Search for Preliminary Figures

Measurement of the groomed jet mass for $R=0.2$ charged-particle jets in $80 < p_\text{T}^\text{ch jet} < 100$ GeV/$c$ in Pb-Pb collisions at $\sqrt{s_\text{NN}}=5.02$ TeV as compared to pp baseline
Measurement of the groomed jet mass for $R=0.2$ charged-particle jets in $60 < p_\text{T}^\text{ch jet} < 80$ GeV/$c$ in Pb-Pb collisions at $\sqrt{s_\text{NN}}=5.02$ TeV as compared to pp baseline
Measurement of the groomed jet mass for $R=0.2$ charged-particle jets in $40 < p_\text{T}^\text{ch jet} < 60$ GeV/$c$ in Pb-Pb collisions at $\sqrt{s_\text{NN}}=5.02$ TeV as compared to pp baseline
Measurement of the ungroomed jet mass for $R=0.2$ charged-particle jets in $80 < p_\text{T}^\text{ch jet} < 100$ GeV/$c$ in Pb-Pb collisions at $\sqrt{s_\text{NN}}=5.02$ TeV as compared to pp baseline
Measurement of the ungroomed jet mass for $R=0.2$ charged-particle jets in $60 < p_\text{T}^\text{ch jet} < 80$ GeV/$c$ in Pb-Pb collisions at $\sqrt{s_\text{NN}}=5.02$ TeV as compared to pp baseline
Measurement of the ungroomed jet mass for $R=0.2$ charged-particle jets in $40 < p_\text{T}^\text{ch jet} < 60$ GeV/$c$ in Pb-Pb collisions at $\sqrt{s_\text{NN}}=5.02$ TeV as compared to pp baseline
Measurement of the groomed jet mass in Pb-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV from $100 < p_\mathrm{T}^\mathrm{ch\;jet} < 150$ GeV/$c$ with $R=0.2$
Measurement of the groomed jet mass in Pb-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV from $80 < p_\mathrm{T}^\mathrm{ch\;jet} < 100$ GeV/$c$ with $R=0.2$
Measurement of the groomed jet mass in Pb-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV from $60 < p_\mathrm{T}^\mathrm{ch\;jet} < 80$ GeV/$c$ with $R=0.2$
Measurement of the groomed jet mass in Pb-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV from $40 < p_\mathrm{T}^\mathrm{ch\;jet} < 60$ GeV/$c$ with $R=0.2$
Measurement of the groomed jet mass in pp collisions at $\sqrt{s} = 5.02$ TeV from $80 < p_\mathrm{T}^\mathrm{ch\;jet} < 100$ GeV/$c$ with $R=0.2$
Measurement of the groomed jet mass in pp collisions at $\sqrt{s} = 5.02$ TeV from $60 < p_\mathrm{T}^\mathrm{ch\;jet} < 80$ GeV/$c$ with $R=0.2$
Measurement of the groomed jet mass in pp collisions at $\sqrt{s} = 5.02$ TeV from $40 < p_\mathrm{T}^\mathrm{ch\;jet} < 60$ GeV/$c$ with $R=0.2$
Measurement of the ungroomed jet mass in pp collisions at $\sqrt{s} = 5.02$ TeV from $80 < p_\mathrm{T}^\mathrm{ch\;jet} < 100$ GeV/$c$ with $R=0.2$
Measurement of the ungroomed jet mass in pp collisions at $\sqrt{s} = 5.02$ TeV from $60 < p_\mathrm{T}^\mathrm{ch\;jet} < 80$ GeV/$c$ with $R=0.2$
Measurement of the ungroomed jet mass in pp collisions at $\sqrt{s} = 5.02$ TeV from $40 < p_\mathrm{T}^\mathrm{ch\;jet} < 60$ GeV/$c$ with $R=0.2$
Measurement of the ungroomed jet mass in Pb-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV from $100 < p_\mathrm{T}^\mathrm{ch\;jet} < 150$ GeV/$c$ with $R=0.2$
Measurement of the ungroomed jet mass in Pb-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV from $80 < p_\mathrm{T}^\mathrm{ch\;jet} < 100$ GeV/$c$ with $R=0.2$
Measurement of the ungroomed jet mass in Pb-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV from $60 < p_\mathrm{T}^\mathrm{ch\;jet} < 80$ GeV/$c$ with $R=0.2$
Measurement of the ungroomed jet mass in Pb-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV from $40 < p_\mathrm{T}^\mathrm{ch\;jet} < 60$ GeV/$c$ with $R=0.2$
Omega over pion ratio as a function of the pion yield in pp collisions at 9 GeV, 7 TeV and 13.6 TeV
  • PWG : PWG-LF (Light Flavour Spectra)
  • Energy: 900 GeV
  • ,
  • Energy: 7 TeV
  • ,
  • Energy: 13.6 TeV
  • System p-p
Kaon over pion ratio as a function of pT in pp collisions at 900 GeV, 13 TeV and 13.6 TeV with Run 3 data
  • PWG : PWG-LF (Light Flavour Spectra)
  • Energy: 900 GeV
  • System p-p
Proton over pion ratio as a function of pT in pp collisions at 900 GeV, 13 TeV and 13.6 TeV with Run 3 data
BR ratio comparisons of $\Omega_{\rm c}^{0}$
Xic/D0 and Xic/Lc ratio in low and high V0M multiplicity classes compared to PYTHIA
Invariant mass distribution of Xic in high multiplicity class
Prompt efficiency of Xic for different multiplicity classes
Away-Side Nuclear Modification factor ($I_{AA}$) of Pb-Pb in 0 - 10% Centrality compared to LF $I_{AA}$
Near-Side Nuclear Modification factor ($I_{AA}$) of Pb-Pb in 0 - 10% Centrality compared to LF $I_{AA}$
Charged jet $R_{AA}$ for R = 0.3 measured in central Pb-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV: Comparison to STAR $R_{AA}$
Charged jet $R_{AA}$ for R = 0.3 measured in central Pb-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV: Comparison to previous ALICE $R_{AA}$ measured with 2015 Pb-Pb data
Charged jet $R_{AA}$ for R = 0.3 measured in central Pb-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV
Corrected charged jet distributions with $p_{T}^{lead} > 3$ GeV/c and $p_{T}^{lead} > 4$ GeV/c for central Pb-Pb collisions at 5.02 TeV
Response matrix for R=0.3 jets with $p_{T}^{lead} > 4$ GeV/c in central Pb-Pb collisions at 5.02 TeV
Response matrix for R=0.3 jets with $p_{T}^{lead} > 3$ GeV/c in central Pb-Pb collisions at 5.02 TeV
Raw correlated quasi-inclusive jet $p_{T,jet}^{reco}$ distribution with $p_{T}^{lead} > 3$ GeV/c for central Pb-Pb collisions at 5.02 TeV
Raw correlated quasi-inclusive jet $p_{T,jet}^{reco}$ distribution with $p_{T}^{lead} > 4$ GeV/c for central Pb-Pb collisions at 5.02 TeV
Raw quasi-inclusive jet $p_{T,jet}^{reco}$ distribution of the SE and ME with $p_{T}^{lead} > 3$ GeV/c for central Pb-Pb collisions at 5.02 TeV
Raw quasi-inclusive jet $p_{T,jet}^{reco}$ distribution of the SE and ME with $p_{T}^{lead} > 4$ GeV/c for central Pb-Pb collisions at 5.02 TeV
Lc/D0_vs_multiplcity_pt_pPb_5.02TeV
D0_corrected_yield_pPb_5.02TeV
Lc_corrected_yield_pPb_5.02TeV
Delta Phi Distribution of heavy-flavor decay electrons and charged particles, Pb-Pb 30 - 50% Centrality and pp, 2 pT bins
Delta Phi Distribution of heavy-flavor decay electrons and charged particles, Pb-Pb 0 - 10% Centrality and pp, 2 pT bins
Delta Phi Distribution of heavy-flavor decay electrons and charged particles with background uncertainty, Pb-Pb 0 - 10%, 2 pT bins
Ratio of the $j_\mathrm{T}$ distributions in high $z$ to the $j_\mathrm{T}$ distributions in inclusive $z$
Ratio of the $j_\mathrm{T}$ distributions in low $z$ to the $j_\mathrm{T}$ distributions in inclusive $z$
$j_\mathrm{T}$ distributions in $60 < p_\mathrm{T,jet}^\mathrm{ch} < 100 \;\mathrm{ GeV}/c$ in differential $z$ compared to HERWIG7
$j_\mathrm{T}$ distributions in $40 < p_\mathrm{T,jet}^\mathrm{ch} < 60 \;\mathrm{ GeV}/c$ in differential $z$ compared to HERWIG7
$j_\mathrm{T}$ distributions in $20 < p_\mathrm{T,jet}^\mathrm{ch} < 40 \;\mathrm{ GeV}/c$ in differential $z$ compared to HERWIG7
$j_\mathrm{T}$ distributions in $10 < p_\mathrm{T,jet}^\mathrm{ch} < 20 \;\mathrm{ GeV}/c$ in differential $z$ compared to HERWIG7
$j_\mathrm{T}$ distributions in $10 < p_\mathrm{T,jet}^\mathrm{ch} < 20 \;\mathrm{ GeV}/c$ in differential $z$ compared to PYTHIA8 Monash
$j_\mathrm{T}$ distributions in $20 < p_\mathrm{T,jet}^\mathrm{ch} < 40 \;\mathrm{ GeV}/c$ in differential $z$ compared to PYTHIA8 Monash
$j_\mathrm{T}$ distributions in $40 < p_\mathrm{T,jet}^\mathrm{ch} < 60 \;\mathrm{ GeV}/c$ in differential $z$ compared to PYTHIA8 Monash
$j_\mathrm{T}$ distributions in $60 < p_\mathrm{T,jet}^\mathrm{ch} < 100 \;\mathrm{ GeV}/c$ in differential $z$ compared to PYTHIA8 Monash
Jet $p_\mathrm{T}$ dependence of $j_\mathrm{T}$ distributions in inclusive $z$
Jet $p_\mathrm{T}$ dependence of $j_\mathrm{T}$ distributions in low $z$
Jet $p_\mathrm{T}$ dependence of $j_\mathrm{T}$ distributions in mid $z$
Jet $p_\mathrm{T}$ dependence of $j_\mathrm{T}$ distributions in high $z$
Invariant mass distribution of Xic+ in high multiplicity class
ROC curve for high multiplicity, transverse momentum 6 to 8 GeV interval
BDT output distribution in high multiplicity, transverse momentum 6 to 8 GeV interval
Prompt efficiency of Xic+ for different multiplicity classes
Xic+ over D0 for different multiplicity classes
Corrected yield of Xic+ for different multiplicity classes with ratio to INEL>0 classes
Corrected yield of \Xi_c^0 in different V0M multiplicity classes
Csic0/D0 and Csic+/D0 ratio in low and high V0M multiplicity classes
Xic/Lc ratio in low and high V0M multiplicity classes
Xic/D0 ratio in low and high V0M multiplicity classes
Xic/Lc ratio measured in \pp collisions at 13TeV in different multiplicity
Xi_c^0/D^0 ratio in different V0M multiplicity classes
psi and jpsi signal extraction from 13.6 TeV pp data
psi-to-jpsi ratio as function of the pT at midrapidity in pp at 13.6 TeV, compared with the similar measurements from forward rapidity
y-differential coherent J/psi photoproduction cross section at pT < 0.3 GeV/c in the centrality range (70-90)% in Pb-Pb collisions at 5.02 TeV with data points only
y-differential raw J/psi yield as a function of pT in the centrality range (70-90)% in Pb-Pb collisions at 5.02 TeV
y-differential J/psi production cross section at forward y as a function of pT in pp collisions at 5.02 TeV
The J/psi nuclear modification factor as a function of pT in the centrality range (70-90)% in Pb-Pb collisions at 5.02 TeV for 3.75 < y < 4
The J/psi nuclear modification factor as a function of pT in the centrality range (70-90)% in Pb-Pb collisions at 5.02 TeV for 3.5 < y < 3.75
The J/psi nuclear modification factor as a function of pT in the centrality range (70-90)% in Pb-Pb collisions at 5.02 TeV for 3.25 < y < 3.5
The J/psi nuclear modification factor as a function of pT in the centrality range (70-90)% in Pb-Pb collisions at 5.02 TeV for 3 < y < 3.25
The J/psi nuclear modification factor as a function of pT in the centrality range (70-90)% in Pb-Pb collisions at 5.02 TeV for 2.75 < y < 3
The J/psi nuclear modification factor as a function of pT in the centrality range (70-90)% in Pb-Pb collisions at 5.02 TeV for 2.5 < y < 2.75
The J/psi nuclear modification factor for six y intervals at forward rapidity as a function of pT, pT < 3 GeV/c, in the centrality range (70-90)% in Pb-Pb collisions at 5.02 TeV
The J/psi nuclear modification factor for six y intervals at forward rapidity as a function of pT in the centrality range (70-90)% in Pb-Pb collisions at 5.02 TeV
y-differential coherent J/psi photoproduction cross section at pT < 0.3 GeV/c in the centrality range (70-90)% in Pb-Pb collisions at 5.02 TeV compared with one set of models of different scenarios
y-differential coherent J/psi photoproduction cross section at pT < 0.3 GeV/c in the centrality range (70-90)% in Pb-Pb collisions at 5.02 TeV
Eta/Pi0 ratio as function of z for different jet pT intervals
Ratio of Pi0 z spectra (Fragmentation function) for data and PYTHIA to parameterization
Eta/Pi0 ratio inside jets as function of pT for different jet pT intervals
Ratio of fully corrected Eta pT spectra inside jets (data and PYTHIA) to parameterization
Eta pT spectra in different jet pT intervals normalized per jet
Ratio of fully corrected Pi0 pT spectra inside jets (data and PYTHIA) to parameterization
Pi0 pT spectra in different jet pT intervals normalized per jet
Ratio of Eta pT spectra in different jet pT intervals to a fit to the inclusive Eta spectrum
Eta pT spectra in different jet pT intervals normalized per event
Ratio of Pi0 pT spectra in different jet pT intervals to a fit to the inclusive Pi0 spectrum
Pi0 pT spectra in different jet pT intervals normalized per event and the inclusive Pi0 spectrum
Pi0 pT spectra in different jet pT intervals normalized per event
Comparison of corrected Eta spectra inside jets from different reconstruction methods as function of z
Comparison of corrected Pi0 spectra inside jets from different reconstruction methods as function of z