Charged-particle density in Transverse Side/region for track pT > 0.5GeV/c in pPb collisions at sqrt(s) = 5.02 TeV
- PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
- Energy: 5.02 TeV
- System p-p ,
- System p-Pb
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Charged-particle density in Away Side/region for track pT > 0.5GeV/c in pPb collisions at sqrt(s) = 5.02 TeV
- PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
- Energy: 5.02 TeV
- System p-p ,
- System p-Pb
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Charged-particle density in Near Side (towards region) for track pT > 0.5GeV/c in pPb collisions at sqrt(s) = 5.02 TeV
- PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
- Energy: 5.02 TeV
- System p-p ,
- System p-Pb
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Charged-particle density in Transverse Side/region for track pT > 0.5GeV/c in pp collisions at sqrt(s) = 5.02 TeV
- PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
- Energy: 5.02 TeV
- System p-p ,
- System p-Pb
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Charged-particle density in Near Side (towards region) for track pT > 0.5GeV/c in pp collisions at sqrt(s) = 5.02 TeV
- PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
- Energy: 5.02 TeV
- System p-p ,
- System p-Pb
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Charged-particle density in Away Side/region for track pT > 0.5GeV/c in pp collisions at sqrt(s) = 5.02 TeV
- PWG : PWG-MM (Monte Carlo generators and Minimum Bias)
- Energy: 5.02 TeV
- System p-p ,
- System p-Pb
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| Pseudorapidity distributions of photons compared with Charged particle measurements at Mid-rapidity in p-Pb collisions at $\sqrt{s\rm_{NN}}$ = 5.02 TeV
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| Centrality dependent Pseudorapidity distributions of photons compared with HIJING in p-Pb collisions at $\sqrt{s\rm_{NN}}$ = 5.02 TeV
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| Centrality dependent Pseudorapidity distributions of photons compared with DPMJET in p-Pb collisions at $\sqrt{s\rm_{NN}}$ = 5.02 TeV
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| Centrality dependent Pseudorapidity distributions of photons in p-Pb collisions at $\sqrt{s\rm_{NN}}$ = 5.02 TeV
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| Pseudorapidity distributions of photons in p-Pb collisions at $\sqrt{s\rm_{NN}}$ = 5.02 TeV
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| Multiplicity distribution of photons in p-Pb collisions at $\sqrt{s\rm_{NN}}$ = 5.02 TeV
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| Normalised Delta v3 of pions
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| Normalised Delta v2 of pions
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| Normalised Delta v3 of hadrons
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| Normalised Delta v2 of hadrons
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| v3vsAch of pions
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| v2vsAch of pions
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| v3vsAch of hadrons
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| v2vsAch of hadrons
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| Normalisedv3slope comparison of hadrons between ALICE and CMS
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| Normalisedv2slope comparison of hadrons between ALICE and CMS
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| Normalisedv3slope comparison of pions between ALICE and STAR
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| Normalisedv2slope comparison of pions between ALICE and STAR
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| Normalisedv3slope comparison of pions with hadrons
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| Normalisedv2v3slope comparison of pions
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| Normalisedv2v3slope comparison of hadrons
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| \Delta\varphi Projection of h-K^0_S - MC comparison
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| Isolated photon-hadron correlation functions in pp and p–Pb at sqrt(s) = 5.02 TeV, remaining zT bins
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| Signal region and background region correlation function comparison in p–Pb at sqrt(s) = 5.02 TeV
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| ML Pb--Pb Spectrum R = 0.4, 0-10%, Compared to AB method
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| 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
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| ML Raa Fragmentation Bias Curves with Model Comparisons R = 0.4, 0-10%
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| ML Full Jet Raa, R = 0.4, 0-10%
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| ML Pb--Pb Full Jet Spectrum R = 0.4, 0-10%
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| ML Raa with Fragmentation Bias Curves
|
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| Acceptance-times-efficiency for J/psi as function of CosTheta and Centrality in the Helicity reference frame
|
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| Fit to the corrected J/psi distribution as a function of cosTheta in 0-20% and 60-90% centrality classes
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| Fit to the J/psi distribution as a function of cosTheta for 0-20% and 60-90% centrality classes
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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
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|
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
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|
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
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|
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
|
|
| ML Full Jet Raa Compared to Area-Based Raa, R=0.4, 10%
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| 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
|
|
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
|
|
| 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
|
|
| 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
|
|
| Transverse pT spectra
|
|
| Scaled width of the V0 asymmetry distribution as a function of V0M/<V0M> in pp 13 TeV
|
|
| Mean V0M asymmetry as a function of V0M/<V0M> for different event bias in pp 13 TeV
|
|
| V0M asymmetry distributions in bins of V0M/<V0M> in pp 13 TeV for TT{6,7}
|
|
| V0M asymmetry distributions in bins of V0M/<V0M> in pp 13 TeV
|
|
| V0M/<V0M> distribution as measured by ALICE in high multiplicity pp 13 TeV in 2016, 2017 and 2018
|
|
| V0M/<V0M> distribution as measured by ALICE in minimum bias pp 13 TeV in 2016, 2017 and 2018
|
|
| V0M/<V0M> distribution as measured by ALICE in minimum bias pp 13 TeV and as simulated by PYTHIA8 Monash
|
|
| V0M/<V0M> distribution as measured by ALICE in minimum bias pp 13 TeV
|
|
| 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
|
|
| 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
|
|
| 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
|
|
| Delta recoil distributions as measured by ALICE compated to PYTHIA events embedded to MB and HM pp 13 TeV
|
|
| Delta recoil distributions as measured by ALICE and simulated by PYTHIA8 particle level in MB and HM pp 13 TeV
|
|
| 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
|
|
| 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
|
|
| 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
|
|
| 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
|
|
| 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
|
|
| Angular correlation functions for unlike-sign pairs of pions, kaons and protons
|
|
| Angular correlations of like-sign particles (pions, kaons, protons) in pp collisions at 13 TeV
|
|
| Projections of angular correlation functions for unlike-sign pairs of pions, kaons and protons
|
|
| Projections of angular correlation functions for like-sign pairs of pions, kaons and protons
|
|
| Eta - Ratio of individual measurements to combined - 0-10% centrality - PbPb 5TeV
|
|
| Eta to pi0 ratio - in-jet and MB - pp 5TeV
|
|
| Eta - in-jet and MB production - pp 5TeV
|
|
| Pi0 - in-jet and MB production - pp 5TeV
|
|
| $p_\textrm{T}$-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 .
|
|
| $p_\textrm{T}$-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 .
|
|
| $p_\textrm{T}$-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 .
|
|
| $p_\textrm{T}$-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 .
|
|
| $p_\textrm{T}$-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 .
|
|
| $p_\textrm{T}$-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 .
|
|
| $p_\textrm{T}$-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 .
|
|
| $p_\textrm{T}$-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 .
|
|
| $p_\textrm{T}$-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 .
|
|
| $p_\textrm{T}$-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 .
|
|
| $p_\textrm{T}$-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 .
|
|
| $p_\textrm{T}$-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 .
|
|
| $p_\textrm{T}$-differential xi-to-pion ratio as a function of $R_\textrm{T}$ in the Away region for pp collisions at $\sqrt{s}$ = 13 TeV .
|
|
| $p_\textrm{T}$-differential xi-to-pion ratio as a function of $R_\textrm{T}$ in the Transverse region for pp collisions at $\sqrt{s}$ = 13 TeV .
|
|
| $p_\textrm{T}$-differential xi-to-pion ratio as a function of $R_\textrm{T}$ in the Toward region for pp collisions at $\sqrt{s}$ = 13 TeV .
|
|
| $p_\textrm{T}$-differential kaon-to-pion ratio as a function of $R_\textrm{T}$ in the Away region for pp collisions at $\sqrt{s}$ = 13 TeV .
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|
