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Public Preliminary figures by analysis

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

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

Direct photon R_gamma in PbPb 5.02TeV

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 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] - 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

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
nudyn[+,-] scaled by dNchdeta
nudyn[+,-] Vs dNch/deta for various collision systems

Hypertriton in pPb and pp

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

v2-[pt] correlation in Pb--Pb and pp collisions at 5.02 and 13 TeV

Correlation between v2 and [pT] of charged tracks in Pb--Pb and pp collisions at 5.02 and 13 TeV -- low multiplicity region -- pp only HM -- IPGlasma + pp models
Correlation between v2 and [pT] of charged tracks in Pb--Pb and pp collisions at 5.02 and 13 TeV -- low multiplicity region -- pp only HM -- IPGlasma+AMPT
Correlation between v2 and [pT] of charged tracks in Pb--Pb and pp collisions at 5.02 and 13 TeV -- low multiplicity region -- pp only HM
Correlation between v2, v3, and [pT] of charged tracks in Pb--Pb collisions at 5.02 TeV
v2 fluctuations in Pb--Pb and pp collisions at 5.02 and 13 TeV
Dynamic [pT] fluctuations in Pb--Pb and pp collisions at 5.02 and 13 TeV
Covariance of v2-[pT] in Pb--Pb and pp collisions at 5.02 and 13 TeV
Correlaiton between v2 and [pT] of charged tracks in Pb--Pb and pp collisions at 5.02 and 13 TeV
Dynamic [pT] fluctuations in Pb--Pb and pp collisions at 5.02 and 13 TeV -- low multiplicity region
v2 fluctuations in Pb--Pb and pp collisions at 5.02 and 13 TeV -- low multiplicity region
Covariance of v2-[pT] in Pb--Pb and pp collisions at 5.02 and 13 TeV -- low multiplicity region
Correlation between v2 and [pT] of charged tracks in Pb--Pb and pp collisions at 5.02 and 13 TeV -- low multiplicity region

Diversity Office May 2021 Figures

ALICE members by gender
Fraction of ALICE members with responsibility roles by region
Fraction of ALICE members with responsibility roles by region
ALICE members by region
ALICE fraction of women and men by responsibility

Measurement on in-jet production of $\Lambda _c$ baryons in pp collisions at $\sqrt{s} = 13$ TeV with radial displacement analysis for $\Lambda _c$ and $D^0$ tagged jets.

radial dependence for ratio Lc/D0 - tagged jets in pp at 13 TeV, data & PYTHIA 8, 6 < pT,HF < 12, 7 < pT,jet < 15
radial dependence for ratio Lc/D0 - tagged jets in pp at 13 TeV, data & PYTHIA 8, 2 < pT,HF < 6, 7 < pT,jet < 15
radial dependence for ratio Lc/D0 - tagged jets in pp at 13 TeV, data & PYTHIA 8, 2 < pT,HF < 6, 5 < pT,jet < 7
radial dependence Lc-tagged jets in pp at 13 TeV, data & PYTHIA 8, 2 < pT,HF < 6, 5 < pT,jet < 7
radial dependence Lc-tagged jets in pp at 13 TeV, data & PYTHIA 8, 2 < pT,HF < 6, 7 < pT,jet < 15
radial dependence Lc-tagged jets in pp at 13 TeV, data & PYTHIA 8, 6 < pT,HF < 12, 7 < pT,jet < 15
radial dependence D0-tagged jets in pp at 13 TeV, data & PYTHIA 8, 6 < pT,HF < 12, 7 < pT,jet < 15
radial dependence D0-tagged jets in pp at 13 TeV, data & PYTHIA 8, 2 < pT,HF < 6, 7 < pT,jet < 15
radial dependence D0-tagged jets in pp at 13 TeV, data & PYTHIA 8, 2 < pT,HF < 6, 5 < pT,jet < 7

D-meson self normalised yields in pp collisions at 13 TeV

Average prompt D-meson, Jpsi and HFe self normalised yields vs relative charged-particle multiplicity at central rapidity in pp at 13 TeV (D mesons for 8 < pT < 12 GeV/c)
Average prompt D-meson, Jpsi and HFe self normalised yields vs relative charged-particle multiplicity at central rapidity in pp at 13 TeV (D mesons for 2 < pT < 4 GeV/c)
Comparison of data with models: Average D-meson double ratios vs charged-particle multiplicity in pp 13 TeV
Average D-meson double ratios vs relative charged-particle multiplicity in pp at 13 TeV
Comparison of data with models: Average D-meson self normalised yields vs charged-particle multiplicity in pp 13 TeV
Comparison of average D-meson self nomalised yields vs relative charged-particle multiplicity in pp 13 TeV with pp 7 TeV
Average D-meson self normalised yields vs relative charged-particle multiplicity in pp at 13 TeV
K0s-Antip correlation function Kyoto + AJ 1 model
  • Fig. Group :
  • PWG : PWG-CF (Flow and Correlations)
  • Energy: 13 TeV
  • System: p-p
K0s-p + K0s-Antip correlation function Kyoto + AJ 1 model
  • Fig. Group :
  • PWG : PWG-CF (Flow and Correlations)
  • Energy: 13 TeV
  • System: p-p
K0s-p + K0s-Antip correlation function Kyoto + AJ 2 model
  • Fig. Group :
  • PWG : PWG-CF (Flow and Correlations)
  • Energy: 13 TeV
  • System: p-p
K0s-Antip correlation function Kyoto + AJ 2 model
  • Fig. Group :
  • PWG : PWG-CF (Flow and Correlations)
  • Energy: 13 TeV
  • System: p-p
K0s-p correlation function Kyoto + AJ 2 model
  • Fig. Group :
  • PWG : PWG-CF (Flow and Correlations)
  • Energy: 13 TeV
  • System: p-p
K0s-p correlation function Kyoto + AJ 1 model
  • Fig. Group :
  • PWG : PWG-CF (Flow and Correlations)
  • Energy: 13 TeV
  • System: p-p
K0s-Antip correlation function Lednicky
  • Fig. Group :
  • PWG : PWG-CF (Flow and Correlations)
  • Energy: 13 TeV
  • System: p-p
K0s-p correlation function Lednicky
  • Fig. Group :
  • PWG : PWG-CF (Flow and Correlations)
  • Energy: 13 TeV
  • System: p-p

$\Xi$ baryon production vs multiplicity and effective energy in pp $\sqrt{s}$ = 13 TeV

Ratio of $\Xi^{-}$ + $\bar{\Xi}^{+}$ yields in V0M selections in two ($\sqrt{s}$ - ZDC) ranges (high and low) to the average charged multiplicity (self-normalised to INEL>0) as a function of the percentile estimator
Ratio of $\Xi^{-}$ + $\bar{\Xi}^{+}$ yields in V0M selections in two ($\sqrt{s}$ - ZDC) ranges (high and low) to the average charged multiplicity as a function of the percentile estimator
Ratio of $\Xi^{-}$ + $\bar{\Xi}^{+}$ yields in ($\sqrt{s}$ - ZDC) selections in two V0M ranges (high and low) to the average charged multiplicity (self-normalised to INEL>0) as a function of the percentile estimator
Ratio of $\Xi^{-}$ + $\bar{\Xi}^{+}$ yields in ($\sqrt{s}$ - ZDC) selections in two V0M ranges (high and low) to the average charged multiplicity as a function of the percentile estimator
Ratio of $\Xi^{-}$ + $\bar{\Xi}^{+}$ yields in V0M selections in two ($\sqrt{s}$ - ZDC) ranges (high and low) to the average charged multiplicity (self-normalised to INEL>0) as a function of the charged particle multiplicity at midrapidity
Ratio of $\Xi^{-}$ + $\bar{\Xi}^{+}$ yields in V0M selections in two ($\sqrt{s}$ - ZDC) ranges (high and low) to the average charged multiplicity as a function of the charged particle multiplicity at midrapidity
Ratio of $\Xi^{-}$ + $\bar{\Xi}^{+}$ yields in ($\sqrt{s}$ - ZDC) selections in two V0M ranges (high and low) to the average charged multiplicity self-normalised to INEL>0 as a function of the charged particle multiplicity at midrapidity
Ratio of $\Xi^{-}$ + $\bar{\Xi}^{+}$ yields in ($\sqrt{s}$ - ZDC) selections in two V0M ranges (high and low) to the average charged multiplicity as a function of the particle multiplicity
Ratio $\Xi^{-}$ + $\bar{\Xi}^{+}$ yields to multiplicity (self-normalised to INEL>0) as a function of the percentile selection
Ratio of $\Xi^{-}$ + $\bar{\Xi}^{+}$ yields to multiplicity (self-normalised to INEL>0) as a function of the average charged particle multiplicity
$\Xi^{-}$ + $\bar{\Xi}^{+}$ $p_{\text{T}}$-spectra in ($\sqrt{s}$ - ZDC) and V0M classes in pp collisions at $\sqrt{s}$ = 13 TeV

Derived plots: Nuclear modification factor of light neutral-meson spectra up to high transverse momentum in p-Pb collisions at $\sqrt{s_{\rm NN}}= 8.16$ TeV

Nuclear modification factor of $\pi^0$ meson and charged hadron spectra in p-Pb collisions at $\sqrt{s_{\rm NN}}= 5.02$ and $8.16$ TeV and in central Pb-Pb collisions at $\sqrt{s_{\rm NN}}= 5.02$ TeV

The Lund plane in pp collisions at 13 TeV with ALICE

Lund plane density unfolded/raw distribution
The unfolded Lund plane in pp collisions
Momentum splitting scale projection ln(kT) for narrow angle splittings
Momentum splitting scale projection ln(kT) for wide angle splittings
Momentum splitting scale projection ln(kT)
Angular splitting scale projection ln(R/dR) for mostly perturbative splittings
Angular splitting scale projection ln(R/dR) for mostly non-perturbative splittings
Angular splitting scale projection ln(R/dR)