Published figures by group
Medium-induced modification of azimuthal correlations of electrons from heavy-flavor hadron decays with charged particles in Pb--Pb collisions at $\sqrt{s_{\rm{NN}} = 5.02}$ TeV
Figure 4b
- Fig. Group : Medium-induced modification of azimuthal correlations of electrons from heavy-flavor hadron decays with charged particles in Pb--Pb collisions at $\sqrt{s_{\rm{NN}} = 5.02}$ TeV
- PWG : PWG-HF (Heavy Flavour)
- System: Pb-Pb
- Energy: 5.02 TeV
Figure 5a
- Fig. Group : Medium-induced modification of azimuthal correlations of electrons from heavy-flavor hadron decays with charged particles in Pb--Pb collisions at $\sqrt{s_{\rm{NN}} = 5.02}$ TeV
- PWG : PWG-HF (Heavy Flavour)
- System: Pb-Pb
- Energy: 5.02 TeV
Figure 5b
- Fig. Group : Medium-induced modification of azimuthal correlations of electrons from heavy-flavor hadron decays with charged particles in Pb--Pb collisions at $\sqrt{s_{\rm{NN}} = 5.02}$ TeV
- PWG : PWG-HF (Heavy Flavour)
- System: Pb-Pb
- Energy: 5.02 TeV
Figure 6a
- Fig. Group : Medium-induced modification of azimuthal correlations of electrons from heavy-flavor hadron decays with charged particles in Pb--Pb collisions at $\sqrt{s_{\rm{NN}} = 5.02}$ TeV
- PWG : PWG-HF (Heavy Flavour)
- System: Pb-Pb
- Energy: 5.02 TeV
Figure 6b
- Fig. Group : Medium-induced modification of azimuthal correlations of electrons from heavy-flavor hadron decays with charged particles in Pb--Pb collisions at $\sqrt{s_{\rm{NN}} = 5.02}$ TeV
- PWG : PWG-HF (Heavy Flavour)
- System: Pb-Pb
- Energy: 5.02 TeV
Figure 7a
- Fig. Group : Medium-induced modification of azimuthal correlations of electrons from heavy-flavor hadron decays with charged particles in Pb--Pb collisions at $\sqrt{s_{\rm{NN}} = 5.02}$ TeV
- PWG : PWG-HF (Heavy Flavour)
- System: Pb-Pb
- Energy: 5.02 TeV
Figure 7b
- Fig. Group : Medium-induced modification of azimuthal correlations of electrons from heavy-flavor hadron decays with charged particles in Pb--Pb collisions at $\sqrt{s_{\rm{NN}} = 5.02}$ TeV
- PWG : PWG-HF (Heavy Flavour)
- System: Pb-Pb
- Energy: 5.02 TeV
Figure 8a
- Fig. Group : Medium-induced modification of azimuthal correlations of electrons from heavy-flavor hadron decays with charged particles in Pb--Pb collisions at $\sqrt{s_{\rm{NN}} = 5.02}$ TeV
- PWG : PWG-HF (Heavy Flavour)
- System: Pb-Pb
- Energy: 5.02 TeV
Figure 8b
- Fig. Group : Medium-induced modification of azimuthal correlations of electrons from heavy-flavor hadron decays with charged particles in Pb--Pb collisions at $\sqrt{s_{\rm{NN}} = 5.02}$ TeV
- PWG : PWG-HF (Heavy Flavour)
- System: Pb-Pb
- Energy: 5.02 TeV
Figure A.1
- Fig. Group : Medium-induced modification of azimuthal correlations of electrons from heavy-flavor hadron decays with charged particles in Pb--Pb collisions at $\sqrt{s_{\rm{NN}} = 5.02}$ TeV
- PWG : PWG-HF (Heavy Flavour)
- System: Pb-Pb
- Energy: 5.02 TeV
Figure A.2
- Fig. Group : Medium-induced modification of azimuthal correlations of electrons from heavy-flavor hadron decays with charged particles in Pb--Pb collisions at $\sqrt{s_{\rm{NN}} = 5.02}$ TeV
- PWG : PWG-HF (Heavy Flavour)
- System: 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
Study of the interaction between $Ξ$ baryons and light mesons via femtoscopy at the LHC
Figure 1
- Fig. Group : Study of the interaction between $Ξ$ baryons and light mesons via femtoscopy at the LHC
- PWG : PWG-CF (Flow and Correlations)
- System: p-p
- Energy: 13 TeV
Figure 2
- Fig. Group : Study of the interaction between $Ξ$ baryons and light mesons via femtoscopy at the LHC
- PWG : PWG-CF (Flow and Correlations)
- System: p-p
- Energy: 13 TeV
Figure 3
- Fig. Group : Study of the interaction between $Ξ$ baryons and light mesons via femtoscopy at the LHC
- PWG : PWG-CF (Flow and Correlations)
- System: p-p
- Energy: 13 TeV
Figure 4
- Fig. Group : Study of the interaction between $Ξ$ baryons and light mesons via femtoscopy at the LHC
- PWG : PWG-CF (Flow and Correlations)
- System: p-p
- Energy: 13 TeV
Figure A.1
- Fig. Group : Study of the interaction between $Ξ$ baryons and light mesons via femtoscopy at the LHC
- PWG : PWG-CF (Flow and Correlations)
- System: p-p
- Energy: 13 TeV
Figure A.2
- Fig. Group : Study of the interaction between $Ξ$ baryons and light mesons via femtoscopy at the LHC
- PWG : PWG-CF (Flow and Correlations)
- System: p-p
- Energy: 13 TeV
Figure A.3
- Fig. Group : Study of the interaction between $Ξ$ baryons and light mesons via femtoscopy at the LHC
- PWG : PWG-CF (Flow and Correlations)
- System: p-p
- Energy: 13 TeV
Measurement of the p$-Σ^+$ correlation function in pp collisions at $\sqrt{\textit{s}}=13$ TeV
Figure 1a
- Fig. Group : Measurement of the p$-Σ^+$ correlation function in pp collisions at $\sqrt{\textit{s}}=13$ TeV
- PWG : PWG-CF (Flow and Correlations)
- System: p-p
- Energy: 13 TeV
Figure 1b
- Fig. Group : Measurement of the p$-Σ^+$ correlation function in pp collisions at $\sqrt{\textit{s}}=13$ TeV
- PWG : PWG-CF (Flow and Correlations)
- System: p-p
- Energy: 13 TeV