Published figures by group
Deuteron coalescence probability in jets in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV
Figure 4
- Fig. Group : Deuteron coalescence probability in jets in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV
- PWG : PWG-LF (Light Flavour Spectra)
- System: p-Pb
- Energy: 5.02 TeV
Figure 5
- Fig. Group : Deuteron coalescence probability in jets in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV
- PWG : PWG-LF (Light Flavour Spectra)
- System: p-Pb
- Energy: 5.02 TeV
Measurements of the production of W$^{\pm}$ and Z$^0$ bosons in pp collisions at $\sqrt{s} = 13$ TeV
Figure 1
- Fig. Group : Measurements of the production of W$^{\pm}$ and Z$^0$ bosons in pp collisions at $\sqrt{s} = 13$ TeV
- PWG : PWG-HF (Heavy Flavour)
- System: p-p
- Energy: 13 TeV
Figure 2a
- Fig. Group : Measurements of the production of W$^{\pm}$ and Z$^0$ bosons in pp collisions at $\sqrt{s} = 13$ TeV
- PWG : PWG-HF (Heavy Flavour)
- System: p-p
- Energy: 13 TeV
Figure 2b
- Fig. Group : Measurements of the production of W$^{\pm}$ and Z$^0$ bosons in pp collisions at $\sqrt{s} = 13$ TeV
- PWG : PWG-HF (Heavy Flavour)
- System: p-p
- Energy: 13 TeV
Figure 3
- Fig. Group : Measurements of the production of W$^{\pm}$ and Z$^0$ bosons in pp collisions at $\sqrt{s} = 13$ TeV
- PWG : PWG-HF (Heavy Flavour)
- System: p-p
- Energy: 13 TeV
Figure 4a
- Fig. Group : Measurements of the production of W$^{\pm}$ and Z$^0$ bosons in pp collisions at $\sqrt{s} = 13$ TeV
- PWG : PWG-HF (Heavy Flavour)
- System: p-p
- Energy: 13 TeV
Figure 4b
- Fig. Group : Measurements of the production of W$^{\pm}$ and Z$^0$ bosons in pp collisions at $\sqrt{s} = 13$ TeV
- PWG : PWG-HF (Heavy Flavour)
- System: p-p
- Energy: 13 TeV
Figure 4c
- Fig. Group : Measurements of the production of W$^{\pm}$ and Z$^0$ bosons in pp collisions at $\sqrt{s} = 13$ TeV
- PWG : PWG-HF (Heavy Flavour)
- System: p-p
- Energy: 13 TeV
Figure 5a
- Fig. Group : Measurements of the production of W$^{\pm}$ and Z$^0$ bosons in pp collisions at $\sqrt{s} = 13$ TeV
- PWG : PWG-HF (Heavy Flavour)
- System: p-p
- Energy: 13 TeV
Figure 5b
- Fig. Group : Measurements of the production of W$^{\pm}$ and Z$^0$ bosons in pp collisions at $\sqrt{s} = 13$ TeV
- PWG : PWG-HF (Heavy Flavour)
- System: p-p
- Energy: 13 TeV
Figure 5c
- Fig. Group : Measurements of the production of W$^{\pm}$ and Z$^0$ bosons in pp collisions at $\sqrt{s} = 13$ TeV
- PWG : PWG-HF (Heavy Flavour)
- System: p-p
- Energy: 13 TeV
Figure 6
- Fig. Group : Measurements of the production of W$^{\pm}$ and Z$^0$ bosons in pp collisions at $\sqrt{s} = 13$ TeV
- PWG : PWG-HF (Heavy Flavour)
- System: p-p
- Energy: 13 TeV
Figure 7a
- Fig. Group : Measurements of the production of W$^{\pm}$ and Z$^0$ bosons in pp collisions at $\sqrt{s} = 13$ TeV
- PWG : PWG-HF (Heavy Flavour)
- System: p-p
- Energy: 13 TeV
Figure 7b
- Fig. Group : Measurements of the production of W$^{\pm}$ and Z$^0$ bosons in pp collisions at $\sqrt{s} = 13$ TeV
- PWG : PWG-HF (Heavy Flavour)
- System: p-p
- Energy: 13 TeV
Figure 8a
- Fig. Group : Measurements of the production of W$^{\pm}$ and Z$^0$ bosons in pp collisions at $\sqrt{s} = 13$ TeV
- PWG : PWG-HF (Heavy Flavour)
- System: p-p
- Energy: 13 TeV
Figure 8b
- Fig. Group : Measurements of the production of W$^{\pm}$ and Z$^0$ bosons in pp collisions at $\sqrt{s} = 13$ TeV
- PWG : PWG-HF (Heavy Flavour)
- System: p-p
- Energy: 13 TeV
Figure 9a
- Fig. Group : Measurements of the production of W$^{\pm}$ and Z$^0$ bosons in pp collisions at $\sqrt{s} = 13$ TeV
- PWG : PWG-HF (Heavy Flavour)
- System: p-p
- Energy: 13 TeV
Figure 9b
- Fig. Group : Measurements of the production of W$^{\pm}$ and Z$^0$ bosons in pp collisions at $\sqrt{s} = 13$ TeV
- PWG : PWG-HF (Heavy Flavour)
- System: p-p
- Energy: 13 TeV
Limits on the chiral magnetic effect from the event shape engineering and participant-spectator correlation techniques in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV
Figure 1
- Fig. Group : Limits on the chiral magnetic effect from the event shape engineering and participant-spectator correlation techniques 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 : Limits on the chiral magnetic effect from the event shape engineering and participant-spectator correlation techniques 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 3
- Fig. Group : Limits on the chiral magnetic effect from the event shape engineering and participant-spectator correlation techniques 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 4
- Fig. Group : Limits on the chiral magnetic effect from the event shape engineering and participant-spectator correlation techniques 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 5
- Fig. Group : Limits on the chiral magnetic effect from the event shape engineering and participant-spectator correlation techniques 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 6
- Fig. Group : Limits on the chiral magnetic effect from the event shape engineering and participant-spectator correlation techniques 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