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Public Preliminary figures by analysis

Measurement of Jet Constituent Yields in 5.02 TeV Pb-Pb Collisions with the ALICE Detector

Out/In Away Side Constituent Yield Ratio compared to JEWEL with no recoils, pT^jet = 20-40 GeV, pT^assoc. > 2 GeV, 5.02 TeV PbPb, 30-50 %
Out/In Near Side Constituent Yield Ratio compared to JEWEL with no recoils, pT^jet = 20-40 GeV, pT^assoc. > 2 GeV, 5.02 TeV PbPb, 30-50 %
Mid/In Away Side Constituent Yield Ratio, pT^jet = 20-40 GeV, pT^assoc. > 2 GeV, 5.02 TeV PbPb, 30-50 %
Mid/In Near Side Constituent Yield Ratio, pT^jet = 20-40 GeV, pT^assoc. > 2 GeV, 5.02 TeV PbPb, 30-50 %
Out/In Away Side Constituent Yield Ratio, pT^jet = 20-40 GeV, pT^assoc. > 2 GeV, 5.02 TeV PbPb, 30-50 %
Out/In Near Side Constituent Yield Ratio, pT^jet = 20-40 GeV, pT^assoc. > 2 GeV, 5.02 TeV PbPb, 30-50 %
Away Side Constituent Yields, pT^jet = 20-40 GeV, pT^assoc. > 2 GeV, 5.02 TeV PbPb, 30-50 %
Near Side Constituent Yields, pT^jet = 20-40 GeV, pT^assoc. > 2 GeV, 5.02 TeV PbPb, 30-50 %

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

Unfolded and UE subtracted $z^{\rm ch}$ distributions for different leading jet $p_{\rm T,jet}^{\rm ch}$ in p-Pb collisions at 5.02 TeV
$z^{\rm ch}$ distribution for leading jet $p_{\rm T,jet}^{\rm ch}$ = 40-60 GeV/$c$ in p-Pb collisions at 5.02 TeV
$z^{\rm ch}$ distribution for leading jet $p_{\rm T,jet}^{\rm ch}$ = 20-30 GeV/$c$ in p-Pb collisions at 5.02 TeV
$\langle N_{\rm ch}\rangle$ distribution as a function of leading jet $p_{\rm T,jet}^{\rm ch}$ in p-Pb collisions at 5.02 TeV

$\Upsilon$(1S) polarization in pp collisions at $\sqrt{s}$ = 13 TeV with ALICE (QM2022)

$\Upsilon$(1S) polarization as a function of transverse momentum
$\Upsilon$(1S) polarization: simultaneous fit to the corrected angular spectra in Helicity and Collins-Soper frames
$\Upsilon$(1S) polarization: Signal extraction

Dijet Invariant mass analysis

Dijet invariant mass spectrum for pp and p-Pb including R_{pA} at 5.02 TeV
Dijet invariant mass background fluctuations for charged jets R=0.4 for p-Pb 5.02 TeV
Dijet invariant mass background fluctuations for charged jets R=0.4 for pp 5.02 TeV

Direct photon R_gamma in PbPb 5.02TeV

Direct photon double ratio in PbPb 5.02TeV from PCM with models
Direct photon double ratio in PbPb 5.02TeV from PCM with pQCD
Direct photon double ratio in PbPb 5.02TeV from PCM
Direct photon double ratio in PbPb 5.02TeV from PCM and Dielectrons with comparison to model calculations

Direct photon spectra in PbPb 5.02TeV

Direct photon spectra PbPb 5TeV ratios to model calculation, LHC
Direct photon spectra PbPb 5TeV ratios to model calculation, with those from dielectrons and RHIC
Direct photon spectra ratios to model calculation
Direct photon spectra in PbPb 5.02TeV from PCM with comparison to pQCD
Direct photon spectra in PbPb 5.02TeV from PCM with comparison to model calculations
Direct photon spectra in PbPb 5.02TeV from PCM and Dielectrons with comparison to model calculations
Direct photon spectra in PbPb 5.02TeV from PCM

[QM2022] - Direct photon HBT correlations in pp and PbPb collisions at 5 TeV

Lambda invariant for PbPb collisions at 5 TeV
Gamma-Gamma correlations in 30-50% PbPb collisions at 5 TeV, 0.35<kT<0.5 GeV/c
Gamma-Gamma correlations in 30-50% PbPb collisions at 5 TeV, 0.25<kT<0.35 GeV/c
Gamma-Gamma correlations in 0-10% PbPb collisions at 5 TeV, 0.35<kT<0.5 GeV/c
Gamma-Gamma correlations in 0-10% PbPb collisions at 5 TeV, 0.25<kT<0.35 GeV/c
Gamma-Gamma correlations in pp collisions at 5 TeV, 0.5<kT<1.0 GeV/c
Gamma-Gamma correlations in pp collisions at 5 TeV, 0.35<kT<0.5 GeV/c
Gamma-Gamma correlations in pp collisions at 5 TeV, 0.25<kT<0.35 GeV/c

Pi0-hadron correlations in PbPb at 5.02 TeV

Pi0-hadron correlations in PbPb at 5.02 TeV 30-50% Central 11-14 GeV/c Pi0s, away-side out/in ratio with model comparison (zoomed out)
Pi0-hadron correlations in PbPb at 5.02 TeV 30-50% Central 11-14 GeV/c Pi0s, near-side out/in ratio with model comparison (zoomed out)
Pi0-hadron correlations in PbPb at 5.02 TeV 30-50% Central 11-14 GeV/c Pi0s, away-side out/in ratio (zoomed out)
Pi0-hadron correlations in PbPb at 5.02 TeV 30-50% Central 11-14 GeV/c Pi0s, near-side out/in ratio (zoomed out)
Pi0-hadron correlations in PbPb at 5.02 TeV 30-50% Central 11-14 GeV/c Pi0s, near-side out/in ratio with model comparison
Pi0-hadron correlations in PbPb at 5.02 TeV 30-50% Central 11-14 GeV/c Pi0s, away-side out/in ratio with model comparison
Pi0-hadron correlations in PbPb at 5.02 TeV 30-50% Central 11-14 GeV/c Pi0s, away-side out/in ratio
Pi0-hadron correlations in PbPb at 5.02 TeV 30-50% Central 11-14 GeV/c Pi0s, near-side out/in ratio

Pion-deuteron femtoscopic study of correlation functions in PbPb

Pion-deuteron radii compared to predictions, Pb-Pb \sqrt{sNN}=5.02 TeV, $m_{T}$ = 1.03
Pion-deuteron radii compared to predictions, Pb-Pb \sqrt{sNN}=5.02 TeV, $m_{T}$ = 0.84 GeV/c
Pion-deuteron radii, multiplicity dependence, Pb-Pb \sqrt{sNN}=5.02 TeV
Pions and deuterons $m_{T}$ scaling Pb-Pb \sqrt{sNN}=5.02 TeV
Pion-deuteron correlation function Pb-Pb \sqrt{sNN}=5.02 TeV with predictions, same charges, cent. 30-50%
Pion-deuteron correlation function Pb-Pb \sqrt{sNN}=5.02 TeV with predictions, same charges, cent. 10-30%
Pion-deuteron correlation function Pb-Pb \sqrt{sNN}=5.02 TeV with predictions, same charges, cent. 0-10%
Pion-deuteron correlation function Pb-Pb \sqrt{sNN}=5.02 TeV with predictions, opposite charges, cent. 30-50%
Pion-deuteron correlation function Pb-Pb \sqrt{sNN}=5.02 TeV with predictions, opposite charges, cent. 10-30%
Pion-deuteron correlation function Pb-Pb \sqrt{sNN}=5.02 TeV with predictions, opposite charges, cent. 0-10%
Pion-deuteron correlation function Pb-Pb \sqrt{sNN}=5.02 TeV, opposite charges, cent. 30-50%
Pion-deuteron correlation function Pb-Pb \sqrt{sNN}=5.02 TeV, opposite charges, cent. 10-30%
Pion-deuteron correlation function Pb-Pb \sqrt{sNN}=5.02 TeV, opposite charges, cent. 0-10%
Pion-deuteron correlation function Pb-Pb \sqrt{sNN}=5.02 TeV, same charges, cent. 30-50%
Pion-deuteron correlation function Pb-Pb \sqrt{sNN}=5.02 TeV, same charges, cent. 10-30%
Pion-deuteron correlation function Pb-Pb \sqrt{sNN}=5.02 TeV, same charges, cent. 0-10%

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

Omega Ratio Of Individual Measurements To Combined Fit in pp 13TeV

Forward-backward multiplicity correlations in Pb-Pb and Xe-Xe collisions with strongly intensive quantity Σ

Ratio of the strongly intensive quantity Σ to MC HIJING in Xe-Xe collisions at √sNN = 5.44 TeV as a function of a distance between forward and backward intervals for 10% centrality bin width
Ratio of the strongly intensive quantity Σ to MC HIJING in Pb-Pb collisions at √sNN = 5.02 TeV as a function of a distance between forward and backward intervals for 10% centrality bin width
Ratio of the strongly intensive quantity Σ to MC HIJING in Pb-Pb collisions at √sNN = 2.76 TeV as a function of a distance between forward and backward intervals for 10% centrality bin width
The strongly intensive quantity Σ in Xe-Xe collisions at √sNN = 5.44 TeV as a function of a distance between forward and backward intervals for 10% centrality bin width
The strongly intensive quantity Σ in Pb-Pb collisions at √sNN = 5.02 TeV as a function of a distance between forward and backward intervals for 10% centrality bin width
The strongly intensive quantity Σ in Pb-Pb collisions at √sNN = 2.76 TeV as a function of a distance between forward and backward intervals for 10% centrality bin width
The strongly intensive quantity Σ in Pb-Pb and Xe-Xe collsions as a function of centrality

Lambda(1520) in pp collisions at 5.02 and 13 TeV

Lambda(1520)/Lambda yield ratio as a function of charged particle multiplicity
Corrected transverse momentum spectra of Lambda(1520) at 13 TeV
Lambda(1520) mean transverse momentum at \sqrt{s} = 5.02 and 13 TeV
Lambda(1520) pT integrated yield (dN/dy) at \srqt{s} = 5.02 TeV and 13 TeV
Corrected transverse momentum spectra of Lambda(1520) at 5.02TeV

Measurement of electrons from beauty-hadron decays in pp collisions at 13 TeV with TPC+TOF

Example of template fit using four templates in 6 < pT < 8 GeV/c
Example of template fit using four templates in 1.3 < pT < 1.5 GeV/c
Ratio of beauty decay electrons in pp collisions at 13 TeV with one in pp collisions at 5.02 TeV
Ratio of beauty decay electrons in pp collisions at 13 TeV with ones in pp at 2.76, 5.02, and 7 TeV
Ratio of beauty decay electrons to heavy-flavour decay electrons in pp collisions at 13 TeV
Cross section of beauty decay electrons in pp collisions at 13 TeV

Non-identical particle (pion-kaon) femtoscopy in Pb$-$Pb collisions at 5.02 TeV with ALICE

$R$ and $\mu$ vs $k_{\mathrm T}$
$R$ and $\mu$ vs $<{\mathrm d}{N_{\mathrm {ch}}}/{\mathrm d}\eta>^{1/3}$
Correlation functions for pion-kaon pairs with their fits for 20-30% centrality
Correlation functions for pion-kaon pairs with non-femtoscopic background for Pb$-$Pb collisions at $\sqrt{s_{\mathrm {NN}}}=5.02$ for 20$-$30% centrality

Charged K* multiplicity dependent analysis in pp collisions at $\sqrt{s} =$ 13 TeV with ALICE (ANA-1237)

K$^{*\pm}$/K$^0_{s}$ double ratio: high multiplicity K$^{*\pm}$/K$^0_{s}$ $p$\textsubscript{T} spectrum divided by the low multiplicity one
K$^{*\pm}$ and K$^{*0}$ $p_{\rm T}$-integrated yields
K$^{*\pm}$ and K$^{*0}$ mean $p_{\rm T}$ spectra
K$^{*\pm}$ and K$^{*0}$ $p$\textsubscript{T} spectra
K$^0_{s}\pi^{\pm}$ invariant mass distribution after the uncorrelated background subtraction
K$^0_{s}$ $\pi^{\pm}$ invariant mass distribution

Net-charge fluctuations nydyn[+,-] for various collision systems (EPS2021)

Effect of hadronic resonance decays: Δη dependence
Scaled nudyn[+,-] Vs dNch/deta
Comparison with lower energies
nudyn[+,-] dependence on Δη in different momentum ranges
Δη dependence of the nudyn[+,-]
nudyn[+,-] scaled by mean multiplicities of accepted particles

Hypertriton in pPb and pp

S_{3} in p-Pb and pp collisions
Hypertriton/$\Lambda$ in p-Pb and p-p

W production at midrapidity via single electrons in pp @ 13 TeV

Raw positrons from W candidates with isolation cuts in |y|<0.6 in pp collisions at 13 TeV
Raw electrons from W candidates with isolation cuts in |y|<0.6 in pp collisions at 13 TeV