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Title
ID number ALI-PUB-XXX
Figure Caption
Journal reference
Scope: PWG
- Any -
PWG-CF (Flow and Correlations)
PWG-DQ (Dileptons and Quarkonia)
PWG-EM (Electromagnetic probes)
PWG-HF (Heavy Flavour)
PWG-JE (Jets)
PWG-LF (Light Flavour Spectra)
PWG-UD (Ultraperipheral and Diffraction)
PWG-MM (Monte Carlo generators and Minimum Bias)
ITS
ITS3
TPC
TRD
TOF
HMPID
PHOS
MCH
MTR
ZDC
Trigger
Computing resources
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DCS
ELECTRONIC
UPGRADE
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MFT
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Diversity Office
General
PWG1
PWG2
PWG3
PWG4
PWG-PP
PWG-GA (Photons, Neutral Mesons)
CC General
SDD
SPD
SSD
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T0
PMD
V0
ACORDE
DAQ
HLT
O2
Offline
DPG
BTG
System
cosmic rays
p-p
Pb-Pb
p-Pb
Xe-Xe
none
Energy
cosmic rays
900 GeV
2.36 TeV
2.76 TeV
5.02 TeV
5.36 TeV
5.44 TeV
5.5 TeV
7 TeV
8 TeV
8.8 TeV
13 TeV
13.6 TeV
14 TeV
none
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Figure
Figure 2
Fig. Group :
Pseudorapidity dependence of anisotropic flow and its decorrelations using long-range multiparticle correlations in Pb-Pb and Xe-Xe collisions
PWG :
PWG-CF (Flow and Correlations)
System:
Pb-Pb
,
System:
Xe-Xe
Energy:
5.02 TeV
,
Energy:
5.44 TeV
Figure 1
Fig. Group :
Pseudorapidity dependence of anisotropic flow and its decorrelations using long-range multiparticle correlations in Pb-Pb and Xe-Xe collisions
PWG :
PWG-CF (Flow and Correlations)
System:
Pb-Pb
,
System:
Xe-Xe
Energy:
5.02 TeV
,
Energy:
5.44 TeV
Figure 4b
Fig. Group :
Modification of charged-particle jets in event-shape engineered Pb$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV
PWG :
PWG-JE (Jets)
System:
Pb-Pb
Energy:
5.02 TeV
Figure 4a
Fig. Group :
Modification of charged-particle jets in event-shape engineered Pb$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV
PWG :
PWG-JE (Jets)
System:
Pb-Pb
Energy:
5.02 TeV
Figure 3
Fig. Group :
Modification of charged-particle jets in event-shape engineered Pb$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV
PWG :
PWG-JE (Jets)
System:
Pb-Pb
Energy:
5.02 TeV
Figure 2b
Fig. Group :
Modification of charged-particle jets in event-shape engineered Pb$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV
PWG :
PWG-JE (Jets)
System:
Pb-Pb
Energy:
5.02 TeV
Figure 2a
Fig. Group :
Modification of charged-particle jets in event-shape engineered Pb$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV
PWG :
PWG-JE (Jets)
System:
Pb-Pb
Energy:
5.02 TeV
Figure 1
Fig. Group :
Modification of charged-particle jets in event-shape engineered Pb$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV
PWG :
PWG-JE (Jets)
System:
Pb-Pb
Energy:
5.02 TeV
Figure 8b
Fig. Group :
K$^{*}$(892)$^{\pm}$ resonance production in Pb$-$Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV
PWG :
PWG-LF (Light Flavour Spectra)
System:
Pb-Pb
Energy:
5.02 TeV
Figure 8a
Fig. Group :
K$^{*}$(892)$^{\pm}$ resonance production in Pb$-$Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV
PWG :
PWG-LF (Light Flavour Spectra)
System:
Pb-Pb
Energy:
5.02 TeV
Figure 7
Fig. Group :
K$^{*}$(892)$^{\pm}$ resonance production in Pb$-$Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV
PWG :
PWG-LF (Light Flavour Spectra)
System:
Pb-Pb
Energy:
5.02 TeV
Figure 6
Fig. Group :
K$^{*}$(892)$^{\pm}$ resonance production in Pb$-$Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV
PWG :
PWG-LF (Light Flavour Spectra)
System:
Pb-Pb
Energy:
5.02 TeV
Figure 5
Fig. Group :
K$^{*}$(892)$^{\pm}$ resonance production in Pb$-$Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV
PWG :
PWG-LF (Light Flavour Spectra)
System:
Pb-Pb
Energy:
5.02 TeV
Figure 4b
Fig. Group :
K$^{*}$(892)$^{\pm}$ resonance production in Pb$-$Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV
PWG :
PWG-LF (Light Flavour Spectra)
System:
Pb-Pb
Energy:
5.02 TeV
Figure 4a
Fig. Group :
K$^{*}$(892)$^{\pm}$ resonance production in Pb$-$Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV
PWG :
PWG-LF (Light Flavour Spectra)
System:
Pb-Pb
Energy:
5.02 TeV
Figure 3
Fig. Group :
K$^{*}$(892)$^{\pm}$ resonance production in Pb$-$Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV
PWG :
PWG-LF (Light Flavour Spectra)
System:
Pb-Pb
Energy:
5.02 TeV
Figure 2
Fig. Group :
K$^{*}$(892)$^{\pm}$ resonance production in Pb$-$Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV
PWG :
PWG-LF (Light Flavour Spectra)
System:
Pb-Pb
Energy:
5.02 TeV
Figure 1b
Fig. Group :
K$^{*}$(892)$^{\pm}$ resonance production in Pb$-$Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV
PWG :
PWG-LF (Light Flavour Spectra)
System:
Pb-Pb
Energy:
5.02 TeV
Figure 1a
Fig. Group :
K$^{*}$(892)$^{\pm}$ resonance production in Pb$-$Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV
PWG :
PWG-LF (Light Flavour Spectra)
System:
Pb-Pb
Energy:
5.02 TeV
Figure 1
Fig. Group :
Skewness and kurtosis of mean transverse momentum fluctuations at the LHC energies
PWG :
PWG-CF (Flow and Correlations)
System:
p-p
,
System:
Pb-Pb
,
System:
Xe-Xe
Energy:
5.02 TeV
,
Energy:
5.44 TeV
Figure 2
Fig. Group :
Skewness and kurtosis of mean transverse momentum fluctuations at the LHC energies
PWG :
PWG-CF (Flow and Correlations)
System:
p-p
,
System:
Pb-Pb
,
System:
Xe-Xe
Energy:
5.02 TeV
,
Energy:
5.44 TeV
Figure 3
Fig. Group :
Skewness and kurtosis of mean transverse momentum fluctuations at the LHC energies
PWG :
PWG-CF (Flow and Correlations)
System:
p-p
,
System:
Pb-Pb
,
System:
Xe-Xe
Energy:
5.02 TeV
,
Energy:
5.44 TeV
Figure 5
Fig. Group :
Skewness and kurtosis of mean transverse momentum fluctuations at the LHC energies
PWG :
PWG-CF (Flow and Correlations)
System:
p-p
,
System:
Pb-Pb
,
System:
Xe-Xe
Energy:
5.02 TeV
,
Energy:
5.44 TeV
Figure 4
Fig. Group :
Skewness and kurtosis of mean transverse momentum fluctuations at the LHC energies
PWG :
PWG-CF (Flow and Correlations)
System:
p-p
,
System:
Pb-Pb
,
System:
Xe-Xe
Energy:
5.02 TeV
,
Energy:
5.44 TeV
Figure 11a
Fig. Group :
Prompt and non-prompt J$/ψ$ production at midrapidity in Pb$-$Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV
PWG :
PWG-DQ (Dileptons and Quarkonia)
System:
Pb-Pb
Energy:
5.02 TeV
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