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Public Preliminary figures by analysis

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

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

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

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

Cross section ratio for e+ <- W+ and e- <-W- as a function of pT in mid rapidity in pp collisions at 13 TeV
Cross section for e- <- W- in 30<pT,e<60 GeV/c in mid rapidity in pp collisions at 13 TeV
Cross section for e+ <- W+ in 30<pT,e<60 GeV/c in mid rapidity in pp collisions at 13 TeV
pT differential cross section for e- <- W- in mid-rapidity in pp collisions at 13 TeV
pT differential cross section for e+ <- W+ in mid-rapidity in pp collisions at 13 TeV

$\Xi$ 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)
Efficiency, purity, and subjet matching purity for the momentum splitting scale ln(kT)
Efficiency, purity, and subjet matching purity for the angular splitting scale ln(R/dR)
Response in momentum splitting scale ln(kt)
Response in angular scale ln(R/dR)

Flow and jet yield extraction from two-particle correlations in pp collisions at $\sqrt{s}=13$ TeV with ALICE

Near-side and away-side jet fragments as a function of multiplicity class with the Pythia8 description.
Near-side jet fragments as a function of multiplicity class with model descriptions
Near-side $\Delta\eta$ projections for various transverse momentum ranges in high-multiplicity and minimum bias pp collisions at 13 TeV with model descriptions,
v3 as a function of event-scale selection in high-multiplicity(0--0.1%) pp collisions at 13 TeV using template fit
v2 as a function of event-scale selection in high-multiplicity(0--0.1%) pp collisions at 13 TeV using template fit
v2 and v3 as a function of transverse momentum in high-multiplicity(0--0.1%) pp collisions at 13 TeV using template fit
Flow extraction using the template fit in high-multiplicity(0--0.1%) pp collisions at 13 TeV for 1$~<p_{\rm{T}}<~$2 GeV/$c$

Transverse momentum dependent flow vector fluctuations in Pb--Pb collisions at 5.02 TeV

Centrality dependence of the flow angle and magnitude fluctuations from v2{2}/v2[2]
Lower and upper limits of flow angle and flow magnitude fluctuations of v2{2}/v2[2] with etagap > 0.0 in centralities 0-5%, 10-20% and 30-40%
Lower and upper limits of flow angle and flow magnitude fluctuations of v2{2}/v2[2] with etagap > 0.0 in centralities 0-5%, 5-10%, 10-20%, 20-30%, 30-40% and 40-50%
<v2(pt)^2 v2^2>/<v2(pt)^2><v2^2> with etagap > 0.0 in centralities 0-5%, 10-20% and 30-40%
<v2(pt)^2 v2^2>/<v2(pt)^2><v2^2> with etagap > 0.0 in centralities 0-5%, 5-10%, 10-20%, 20-30%, 30-40% and 40-50%
F(Psi_2^a,\Psi_2) with etagap > 0.0 in centralities 0-5%, 10-20% and 30-40%
F(Psi_2^a,\Psi_2) with etagap > 0.0 in centralities 0-5%, 5-10%, 10-20%, 20-30%, 30-40% and 40-50%

Characterizing system dynamics with two-particle transverse momentum correlations in pp, p--Pb, and Pb--Pb collisions

Charged particle multiplicity evolution of the azimuthal widths of $G_{2}^{\rm CI}$ in pp collisions at $\sqrt{s} = 7$, p--Pb at $\sqrt{s_{\rm NN}} = 5.02$ and Pb--Pb at $\sqrt{s_{\rm NN}} = 2.76\;\text{TeV}$ compared to model predictions
Charged particle multiplicity evolution of the azimuthal widths of $G_{2}^{\rm CD}$ in pp collisions at $\sqrt{s} = 7$, p--Pb at $\sqrt{s_{\rm NN}} = 5.02$ and Pb--Pb at $\sqrt{s_{\rm NN}} = 2.76\;\text{TeV}$ compared to model predictions
Charged particle multiplicity evolution of the longitudinal widths of $G_{2}^{\rm CI}$ in pp collisions at $\sqrt{s} = 7$, p--Pb at $\sqrt{s_{\rm NN}} = 5.02$ and Pb--Pb at $\sqrt{s_{\rm NN}} = 2.76\;\text{TeV}$ compared to model predictions
Charged particle multiplicity evolution of the longitudinal widths of $G_{2}^{\rm CD}$ in pp collisions at $\sqrt{s} = 7$, p--Pb at $\sqrt{s_{\rm NN}} = 5.02$ and Pb--Pb at $\sqrt{s_{\rm NN}} = 2.76\;\text{TeV}$ compared to model predictions
Azimuthal projection of the two-particle transverse momentum correlation $G_{2}^{\rm CI}$ from 70--80% multiplicity class pp collisions at $\sqrt{s} = 7\;\text{TeV}$ compared to models
Azimuthal projection of the two-particle transverse momentum correlation $G_{2}^{\rm CI}$ from 30--40% multiplicity class pp collisions at $\sqrt{s} = 7\;\text{TeV}$ compared to models
Azimuthal projection of the two-particle transverse momentum correlation $G_{2}^{\rm CI}$ from 0--5% multiplicity class pp collisions at $\sqrt{s} = 7\;\text{TeV}$ compared to models
Azimuthal projection of the two-particle transverse momentum correlation $G_{2}^{\rm CD}$ from 70--80% multiplicity class pp collisions at $\sqrt{s} = 7\;\text{TeV}$ compared to models
Azimuthal projection of the two-particle transverse momentum correlation $G_{2}^{\rm CD}$ from 30--40% multiplicity class pp collisions at $\sqrt{s} = 7\;\text{TeV}$ compared to models
Azimuthal projection of the two-particle transverse momentum correlation $G_{2}^{\rm CD}$ from 0--5% multiplicity class pp collisions at $\sqrt{s} = 7\;\text{TeV}$ compared to models
Near side $(|\Delta\varphi|<\pi/2)$ longitudinal projection of the two-particle transverse momentum correlation $G_{2}^{\rm CI}$ from 70--80% multiplicity class pp collisions at $\sqrt{s} = 7\;\text{TeV}$ compared to models
Near side $(|\Delta\varphi|<\pi/2)$ longitudinal projection of the two-particle transverse momentum correlation $G_{2}^{\rm CI}$ from 30--40% multiplicity class pp collisions at $\sqrt{s} = 7\;\text{TeV}$ compared to models
Near side $(|\Delta\varphi|<\pi/2)$ longitudinal projection of the two-particle transverse momentum correlation $G_{2}^{\rm CI}$ from 0--5% multiplicity class pp collisions at $\sqrt{s} = 7\;\text{TeV}$ compared to models
Near side $(|\Delta\varphi|<\pi/2)$ longitudinal projection of the two-particle transverse momentum correlation $G_{2}^{\rm CD}$ from 70--80% multiplicity class pp collisions at $\sqrt{s} = 7\;\text{TeV}$ compared to models