| 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
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| ICP as a function of <Npart> for pT = 6-8 GeV/c in Pb-Pb collisions at 5.36 TeV
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| ICP as a function of <Npart> for pT = 4-6 GeV/c in Pb-Pb collisions at 5.36 TeV
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| ICP as a function of <Npart> for pT = 3-4 GeV/c in Pb-Pb collisions at 5.36 TeV
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| Invariant-mass distribution of $\mathrm{D^0}$ candidates with $12 < p_\mathrm{T} < 16$ in pp collisions at $\sqrt{s} = 13.6$ TeV
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| $\mathrm{D_s^+/D^+}$ production yield ratio measured in pp collisions at $\sqrt{s}=13.6$ TeV compared to PYTHIA 8, Catania and POWLANG predictions
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| $\mathrm{D_s^+/D^+}$ 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
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| $\mathrm{D_s^+/D^+}$ production yield ratio measured in pp collisions at $\sqrt{s}=13.6$ TeV compared to measurements by ALICE at different centre-of-mass energies
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| 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
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| 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
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| ppΛ correlation function in Run3
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| ppp correlation function in Run3
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| ppΛ correlation function in Run3 compared to Run 2
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| ppp correlation function in Run3 compared to Run 2
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| $\Sigma_{\rm c}^{0,++}(2520)/\Sigma_{\rm c}^{0,++}(2455)$ ratio in pp collisions at $\sqrt{s} = 13.6$ TeV compared with PYTHIA 8 predictions with Mode2, with variations on parameter probQQ1toQQ0join_charm
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| $M({\rm pK\pi\pi}) - M({\rm pK\pi})$ distribution in the interval $8 < p_{\rm T} < 12$ GeV/$c$ in pp collisions at $\sqrt{s} = 13.6$ TeV
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| Invariant-mass fit of non-prompt $\rm D^0$ in pp collisions at 13.6 TeV
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| Non-prompt $\rm D^0$ fraction as a function of $p_{\rm T}$
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| Contributions of the estimated prompt and non-prompt $\rm D^0$ with the cut-variation method
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| Invariant-mass fit of non-prompt $\rm D^0$ in pp collisions at 13.6 TeV
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| 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
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| 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
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| 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
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| 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
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| 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
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| 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
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| 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 $R=0.2$
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| 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 $R=0.2$
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| 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 $R=0.2$
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| 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 $R=0.2$
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| 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 $R=0.2$
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| 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 $R=0.2$
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| 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 $R=0.2$
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| 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 $R=0.2$
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| 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 $R=0.2$
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| 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 $R=0.2$
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| 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 $R=0.2$
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| 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 $R=0.2$
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| 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 $R=0.2$
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| 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 $R=0.2$
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Omega over pion ratio as a function of the pion yield in pp collisions at 9 GeV, 7 TeV and 13.6 TeV
- PWG : PWG-LF (Light Flavour Spectra)
- Energy: 900 GeV
, - Energy: 7 TeV
, - Energy: 13.6 TeV
- System p-p
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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
- PWG : PWG-LF (Light Flavour Spectra)
- Energy: 900 GeV
- System p-p
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| 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
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| Xic/D0 and Xic/Lc ratio in low and high V0M multiplicity classes compared to PYTHIA
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| Invariant mass distribution of Xic in high multiplicity class
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| Prompt efficiency of Xic for different multiplicity classes
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| Away-Side Nuclear Modification factor ($I_{AA}$) of Pb-Pb in 0 - 10% Centrality compared to LF $I_{AA}$
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| Near-Side Nuclear Modification factor ($I_{AA}$) of Pb-Pb in 0 - 10% Centrality compared to LF $I_{AA}$
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| Charged jet $R_{AA}$ for R = 0.3 measured in central Pb-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV: Comparison to STAR $R_{AA}$
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| 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
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| Charged jet $R_{AA}$ for R = 0.3 measured in central Pb-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV
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| 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
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| Response matrix for R=0.3 jets with $p_{T}^{lead} > 4$ GeV/c in central Pb-Pb collisions at 5.02 TeV
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| Response matrix for R=0.3 jets with $p_{T}^{lead} > 3$ GeV/c in central Pb-Pb collisions at 5.02 TeV
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| 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
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| 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
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| 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
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| 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
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| Lc/D0_vs_multiplcity_pt_pPb_5.02TeV
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| D0_corrected_yield_pPb_5.02TeV
|
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| Lc_corrected_yield_pPb_5.02TeV
|
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| Delta Phi Distribution of heavy-flavor decay electrons and charged particles, Pb-Pb 30 - 50% Centrality and pp, 2 pT bins
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| Delta Phi Distribution of heavy-flavor decay electrons and charged particles, Pb-Pb 0 - 10% Centrality and pp, 2 pT bins
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| Delta Phi Distribution of heavy-flavor decay electrons and charged particles with background uncertainty, Pb-Pb 0 - 10%, 2 pT bins
|
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| Ratio of the $j_\mathrm{T}$ distributions in high $z$ to the $j_\mathrm{T}$ distributions in inclusive $z$
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| Ratio of the $j_\mathrm{T}$ distributions in low $z$ to the $j_\mathrm{T}$ distributions in inclusive $z$
|
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| $j_\mathrm{T}$ distributions in $60 < p_\mathrm{T,jet}^\mathrm{ch} < 100 \;\mathrm{ GeV}/c$ in differential $z$ compared to HERWIG7
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| $j_\mathrm{T}$ distributions in $40 < p_\mathrm{T,jet}^\mathrm{ch} < 60 \;\mathrm{ GeV}/c$ in differential $z$ compared to HERWIG7
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| $j_\mathrm{T}$ distributions in $20 < p_\mathrm{T,jet}^\mathrm{ch} < 40 \;\mathrm{ GeV}/c$ in differential $z$ compared to HERWIG7
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| $j_\mathrm{T}$ distributions in $10 < p_\mathrm{T,jet}^\mathrm{ch} < 20 \;\mathrm{ GeV}/c$ in differential $z$ compared to HERWIG7
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| $j_\mathrm{T}$ distributions in $10 < p_\mathrm{T,jet}^\mathrm{ch} < 20 \;\mathrm{ GeV}/c$ in differential $z$ compared to PYTHIA8 Monash
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| $j_\mathrm{T}$ distributions in $20 < p_\mathrm{T,jet}^\mathrm{ch} < 40 \;\mathrm{ GeV}/c$ in differential $z$ compared to PYTHIA8 Monash
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| $j_\mathrm{T}$ distributions in $40 < p_\mathrm{T,jet}^\mathrm{ch} < 60 \;\mathrm{ GeV}/c$ in differential $z$ compared to PYTHIA8 Monash
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| $j_\mathrm{T}$ distributions in $60 < p_\mathrm{T,jet}^\mathrm{ch} < 100 \;\mathrm{ GeV}/c$ in differential $z$ compared to PYTHIA8 Monash
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| Jet $p_\mathrm{T}$ dependence of $j_\mathrm{T}$ distributions in inclusive $z$
|
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| Jet $p_\mathrm{T}$ dependence of $j_\mathrm{T}$ distributions in low $z$
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| Jet $p_\mathrm{T}$ dependence of $j_\mathrm{T}$ distributions in mid $z$
|
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| Jet $p_\mathrm{T}$ dependence of $j_\mathrm{T}$ distributions in high $z$
|
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| Invariant mass distribution of Xic+ in high multiplicity class
|
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| ROC curve for high multiplicity, transverse momentum 6 to 8 GeV interval
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| BDT output distribution in high multiplicity, transverse momentum 6 to 8 GeV interval
|
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| Prompt efficiency of Xic+ for different multiplicity classes
|
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| Xic+ over D0 for different multiplicity classes
|
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| Corrected yield of Xic+ for different multiplicity classes with ratio to INEL>0 classes
|
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| Corrected yield of \Xi_c^0 in different V0M multiplicity classes
|
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| Csic0/D0 and Csic+/D0 ratio in low and high V0M multiplicity classes
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| Xic/Lc ratio in low and high V0M multiplicity classes
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| Xic/D0 ratio in low and high V0M multiplicity classes
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| Xic/Lc ratio measured in \pp collisions at 13TeV in different multiplicity
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| Xi_c^0/D^0 ratio in different V0M multiplicity classes
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| psi and jpsi signal extraction from 13.6 TeV pp data
|
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| 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
|
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| 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
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| 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
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| y-differential J/psi production cross section at forward y as a function of pT in pp collisions at 5.02 TeV
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| 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
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| 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
|
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| 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
|
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| 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
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| 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
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