Published figures by group
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 prompt and non-prompt J/$ψ$ production at midrapidity in pp collisions at $\sqrt{s} = 13$ TeV
Figure 1
- Fig. Group : Multiplicity dependence of prompt and non-prompt J/$ψ$ production at midrapidity in pp collisions at $\sqrt{s} = 13$ TeV
- PWG : PWG-DQ (Dileptons and Quarkonia)
- System: p-p
- Energy: 13 TeV
Figure 2
- Fig. Group : Multiplicity dependence of prompt and non-prompt J/$ψ$ production at midrapidity in pp collisions at $\sqrt{s} = 13$ TeV
- PWG : PWG-DQ (Dileptons and Quarkonia)
- System: p-p
- Energy: 13 TeV
Figure 3
- Fig. Group : Multiplicity dependence of prompt and non-prompt J/$ψ$ production at midrapidity in pp collisions at $\sqrt{s} = 13$ TeV
- PWG : PWG-DQ (Dileptons and Quarkonia)
- System: p-p
- Energy: 13 TeV
Figure 4
- Fig. Group : Multiplicity dependence of prompt and non-prompt J/$ψ$ production at midrapidity in pp collisions at $\sqrt{s} = 13$ TeV
- PWG : PWG-DQ (Dileptons and Quarkonia)
- System: p-p
- Energy: 13 TeV
Figure 5
- Fig. Group : Multiplicity dependence of prompt and non-prompt J/$ψ$ production at midrapidity in pp collisions at $\sqrt{s} = 13$ TeV
- PWG : PWG-DQ (Dileptons and Quarkonia)
- System: p-p
- Energy: 13 TeV
Figure 6
- Fig. Group : Multiplicity dependence of prompt and non-prompt J/$ψ$ production at midrapidity in pp collisions at $\sqrt{s} = 13$ TeV
- PWG : PWG-DQ (Dileptons and Quarkonia)
- System: p-p
- Energy: 13 TeV
Figure 7
- Fig. Group : Multiplicity dependence of prompt and non-prompt J/$ψ$ production at midrapidity in pp collisions at $\sqrt{s} = 13$ TeV
- PWG : PWG-DQ (Dileptons and Quarkonia)
- System: p-p
- Energy: 13 TeV
Figure 8
- Fig. Group : Multiplicity dependence of prompt and non-prompt J/$ψ$ production at midrapidity in pp collisions at $\sqrt{s} = 13$ TeV
- PWG : PWG-DQ (Dileptons and Quarkonia)
- System: p-p
- Energy: 13 TeV
Figure 9
- Fig. Group : Multiplicity dependence of prompt and non-prompt J/$ψ$ production at midrapidity in pp collisions at $\sqrt{s} = 13$ TeV
- PWG : PWG-DQ (Dileptons and Quarkonia)
- System: p-p
- Energy: 13 TeV
Figure 10
- Fig. Group : Multiplicity dependence of prompt and non-prompt J/$ψ$ production at midrapidity in pp collisions at $\sqrt{s} = 13$ TeV
- PWG : PWG-DQ (Dileptons and Quarkonia)
- System: p-p
- Energy: 13 TeV
Figure 11
- Fig. Group : Multiplicity dependence of prompt and non-prompt J/$ψ$ production at midrapidity in pp collisions at $\sqrt{s} = 13$ TeV
- PWG : PWG-DQ (Dileptons and Quarkonia)
- System: p-p
- Energy: 13 TeV
Figure 12
- Fig. Group : Multiplicity dependence of prompt and non-prompt J/$ψ$ production at midrapidity in pp collisions at $\sqrt{s} = 13$ TeV
- PWG : PWG-DQ (Dileptons and Quarkonia)
- System: p-p
- Energy: 13 TeV
Figure A.1
- Fig. Group : Multiplicity dependence of prompt and non-prompt J/$ψ$ production at midrapidity in pp collisions at $\sqrt{s} = 13$ TeV
- PWG : PWG-DQ (Dileptons and Quarkonia)
- System: p-p
- Energy: 13 TeV
Figure A.2
- Fig. Group : Multiplicity dependence of prompt and non-prompt J/$ψ$ production at midrapidity in pp collisions at $\sqrt{s} = 13$ TeV
- PWG : PWG-DQ (Dileptons and Quarkonia)
- System: p-p
- Energy: 13 TeV
Figure A.3
- Fig. Group : Multiplicity dependence of prompt and non-prompt J/$ψ$ production at midrapidity in pp collisions at $\sqrt{s} = 13$ TeV
- PWG : PWG-DQ (Dileptons and Quarkonia)
- System: p-p
- Energy: 13 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