Public Preliminary figures by analysis
Forward-backward multiplicity correlations in pp collisions expressed in terms of strongly intensive observable Σ
Σ − 1 measured for windows separated in pseudorapidity and azimuth at √s = 7 TeV
- Fig. Group : Forward-backward multiplicity correlations in pp collisions expressed in terms of strongly intensive observable Σ
- PWG : PWG-CF (Flow and Correlations)
- Energy: 7 TeV
- System: p-p
Σ − 1 measured for windows separated in pseudorapidity and azimuth at √s = 5.02 TeV
- Fig. Group : Forward-backward multiplicity correlations in pp collisions expressed in terms of strongly intensive observable Σ
- PWG : PWG-CF (Flow and Correlations)
- Energy: 5.02 TeV
- System: p-p
Σ − 1 measured for windows separated in pseudorapidity and azimuth at √s = 2.76 TeV
- Fig. Group : Forward-backward multiplicity correlations in pp collisions expressed in terms of strongly intensive observable Σ
- PWG : PWG-CF (Flow and Correlations)
- Energy: 2.76 TeV
- System: p-p
Σ − 1 measured for windows separated in pseudorapidity and azimuth at √s = 0.9 TeV
- Fig. Group : Forward-backward multiplicity correlations in pp collisions expressed in terms of strongly intensive observable Σ
- PWG : PWG-CF (Flow and Correlations)
- Energy: 900 GeV
- System: p-p
Σ - 1 in pp collisions compared to phenomenological string model at √s = 0.9, 2.76 and 7 TeV
- Fig. Group : Forward-backward multiplicity correlations in pp collisions expressed in terms of strongly intensive observable Σ
- PWG : PWG-CF (Flow and Correlations)
- Energy: 900 GeV, 2.76 TeV, 5.02 TeV, 7 TeV, 13 TeV
- System: p-p
Σ - 1 in pp collisions compared to PYTHIA8 Monash2013 with ColourReconnection off at √s = 0.9, 2.76, 5.02, 7 and 13 TeV, and EPOS at √s = 13 TeV
- Fig. Group : Forward-backward multiplicity correlations in pp collisions expressed in terms of strongly intensive observable Σ
- PWG : PWG-CF (Flow and Correlations)
- Energy: 900 GeV, 2.76 TeV, 5.02 TeV, 7 TeV, 13 TeV
- System: p-p
Σ - 1 in pp collisions compared to PYTHIA8 Monash2013 tune at √s = 0.9, 2.76, 5.02, 7 and 13 TeV, and EPOS at √s = 13 TeV
- Fig. Group : Forward-backward multiplicity correlations in pp collisions expressed in terms of strongly intensive observable Σ
- PWG : PWG-CF (Flow and Correlations)
- Energy: 900 GeV, 2.76 TeV, 5.02 TeV, 7 TeV, 13 TeV
- System: p-p
Collision energy dependence of Σ - 1
- Fig. Group : Forward-backward multiplicity correlations in pp collisions expressed in terms of strongly intensive observable Σ
- PWG : PWG-CF (Flow and Correlations)
- Energy: 900 GeV, 2.76 TeV, 5.02 TeV, 7 TeV, 13 TeV
- System: p-p
Multiplicity class dependence of Σ - 1
- Fig. Group : Forward-backward multiplicity correlations in pp collisions expressed in terms of strongly intensive observable Σ
- PWG : PWG-CF (Flow and Correlations)
- Energy: 13 TeV
- System: p-p
Lambda baryon polarization along beam direction in Pb-Pb collisions at 5.02 TeV
The rapidity dependence of the second Fourier sine coefficient of the (Λ+Λ ̄) polarization along the beam direction in Pb-Pb collisions at √sNN = 5.02 TeV.
- Fig. Group : Lambda baryon polarization along beam direction in Pb-Pb collisions at 5.02 TeV
- PWG : PWG-CF (Flow and Correlations)
- Energy: 5.02 TeV
- System: Pb-Pb
Transverse momentum dependence of the (Λ+Λ ̄) polarization along the beam direction in Pb-Pb collisions at √sNN = 5.02 TeV in semi-central collisions
- Fig. Group : Lambda baryon polarization along beam direction in Pb-Pb collisions at 5.02 TeV
- PWG : PWG-CF (Flow and Correlations)
- Energy: 5.02 TeV
- System: Pb-Pb
Centrality dependence of the second Fourier sine coefficient of the (Λ+Λ ̄) polarization along the beam direction in Pb-Pb collisions at √sNN = 5.02 TeV
- Fig. Group : Lambda baryon polarization along beam direction in Pb-Pb collisions at 5.02 TeV
- PWG : PWG-CF (Flow and Correlations)
- Energy: 5.02 TeV
- System: Pb-Pb
Fitting of second order sine Fourier coefficient of ⟨cos(θ*p⟩ as a function of invariant mass to estimate the (anti) lambda polarization along beam direction
- Fig. Group : Lambda baryon polarization along beam direction in Pb-Pb collisions at 5.02 TeV
- PWG : PWG-CF (Flow and Correlations)
- Energy: 5.02 TeV
- System: Pb-Pb
Invariant mass distribution of anti-lambda candidates in Pb-Pb collisions at 5.02 TeV
- Fig. Group : Lambda baryon polarization along beam direction in Pb-Pb collisions at 5.02 TeV
- PWG : PWG-CF (Flow and Correlations)
- Energy: 5.02 TeV
- System: Pb-Pb
v2 of jet particles in p-Pb and Pb-Pb collisions at 5.02 TeV
The jet v2 as the function of trigger particle pT, compare to ATLAS jet trigger event v2 results
- Fig. Group : v2 of jet particles in p-Pb and Pb-Pb collisions at 5.02 TeV
- PWG : PWG-CF (Flow and Correlations)
- Energy: 5.02 TeV
- System: p-Pb
The positive significance of jet v2 as the function of trigger particle pT
- Fig. Group : v2 of jet particles in p-Pb and Pb-Pb collisions at 5.02 TeV
- PWG : PWG-CF (Flow and Correlations)
- Energy: 5.02 TeV
- System: p-Pb
The jet v2 as the function of trigger particle pT, compare to inclusive v2 in p-Pb collisions
- Fig. Group : v2 of jet particles in p-Pb and Pb-Pb collisions at 5.02 TeV
- PWG : PWG-CF (Flow and Correlations)
- Energy: 5.02 TeV
- System: p-Pb
The v2 distribution and fit of TPC-TPC pairs with 3< \it{p}_{\rm T}(trig)<5 GeV/\it{c}, 1.5< \it{p}_{\rm T}(assoc)<5 GeV/\it{c}
- Fig. Group : v2 of jet particles in p-Pb and Pb-Pb collisions at 5.02 TeV
- PWG : PWG-CF (Flow and Correlations)
- Energy: 5.02 TeV
- System: p-Pb
The v2 distribution and fit of TPC-TPC pairs with 2< \it{p}_{\rm T}(trig)<3 GeV/\it{c}, 1< \it{p}_{\rm T}(assoc)<5 GeV/\it{c}
- Fig. Group : v2 of jet particles in p-Pb and Pb-Pb collisions at 5.02 TeV
- PWG : PWG-CF (Flow and Correlations)
- Energy: 5.02 TeV
- System: p-Pb
The v2 distribution and fit of TPC-TPC pairs with 1.5< \it{p}_{\rm T}(trig)<2 GeV/\it{c}, 0.5< \it{p}_{\rm T}(assoc)<5 GeV/\it{c}
- Fig. Group : v2 of jet particles in p-Pb and Pb-Pb collisions at 5.02 TeV
- PWG : PWG-CF (Flow and Correlations)
- Energy: 5.02 TeV
- System: p-Pb
The jet signal fit and background fit in TPC-TPC correlation with 3< \it{p}_{\rm T}(trig)<5 GeV/\it{c}, 1.5< \it{p}_{\rm T}(assoc)<5 GeV/\it{c}
- Fig. Group : v2 of jet particles in p-Pb and Pb-Pb collisions at 5.02 TeV
- PWG : PWG-CF (Flow and Correlations)
- Energy: 5.02 TeV
- System: p-Pb
The jet signal fit and background fit in TPC-TPC correlation with 2< \it{p}_{\rm T}(trig)<3 GeV/\it{c}, 1< \it{p}_{\rm T}(assoc)<5 GeV/\it{c}
- Fig. Group : v2 of jet particles in p-Pb and Pb-Pb collisions at 5.02 TeV
- PWG : PWG-CF (Flow and Correlations)
- Energy: 5.02 TeV
- System: p-Pb
The jet signal fit and background fit in TPC-TPC correlation with 1.5< \it{p}_{\rm T}(trig)<2 GeV/\it{c}, 0.5< \it{p}_{\rm T}(assoc)<5 GeV/\it{c}
- Fig. Group : v2 of jet particles in p-Pb and Pb-Pb collisions at 5.02 TeV
- PWG : PWG-CF (Flow and Correlations)
- Energy: 5.02 TeV
- System: p-Pb
The TPC-TPC correlation and related fit in 3< \it{p}_{\rm T}(trig)<5 GeV/\it{c}, 1.5< \it{p}_{\rm T}(assoc)<5 GeV/\it{c}
- Fig. Group : v2 of jet particles in p-Pb and Pb-Pb collisions at 5.02 TeV
- PWG : PWG-CF (Flow and Correlations)
- Energy: 5.02 TeV
- System: p-Pb
The TPC-TPC correlation and related fit in 2< \it{p}_{\rm T}(trig)<3 GeV/\it{c}, 1< \it{p}_{\rm T}(assoc)<5 GeV/\it{c}
- Fig. Group : v2 of jet particles in p-Pb and Pb-Pb collisions at 5.02 TeV
- PWG : PWG-CF (Flow and Correlations)
- Energy: 5.02 TeV
- System: p-Pb
The TPC-TPC correlation and related fit in 1.5< \it{p}_{\rm T}(trig)<2 GeV/\it{c}, 0.5< \it{p}_{\rm T}(assoc)<5 GeV/\it{c}
- Fig. Group : v2 of jet particles in p-Pb and Pb-Pb collisions at 5.02 TeV
- PWG : PWG-CF (Flow and Correlations)
- Energy: 5.02 TeV
- System: p-Pb
ZDC vs. midrapidity activity analysis
ZP vs. multiplicity in pp collisions at 13 TeV
- Fig. Group : ZDC vs. midrapidity activity analysis
- PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
- Energy: 13 TeV
- System: p-p
ZN vs. multiplicity in pp collisions at 13 TeV
- Fig. Group : ZDC vs. midrapidity activity analysis
- PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
- Energy: 13 TeV
- System: p-p
ZP vs. leading pT
- Fig. Group : ZDC vs. midrapidity activity analysis
- PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
- Energy: 13 TeV
- System: p-p
ZN vs. leading pT
- Fig. Group : ZDC vs. midrapidity activity analysis
- PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
- Energy: 13 TeV
- System: p-p
ZN spectrum in multiplicity bins in pp collisions at 13 TeV: ratio to MB
- Fig. Group : ZDC vs. midrapidity activity analysis
- PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
- Energy: 13 TeV
- System: p-p
ZN spectrum in multiplicity bins in pp collisions at 13 TeV
- Fig. Group : ZDC vs. midrapidity activity analysis
- PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
- Energy: 13 TeV
- System: p-p
p-side ZN signal vs. Ncoll in p-Pb collisions
- Fig. Group : ZDC vs. midrapidity activity analysis
- PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
- Energy: 5.02 TeV, 8 TeV
- System: p-Pb
p-side ZN signal vs. centrality in p-Pb collisions
- Fig. Group : ZDC vs. midrapidity activity analysis
- PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
- Energy: 5.02 TeV, 8 TeV
- System: p-Pb
Pb-side ZN signal vs. centrality in p-Pb collisions
- Fig. Group : ZDC vs. midrapidity activity analysis
- PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
- Energy: 5.02 TeV, 8 TeV
- System: p-Pb
ZDC asymmetry in multiplicity bins in pp collisions at 13 TeV
- Fig. Group : ZDC vs. midrapidity activity analysis
- PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
- Energy: 13 TeV
- System: p-p
ZN and ZP asymmetry in pp collisions at 13 TeV
- Fig. Group : ZDC vs. midrapidity activity analysis
- PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
- Energy: 13 TeV
- System: p-p
Very forward energy vs. multiplicity measured at midrapidity in pp and p-Pb collisions
- Fig. Group : ZDC vs. midrapidity activity analysis
- PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
- Energy: 8 TeV, 13 TeV
- System: p-p, p-Pb
ZDCA vs. ZDCC in pp collisions at 13 TeV
- Fig. Group : ZDC vs. midrapidity activity analysis
- PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
- Energy: 13 TeV
- System: p-p
ZPA vs. ZPC in pp collisions at 13 TeV
- Fig. Group : ZDC vs. midrapidity activity analysis
- PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
- Energy: 13 TeV
- System: p-p
ZNA vs. ZNC in pp collisions at 13 TeV
- Fig. Group : ZDC vs. midrapidity activity analysis
- PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
- Energy: 13 TeV
- System: p-p
B -> J/psi in p-Pb collisions at 8.16 TeV
Likelihood fit projections on invariant mass and pseudoproper decay length distributions (4 < pT < 5 GeV/c)
- Fig. Group : B -> J/psi in p-Pb collisions at 8.16 TeV
- PWG : PWG-DQ (Dileptons and Quarkonia)
- Energy: 8 TeV
- System: p-Pb
Fraction of J/ψ from beauty hadron decays in p-Pb collisions at 8.16 TeV in comparison with p-Pb measurements
- Fig. Group : B -> J/psi in p-Pb collisions at 8.16 TeV
- PWG : PWG-DQ (Dileptons and Quarkonia)
- Energy: 8 TeV
- System: p-Pb
Fraction of J/ψ from beauty hadron decays in p-Pb collisions at 8.16 TeV in comparison with pp measurements
- Fig. Group : B -> J/psi in p-Pb collisions at 8.16 TeV
- PWG : PWG-DQ (Dileptons and Quarkonia)
- Energy: 8 TeV
- System: p-Pb
Average-pT in NS-TS (Near Side/towards region) for track pT > 0.5GeV/c in pp and pPb collisions at sqrt(s) = 5.02 TeV.
- Fig. Group :
- PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
- Energy: 5.02 TeV
- System: p-p, p-Pb
Average-pT in AS-TS (Away Side/region) for track pT > 0.5GeV/c in pp and pPb collisions at sqrt(s) = 5.02 TeV.
- Fig. Group :
- PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
- Energy: 5.02 TeV
- System: p-p, p-Pb
Charged-particle sum-pT density in AS-TS (Away Side/region) for track pT > 0.5GeV/c in pp and pPb collisions at sqrt(s) = 5.02 TeV
- Fig. Group :
- PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
- Energy: 5.02 TeV
- System: p-p, p-Pb
Charged-particle sum-pT density in NS-TS (Near Side/towards region) for track pT > 0.5GeV/c in pp and pPb collisions at sqrt(s) = 5.02 TeV
- Fig. Group :
- PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
- Energy: 5.02 TeV
- System: p-p, p-Pb
Charged-particle density in AS-TS (Away Side/region) for track pT > 0.5GeV/c in pp and pPb collisions at sqrt(s) = 5.02 TeV
- Fig. Group :
- PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
- Energy: 5.02 TeV
- System: p-p, p-Pb
Charged-particle density in NS-TS (Near Side/towards region) for track pT > 0.5GeV/c in pp and pPb collisions at sqrt(s) = 5.02 TeV
- Fig. Group :
- PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
- Energy: 5.02 TeV
- System: p-p, p-Pb
Charged-particle sum-pT density in Near Side (Toward region) for track pT > 0.5GeV/c in pPb collisions at sqrt(s) = 5.02 TeV
- Fig. Group :
- PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
- Energy: 5.02 TeV
- System: p-p, p-Pb
Charged-particle sum-pT density in Transverse Side/region for track pT > 0.5GeV/c in pPb collisions at sqrt(s) = 5.02 TeV
- Fig. Group :
- PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
- Energy: 5.02 TeV
- System: p-p, p-Pb
Charged-particle sum-pT density in Away Side/region for track pT > 0.5GeV/c in pPb collisions at sqrt(s) = 5.02 TeV
- Fig. Group :
- PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
- Energy: 5.02 TeV
- System: p-p, p-Pb
Charged-particle sum-pT density in Transverse Side/region for track pT > 0.5GeV/c in pp collisions at sqrt(s) = 5.02 TeV
- Fig. Group :
- PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
- Energy: 5.02 TeV
- System: p-p, p-Pb
Charged-particle sum-pT density in Away Side/region for track pT > 0.5GeV/c in pp collisions at sqrt(s) = 5.02 TeV
- Fig. Group :
- PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
- Energy: 5.02 TeV
- System: p-p, p-Pb
Charged-particle sum-pT density in Near Side (Toward region) for track pT > 0.5GeV/c in pp collisions at sqrt(s) = 5.02 TeV
- Fig. Group :
- PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
- Energy: 5.02 TeV
- System: p-p, p-Pb
Charged-particle density in Transverse Side/region for track pT > 0.5GeV/c in pPb collisions at sqrt(s) = 5.02 TeV
- Fig. Group :
- PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
- Energy: 5.02 TeV
- System: p-p, p-Pb
Charged-particle density in Away Side/region for track pT > 0.5GeV/c in pPb collisions at sqrt(s) = 5.02 TeV
- Fig. Group :
- PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
- Energy: 5.02 TeV
- System: p-p, p-Pb
Charged-particle density in Near Side (towards region) for track pT > 0.5GeV/c in pPb collisions at sqrt(s) = 5.02 TeV
- Fig. Group :
- PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
- Energy: 5.02 TeV
- System: p-p, p-Pb
Charged-particle density in Transverse Side/region for track pT > 0.5GeV/c in pp collisions at sqrt(s) = 5.02 TeV
- Fig. Group :
- PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
- Energy: 5.02 TeV
- System: p-p, p-Pb
Charged-particle density in Near Side (towards region) for track pT > 0.5GeV/c in pp collisions at sqrt(s) = 5.02 TeV
- Fig. Group :
- PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
- Energy: 5.02 TeV
- System: p-p, p-Pb
Charged-particle density in Away Side/region for track pT > 0.5GeV/c in pp collisions at sqrt(s) = 5.02 TeV
- Fig. Group :
- PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
- Energy: 5.02 TeV
- System: p-p, p-Pb
Multiplicity and Pseudorapidity distributions of photons in p-Pb collisions at $\sqrt{s\rm_{NN}}$ = 5.02 TeV
Pseudorapidity distributions of photons compared with Charged particle measurements at Mid-rapidity in p-Pb collisions at $\sqrt{s\rm_{NN}}$ = 5.02 TeV
- Fig. Group : Multiplicity and Pseudorapidity distributions of photons in p-Pb collisions at $\sqrt{s\rm_{NN}}$ = 5.02 TeV
- PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
- Energy: 5.02 TeV
- System: p-Pb
Centrality dependent Pseudorapidity distributions of photons compared with HIJING in p-Pb collisions at $\sqrt{s\rm_{NN}}$ = 5.02 TeV
- Fig. Group : Multiplicity and Pseudorapidity distributions of photons in p-Pb collisions at $\sqrt{s\rm_{NN}}$ = 5.02 TeV
- PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
- Energy: 5.02 TeV
- System: p-Pb
Centrality dependent Pseudorapidity distributions of photons compared with DPMJET in p-Pb collisions at $\sqrt{s\rm_{NN}}$ = 5.02 TeV
- Fig. Group : Multiplicity and Pseudorapidity distributions of photons in p-Pb collisions at $\sqrt{s\rm_{NN}}$ = 5.02 TeV
- PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
- Energy: 5.02 TeV
- System: p-Pb
Centrality dependent Pseudorapidity distributions of photons in p-Pb collisions at $\sqrt{s\rm_{NN}}$ = 5.02 TeV
- Fig. Group : Multiplicity and Pseudorapidity distributions of photons in p-Pb collisions at $\sqrt{s\rm_{NN}}$ = 5.02 TeV
- PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
- Energy: 5.02 TeV
- System: p-Pb
Pseudorapidity distributions of photons in p-Pb collisions at $\sqrt{s\rm_{NN}}$ = 5.02 TeV
- Fig. Group : Multiplicity and Pseudorapidity distributions of photons in p-Pb collisions at $\sqrt{s\rm_{NN}}$ = 5.02 TeV
- PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
- Energy: 5.02 TeV
- System: p-Pb
Multiplicity distribution of photons in p-Pb collisions at $\sqrt{s\rm_{NN}}$ = 5.02 TeV
- Fig. Group : Multiplicity and Pseudorapidity distributions of photons in p-Pb collisions at $\sqrt{s\rm_{NN}}$ = 5.02 TeV
- PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
- Energy: 5.02 TeV
- System: p-Pb
Search for Chiral Magnetic Wave using ALICE detector in Pb-Pb collisions at $\sqrt{s_{NN}} =$ 5.02 TeV
Normalised Delta v3 of pions
- Fig. Group : Search for Chiral Magnetic Wave using ALICE detector in Pb-Pb collisions at $\sqrt{s_{NN}} =$ 5.02 TeV
- PWG : PWG-CF (Flow and Correlations)
- Energy: 5.02 TeV
- System: Pb-Pb
Normalised Delta v2 of pions
- Fig. Group : Search for Chiral Magnetic Wave using ALICE detector in Pb-Pb collisions at $\sqrt{s_{NN}} =$ 5.02 TeV
- PWG : PWG-CF (Flow and Correlations)
- Energy: 5.02 TeV
- System: Pb-Pb
Normalised Delta v3 of hadrons
- Fig. Group : Search for Chiral Magnetic Wave using ALICE detector in Pb-Pb collisions at $\sqrt{s_{NN}} =$ 5.02 TeV
- PWG : PWG-CF (Flow and Correlations)
- Energy: 5.02 TeV
- System: Pb-Pb
Normalised Delta v2 of hadrons
- Fig. Group : Search for Chiral Magnetic Wave using ALICE detector in Pb-Pb collisions at $\sqrt{s_{NN}} =$ 5.02 TeV
- PWG : PWG-CF (Flow and Correlations)
- Energy: 5.02 TeV
- System: Pb-Pb
v3vsAch of pions
- Fig. Group : Search for Chiral Magnetic Wave using ALICE detector in Pb-Pb collisions at $\sqrt{s_{NN}} =$ 5.02 TeV
- PWG : PWG-CF (Flow and Correlations)
- Energy: 5.02 TeV
- System: Pb-Pb
v2vsAch of pions
- Fig. Group : Search for Chiral Magnetic Wave using ALICE detector in Pb-Pb collisions at $\sqrt{s_{NN}} =$ 5.02 TeV
- PWG : PWG-CF (Flow and Correlations)
- Energy: 5.02 TeV
- System: Pb-Pb
v3vsAch of hadrons
- Fig. Group : Search for Chiral Magnetic Wave using ALICE detector in Pb-Pb collisions at $\sqrt{s_{NN}} =$ 5.02 TeV
- PWG : PWG-CF (Flow and Correlations)
- Energy: 5.02 TeV
- System: Pb-Pb
v2vsAch of hadrons
- Fig. Group : Search for Chiral Magnetic Wave using ALICE detector in Pb-Pb collisions at $\sqrt{s_{NN}} =$ 5.02 TeV
- PWG : PWG-CF (Flow and Correlations)
- Energy: 5.02 TeV
- System: Pb-Pb
Normalisedv3slope comparison of hadrons between ALICE and CMS
- Fig. Group : Search for Chiral Magnetic Wave using ALICE detector in Pb-Pb collisions at $\sqrt{s_{NN}} =$ 5.02 TeV
- PWG : PWG-CF (Flow and Correlations)
- Energy: 5.02 TeV
- System: Pb-Pb
Normalisedv2slope comparison of hadrons between ALICE and CMS
- Fig. Group : Search for Chiral Magnetic Wave using ALICE detector in Pb-Pb collisions at $\sqrt{s_{NN}} =$ 5.02 TeV
- PWG : PWG-CF (Flow and Correlations)
- Energy: 5.02 TeV
- System: Pb-Pb
Normalisedv3slope comparison of pions between ALICE and STAR
- Fig. Group : Search for Chiral Magnetic Wave using ALICE detector in Pb-Pb collisions at $\sqrt{s_{NN}} =$ 5.02 TeV
- PWG : PWG-CF (Flow and Correlations)
- Energy: 5.02 TeV
- System: Pb-Pb
Normalisedv2slope comparison of pions between ALICE and STAR
- Fig. Group : Search for Chiral Magnetic Wave using ALICE detector in Pb-Pb collisions at $\sqrt{s_{NN}} =$ 5.02 TeV
- PWG : PWG-CF (Flow and Correlations)
- Energy: 5.02 TeV
- System: Pb-Pb
Normalisedv3slope comparison of pions with hadrons
- Fig. Group : Search for Chiral Magnetic Wave using ALICE detector in Pb-Pb collisions at $\sqrt{s_{NN}} =$ 5.02 TeV
- PWG : PWG-CF (Flow and Correlations)
- Energy: 5.02 TeV
- System: Pb-Pb
Normalisedv2v3slope comparison of pions
- Fig. Group : Search for Chiral Magnetic Wave using ALICE detector in Pb-Pb collisions at $\sqrt{s_{NN}} =$ 5.02 TeV
- PWG : PWG-CF (Flow and Correlations)
- Energy: 5.02 TeV
- System: Pb-Pb
Normalisedv2v3slope comparison of hadrons
- Fig. Group : Search for Chiral Magnetic Wave using ALICE detector in Pb-Pb collisions at $\sqrt{s_{NN}} =$ 5.02 TeV
- PWG : PWG-CF (Flow and Correlations)
- Energy: 5.02 TeV
- System: Pb-Pb
Per-trigger associated yield, K-h, h-K for [HP2020]
\Delta\varphi Projection of h-K^0_S - MC comparison
- Fig. Group : Per-trigger associated yield, K-h, h-K for [HP2020]
- PWG : PWG-CF (Flow and Correlations)
- Energy: 13 TeV
- System: p-p
Paper Figures: Measurement of isolated photon–hadron correlations in pp and p–Pb collisions at 5TeV
Isolated photon-hadron correlation functions in pp and p–Pb at sqrt(s) = 5.02 TeV, remaining zT bins
- Fig. Group : Paper Figures: Measurement of isolated photon–hadron correlations in pp and p–Pb collisions at 5TeV
- PWG : PWG-GA (Photons, Neutral Mesons)
- Energy: 5.02 TeV
- System: p-p, p-Pb
Signal region and background region correlation function comparison in p–Pb at sqrt(s) = 5.02 TeV
- Fig. Group : Paper Figures: Measurement of isolated photon–hadron correlations in pp and p–Pb collisions at 5TeV
- PWG : PWG-GA (Photons, Neutral Mesons)
- Energy: 5.02 TeV
- System: p-Pb
ML based background correction for full jets in Pb--Pb at 5.02 TeV
ML Pb--Pb Spectrum R = 0.4, 0-10%, Compared to AB method
- Fig. Group : ML based background correction for full jets in Pb--Pb at 5.02 TeV
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: Pb-Pb
ML Raa Fragmentation Bias Curves with Model Comparisons R = 0.4, 0-10%
- Fig. Group : ML based background correction for full jets in Pb--Pb at 5.02 TeV
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: Pb-Pb
ML Full Jet Raa, R = 0.4, 0-10%
- Fig. Group : ML based background correction for full jets in Pb--Pb at 5.02 TeV
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: Pb-Pb
ML Pb--Pb Full Jet Spectrum R = 0.4, 0-10%
- Fig. Group : ML based background correction for full jets in Pb--Pb at 5.02 TeV
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: Pb-Pb
ML Raa with Fragmentation Bias Curves
- Fig. Group : ML based background correction for full jets in Pb--Pb at 5.02 TeV
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: Pb-Pb
hadron+jet acoplanarity measurement in Pb-Pb collisions (HP2020)
R=0.2 Uncorrected (raw) hadron+jet $\Delta_{recoil}$ vs $\Delta\phi$ distributions for $30 < p_{\mathrm{T,jet}^{ch}} < 40$ GeV/c in 0-10% Pb-Pb collisions at $\sqrt{\it{s}_{NN}} = 5.02$ TeV
- Fig. Group : hadron+jet acoplanarity measurement in Pb-Pb collisions (HP2020)
- PWG : PWG-JE (Jets)
- Energy: 5.02 TeV
- System: Pb-Pb
Jpsi polarization in PbPb collisions at sqrtsNN 5.02 TeV
Acceptance-times-efficiency for J/psi as function of CosTheta and Centrality in the Helicity reference frame
- Fig. Group : Jpsi polarization in PbPb collisions at sqrtsNN 5.02 TeV
- PWG : PWG-DQ (Dileptons and Quarkonia)
- Energy: 5.02 TeV
- System: Pb-Pb
Fit to the corrected J/psi distribution as a function of cosTheta in 0-20% and 60-90% centrality classes
- Fig. Group : Jpsi polarization in PbPb collisions at sqrtsNN 5.02 TeV
- PWG : PWG-DQ (Dileptons and Quarkonia)
- Energy: 5.02 TeV
- System: Pb-Pb
Fit to the J/psi distribution as a function of cosTheta for 0-20% and 60-90% centrality classes
- Fig. Group : Jpsi polarization in PbPb collisions at sqrtsNN 5.02 TeV
- PWG : PWG-DQ (Dileptons and Quarkonia)
- Energy: 5.02 TeV
- System: Pb-Pb
Low mass dimuons
Self normalization yield of omega-meson at 6.0-8.0 GeV/c at forward-rapidity (2.5<y<4.0) as a function of the charged particle multiplicity at mid-rapidity (|\eta|<1.0) compared with Pythia8 predictions (Color rope + hadronic rescattering)
- Fig. Group : Low mass dimuons
- PWG : PWG-LF (Light Flavour Spectra)
- Energy: 13 TeV
- System: p-p
Self normalization yield of omega-meson at 2.5-3.0 GeV/c at forward-rapidity (2.5<y<4.0) as a function of the charged particle multiplicity at mid-rapidity (|\eta|<1.0) compared with Pythia8 predictions (Color rope + hadronic rescattering)
- Fig. Group : Low mass dimuons
- PWG : PWG-LF (Light Flavour Spectra)
- Energy: 13 TeV
- System: p-p
Self normalization yield of omega-meson at 0.5-1.0 GeV/c at forward-rapidity (2.5<y<4.0) as a function of the charged particle multiplicity at mid-rapidity (|\eta|<1.0) compared with Pythia8 predictions (Color rope + hadronic rescattering)
- Fig. Group : Low mass dimuons
- PWG : PWG-LF (Light Flavour Spectra)
- Energy: 13 TeV
- System: p-p
Self normalization yield of phi-meson at 6.0-8.0 GeV/c at forward-rapidity (2.5<y<4.0) as a function of the charged particle multiplicity at mid-rapidity (|\eta|<1.0) compared with Pythia8 predictions (Color rope + hadronic rescattering)
- Fig. Group : Low mass dimuons
- PWG : PWG-LF (Light Flavour Spectra)
- Energy: 13 TeV
- System: p-p
Self normalization yield of phi-meson at 2.5-3.0 GeV/c at forward-rapidity (2.5<y<4.0) as a function of the charged particle multiplicity at mid-rapidity (|\eta|<1.0) compared with Pythia8 predictions (Color rope + hadronic rescattering)
- Fig. Group : Low mass dimuons
- PWG : PWG-LF (Light Flavour Spectra)
- Energy: 13 TeV
- System: p-p