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>
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
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
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
JPsi and Psi(2S) RAA as a function of pT with theory model
JPsi and Psi(2S) invariant mass plot "a la CMS" logarithmic scale
JPsi and Psi(2S) invariant mass plot "a la CMS" linear scale
JPsi and Psi(2S) RAA as a function of pT with theory model and CMS
$\it{p}_{T}$-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)
JPsi and Psi(2S) RAA as a function of pT
JPsi and Psi(2S) RAA as a function of centrality compared to theory curves
$\it{p}_{T}$-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)
JPsi and Psi(2S) RAA as a function of centrality
Psi(2S)/JPsi single and double ratio as a function of pT
Psi(2S)/JPsi single and double ratio as a function of centrality, compared to theory calculations and to the NA50 results
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
Invariant mass spectrum, JPsi and Psi(2S) region, in 0-20%
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
Comparisons to models for KNO variables in the trans-max region in pp collisions at sqrt(s) = 2.76 TeV
Comparisons to models for KNO variables in the transverse region in pp collisions at sqrt(s) = 2.76 TeV
Comparisons to models for charged particles multiplicity distributions in the trans-min region in pp collisions at sqrt(s) = 13 TeV
Comparisons to models for charged particles multiplicity distributions in the trans-max region in pp collisions at sqrt(s) = 13 TeV
Comparisons to models for charged particles multiplicity distributions in the transverse region in pp collisions at sqrt(s) = 13 TeV
Comparisons to models for charged particles multiplicity distributions in the trans-min region in pp collisions at sqrt(s) = 5.02 TeV
Comparisons to models for charged particles multiplicity distributions in the trans-max region in pp collisions at sqrt(s) = 5.02 TeV