User

Roles
Anonymous

Public Preliminary figures by analysis

Public Preliminary figures by analysis

Hypertriton in pPb and pp

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

v2 of jet particles in p-Pb and Pb-Pb collisions at 5.02 TeV

The comparisons between the jet particle v2 and inclusive v2 in p-Pb and Pb-Pb collisions, simplified version1 (scaled Pb-Pb v2)
The comparisons between the jet particle v2 and inclusive v2 in p-Pb and Pb-Pb collisions, simplified version1 (scaled p-Pb v2)
The comparisons between the jet particle v2 and inclusive v2 in p-Pb and Pb-Pb collisions, and jet v2 in Pb-Pb collisions
The comparisons between the jet particle v2 and inclusive v2 in p-Pb and Pb-Pb collisions
The jet particle v2 as the function of trigger particle pT, compare to inclusive v2, in Pb-Pb collisions
The jet particle v2 as the function of trigger particle pT, compare to new inclusive v2, in p-Pb collisions
The TPC-TPC correlation and related fit in 4< \it{p}_{\rm T}(trig)<5 GeV/\it{c}, 2< \it{p}_{\rm T}(assoc) in Pb-Pb collisions

Nuclear deformation in Pb-Pb and Xe-Xe collisions

rho(v3^2, [pT]) in Xe-Xe collisions as function of centrality with TRENTo-based initial and final state calculations
rho(v2^2, [pT]) in Xe-Xe collisions as function of centrality with TRENTo-based initial and final state calculations
rho(v3^2, [pT]) in Pb-Pb collisions as function of centrality with TRENTo-based initial and final state calculations
rho(v2^2, [pT]) in Pb-Pb collisions as function of centrality with TRENTo-based initial and final state calculations
rho(v3^2, [pT]) in Pb-Pb collisions as function of centrality with IP-Glasma-based initial and final state calculations
rho(v3^2, [pT]) in Xe-Xe collisions as function of centrality with IP-Glasma-based initial and final state calculations
rho(v2^2, [pT]) in Xe-Xe collisions as function of centrality with IP-Glasma-based initial and final state calculations
rho(v2^2, [pT]) in Pb-Pb collisions as function of centrality with IP-Glasma-based initial and final state calculations
rho(v3^2, [pT]) in Xe-Xe collisions as function of centrality with initial state calculations
rho(v3^2, [pT]) in Pb-Pb collisions as function of centrality with initial state calculations
rho(v3^2, [pT]) in Xe-Xe collisions as function of centrality with hydrodynamic calculations
rho(v3^2, [pT]) in Pb-Pb collisions as function of centrality with hydrodynamic calculations
rho(v2^2, [pT]) in Xe-Xe collisions as function of centrality with initial state calculations
rho(v2^2, [pT]) in Pb-Pb collisions as function of centrality with initial state calculations
rho(v2^2, [pT]) in Xe-Xe collisions as function of centrality with hydrodynamic calculations
rho(v2^2, [pT]) in Pb-Pb collisions as function of centrality with hydrodynamic calculations
rho(v2^2,v3^2,[pt]) in Pb-Pb collisions as function of centrality
rho(v2^2, [pT]) in Pb-Pb as function of centrality with various centrality estimation methods with 0.5 < pt < 5.0 GeV/c
rho(v2^2, [pT]) in Pb-Pb as function of centrality with various centrality estimation methods with 0.2 < pt < 3.0 GeV/c
rho(v2^2, [pT]) in Pb-Pb as function of centrality with various eta ranges
rho(v2^2, [pT]) in Pb-Pb as function of centrality with various pT ranges
v3-delta pT in Pb-Pb and Xe-Xe collisions at 0-1% centrality
v2-delta pT in Pb-Pb and Xe-Xe collisions at 0-1% centrality
rho(v3^2, [pT]) in Pb-Pb and Xe-Xe collisions as function of centrality with TRENTo-based initial and final state calculations
rho(v2^2, [pT]) in Pb-Pb and Xe-Xe collisions as function of centrality with TRENTo-based initial and final state calculations
rho(v3^2, [pT]) in Pb-Pb and Xe-Xe collisions as function of centrality with IP-Glasma-based initial and final state calculations
rho(v2^2, [pT]) in Pb-Pb and Xe-Xe collisions as function of centrality with IP-Glasma-based initial and final state calculations
rho(v3^2, [pT]) in Pb-Pb and Xe-Xe collisions as function of centrality with initial state calculations
rho(v2^2, [pT]) in Pb-Pb and Xe-Xe collisions as function of centrality with initial state calculations
rho(v3^2, [pT]) in Pb-Pb and Xe-Xe collisions as function of centrality with hydrodynamic calculations
rho(v2^2, [pT]) in Pb-Pb and Xe-Xe collisions as function of centrality with hydrodynamic calculations

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

V0-h & h-h correlations in pp and Pb-Pb at 5.02TeV

Away-side yield ratio of $(\Lambda+\bar{\Lambda})$-h/h-h correlations in pp $\sqrt{s} = $ 5.02 TeV Model Comparison
Near-side yield ratio of $(\Lambda+\bar{\Lambda})$-h/h-h correlations in pp $\sqrt{s} = $ 5.02 TeV Model Comparison
Away-side yield ratio of $(\Lambda+\bar{\Lambda})$-h/h-h correlations in Pb$-$Pb (0$-$10$\%$) at $\sqrt{s_{\rm NN}} = $ 5.02 TeV Model Comparison
Near-side yield ratio of $(\Lambda+\bar{\Lambda})$-h/h-h correlations in Pb$-$Pb (0$-$10$\%$) at $\sqrt{s_{\rm NN}} = $ 5.02 TeV Model Comparison
Away-side yield ratio of $\rm{K}^{0}_{s}$-h/h-h correlations in pp $\sqrt{s} = $ 5.02 TeV Model Comparison
Near-side yield ratio of $\rm{K}^{0}_{s}$-h/h-h correlations in pp $\sqrt{s} = $ 5.02 TeV Model Comparison
Away-side yield ratio of $\rm{K}^{0}_{s}$-h/h-h correlations in Pb$-$Pb (0$-$10$\%$) at $\sqrt{s_{\rm NN}} = $ 5.02 TeV Model Comparison
Near-side yield ratio of $\rm{K}^{0}_{s}$-h/h-h correlations in Pb$-$Pb (0$-$10$\%$) at $\sqrt{s_{\rm NN}} = $ 5.02 TeV Model Comparison
Away-side $\it{I}_{\rm AA}$ of h-h correlations in Pb$-$Pb (0$-$10$\%$) at $\sqrt{s_{\rm NN}} = $ 5.02 TeV Model Comparison
Near-side $\it{I}_{\rm AA}$ of h-h correlations in Pb$-$Pb (0$-$10$\%$) at $\sqrt{s_{\rm NN}} = $ 5.02 TeV Model Comparison
Away-side $\it{I}_{\rm AA}$ of $(\Lambda+\bar{\Lambda})$-h correlations in Pb$-$Pb (0$-$10$\%$) at $\sqrt{s_{\rm NN}} = $ 5.02 TeV Model Comparison
Near-side $\it{I}_{\rm AA}$ of $(\Lambda+\bar{\Lambda})$-h correlations in Pb$-$Pb (0$-$10$\%$) at $\sqrt{s_{\rm NN}} = $ 5.02 TeV Model Comparison
Away-side $\it{I}_{\rm AA}$ of $\rm{K}^{0}_{s}$-h correlations in Pb$-$Pb (0$-$10$\%$) at $\sqrt{s_{\rm NN}} = $ 5.02 TeV Model Comparison
Near-side $\it{I}_{\rm AA}$ of $\rm{K}^{0}_{s}$-h correlations in Pb$-$Pb (0$-$10$\%$) at $\sqrt{s_{\rm NN}} = $ 5.02 TeV Model Comparison
Away-side yield of h-h correlations in pp $\sqrt{s} = $ 5.02 TeV Model Comparison
Near-side yield of h-h correlations in pp $\sqrt{s} = $ 5.02 TeV Model Comparison
Away-side yield of h-h correlations in Pb$-$Pb (0$-$10$\%$) at $\sqrt{s_{\rm NN}} = $ 5.02 TeV Model comparison
Near-side yield of h-h correlations in Pb$-$Pb (0$-$10$\%$) at $\sqrt{s_{\rm NN}} = $ 5.02 TeV Model comparison
Away-side yield of $(\Lambda+\bar{\Lambda})$-h correlations in pp $\sqrt{s} = $ 5.02 TeV Model Comparison
Near-side yield of $(\Lambda+\bar{\Lambda})$-h correlations in pp $\sqrt{s} = $ 5.02 TeV Model Comparison
Away-side yield of $(\Lambda+\bar{\Lambda})$-h correlations in Pb$-$Pb (0$-$10$\%$) at $\sqrt{s_{\rm NN}} = $ 5.02 TeV Model comparison
Near-side yield of $(\Lambda+\bar{\Lambda})$-h correlations in Pb$-$Pb (0$-$10$\%$) at $\sqrt{s_{\rm NN}} = $ 5.02 TeV Model comparison
Away-side yield of $\rm{K}^{0}_{s}$-h correlations in pp $\sqrt{s} = $ 5.02 TeV Model Comparison
Near-side yield of $\rm{K}^{0}_{s}$-h correlations in pp $\sqrt{s} = $ 5.02 TeV Model Comparison
Away-side yield of $\rm{K}^{0}_{s}$-h correlations in Pb$-$Pb (0$-$10$\%$) at $\sqrt{s_{\rm NN}} = $ 5.02 TeV Model Comparison
Near-side yield of $\rm{K}^{0}_{s}$-h correlations in Pb$-$Pb (0$-$10$\%$) at $\sqrt{s_{\rm NN}} = $ 5.02 TeV Model Comparison
Away-side yield ratios of $\rm{K}^{0}_{s}$-h/h-h and $(\Lambda+\bar{\Lambda})$-h/h-h correlations in pp $\sqrt{s} = $ 5.02 TeV
Near-side yield ratios of $\rm{K}^{0}_{s}$-h/h-h and $(\Lambda+\bar{\Lambda})$-h/h-h correlations in pp $\sqrt{s} = $ 5.02 TeV
Away-side yield ratios of $\rm{K}^{0}_{s}$-h/h-h and $(\Lambda+\bar{\Lambda})$-h/h-h correlations in Pb$-$Pb (0$-$10$\%$) at $\sqrt{s_{\rm NN}} = $ 5.02 TeV
Near-side yield ratios of $\rm{K}^{0}_{s}$-h/h-h and $(\Lambda+\bar{\Lambda})$-h/h-h in Pb$-$Pb (0$-$10$\%$) at $\sqrt{s_{\rm NN}} = $ 5.02 TeV
Away-side $\it{I}_{\rm AA}$ of h-h correlations in Pb$-$Pb (0$-$10$\%$) at $\sqrt{s_{\rm NN}} = $ 5.02 TeV Compare to published.
Near-side $\it{I}_{\rm AA}$ of h-h correlations in Pb$-$Pb (0$-$10$\%$) at $\sqrt{s_{\rm NN}} = $ 5.02 TeV Compare to published.
Away-side $\it{I}_{\rm AA}$ of $\rm{K}^{0}_{s}-$h ,$(\Lambda+\bar{\Lambda})-$h and h-h correlations in Pb$-$Pb (0$-$10$\%$) at $\sqrt{s_{\rm NN}} = $ 5.02 TeV
Near-side $\it{I}_{\rm AA}$ of $\rm{K}^{0}_{s}-$h ,$(\Lambda+\bar{\Lambda})-$h and h-h correlations in Pb$-$Pb (0$-$10$\%$) at $\sqrt{s_{\rm NN}} = $ 5.02 TeV
$\Delta\varphi$ distributions of $\rm{K}^{0}_{s}-$h,$(\Lambda+\bar{\Lambda})-$h and h-h correlations in Pb$-$Pb (0$-$10$\%$) at $\sqrt{s_{\rm NN}} = $ 5.02 TeV
$\Delta\varphi$ distribution of $\rm{K}^{0}_{s}-$h,$(\Lambda+\bar{\Lambda})-$h and h-h correlations in pp $\sqrt{s} = $ 5.02 TeV
Away-side yield of $\rm{K}^{0}_{s}-$h,$(\Lambda+\bar{\Lambda})-$h and h-h correlations in pp $\sqrt{s} = $ 5.02 TeV
Near-side yield of $\rm{K}^{0}_{s}-$h , $(\Lambda+\bar{\Lambda})-$h and h-h correlations in pp $\sqrt{s} = $ 5.02 TeV
Near-side yield of $\rm{K}^{0}_{s}-$h ,$(\Lambda+\bar{\Lambda})-$h and h-h correlations in Pb$-$Pb (0$-$10$\%$) at $\sqrt{s_{\rm NN}} = $ 5.02 TeV
Away-side yield of $\rm{K}^{0}_{s}-$h ,$(\Lambda+\bar{\Lambda})-$h and h-h correlations in Pb$-$Pb (0$-$10$\%$) at $\sqrt{s_{\rm NN}} = $ 5.02 TeV

Measurements of inclusive and leading subjet fragmentation in pp and Pb–Pb collisions at 5.02 TeV

Leading subjet fragmentation in Pb-Pb collisions, r=0.2
Leading subjet fragmentation in Pb-Pb collisions, r=0.1
Inclusive subjet fragmentation in pp collisions
Leading subjet fragmentation in pp collisions

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

Xi-pi and Xi-K correlations in pp collisions at 13 TeV

$\Xi-\rm K$ correlations projected in $\Delta\varphi$, multiplicity dependence

Xi-baryon correlations at 13 TeV

$\Xi-\rm p$ correlations projected in $\Delta\varphi$, multiplicity dependence