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
Multiplicity dependence of $Ξ_c^+$ and $Ξ_c^0$ production in pp collisions at $\sqrt{s} = 13$ TeV
Figure 1a
- Fig. Group : Multiplicity dependence of $Ξ_c^+$ and $Ξ_c^0$ production in pp collisions at $\sqrt{s} = 13$ TeV
- PWG : PWG-HF (Heavy Flavour)
- System: p-p
- Energy: 13 TeV
Figure 1b
- Fig. Group : Multiplicity dependence of $Ξ_c^+$ and $Ξ_c^0$ production in pp collisions at $\sqrt{s} = 13$ TeV
- PWG : PWG-HF (Heavy Flavour)
- System: p-p
- Energy: 13 TeV
Figure 2a
- Fig. Group : Multiplicity dependence of $Ξ_c^+$ and $Ξ_c^0$ production in pp collisions at $\sqrt{s} = 13$ TeV
- PWG : PWG-HF (Heavy Flavour)
- System: p-p
- Energy: 13 TeV
Figure 2b
- Fig. Group : Multiplicity dependence of $Ξ_c^+$ and $Ξ_c^0$ production in pp collisions at $\sqrt{s} = 13$ TeV
- PWG : PWG-HF (Heavy Flavour)
- System: p-p
- Energy: 13 TeV
Figure 3
- Fig. Group : Multiplicity dependence of $Ξ_c^+$ and $Ξ_c^0$ production in pp collisions at $\sqrt{s} = 13$ TeV
- PWG : PWG-HF (Heavy Flavour)
- System: p-p
- Energy: 13 TeV
Figure 4
- Fig. Group : Multiplicity dependence of $Ξ_c^+$ and $Ξ_c^0$ production in pp collisions at $\sqrt{s} = 13$ TeV
- PWG : PWG-HF (Heavy Flavour)
- System: p-p
- Energy: 13 TeV
Figure 5
- Fig. Group : Multiplicity dependence of $Ξ_c^+$ and $Ξ_c^0$ production in pp collisions at $\sqrt{s} = 13$ TeV
- PWG : PWG-HF (Heavy Flavour)
- System: p-p
- Energy: 13 TeV
Figure 6
- Fig. Group : Multiplicity dependence of $Ξ_c^+$ and $Ξ_c^0$ production in pp collisions at $\sqrt{s} = 13$ TeV
- PWG : PWG-HF (Heavy Flavour)
- System: p-p
- Energy: 13 TeV
Measurement of $ω$ meson production in pp and p$-$Pb collisions at $\mathbf{\sqrt{s_{\rm NN}} = 5.02}$ TeV
Figure 1a
- Fig. Group : Measurement of $ω$ meson production in pp and p$-$Pb collisions at $\mathbf{\sqrt{s_{\rm NN}} = 5.02}$ TeV
- PWG : PWG-EM (Electromagnetic probes)
- System: p-p, p-Pb
- Energy: 5.02 TeV
Figure 1b
- Fig. Group : Measurement of $ω$ meson production in pp and p$-$Pb collisions at $\mathbf{\sqrt{s_{\rm NN}} = 5.02}$ TeV
- PWG : PWG-EM (Electromagnetic probes)
- System: p-p, p-Pb
- Energy: 5.02 TeV
Figure 1c
- Fig. Group : Measurement of $ω$ meson production in pp and p$-$Pb collisions at $\mathbf{\sqrt{s_{\rm NN}} = 5.02}$ TeV
- PWG : PWG-EM (Electromagnetic probes)
- System: p-p, p-Pb
- Energy: 5.02 TeV
Figure 1d
- Fig. Group : Measurement of $ω$ meson production in pp and p$-$Pb collisions at $\mathbf{\sqrt{s_{\rm NN}} = 5.02}$ TeV
- PWG : PWG-EM (Electromagnetic probes)
- System: p-p, p-Pb
- Energy: 5.02 TeV
Figure 1e
- Fig. Group : Measurement of $ω$ meson production in pp and p$-$Pb collisions at $\mathbf{\sqrt{s_{\rm NN}} = 5.02}$ TeV
- PWG : PWG-EM (Electromagnetic probes)
- System: p-p, p-Pb
- Energy: 5.02 TeV
Figure 1f
- Fig. Group : Measurement of $ω$ meson production in pp and p$-$Pb collisions at $\mathbf{\sqrt{s_{\rm NN}} = 5.02}$ TeV
- PWG : PWG-EM (Electromagnetic probes)
- System: p-p, p-Pb
- Energy: 5.02 TeV
Figure 2
- Fig. Group : Measurement of $ω$ meson production in pp and p$-$Pb collisions at $\mathbf{\sqrt{s_{\rm NN}} = 5.02}$ TeV
- PWG : PWG-EM (Electromagnetic probes)
- System: p-p, p-Pb
- Energy: 5.02 TeV
Figure 3a
- Fig. Group : Measurement of $ω$ meson production in pp and p$-$Pb collisions at $\mathbf{\sqrt{s_{\rm NN}} = 5.02}$ TeV
- PWG : PWG-EM (Electromagnetic probes)
- System: p-p, p-Pb
- Energy: 5.02 TeV
Figure 3b
- Fig. Group : Measurement of $ω$ meson production in pp and p$-$Pb collisions at $\mathbf{\sqrt{s_{\rm NN}} = 5.02}$ TeV
- PWG : PWG-EM (Electromagnetic probes)
- System: p-p, p-Pb
- Energy: 5.02 TeV
Figure 4
- Fig. Group : Measurement of $ω$ meson production in pp and p$-$Pb collisions at $\mathbf{\sqrt{s_{\rm NN}} = 5.02}$ TeV
- PWG : PWG-EM (Electromagnetic probes)
- System: p-p, p-Pb
- Energy: 5.02 TeV
Figure 5a
- Fig. Group : Measurement of $ω$ meson production in pp and p$-$Pb collisions at $\mathbf{\sqrt{s_{\rm NN}} = 5.02}$ TeV
- PWG : PWG-EM (Electromagnetic probes)
- System: p-p, p-Pb
- Energy: 5.02 TeV
Figure 5b
- Fig. Group : Measurement of $ω$ meson production in pp and p$-$Pb collisions at $\mathbf{\sqrt{s_{\rm NN}} = 5.02}$ TeV
- PWG : PWG-EM (Electromagnetic probes)
- System: p-p, p-Pb
- Energy: 5.02 TeV
Figure 6a
- Fig. Group : Measurement of $ω$ meson production in pp and p$-$Pb collisions at $\mathbf{\sqrt{s_{\rm NN}} = 5.02}$ TeV
- PWG : PWG-EM (Electromagnetic probes)
- System: p-p, p-Pb
- Energy: 5.02 TeV
Figure 6b
- Fig. Group : Measurement of $ω$ meson production in pp and p$-$Pb collisions at $\mathbf{\sqrt{s_{\rm NN}} = 5.02}$ TeV
- PWG : PWG-EM (Electromagnetic probes)
- System: p-p, p-Pb
- Energy: 5.02 TeV
Figure 7
- Fig. Group : Measurement of $ω$ meson production in pp and p$-$Pb collisions at $\mathbf{\sqrt{s_{\rm NN}} = 5.02}$ TeV
- PWG : PWG-EM (Electromagnetic probes)
- System: p-p, p-Pb
- Energy: 5.02 TeV