Public Preliminary figures by analysis
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
ML Full Jet Raa Compared to Area-Based Raa, R=0.4, 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
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
lambda_Theta, lambda_Phi, lambda_ThetaPhi vs centrality in Pb-Pb collisions at sqrt(s_NN) = 5.02 TeV, in the Helicity and Collins-Soper reference frames
- 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
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
- 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
- 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
- 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 densities at mid-rapidity (|\eta|<1.0)
- 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 densities at mid-rapidity (|\eta|<1.0)
- 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
- Fig. Group : Low mass dimuons
- PWG : PWG-LF (Light Flavour Spectra)
- Energy: 13 TeV
- System: p-p
pT spectra of omega-meson in pp collisions in SPDTrk multiplicity classes and Ratios to INEL>0 with SPDTrk percentile
- Fig. Group : Low mass dimuons
- PWG : PWG-LF (Light Flavour Spectra)
- Energy: 13 TeV
- System: p-p
pT spectra of phi-meson in pp collisions in SPD Trk multiplicity classes and Ratios to INEL>0 with SPDTrk percentile
- Fig. Group : Low mass dimuons
- PWG : PWG-LF (Light Flavour Spectra)
- Energy: 13 TeV
- System: p-p
RT dependence of charged particle production in pp, p-Pb and Pb-Pb collisions at 5.02 TeV
Ipp, IpA and IAA as a function of average multiplicity in transverse region for near side in pp, p-Pb and Pb-Pb collisions at 5.02 TeV
- Fig. Group : RT dependence of charged particle production in pp, p-Pb and Pb-Pb collisions at 5.02 TeV
- PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
- Energy: 5.02 TeV
- System: p-p, Pb-Pb, p-Pb
Cascades production as function of charged particle multiplicity in pp collisions at √s=5.02TeV[Spring2020]
Omega^{-} + anti-Omega^{+} pT-integrated yield as a function of charged particle multiplicity in pp collisions at \sqrt{s} = 5.02 compared with results in p-Pb collisions at \sqrt{s} = 5.02 TeV
- Fig. Group : Cascades production as function of charged particle multiplicity in pp collisions at √s=5.02TeV[Spring2020]
- PWG : PWG-LF (Light Flavour Spectra)
- Energy: 5.02 TeV
- System: p-p
Xi^{-} + anti-Xi^{+} pT-integrated yield as a function of charged particle multiplicity in pp collisions at \sqrt{s} = 5.02 compared with results in p-Pb collisions at \sqrt{s} = 5.02 TeV
- Fig. Group : Cascades production as function of charged particle multiplicity in pp collisions at √s=5.02TeV[Spring2020]
- PWG : PWG-LF (Light Flavour Spectra)
- Energy: 5.02 TeV
- System: p-p
Xi^{-} + anti-Xi^{+} average pT as a function of charged particle multiplicity at \sqrt{s} = 5.02 compared with results at \sqrt{s} = 7 and 13 TeV
- Fig. Group : Cascades production as function of charged particle multiplicity in pp collisions at √s=5.02TeV[Spring2020]
- PWG : PWG-LF (Light Flavour Spectra)
- Energy: 5.02 TeV
- System: p-p
Omega^{-} + anti-Omega^{+} average pT as a function of charged particle multiplicity at \sqrt{s} = 5.02 compared with results at \sqrt{s} = 7 and 13 TeV
- Fig. Group : Cascades production as function of charged particle multiplicity in pp collisions at √s=5.02TeV[Spring2020]
- PWG : PWG-LF (Light Flavour Spectra)
- Energy: 5.02 TeV
- System: p-p
Omega^{-} + anti-Omega^{+} pT-integrated yield as a function of charged particle multiplicity at \sqrt{s} = 5.02 compared with results at \sqrt{s} = 7 and 13 TeV
- Fig. Group : Cascades production as function of charged particle multiplicity in pp collisions at √s=5.02TeV[Spring2020]
- PWG : PWG-LF (Light Flavour Spectra)
- Energy: 5.02 TeV
- System: p-p
Xi^{-} + anti-Xi^{+} pT-integrated yield as a function of charged particle multiplicity at \sqrt{s} = 5.02 compared with results at \sqrt{s} = 7 and 13 TeV
- Fig. Group : Cascades production as function of charged particle multiplicity in pp collisions at √s=5.02TeV[Spring2020]
- PWG : PWG-LF (Light Flavour Spectra)
- Energy: 5.02 TeV
- System: p-p
Xi^{-} + anti-Xi^{+} pT-spectra in different multiplicity bins in proton-proton collisions at \sqrt(s) = 5.02 TeV
- Fig. Group : Cascades production as function of charged particle multiplicity in pp collisions at √s=5.02TeV[Spring2020]
- PWG : PWG-LF (Light Flavour Spectra)
- Energy: 5.02 TeV
- System: p-p
Omega^{-} + anti-Omega^{+} pT-spectra in different multiplicity bins in proton-proton collisions at \sqrt(s) = 5.02 TeV
- Fig. Group : Cascades production as function of charged particle multiplicity in pp collisions at √s=5.02TeV[Spring2020]
- PWG : PWG-LF (Light Flavour Spectra)
- Energy: 5.02 TeV
- System: p-p
QM19 talk: vn ESE in Pb-Pb and Xe-Xe collisions
vn of inclusive and identified particles for unbiased, 0-10% and 90-100% qn classes for 5-10% and 30-40% centrality classes in Pb-Pb collisions
- Fig. Group : QM19 talk: vn ESE in Pb-Pb and Xe-Xe collisions
- PWG : PWG-CF (Flow and Correlations)
- Energy: 5.02 TeV
- System: Pb-Pb
Transverse momentum spectra of charged particles as a function of Underlying Event activity in pp collisions at 13 TeV
Transverse pT spectra
- Fig. Group : Transverse momentum spectra of charged particles as a function of Underlying Event activity in pp collisions at 13 TeV
- PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
- Energy: 13 TeV
- System: p-p
QM2019 h+jet correlations pp 13 TeV
Scaled width of the V0 asymmetry distribution as a function of V0M/<V0M> in pp 13 TeV
- Fig. Group : QM2019 h+jet correlations pp 13 TeV
- PWG : PWG-JE (Jets)
- Energy: 13 TeV
- System: Pb-Pb
Mean V0M asymmetry as a function of V0M/<V0M> for different event bias in pp 13 TeV
- Fig. Group : QM2019 h+jet correlations pp 13 TeV
- PWG : PWG-JE (Jets)
- Energy: 13 TeV
- System: Pb-Pb
V0M asymmetry distributions in bins of V0M/<V0M> in pp 13 TeV for TT{6,7}
- Fig. Group : QM2019 h+jet correlations pp 13 TeV
- PWG : PWG-JE (Jets)
- Energy: 13 TeV
- System: Pb-Pb
V0M asymmetry distributions in bins of V0M/<V0M> in pp 13 TeV
- Fig. Group : QM2019 h+jet correlations pp 13 TeV
- PWG : PWG-JE (Jets)
- Energy: 13 TeV
- System: Pb-Pb
V0M/<V0M> distribution as measured by ALICE in high multiplicity pp 13 TeV in 2016, 2017 and 2018
- Fig. Group : QM2019 h+jet correlations pp 13 TeV
- PWG : PWG-JE (Jets)
- Energy: 13 TeV
- System: Pb-Pb
V0M/<V0M> distribution as measured by ALICE in minimum bias pp 13 TeV in 2016, 2017 and 2018
- Fig. Group : QM2019 h+jet correlations pp 13 TeV
- PWG : PWG-JE (Jets)
- Energy: 13 TeV
- System: Pb-Pb
V0M/<V0M> distribution as measured by ALICE in minimum bias pp 13 TeV and as simulated by PYTHIA8 Monash
- Fig. Group : QM2019 h+jet correlations pp 13 TeV
- PWG : PWG-JE (Jets)
- Energy: 13 TeV
- System: Pb-Pb
V0M/<V0M> distribution as measured by ALICE in minimum bias pp 13 TeV
- Fig. Group : QM2019 h+jet correlations pp 13 TeV
- PWG : PWG-JE (Jets)
- Energy: 13 TeV
- System: Pb-Pb
Per trigger normalized recoil jet yields associated to TT{20,30} and TT{6,7} and the corresponding Delta recoil spectrum as a function of jet pT in HM pp 13 TeV events
- Fig. Group : QM2019 h+jet correlations pp 13 TeV
- PWG : PWG-JE (Jets)
- Energy: 13 TeV
- System: Pb-Pb
Per trigger normalized recoil jet yields associated to TT{20,30} and TT{6,7} and the corresponding Delta recoil spectrum as a function of azimuth in HM pp 13 TeV events
- Fig. Group : QM2019 h+jet correlations pp 13 TeV
- PWG : PWG-JE (Jets)
- Energy: 13 TeV
- System: Pb-Pb
Delta recoil distributions for 15<pT,jet<20 GeV jet as measured by ALICE compated to PYTHIA events embedded to MB and HM pp 13 TeV
- Fig. Group : QM2019 h+jet correlations pp 13 TeV
- PWG : PWG-JE (Jets)
- Energy: 13 TeV
- System: Pb-Pb
Delta recoil distributions as measured by ALICE compated to PYTHIA events embedded to MB and HM pp 13 TeV
- Fig. Group : QM2019 h+jet correlations pp 13 TeV
- PWG : PWG-JE (Jets)
- Energy: 13 TeV
- System: Pb-Pb
Delta recoil distributions as measured by ALICE and simulated by PYTHIA8 particle level in MB and HM pp 13 TeV
- Fig. Group : QM2019 h+jet correlations pp 13 TeV
- PWG : PWG-JE (Jets)
- Energy: 13 TeV
- System: Pb-Pb
Per trigger normalized yield of 15<pT,jet<20 GeV recoil jets in MB and HM events for TT{20,30} in pp 13 TeV
- Fig. Group : QM2019 h+jet correlations pp 13 TeV
- PWG : PWG-JE (Jets)
- Energy: 13 TeV
- System: Pb-Pb
Delta_recoil distribution as a function of azimuth for charged akt R=0.4 jets with 40< pT,jet<60 GeV/c in pp 13 TeV
- Fig. Group : QM2019 h+jet correlations pp 13 TeV
- PWG : PWG-JE (Jets)
- Energy: 13 TeV
- System: Pb-Pb
Delta_recoil distribution as a function of azimuth for charged akt R=0.4 jets with 20< pT,jet<30 GeV/c in pp 13 TeV
- Fig. Group : QM2019 h+jet correlations pp 13 TeV
- PWG : PWG-JE (Jets)
- Energy: 13 TeV
- System: Pb-Pb
Delta_recoil distribution as a function of azimuth for charged akt R=0.4 jets with 15< pT,jet<20 GeV/c in pp 13 TeV
- Fig. Group : QM2019 h+jet correlations pp 13 TeV
- PWG : PWG-JE (Jets)
- Energy: 13 TeV
- System: Pb-Pb
Delta_recoil distribution as a function of azimuth for charged akt R=0.4 jets with 10< pT,jet<15 GeV/c in pp 13 TeV
- Fig. Group : QM2019 h+jet correlations pp 13 TeV
- PWG : PWG-JE (Jets)
- Energy: 13 TeV
- System: Pb-Pb
DEta-DPhi correlation functions in 13 TeV
Angular correlation functions for unlike-sign pairs of pions, kaons and protons
- Fig. Group : DEta-DPhi correlation functions in 13 TeV
- PWG : PWG-CF (Flow and Correlations)
- Energy: 13 TeV
- System: p-p
Angular correlations of like-sign particles (pions, kaons, protons) in pp collisions at 13 TeV
- Fig. Group : DEta-DPhi correlation functions in 13 TeV
- PWG : PWG-CF (Flow and Correlations)
- Energy: 13 TeV
- System: p-p
Projections of angular correlation functions for unlike-sign pairs of pions, kaons and protons
- Fig. Group : DEta-DPhi correlation functions in 13 TeV
- PWG : PWG-CF (Flow and Correlations)
- Energy: 13 TeV
- System: p-p
Projections of angular correlation functions for like-sign pairs of pions, kaons and protons
- Fig. Group : DEta-DPhi correlation functions in 13 TeV
- PWG : PWG-CF (Flow and Correlations)
- Energy: 13 TeV
- System: p-p
Preliminary - Neutral mesons in pp 5TeV and PbPb 5TeV
Eta - Ratio of individual measurements to combined - 0-10% centrality - PbPb 5TeV
- Fig. Group : Preliminary - Neutral mesons in pp 5TeV and PbPb 5TeV
- PWG : PWG-GA (Photons, Neutral Mesons)
- Energy: 5.02 TeV
- System: Pb-Pb
Eta to pi0 ratio - in-jet and MB - pp 5TeV
- Fig. Group : Preliminary - Neutral mesons in pp 5TeV and PbPb 5TeV
- PWG : PWG-GA (Photons, Neutral Mesons)
- Energy: 5.02 TeV
- System: p-p
Eta - in-jet and MB production - pp 5TeV
- Fig. Group : Preliminary - Neutral mesons in pp 5TeV and PbPb 5TeV
- PWG : PWG-GA (Photons, Neutral Mesons)
- Energy: 5.02 TeV
- System: p-p
Pi0 - in-jet and MB production - pp 5TeV
- Fig. Group : Preliminary - Neutral mesons in pp 5TeV and PbPb 5TeV
- PWG : PWG-GA (Photons, Neutral Mesons)
- Energy: 5.02 TeV
- System: p-p
Light-Flavour Hadron Production in pp Collisions at $\sqrt{s}$ = 13 TeV as a Function of $R_\textrm{T}$
$p_\textrm{T}$-differential model comparison of xi-to-pion ratio as a function of $R_\textrm{T}$ in the Away region for pp collisions at $\sqrt{s}$ = 13 TeV .
- Fig. Group : Light-Flavour Hadron Production in pp Collisions at $\sqrt{s}$ = 13 TeV as a Function of $R_\textrm{T}$
- PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
- Energy: 13 TeV
- System: p-p
$p_\textrm{T}$-differential model comparison of xi-to-pion ratio as a function of $R_\textrm{T}$ in the Transverse region for pp collisions at $\sqrt{s}$ = 13 TeV .
- Fig. Group : Light-Flavour Hadron Production in pp Collisions at $\sqrt{s}$ = 13 TeV as a Function of $R_\textrm{T}$
- PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
- Energy: 13 TeV
- System: p-p
$p_\textrm{T}$-differential model comparison of xi-to-pion ratio as a function of $R_\textrm{T}$ in the Toward region for pp collisions at $\sqrt{s}$ = 13 TeV .
- Fig. Group : Light-Flavour Hadron Production in pp Collisions at $\sqrt{s}$ = 13 TeV as a Function of $R_\textrm{T}$
- PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
- Energy: 13 TeV
- System: p-p
$p_\textrm{T}$-differential model comparison of kaon-to-pion ratio as a function of $R_\textrm{T}$ in the Away region for pp collisions at $\sqrt{s}$ = 13 TeV .
- Fig. Group : Light-Flavour Hadron Production in pp Collisions at $\sqrt{s}$ = 13 TeV as a Function of $R_\textrm{T}$
- PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
- Energy: 13 TeV
- System: p-p
$p_\textrm{T}$-differential model comparison of kaon-to-pion ratio as a function of $R_\textrm{T}$ in the Transverse region for pp collisions at $\sqrt{s}$ = 13 TeV .
- Fig. Group : Light-Flavour Hadron Production in pp Collisions at $\sqrt{s}$ = 13 TeV as a Function of $R_\textrm{T}$
- PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
- Energy: 13 TeV
- System: p-p
$p_\textrm{T}$-differential model comparison of kaon-to-pion ratio as a function of $R_\textrm{T}$ in the Toward region for pp collisions at $\sqrt{s}$ = 13 TeV .
- Fig. Group : Light-Flavour Hadron Production in pp Collisions at $\sqrt{s}$ = 13 TeV as a Function of $R_\textrm{T}$
- PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
- Energy: 13 TeV
- System: p-p
$p_\textrm{T}$-differential model comparison of proton-to-pion ratio as a function of $R_\textrm{T}$ in the Away region for pp collisions at $\sqrt{s}$ = 13 TeV .
- Fig. Group : Light-Flavour Hadron Production in pp Collisions at $\sqrt{s}$ = 13 TeV as a Function of $R_\textrm{T}$
- PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
- Energy: 13 TeV
- System: p-p
$p_\textrm{T}$-differential model comparison of proton-to-pion ratio as a function of $R_\textrm{T}$ in the Transverse region for pp collisions at $\sqrt{s}$ = 13 TeV .
- Fig. Group : Light-Flavour Hadron Production in pp Collisions at $\sqrt{s}$ = 13 TeV as a Function of $R_\textrm{T}$
- PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
- Energy: 13 TeV
- System: p-p
$p_\textrm{T}$-differential model comparison of proton-to-pion ratio as a function of $R_\textrm{T}$ in the Toward region for pp collisions at $\sqrt{s}$ = 13 TeV .
- Fig. Group : Light-Flavour Hadron Production in pp Collisions at $\sqrt{s}$ = 13 TeV as a Function of $R_\textrm{T}$
- PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
- Energy: 13 TeV
- System: p-p
$p_\textrm{T}$-differential model comparison of phi-to-pion ratio as a function of $R_\textrm{T}$ in the Away region for pp collisions at $\sqrt{s}$ = 13 TeV .
- Fig. Group : Light-Flavour Hadron Production in pp Collisions at $\sqrt{s}$ = 13 TeV as a Function of $R_\textrm{T}$
- PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
- Energy: 13 TeV
- System: p-p
$p_\textrm{T}$-differential model comparison of phi-to-pion ratio as a function of $R_\textrm{T}$ in the Transverse region for pp collisions at $\sqrt{s}$ = 13 TeV .
- Fig. Group : Light-Flavour Hadron Production in pp Collisions at $\sqrt{s}$ = 13 TeV as a Function of $R_\textrm{T}$
- PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
- Energy: 13 TeV
- System: p-p
$p_\textrm{T}$-differential model comparison of phi-to-pion ratio as a function of $R_\textrm{T}$ in the Toward region for pp collisions at $\sqrt{s}$ = 13 TeV .
- Fig. Group : Light-Flavour Hadron Production in pp Collisions at $\sqrt{s}$ = 13 TeV as a Function of $R_\textrm{T}$
- PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
- Energy: 13 TeV
- System: p-p
$p_\textrm{T}$-differential xi-to-pion ratio as a function of $R_\textrm{T}$ in the Away region for pp collisions at $\sqrt{s}$ = 13 TeV .
- Fig. Group : Light-Flavour Hadron Production in pp Collisions at $\sqrt{s}$ = 13 TeV as a Function of $R_\textrm{T}$
- PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
- Energy: 13 TeV
- System: p-p
$p_\textrm{T}$-differential xi-to-pion ratio as a function of $R_\textrm{T}$ in the Transverse region for pp collisions at $\sqrt{s}$ = 13 TeV .
- Fig. Group : Light-Flavour Hadron Production in pp Collisions at $\sqrt{s}$ = 13 TeV as a Function of $R_\textrm{T}$
- PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
- Energy: 13 TeV
- System: p-p