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Public Preliminary figures by analysis

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

Compilation of Invariant Cross-Sections for R = 0.3 in pp Full Jet Spectra - 5, 8, 13 TeV
Compilation of Invariant Cross-Sections for R = 0.2 in pp Full Jet Spectra - 2.76, 5, 8, 13 TeV
Compilation of Invariant Cross-Section Ratios of R = 0.2/0.5 in pp Full Jet Spectra - 5, 8, 13 TeV
Compilation of Invariant Cross-Section Ratios of R = 0.2/0.4 in pp Full Jet Spectra - 2.76, 5, 8, 13 TeV
Compilation of Invariant Cross-Section Ratios of R = 0.2/0.3 in pp Full Jet Spectra - 5, 8, 13 TeV
Invariant Cross-Section Ratios of Different Jet Radii for pp Full Jet Spectra 8 TeV
Invariant Cross-Section pp Full Jet Spectra 8 TeV, R = 0.2 -0.5
Fraction of Women in ALICE by Employment Category and Time (2014-2021, Final)
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Strangeness production in jets and out of jets in pp collisions at \sqrt{s} =13 TeV and at \sqrt{s} =5.02 TeV

Fraction of events with trigger particle vs multiplicity

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 z_cut = 0.2, comparison with Hybrid model with Moliere scattering​
Hardest $k_{\mathrm{T}}$ jet splitting for R = 0.2 jets in 30-50% PbPb collisions - Dynamical grooming a = 2.0, comparison with Hybrid model with Moliere scattering​
Hardest $k_{\mathrm{T}}$ jet splitting for R = 0.2 jets in 30-50% PbPb collisions - Dynamical grooming a = 1.0, comparison with Hybrid model with Moliere scattering
Hardest $k_{\mathrm{T}}$ jet splitting for R = 0.2 jets in 30-50% PbPb collisions - Dynamical grooming a = 0.5, comparison with Hybrid model with Moliere scattering

Nuclear modification factor and isolated photon cross section for 5.02 TeV pp and p-Pb

Isolated photon differential cross section measured in p-Pb collisions at sqrt(s) = 5.02 TeV compared with JETPHOX and NLO theory
Ratio to JETPHOX of Isolated photon differential cross section measured in p-Pb collisions at sqrt(s) = 5.02 TeV
Isolated photon differential cross section measured in p-Pb collisions at sqrt(s) = 5.02 TeV

Direct photon spectra in PbPb 5.02TeV

Direct photon spectra PbPb 5TeV ratios to model calculation, with PHENIX, 20-40%
Direct photon spectra in PbPb 5.02TeV from PCM with comparison to all model calculations

Longitudinal Fluctuations in Heavy-Ion Collisions with the ALICE Detector

Charge conservation effect in first longitudinal coefficient a_{1} as a function of <dNch/deta> in Xe-Xe collisions
Charge conservation effect in first longitudinal coefficient a_{1} as a function of <dNch/deta> in Pb-Pb collisions
First longitudinal coefficient a_{1} scaled with sqrt(<dNch/deta>) as a function of <dNch/deta> in Pb-Pb and Xe-Xe collisions
First longitudinal coefficient a_{1} in Xe-Xe and Pb-Pb collisions as a function of <dNch/deta>

$J/\psi$ $v_{2}$ in pp collisions at 13 TeV - QM2022

$p_T$ dependence of $J/\psi$ $v_2$ for various collision systems
Procedure of $V_{2,J/\psi-tracklet}$ extraction from $V_{2,dimuon-tracklet}(m_{\mu\mu})$
$p_T$ dependence of $J/\psi$ $v_2$ in pp collisions at 13 TeV - Yield subtraction method
$p_T$ dependence of $J/\psi$ $v_2$ in pp collisions at 13 TeV

Direct photon R_gamma in PbPb 5.02TeV

Direct photon double ratio in PbPb 5.02TeV from PCM with all models
Double ratio 0-20% from PCM and 0-10% from Dielectrons
Double ratio 60-80% with different model calculations
Double ratio 40-60% with different model calculations
Double ratio 20-40% with different model calculations
Double ratio 0-20% with different model calculations

Low $p_{T}$ $J/\psi$ excess at midrapidity in peripheral Pb-Pb collisions at 5.02 TeV with full Run 2 + projections for Run3/4 (QM2022)

Ratio of coherent $ J/\psi$ cross section measured in collisions with nuclear overlap over ultraperipheral Pb-Pb collisions at forward and midrapidity
Coherent $ J/\psi$ cross section vs Npart in Pb-Pb collisions at $\sqrt{s_{\mathrm {NN}}}$ =5.02 TeV measured at midrapidty and forward rapidity

Measurement of isolated photon-jet correlations in 5.02 TeV Pb-Pb collisions

Truncated mean of momentum imbalance between isolated photons and jets in 5.02 TeV Pb-Pb collisions with PYTHIA comparison
Momentum imbalance between isolated photons and jets in 5.02 TeV Pb-Pb collisions with PYTHIA comparison
Angular correlations between isolated photons and jets in 5.02 TeV Pb-Pb collisions with PYTHIA comparison

Event shape and multiplicity dependence of K*(892)$^{\mathbf{\pm}}$ production at mid-rapidity in pp collisions at $\sqrt{s}$ = 13 TeV

$\it{p}_{T}$-differential K*(892)$^{\mathbf{\pm}}$-to-Proton ratio as a function of spherocity ($S_{0}^{p_{T}=1}$) in pp collisions at $\sqrt{s}$ = 13 TeV (I-III V0M multiplicity class)
$\it{p}_{T}$-differential K*(892)$^{\mathbf{\pm}}$-to-Kaon ratio as a function of spherocity ($S_{0}^{p_{T}=1}$) in pp collisions at $\sqrt{s}$ = 13 TeV (I-III V0M multiplicity class)
$\it{p}_{T}$-differential K*(892)$^{\mathbf{\pm}}$-to-Pion ratio as a function of spherocity ($S_{0}^{p_{T}=1}$) in pp collisions at $\sqrt{s}$ = 13 TeV (I-III V0M multiplicity class)
Transverse Momentum spectra of K*(892)$^{\mathbf{\pm}}$ in (I-III) V0M Multiplicity class and 5% $S_{0}^{p_{T}=1}$ in pp collisions at $\sqrt{s}$ = 13 TeV
Transverse Momentum spectra of K*(892)$^{\mathbf{\pm}}$ in (I-III) V0M Multiplicity class and 10% $S_{0}^{p_{T}=1}$ in pp collisions at $\sqrt{s}$ = 13 TeV
Transverse Momentum spectra of K*(892)$^{\mathbf{\pm}}$ in (I-III) V0M Multiplicity class and 20% $S_{0}^{p_{T}=1}$ in pp collisions at $\sqrt{s}$ = 13 TeV

D0-Jet in 0-10% Pb-Pb collisions at 5.02 TeV (2018)

Raw D0-Jet pT spectrum for D0 pT in the range 4 to 5 GeV/c
Invariant mass analysis (Kpi) in D0 pT range 10 to 12 GeV/c
Invariant mass analysis (Kpi) in D0 pT range 4 to 5 GeV/c

$\phi$-meson pair measurement

Results for $\phi$ meson production characterisation in pp collisions at $\sqrt{s}$ = 7 TeV

Flow of identified particles in pp and p-Pb collisions

v2 in central p-Pb collisions with pi, K, p,Lambda using improved template fit method compared to AMPT with string melting
v2 in central p-Pb collisions with pi, K, p,Lambda using template fit method compared to AMPT with string melting

[QM2022] - Neutral meson production in MB and multiplicity dependent pp collisions at 13TeV

Ratio of eta meson invariant cross sections for 6 energies together with NLO calculations and Pythia
Ratio of pi0 invariant cross sections for 6 energies together with NLO calculations and Pythia

Isolated photon cross section in different energies and systems (QM2022)

Isolated photon cross section ratios in pp collisions $\sqrt s = $ 8 to 7 TeV
Isolated photon cross section ratios in pp collisions $\sqrt s = $ 13 to 8 TeV
Isolated photon cross section ratios in pp collisions $\sqrt s = $ 13 to 7 TeV
Isolated photon cross section in pp collisions at $\sqrt s = $ 7, 8 and 13 TeV and p-Pb collisions at $\sqrt {s_{\rm NN}} = $ 5.02 TeV
Isolated photon cross section in pp collisions at $\sqrt s = $ 7, 8 and 13 TeV

[QM2022] - omega meson production in pp collisions at 13 TeV

Acceptance Times Efficiency

Charged-particle jet properties in p-Pb collisions at 5.02 TeV

Underlying event (UE) subtraction procedure for $z^{\rm ch}$ distribution for leading jet $p_{\rm T,jet}^{\rm ch}$ = 40-60 GeV/$c$ in p-Pb collisions at 5.02 TeV
Underlying event (UE) subtraction procedure for $\langle N_{\rm ch}\rangle$ distribution as a function of leading jet $p_{\rm T,jet}^{\rm ch}$ in p-Pb collisions at 5.02 TeV

Groomed and ungroomed jet angularities and mass in Pb-Pb collisions at $\sqrt{s_\text{NN}}=5.02$ TeV

Groomed $\lambda_{\alpha=3}^{\kappa=1}$ 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
Groomed $\lambda_{\alpha=2}^{\kappa=1}$ 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
Groomed $\lambda_{\alpha=1.5}^{\kappa=1}$ 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
Groomed $\lambda_{\alpha=1}^{\kappa=1}$ 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
Ungroomed $\lambda_{\alpha=3}^{\kappa=1}$ 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
Ungroomed $\lambda_{\alpha=2}^{\kappa=1}$ 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
Ungroomed $\lambda_{\alpha=1.5}^{\kappa=1}$ 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
Ungroomed $\lambda_{\alpha=1}^{\kappa=1}$ 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
Groomed $\lambda_{\alpha=3}^{\kappa=1}$ 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
Groomed $\lambda_{\alpha=2}^{\kappa=1}$ 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
Groomed $\lambda_{\alpha=1.5}^{\kappa=1}$ 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
Groomed $\lambda_{\alpha=1}^{\kappa=1}$ 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
Ungroomed $\lambda_{\alpha=3}^{\kappa=1}$ 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
Ungroomed $\lambda_{\alpha=2}^{\kappa=1}$ 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
Ungroomed $\lambda_{\alpha=1.5}^{\kappa=1}$ 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
Ungroomed $\lambda_{\alpha=1}^{\kappa=1}$ 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
Groomed $\lambda_{\alpha=3}^{\kappa=1}$ 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
Groomed $\lambda_{\alpha=2}^{\kappa=1}$ 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
Groomed $\lambda_{\alpha=1.5}^{\kappa=1}$ 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
Groomed $\lambda_{\alpha=1}^{\kappa=1}$ 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
Ungroomed $\lambda_{\alpha=3}^{\kappa=1}$ 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
Ungroomed $\lambda_{\alpha=2}^{\kappa=1}$ 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
Ungroomed $\lambda_{\alpha=1.5}^{\kappa=1}$ 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

Isolated photons cross section in pp collisions at 8 TeV

Isolated photons cross section ratio with theory prediction
Isolated photons cross section comparison with theory
Isolated photons cross section comparison with theory and ratio
Purity: isolated photons purity distribution @ pp 8 TeV
Systematic Uncertainty: isolated photons cross section systematic uncertainties @ pp 8 TeV
Cross section: isolated photons cross section @ pp 8 TeV

V0s in p-Pb 8.16 TeV

Nuclear Modification Factor in p-Pb 8.16 TeV for K0S and Lambda
Ratio of Lambda to K0s as a function of charge particle multiplicity
Ratio of Lambda to K0s as a function of transverse momentum
Ratio of Lambda yield to pions yield as a function of multiplicity
Ratio of K0S yield to pions yield as a function of multiplicity
Average transverse momentum as a function of multiplicity for Lambda including Pb-Pb data points

Preliminary -- IsoGamma CS in pp 13TeV

Cross section -- IsoGamma cross section in pp 13TeV
Ratio of CS to theory comparison -- IsoGamma cross section in pp 13TeV
CS and model pt comparison-- IsoGamma cross section in pp 13TeV
CS comparison with theory -- pt and ratio -- IsoGamma cross section in pp 13TeV
purity -- IsoGamma cross section in pp 13TeV
SysUncertainty -- IsoGamma cross section in pp 13TeV