Published figures by group
Accessing the deuteron source with pion-deuteron femtoscopy in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV
Figure 1
- Fig. Group : Accessing the deuteron source with pion-deuteron femtoscopy in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV
- PWG : PWG-CF (Flow and Correlations)
- System: Pb-Pb
- Energy: 5.02 TeV
Figure 2
- Fig. Group : Accessing the deuteron source with pion-deuteron femtoscopy in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV
- PWG : PWG-CF (Flow and Correlations)
- System: Pb-Pb
- Energy: 5.02 TeV
First observation of ultra-long-range azimuthal correlations in low multiplicity pp and p-Pb collisions at the LHC
Figure 1
- Fig. Group : First observation of ultra-long-range azimuthal correlations in low multiplicity pp and p-Pb collisions at the LHC
- PWG : PWG-CF (Flow and Correlations)
- System: p-p, p-Pb
- Energy: 5.02 TeV, 13 TeV
Figure 2
- Fig. Group : First observation of ultra-long-range azimuthal correlations in low multiplicity pp and p-Pb collisions at the LHC
- PWG : PWG-CF (Flow and Correlations)
- System: p-p, p-Pb
- Energy: 5.02 TeV, 13 TeV
Figure 3a
- Fig. Group : First observation of ultra-long-range azimuthal correlations in low multiplicity pp and p-Pb collisions at the LHC
- PWG : PWG-CF (Flow and Correlations)
- System: p-p, p-Pb
- Energy: 5.02 TeV, 13 TeV
Figure 3b
- Fig. Group : First observation of ultra-long-range azimuthal correlations in low multiplicity pp and p-Pb collisions at the LHC
- PWG : PWG-CF (Flow and Correlations)
- System: p-p, p-Pb
- Energy: 5.02 TeV, 13 TeV
Revealing the microscopic mechanism of deuteron formation at the LHC
Figure 1
- Fig. Group : Revealing the microscopic mechanism of deuteron formation at the LHC
- PWG : PWG-CF (Flow and Correlations)
- System: p-p
- Energy: 13 TeV
Figure 2a
- Fig. Group : Revealing the microscopic mechanism of deuteron formation at the LHC
- PWG : PWG-CF (Flow and Correlations)
- System: p-p
- Energy: 13 TeV
Figure 2b
- Fig. Group : Revealing the microscopic mechanism of deuteron formation at the LHC
- PWG : PWG-CF (Flow and Correlations)
- System: p-p
- Energy: 13 TeV
Figure A.1
- Fig. Group : Revealing the microscopic mechanism of deuteron formation at the LHC
- PWG : PWG-CF (Flow and Correlations)
- System: p-p
- Energy: 13 TeV
Centrality dependence of charged-particle pseudorapidity density at midrapidity in Pb-Pb collisions at $\mathbf{\sqrt{\textit{s}_{\rm NN}} = 5.36}$ TeV
Figure 1
- Fig. Group : Centrality dependence of charged-particle pseudorapidity density at midrapidity in Pb-Pb collisions at $\mathbf{\sqrt{\textit{s}_{\rm NN}} = 5.36}$ TeV
- PWG : PWG-LF (Light Flavour Spectra)
- System: Pb-Pb
- Energy: 5.36 TeV
Figure 2
- Fig. Group : Centrality dependence of charged-particle pseudorapidity density at midrapidity in Pb-Pb collisions at $\mathbf{\sqrt{\textit{s}_{\rm NN}} = 5.36}$ TeV
- PWG : PWG-LF (Light Flavour Spectra)
- System: Pb-Pb
- Energy: 5.36 TeV
Figure 3
- Fig. Group : Centrality dependence of charged-particle pseudorapidity density at midrapidity in Pb-Pb collisions at $\mathbf{\sqrt{\textit{s}_{\rm NN}} = 5.36}$ TeV
- PWG : PWG-LF (Light Flavour Spectra)
- System: Pb-Pb
- Energy: 5.36 TeV
Figure 4
- Fig. Group : Centrality dependence of charged-particle pseudorapidity density at midrapidity in Pb-Pb collisions at $\mathbf{\sqrt{\textit{s}_{\rm NN}} = 5.36}$ TeV
- PWG : PWG-LF (Light Flavour Spectra)
- System: Pb-Pb
- Energy: 5.36 TeV
Figure 5
- Fig. Group : Centrality dependence of charged-particle pseudorapidity density at midrapidity in Pb-Pb collisions at $\mathbf{\sqrt{\textit{s}_{\rm NN}} = 5.36}$ TeV
- PWG : PWG-LF (Light Flavour Spectra)
- System: Pb-Pb
- Energy: 5.36 TeV
D$^{0}$-meson-tagged jet axes difference in proton-proton collisions at $\mathbf{\sqrt{\textit{s}} = 5.02}$ TeV
Figure 1a
- Fig. Group : D$^{0}$-meson-tagged jet axes difference in proton-proton collisions at $\mathbf{\sqrt{\textit{s}} = 5.02}$ TeV
- PWG : PWG-HF (Heavy Flavour)
- System: p-p
- Energy: 5.02 TeV
Figure 1b
- Fig. Group : D$^{0}$-meson-tagged jet axes difference in proton-proton collisions at $\mathbf{\sqrt{\textit{s}} = 5.02}$ TeV
- PWG : PWG-HF (Heavy Flavour)
- System: p-p
- Energy: 5.02 TeV
Figure 2a
- Fig. Group : D$^{0}$-meson-tagged jet axes difference in proton-proton collisions at $\mathbf{\sqrt{\textit{s}} = 5.02}$ TeV
- PWG : PWG-HF (Heavy Flavour)
- System: p-p
- Energy: 5.02 TeV
Figure 2b
- Fig. Group : D$^{0}$-meson-tagged jet axes difference in proton-proton collisions at $\mathbf{\sqrt{\textit{s}} = 5.02}$ TeV
- PWG : PWG-HF (Heavy Flavour)
- System: p-p
- Energy: 5.02 TeV
Figure 3
- Fig. Group : D$^{0}$-meson-tagged jet axes difference in proton-proton collisions at $\mathbf{\sqrt{\textit{s}} = 5.02}$ TeV
- PWG : PWG-HF (Heavy Flavour)
- System: p-p
- Energy: 5.02 TeV
Figure 4
- Fig. Group : D$^{0}$-meson-tagged jet axes difference in proton-proton collisions at $\mathbf{\sqrt{\textit{s}} = 5.02}$ TeV
- PWG : PWG-HF (Heavy Flavour)
- System: p-p
- Energy: 5.02 TeV
Figure 5
- Fig. Group : D$^{0}$-meson-tagged jet axes difference in proton-proton collisions at $\mathbf{\sqrt{\textit{s}} = 5.02}$ TeV
- PWG : PWG-HF (Heavy Flavour)
- System: p-p
- Energy: 5.02 TeV
Figure 6
- Fig. Group : D$^{0}$-meson-tagged jet axes difference in proton-proton collisions at $\mathbf{\sqrt{\textit{s}} = 5.02}$ TeV
- PWG : PWG-HF (Heavy Flavour)
- System: p-p
- Energy: 5.02 TeV
Figure 7
- Fig. Group : D$^{0}$-meson-tagged jet axes difference in proton-proton collisions at $\mathbf{\sqrt{\textit{s}} = 5.02}$ TeV
- PWG : PWG-HF (Heavy Flavour)
- System: p-p
- Energy: 5.02 TeV
Figure 8
- Fig. Group : D$^{0}$-meson-tagged jet axes difference in proton-proton collisions at $\mathbf{\sqrt{\textit{s}} = 5.02}$ TeV
- PWG : PWG-HF (Heavy Flavour)
- System: p-p
- Energy: 5.02 TeV