Published figures by group
$\mathbf{\textbf{K}^{0}_{\textbf{S}}}-\mathbf{\textbf{K}^{0}_{\textbf{S}}}$ femtoscopy in Pb$-$Pb collisions at $\mathbf{\sqrt{\textit{s}_{\rm NN}} = 5.02}$ TeV at the LHC
Figure 4
- Fig. Group : $\mathbf{\textbf{K}^{0}_{\textbf{S}}}-\mathbf{\textbf{K}^{0}_{\textbf{S}}}$ femtoscopy in Pb$-$Pb collisions at $\mathbf{\sqrt{\textit{s}_{\rm NN}} = 5.02}$ TeV at the LHC
- PWG : PWG-CF (Flow and Correlations)
- System: Pb-Pb
- Energy: 5.02 TeV
Figure 5
- Fig. Group : $\mathbf{\textbf{K}^{0}_{\textbf{S}}}-\mathbf{\textbf{K}^{0}_{\textbf{S}}}$ femtoscopy in Pb$-$Pb collisions at $\mathbf{\sqrt{\textit{s}_{\rm NN}} = 5.02}$ TeV at the LHC
- PWG : PWG-CF (Flow and Correlations)
- System: Pb-Pb
- Energy: 5.02 TeV
Figure A.1
- Fig. Group : $\mathbf{\textbf{K}^{0}_{\textbf{S}}}-\mathbf{\textbf{K}^{0}_{\textbf{S}}}$ femtoscopy in Pb$-$Pb collisions at $\mathbf{\sqrt{\textit{s}_{\rm NN}} = 5.02}$ TeV at the LHC
- PWG : PWG-CF (Flow and Correlations)
- System: Pb-Pb
- Energy: 5.02 TeV
Figure A.2
- Fig. Group : $\mathbf{\textbf{K}^{0}_{\textbf{S}}}-\mathbf{\textbf{K}^{0}_{\textbf{S}}}$ femtoscopy in Pb$-$Pb collisions at $\mathbf{\sqrt{\textit{s}_{\rm NN}} = 5.02}$ TeV at the LHC
- PWG : PWG-CF (Flow and Correlations)
- System: Pb-Pb
- Energy: 5.02 TeV
Figure A.3
- Fig. Group : $\mathbf{\textbf{K}^{0}_{\textbf{S}}}-\mathbf{\textbf{K}^{0}_{\textbf{S}}}$ femtoscopy in Pb$-$Pb collisions at $\mathbf{\sqrt{\textit{s}_{\rm NN}} = 5.02}$ TeV at the LHC
- PWG : PWG-CF (Flow and Correlations)
- System: Pb-Pb
- Energy: 5.02 TeV
Wave-Function Femtometry: Hypertriton - The Ultimate Halo Nucleus
Figure 1
- Fig. Group : Wave-Function Femtometry: Hypertriton - The Ultimate Halo Nucleus
- PWG : PWG-LF (Light Flavour Spectra)
- System: p-p
- Energy: 13 TeV
Figure 2
- Fig. Group : Wave-Function Femtometry: Hypertriton - The Ultimate Halo Nucleus
- PWG : PWG-LF (Light Flavour Spectra)
- System: p-p
- Energy: 13 TeV
Figure 3
- Fig. Group : Wave-Function Femtometry: Hypertriton - The Ultimate Halo Nucleus
- PWG : PWG-LF (Light Flavour Spectra)
- System: p-p
- Energy: 13 TeV
Figure A.1a
- Fig. Group : Wave-Function Femtometry: Hypertriton - The Ultimate Halo Nucleus
- PWG : PWG-LF (Light Flavour Spectra)
- System: p-p
- Energy: 13 TeV
Figure A.1b
- Fig. Group : Wave-Function Femtometry: Hypertriton - The Ultimate Halo Nucleus
- PWG : PWG-LF (Light Flavour Spectra)
- System: p-p
- Energy: 13 TeV
Figure A.2
- Fig. Group : Wave-Function Femtometry: Hypertriton - The Ultimate Halo Nucleus
- PWG : PWG-LF (Light Flavour Spectra)
- System: p-p
- Energy: 13 TeV
Dijet invariant mass of charged-particle jets in pp and p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV
Figure 1
- Fig. Group : Dijet invariant mass of charged-particle jets in pp and p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV
- PWG : PWG-JE (Jets)
- System: p-p, p-Pb
- Energy: 5.02 TeV
Figure 2
- Fig. Group : Dijet invariant mass of charged-particle jets in pp and p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV
- PWG : PWG-JE (Jets)
- System: p-p, p-Pb
- Energy: 5.02 TeV
Multiplicity dependence of f$_0$(980) production in pp collisions at $\sqrt{s} = 13$ TeV
Figure 1a
- Fig. Group : Multiplicity dependence of f$_0$(980) production in pp collisions at $\sqrt{s} = 13$ TeV
- PWG : PWG-LF (Light Flavour Spectra)
- System: p-p
- Energy: 13 TeV
Figure 1b
- Fig. Group : Multiplicity dependence of f$_0$(980) production in pp collisions at $\sqrt{s} = 13$ TeV
- PWG : PWG-LF (Light Flavour Spectra)
- System: p-p
- Energy: 13 TeV
Figure 2
- Fig. Group : Multiplicity dependence of f$_0$(980) production in pp collisions at $\sqrt{s} = 13$ TeV
- PWG : PWG-LF (Light Flavour Spectra)
- System: p-p
- Energy: 13 TeV
Figure 3a
- Fig. Group : Multiplicity dependence of f$_0$(980) production in pp collisions at $\sqrt{s} = 13$ TeV
- PWG : PWG-LF (Light Flavour Spectra)
- System: p-p
- Energy: 13 TeV
Figure 3b
- Fig. Group : Multiplicity dependence of f$_0$(980) production in pp collisions at $\sqrt{s} = 13$ TeV
- PWG : PWG-LF (Light Flavour Spectra)
- System: p-p
- Energy: 13 TeV
Figure 4
- Fig. Group : Multiplicity dependence of f$_0$(980) production in pp collisions at $\sqrt{s} = 13$ TeV
- PWG : PWG-LF (Light Flavour Spectra)
- System: p-p
- Energy: 13 TeV
Figure 5
- Fig. Group : Multiplicity dependence of f$_0$(980) production in pp collisions at $\sqrt{s} = 13$ TeV
- PWG : PWG-LF (Light Flavour Spectra)
- System: p-p
- Energy: 13 TeV
Figure 6a
- Fig. Group : Multiplicity dependence of f$_0$(980) production in pp collisions at $\sqrt{s} = 13$ TeV
- PWG : PWG-LF (Light Flavour Spectra)
- System: p-p
- Energy: 13 TeV
Figure 6b
- Fig. Group : Multiplicity dependence of f$_0$(980) production in pp collisions at $\sqrt{s} = 13$ TeV
- PWG : PWG-LF (Light Flavour Spectra)
- System: p-p
- Energy: 13 TeV
Figure 7a
- Fig. Group : Multiplicity dependence of f$_0$(980) production in pp collisions at $\sqrt{s} = 13$ TeV
- PWG : PWG-LF (Light Flavour Spectra)
- System: p-p
- Energy: 13 TeV
Figure 7b
- Fig. Group : Multiplicity dependence of f$_0$(980) production in pp collisions at $\sqrt{s} = 13$ TeV
- PWG : PWG-LF (Light Flavour Spectra)
- System: p-p
- Energy: 13 TeV
Production of $Ξ$ and $Ω$ hyperons in high-multiplicity proton-proton collisions at $\sqrt{s}$ = 13 TeV
Figure 1a
- Fig. Group : Production of $Ξ$ and $Ω$ hyperons in high-multiplicity proton-proton collisions at $\sqrt{s}$ = 13 TeV
- PWG : PWG-LF (Light Flavour Spectra)
- System: p-p
- Energy: 13 TeV