User

Roles
Anonymous

Public Preliminary figures by analysis

Public Preliminary figures by analysis

J/psi production at mid-rapidity 5.02 TeV Pb-Pb Run 2018

RAA vs charged particle density of inclusive jpsi at mid-rapidity at sNN = 5.02 (2018 dataset), 2.76 and 0.2 TeV

  • Fig. Group : J/psi production at mid-rapidity 5.02 TeV Pb-Pb Run 2018
  • PWG : PWG-DQ (Dileptons and Quarkonia)
  • Energy: 5.02 TeV
  • System: Pb-Pb

    • Antinuclei inelastic cross section constraints in high multiplicity pp [Spring2020]

    Comparison of antideuteron-to-deuteron ratio in pp and in p-Pb collisions

  • Fig. Group : Antinuclei inelastic cross section constraints in high multiplicity pp [Spring2020]
  • PWG : PWG-LF (Light Flavour Spectra)
  • Energy: 5.02 TeV
    • ,
  • Energy: 13 TeV
  • System: p-p
    • ,
  • System: Pb-Pb

    • Comparison of antiproton-to-proton ratio in pp and in p-Pb collisions

  • Fig. Group : Antinuclei inelastic cross section constraints in high multiplicity pp [Spring2020]
  • PWG : PWG-LF (Light Flavour Spectra)
  • Energy: 5.02 TeV
    • ,
  • Energy: 13 TeV
  • System: p-p
    • ,
  • System: p-Pb

    • Per-trigger associated yield, K-h, h-K for [HP2020]

    Per-trigger associated yield from h-K correlations - 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

    • Ratios of per-trigger yield of the away-side peak (K0-h/h-h) - multiplicity -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

    • Ratios of per-trigger yield of the near-side peak (K0-h/h-h) - multiplicity -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

    • Ratios of per-trigger yield of the near-side peak (h-K0/h-h) - multiplicity -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

    • Ratios of per-trigger yield of the away-side peak (h-K0/h-h) - multiplicity -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

    • Ratios of per-trigger yield of the away-side peak (K0-h/h-h) as a function of p_T^{assoc} -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

    • Ratios of per-trigger yield of the near-side peak (K0-h/h-h) as a function of p_T^{assoc} -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

    • Ratios of per-trigger yield of the near-side peak (h-K0/h-h) as a function of p_T^{assoc} -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

    • Ratios of per-trigger yield of the away-side peak (h-K0/h-h) as a function of p_T^{assoc} - 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

    • \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
    • ,
  • System: 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

    • Groomed substructure of D0-tagged and inclusive jets in pp at 13 TeV

    Rg of inclusive jets in pp at 13 TeV, response matrix

  • Fig. Group : Groomed substructure of D0-tagged and inclusive jets in pp at 13 TeV
  • PWG : PWG-JE (Jets)
  • Energy: 13 TeV
  • System: p-p

    • zg of inclusive jets in pp at 13 TeV, response matrix

  • Fig. Group : Groomed substructure of D0-tagged and inclusive jets in pp at 13 TeV
  • PWG : PWG-JE (Jets)
  • Energy: 13 TeV
  • System: p-p

    • nSD of inclusive jets in pp at 13 TeV, response matrix

  • Fig. Group : Groomed substructure of D0-tagged and inclusive jets in pp at 13 TeV
  • PWG : PWG-JE (Jets)
  • Energy: 13 TeV
  • System: p-p

    • Rg of inclusive jets in pp at 13 TeV, systematic uncertainties

  • Fig. Group : Groomed substructure of D0-tagged and inclusive jets in pp at 13 TeV
  • PWG : PWG-JE (Jets)
  • Energy: 13 TeV
  • System: p-p

    • zg of inclusive jets in pp at 13 TeV, systematic uncertainties

  • Fig. Group : Groomed substructure of D0-tagged and inclusive jets in pp at 13 TeV
  • PWG : PWG-JE (Jets)
  • Energy: 13 TeV
  • System: p-p

    • nSD of inclusive jets in pp at 13 TeV, systematic uncertainties

  • Fig. Group : Groomed substructure of D0-tagged and inclusive jets in pp at 13 TeV
  • PWG : PWG-JE (Jets)
  • Energy: 13 TeV
  • System: p-p

    • Rg of D0-tagged jets in pp at 13 TeV, response matrix

  • Fig. Group : Groomed substructure of D0-tagged and inclusive jets in pp at 13 TeV
  • PWG : PWG-JE (Jets)
  • Energy: 13 TeV
  • System: p-p

    • zg of D0-tagged jets in pp at 13 TeV, response matrix

  • Fig. Group : Groomed substructure of D0-tagged and inclusive jets in pp at 13 TeV
  • PWG : PWG-JE (Jets)
  • Energy: 13 TeV
  • System: p-p

    • nSD of D0-tagged jets in pp at 13 TeV, response matrix

  • Fig. Group : Groomed substructure of D0-tagged and inclusive jets in pp at 13 TeV
  • PWG : PWG-JE (Jets)
  • Energy: 13 TeV
  • System: p-p

    • Rg of D0-tagged jets in pp at 13 TeV, systematic uncertainties

  • Fig. Group : Groomed substructure of D0-tagged and inclusive jets in pp at 13 TeV
  • PWG : PWG-JE (Jets)
  • Energy: 13 TeV
  • System: p-p

    • zg of D0-tagged jets in pp at 13 TeV, systematic uncertainties

  • Fig. Group : Groomed substructure of D0-tagged and inclusive jets in pp at 13 TeV
  • PWG : PWG-JE (Jets)
  • Energy: 13 TeV
  • System: p-p

    • nSD of D0-tagged jets in pp at 13 TeV, systematic uncertainties

  • Fig. Group : Groomed substructure of D0-tagged and inclusive jets in pp at 13 TeV
  • PWG : PWG-JE (Jets)
  • Energy: 13 TeV
  • System: p-p

    • Rg of D0-tagged jets in pp at 13 TeV, feed-down fraction

  • Fig. Group : Groomed substructure of D0-tagged and inclusive jets in pp at 13 TeV
  • PWG : PWG-JE (Jets)
  • Energy: 13 TeV
  • System: p-p

    • zg of D0-tagged jets in pp at 13 TeV, feed-down fraction

  • Fig. Group : Groomed substructure of D0-tagged and inclusive jets in pp at 13 TeV
  • PWG : PWG-JE (Jets)
  • Energy: 13 TeV
  • System: p-p

    • nSD of D0-tagged jets in pp at 13 TeV, feed-down fraction

  • Fig. Group : Groomed substructure of D0-tagged and inclusive jets in pp at 13 TeV
  • PWG : PWG-JE (Jets)
  • Energy: 13 TeV
  • System: p-p

    • Rg of D0-tagged jets in pp at 13 TeV, sideband subtraction, pT D0 12-16 GeV/c

  • Fig. Group : Groomed substructure of D0-tagged and inclusive jets in pp at 13 TeV
  • PWG : PWG-JE (Jets)
  • Energy: 13 TeV
  • System: p-p

    • Measurements of groomed jet splittings in semi-central and pp collisions at 5.02 TeV

    Fully unfolded nSD distribution in semi-central and pp collisions with zcut=0.2 (theory comparison)

  • Fig. Group : Measurements of groomed jet splittings in semi-central and pp collisions at 5.02 TeV
  • PWG : PWG-JE (Jets)
  • Energy: 5.02 TeV
  • System: Pb-Pb

    • Fully unfolded zg distribution in semi-central and pp collisions (theory comparison)

  • Fig. Group : Measurements of groomed jet splittings in semi-central and pp collisions at 5.02 TeV
  • PWG : PWG-JE (Jets)
  • Energy: 5.02 TeV
  • System: Pb-Pb

    • Performance of the event-by-event constituent subtraction method on the residual pT distribution in embedded PYTHIA with SD z=0.2 for different Rmax values

  • Fig. Group : Measurements of groomed jet splittings in semi-central and pp collisions at 5.02 TeV
  • PWG : PWG-JE (Jets)
  • Energy: 5.02 TeV
  • System: Pb-Pb

    • Performance of the event-by-event constituent subtraction method on the Rg distribution in embedded PYTHIA with SD z=0.2 for different Rmax values

  • Fig. Group : Measurements of groomed jet splittings in semi-central and pp collisions at 5.02 TeV
  • PWG : PWG-JE (Jets)
  • Energy: 5.02 TeV
  • System: Pb-Pb

    • Performance of the event-by-event constituent subtraction method on the Rg distribution in embedded PYTHIA with SD z=0.4

  • Fig. Group : Measurements of groomed jet splittings in semi-central and pp collisions at 5.02 TeV
  • PWG : PWG-JE (Jets)
  • Energy: 5.02 TeV
  • System: Pb-Pb

    • Performance of the event-by-event constituent subtraction method on the Rg distribution in embedded PYTHIA with SD z=0.2

  • Fig. Group : Measurements of groomed jet splittings in semi-central and pp collisions at 5.02 TeV
  • PWG : PWG-JE (Jets)
  • Energy: 5.02 TeV
  • System: Pb-Pb

    • Fully unfolded Rg distribution in semi-central and pp collisions with zcut=0.4 (theory comparison)

  • Fig. Group : Measurements of groomed jet splittings in semi-central and pp collisions at 5.02 TeV
  • PWG : PWG-JE (Jets)
  • Energy: 5.02 TeV
  • System: Pb-Pb

    • Fully unfolded Rg distribution in semi-central and pp collisions with zcut=0.2 (theory comparison)

  • Fig. Group : Measurements of groomed jet splittings in semi-central and pp collisions at 5.02 TeV
  • PWG : PWG-JE (Jets)
  • Energy: 5.02 TeV
  • System: Pb-Pb

    • Performance of the jet-by-jet and event-by-event constituent subtraction method on the Rg distribution in embedded PYTHIA

  • Fig. Group : Measurements of groomed jet splittings in semi-central and pp collisions at 5.02 TeV
  • PWG : PWG-JE (Jets)
  • Energy: 5.02 TeV
  • System: Pb-Pb

    • Fully unfolded nSD distribution in pp collisions compared to PYTHIA8

  • Fig. Group : Measurements of groomed jet splittings in semi-central and pp collisions at 5.02 TeV
  • PWG : PWG-JE (Jets)
  • Energy: 5.02 TeV
  • System: Pb-Pb

    • Fully unfolded Rg distribution in pp collisions compared to Pythia8 with SD zcut=0.4

  • Fig. Group : Measurements of groomed jet splittings in semi-central and pp collisions at 5.02 TeV
  • PWG : PWG-JE (Jets)
  • Energy: 5.02 TeV
  • System: Pb-Pb

    • Fully unfolded Rg distribution in semi-central and pp collisions with zcut=0.4

  • Fig. Group : Measurements of groomed jet splittings in semi-central and pp collisions at 5.02 TeV
  • PWG : PWG-JE (Jets)
  • Energy: 5.02 TeV
  • System: Pb-Pb

    • Fully unfolded nSD distribution in semi-central and pp collisions

  • Fig. Group : Measurements of groomed jet splittings in semi-central and pp collisions at 5.02 TeV
  • PWG : PWG-JE (Jets)
  • Energy: 5.02 TeV
  • System: Pb-Pb

    • Fully unfolded zg distribution in semi-central and pp collisions

  • Fig. Group : Measurements of groomed jet splittings in semi-central and pp collisions at 5.02 TeV
  • PWG : PWG-JE (Jets)
  • Energy: 5.02 TeV
  • System: Pb-Pb

    • Fully unfolded Rg distribution in semi-central and pp collisions with zcut=0.2

  • Fig. Group : Measurements of groomed jet splittings in semi-central and pp collisions at 5.02 TeV
  • PWG : PWG-JE (Jets)
  • Energy: 5.02 TeV
  • System: Pb-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

    R=0.2 azimuthal charged jet resolution for 0-10% Pb-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV

  • Fig. Group : hadron+jet acoplanarity measurement in Pb-Pb collisions
  • PWG : PWG-JE (Jets)
  • Energy: 5.02 TeV
  • System: Pb-Pb

    • 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
  • PWG : PWG-JE (Jets)
  • Energy: 5.02 TeV
  • System: Pb-Pb

    • R=0.2 hadron+jet $\Delta\phi$ distribution for $30 < p_{\mathrm{T,jet}^{ch}} < 40$ GeV/c in 0-10% Pb-Pb collisions at $\sqrt{\it{s}_{NN}} = 5.02$ TeV, compared to PYTHIA

  • Fig. Group : hadron+jet acoplanarity measurement in Pb-Pb collisions
  • PWG : PWG-JE (Jets)
  • Energy: 5.02 TeV
  • System: Pb-Pb

    • Measurements of the groomed jet radius and groomed momentum fraction in pp and central Pb–Pb collisions at 5.02 TeV

    Subleading prong residual, R=0.4

  • Fig. Group : Measurements of the groomed jet radius and groomed momentum fraction in pp and central Pb–Pb collisions at 5.02 TeV
  • PWG : PWG-JE (Jets)
  • Energy: 5.02 TeV
  • System: p-p
    • ,
  • System: Pb-Pb

    • Subleading prong purity, R=0.4

  • Fig. Group : Measurements of the groomed jet radius and groomed momentum fraction in pp and central Pb–Pb collisions at 5.02 TeV
  • PWG : PWG-JE (Jets)
  • Energy: 5.02 TeV
  • System: p-p
    • ,
  • System: Pb-Pb

    • zg for R=0.4, zcut=0.2

  • Fig. Group : Measurements of the groomed jet radius and groomed momentum fraction in pp and central Pb–Pb collisions at 5.02 TeV
  • PWG : PWG-JE (Jets)
  • Energy: 5.02 TeV
  • System: p-p
    • ,
  • System: Pb-Pb

    • zg for R=0.2, zcut=0.2

  • Fig. Group : Measurements of the groomed jet radius and groomed momentum fraction in pp and central Pb–Pb collisions at 5.02 TeV
  • PWG : PWG-JE (Jets)
  • Energy: 5.02 TeV
  • System: p-p
    • ,
  • System: Pb-Pb

    • theta_g for R=0.4, zcut=0.2

  • Fig. Group : Measurements of the groomed jet radius and groomed momentum fraction in pp and central Pb–Pb collisions at 5.02 TeV
  • PWG : PWG-JE (Jets)
  • Energy: 5.02 TeV
  • System: p-p
    • ,
  • System: Pb-Pb

    • theta_g for R=0.2, zcut=0.2

  • Fig. Group : Measurements of the groomed jet radius and groomed momentum fraction in pp and central Pb–Pb collisions at 5.02 TeV
  • PWG : PWG-JE (Jets)
  • Energy: 5.02 TeV
  • System: p-p
    • ,
  • System: Pb-Pb

    • Dynamical grooming: $z_g$ in pp collisions

  • Fig. Group : Measurements of the groomed jet radius and groomed momentum fraction in pp and central Pb–Pb collisions at 5.02 TeV
  • PWG : PWG-JE (Jets)
  • Energy: 5.02 TeV
  • System: p-p

    • Dynamical grooming: $\theta_g$ in pp collisions

  • Fig. Group : Measurements of the groomed jet radius and groomed momentum fraction in pp and central Pb–Pb collisions at 5.02 TeV
  • PWG : PWG-JE (Jets)
  • Energy: 5.02 TeV
  • System: p-p

    • Hardest kt splittings in pp and PYTHIA at 5 TeV

    Hardest $k_{\mathrm{T}}$ jet splitting in pp collisions for dynamical time grooming

  • Fig. Group : Hardest kt splittings in pp and PYTHIA at 5 TeV
  • PWG : PWG-JE (Jets)
  • Energy: 5.02 TeV
  • System: p-p

    • Hardest $k_{\mathrm{T}}$ jet splitting in pp collisions for dynamical $k_{\mathrm{T}}$

  • Fig. Group : Hardest kt splittings in pp and PYTHIA at 5 TeV
  • PWG : PWG-JE (Jets)
  • Energy: 5.02 TeV
  • System: p-p

    • Hardest $k_{\mathrm{T}}$ jet splitting in pp collisions for leading $k_{\mathrm{T}}$ with z > 0.2

  • Fig. Group : Hardest kt splittings in pp and PYTHIA at 5 TeV
  • PWG : PWG-JE (Jets)
  • Energy: 5.02 TeV
  • System: p-p

    • Hardest $k_{\mathrm{T}}$ jet splitting in pp collisions for leading $k_{\mathrm{T}}$

  • Fig. Group : Hardest kt splittings in pp and PYTHIA at 5 TeV
  • PWG : PWG-JE (Jets)
  • Energy: 5.02 TeV
  • System: p-p

    • Hardest $k_{\mathrm{T}}$ jet splitting in pp collisions - comparison of grooming methods with PYTHIA

  • Fig. Group : Hardest kt splittings in pp and PYTHIA at 5 TeV
  • PWG : PWG-JE (Jets)
  • Energy: 5.02 TeV
  • System: p-p

    • Hardest $k_{\mathrm{T}}$ jet splitting in pp collisions - comparison of grooming methods

  • Fig. Group : Hardest kt splittings in pp and PYTHIA at 5 TeV
  • PWG : PWG-JE (Jets)
  • Energy: 5.02 TeV
  • System: p-p

    • W measurement in the single-muon channel at forward rapidity in p-Pb at 8.16 TeV

    Lepton charge asymmetry of mu from W in p-Pb at 8.16 TeV compared to theory

  • Fig. Group : W measurement in the single-muon channel at forward rapidity in p-Pb at 8.16 TeV
  • PWG : PWG-HF (Heavy Flavour)
  • Energy: 8 TeV
  • System: p-Pb

    • Differential cross section of W+ at backward vs theory

  • Fig. Group : W measurement in the single-muon channel at forward rapidity in p-Pb at 8.16 TeV
  • PWG : PWG-HF (Heavy Flavour)
  • Energy: 8 TeV
  • System: p-Pb

    • Differential cross section of W- at backward vs theory

  • Fig. Group : W measurement in the single-muon channel at forward rapidity in p-Pb at 8.16 TeV
  • PWG : PWG-HF (Heavy Flavour)
  • Energy: 8 TeV
  • System: p-Pb

    • Differential cross section of W+ at forward vs theory

  • Fig. Group : W measurement in the single-muon channel at forward rapidity in p-Pb at 8.16 TeV
  • PWG : PWG-HF (Heavy Flavour)
  • Energy: 8 TeV
  • System: p-Pb

    • Differential cross section of W- at forward vs theory

  • Fig. Group : W measurement in the single-muon channel at forward rapidity in p-Pb at 8.16 TeV
  • PWG : PWG-HF (Heavy Flavour)
  • Energy: 8 TeV
  • System: p-Pb

    • Cross section of mu+ from W+ in p-Pb at 8.16 TeV compared to theory

  • Fig. Group : W measurement in the single-muon channel at forward rapidity in p-Pb at 8.16 TeV
  • PWG : PWG-HF (Heavy Flavour)
  • Energy: 8 TeV
  • System: p-Pb

    • Cross section of mu- from W- in p-Pb at 8.16 TeV compared to theory

  • Fig. Group : W measurement in the single-muon channel at forward rapidity in p-Pb at 8.16 TeV
  • PWG : PWG-HF (Heavy Flavour)
  • Energy: 8 TeV
  • System: p-Pb

    • Transverse momentum dependent flow vector fluctuations in Pb--Pb collisions at 5.02 TeV

    <cos 4[Psi_2(p_T^a) - Psi_2(p_T^t)]> with etagap > 0.8 for various trigger particle pT in centrality 0-5%, 20-30% and 40-50%

  • Fig. Group : Transverse momentum dependent flow vector fluctuations in Pb--Pb collisions at 5.02 TeV
  • PWG : PWG-CF (Flow and Correlations)
  • Energy: 5.02 TeV
  • System: Pb-Pb

    • <cos 4[Psi_2(p_T^a) - Psi_2(p_T^t)]> with etagap > 0.8 in centrality 0-5%, 5-10%, 10-20%, 20-30%. 30-40% and 40-50%

  • Fig. Group : Transverse momentum dependent flow vector fluctuations in Pb--Pb collisions at 5.02 TeV
  • PWG : PWG-CF (Flow and Correlations)
  • Energy: 5.02 TeV
  • System: Pb-Pb

    • NSC(3,2_pt) and NSC(2,3_pt) and the comparison to hydrodynamic calculations in centrality 5-10%, 10-20%, 20-30%, 30-40% and 40-50%

  • Fig. Group : Transverse momentum dependent flow vector fluctuations in Pb--Pb collisions at 5.02 TeV
  • PWG : PWG-CF (Flow and Correlations)
  • Energy: 5.02 TeV
  • System: Pb-Pb

    • NSC(3,2_pt) and NSC(4,2_pt) and the comparison to hydrodynamic calculations in centrality 5-10%, 10-20%, 20-30%, 30-40% and 40-50%

  • Fig. Group : Transverse momentum dependent flow vector fluctuations in Pb--Pb collisions at 5.02 TeV
  • PWG : PWG-CF (Flow and Correlations)
  • Energy: 5.02 TeV
  • System: Pb-Pb

    • r3 with etagap > 0.8 for various trigger particle pT in centrality 0-5%, 20-30% and 40-50%

  • Fig. Group : Transverse momentum dependent flow vector fluctuations in Pb--Pb collisions at 5.02 TeV
  • PWG : PWG-CF (Flow and Correlations)
  • Energy: 5.02 TeV
  • System: Pb-Pb

    • r3 with etagap > 0.8 in centrality 0-5%, 5-10%, 10-20%, 20-30%, 30-40% and 40-50%

  • Fig. Group : Transverse momentum dependent flow vector fluctuations in Pb--Pb collisions at 5.02 TeV
  • PWG : PWG-CF (Flow and Correlations)
  • Energy: 5.02 TeV
  • System: Pb-Pb

    • r2 with etagap > 0.8 for various trigger particle pT in centrality 0-5%, 20-30% and 40-50%

  • Fig. Group : Transverse momentum dependent flow vector fluctuations in Pb--Pb collisions at 5.02 TeV
  • PWG : PWG-CF (Flow and Correlations)
  • Energy: 5.02 TeV
  • System: Pb-Pb

    • r2 with etagap > 0.8 and the comparison to hydrodynamic calculation in centrality 0-5%, 5-10%, 10-20%, 20-30%, 30-40% and 40-50%

  • Fig. Group : Transverse momentum dependent flow vector fluctuations in Pb--Pb collisions at 5.02 TeV
  • PWG : PWG-CF (Flow and Correlations)
  • Energy: 5.02 TeV
  • System: Pb-Pb

    • v4{2}/v4[2] with etagap > 0.8 and the comparison to hydrodynamic calculation in centrality 0-5%, 5-10%, 10-20%, 20-30%, 30-40% and 40-50%

  • Fig. Group : Transverse momentum dependent flow vector fluctuations in Pb--Pb collisions at 5.02 TeV
  • PWG : PWG-CF (Flow and Correlations)
  • Energy: 5.02 TeV
  • System: Pb-Pb

    • v3{2}/v3[2] with etagap > 0.8 and the comparison to hydrodynamic calculation in centrality 0-5%, 5-10%, 10-20%, 20-30%, 30-40% and 40-50%

  • Fig. Group : Transverse momentum dependent flow vector fluctuations in Pb--Pb collisions at 5.02 TeV
  • PWG : PWG-CF (Flow and Correlations)
  • Energy: 5.02 TeV
  • System: Pb-Pb

    • v2{2}/v2[2] with etagap > 0.8 and the comparison to hydrodynamic calculation in centrality 0-5%, 5-10%, 10-20%, 20-30%, 30-40% and 40-50%

  • Fig. Group : Transverse momentum dependent flow vector fluctuations in Pb--Pb collisions at 5.02 TeV
  • PWG : PWG-CF (Flow and Correlations)
  • Energy: 5.02 TeV
  • System: Pb-Pb

    • Preliminary: Neutral meson measurements in p-Pb collisions at √s = 8.16 TeV

    Ratio of combined $\pi^0$ meson measurement to fit in referece measurement in pp collisions at 8 TeV with theory

  • Fig. Group : Preliminary: Neutral meson measurements in p-Pb collisions at √s = 8.16 TeV
  • PWG : PWG-GA (Photons, Neutral Mesons)
  • Energy: 8 TeV
  • System: p-p

    • Ratio of individual $\pi^0$ meson measurements to combined fit in the reference measurement in pp collisions at 8 TeV

  • Fig. Group : Preliminary: Neutral meson measurements in p-Pb collisions at √s = 8.16 TeV
  • PWG : PWG-GA (Photons, Neutral Mesons)
  • Energy: 8 TeV
  • System: p-p

    • Ratio of combined $\eta$ meson measurement to fit in p-Pb collisions at 8.16 TeV

  • Fig. Group : Preliminary: Neutral meson measurements in p-Pb collisions at √s = 8.16 TeV
  • PWG : PWG-GA (Photons, Neutral Mesons)
  • Energy: 8 TeV
  • System: p-Pb

    • Ratio of combined $\pi^0$ meson measurement to fit in p-Pb collisions at 8.16 TeV

  • Fig. Group : Preliminary: Neutral meson measurements in p-Pb collisions at √s = 8.16 TeV
  • PWG : PWG-GA (Photons, Neutral Mesons)
  • Energy: 8 TeV
  • System: p-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

    • Self normalization yield of phi-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

    • Upsilon -> mu+mu-

    Quarkonia production as a function of mid-rapidity charged-particle multiplicity in pp collisions at 13 TeV

  • Fig. Group : Upsilon -> mu+mu-
  • PWG : PWG-DQ (Dileptons and Quarkonia)
  • Energy: 13 TeV
  • System: p-p