Search for Preliminary Figures

Search for Preliminary Figures

Fraction of Women in ALICE by Employment Category and Time (2014-2021, Final)
  • PWG : Diversity Office
  • Energy: none
  • System none
Fraction of events with trigger particle vs multiplicity
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
R = 0.6, 0-10%, ML-based Raa
R = 0.4, 0-10%, ML-based vs. Area-based comparison
R = 0.2, 0-10%, ML-based and Area -Based Comparisons
Modelcomparisons
Raa R = 0.6, 30-50%, ML-based vs. area based comparisons
R = 0.4, 30-50%, Area-Based and ML comparison
R = 0.2, 30-50%, Area based and ML comparison
Raa for R = 0.6 30-50% with model comparisons
Raa for R = 0.2 30-50% with model comparisons
Raa for R = 0.4 30-50% with model comparisons
R=0.4 hadron+jet $\Delta\phi$ distribution for $20 < p_{\mathrm{T,jet}^{ch}} < 30$ GeV/c in 0-10% Pb-Pb collisions and pp collisions at $\sqrt{\it{s}_{NN}} = 5.02$ TeV compared to JETSCAPE and pQCD+NLO + Sudakov broadening calculation
R=0.2 hadron+jet $\Delta\phi$ distribution for $30 < p_{\mathrm{T,jet}^{ch}} < 50$ GeV/c in 0-10% Pb-Pb collisions and pp collisions at $\sqrt{\it{s}_{NN}} = 5.02$ TeV compared to JETSCAPE and pQCD+NLO + Sudakov broadening calculation
R=0.4 hadron+jet $\Delta\phi$ distribution for $30 < p_{\mathrm{T,jet}^{ch}} < 50$ GeV/c in 0-10% Pb-Pb collisions and pp collisions at $\sqrt{\it{s}_{NN}} = 5.02$ TeV compared to JETSCAPE and pQCD+NLO + Sudakov broadening calculation
Prompt J/ψ yields as a function of transverse momentum at most central collisions compared with ATLAS
Non-prompt J/ψ yields as a function of transverse momentum at most central collisions compared with ATLAS
Isolated photon differential cross section measured in p-Pb collisions at sqrt(s) = 5.02 TeV compared with JETPHOX and NLO theory
KNO variables in the transverse region in pp collisions at sqrt(s) = 2.76, 5.02, 7 and 13 TeV
Direct photon spectra PbPb 5TeV ratios to model calculation, with PHENIX, 20-40%
Charge conservation effect in first longitudinal coefficient a_{1} as a function of <dNch/deta> in Xe-Xe collisions
$p_T$ dependence of $J/\psi$ $v_2$ for various collision systems
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
Direct photon spectra in PbPb 5.02TeV from PCM with comparison to all model calculations
First longitudinal coefficient a_{1} in Xe-Xe and Pb-Pb collisions as a function of <dNch/deta>
Direct photon double ratio in PbPb 5.02TeV from PCM with all models
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
R=0.2 and R=0.4 hadron+jet $\Delta\phi$ distribution summary plot 0-10% Pb-Pb collisions and pp collisions at $\sqrt{\it{s}_{NN}} = 5.02$ TeV
Contour plot DPi scattering lengths compared to models
p-p-K$^{-}$ cumulant
p-p-K$^{-}$ correlation function compared to the lower-order contributions
p-p-K$^{-}$ total lower-order correlations
(p-K$^{-}$)-p correlation function
(p-p)-K$^{-}$ correlation function
p-p-K$^{-}$ correlation function
p-p-K$^{+}$ cumulant (projector method)
p-p-K$^{+}$ cumulant
p-p-K$^{+}$ correlation function compared to the lower-order contributions
p-p-K$^{+}$ correlation function compared to the lower-order contributions (projector method)
p-p-K$^{+}$ total lower-order correlations (data-driven approach VS projector method)
p-p-K$^{+}$ total lower-order correlations
(p-K$^{+}$)-p correlation function (data-driven approach VS projector method)
(p-K$^{+}$)-p correlation function
(p-p)-K$^{+}$ correlation function (data-driven approach VS projector method)
(p-p)-K$^{+}$ correlation function
p-p-K$^{+}$ correlation function
p-K$^{+}$ correlation function (Projected)
p-p correlation function (Projected)
p-K$^{+}$ correlation function
p-p correlation function
Prompt and non-prompt $J/\psi$ $R_{\rm AA}$ vs $< N_{part} >$ for integrated-$p_{\rm T}$ (1.5 $< p_{\rm T} < $ 10 GeV/$c$ ) in Pb-Pb collisions at 5.02 TeV
Non-prompt $J/\psi$ $R_{\rm AA}$ vs $p_{\rm T}$ for 0-10%, 10-30% and 30-50% centrality in Pb-Pb collisions at 5.02 TeV
Prompt $J/\psi$ $R_{\rm AA}$ vs $p_{\rm T}$ for 0-10%, 10-30% and 30-50% centrality in Pb-Pb collisions at 5.02 TeV
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
Truncated mean of momentum imbalance between isolated photons and jets in 5.02 TeV Pb-Pb collisions with PYTHIA comparison
Raa for R = 0.2 (0-10%) with model comparisons
Raa for R = 0.4 0-10% with Model Comparisons
Raa for R = 0.6 for 0-10% with Model Comparisons
Raa Ratios (R = 0.4)/(R = 0.2) 0-10% Model Comparisons
Raa Ratios (R = 0.6)/(R = 0.2) 0-10% Model Comparisons
dielectron mee spectrum and PHSD in 30-50%
dielectron mee spectrum and PHSD in 0-10%
dielectron pTee spectrum for 1.1 < mee < 2.7 GeV/c2 in 30-50% 3panels
dielectron pTee spectrum for 0.5 < mee < 1.1 GeV/c2 in 30-50% 3panels
dielectron pTee spectrum for 0.14 < mee < 0.5 GeV/c2 in 30-50% 3panels
dielectron pTee spectrum for 1.1 < mee < 2.7 GeV/c2 in 0-10% 3panels
dielectron pTee spectrum for 0.5 < mee < 1.1 GeV/c2 in 0-10% 3panels
dielectron pTee spectrum for 0.14 < mee < 0.5 GeV/c2 in 0-10% 3panels
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
$\it{p}_{T}$-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)
Comparisons to models for centre-of-mass energy dependence of the average charged-particle densities in the trans-min region in pp collisions at sqrt(s) = 2.76, 5.02, 7 and 13 TeV
Comparisons to models for centre-of-mass energy dependence of the average charged-particle densities in the trans-max region in pp collisions at sqrt(s) = 2.76, 5.02, 7 and 13 TeV
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
Comparisons to models for centre-of-mass energy dependence of the average charged-particle densities in the transverse region in pp collisions at sqrt(s) = 2.76, 5.02, 7 and 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
Comparison to parameterization for centre-of-mass energy dependence of the average charged-particle densities in the transverse, trans-max and trans-min regions
Centre-of-mass energy dependence of the average charged-particle densities in the transverse, trans-max and trans-min regions
Centre-of-mass energy dependence of the average charged-particle densities in the transverse region
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
Comparisons to models for KNO variables in the trans-min region in pp collisions at sqrt(s) = 13 TeV
Comparisons to models for KNO variables in the trans-max region in pp collisions at sqrt(s) = 13 TeV
Comparisons to models for KNO variables in the transverse region in pp collisions at sqrt(s) = 13 TeV
Comparisons to models for KNO variables in the trans-min region in pp collisions at sqrt(s) = 5.02 TeV
Comparisons to models for KNO variables in the trans-max region in pp collisions at sqrt(s) = 5.02 TeV
Comparisons to models for KNO variables in the transverse region in pp collisions at sqrt(s) = 5.02 TeV
Comparisons to models for KNO variables in the trans-min region in pp collisions at sqrt(s) = 2.76 TeV