Published figures by group
Direct-photon production in inelastic and high-multiplicity proton-proton collisions at $\sqrt{s} =$ 13 TeV
Figure 1a
- Fig. Group : Direct-photon production in inelastic and high-multiplicity proton-proton collisions at $\sqrt{s} =$ 13 TeV
- PWG : PWG-EM (Electromagnetic probes)
- System: p-p
- Energy: 13 TeV
Figure 1b
- Fig. Group : Direct-photon production in inelastic and high-multiplicity proton-proton collisions at $\sqrt{s} =$ 13 TeV
- PWG : PWG-EM (Electromagnetic probes)
- System: p-p
- Energy: 13 TeV
Figure 2a
- Fig. Group : Direct-photon production in inelastic and high-multiplicity proton-proton collisions at $\sqrt{s} =$ 13 TeV
- PWG : PWG-EM (Electromagnetic probes)
- System: p-p
- Energy: 13 TeV
Figure 2b
- Fig. Group : Direct-photon production in inelastic and high-multiplicity proton-proton collisions at $\sqrt{s} =$ 13 TeV
- PWG : PWG-EM (Electromagnetic probes)
- System: p-p
- Energy: 13 TeV
Figure 3a
- Fig. Group : Direct-photon production in inelastic and high-multiplicity proton-proton collisions at $\sqrt{s} =$ 13 TeV
- PWG : PWG-EM (Electromagnetic probes)
- System: p-p
- Energy: 13 TeV
Figure 3b
- Fig. Group : Direct-photon production in inelastic and high-multiplicity proton-proton collisions at $\sqrt{s} =$ 13 TeV
- PWG : PWG-EM (Electromagnetic probes)
- System: p-p
- Energy: 13 TeV
Figure 4
- Fig. Group : Direct-photon production in inelastic and high-multiplicity proton-proton collisions at $\sqrt{s} =$ 13 TeV
- PWG : PWG-EM (Electromagnetic probes)
- System: p-p
- Energy: 13 TeV
Figure A.1a
- Fig. Group : Direct-photon production in inelastic and high-multiplicity proton-proton collisions at $\sqrt{s} =$ 13 TeV
- PWG : PWG-EM (Electromagnetic probes)
- System: p-p
- Energy: 13 TeV
Figure A.1b
- Fig. Group : Direct-photon production in inelastic and high-multiplicity proton-proton collisions at $\sqrt{s} =$ 13 TeV
- PWG : PWG-EM (Electromagnetic probes)
- System: p-p
- Energy: 13 TeV
Figure A.2a
- Fig. Group : Direct-photon production in inelastic and high-multiplicity proton-proton collisions at $\sqrt{s} =$ 13 TeV
- PWG : PWG-EM (Electromagnetic probes)
- System: p-p
- Energy: 13 TeV
Figure A.2b
- Fig. Group : Direct-photon production in inelastic and high-multiplicity proton-proton collisions at $\sqrt{s} =$ 13 TeV
- PWG : PWG-EM (Electromagnetic probes)
- System: p-p
- Energy: 13 TeV
Studying charm hadronisation into baryons with azimuthal correlations of $Λ_{\rm c}^{+}$ with charged particles in pp collisions at $\mathbf{\sqrt{s} = 13}$ TeV
Figure 1
- Fig. Group : Studying charm hadronisation into baryons with azimuthal correlations of $Λ_{\rm c}^{+}$ with charged particles in pp collisions at $\mathbf{\sqrt{s} = 13}$ 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 $\mathbf{\sqrt{s} = 13}$ 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 $\mathbf{\sqrt{s} = 13}$ 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 $\mathbf{\sqrt{s} = 13}$ 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 $\mathbf{\sqrt{s} = 13}$ 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 $\mathbf{\sqrt{s} = 13}$ 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 $\mathbf{\sqrt{s} = 13}$ TeV
- PWG : PWG-HF (Heavy Flavour)
- System: p-p
- Energy: 13 TeV
Observation of partonic flow in proton-proton and proton-nucleus collisions
Figure 1
- Fig. Group : Observation of partonic flow in proton-proton and proton-nucleus collisions
- PWG : PWG-CF (Flow and Correlations)
- System: p-p, p-Pb
- Energy: 5.02 TeV, 13 TeV
Figure 2
- Fig. Group : Observation of partonic flow in proton-proton and proton-nucleus collisions
- PWG : PWG-CF (Flow and Correlations)
- System: p-p, p-Pb
- Energy: 5.02 TeV, 13 TeV
Figure 3
- Fig. Group : Observation of partonic flow in proton-proton and proton-nucleus collisions
- PWG : PWG-CF (Flow and Correlations)
- System: p-p, p-Pb
- Energy: 5.02 TeV, 13 TeV
Figure 4
- Fig. Group : Observation of partonic flow in proton-proton and proton-nucleus collisions
- PWG : PWG-CF (Flow and Correlations)
- System: p-p, p-Pb
- Energy: 5.02 TeV, 13 TeV
System size and energy dependence of the mean transverse momentum fluctuations at the LHC
Figure 1
- 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 2a
- 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 2b
- 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