Published figures by group
Multiplicity dependence of the size of the common hadron emission source in pp collisions at the LHC
Figure A.9a
- Fig. Group : Multiplicity dependence of the size of the common hadron emission source in pp collisions at the LHC
- PWG : PWG-CF (Flow and Correlations)
- System: p-p
- Energy: 13.6 TeV
Figure A.9b
- Fig. Group : Multiplicity dependence of the size of the common hadron emission source in pp collisions at the LHC
- PWG : PWG-CF (Flow and Correlations)
- System: p-p
- Energy: 13.6 TeV
Figure A.10a
- Fig. Group : Multiplicity dependence of the size of the common hadron emission source in pp collisions at the LHC
- PWG : PWG-CF (Flow and Correlations)
- System: p-p
- Energy: 13.6 TeV
Figure A.10b
- Fig. Group : Multiplicity dependence of the size of the common hadron emission source in pp collisions at the LHC
- PWG : PWG-CF (Flow and Correlations)
- System: p-p
- Energy: 13.6 TeV
Figure A.11a
- Fig. Group : Multiplicity dependence of the size of the common hadron emission source in pp collisions at the LHC
- PWG : PWG-CF (Flow and Correlations)
- System: p-p
- Energy: 13.6 TeV
Figure A.11b
- Fig. Group : Multiplicity dependence of the size of the common hadron emission source in pp collisions at the LHC
- PWG : PWG-CF (Flow and Correlations)
- System: p-p
- Energy: 13.6 TeV
Figure A.12a
- Fig. Group : Multiplicity dependence of the size of the common hadron emission source in pp collisions at the LHC
- PWG : PWG-CF (Flow and Correlations)
- System: p-p
- Energy: 13.6 TeV
Figure A.12b
- Fig. Group : Multiplicity dependence of the size of the common hadron emission source in pp collisions at the LHC
- PWG : PWG-CF (Flow and Correlations)
- System: p-p
- Energy: 13.6 TeV
Figure A.13a
- Fig. Group : Multiplicity dependence of the size of the common hadron emission source in pp collisions at the LHC
- PWG : PWG-CF (Flow and Correlations)
- System: p-p
- Energy: 13.6 TeV
Figure A.13b
- Fig. Group : Multiplicity dependence of the size of the common hadron emission source in pp collisions at the LHC
- PWG : PWG-CF (Flow and Correlations)
- System: p-p
- Energy: 13.6 TeV
Figure A.14a
- Fig. Group : Multiplicity dependence of the size of the common hadron emission source in pp collisions at the LHC
- PWG : PWG-CF (Flow and Correlations)
- System: p-p
- Energy: 13.6 TeV
Figure A.14b
- Fig. Group : Multiplicity dependence of the size of the common hadron emission source in pp collisions at the LHC
- PWG : PWG-CF (Flow and Correlations)
- System: p-p
- Energy: 13.6 TeV
Figure A.15a
- Fig. Group : Multiplicity dependence of the size of the common hadron emission source in pp collisions at the LHC
- PWG : PWG-CF (Flow and Correlations)
- System: p-p
- Energy: 13.6 TeV
Figure A.15b
- Fig. Group : Multiplicity dependence of the size of the common hadron emission source in pp collisions at the LHC
- PWG : PWG-CF (Flow and Correlations)
- System: p-p
- Energy: 13.6 TeV
Figure A.16
- Fig. Group : Multiplicity dependence of the size of the common hadron emission source in pp collisions at the LHC
- PWG : PWG-CF (Flow and Correlations)
- System: p-p
- Energy: 13.6 TeV
Figure A.17
- Fig. Group : Multiplicity dependence of the size of the common hadron emission source in pp collisions at the LHC
- PWG : PWG-CF (Flow and Correlations)
- System: p-p
- Energy: 13.6 TeV
Figure A.18
- Fig. Group : Multiplicity dependence of the size of the common hadron emission source in pp collisions at the LHC
- PWG : PWG-CF (Flow and Correlations)
- System: p-p
- Energy: 13.6 TeV
Figure A.19
- Fig. Group : Multiplicity dependence of the size of the common hadron emission source in pp collisions at the LHC
- PWG : PWG-CF (Flow and Correlations)
- System: p-p
- Energy: 13.6 TeV
Figure A.20
- Fig. Group : Multiplicity dependence of the size of the common hadron emission source in pp collisions at the LHC
- PWG : PWG-CF (Flow and Correlations)
- System: p-p
- Energy: 13.6 TeV
Evidence for parton energy loss in oxygen$-$oxygen collisions at $\mathbf{\sqrt{s_{\rm NN}}=5.36}$ TeV
Figure 1
- Fig. Group : Evidence for parton energy loss in oxygen$-$oxygen collisions at $\mathbf{\sqrt{s_{\rm NN}}=5.36}$ TeV
- PWG : PWG-EM (Electromagnetic probes)
- System: O-O, p-O, p-p
- Energy: 5.36 TeV, 9.61 TeV, 13.6 TeV
Figure 2
- Fig. Group : Evidence for parton energy loss in oxygen$-$oxygen collisions at $\mathbf{\sqrt{s_{\rm NN}}=5.36}$ TeV
- PWG : PWG-EM (Electromagnetic probes)
- System: O-O, p-O, p-p
- Energy: 5.36 TeV, 9.61 TeV, 13.6 TeV
Figure 3
- Fig. Group : Evidence for parton energy loss in oxygen$-$oxygen collisions at $\mathbf{\sqrt{s_{\rm NN}}=5.36}$ TeV
- PWG : PWG-EM (Electromagnetic probes)
- System: O-O, p-O, p-p
- Energy: 5.36 TeV, 9.61 TeV, 13.6 TeV
Probing flavor effects in the QCD parton shower using $\mathbf{{\rm D}^0}$-tagged jet angularities in proton$-$proton collisions at $\mathbf{ \sqrt{s} = 5.02}$ TeV
Figure 1a
- Fig. Group : Probing flavor effects in the QCD parton shower using $\mathbf{{\rm D}^0}$-tagged jet angularities in proton$-$proton collisions at $\mathbf{ \sqrt{s} = 5.02}$ TeV
- PWG : PWG-HF (Heavy Flavour)
- System: p-p
- Energy: 5.02 TeV
Figure 1b
- Fig. Group : Probing flavor effects in the QCD parton shower using $\mathbf{{\rm D}^0}$-tagged jet angularities in proton$-$proton collisions at $\mathbf{ \sqrt{s} = 5.02}$ TeV
- PWG : PWG-HF (Heavy Flavour)
- System: p-p
- Energy: 5.02 TeV
Figure 2
- Fig. Group : Probing flavor effects in the QCD parton shower using $\mathbf{{\rm D}^0}$-tagged jet angularities in proton$-$proton collisions at $\mathbf{ \sqrt{s} = 5.02}$ TeV
- PWG : PWG-HF (Heavy Flavour)
- System: p-p
- Energy: 5.02 TeV