Published figures by group
System size and energy dependence of the mean transverse momentum fluctuations at the LHC
Figure 7
- Fig. Group : System size and energy dependence of the mean transverse momentum fluctuations at the LHC
- PWG : PWG-CF (Flow and Correlations)
- System: p-p, Pb-Pb, Xe-Xe
- Energy: 5.02 TeV, 5.44 TeV, 13 TeV
Figure 8
- Fig. Group : System size and energy dependence of the mean transverse momentum fluctuations at the LHC
- PWG : PWG-CF (Flow and Correlations)
- System: p-p, Pb-Pb, Xe-Xe
- Energy: 5.02 TeV, 5.44 TeV, 13 TeV
Studying charm hadronisation into baryons with azimuthal correlations of $Λ_{\rm c}^{+}$ with charged particles in pp collisions at $\mathbf{\sqrt{\it s} = 13}$ TeV
Figure 1
- Fig. Group : Studying charm hadronisation into baryons with azimuthal correlations of $Λ_{\rm c}^{+}$ with charged particles in pp collisions at $\mathbf{\sqrt{\it s} = 13}$ TeV
- PWG : PWG-HF (Heavy Flavour)
- System: p-p
- Energy: 13 TeV
Figure 2
- Fig. Group : Studying charm hadronisation into baryons with azimuthal correlations of $Λ_{\rm c}^{+}$ with charged particles in pp collisions at $\mathbf{\sqrt{\it s} = 13}$ TeV
- PWG : PWG-HF (Heavy Flavour)
- System: p-p
- Energy: 13 TeV
Figure 3
- Fig. Group : Studying charm hadronisation into baryons with azimuthal correlations of $Λ_{\rm c}^{+}$ with charged particles in pp collisions at $\mathbf{\sqrt{\it s} = 13}$ TeV
- PWG : PWG-HF (Heavy Flavour)
- System: p-p
- Energy: 13 TeV
Figure 4
- Fig. Group : Studying charm hadronisation into baryons with azimuthal correlations of $Λ_{\rm c}^{+}$ with charged particles in pp collisions at $\mathbf{\sqrt{\it s} = 13}$ TeV
- PWG : PWG-HF (Heavy Flavour)
- System: p-p
- Energy: 13 TeV
Figure 5
- Fig. Group : Studying charm hadronisation into baryons with azimuthal correlations of $Λ_{\rm c}^{+}$ with charged particles in pp collisions at $\mathbf{\sqrt{\it s} = 13}$ TeV
- PWG : PWG-HF (Heavy Flavour)
- System: p-p
- Energy: 13 TeV
Figure 6a
- Fig. Group : Studying charm hadronisation into baryons with azimuthal correlations of $Λ_{\rm c}^{+}$ with charged particles in pp collisions at $\mathbf{\sqrt{\it s} = 13}$ TeV
- PWG : PWG-HF (Heavy Flavour)
- System: p-p
- Energy: 13 TeV
Figure 6b
- Fig. Group : Studying charm hadronisation into baryons with azimuthal correlations of $Λ_{\rm c}^{+}$ with charged particles in pp collisions at $\mathbf{\sqrt{\it s} = 13}$ TeV
- PWG : PWG-HF (Heavy Flavour)
- System: p-p
- Energy: 13 TeV
Search for quasi-particle scattering in the quark-gluon plasma with jet splittings in pp and Pb$-$Pb collisions at $\mathbf{\sqrt{\textit{s}_{\rm NN}} = 5.02}$ TeV
Figure 1
- Fig. Group : Search for quasi-particle scattering in the quark-gluon plasma with jet splittings in pp and Pb$-$Pb collisions at $\mathbf{\sqrt{\textit{s}_{\rm NN}} = 5.02}$ TeV
- PWG : PWG-JE (Jets)
- System: p-p, Pb-Pb
- Energy: 5.02 TeV
Figure 2
- Fig. Group : Search for quasi-particle scattering in the quark-gluon plasma with jet splittings in pp and Pb$-$Pb collisions at $\mathbf{\sqrt{\textit{s}_{\rm NN}} = 5.02}$ TeV
- PWG : PWG-JE (Jets)
- System: p-p, Pb-Pb
- Energy: 5.02 TeV
Figure 3
- Fig. Group : Search for quasi-particle scattering in the quark-gluon plasma with jet splittings in pp and Pb$-$Pb collisions at $\mathbf{\sqrt{\textit{s}_{\rm NN}} = 5.02}$ TeV
- PWG : PWG-JE (Jets)
- System: p-p, Pb-Pb
- Energy: 5.02 TeV
Figure A.1
- Fig. Group : Search for quasi-particle scattering in the quark-gluon plasma with jet splittings in pp and Pb$-$Pb collisions at $\mathbf{\sqrt{\textit{s}_{\rm NN}} = 5.02}$ TeV
- PWG : PWG-JE (Jets)
- System: p-p, Pb-Pb
- Energy: 5.02 TeV
Multiplicity dependence of K$^*(892)^{\pm}$ production in pp collisions at $\sqrt{s}$ = 13 TeV
Figure 1
- Fig. Group : Multiplicity dependence of K$^*(892)^{\pm}$ 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 K$^*(892)^{\pm}$ production in pp collisions at $\sqrt{s}$ = 13 TeV
- PWG : PWG-LF (Light Flavour Spectra)
- System: p-p
- Energy: 13 TeV
Figure 3
- Fig. Group : Multiplicity dependence of K$^*(892)^{\pm}$ 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 K$^*(892)^{\pm}$ 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 K$^*(892)^{\pm}$ production in pp collisions at $\sqrt{s}$ = 13 TeV
- PWG : PWG-LF (Light Flavour Spectra)
- 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
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