Published figures by group
Pseudorapidity dependence of anisotropic flow and its decorrelations using long-range multiparticle correlations in Pb-Pb and Xe-Xe collisions
Figure 9
- 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, Xe-Xe
- Energy: 5.02 TeV, 5.44 TeV
Figure 10
- 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, Xe-Xe
- Energy: 5.02 TeV, 5.44 TeV
Modification of charged-particle jets in event-shape engineered Pb$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ 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 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 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 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 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 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
K$^{*}$(892)$^{\pm}$ resonance production in Pb$-$Pb collisions at $\sqrt{s_{\rm NN}}$ = 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 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 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 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 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 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 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 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 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 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 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
Skewness and kurtosis of mean transverse momentum fluctuations at the LHC energies
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, Pb-Pb, Xe-Xe
- Energy: 5.02 TeV, 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, Pb-Pb, Xe-Xe
- Energy: 5.02 TeV, 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, Pb-Pb, Xe-Xe
- Energy: 5.02 TeV, 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, Pb-Pb, Xe-Xe
- Energy: 5.02 TeV, 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, Pb-Pb, Xe-Xe
- Energy: 5.02 TeV, 5.44 TeV
Prompt and non-prompt J$/ψ$ production at midrapidity in Pb$-$Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 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