100 < p_\mathrm{T}^\mathrm{ch\;jet} < 150$ GeV/$c$ with $R=0.2$
Measurement of the groomed jet mass in Pb-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV from $80 < p_\mathrm{T}^\mathrm{ch\;jet} < 100$ GeV/$c$ with $R=0.2$
Measurement of the groomed jet mass in Pb-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV from $60 < p_\mathrm{T}^\mathrm{ch\;jet} < 80$ GeV/$c$ with $R=0.2$
Measurement of the groomed jet mass in Pb-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV from $40 < p_\mathrm{T}^\mathrm{ch\;jet} < 60$ GeV/$c$ with $R=0.2$
Measurement of the groomed jet mass in pp collisions at $\sqrt{s} = 5.02$ TeV from $80 < p_\mathrm{T}^\mathrm{ch\;jet} < 100$ GeV/$c$ with $R=0.2$
Measurement of the groomed jet mass in pp collisions at $\sqrt{s} = 5.02$ TeV from $60 < p_\mathrm{T}^\mathrm{ch\;jet} < 80$ GeV/$c$ with $R=0.2$
Measurement of the groomed jet mass in pp collisions at $\sqrt{s} = 5.02$ TeV from $40 < p_\mathrm{T}^\mathrm{ch\;jet} < 60$ GeV/$c$ with $R=0.2$
Measurement of the ungroomed jet mass in pp collisions at $\sqrt{s} = 5.02$ TeV from $80 < p_\mathrm{T}^\mathrm{ch\;jet} < 100$ GeV/$c$ with $R=0.2$
Measurement of the ungroomed jet mass in pp collisions at $\sqrt{s} = 5.02$ TeV from $60 < p_\mathrm{T}^\mathrm{ch\;jet} < 80$ GeV/$c$ with $R=0.2$
Measurement of the ungroomed jet mass in pp collisions at $\sqrt{s} = 5.02$ TeV from $40 < p_\mathrm{T}^\mathrm{ch\;jet} < 60$ GeV/$c$ with $R=0.2$
Measurement of the ungroomed jet mass in Pb-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV from $100 < p_\mathrm{T}^\mathrm{ch\;jet} < 150$ GeV/$c$ with $R=0.2$
Measurement of the ungroomed jet mass in Pb-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV from $80 < p_\mathrm{T}^\mathrm{ch\;jet} < 100$ GeV/$c$ with $R=0.2$
Measurement of the ungroomed jet mass in Pb-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV from $60 < p_\mathrm{T}^\mathrm{ch\;jet} < 80$ GeV/$c$ with $R=0.2$
Measurement of the ungroomed jet mass in Pb-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV from $40 < p_\mathrm{T}^\mathrm{ch\;jet} < 60$ GeV/$c$ with $R=0.2$
Omega over pion ratio as a function of the pion yield in pp collisions at 9 GeV, 7 TeV and 13.6 TeV
  • Fig. Group :
  • PWG : PWG-LF (Light Flavour Spectra)
  • Energy: 900 GeV, 7 TeV, 13.6 TeV
  • System: p-p
Kaon over pion ratio as a function of pT in pp collisions at 900 GeV, 13 TeV and 13.6 TeV with Run 3 data
  • Fig. Group :
  • PWG : PWG-LF (Light Flavour Spectra)
  • Energy: 900 GeV
  • System: p-p

Physics Analysis Group: Spectra

Proton over pion ratio as a function of pT in pp collisions at 900 GeV, 13 TeV and 13.6 TeV with Run 3 data

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

Xic/D0 and Xic/Lc ratio in low and high V0M multiplicity classes compared to PYTHIA
Invariant mass distribution of Xic in high multiplicity class
Prompt efficiency of Xic for different multiplicity classes
Corrected yield of \Xi_c^0 in different V0M multiplicity classes
Csic0/D0 and Csic+/D0 ratio in low and high V0M multiplicity classes
Xic/Lc ratio in low and high V0M multiplicity classes
Xic/D0 ratio in low and high V0M multiplicity classes
Xic/Lc ratio measured in \pp collisions at 13TeV in different multiplicity
Xi_c^0/D^0 ratio in different V0M multiplicity classes

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

Away-Side Nuclear Modification factor ($I_{AA}$) of Pb-Pb in 0 - 10% Centrality compared to LF $I_{AA}$
Near-Side Nuclear Modification factor ($I_{AA}$) of Pb-Pb in 0 - 10% Centrality compared to LF $I_{AA}$
Delta Phi Distribution of heavy-flavor decay electrons and charged particles, Pb-Pb 30 - 50% Centrality and pp, 2 pT bins
Delta Phi Distribution of heavy-flavor decay electrons and charged particles, Pb-Pb 0 - 10% Centrality and pp, 2 pT bins
Delta Phi Distribution of heavy-flavor decay electrons and charged particles with background uncertainty, Pb-Pb 0 - 10%, 2 pT bins

Measurement of inclusive jet distributions in central Pb-Pb collisions at 5.02 TeV with a novel mixed-event approach.

Charged jet $R_{AA}$ for R = 0.3 measured in central Pb-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV: Comparison to STAR $R_{AA}$
Charged jet $R_{AA}$ for R = 0.3 measured in central Pb-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV: Comparison to previous ALICE $R_{AA}$ measured with 2015 Pb-Pb data
Charged jet $R_{AA}$ for R = 0.3 measured in central Pb-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV
Corrected charged jet distributions with $p_{T}^{lead} > 3$ GeV/c and $p_{T}^{lead} > 4$ GeV/c for central Pb-Pb collisions at 5.02 TeV
Response matrix for R=0.3 jets with $p_{T}^{lead} > 4$ GeV/c in central Pb-Pb collisions at 5.02 TeV
Response matrix for R=0.3 jets with $p_{T}^{lead} > 3$ GeV/c in central Pb-Pb collisions at 5.02 TeV
Raw correlated quasi-inclusive jet $p_{T,jet}^{reco}$ distribution with $p_{T}^{lead} > 3$ GeV/c for central Pb-Pb collisions at 5.02 TeV
Raw correlated quasi-inclusive jet $p_{T,jet}^{reco}$ distribution with $p_{T}^{lead} > 4$ GeV/c for central Pb-Pb collisions at 5.02 TeV
Raw quasi-inclusive jet $p_{T,jet}^{reco}$ distribution of the SE and ME with $p_{T}^{lead} > 3$ GeV/c for central Pb-Pb collisions at 5.02 TeV
Raw quasi-inclusive jet $p_{T,jet}^{reco}$ distribution of the SE and ME with $p_{T}^{lead} > 4$ GeV/c for central Pb-Pb collisions at 5.02 TeV

LcOverD0_pPb_5.02TeV

D0_corrected_yield_pPb_5.02TeV
Lc_corrected_yield_pPb_5.02TeV

[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

Ratio of the $j_\mathrm{T}$ distributions in high $z$ to the $j_\mathrm{T}$ distributions in inclusive $z$
Ratio of the $j_\mathrm{T}$ distributions in low $z$ to the $j_\mathrm{T}$ distributions in inclusive $z$
$j_\mathrm{T}$ distributions in $60 < p_\mathrm{T,jet}^\mathrm{ch} < 100 \;\mathrm{ GeV}/c$ in differential $z$ compared to HERWIG7
$j_\mathrm{T}$ distributions in $40 < p_\mathrm{T,jet}^\mathrm{ch} < 60 \;\mathrm{ GeV}/c$ in differential $z$ compared to HERWIG7
$j_\mathrm{T}$ distributions in $20 < p_\mathrm{T,jet}^\mathrm{ch} < 40 \;\mathrm{ GeV}/c$ in differential $z$ compared to HERWIG7
$j_\mathrm{T}$ distributions in $10 < p_\mathrm{T,jet}^\mathrm{ch} < 20 \;\mathrm{ GeV}/c$ in differential $z$ compared to HERWIG7
$j_\mathrm{T}$ distributions in $10 < p_\mathrm{T,jet}^\mathrm{ch} < 20 \;\mathrm{ GeV}/c$ in differential $z$ compared to PYTHIA8 Monash
$j_\mathrm{T}$ distributions in $20 < p_\mathrm{T,jet}^\mathrm{ch} < 40 \;\mathrm{ GeV}/c$ in differential $z$ compared to PYTHIA8 Monash
$j_\mathrm{T}$ distributions in $40 < p_\mathrm{T,jet}^\mathrm{ch} < 60 \;\mathrm{ GeV}/c$ in differential $z$ compared to PYTHIA8 Monash
$j_\mathrm{T}$ distributions in $60 < p_\mathrm{T,jet}^\mathrm{ch} < 100 \;\mathrm{ GeV}/c$ in differential $z$ compared to PYTHIA8 Monash
Jet $p_\mathrm{T}$ dependence of $j_\mathrm{T}$ distributions in inclusive $z$
Jet $p_\mathrm{T}$ dependence of $j_\mathrm{T}$ distributions in low $z$
Jet $p_\mathrm{T}$ dependence of $j_\mathrm{T}$ distributions in mid $z$
Jet $p_\mathrm{T}$ dependence of $j_\mathrm{T}$ distributions in high $z$

Xic+ to Xi pi pi versus multiplicity in pp at 13 TeV

Invariant mass distribution of Xic+ in high multiplicity class
ROC curve for high multiplicity, transverse momentum 6 to 8 GeV interval
BDT output distribution in high multiplicity, transverse momentum 6 to 8 GeV interval
Prompt efficiency of Xic+ for different multiplicity classes
Xic+ over D0 for different multiplicity classes
Corrected yield of Xic+ for different multiplicity classes with ratio to INEL>0 classes

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

psi and jpsi signal extraction from 13.6 TeV pp data
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

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